From 80016c7c4665827493d4f9985dbe8a455083c2a6 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 5 Jun 2017 17:15:32 -0700 Subject: [PATCH 001/216] Started work on mesh for 3-D subduction zone example. --- examples/3d/subduction/mesh/README | 1 + .../3d/subduction/mesh/generate_slabtop.py | 194 ++++++++++++++++++ examples/3d/subduction/mesh/geometry.jou | 93 +++++++++ 3 files changed, 288 insertions(+) create mode 100644 examples/3d/subduction/mesh/README create mode 100755 examples/3d/subduction/mesh/generate_slabtop.py create mode 100644 examples/3d/subduction/mesh/geometry.jou diff --git a/examples/3d/subduction/mesh/README b/examples/3d/subduction/mesh/README new file mode 100644 index 0000000000..80e3e92e48 --- /dev/null +++ b/examples/3d/subduction/mesh/README @@ -0,0 +1 @@ +./generate_slabtop.py --slab-filename=cas_contours_dep.in.txt --journal-filename=slabtop_surf.jou --stride=10 diff --git a/examples/3d/subduction/mesh/generate_slabtop.py b/examples/3d/subduction/mesh/generate_slabtop.py new file mode 100755 index 0000000000..3c7c67c148 --- /dev/null +++ b/examples/3d/subduction/mesh/generate_slabtop.py @@ -0,0 +1,194 @@ +#!/usr/bin/env python +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# Generate CUBIT/Trelis journal file to create slab surface from Slab +# 1.0 contours. +# +# We decimate the contours from Slab 1.0 in order to reduce the +# complexity of the slab geometry so that the mesh generation is +# faster. +# +# The Slab contours can be downloaded from: +# https://earthquake.usgs.gov/data/slab/models.php +# +# The reference for the Slab 1.0 model is: +# +# Hayes, G. P., D. J. Wald, and R. L. Johnson (2012), Slab1.0: A +# three-dimensional model of global subduction zone geometries, +# J. Geophys. Res., 117, B01302, doi:10.1029/2011JB008524. + +import numpy +from collections import OrderedDict + +# ---------------------------------------------------------------------- +class JournalFile(object): + """JournalFile object for writing CUBIT/Trelis journal file. + """ + + def __init__(self, filename): + """Constructor. + """ + self.file = open(filename, "w") + return + + + def writeHeader(self): + """Write header for journal file. + """ + self.file.write("# CUBIT/Trelis journal file generated by generate_slabtop.py\n" \ + "#\n" \ + "# Create an ACIS NURBS surface from contours.\n" \ + "#\n" \ + "reset\n\n") + return + + def writeTrailer(self): + """Write trailer for journal file. + """ + self.file.write("# Create surface from curves.\n" \ + "create surface skin curve all\n" \ + "delete curve all\n\n" \ + "# Save surface to ACIS file for later use.\n" \ + "export acis 'slabtop_surf.sat' overwrite\n") + return + + + def writeContour(self, points): + """Write contour to journal file. + """ + self.file.write("# Contour\n") + self.file.write("create vertex x %12.6e y %12.6e z %12.6e\n" % tuple(points[0])) + self.file.write("${pBegin=Id('vertex')}\n") + for pt in points[1:]: + self.file.write("create vertex x %12.6e y %12.6e z %12.6e\n" % tuple(pt)) + self.file.write("${pEnd=Id('vertex')}\n"\ + "create curve spline vertex {pBegin} to {pEnd} delete\n\n") + return + + + def close(self): + self.file.close() + self.file = None + return + + +# ---------------------------------------------------------------------- +class SlabContoursFile(object): + """SlabContourFile object for reading contours from a Slab 1.0 contour file.. + """ + + def __init__(self, filename): + self.filename = filename + return + + + def read(self): + """Read contours from Slab 1.0 file. + """ + with open(self.filename, "r") as file: + lines = file.readlines() + contours = {} + points = [] + key = None + for line in lines: + if line.strip() == "END": + contours[key] = points + points = [] + continue + if len(line.split()) == 1: + key = int(line) + continue + pt = map(float, line.strip().split()) + points.append(pt) + # Sort contours by key (depth) + self.contours = OrderedDict(sorted(contours.items(), key=lambda x: x[0])).values() + + +# ---------------------------------------------------------------------- +class ContourApp(object): + """ContourApp object for top-level application workflow. + """ + + def __init__(self): + """Constructor. + """ + self.sfilename = None + self.jfilename = None + self.pointsStride = 1 + return + + + def run(self): + """Open Slab 1.0 input file and journal output file and loop over + contours. + """ + jfile = JournalFile(self.jfilename) + jfile.writeHeader() + + sfile = SlabContoursFile(self.sfilename) + sfile.read() + + for contour in sfile.contours: + points = self._decimate(contour) + self._toXYZ(points) + jfile.writeContour(points) + jfile.writeTrailer() + jfile.close() + return + + + def _decimate(self, points): + """Decimate the number of points in a contour. + """ + pointsD = numpy.array(points[::self.pointsStride], dtype=numpy.float64) + if (len(points)-1) % self.pointsStride: + pointsD = numpy.vstack((pointsD, numpy.array([points[-1]]),)) + return pointsD + + def _toXYZ(self, points): + """Transform from geographic coordinates and depth in km to geographic + projected coordinate system. The coordinate system is imported + from coordsys.py. + + """ + import coordsys + coordsys.geoToMesh(points) + points[:,2] *= 1.0e+3 + return + + +# ====================================================================== +if __name__ == "__main__": + import argparse + + DESCRIPTION = "Python script to create a CUBIT/Trelis "\ + "journal file that generates the surface from Slab 1.0." + + parser = argparse.ArgumentParser(description=DESCRIPTION) + parser.add_argument("--stride", action="store", dest="stride", type=int, default=5) + parser.add_argument("--journal-filename", action="store", dest="jfilename", default="contours.jou") + parser.add_argument("--slab-filename", action="store", dest="sfilename", default=None, required=True) + args = parser.parse_args() + + app = ContourApp() + app.sfilename = args.sfilename + app.jfilename = args.jfilename + app.pointsStride = args.stride + app.run() + + +# End of file diff --git a/examples/3d/subduction/mesh/geometry.jou b/examples/3d/subduction/mesh/geometry.jou new file mode 100644 index 0000000000..a21704b38c --- /dev/null +++ b/examples/3d/subduction/mesh/geometry.jou @@ -0,0 +1,93 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# CUBIT journal file with geometry for example showing how to import +# several surfaces (topography, subduction interface, splay fault), and +# mesh the resulting volumes. +# +# We also use the CUBIT support for APREPRO (the expressions in +# braces), which includes units and mathematical functions. See the +# APREPRO section in the appendix of the CUBIT documentation for more +# information. +# +# ---------------------------------------------------------------------- +# Set units to SI. +# ---------------------------------------------------------------------- +${Units('si')} +# +# ---------------------------------------------------------------------- +# Reset geometry. +# ---------------------------------------------------------------------- +reset + +# ---------------------------------------------------------------------- +# Create block +# ---------------------------------------------------------------------- +# Block is 800 km x 800 km x 400 km +${blockLength=800.0*km} +${blockWidth=800.0*km} +${blockHeight=400.0*km} + +brick x {blockLength} y {blockWidth} z {blockHeight} +${idVol=Id("volume")} + +# Translate block so top is a z=0. +${moveX=-60.0*km} +${moveY=0.0*km} + +volume {idVol} move x {moveX} y {moveY} z {-0.5*blockHeight} + +# ---------------------------------------------------------------------- +# Import subduction interface. +# ---------------------------------------------------------------------- +import Acis "slabtop_surf.sat" +${idSurf=Id("surface")} +surface {idSurf} name "s_slabtop" + +# Slab bottom +${n_x=-0.209} +${n_y=+0.016} +${n_z=-0.979} +${slabThickness=50.0*km} +surface s_slabtop copy move x {n_x*slabThickness} y {n_y*slabThickness} z {n_z*slabThickness} + +# ---------------------------------------------------------------------- +# Webcut block with topography and delete volume lying above topography. +# ---------------------------------------------------------------------- +webcut volume {idVol} with sheet surface 7 +delete volume 1 +delete body 2 + +# ---------------------------------------------------------------------- +# Webcut remaining portion of block with subduction interface. +# ---------------------------------------------------------------------- +webcut volume 5 with sheet surface 8 +delete body 3 + +# ---------------------------------------------------------------------- +# Webcut volume above subduction interface with splay fault. +# ---------------------------------------------------------------------- +webcut volume 5 with sheet surface 9 +delete body 4 + +# ---------------------------------------------------------------------- +# Imprint all volumes, then merge. +# ---------------------------------------------------------------------- +imprint all with volume all +merge all + +# End of file + From a3273bd500eb5bba8be4aa4e8aa19104c613fa3d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 6 Jun 2017 17:17:35 -0700 Subject: [PATCH 002/216] More work on 3-D subduction zone mesh. --- examples/3d/subduction/mesh/README | 5 + .../mesh/cas_contours_dep.in.txt.gz | Bin 0 -> 43302 bytes ...erate_slabtop.py => generate_slabsurfs.py} | 188 ++++++++++++++---- examples/3d/subduction/mesh/geometry.jou | 80 +++++--- 4 files changed, 211 insertions(+), 62 deletions(-) create mode 100644 examples/3d/subduction/mesh/cas_contours_dep.in.txt.gz rename examples/3d/subduction/mesh/{generate_slabtop.py => generate_slabsurfs.py} (51%) diff --git a/examples/3d/subduction/mesh/README b/examples/3d/subduction/mesh/README index 80e3e92e48..09f121c1f2 100644 --- a/examples/3d/subduction/mesh/README +++ b/examples/3d/subduction/mesh/README @@ -1 +1,6 @@ ./generate_slabtop.py --slab-filename=cas_contours_dep.in.txt --journal-filename=slabtop_surf.jou --stride=10 + + + + +CUBIT> surface 16 Scheme TriMesh geometry approximation angle 90.0 \ No newline at end of file diff --git a/examples/3d/subduction/mesh/cas_contours_dep.in.txt.gz b/examples/3d/subduction/mesh/cas_contours_dep.in.txt.gz new file mode 100644 index 0000000000000000000000000000000000000000..7e80755e1626afd266ef56360df6e609e0ae3d3f GIT binary patch literal 43302 zcmV(xKbZ>QXb6;d-a4u`~{~dpl%~u|!5~H)QV9=W&FTHm5A9`$mZV`%-x@kf9GPtF81qeUB!s 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examples/3d/subduction/mesh/generate_slabtop.py rename to examples/3d/subduction/mesh/generate_slabsurfs.py index 3c7c67c148..b98d33a30c 100755 --- a/examples/3d/subduction/mesh/generate_slabtop.py +++ b/examples/3d/subduction/mesh/generate_slabsurfs.py @@ -49,26 +49,32 @@ def __init__(self, filename): def writeHeader(self): """Write header for journal file. """ - self.file.write("# CUBIT/Trelis journal file generated by generate_slabtop.py\n" \ - "#\n" \ - "# Create an ACIS NURBS surface from contours.\n" \ + self.file.write("# CUBIT/Trelis journal file generated by generate_slabsurfs.py\n" \ "#\n" \ + "# Create ACIS NURBS surfaces for top and bottom of slab.\n\n") + return + + def newSurface(self): + """ + """ + self.file.write("# New surface.\n" \ "reset\n\n") return - def writeTrailer(self): - """Write trailer for journal file. + + def skinSurface(self, filename): + """Create surface and save it in an ACIS file. """ self.file.write("# Create surface from curves.\n" \ "create surface skin curve all\n" \ "delete curve all\n\n" \ "# Save surface to ACIS file for later use.\n" \ - "export acis 'slabtop_surf.sat' overwrite\n") + "export acis '%s' overwrite\n\n" % filename) return - def writeContour(self, points): - """Write contour to journal file. + def addContour(self, points): + """Add contour to journal file. """ self.file.write("# Contour\n") self.file.write("create vertex x %12.6e y %12.6e z %12.6e\n" % tuple(points[0])) @@ -106,7 +112,7 @@ def read(self): key = None for line in lines: if line.strip() == "END": - contours[key] = points + contours[key] = numpy.array(points, dtype=numpy.float64) points = [] continue if len(line.split()) == 1: @@ -114,9 +120,103 @@ def read(self): continue pt = map(float, line.strip().split()) points.append(pt) - # Sort contours by key (depth) - self.contours = OrderedDict(sorted(contours.items(), key=lambda x: x[0])).values() + self.contours = contours + return + + +# ---------------------------------------------------------------------- +class ExtendSlab(object): + + def __init__(self, slab, stride): + """Constructor. + """ + self.contours = slab.contours + self._decimate(stride) + self._toXYZ() + return + + + def addUpDipContours(self, elevKm=1.0, strikeDeg=0.0, dipDeg=10.0, extendDistKm=600.0): + """Add contours up-dip from original contours. + Keyword arguments: + elevKm -- Elevation in kilometers of additional contours. + strikeDeg -- Approximate strike of fault in degrees (default 0.0). + dipDeg -- Dip angle in degrees at up-dip edge of fault (default 10.0). + extendDistKm -- Distance in kilometers to extend slab surface in up-dip direction. + + We increase the horizontal distance between the contours at a + geometric rate. The first contour is at a distance of + distHoriz, followed by 2*distHoriz, 4*distHoriz, etc. + + The horizontal distance of contour n from the original one is + (2**(n+1)-1)) * distHoriz, n=0,1,2,... + + """ + import math + key = min(self.contours.keys()) + contourTop = self.contours[key] + zTop = contourTop[0][2] + + distHoriz = (elevKm*1.0e+3-zTop)/math.tan(dipDeg*math.pi/180.0) + dx = -distHoriz*math.cos(strikeDeg*math.pi/180.0) + dy = distHoriz*math.sin(strikeDeg*math.pi/180.0) + + contoursUpDip = {} + numContours = int(math.ceil(math.log((extendDistKm*1.0e+3/distHoriz)+1)/math.log(2.0))) + for i in xrange(numContours): + contour = numpy.array(contourTop) + contour[:,0] += (2**i)*dx + contour[:,1] += (2**i)*dy + contour[:,2] = elevKm*1.0e+3 + contoursUpDip[-i] = contour + self.contoursUpDip = contoursUpDip + return + + + def getContours(self, spacingKm=10.0): + keys = [] + for k in self.contours.keys(): + if 0 == k % spacingKm: + keys.append(k) + contours = [self.contours[k] for k in sorted(keys)] + return contours + + + def getUpDipContours(self): + contoursUpDip = [self.contoursUpDip[k] for k in sorted(self.contoursUpDip.keys())] + return contoursUpDip + + + def getAllContours(self, spacingKm=10.0): + contours = self.getUpDipContours() + contours += self.getContours(spacingKm) + return contours + + + def _decimate(self, stride): + """Decimate the number of points in a contour. + """ + for key,points in self.contours.items(): + pointsD = points[::stride] + if (len(points)-1) % stride: + pointsD = numpy.vstack((pointsD, points[-1],)) + self.contours[key] = numpy.ascontiguousarray(pointsD) + return + + + def _toXYZ(self): + """Transform from geographic coordinates and depth in km to geographic + projected coordinate system. The coordinate system is imported + from coordsys.py. + + """ + import coordsys + for points in self.contours.values(): + coordsys.geoToMesh(points) + points[:,2] *= 1.0e+3 + return + # ---------------------------------------------------------------------- class ContourApp(object): @@ -136,38 +236,50 @@ def run(self): """Open Slab 1.0 input file and journal output file and loop over contours. """ - jfile = JournalFile(self.jfilename) - jfile.writeHeader() - sfile = SlabContoursFile(self.sfilename) sfile.read() - for contour in sfile.contours: - points = self._decimate(contour) - self._toXYZ(points) - jfile.writeContour(points) - jfile.writeTrailer() - jfile.close() - return + extender = ExtendSlab(sfile, self.pointsStride) + extender.addUpDipContours() + jfile = JournalFile(self.jfilename) + jfile.writeHeader() - def _decimate(self, points): - """Decimate the number of points in a contour. - """ - pointsD = numpy.array(points[::self.pointsStride], dtype=numpy.float64) - if (len(points)-1) % self.pointsStride: - pointsD = numpy.vstack((pointsD, numpy.array([points[-1]]),)) - return pointsD + # Top of slab + jfile.newSurface() + for contour in extender.getAllContours(): + jfile.addContour(contour) + jfile.skinSurface("surf_slabtop.sat") - def _toXYZ(self, points): - """Transform from geographic coordinates and depth in km to geographic - projected coordinate system. The coordinate system is imported - from coordsys.py. + # Bottom of slab + normalX = -0.209 + normalY = +0.016 + normalZ = -0.979 + slabThicknessKm = 50.0 + + jfile.newSurface() + for contour in extender.getUpDipContours(): + contour[:,2] = -slabThicknessKm*1.0e+3 + jfile.addContour(contour) + + for contour in extender.getContours(): + contour[:,0] += normalX*slabThicknessKm*1.0e+3 + contour[:,1] += normalY*slabThicknessKm*1.0e+3 + contour[:,2] += normalZ*slabThicknessKm*1.0e+3 + jfile.addContour(contour) + jfile.skinSurface("surf_slabbot.sat") - """ - import coordsys - coordsys.geoToMesh(points) - points[:,2] *= 1.0e+3 + # Splay fault + jfile.newSurface() + contour = extender.contours[15] + contour[:,2] -= 5.0e+3 + jfile.addContour(contour) + contour[:,2] = 1.0e+3 + contour[:,0] -= 15.0e+3 + jfile.addContour(contour) + jfile.skinSurface("surf_splay.sat") + + jfile.close() return @@ -179,8 +291,8 @@ def _toXYZ(self, points): "journal file that generates the surface from Slab 1.0." parser = argparse.ArgumentParser(description=DESCRIPTION) - parser.add_argument("--stride", action="store", dest="stride", type=int, default=5) - parser.add_argument("--journal-filename", action="store", dest="jfilename", default="contours.jou") + parser.add_argument("--stride", action="store", dest="stride", type=int, default=10) + parser.add_argument("--journal-filename", action="store", dest="jfilename", default="slabsurfs.jou") parser.add_argument("--slab-filename", action="store", dest="sfilename", default=None, required=True) args = parser.parse_args() diff --git a/examples/3d/subduction/mesh/geometry.jou b/examples/3d/subduction/mesh/geometry.jou index a21704b38c..b8065fd1b6 100644 --- a/examples/3d/subduction/mesh/geometry.jou +++ b/examples/3d/subduction/mesh/geometry.jou @@ -33,6 +33,22 @@ ${Units('si')} # ---------------------------------------------------------------------- reset +# ---------------------------------------------------------------------- +# Import slab surfaces and construct slab. +# ---------------------------------------------------------------------- +import Acis "surf_slabtop.sat" +${idSurf=Id("surface")} +surface {idSurf} name "s_slabtop" + +import Acis "surf_slabbot.sat" +${idSurf=Id("surface")} +surface {idSurf} name "s_slabbot" + +create volume loft surface s_slabtop s_slabbot +${idVol=Id("volume")} +volume {idVol} name "v_slab" +delete surface s_slabtop s_slabbot + # ---------------------------------------------------------------------- # Create block # ---------------------------------------------------------------------- @@ -43,45 +59,59 @@ ${blockHeight=400.0*km} brick x {blockLength} y {blockWidth} z {blockHeight} ${idVol=Id("volume")} +volume {idVol} name "v_domain" # Translate block so top is a z=0. ${moveX=-60.0*km} ${moveY=0.0*km} +volume v_domain move x {moveX} y {moveY} z {-0.5*blockHeight} -volume {idVol} move x {moveX} y {moveY} z {-0.5*blockHeight} +# ---------------------------------------------------------------------- +# Webcut block with slab. +# ---------------------------------------------------------------------- +chop volume v_domain with volume v_slab # ---------------------------------------------------------------------- -# Import subduction interface. +# Create planar surface for continental crust/mantle boundary. # ---------------------------------------------------------------------- -import Acis "slabtop_surf.sat" +create planar surface with plane zplane offset {-40.0*km} ${idSurf=Id("surface")} -surface {idSurf} name "s_slabtop" +surface {idSurf} name "s_moho" -# Slab bottom -${n_x=-0.209} -${n_y=+0.016} -${n_z=-0.979} -${slabThickness=50.0*km} -surface s_slabtop copy move x {n_x*slabThickness} y {n_y*slabThickness} z {n_z*slabThickness} +webcut volume v_domain@A with plane surface s_moho +delete surface s_moho -# ---------------------------------------------------------------------- -# Webcut block with topography and delete volume lying above topography. -# ---------------------------------------------------------------------- -webcut volume {idVol} with sheet surface 7 -delete volume 1 -delete body 2 -# ---------------------------------------------------------------------- -# Webcut remaining portion of block with subduction interface. -# ---------------------------------------------------------------------- -webcut volume 5 with sheet surface 8 -delete body 3 +# Create fault patch +${patchLength=200.0*km} +create planar surface with plane yplane offset {-0.5*patchLength} +${idSurf=Id("surface")} +surface {idSurf} name "s_southlimit" + +project curve 83 onto surface s_slabtop@B trim +split surface s_slabtop@B across location vertex 59 location vertex 60 + +create planar surface with plane yplane offset {+0.5*patchLength} +${idSurf=Id("surface")} +surface {idSurf} name "s_northlimit" + +project curve 93 onto surface s_slabtop@D trim +split surface s_slabtop@D across location vertex 67 location vertex 68 + +delete curve all # ---------------------------------------------------------------------- -# Webcut volume above subduction interface with splay fault. +# Import splay surface and cut volume. # ---------------------------------------------------------------------- -webcut volume 5 with sheet surface 9 -delete body 4 +import Acis "surf_splay.sat" +${idSurf=Id("surface")} +surface {idSurf} name "s_splay" + +webcut volume v_domain@A with sheet surface s_splay +delete surface s_splay + + + # ---------------------------------------------------------------------- # Imprint all volumes, then merge. @@ -91,3 +121,5 @@ merge all # End of file + + From 7554620bace25c4722c2686518875005a446a4e0 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 6 Jun 2017 20:45:43 -0700 Subject: [PATCH 003/216] Added missing file. --- examples/3d/subduction/mesh/coordsys.py | 71 +++++++++++++++++++++++++ 1 file changed, 71 insertions(+) create mode 100644 examples/3d/subduction/mesh/coordsys.py diff --git a/examples/3d/subduction/mesh/coordsys.py b/examples/3d/subduction/mesh/coordsys.py new file mode 100644 index 0000000000..fdcee78f03 --- /dev/null +++ b/examples/3d/subduction/mesh/coordsys.py @@ -0,0 +1,71 @@ +# Coordinate systems + +from spatialdata.geocoords.CSGeo import CSGeo +from spatialdata.geocoords.CSGeoProj import CSGeoProj + +# Geographic lat/lon coordinates in WGS84 datum +def cs_geo(): + """Geographic lat/lon coordinates in WGS84 datum. + """ + cs = CSGeo() + cs.inventory.datumHoriz = "WGS84" + cs.inventory.datumVert = "mean sea level" + cs.inventory.spaceDim = 2 + cs._configure() + cs.initialize() + return cs + + +def cs_geo3D(): + """Geographic lat/lon/elev coordinates in WGS84 datum with mean sea + level as vertical datum. + + """ + cs = CSGeo() + cs.inventory.datumHoriz = "WGS84" + cs.inventory.datumVert = "mean sea level" + cs.inventory.spaceDim = 3 + cs._configure() + cs.initialize() + return cs + + +def cs_mesh(): + """Cartesian coordinates for mesh with Portland as the origin and mean + sea level as vertical datum. + + """ + cs = CSGeoProj() + cs.inventory.datumHoriz = "WGS84" + cs.inventory.datumVert = "mean sea level" + cs.inventory.spaceDim = 3 + cs.inventory.projector.inventory.projection = "tmerc" + cs.inventory.projector.inventory.projOptions = "+lat_0=45.5231 +lon_0=-122.6765 +k=0.9996" + cs.inventory.projector._configure() + cs._configure() + cs.initialize() + return cs + + +def geoToMesh(xyz): + """Convert coordinates from geographic coordinates to mesh coordinates. + """ + from spatialdata.geocoords.Converter import convert + convert(xyz, cs_mesh(), cs_geo3D()) + return + + +def bbox_mesh(): + """ + """ + xdim = 2000.0e+3 + ydim = 2000.0e+3 + xoffset = 0.0e+3 + yoffset = 0.0e+3 + + bbox = (xoffset-0.5*xdim, yoffset-0.5*ydim, + xoffset+0.5*xdim, yoffset+0.5*ydim) + return bbox + + +# End of file From 8a8796a7247f426fe522de8902c12124f1716e68 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 6 Jun 2017 21:24:34 -0700 Subject: [PATCH 004/216] Improve geometry construction. --- ...erate_slabsurfs.py => generate_surfjou.py} | 0 examples/3d/subduction/mesh/geometry.jou | 33 ++++++++----------- 2 files changed, 14 insertions(+), 19 deletions(-) rename examples/3d/subduction/mesh/{generate_slabsurfs.py => generate_surfjou.py} (100%) diff --git a/examples/3d/subduction/mesh/generate_slabsurfs.py b/examples/3d/subduction/mesh/generate_surfjou.py similarity index 100% rename from examples/3d/subduction/mesh/generate_slabsurfs.py rename to examples/3d/subduction/mesh/generate_surfjou.py diff --git a/examples/3d/subduction/mesh/geometry.jou b/examples/3d/subduction/mesh/geometry.jou index b8065fd1b6..9350b03d47 100644 --- a/examples/3d/subduction/mesh/geometry.jou +++ b/examples/3d/subduction/mesh/geometry.jou @@ -39,15 +39,18 @@ reset import Acis "surf_slabtop.sat" ${idSurf=Id("surface")} surface {idSurf} name "s_slabtop" +${idVol=Id("volume")} +volume {idVol} name "v_slabtop" import Acis "surf_slabbot.sat" ${idSurf=Id("surface")} surface {idSurf} name "s_slabbot" +${idVol=Id("volume")} +volume {idVol} name "v_slabbot" create volume loft surface s_slabtop s_slabbot ${idVol=Id("volume")} volume {idVol} name "v_slab" -delete surface s_slabtop s_slabbot # ---------------------------------------------------------------------- # Create block @@ -81,24 +84,18 @@ surface {idSurf} name "s_moho" webcut volume v_domain@A with plane surface s_moho delete surface s_moho - +# ---------------------------------------------------------------------- # Create fault patch +# ---------------------------------------------------------------------- ${patchLength=200.0*km} -create planar surface with plane yplane offset {-0.5*patchLength} -${idSurf=Id("surface")} -surface {idSurf} name "s_southlimit" - -project curve 83 onto surface s_slabtop@B trim -split surface s_slabtop@B across location vertex 59 location vertex 60 - -create planar surface with plane yplane offset {+0.5*patchLength} -${idSurf=Id("surface")} -surface {idSurf} name "s_northlimit" - -project curve 93 onto surface s_slabtop@D trim -split surface s_slabtop@D across location vertex 67 location vertex 68 +brick x {400.0*km} y {patchLength} z {100.0*km} +${idVol=Id("volume")} +volume {idVol} name "v_patchblock" +move volume v_patchblock x {-100*km} y 0 z 0 -delete curve all +chop volume v_slabtop with volume v_patchblock +imprint volume v_domain@A with volume v_slabtop +delete volume v_slabtop v_slabtop@A v_slabbot # ---------------------------------------------------------------------- # Import splay surface and cut volume. @@ -110,9 +107,6 @@ surface {idSurf} name "s_splay" webcut volume v_domain@A with sheet surface s_splay delete surface s_splay - - - # ---------------------------------------------------------------------- # Imprint all volumes, then merge. # ---------------------------------------------------------------------- @@ -123,3 +117,4 @@ merge all + From ea95688f808ade1699f022979b5c244d515b320d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 7 Jun 2017 17:10:27 -0700 Subject: [PATCH 005/216] Started converting surface generation script to Pyre. --- .../3d/subduction/mesh/generate_surfjou.py | 219 ++++++++++++------ 1 file changed, 144 insertions(+), 75 deletions(-) diff --git a/examples/3d/subduction/mesh/generate_surfjou.py b/examples/3d/subduction/mesh/generate_surfjou.py index b98d33a30c..3894fa354b 100755 --- a/examples/3d/subduction/mesh/generate_surfjou.py +++ b/examples/3d/subduction/mesh/generate_surfjou.py @@ -1,4 +1,4 @@ -#!/usr/bin/env python +#!/usr/bin/env nemesis # # ---------------------------------------------------------------------- # @@ -31,24 +31,38 @@ # three-dimensional model of global subduction zone geometries, # J. Geophys. Res., 117, B01302, doi:10.1029/2011JB008524. +# ---------------------------------------------------------------------- +from pyre.applications.Script import Script as Application +from pyre.components.Component import Component +import pyre.inventory + import numpy -from collections import OrderedDict # ---------------------------------------------------------------------- -class JournalFile(object): +class JournalFile(Component): """JournalFile object for writing CUBIT/Trelis journal file. """ + + class Inventory(Component.Inventory): + """Pyre properties and facilities for JournalFile. + """ + filename = pyre.inventory.str("filename", default="geometry_surfs.jou") + filename.meta["tip"] = "Name of generated CUBIT/Trelis journal file." + - def __init__(self, filename): + def __init__(self, name="journalfile"): """Constructor. """ - self.file = open(filename, "w") + Component.__init__(self, name=name, facility="journalfile") + self.file = None return def writeHeader(self): """Write header for journal file. """ + if not self.file: + self.file = open(self.filename, "w") self.file.write("# CUBIT/Trelis journal file generated by generate_slabsurfs.py\n" \ "#\n" \ "# Create ACIS NURBS surfaces for top and bottom of slab.\n\n") @@ -93,49 +107,92 @@ def close(self): # ---------------------------------------------------------------------- -class SlabContoursFile(object): +class SlabContoursFile(Component): """SlabContourFile object for reading contours from a Slab 1.0 contour file.. """ - def __init__(self, filename): - self.filename = filename + class Inventory(Component.Inventory): + """Pyre properties and facilities for SlabContourFile. + """ + filename = pyre.inventory.str("filename", default="cas_contours_dep.in.txt.gz") + filename.meta["tip"] = "Name of ASCII file with slab contours." + + + def __init__(self, name="slabcontourfile"): + Component.__init__(self, name=name, facility="slabcontourfile") return - + def read(self): """Read contours from Slab 1.0 file. """ - with open(self.filename, "r") as file: - lines = file.readlines() - contours = {} - points = [] - key = None - for line in lines: - if line.strip() == "END": - contours[key] = numpy.array(points, dtype=numpy.float64) - points = [] - continue - if len(line.split()) == 1: - key = int(line) - continue - pt = map(float, line.strip().split()) - points.append(pt) + + if self.filename.endswith(".gz"): + import gzip + with gzip.open(self.filename, "rb") as file: + lines = file.readlines() + else: + with open(self.filename, "r") as file: + lines = file.readlines() + + contours = {} + points = [] + key = None + for line in lines: + if line.strip() == "END": + contours[key] = numpy.array(points, dtype=numpy.float64) + points = [] + continue + if len(line.split()) == 1: + key = int(line) + continue + pt = map(float, line.strip().split()) + points.append(pt) self.contours = contours return # ---------------------------------------------------------------------- -class ExtendSlab(object): +class SlabExtender(Component): + + class Inventory(Component.Inventory): + """Pyre properties and facilities for SlabExtender. + """ + from pyre.units.length import km + from pyre.units.angle import deg + + upDipElev = pyre.inventory.dimensional("up_dip_elev", default=1,0*km) + upDipElev.meta["tip"] = "Elevation of contours extended in up-dip direction." + + upDipDist = pyre.inventory.dimensional("up_dip_dist", default=600,0*km) + upDipDist.meta["tip"] = "Distance to extend contours in up-dip direction." + + upDipAngle = pyre.inventory.dimensional("up_dip_angle", default=10.0*deg) + upDipAngle.meta["tip"] = "Distance to extend contours in up-dip direction." + + faultStrike = pyre.inventory.dimensional("fault_strike", default=0.0*deg) + faultString.meta["tip"] = "Approximate strike of fault." - def __init__(self, slab, stride): + contourStride = pyre.inventory.int("contour_stride", default=4) + contourStride.meta["tip"] = "Stride to use in decimating number of contours." + + pointsStride = pyre.inventory.int("points_stride", default=20) + pointsStride.meta["tip"] = "Stride to use in decimating number of points in a contour." + + + def __init__(self, name="slabextender"): """Constructor. """ + Component.__init__(self, name=name, facility="slabextender") + return + + + def initialize(self, slab): self.contours = slab.contours self._decimate(stride) self._toXYZ() - return + - def addUpDipContours(self, elevKm=1.0, strikeDeg=0.0, dipDeg=10.0, extendDistKm=600.0): """Add contours up-dip from original contours. @@ -219,37 +276,62 @@ def _toXYZ(self): # ---------------------------------------------------------------------- -class ContourApp(object): - """ContourApp object for top-level application workflow. +class SurfaceApp(Application): + """SurfaceApp object for top-level application workflow. """ + + class Inventory(Component.Inventory): + """Pyre properties and facilities for SurfaceApp. + """ + from pyre.units.length import km + from pyre.units.angle import deg + + modeler = pyre.inventory.facility("cubit", factory=JournalFile) + modeler.meta["tip"] = "Surface modeler for slab." + + contours = pyre.inventory.facility("slab", factory=SlabContoursFile) + contours.meta["tip"] = "Slab contours." + + extender = pyre.inventory.facility("extender", factory=SlabExtender) + extender.meta["tip"] = "Extender for slab." + + slabTopFilename = pyre.inventory.str("slab_top_filename", default="surf_slabtop.sat") + slabTopFilename.meta["tip"] = "Name of ACIS file with slab top surface." + + slabBotFilename = pyre.inventory.str("slab_bot_filename", default="surf_slabbot.sat") + slabBotFilename.meta["tip"] = "Name of ACIS file with slab bottom surface." + + splayFilename = pyre.inventory.str("splay_filename", default="surf_splay.sat") + splayFilename.meta["tip"] = "Name of ACIS file with splay fault surface." + + slabNormalDir = pyre.inventory.list("slab_normal_dir", default=[0,0,1]) + slabNormalDir.meta["tip"] = "Approximate average upward normal direction for slab." + - def __init__(self): + def __init__(self, name="surfaceapp"): """Constructor. """ - self.sfilename = None - self.jfilename = None - self.pointsStride = 1 + Application.__init__(self, name) return - def run(self): + def main(self): """Open Slab 1.0 input file and journal output file and loop over contours. """ - sfile = SlabContoursFile(self.sfilename) - sfile.read() + + self.contours.read() - extender = ExtendSlab(sfile, self.pointsStride) - extender.addUpDipContours() + self.extender.initialize(self.contours) + self.extender.addUpDipContours() - jfile = JournalFile(self.jfilename) - jfile.writeHeader() + self.modeler.writeHeader() # Top of slab - jfile.newSurface() - for contour in extender.getAllContours(): - jfile.addContour(contour) - jfile.skinSurface("surf_slabtop.sat") + self.modeler.newSurface() + for contour in self.extender.getAllContours(): + self.modeler.addContour(contour) + self.modeler.skinSurface("surf_slabtop.sat") # Bottom of slab normalX = -0.209 @@ -257,50 +339,37 @@ def run(self): normalZ = -0.979 slabThicknessKm = 50.0 - jfile.newSurface() - for contour in extender.getUpDipContours(): + self.modeler.newSurface() + for contour in self.extender.getUpDipContours(): contour[:,2] = -slabThicknessKm*1.0e+3 - jfile.addContour(contour) + self.modeler.addContour(contour) - for contour in extender.getContours(): - contour[:,0] += normalX*slabThicknessKm*1.0e+3 - contour[:,1] += normalY*slabThicknessKm*1.0e+3 - contour[:,2] += normalZ*slabThicknessKm*1.0e+3 - jfile.addContour(contour) - jfile.skinSurface("surf_slabbot.sat") + for contour in self.extender.getContours(): + contour[:,0] += slabNormalDir[0]*slabThicknessKm*1.0e+3 + contour[:,1] += slabNormalDir[1]*slabThicknessKm*1.0e+3 + contour[:,2] += slabNormalDir[2]*slabThicknessKm*1.0e+3 + self.modeler.addContour(contour) + self.modeler.skinSurface("surf_slabbot.sat") # Splay fault - jfile.newSurface() + self.modeler.newSurface() contour = extender.contours[15] contour[:,2] -= 5.0e+3 - jfile.addContour(contour) + self.modeler.addContour(contour) contour[:,2] = 1.0e+3 contour[:,0] -= 15.0e+3 - jfile.addContour(contour) - jfile.skinSurface("surf_splay.sat") + self.modeler.addContour(contour) + self.modeler.skinSurface("surf_splay.sat") - jfile.close() + self.modeler.close() return # ====================================================================== if __name__ == "__main__": - import argparse - - DESCRIPTION = "Python script to create a CUBIT/Trelis "\ - "journal file that generates the surface from Slab 1.0." - - parser = argparse.ArgumentParser(description=DESCRIPTION) - parser.add_argument("--stride", action="store", dest="stride", type=int, default=10) - parser.add_argument("--journal-filename", action="store", dest="jfilename", default="slabsurfs.jou") - parser.add_argument("--slab-filename", action="store", dest="sfilename", default=None, required=True) - args = parser.parse_args() - - app = ContourApp() - app.sfilename = args.sfilename - app.jfilename = args.jfilename - app.pointsStride = args.stride - app.run() + + from pyre.applications import start + start(applicationClass=SurfaceApp) # End of file From 680c372a8b69276397a14674012285f4d7a53048 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 8 Jun 2017 10:22:55 -0700 Subject: [PATCH 006/216] Finished conversion to Pyre. --- .../3d/subduction/mesh/generate_surfjou.py | 131 +++++++++++------- 1 file changed, 83 insertions(+), 48 deletions(-) diff --git a/examples/3d/subduction/mesh/generate_surfjou.py b/examples/3d/subduction/mesh/generate_surfjou.py index 3894fa354b..fae7069721 100755 --- a/examples/3d/subduction/mesh/generate_surfjou.py +++ b/examples/3d/subduction/mesh/generate_surfjou.py @@ -105,6 +105,12 @@ def close(self): self.file = None return + + def _configure(self): + Component._configure(self) + self.filename = self.inventory.filename + return + # ---------------------------------------------------------------------- class SlabContoursFile(Component): @@ -126,7 +132,6 @@ def __init__(self, name="slabcontourfile"): def read(self): """Read contours from Slab 1.0 file. """ - if self.filename.endswith(".gz"): import gzip with gzip.open(self.filename, "rb") as file: @@ -152,6 +157,12 @@ def read(self): return + def _configure(self): + Component._configure(self) + self.filename = self.inventory.filename + return + + # ---------------------------------------------------------------------- class SlabExtender(Component): @@ -161,25 +172,36 @@ class Inventory(Component.Inventory): from pyre.units.length import km from pyre.units.angle import deg - upDipElev = pyre.inventory.dimensional("up_dip_elev", default=1,0*km) + upDipElev = pyre.inventory.dimensional("up_dip_elev", default=1.0*km) upDipElev.meta["tip"] = "Elevation of contours extended in up-dip direction." - upDipDist = pyre.inventory.dimensional("up_dip_dist", default=600,0*km) + upDipDist = pyre.inventory.dimensional("up_dip_dist", default=600.0*km) upDipDist.meta["tip"] = "Distance to extend contours in up-dip direction." upDipAngle = pyre.inventory.dimensional("up_dip_angle", default=10.0*deg) upDipAngle.meta["tip"] = "Distance to extend contours in up-dip direction." faultStrike = pyre.inventory.dimensional("fault_strike", default=0.0*deg) - faultString.meta["tip"] = "Approximate strike of fault." + faultStrike.meta["tip"] = "Approximate strike of fault." - contourStride = pyre.inventory.int("contour_stride", default=4) - contourStride.meta["tip"] = "Stride to use in decimating number of contours." + contoursStride = pyre.inventory.int("contour_stride", default=4) + contoursStride.meta["tip"] = "Stride to use in decimating number of contours." pointsStride = pyre.inventory.int("points_stride", default=20) pointsStride.meta["tip"] = "Stride to use in decimating number of points in a contour." + def _configure(self): + Component._configure(self) + self.upDipElev = self.inventory.upDipElev + self.upDipDist = self.inventory.upDipDist + self.upDipAngle = self.inventory.upDipAngle + self.faultStrike = self.inventory.faultStrike + self.contoursStride = self.inventory.contoursStride + self.pointsStride = self.inventory.pointsStride + return + + def __init__(self, name="slabextender"): """Constructor. """ @@ -189,18 +211,12 @@ def __init__(self, name="slabextender"): def initialize(self, slab): self.contours = slab.contours - self._decimate(stride) + self._decimate(self.pointsStride) self._toXYZ() - def addUpDipContours(self, elevKm=1.0, strikeDeg=0.0, dipDeg=10.0, extendDistKm=600.0): + def addUpDipContours(self): """Add contours up-dip from original contours. - - Keyword arguments: - elevKm -- Elevation in kilometers of additional contours. - strikeDeg -- Approximate strike of fault in degrees (default 0.0). - dipDeg -- Dip angle in degrees at up-dip edge of fault (default 10.0). - extendDistKm -- Distance in kilometers to extend slab surface in up-dip direction. We increase the horizontal distance between the contours at a geometric rate. The first contour is at a distance of @@ -211,43 +227,50 @@ def addUpDipContours(self, elevKm=1.0, strikeDeg=0.0, dipDeg=10.0, extendDistKm= """ import math + from pyre.units.length import m + key = min(self.contours.keys()) contourTop = self.contours[key] - zTop = contourTop[0][2] + zTop = contourTop[0][2]*m - distHoriz = (elevKm*1.0e+3-zTop)/math.tan(dipDeg*math.pi/180.0) - dx = -distHoriz*math.cos(strikeDeg*math.pi/180.0) - dy = distHoriz*math.sin(strikeDeg*math.pi/180.0) + distHoriz = (self.upDipElev - zTop) / math.tan(self.upDipAngle) + dx = -distHoriz * math.cos(self.faultStrike) + dy = distHoriz * math.sin(self.faultStrike) contoursUpDip = {} - numContours = int(math.ceil(math.log((extendDistKm*1.0e+3/distHoriz)+1)/math.log(2.0))) + numContours = int(math.ceil(math.log((self.upDipDist/distHoriz)+1)/math.log(2.0))) for i in xrange(numContours): contour = numpy.array(contourTop) - contour[:,0] += (2**i)*dx - contour[:,1] += (2**i)*dy - contour[:,2] = elevKm*1.0e+3 + contour[:,0] += (2**i)*dx.value + contour[:,1] += (2**i)*dy.value + contour[:,2] = self.upDipElev.value contoursUpDip[-i] = contour self.contoursUpDip = contoursUpDip return - def getContours(self, spacingKm=10.0): - keys = [] - for k in self.contours.keys(): - if 0 == k % spacingKm: - keys.append(k) - contours = [self.contours[k] for k in sorted(keys)] - return contours + def getContours(self): + """Get contours for slab surface. + """ + contours = [self.contours[k] for k in sorted(self.contours.keys())] + contoursD = contours[::self.contoursStride] + if (len(contours)-1) % self.contoursStride: + contoursD += [contours[-1]] + return contoursD def getUpDipContours(self): + """Get contours for up-dip extension of slab surface. + """ contoursUpDip = [self.contoursUpDip[k] for k in sorted(self.contoursUpDip.keys())] return contoursUpDip - def getAllContours(self, spacingKm=10.0): + def getAllContours(self): + """Get all contours for slab surface. + """ contours = self.getUpDipContours() - contours += self.getContours(spacingKm) + contours += self.getContours() return contours @@ -255,8 +278,8 @@ def _decimate(self, stride): """Decimate the number of points in a contour. """ for key,points in self.contours.items(): - pointsD = points[::stride] - if (len(points)-1) % stride: + pointsD = points[::self.pointsStride] + if (len(points)-1) % self.pointsStride: pointsD = numpy.vstack((pointsD, points[-1],)) self.contours[key] = numpy.ascontiguousarray(pointsD) return @@ -280,7 +303,7 @@ class SurfaceApp(Application): """SurfaceApp object for top-level application workflow. """ - class Inventory(Component.Inventory): + class Inventory(Application.Inventory): """Pyre properties and facilities for SurfaceApp. """ from pyre.units.length import km @@ -304,7 +327,10 @@ class Inventory(Component.Inventory): splayFilename = pyre.inventory.str("splay_filename", default="surf_splay.sat") splayFilename.meta["tip"] = "Name of ACIS file with splay fault surface." - slabNormalDir = pyre.inventory.list("slab_normal_dir", default=[0,0,1]) + slabThickness = pyre.inventory.dimensional("slab_thickness", default=50.0*km) + slabThickness.meta["tip"] = "Thickness of slab." + + slabNormalDir = pyre.inventory.list("slab_normal_dir", default=[+0.209, -0.016, +0.979]) slabNormalDir.meta["tip"] = "Approximate average upward normal direction for slab." @@ -315,11 +341,10 @@ def __init__(self, name="surfaceapp"): return - def main(self): + def main(self, *args, **kwds): """Open Slab 1.0 input file and journal output file and loop over contours. """ - self.contours.read() self.extender.initialize(self.contours) @@ -331,40 +356,50 @@ def main(self): self.modeler.newSurface() for contour in self.extender.getAllContours(): self.modeler.addContour(contour) - self.modeler.skinSurface("surf_slabtop.sat") + self.modeler.skinSurface(self.slabTopFilename) # Bottom of slab normalX = -0.209 normalY = +0.016 normalZ = -0.979 - slabThicknessKm = 50.0 self.modeler.newSurface() for contour in self.extender.getUpDipContours(): - contour[:,2] = -slabThicknessKm*1.0e+3 + contour[:,2] = -self.slabThickness.value self.modeler.addContour(contour) for contour in self.extender.getContours(): - contour[:,0] += slabNormalDir[0]*slabThicknessKm*1.0e+3 - contour[:,1] += slabNormalDir[1]*slabThicknessKm*1.0e+3 - contour[:,2] += slabNormalDir[2]*slabThicknessKm*1.0e+3 + contour[:,0] -= self.slabNormalDir[0]*self.slabThickness.value + contour[:,1] -= self.slabNormalDir[1]*self.slabThickness.value + contour[:,2] -= self.slabNormalDir[2]*self.slabThickness.value self.modeler.addContour(contour) - self.modeler.skinSurface("surf_slabbot.sat") + self.modeler.skinSurface(self.slabBotFilename) # Splay fault self.modeler.newSurface() - contour = extender.contours[15] - contour[:,2] -= 5.0e+3 + contour = self.extender.contours[15] + contour[:,2] -= 8.0e+3 self.modeler.addContour(contour) contour[:,2] = 1.0e+3 - contour[:,0] -= 15.0e+3 + contour[:,0] -= 24.0e+3 self.modeler.addContour(contour) - self.modeler.skinSurface("surf_splay.sat") + self.modeler.skinSurface(self.splayFilename) self.modeler.close() return + def _configure(self): + Application._configure(self) + self.modeler = self.inventory.modeler + self.contours = self.inventory.contours + self.extender = self.inventory.extender + self.slabTopFilename = self.inventory.slabTopFilename + self.slabBotFilename = self.inventory.slabBotFilename + self.splayFilename = self.inventory.splayFilename + self.slabThickness = self.inventory.slabThickness + self.slabNormalDir = self.inventory.slabNormalDir + # ====================================================================== if __name__ == "__main__": From 9b7417a56b2da75e3d9895fdfd349f596efe4fda Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 8 Jun 2017 10:23:22 -0700 Subject: [PATCH 007/216] Fixed some small issues with geometry construction. --- examples/3d/subduction/mesh/geometry.jou | 50 +++++++++++++++++------- 1 file changed, 36 insertions(+), 14 deletions(-) diff --git a/examples/3d/subduction/mesh/geometry.jou b/examples/3d/subduction/mesh/geometry.jou index 9350b03d47..d4f9e236d2 100644 --- a/examples/3d/subduction/mesh/geometry.jou +++ b/examples/3d/subduction/mesh/geometry.jou @@ -14,13 +14,15 @@ # # ---------------------------------------------------------------------- # -# CUBIT journal file with geometry for example showing how to import +# This file is called from the mesh file (mesh_tet.jou or mesh_hex.jou). +# +# CUBIT/Trelis journal file with geometry for example showing how to import # several surfaces (topography, subduction interface, splay fault), and # mesh the resulting volumes. # -# We also use the CUBIT support for APREPRO (the expressions in +# We also use the CUBIT/Trelis support for APREPRO (the expressions in # braces), which includes units and mathematical functions. See the -# APREPRO section in the appendix of the CUBIT documentation for more +# APREPRO section in the appendix of the CUBIT/Trelis documentation for more # information. # # ---------------------------------------------------------------------- @@ -41,17 +43,23 @@ ${idSurf=Id("surface")} surface {idSurf} name "s_slabtop" ${idVol=Id("volume")} volume {idVol} name "v_slabtop" +${idBody=Id("body")} +body {idBody} name "b_slabtop" import Acis "surf_slabbot.sat" ${idSurf=Id("surface")} surface {idSurf} name "s_slabbot" ${idVol=Id("volume")} volume {idVol} name "v_slabbot" +${idBody=Id("body")} +body {idBody} name "b_slabbot" create volume loft surface s_slabtop s_slabbot ${idVol=Id("volume")} volume {idVol} name "v_slab" +delete body b_slabbot + # ---------------------------------------------------------------------- # Create block # ---------------------------------------------------------------------- @@ -84,28 +92,41 @@ surface {idSurf} name "s_moho" webcut volume v_domain@A with plane surface s_moho delete surface s_moho +# ---------------------------------------------------------------------- +# Import splay surface and cut volume. +# ---------------------------------------------------------------------- +import Acis "surf_splay.sat" +${idSurf=Id("surface")} +surface {idSurf} name "s_splay" +${idVol=Id("volume")} +volume {idVol} name "v_splay" +${idBody=Id("body")} +body {idBody} name "b_splay" + +webcut volume v_domain@A with sheet surface s_splay + # ---------------------------------------------------------------------- # Create fault patch # ---------------------------------------------------------------------- +# Create block to create rupture patch. ${patchLength=200.0*km} brick x {400.0*km} y {patchLength} z {100.0*km} ${idVol=Id("volume")} volume {idVol} name "v_patchblock" move volume v_patchblock x {-100*km} y 0 z 0 -chop volume v_slabtop with volume v_patchblock -imprint volume v_domain@A with volume v_slabtop -delete volume v_slabtop v_slabtop@A v_slabbot +# Scribe rupture patch onto surface geometry (volumes of sheet bodies). +chop volume v_slabtop with volume v_patchblock keep +chop volume v_splay with volume v_patchblock -# ---------------------------------------------------------------------- -# Import splay surface and cut volume. -# ---------------------------------------------------------------------- -import Acis "surf_splay.sat" -${idSurf=Id("surface")} -surface {idSurf} name "s_splay" +# Imprint rupture patch from sheet bodies onto domain volumes. +imprint volume v_domain@A with volume v_slabtop@A +imprint volume v_domain@C with volume v_slabtop@A +imprint volume v_domain@A with volume v_splay -webcut volume v_domain@A with sheet surface s_splay -delete surface s_splay +# Remove sheet body volumes. +delete body b_slabtop b_slabtop@A b_slabtop@B +delete body b_splay b_splay@A # ---------------------------------------------------------------------- # Imprint all volumes, then merge. @@ -118,3 +139,4 @@ merge all + From 275e0cadcb905850473303574662c530dd653bc4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 8 Jun 2017 10:23:47 -0700 Subject: [PATCH 008/216] Started work on tet mesh script. --- examples/3d/subduction/mesh/mesh_tet.jou | 33 ++++++++++++++++++++++++ 1 file changed, 33 insertions(+) create mode 100644 examples/3d/subduction/mesh/mesh_tet.jou diff --git a/examples/3d/subduction/mesh/mesh_tet.jou b/examples/3d/subduction/mesh/mesh_tet.jou new file mode 100644 index 0000000000..eb877c8091 --- /dev/null +++ b/examples/3d/subduction/mesh/mesh_tet.jou @@ -0,0 +1,33 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# CUBIT/Trelis journal file for generating a tet mesh of the subduction zone. + +# ---------------------------------------------------------------------- +# Generate geometry +# ---------------------------------------------------------------------- +playback 'geometry.jou' + +volume all scheme tetmesh +volume all size {25.0*km} + +mesh volume all + + + + + +# End of file From 4ce7447c883035eac78772dff0c69a1cc121abd4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 8 Jun 2017 10:24:01 -0700 Subject: [PATCH 009/216] Create journal file for boundary conditions. --- examples/3d/subduction/mesh/bc.jou | 187 +++++++++++++++++++++++++++++ 1 file changed, 187 insertions(+) create mode 100644 examples/3d/subduction/mesh/bc.jou diff --git a/examples/3d/subduction/mesh/bc.jou b/examples/3d/subduction/mesh/bc.jou new file mode 100644 index 0000000000..d16cd80452 --- /dev/null +++ b/examples/3d/subduction/mesh/bc.jou @@ -0,0 +1,187 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# This file is called from the mesh file (mesh_tet.jou or mesh_hex.jou). +# +# CUBIT/Trelis journal file for setting blocks and nodesets for the meshes +# created by mesh_tet.jou and mesh_hex.jou. +# + +# ---------------------------------------------------------------------- +# Create blocks for materials +# ---------------------------------------------------------------------- +block 1 volume v_domain +block 1 name "slab" + +block 2 volume v_domain@A +block 2 name "wedge" + +block 3 volume v_domain@B +block 3 name "mantle" + +block 4 volume v_domain@C +block 4 name "crust" + +# ---------------------------------------------------------------------- +# Create nodesets for faults and boundary conditions. +# ---------------------------------------------------------------------- + +# ---------------------------------------------------------------------- +# FAULT INTERFACES +# ---------------------------------------------------------------------- + +# Entire top of slab +group "fault_slabtop" add node in s_slabtop@A +group "fault_slabtop" add node in s_slabtop@B +group "fault_slabtop" add node in s_slabtop@C +group "fault_slabtop" add node in s_slabtop@D +group "fault_slabtop" add node in s_slabtop@E +group "fault_slabtop" add node in s_slabtop@G +group "fault_slabtop" add node in s_slabtop@H +nodeset 10 group fault_slabtop +nodeset 10 name "fault_slabtop" + +# Buried edge for top of slab. +group "fault_slabtop_edge" add node in curve 38 +nodeset 11 group fault_slabtop_edge +nodeset 11 name "fault_slabtop_edge" + + +# Entire bottom of slab +group "fault_slabbot" add node in s_slabbot@A +nodeset 20 group fault_slabtop +nodeset 20 name "fault_slabtop" + +# Buried edge for bottom of slab. +group "fault_slabbot_edge" add node in curve 36 +nodeset 21 group fault_slabbot_edge +nodeset 21 name "fault_slabbot_edge" + + +# Entire splay fault +group "fault_splay" add node in s_splay@A +group "fault_splay" add node in s_splay@C +group "fault_splay" add node in s_splay@D +nodeset 30 group fault_splay +nodeset 30 name "fault_splay" + +# Buried edge for splay fault. +group "fault_splay_edge" add node in curve 138 +group "fault_splay_edge" add node in curve 141 +group "fault_splay_edge" add node in curve 142 +nodeset 31 group fault_splay_edge +nodeset 31 name "fault_splay_edge" + + +# Top of slab rupture patch. +group "fault_slabtop_patch" add node in s_slabtop@E +group "fault_slabtop_patch" add node in s_slabtop@H +nodeset 40 group fault_slabtop_patch +nodeset 40 name "fault_slabtop_patch" + +# Buried edge for top of slab rupture patch. +group "fault_slabtop_patch_edge" add node in curve 136 +group "fault_slabtop_patch_edge" add node in curve 155 +group "fault_slabtop_patch_edge" add node in curve 156 +group "fault_slabtop_patch_edge" add node in curve 152 +group "fault_slabtop_patch_edge" add node in curve 139 +nodeset 41 group fault_slabtop_patch_edge +nodeset 41 name "fault_slabtop_patch_edge" + + +# Splay fault rupture patch. +group "fault_splay_patch" add node in s_splay@C +nodeset 50 group fault_splay_patch +nodeset 50 name "fault_splay_patch" + +# Buried edge for top of slab rupture patch. +group "fault_splay_patch_edge" add node in curve 165 +group "fault_splay_patch_edge" add node in curve 141 +group "fault_splay_patch_edge" add node in curve 167 +nodeset 51 group fault_splay_patch_edge +nodeset 51 name "fault_splay_patch_edge" + +# ---------------------------------------------------------------------- +# BOUNDARIES +# ---------------------------------------------------------------------- + +# +x +group "boundary_xpos" add node in surface 33 +group "boundary_xpos" add node in surface 37 +nodeset 80 group boundary_xpos +nodeset 80 name "boundary_xpos" + +# -x +group "boundary_xneg" add node in surface 20 +group "boundary_xneg" add node in surface 28 +nodeset 80 group boundary_xneg +nodeset 80 name "boundary_xneg" + +# -x w/o fault +group "boundary_xneg_nofault" add node in group boundary_xneg +group "boundary_xneg_nofault" remove node in group fault_slabbot +nodeset 81 group boundary_xneg_nofault +nodeset 81 name "boundary_xneg_nofault" + + +# +y +group "boundary_ypos" add node in surface 18 +group "boundary_ypos" add node in surface 45 +group "boundary_ypos" add node in surface 48 +group "boundary_ypos" add node in surface 39 +nodeset 82 group boundary_ypos +nodeset 82 name "boundary_ypos" + +# +y w/o fault +group "boundary_ypos_nofault" add node in group boundary_ypos +group "boundary_ypos_nofault" remove node in group fault_slabtop +group "boundary_ypos_nofault" remove node in group fault_slabbot +group "boundary_ypos_nofault" remove node in group fault_splay +nodeset 83 group boundary_ypos_nofault +nodeset 83 name "boundary_ypos_nofault" + + +# -y +group "boundary_yneg" add node in surface 21 +group "boundary_yneg" add node in surface 43 +group "boundary_yneg" add node in surface 50 +group "boundary_yneg" add node in surface 36 +nodeset 84 group boundary_yneg +nodeset 84 name "boundary_yneg" + +# -y w/o fault +group "boundary_yneg_nofault" add node in group boundary_yneg +group "boundary_yneg_nofault" remove node in group fault_slabtop +group "boundary_yneg_nofault" remove node in group fault_slabbot +group "boundary_yneg_nofault" remove node in group fault_splay +nodeset 85 group boundary_yneg_nofault +nodeset 85 name "boundary_yneg_nofault" + +# -z +group "boundary_zneg" add node in surface 10 +nodeset 86 group boundary_zneg +nodeset 86 name "boundary_zneg" + +# +z +group "boundary_zpos" add node in surface 47 +group "boundary_zpos" add node in surface 42 +group "boundary_zpos" add node in surface 19 +nodeset 86 group boundary_zpos +nodeset 86 name "boundary_zpos" + + +# End of file + From 37bc3cb750b0a323069f6b1700f963dc746b2588 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 8 Jun 2017 13:31:00 -0700 Subject: [PATCH 010/216] Setup tet and hex uniform resolution meshes and started work on example sims. --- examples/3d/subduction/README | 76 ++++++++++++++ examples/3d/subduction/mesh/mesh_hex.jou | 54 ++++++++++ examples/3d/subduction/mesh/mesh_tet.jou | 11 ++- examples/3d/subduction/pylithapp.cfg | 121 +++++++++++++++++++++++ examples/3d/subduction/step01.cfg | 118 ++++++++++++++++++++++ 5 files changed, 379 insertions(+), 1 deletion(-) create mode 100644 examples/3d/subduction/README create mode 100644 examples/3d/subduction/mesh/mesh_hex.jou create mode 100644 examples/3d/subduction/pylithapp.cfg create mode 100644 examples/3d/subduction/step01.cfg diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README new file mode 100644 index 0000000000..a6dea18281 --- /dev/null +++ b/examples/3d/subduction/README @@ -0,0 +1,76 @@ +Features: + + Spatial databases + + SimpleDB + + UniformDB + + SimpleGridDB + + CompositeDB + + - Geographic coordinates with SimpleGridDB + - Depth profile with SimpleGridDB + + Dirichlet Boundary conditions + + Fixed displacement + + Fixed velocity + + Time history + + Materials + + Elastic + + Linear Maxwell viscoelastic + + Powerlaw [exercise] + + Preconditioners + + LU + + AMG (ML) + + AMG (ML) + custom preconditioner + + Uniform refinement [exercise] + + Output + + Output of solution + + Output of solution on ground surface + + Output of solution at points + + Output of state variables + + + HDF5 + + Visualization with ParaView Python scripts + + Generation of spatial databases via Python + + Faults + + Buried edges + + Intersecting + + Multiple faults + + Prescribed slip + + Prescribed slip w/multiple ruptures + + Fault friction + +Step01: Compression [tutorial] + UniformDB for material properties + +Step02: Coseismic [exercise] + Prescribed slip on fault patch with viscoelastic relaxation + Viscosity via CompositeDB + +Step03: Interseismic [tutorial] + Compression with slab creep + + +Step04: Earthquake cycle [exercise] + + +Step05: Compression with frictional interface [tutorial] + +Step06: Slow slip event [tutorial] + Prescribed slow slip on fault patch + +Step07: Green's functions [tutorial] + Generate Green's functions (slab patch + splay patch?) + Simple inversion of GPS data (slip on slab or splay?) + +Step08: Gravity + uniform density, demonstrate initial stresses + variable density, elastic: demonstrate deviation + variable density, elastic+viscoelastic: demonstrate problems + diff --git a/examples/3d/subduction/mesh/mesh_hex.jou b/examples/3d/subduction/mesh/mesh_hex.jou new file mode 100644 index 0000000000..abf7fc7cfc --- /dev/null +++ b/examples/3d/subduction/mesh/mesh_hex.jou @@ -0,0 +1,54 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# CUBIT/Trelis journal file for generating a tet mesh of the subduction zone. + +# ---------------------------------------------------------------------- +# Generate geometry +# ---------------------------------------------------------------------- +playback 'geometry.jou' + +# Set paving scheme on +y boundary. +surface 45 48 39 18 scheme pave + +# Set paving scheme on -y boundary. +surface 43 50 21 36 scheme pave + +surface all size {25.0*km} + +volume v_domain scheme sweep source surface 18 target surface 21 +volume v_domain@A scheme sweep source surface 43 target surface 45 +volume v_domain@B scheme sweep source surface 39 target surface 36 +volume v_domain@C scheme sweep source surface 48 target surface 50 + +volume all size {25.0*km} +mesh volume all + +# ---------------------------------------------------------------------- +# Create blocks and nodesets for materials and boundary conditions. +# ---------------------------------------------------------------------- +playback 'bc.jou' + + +# ---------------------------------------------------------------------- +# Export exodus file +# ---------------------------------------------------------------------- +export mesh "mesh_hex.exo" dimension 3 overwrite + + +# End of file + + diff --git a/examples/3d/subduction/mesh/mesh_tet.jou b/examples/3d/subduction/mesh/mesh_tet.jou index eb877c8091..5cbcd47818 100644 --- a/examples/3d/subduction/mesh/mesh_tet.jou +++ b/examples/3d/subduction/mesh/mesh_tet.jou @@ -21,13 +21,22 @@ # ---------------------------------------------------------------------- playback 'geometry.jou' +# Uniform resolution tetmesh. volume all scheme tetmesh volume all size {25.0*km} - mesh volume all +# ---------------------------------------------------------------------- +# Create blocks and nodesets for materials and boundary conditions. +# ---------------------------------------------------------------------- +playback 'bc.jou' +# ---------------------------------------------------------------------- +# Export exodus file +# ---------------------------------------------------------------------- +export mesh "mesh_tet.exo" dimension 3 overwrite # End of file + diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg new file mode 100644 index 0000000000..0a1b2f8e4c --- /dev/null +++ b/examples/3d/subduction/pylithapp.cfg @@ -0,0 +1,121 @@ +[pylithapp] + +# This is not a self-contained simulation configuration file. This +# file only specifies the general parameters common to the simulations +# in this directory. + +# ---------------------------------------------------------------------- +# journal +# ---------------------------------------------------------------------- +# Turn on some journals to show progress. +[pylithapp.journal.info] +pylithapp = 1 +timedependent = 1 +greensfns = 1 +implicit = 1 +petsc = 1 +solverlinear = 1 +meshiocubit = 1 +implicitelasticity = 1 +faultcohesivekin = 1 +fiatlagrange = 1 +materials = 1 +mesh_distributor = 1 + +# ---------------------------------------------------------------------- +# mesh_generator +# ---------------------------------------------------------------------- +# We use a mesh from CUBIT/Trelis, so we need to change the reader +# from the default (MeshIOAscii) and set the filename. +[pylithapp.mesh_generator] +reader = pylith.meshio.MeshIOCubit +reader.filename = mesh/mesh_tet.exo + +# Optimize ordering of mesh cells and vertices using reverse +# Cuthill-KcKee algorithm. +reorder_mesh = True + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# For have a material for each block we created in CUBIT/Trelis. +# +# We have 4 blocks: +# - slab (block 1) +# - wedge (block 2) +# - crust (block 3) +# - mantle (block 4) +# +# We use the default material (ElasticIsotropic3D: 3-D isotropic, +# linear elastic material). + +[pylithapp.problem] +materials = [slab, wdge, crust, mantle] + +[pylithapp.problem.materials.slab] +label = Subducting slab +id = 1 +db_properties.label = Properties for subducting slab +db_properties.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 3 + +[pylithapp.problem.materials.wedge] +label = Accretionary wedge +id = 2 +db_properties.label = Properties for accretionary wedge +db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 3 + +[pylithapp.problem.materials.crust] +label = Continental crust +id = 3 +db_properties.label = Properties for continental crust +db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 3 + +[pylithapp.problem.materials.mantle] +label = Mantle +id = 4 +db_properties.label = Properties for mantle +db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 3 + + +# ---------------------------------------------------------------------- +# PETSc +# ---------------------------------------------------------------------- +# Set the solver options. +[pylithapp.petsc] +malloc_dump = + +# Convergence parameters. +ksp_rtol = 1.0e-10 +ksp_atol = 1.0e-20 +ksp_max_it = 500 +ksp_gmres_restart = 50 + +# Linear solver monitoring options. +ksp_monitor = true +#ksp_view = true +ksp_converged_reason = true +ksp_error_if_not_converged = true + +# Nonlinear solver monitoring options. +snes_rtol = 1.0e-10 +snes_atol = 1.0e-9 +snes_max_it = 100 +snes_monitor = true +snes_linesearch_monitor = true +#snes_view = true +snes_converged_reason = true +snes_error_if_not_converged = true + +# PETSc summary -- useful for performance information. +log_view = true + + +# End of file \ No newline at end of file diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg new file mode 100644 index 0000000000..d26aaa193b --- /dev/null +++ b/examples/3d/subduction/step01.cfg @@ -0,0 +1,118 @@ +[pylithapp] + +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- + +# +# This is a purely elastic static problem using only Dirichlet +# (displacement) boundary conditions. The lower (minimum z) boundary is +# held fixed in the z-direction. On the positive and negative x-boundaries, +# displacements are applied corresponding to 1 m of shear displacement in +# the positive and negative y-directions, and 1 m of axial (x) compression +# on each side. + +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- + +# This is not a self-contained simulation configuration file. This +# file only specifies parameters specific to tutorial step01. +# The general parameters are specificed in the pylithapp.cfg +# file which PyLith reads by default. +# +# To run the simulation: +# pylith step01.cfg +# +# Output will be directed to the directory output. + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.timedependent.formulation.time_step] +# Define the total time for the simulation and the default time step size. +total_time = 0.0*s ; total time of simulation +# Define an appropriat time step for simulations. Important for +# nondimensionalization of velocities and slip rates. +dt = 5.0*year + +[pylithapp.timedependent] +# Set bc to an array of 3 boundary conditions: 'x_pos','x_neg', and 'z_neg'. +bc = [x_pos,x_neg,z_neg] + +# MGK Testing CUDA +#formulation = pylith.problems.ImplicitCUDA + +[pylithapp.timedependent.implicit] +# Set the output to an array of 2 output managers. +# We will output the solution over the domain and the ground surface. +output = [domain,subdomain] + +# Set subdomain component to OutputSolnSubset (boundary of the domain). +output.subdomain = pylith.meshio.OutputSolnSubset + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +# Set the parameters for Dirichlet boundary conditions applied on the +# +x, -x, and -z faces of the box. +# +# We fix the x and y degrees of freedom on the +x and -x faces, and +# fix the z degree of freedom on the bottom (-z) face. +# +# For x_pos and x_neg, we change the database from ZeroDispDB (which +# specifies a zero value) to SimpleDB (which uses a data file to +# specify a spatial variation). +# +# For z_neg, we keep the default ZeroDispDB, since we just want zero +# z-displacements on that boundary. +# + +# The label corresponds to the name of the nodeset in CUBIT. + +# +x face +[pylithapp.timedependent.bc.x_pos] +bc_dof = [0, 1] +label = face_xpos +db_initial = spatialdata.spatialdb.SimpleDB +db_initial.label = Dirichlet BC on +x +db_initial.iohandler.filename = spatialdb/fixeddisp_axial_shear.spatialdb + +# -x face +[pylithapp.timedependent.bc.x_neg] +bc_dof = [0, 1] +label = face_xneg +db_initial = spatialdata.spatialdb.SimpleDB +db_initial.label = Dirichlet BC on -x +db_initial.iohandler.filename = spatialdb/fixeddisp_axial_shear.spatialdb + +# -z face +[pylithapp.timedependent.bc.z_neg] +bc_dof = [2] +label = face_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# Give basename for VTK domain output of solution over domain. +[pylithapp.problem.formulation.output.domain.writer] +filename = output/step01.vtk + +# Give basename for VTK domain output of solution over ground surface. +[pylithapp.problem.formulation.output.subdomain] +# Name of nodeset for ground surface. +label = face_zpos +writer.filename = output/step01-groundsurf.vtk + +# Give basename for VTK output of upper_crust state variables. +[pylithapp.timedependent.materials.upper_crust.output] +# Average values over quadrature points. +cell_filter = pylith.meshio.CellFilterAvg +writer.filename = output/step01-upper_crust.vtk + +# Give basename for VTK output of lower_crust state variables. +[pylithapp.timedependent.materials.lower_crust.output] +# Average values over quadrature points. +cell_filter = pylith.meshio.CellFilterAvg +writer.filename = output/step01-lower_crust.vtk From 0d2fe9e558ff15130b0d7e96a3b20de71a83d79e Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 11 Jun 2017 12:33:48 -0700 Subject: [PATCH 011/216] More work on README outlining example features. --- examples/3d/subduction/README | 49 ++++++++++++++++++++++++++++------- 1 file changed, 39 insertions(+), 10 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index a6dea18281..16bf541800 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -46,31 +46,60 @@ Features: + Prescribed slip w/multiple ruptures + Fault friction -Step01: Compression [tutorial] - UniformDB for material properties +Step01: Axial compression [tutorial] + Dirichlet BC with initial values + UniformDB with properties for each material + Static + LU preconditioner + + ParaView + Python script to view displacement field + Python script to view material properties (shear modulus) + + Exercise: Shear instead of axial compression Step02: Coseismic [exercise] - Prescribed slip on fault patch with viscoelastic relaxation - Viscosity via CompositeDB + DirichletBC constraining normal displacement on lateral and bottom boundaries + Prescribed uniform slip (UniformDB) on slab fault patch with viscoelastic relaxation + Viscosity via CompositeDB (single SimpleGridDB with viscosity as a fn of depth) + Quasistatic + field split + custom preconditioner -Step03: Interseismic [tutorial] - Compression with slab creep + ParaView + Python script to view prescribed slip + Python script to view relaxation of shear stress + Exercise: Change slip on slab to slip on splay fault + Exercise: Slip on lower slab and splay fault + Exercise: Slip on slab and splay fault + +Step03: Interseismic [tutorial] + DirichletBC with constant velocity (compression) + Prescribed fault slip with constant slip rate (UniformDB) [lower slab] + Prescribed fault slip with constant slip rate at depth (SimpleGridDB) [top slab] + Quasistatic Step04: Earthquake cycle [exercise] - + Interseismic + coseismic Step05: Compression with frictional interface [tutorial] + Interseismic + rate- and state-friction + Quasistatic Step06: Slow slip event [tutorial] - Prescribed slow slip on fault patch + DirichletBC constraining normal displacement on lateral and bottom boundaries + Prescribed slow slip on slab fault patch (SimpleGridDB 2-D in geo coordinates) + Time history slip-time function + Quasistatic + OutputSolnPoints Step07: Green's functions [tutorial] Generate Green's functions (slab patch + splay patch?) Simple inversion of GPS data (slip on slab or splay?) + OutputSolnPoints Step08: Gravity - uniform density, demonstrate initial stresses - variable density, elastic: demonstrate deviation + uniform density (SimpleDB), demonstrate initial stresses to compensate gravity + variable density (match Step01), initial stress matches avg desnity, elastic: demonstrate deviation variable density, elastic+viscoelastic: demonstrate problems From d188ff2dec0b3ae3b1b47fca6db0e39bb36670db Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 11 Jun 2017 12:37:25 -0700 Subject: [PATCH 012/216] Add notes on directory structure. --- examples/3d/subduction/README | 4 ++++ 1 file changed, 4 insertions(+) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 16bf541800..fb7d1ef263 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -1,3 +1,7 @@ +Directory structure: + mesh (mesh related files) + spatialdb (spatial database related files) + Features: Spatial databases From 84585aed9a9a04b5f225cba20273ceccce036210 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 12 Jun 2017 09:50:20 +1200 Subject: [PATCH 013/216] Fixed a couple of typos in bc.jou. --- examples/3d/subduction/mesh/bc.jou | 36 +++++++++++++++--------------- 1 file changed, 18 insertions(+), 18 deletions(-) diff --git a/examples/3d/subduction/mesh/bc.jou b/examples/3d/subduction/mesh/bc.jou index d16cd80452..6a5ac80169 100644 --- a/examples/3d/subduction/mesh/bc.jou +++ b/examples/3d/subduction/mesh/bc.jou @@ -62,8 +62,8 @@ nodeset 11 name "fault_slabtop_edge" # Entire bottom of slab group "fault_slabbot" add node in s_slabbot@A -nodeset 20 group fault_slabtop -nodeset 20 name "fault_slabtop" +nodeset 20 group fault_slabbot +nodeset 20 name "fault_slabbot" # Buried edge for bottom of slab. group "fault_slabbot_edge" add node in curve 36 @@ -127,14 +127,14 @@ nodeset 80 name "boundary_xpos" # -x group "boundary_xneg" add node in surface 20 group "boundary_xneg" add node in surface 28 -nodeset 80 group boundary_xneg -nodeset 80 name "boundary_xneg" +nodeset 81 group boundary_xneg +nodeset 81 name "boundary_xneg" # -x w/o fault group "boundary_xneg_nofault" add node in group boundary_xneg group "boundary_xneg_nofault" remove node in group fault_slabbot -nodeset 81 group boundary_xneg_nofault -nodeset 81 name "boundary_xneg_nofault" +nodeset 82 group boundary_xneg_nofault +nodeset 82 name "boundary_xneg_nofault" # +y @@ -142,16 +142,16 @@ group "boundary_ypos" add node in surface 18 group "boundary_ypos" add node in surface 45 group "boundary_ypos" add node in surface 48 group "boundary_ypos" add node in surface 39 -nodeset 82 group boundary_ypos -nodeset 82 name "boundary_ypos" +nodeset 83 group boundary_ypos +nodeset 83 name "boundary_ypos" # +y w/o fault group "boundary_ypos_nofault" add node in group boundary_ypos group "boundary_ypos_nofault" remove node in group fault_slabtop group "boundary_ypos_nofault" remove node in group fault_slabbot group "boundary_ypos_nofault" remove node in group fault_splay -nodeset 83 group boundary_ypos_nofault -nodeset 83 name "boundary_ypos_nofault" +nodeset 84 group boundary_ypos_nofault +nodeset 84 name "boundary_ypos_nofault" # -y @@ -159,28 +159,28 @@ group "boundary_yneg" add node in surface 21 group "boundary_yneg" add node in surface 43 group "boundary_yneg" add node in surface 50 group "boundary_yneg" add node in surface 36 -nodeset 84 group boundary_yneg -nodeset 84 name "boundary_yneg" +nodeset 85 group boundary_yneg +nodeset 85 name "boundary_yneg" # -y w/o fault group "boundary_yneg_nofault" add node in group boundary_yneg group "boundary_yneg_nofault" remove node in group fault_slabtop group "boundary_yneg_nofault" remove node in group fault_slabbot group "boundary_yneg_nofault" remove node in group fault_splay -nodeset 85 group boundary_yneg_nofault -nodeset 85 name "boundary_yneg_nofault" +nodeset 86 group boundary_yneg_nofault +nodeset 86 name "boundary_yneg_nofault" # -z group "boundary_zneg" add node in surface 10 -nodeset 86 group boundary_zneg -nodeset 86 name "boundary_zneg" +nodeset 87 group boundary_zneg +nodeset 87 name "boundary_zneg" # +z group "boundary_zpos" add node in surface 47 group "boundary_zpos" add node in surface 42 group "boundary_zpos" add node in surface 19 -nodeset 86 group boundary_zpos -nodeset 86 name "boundary_zpos" +nodeset 88 group boundary_zpos +nodeset 88 name "boundary_zpos" # End of file From b75367d44c9a1eefea05b92194e9bc0217f6e76c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 13 Jun 2017 12:33:31 -0700 Subject: [PATCH 014/216] Initial setup for examples/3d/subduction/step01. --- .gitignore | 31 +--- examples/3d/subduction/plot_dispvec.py | 87 +++++++++ examples/3d/subduction/plot_dispwarp.py | 84 +++++++++ examples/3d/subduction/pylithapp.cfg | 14 +- .../spatialdb/mat_crust_elastic.spatialdb | 26 +++ .../spatialdb/mat_mantle_elastic.spatialdb | 26 +++ .../spatialdb/mat_slab_elastic.spatialdb | 26 +++ .../spatialdb/mat_wedge_elastic.spatialdb | 26 +++ examples/3d/subduction/step01.cfg | 170 ++++++++++-------- 9 files changed, 391 insertions(+), 99 deletions(-) create mode 100644 examples/3d/subduction/plot_dispvec.py create mode 100644 examples/3d/subduction/plot_dispwarp.py create mode 100644 examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb create mode 100644 examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb create mode 100644 examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb create mode 100644 examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb diff --git a/.gitignore b/.gitignore index 9856009409..4766c64016 100644 --- a/.gitignore +++ b/.gitignore @@ -2,33 +2,14 @@ /GRTAGS /GSYMS /GTAGS +/doc/userguide/userguide.pdf +pylith_parameters.json +modulesrc/*/*_wrap.cxx +modulesrc/*/*.py /templates/friction/frictioncontrib.py /templates/friction/frictioncontrib_wrap.cxx /templates/materials/materialscontrib.py /templates/materials/materialscontrib_wrap.cxx -/doc/userguide/userguide.pdf -modulesrc/bc/bc.py -modulesrc/bc/bc_wrap.cxx -modulesrc/faults/faults.py -modulesrc/faults/faults_wrap.cxx -modulesrc/feassemble/feassemble.py -modulesrc/feassemble/feassemble_wrap.cxx -modulesrc/friction/friction.py -modulesrc/friction/friction_wrap.cxx -modulesrc/materials/materials.py -modulesrc/materials/materials_wrap.cxx -modulesrc/meshio/meshio.py -modulesrc/meshio/meshio_wrap.cxx -modulesrc/mpi/mpi.py -modulesrc/mpi/mpi_wrap.cxx -modulesrc/utils/petsc.py -modulesrc/utils/petsc_wrap.cxx -modulesrc/problems/problems.py -modulesrc/problems/problems_wrap.cxx -modulesrc/topology/topology.py -modulesrc/topology/topology_wrap.cxx -modulesrc/utils/utils.py -modulesrc/utils/utils_wrap.cxx configure aclocal.m4 Makefile.in @@ -49,3 +30,7 @@ tests_auto/*/*/*_disp.spatialdb tests_auto/*/*/output tests_auto/*/*/output examples/3d/hex8/output +examples/3d/subduction/output +examples/3d/subduction/mesh/geometry_surfs.jou +examples/3d/subduction/mesh/*.exo +examples/3d/subduction/mesh/*.sat diff --git a/examples/3d/subduction/plot_dispvec.py b/examples/3d/subduction/plot_dispvec.py new file mode 100644 index 0000000000..644ae91057 --- /dev/null +++ b/examples/3d/subduction/plot_dispvec.py @@ -0,0 +1,87 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the domain, colored by the magnitude of the displacement +# vector, with white arrows showing the displacement vectors. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters + +# Root name for simulation. +SIM_NAME = "step01" + +# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) +DATA_FORMAT = "vtk" + +# Scale used to exaggerate deformation. +DISPLACEMENT_SCALE = 10.0e+3 + + +# ---------------------------------------------------------------------- +# We create sources, filters, etc using the servermanager so that we can set the +# name of the proxy shown in the pipeline using Register(registrationName=NAME). + +from paraview.simple import * +# Disable automatic camera reset on "Show" +paraview.simple._DisableFirstRenderCameraReset() + +# Read data +if DATA_FORMAT.lower() == "vtk": + dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) +elif DATA_FORMAT.lower() == "hdf5": + pass +else: + raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) +servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) +view = GetActiveViewOrCreate('RenderView') + +# Show undeformed domain, colored by magnitude of displacement vector. +domainDisplay = Show(dataDomain, view) +ColorBy(domainDisplay, ("POINTS", "displacement", "Magnitude")) +domainDisplay.RescaleTransferFunctionToDataRange(True) +domainDisplay.SetScalarBarVisibility(view, True) +domainDisplay.SetRepresentationType("Surface With Edges") + +# Rescale color and/or opacity maps used to exactly fit the current data range +displacementLUT = GetColorTransferFunction('displacement') +domainDisplay.RescaleTransferFunctionToDataRange(False, False) +# Update scalar bar component title. +UpdateScalarBarsComponentTitle(displacementLUT, domainDisplay) + + +# Add arrows to show displacement vectors. +glyph = servermanager.filters.Glyph(Input=dataDomain, GlyphType="Arrow") +servermanager.Register(glyph, registrationName="%s-domain-glyph" % SIM_NAME) +glyph.Vectors = ["POINTS", "displacement"] +glyph.ScaleFactor = DISPLACEMENT_SCALE +glyph.ScaleMode = "vector" +glyph.GlyphMode = "All Points" + +glyphDisplay = Show(glyph, view) +glyphDisplay.Representation = "Surface" + +view.ResetCamera() + +Render() + +# Uncomment if running from shell outside ParaView. +#Interact() + + +# End of file diff --git a/examples/3d/subduction/plot_dispwarp.py b/examples/3d/subduction/plot_dispwarp.py new file mode 100644 index 0000000000..4bc65ba387 --- /dev/null +++ b/examples/3d/subduction/plot_dispwarp.py @@ -0,0 +1,84 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the deformed +# domain, colored by the value of the x-displacemenet. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters + +# Root name for simulation. +SIM_NAME = "step01" + +# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) +DATA_FORMAT = "vtk" + +# Scale used to exaggerate deformation. +DISPLACEMENT_SCALE = 10.0e+3 + +# ---------------------------------------------------------------------- +# We create sources, filters, etc using the servermanager so that we can set the +# name of the proxy shown in the pipeline using Register(registrationName=NAME). + +from paraview.simple import * +# Disable automatic camera reset on "Show" +paraview.simple._DisableFirstRenderCameraReset() + +# Read data +if DATA_FORMAT == "vtk": + dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) +elif DATA_FORMAT == "HDF5": + pass +else: + raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) +servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) +view = GetActiveViewOrCreate('RenderView') + +# Gray wireframe for undeformed domain. +domainDisplay = Show(dataDomain, view) +domainDisplay.Representation = 'Wireframe' +domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + +# Warp domain to show deformation +warp = servermanager.filters.WarpByVector(Input=dataDomain) +servermanager.Register(warp, registrationName="%s-domain-warp" % SIM_NAME) +warp.Vectors = ['POINTS', 'displacement'] +warp.ScaleFactor = DISPLACEMENT_SCALE + +warpDisplay = Show(warp, view) +ColorBy(warpDisplay, ('POINTS', 'displacement', 'X')) +warpDisplay.RescaleTransferFunctionToDataRange(True) +warpDisplay.SetScalarBarVisibility(view, True) +warpDisplay.SetRepresentationType('Surface With Edges') + +# Rescale color and/or opacity maps used to exactly fit the current data range +displacementLUT = GetColorTransferFunction('displacement') +warpDisplay.RescaleTransferFunctionToDataRange(False, False) +# Update a scalar bar component title. +UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) + +view.ResetCamera() + +Render() + +# Uncomment if running from shell outside ParaView. +#Interact() + + +# End of file diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 0a1b2f8e4c..00f16fde78 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -50,7 +50,7 @@ reorder_mesh = True # linear elastic material). [pylithapp.problem] -materials = [slab, wdge, crust, mantle] +materials = [slab, wedge, crust, mantle] [pylithapp.problem.materials.slab] label = Subducting slab @@ -60,6 +60,9 @@ db_properties.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 +# Average cell output over quadrature points, yielding one point per cell +output.cell_filter = pylith.meshio.CellFilterAvg + [pylithapp.problem.materials.wedge] label = Accretionary wedge id = 2 @@ -68,6 +71,8 @@ db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 +output.cell_filter = pylith.meshio.CellFilterAvg + [pylithapp.problem.materials.crust] label = Continental crust id = 3 @@ -76,6 +81,8 @@ db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 +output.cell_filter = pylith.meshio.CellFilterAvg + [pylithapp.problem.materials.mantle] label = Mantle id = 4 @@ -84,6 +91,8 @@ db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 +output.cell_filter = pylith.meshio.CellFilterAvg + # ---------------------------------------------------------------------- # PETSc @@ -92,6 +101,9 @@ quadrature.cell.dimension = 3 [pylithapp.petsc] malloc_dump = +# Use LU preconditioner (helful for learning and debugging, not production simulations) +pc_type = lu + # Convergence parameters. ksp_rtol = 1.0e-10 ksp_atol = 1.0e-20 diff --git a/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb new file mode 100644 index 0000000000..526fab2c28 --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb @@ -0,0 +1,26 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the distribution of material +// properties. In this case, the material properties are uniform. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 3 // number of material property values + value-names = density vs vp // names of the material property values + value-units = kg/m**3 m/s m/s // units + num-locs = 1 // number of locations + data-dim = 0 + space-dim = 3 + cs-data = cartesian { + to-meters = 1.0 + space-dim = 3 + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) density (kg/m^3) +// (5) vs (m/s) +// (6) vp (m/s) +0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 diff --git a/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb new file mode 100644 index 0000000000..526fab2c28 --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb @@ -0,0 +1,26 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the distribution of material +// properties. In this case, the material properties are uniform. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 3 // number of material property values + value-names = density vs vp // names of the material property values + value-units = kg/m**3 m/s m/s // units + num-locs = 1 // number of locations + data-dim = 0 + space-dim = 3 + cs-data = cartesian { + to-meters = 1.0 + space-dim = 3 + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) density (kg/m^3) +// (5) vs (m/s) +// (6) vp (m/s) +0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 diff --git a/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb new file mode 100644 index 0000000000..526fab2c28 --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb @@ -0,0 +1,26 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the distribution of material +// properties. In this case, the material properties are uniform. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 3 // number of material property values + value-names = density vs vp // names of the material property values + value-units = kg/m**3 m/s m/s // units + num-locs = 1 // number of locations + data-dim = 0 + space-dim = 3 + cs-data = cartesian { + to-meters = 1.0 + space-dim = 3 + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) density (kg/m^3) +// (5) vs (m/s) +// (6) vp (m/s) +0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 diff --git a/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb new file mode 100644 index 0000000000..526fab2c28 --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb @@ -0,0 +1,26 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the distribution of material +// properties. In this case, the material properties are uniform. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 3 // number of material property values + value-names = density vs vp // names of the material property values + value-units = kg/m**3 m/s m/s // units + num-locs = 1 // number of locations + data-dim = 0 + space-dim = 3 + cs-data = cartesian { + to-meters = 1.0 + space-dim = 3 + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) density (kg/m^3) +// (5) vs (m/s) +// (6) vp (m/s) +0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index d26aaa193b..e11596ca35 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -1,118 +1,138 @@ -[pylithapp] - +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- - +# # # This is a purely elastic static problem using only Dirichlet -# (displacement) boundary conditions. The lower (minimum z) boundary is -# held fixed in the z-direction. On the positive and negative x-boundaries, -# displacements are applied corresponding to 1 m of shear displacement in -# the positive and negative y-directions, and 1 m of axial (x) compression -# on each side. - +# (displacement) boundary conditions. +# +# The positive and negative x-boundaries yield 4 m of axial +# compression. The negative z-boundary and positive and negative +# y-boundaries are held fixed in the direction normal to the boundary. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- - +# # This is not a self-contained simulation configuration file. This # file only specifies parameters specific to tutorial step01. -# The general parameters are specificed in the pylithapp.cfg +# The general parameters are specified in the pylithapp.cfg # file which PyLith reads by default. # # To run the simulation: # pylith step01.cfg # -# Output will be directed to the directory output. +# Output will be directed to the "output" directory.. # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- -[pylithapp.timedependent.formulation.time_step] +[pylithapp.problem.formulation.time_step] # Define the total time for the simulation and the default time step size. -total_time = 0.0*s ; total time of simulation -# Define an appropriat time step for simulations. Important for -# nondimensionalization of velocities and slip rates. -dt = 5.0*year - -[pylithapp.timedependent] -# Set bc to an array of 3 boundary conditions: 'x_pos','x_neg', and 'z_neg'. -bc = [x_pos,x_neg,z_neg] - -# MGK Testing CUDA -#formulation = pylith.problems.ImplicitCUDA - -[pylithapp.timedependent.implicit] -# Set the output to an array of 2 output managers. -# We will output the solution over the domain and the ground surface. -output = [domain,subdomain] - -# Set subdomain component to OutputSolnSubset (boundary of the domain). -output.subdomain = pylith.meshio.OutputSolnSubset +total_time = 0.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -# Set the parameters for Dirichlet boundary conditions applied on the -# +x, -x, and -z faces of the box. -# -# We fix the x and y degrees of freedom on the +x and -x faces, and -# fix the z degree of freedom on the bottom (-z) face. -# -# For x_pos and x_neg, we change the database from ZeroDispDB (which -# specifies a zero value) to SimpleDB (which uses a data file to -# specify a spatial variation). -# -# For z_neg, we keep the default ZeroDispDB, since we just want zero -# z-displacements on that boundary. +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. # +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (UniformDB to specify x-displacement) +# x_pos (UniformDB to specify x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] # The label corresponds to the name of the nodeset in CUBIT. +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +# Use a UniformDB +db_initial = spatialdata.spatialdb.UniformDB +db_initial.label = Dirichlet BC on -x +db_initial.values = [displacement-x] +db_initial.data = [+2.0*m] + # +x face -[pylithapp.timedependent.bc.x_pos] -bc_dof = [0, 1] -label = face_xpos -db_initial = spatialdata.spatialdb.SimpleDB +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial = spatialdata.spatialdb.UniformDB db_initial.label = Dirichlet BC on +x -db_initial.iohandler.filename = spatialdb/fixeddisp_axial_shear.spatialdb +db_initial.values = [displacement-x] +db_initial.data = [-2.0*m] -# -x face -[pylithapp.timedependent.bc.x_neg] -bc_dof = [0, 1] -label = face_xneg -db_initial = spatialdata.spatialdb.SimpleDB -db_initial.label = Dirichlet BC on -x -db_initial.iohandler.filename = spatialdb/fixeddisp_axial_shear.spatialdb +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y # -z face -[pylithapp.timedependent.bc.z_neg] +[pylithapp.problem.bc.z_neg] bc_dof = [2] -label = face_zneg +label = boundary_zneg db_initial.label = Dirichlet BC on -z # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- -# Give basename for VTK domain output of solution over domain. -[pylithapp.problem.formulation.output.domain.writer] -filename = output/step01.vtk +# We output the solution over the entire domain and over the top surface. +# +# We write the output using VTK data files (default). + +[pylithapp.problem.implicit] +output = [domain, subdomain] + +# Set subdomain component to OutputSolnSubset (boundary of the domain). +output.subdomain = pylith.meshio.OutputSolnSubset + +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step01-domain.vtk -# Give basename for VTK domain output of solution over ground surface. [pylithapp.problem.formulation.output.subdomain] -# Name of nodeset for ground surface. -label = face_zpos +# Name of nodeset for top surface. +label = boundary_zpos writer.filename = output/step01-groundsurf.vtk -# Give basename for VTK output of upper_crust state variables. -[pylithapp.timedependent.materials.upper_crust.output] -# Average values over quadrature points. -cell_filter = pylith.meshio.CellFilterAvg -writer.filename = output/step01-upper_crust.vtk - -# Give basename for VTK output of lower_crust state variables. -[pylithapp.timedependent.materials.lower_crust.output] -# Average values over quadrature points. -cell_filter = pylith.meshio.CellFilterAvg -writer.filename = output/step01-lower_crust.vtk +# Output for materials ---------------------------------------- +[pylithapp.problem.materials.slab.output] +writer.filename = output/step01-slab.vtk + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step01-wedge.vtk + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step01-crust.vtk + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step01-mantle.vtk + + +# End of file From 0d8380225c318f061d80aa6d9038986683520ecb Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 14 Jun 2017 11:04:42 +1200 Subject: [PATCH 015/216] Added shell and Python scripts to create coastline VTK file. --- examples/3d/subduction/get_coast.sh | 33 ++++++++++++ examples/3d/subduction/seg2vtk.py | 84 +++++++++++++++++++++++++++++ 2 files changed, 117 insertions(+) create mode 100755 examples/3d/subduction/get_coast.sh create mode 100755 examples/3d/subduction/seg2vtk.py diff --git a/examples/3d/subduction/get_coast.sh b/examples/3d/subduction/get_coast.sh new file mode 100755 index 0000000000..44d838edd7 --- /dev/null +++ b/examples/3d/subduction/get_coast.sh @@ -0,0 +1,33 @@ +#!/bin/sh +# Script to get coastline from GMT and make a VTK file for visualization. +# Note that GMT4 is used. Parameters and Python script would need modification +# for GMT5. + +# Filenames. +txtwgs84="cascadia_wgs84.txt" +txttm="cascadia_tm.txt" +vtktm="cascadia_tm.vtk" + +# Region. +region="-R-129/-117/41/50" + +# Resolution: (f)ull, (h)igh, (i)ntermediate, (l)ow, or (c)rude. +reso="-Dh" + +# Draw rivers option. +# rivers="-Ia" +rivers="-I1" + +# Draw political boundaries option. +political="-Na" + +# Get coastlines from pscoast. +pscoast $region $reso $rivers $political -Jx1.0d -W -m'#' > $txtwgs84 + +# Do coordinate conversion to local Transverse Mercator. +cs2cs +proj=lonlat +ellps=WGS84 +datum=WGS84 +to +proj=tmerc +lon_0=-122.6765 +lat_0=45.5231 +datum=WGS84 +k=0.9996 $txtwgs84 > $txttm + +# Run seg2vtk.py script to convert pscoast info to VTK file. +./seg2vtk.py --in_file=$txttm --out_file=$vtktm --elevation=0.1 + +/bin/rm $txtwgs84 $txttm diff --git a/examples/3d/subduction/seg2vtk.py b/examples/3d/subduction/seg2vtk.py new file mode 100755 index 0000000000..e9a8fc0f4d --- /dev/null +++ b/examples/3d/subduction/seg2vtk.py @@ -0,0 +1,84 @@ +#!/usr/bin/env python +import math +import numpy +import pdb +# pdb.set_trace() + +# Get command-line arguments. +from optparse import OptionParser +parser = OptionParser() +parser.add_option("-i", "--in_file", action="store", type="string", + dest="in_file", help="input file from GMT") +parser.add_option("-o", "--out_file", action="store", type="string", + dest="out_file", help="output VTK file") +parser.add_option("-e", "--elevation", action="store", type="float", + default=0.0, dest="elevation", + help="z-value assigned to segments [default: %default]") + +(options, args) = parser.parse_args() + +if (not options.in_file): + parser.error("input file must be specified") + +if (not options.out_file): + parser.error("output file must be specified") + +in_file = options.in_file +out_file = options.out_file +elevation = options.elevation + +f = open(in_file, 'r') +g = open(out_file, 'w') + +g.write('# vtk DataFile Version 2.0\n') +g.write('New Zealand coastlines.\n') +g.write('ASCII\n') +g.write('DATASET POLYDATA\n') + +numvertices = 0 +numlines = 0 +vertsperline = [] +totallineentries = 0 +x = [] +y = [] +z = elevation + +for line in f: + if( line.startswith('#')): + numlines += 1 + vertsperline.append(0) + totallineentries += 1 + else: + numvertices += 1 + vertsperline[numlines - 1] += 1 + totallineentries += 1 + data = line.split() + x.append(float(data[0])) + y.append(float(data[1])) + +f.close() + +g.write('POINTS %8d double\n' % numvertices) + +for vertex in range(numvertices): + g.write('%.10f' % x[vertex]) + g.write(' %.10f' % y[vertex]) + g.write(' %.10f' % z) + g.write('\n') + +g.write('LINES %8d ' % numlines) +g.write('%8d\n' % totallineentries) + +startvertex = 0 +for line in range(numlines): + g.write('%8d' % vertsperline[line]) + for vertex in range(startvertex, startvertex + vertsperline[line]): + g.write(' %8d' % vertex) + startvertex += vertsperline[line] + + g.write('\n') + +g.close() +print "Number of vertices: ", numvertices +print "Number of lines: ", numlines +print "Number of line entries: ", totallineentries From 7b75bdbea8ea085d5af4faad1ba6823ade7a8d98 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 14 Jun 2017 11:09:36 +1200 Subject: [PATCH 016/216] Listed dependencies in shell script, removed unneeded packages from Python script, and changed VTK header to not mention New Zealand. --- examples/3d/subduction/get_coast.sh | 1 + examples/3d/subduction/seg2vtk.py | 6 ++---- 2 files changed, 3 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/get_coast.sh b/examples/3d/subduction/get_coast.sh index 44d838edd7..77d0811b22 100755 --- a/examples/3d/subduction/get_coast.sh +++ b/examples/3d/subduction/get_coast.sh @@ -2,6 +2,7 @@ # Script to get coastline from GMT and make a VTK file for visualization. # Note that GMT4 is used. Parameters and Python script would need modification # for GMT5. +# PROJ.4 is also required for coordinate conversions. # Filenames. txtwgs84="cascadia_wgs84.txt" diff --git a/examples/3d/subduction/seg2vtk.py b/examples/3d/subduction/seg2vtk.py index e9a8fc0f4d..9045eb3403 100755 --- a/examples/3d/subduction/seg2vtk.py +++ b/examples/3d/subduction/seg2vtk.py @@ -1,7 +1,5 @@ #!/usr/bin/env python -import math -import numpy -import pdb +# import pdb # pdb.set_trace() # Get command-line arguments. @@ -31,7 +29,7 @@ g = open(out_file, 'w') g.write('# vtk DataFile Version 2.0\n') -g.write('New Zealand coastlines.\n') +g.write('Coastline segments.\n') g.write('ASCII\n') g.write('DATASET POLYDATA\n') From feba7dd75a36db5cd33f6e44975b792f9a0eaf4a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 13 Jun 2017 17:05:45 -0700 Subject: [PATCH 017/216] Updated README. --- examples/3d/subduction/README | 15 +++++++++++++-- examples/3d/subduction/mesh/coordsys.py | 13 ------------- 2 files changed, 13 insertions(+), 15 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index fb7d1ef263..a328554c61 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -2,6 +2,17 @@ Directory structure: mesh (mesh related files) spatialdb (spatial database related files) + +Elastic properties loosely based on + +Stephenson, W.J., 2007, Velocity and density models incorporating the +Cascadia subduction zone for 3D earthquake ground motion simulations, +Version 1.3: U.S. Geological Survey, Earthquake Hazards Ground Motion +Investigations, Open-File Report 2007–1348, 24 pages, +https://pubs.usgs.gov/of/2007/1348/. + + + Features: Spatial databases @@ -51,8 +62,8 @@ Features: + Fault friction Step01: Axial compression [tutorial] - Dirichlet BC with initial values - UniformDB with properties for each material + Dirichlet BC with initial values (UniformDB) + SimpleDB with properties for each material Static LU preconditioner diff --git a/examples/3d/subduction/mesh/coordsys.py b/examples/3d/subduction/mesh/coordsys.py index fdcee78f03..f51b63bd32 100644 --- a/examples/3d/subduction/mesh/coordsys.py +++ b/examples/3d/subduction/mesh/coordsys.py @@ -55,17 +55,4 @@ def geoToMesh(xyz): return -def bbox_mesh(): - """ - """ - xdim = 2000.0e+3 - ydim = 2000.0e+3 - xoffset = 0.0e+3 - yoffset = 0.0e+3 - - bbox = (xoffset-0.5*xdim, yoffset-0.5*ydim, - xoffset+0.5*xdim, yoffset+0.5*ydim) - return bbox - - # End of file From 52f024eee89bbc66d8c51eda85d0640a48af7818 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 13 Jun 2017 17:06:25 -0700 Subject: [PATCH 018/216] Change output to HDF5. --- examples/3d/subduction/plot_dispvec.py | 4 +-- examples/3d/subduction/plot_dispwarp.py | 8 ++--- examples/3d/subduction/pylithapp.cfg | 45 +++++++++++++++++++------ examples/3d/subduction/step01.cfg | 26 +++++--------- 4 files changed, 49 insertions(+), 34 deletions(-) diff --git a/examples/3d/subduction/plot_dispvec.py b/examples/3d/subduction/plot_dispvec.py index 644ae91057..cb209267a9 100644 --- a/examples/3d/subduction/plot_dispvec.py +++ b/examples/3d/subduction/plot_dispvec.py @@ -27,7 +27,7 @@ SIM_NAME = "step01" # Format of simulation output (choices=["vtk", "hdf5"], case insentitive) -DATA_FORMAT = "vtk" +DATA_FORMAT = "hdf5" # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 @@ -45,7 +45,7 @@ if DATA_FORMAT.lower() == "vtk": dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) elif DATA_FORMAT.lower() == "hdf5": - pass + dataDomain = servermanager.sources.XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) else: raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) diff --git a/examples/3d/subduction/plot_dispwarp.py b/examples/3d/subduction/plot_dispwarp.py index 4bc65ba387..d67a989952 100644 --- a/examples/3d/subduction/plot_dispwarp.py +++ b/examples/3d/subduction/plot_dispwarp.py @@ -27,7 +27,7 @@ SIM_NAME = "step01" # Format of simulation output (choices=["vtk", "hdf5"], case insentitive) -DATA_FORMAT = "vtk" +DATA_FORMAT = "hdf5" # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 @@ -41,10 +41,10 @@ paraview.simple._DisableFirstRenderCameraReset() # Read data -if DATA_FORMAT == "vtk": +if DATA_FORMAT.lower() == "vtk": dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) -elif DATA_FORMAT == "HDF5": - pass +elif DATA_FORMAT.lower() == "hdf5": + dataDomain = servermanager.sources.XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) else: raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 00f16fde78..7cf0bed62b 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -43,8 +43,8 @@ reorder_mesh = True # We have 4 blocks: # - slab (block 1) # - wedge (block 2) -# - crust (block 3) -# - mantle (block 4) +# - mantle (block 3) +# - crust (block 4) # # We use the default material (ElasticIsotropic3D: 3-D isotropic, # linear elastic material). @@ -62,6 +62,8 @@ quadrature.cell.dimension = 3 # Average cell output over quadrature points, yielding one point per cell output.cell_filter = pylith.meshio.CellFilterAvg +output.writer = pylith.meshio.DataWriterHDF5 + [pylithapp.problem.materials.wedge] label = Accretionary wedge @@ -72,27 +74,50 @@ quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 output.cell_filter = pylith.meshio.CellFilterAvg +output.writer = pylith.meshio.DataWriterHDF5 -[pylithapp.problem.materials.crust] -label = Continental crust +[pylithapp.problem.materials.mantle] +label = Mantle id = 3 -db_properties.label = Properties for continental crust -db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb +db_properties.label = Properties for mantle +db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 output.cell_filter = pylith.meshio.CellFilterAvg +output.writer = pylith.meshio.DataWriterHDF5 -[pylithapp.problem.materials.mantle] -label = Mantle +[pylithapp.problem.materials.crust] +label = Continental crust id = 4 -db_properties.label = Properties for mantle -db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb +db_properties.label = Properties for continental crust +db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 output.cell_filter = pylith.meshio.CellFilterAvg +output.writer = pylith.meshio.DataWriterHDF5 + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# We output the solution over the entire domain and over the top surface. +# +# We write the output using HDF5/Xdmf files. + +[pylithapp.problem.implicit] +output = [domain, subdomain] + +# Set subdomain component to OutputSolnSubset (boundary of the domain). +output.subdomain = pylith.meshio.OutputSolnSubset + +[pylithapp.problem.formulation.output.domain] +writer = pylith.meshio.DataWriterHDF5 +[pylithapp.problem.formulation.output.subdomain] +# Name of nodeset for top surface. +label = boundary_zpos +writer = pylith.meshio.DataWriterHDF5 # ---------------------------------------------------------------------- # PETSc diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index e11596ca35..92263e3af8 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -103,36 +103,26 @@ db_initial.label = Dirichlet BC on -z # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- -# We output the solution over the entire domain and over the top surface. -# -# We write the output using VTK data files (default). - -[pylithapp.problem.implicit] -output = [domain, subdomain] - -# Set subdomain component to OutputSolnSubset (boundary of the domain). -output.subdomain = pylith.meshio.OutputSolnSubset +# Domain and subdomain output ------------------------------------------ [pylithapp.problem.formulation.output.domain] -writer.filename = output/step01-domain.vtk +writer.filename = output/step01-domain.h5 [pylithapp.problem.formulation.output.subdomain] -# Name of nodeset for top surface. -label = boundary_zpos -writer.filename = output/step01-groundsurf.vtk +writer.filename = output/step01-groundsurf.h5 -# Output for materials ---------------------------------------- +# Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] -writer.filename = output/step01-slab.vtk +writer.filename = output/step01-slab.h5 [pylithapp.problem.materials.wedge.output] -writer.filename = output/step01-wedge.vtk +writer.filename = output/step01-wedge.h5 [pylithapp.problem.materials.crust.output] -writer.filename = output/step01-crust.vtk +writer.filename = output/step01-crust.h5 [pylithapp.problem.materials.mantle.output] -writer.filename = output/step01-mantle.vtk +writer.filename = output/step01-mantle.h5 # End of file From f34b3dd7dd7effde9081174985470933d9eb8d55 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 13 Jun 2017 17:06:44 -0700 Subject: [PATCH 019/216] Update elastic material properties. --- .../3d/subduction/spatialdb/mat_crust_elastic.spatialdb | 8 ++++---- .../3d/subduction/spatialdb/mat_mantle_elastic.spatialdb | 8 ++++---- .../3d/subduction/spatialdb/mat_slab_elastic.spatialdb | 8 ++++---- .../3d/subduction/spatialdb/mat_wedge_elastic.spatialdb | 8 ++++---- 4 files changed, 16 insertions(+), 16 deletions(-) diff --git a/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb index 526fab2c28..2af855ab9c 100644 --- a/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb @@ -7,7 +7,7 @@ SimpleDB { num-values = 3 // number of material property values value-names = density vs vp // names of the material property values - value-units = kg/m**3 m/s m/s // units + value-units = kg/m**3 km/s km/s // units num-locs = 1 // number of locations data-dim = 0 space-dim = 3 @@ -21,6 +21,6 @@ SimpleDB { // (2) y coordinate (m) // (3) z coordinate (m) // (4) density (kg/m^3) -// (5) vs (m/s) -// (6) vp (m/s) -0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 +// (5) vs (km/s) +// (6) vp (km/s) +0.0 0.0 0.0 3000.0 4.0 7.0 diff --git a/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb index 526fab2c28..a22038c63e 100644 --- a/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb @@ -7,7 +7,7 @@ SimpleDB { num-values = 3 // number of material property values value-names = density vs vp // names of the material property values - value-units = kg/m**3 m/s m/s // units + value-units = kg/m**3 km/s km/s // units num-locs = 1 // number of locations data-dim = 0 space-dim = 3 @@ -21,6 +21,6 @@ SimpleDB { // (2) y coordinate (m) // (3) z coordinate (m) // (4) density (kg/m^3) -// (5) vs (m/s) -// (6) vp (m/s) -0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 +// (5) vs (km/s) +// (6) vp (km/s) +0.0 0.0 0.0 3300.0 4.2 7.5 diff --git a/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb index 526fab2c28..98d4cff36c 100644 --- a/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb @@ -7,7 +7,7 @@ SimpleDB { num-values = 3 // number of material property values value-names = density vs vp // names of the material property values - value-units = kg/m**3 m/s m/s // units + value-units = kg/m**3 km/s km/s // units num-locs = 1 // number of locations data-dim = 0 space-dim = 3 @@ -21,6 +21,6 @@ SimpleDB { // (2) y coordinate (m) // (3) z coordinate (m) // (4) density (kg/m^3) -// (5) vs (m/s) -// (6) vp (m/s) -0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 +// (5) vs (km/s) +// (6) vp (km/s) +0.0 0.0 0.0 3400.0 4.5 8.0 diff --git a/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb index 526fab2c28..59e1f7cb9d 100644 --- a/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb @@ -7,7 +7,7 @@ SimpleDB { num-values = 3 // number of material property values value-names = density vs vp // names of the material property values - value-units = kg/m**3 m/s m/s // units + value-units = kg/m**3 km/s km/s // units num-locs = 1 // number of locations data-dim = 0 space-dim = 3 @@ -21,6 +21,6 @@ SimpleDB { // (2) y coordinate (m) // (3) z coordinate (m) // (4) density (kg/m^3) -// (5) vs (m/s) -// (6) vp (m/s) -0.0 0.0 0.0 2500.0 3000.0 5291.502622129181 +// (5) vs (km/s) +// (6) vp (km/s) +0.0 0.0 0.0 2400.0 3.5 6.2 From 092620612b5188c8645e9a351f789610824577ad Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 13 Jun 2017 17:07:02 -0700 Subject: [PATCH 020/216] Add Python script for plotting material properties. --- examples/3d/subduction/plot_matprops.py | 83 +++++++++++++++++++++++++ 1 file changed, 83 insertions(+) create mode 100644 examples/3d/subduction/plot_matprops.py diff --git a/examples/3d/subduction/plot_matprops.py b/examples/3d/subduction/plot_matprops.py new file mode 100644 index 0000000000..ac13915b90 --- /dev/null +++ b/examples/3d/subduction/plot_matprops.py @@ -0,0 +1,83 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the domain, colored by material properties. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters + +# Root name for simulation. +SIM_NAME = "step01" + +# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) +DATA_FORMAT = "hdf5" + +# Material property and materials to plot. +INFO_FIELD = "mu" +MATERIALS = ["crust", "mantle", "wedge", "slab"] + +# ---------------------------------------------------------------------- +# We create sources, filters, etc using the servermanager so that we can set the +# name of the proxy shown in the pipeline using Register(registrationName=NAME). + +from paraview.simple import * +# Disable automatic camera reset on "Show" +paraview.simple._DisableFirstRenderCameraReset() + + +dataAll = [] +for material in MATERIALS: + + # Read data + if DATA_FORMAT.lower() == "vtk": + pass + elif DATA_FORMAT.lower() == "hdf5": + dataMaterial = servermanager.sources.XDMFReader(FileNames=["output/%s-%s_info.xmf" % (SIM_NAME, material)]) + else: + raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) + servermanager.Register(dataMaterial, registrationName="%s-%s" % (SIM_NAME, material)) + dataAll.append(dataMaterial) + +view = GetActiveViewOrCreate('RenderView') + +groupMaterials = GroupDatasets(Input=dataAll) + +# Show domain, colored by magnitude of displacement vector. +materialDisplay = Show(groupMaterials, view) +ColorBy(materialDisplay, ("CELLS", INFO_FIELD)) +materialDisplay.RescaleTransferFunctionToDataRange(True) +materialDisplay.SetScalarBarVisibility(view, True) +materialDisplay.SetRepresentationType("Surface With Edges") + +# Rescale color and/or opacity maps used to exactly fit the current data range +materialLUT = GetColorTransferFunction(INFO_FIELD) +materialDisplay.RescaleTransferFunctionToDataRange(False, False) +# Update scalar bar component title. +UpdateScalarBarsComponentTitle(materialLUT, materialDisplay) + + +view.ResetCamera() + +Render() + +# Uncomment if running from shell outside ParaView. +#Interact() + + +# End of file From cd6047f5f17ae93ba917a0a096ba7d80e0b24c85 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 14 Jun 2017 17:46:57 +1200 Subject: [PATCH 021/216] Added simple Python script and .cfg file to create spatial and temporal databases for SSE problem. Parameters still need adjusting. --- examples/3d/subduction/synth_sse.cfg | 27 +++ examples/3d/subduction/synth_sse.py | 253 +++++++++++++++++++++++++++ 2 files changed, 280 insertions(+) create mode 100644 examples/3d/subduction/synth_sse.cfg create mode 100755 examples/3d/subduction/synth_sse.py diff --git a/examples/3d/subduction/synth_sse.cfg b/examples/3d/subduction/synth_sse.cfg new file mode 100644 index 0000000000..69e4d3554a --- /dev/null +++ b/examples/3d/subduction/synth_sse.cfg @@ -0,0 +1,27 @@ +[synth_sse] +rake = 45.0 +slip_center = [-122.6765, 45.5231] +slip_radius = 0.5 +slip_max = 5.0 +slip_sigma_lon = 0.2 +slip_sigma_lat = 0.2 + +slip_times = [0.0, 0.2, 0.4, 0.6, 0.8, 1.0] +slip_amplitudes = [0.0, 0.2, 0.5, 0.8, 0.9, 1.0] + +grid_lon_range = [-123.0, -122.0] +grid_lat_range = [45.0, 46.0] +grid_incr = 0.04 + +time_db_filename = spatialdb/sse_slip.timedb + +coordsys = spatialdata.geocoords.CSGeo +iohandler = spatialdata.spatialdb.SimpleGridAscii + +[synth_sse.coordsys] +space_dim = 3 +datum_horiz = WGS84 +datum_vert = mean sea level + +[synth_sse.iohandler] +filename = spatialdb/sse_slip.spatialdb diff --git a/examples/3d/subduction/synth_sse.py b/examples/3d/subduction/synth_sse.py new file mode 100755 index 0000000000..35ae260974 --- /dev/null +++ b/examples/3d/subduction/synth_sse.py @@ -0,0 +1,253 @@ +#!/usr/bin/env python + +## @file synth_sse.py + +## @brief Python application to create spatial databases for a synthetic +## SSE with time-varying circular slip. + +# import pdb +import math +import numpy +from spatialdata.spatialdb.SimpleGridDB import SimpleGridDB +from spatialdata.spatialdb.SimpleGridAscii import SimpleGridAscii +from spatialdata.spatialdb import TimeHistoryIO +from spatialdata.geocoords.CSGeo import CSGeo +from spatialdata.geocoords.CoordSys import CoordSys +from spatialdata.geocoords.CSGeoProj import CSGeoProj +from spatialdata.geocoords.Converter import convert + + +from pyre.applications.Script import Script as Application + +class SynthSse(Application): + """ + Python application to create spatial databases for a synthetic + SSE with time-varying Gaussian slip. + """ + + import pyre.inventory + ## Python object for managing SynthSse facilities and properties. + ## + ## \b Properties + ## @li \b rake Rake of fault slip (degrees). + ## @li \b slip_center (lon,lat) coordinates of slip center. + ## @li \b slip_radius Radius of slip region (degrees). + ## @li \b slip_max Maximum slip value (meters). + ## @li \b slip_sigma_lon Sigma value for longitude. + ## @li \b slip_sigma_lat Sigma value for latitude. + ## @li \b slip_times List of times for which to provide amplitudes. + ## @li \b slip_time_units Units used for slip times. + ## @li \b slip_amplitudes List of slip amplitudes. + ## @li \b grid_lon_range Min and max longitude values for grid. + ## @li \b grid_lat_range Min and max latitude values for grid. + ## @li \b grid_incr Grid increment (degrees) for spatial database. + ## @li \b time_db_filename Name of temporal DB output file. + ## + ## \b Facilities + ## @li \b coordsys Coordinate system for output database. + ## @li \b iohandler Object for writing spatial database. + + rake = pyre.inventory.float("rake", default=1.0) + rake.meta['tip'] = "Rake of fault slip (degrees)." + + slipCenter = pyre.inventory.list("slip_center", default=[0.0, 0.0]) + slipCenter.meta['tip'] = "(lon,lat) coordinates of slip center." + + slipRadius = pyre.inventory.float("slip_radius", default=1.0) + slipRadius.meta['tip'] = "Radius of slip region (degrees)." + + slipMax = pyre.inventory.float("slip_max", default=5.0) + slipMax.meta['tip'] = "Maximum slip value (meters)." + + slipSigmaLon = pyre.inventory.float("slip_sigma_lon", default=0.2) + slipSigmaLon.meta['tip'] = "Sigma value for longitude." + + slipSigmaLat = pyre.inventory.float("slip_sigma_lat", default=0.2) + slipSigmaLat.meta['tip'] = "Sigma value for latitude." + + slipTimes = pyre.inventory.list("slip_times", default=[0.0, 0.5, 1.0]) + slipTimes.meta['tip'] = "List of times for which to provide amplitudes." + + slipTimeUnits = pyre.inventory.str("slip_time_units", default="year") + slipTimeUnits.meta['tip'] = "Units used for slip times." + + slipAmplitudes = pyre.inventory.list("slip_amplitudes", + default=[0.0, 0.5, 1.0]) + slipAmplitudes.meta['tip'] = "List of slip amplitudes." + + gridLonRange = pyre.inventory.list("grid_lon_range", default=[-123.0, -124.0]) + gridLonRange.meta['tip'] = "Min and max longitude values for grid." + + gridLatRange = pyre.inventory.list("grid_lat_range", default=[45.0, 46.0]) + gridLatRange.meta['tip'] = "Min and max latitude values for grid." + + gridIncr = pyre.inventory.float("grid_incr", default=0.05) + gridIncr.meta['tip'] = "Sigma value for latitude." + + timeDbFilename = pyre.inventory.str("time_db_filename", default="slip.timedb") + timeDbFilename.meta['tip'] = "Filename of temporal DB output file." + + coordsys = pyre.inventory.facility("coordsys", + family="coordsys", + factory=CSGeo) + coordsys.meta['tip'] = "Coordinate system for output database." + + iohandler = pyre.inventory.facility("iohandler", family="simplegrid_io", + factory=SimpleGridAscii) + iohandler.meta['tip'] = "Object for writing spatial database." + + + # PUBLIC METHODS ///////////////////////////////////////////////////// + + def __init__(self, name="synth_sse"): + Application.__init__(self, name) + + self.lon = None + self.lat = None + self.z = None + self.grid = None + self.faultSlip = None + + return + + + def main(self): + # pdb.set_trace() + self.coordsys._configure() + self.coordsys.initialize() + + self._makeGrid() + self._computeGauss() + self._writeSpatialdb() + self._writeTemporaldb() + + return + + + # PRIVATE METHODS ///////////////////////////////////////////////////// + + + def _configure(self): + """ + Setup members using inventory. + """ + Application._configure(self) + + return + + + def _makeGrid(self): + """ + Function to create a mesh grid for computations. + """ + + lonMin = float(self.gridLonRange[0]) + lonMax = float(self.gridLonRange[1]) + latMin = float(self.gridLatRange[0]) + latMax = float(self.gridLatRange[1]) + + lonDiff = lonMax - lonMin + latDiff = latMax - latMin + numLon = int(round(lonDiff/self.gridIncr)) + 1 + numLat = int(round(latDiff/self.gridIncr)) + 1 + + self.lon = numpy.linspace(lonMin, lonMax, num=numLon, dtype=numpy.float64) + self.lat = numpy.linspace(latMin, latMax, num=numLat, dtype=numpy.float64) + self.z = numpy.zeros(1, dtype=numpy.float64) + + lonGrid, latGrid = numpy.meshgrid(self.lon, self.lat) + zGrid = numpy.zeros_like(lonGrid) + self.grid = numpy.column_stack((lonGrid.flatten(), latGrid.flatten(), + zGrid.flatten())) + + return + + + def _computeGauss(self): + """ + Function to compute 2D Gaussian slip distribution. + """ + + lonShift = self.grid[:,0] - float(self.slipCenter[0]) + latShift = self.grid[:,1] - float(self.slipCenter[1]) + + distance = numpy.sqrt(lonShift * lonShift + latShift * latShift) + outside = numpy.where(distance > self.slipRadius) + + lonFac = 0.5 * lonShift * lonShift/(self.slipSigmaLon * self.slipSigmaLon) + latFac = 0.5 * latShift * latShift/(self.slipSigmaLat * self.slipSigmaLat) + + slip = self.slipMax * numpy.exp(-(lonFac + latFac)) + slip[outside] = 0.0 + + rakeRadians = math.radians(self.rake) + llComp = math.cos(rakeRadians) + udComp = math.sin(rakeRadians) + + llSlip = llComp * slip + udSlip = udComp * slip + opSlip = numpy.zeros_like(llSlip) + + self.faultSlip = numpy.column_stack((llSlip, udSlip, opSlip)) + + return + + + def _writeSpatialdb(self): + """ + Write spatial database with fault slip. + """ + + print "Writing spatial database:" + + llSlipInfo = {'name': "left-lateral-slip", + 'units': "m", + 'data': self.faultSlip[:,0]} + + udSlipInfo = {'name': "reverse-slip", + 'units': "m", + 'data': self.faultSlip[:,1]} + + openInfo = {'name': "fault-opening", + 'units': "m", + 'data': self.faultSlip[:,2]} + + data = {'num-x': self.lon.shape[0], + 'num-y': self.lat.shape[0], + 'num-z': 1, + 'points': self.grid, + 'x': self.lon, + 'y': self.lat, + 'z': self.z, + 'coordsys': self.coordsys, + 'data_dim': 2, + 'values': [llSlipInfo, udSlipInfo, openInfo]} + + self.iohandler.write(data) + + return + + + def _writeTemporaldb(self): + """ + Write temporal database with time variation of fault slip. + """ + + time = [float(i) for i in self.slipTimes] + timeArr = numpy.array(time, dtype=numpy.float64) + + amplitude = [float(i) for i in self.slipAmplitudes] + amplitudeArr = numpy.array(amplitude, dtype=numpy.float64) + + TimeHistoryIO.write(timeArr, amplitudeArr, self.slipTimeUnits, + self.timeDbFilename) + + return + + +# ---------------------------------------------------------------------- +if __name__ == '__main__': + app = SynthSse() + app.run() + +# End of file From b3a049464198d7395fe1e6c1e5a04ed23989bc81 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 14 Jun 2017 17:50:06 +1200 Subject: [PATCH 022/216] Removed imports that weren't needed. --- examples/3d/subduction/synth_sse.py | 4 ---- 1 file changed, 4 deletions(-) diff --git a/examples/3d/subduction/synth_sse.py b/examples/3d/subduction/synth_sse.py index 35ae260974..288e521b3c 100755 --- a/examples/3d/subduction/synth_sse.py +++ b/examples/3d/subduction/synth_sse.py @@ -12,10 +12,6 @@ from spatialdata.spatialdb.SimpleGridAscii import SimpleGridAscii from spatialdata.spatialdb import TimeHistoryIO from spatialdata.geocoords.CSGeo import CSGeo -from spatialdata.geocoords.CoordSys import CoordSys -from spatialdata.geocoords.CSGeoProj import CSGeoProj -from spatialdata.geocoords.Converter import convert - from pyre.applications.Script import Script as Application From 13597a5d893fd7d2cc08eb8a5cdef25789583b80 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 14:05:19 -0700 Subject: [PATCH 023/216] Added step02. --- examples/3d/subduction/plot_faultslip.py | 80 ++++++++ examples/3d/subduction/solver_fieldsplit.cfg | 45 ++++ examples/3d/subduction/step02.cfg | 205 +++++++++++++++++++ 3 files changed, 330 insertions(+) create mode 100644 examples/3d/subduction/plot_faultslip.py create mode 100644 examples/3d/subduction/solver_fieldsplit.cfg create mode 100644 examples/3d/subduction/step02.cfg diff --git a/examples/3d/subduction/plot_faultslip.py b/examples/3d/subduction/plot_faultslip.py new file mode 100644 index 0000000000..3f23f54a0a --- /dev/null +++ b/examples/3d/subduction/plot_faultslip.py @@ -0,0 +1,80 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the fault +# surfaces, colored by the magnitude of fault slip. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters + +# Root name for simulation. +SIM_NAME = "step02" + +# Names of faults for output files. +FAULTS = ["fault-slab"] + +# ---------------------------------------------------------------------- +from paraview.simple import * +# Disable automatic camera reset on "Show" +paraview.simple._DisableFirstRenderCameraReset() + +# Read domain data +dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) +RenameSource("%s-domain" % SIM_NAME, dataDomain) + +scene = GetAnimationScene() +scene.UpdateAnimationUsingDataTimeSteps() +view = GetActiveViewOrCreate('RenderView') + +# Gray wireframe for undeformed domain. +domainDisplay = Show(dataDomain, view) +domainDisplay.Representation = 'Wireframe' +domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + +# Read fault data +dataFaults = [] +for fault in FAULTS: + data = XDMFReader(FileNames=["output/%s-%s.xmf" % (SIM_NAME, fault)]) + RenameSource("%s-%s" % (SIM_NAME, fault), data) + dataFaults.append(data) + +groupFaults = GroupDatasets(Input=dataFaults) + +faultDisplay = Show(groupFaults, view) +ColorBy(faultDisplay, ('POINTS', 'slip', 'Magnitude')) +faultDisplay.RescaleTransferFunctionToDataRange(True) +faultDisplay.SetScalarBarVisibility(view, True) +faultDisplay.SetRepresentationType('Surface With Edges') + +# Rescale color and/or opacity maps used to exactly fit the current data range +slipLUT = GetColorTransferFunction('slip') +faultDisplay.RescaleTransferFunctionToDataRange(False, False) +# Update a scalar bar component title. +UpdateScalarBarsComponentTitle(slipLUT, faultDisplay) + +view.ResetCamera() +view.Update() + +Render() + +# Uncomment if running from shell outside ParaView. +#Interact() + + +# End of file diff --git a/examples/3d/subduction/solver_fieldsplit.cfg b/examples/3d/subduction/solver_fieldsplit.cfg new file mode 100644 index 0000000000..bf14ee0a2c --- /dev/null +++ b/examples/3d/subduction/solver_fieldsplit.cfg @@ -0,0 +1,45 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# This file provides an optimized solver, the analogue of LU factorization, for the +# saddle point system arising from problems with a fault. This should be used for +# large production runs. + +[pylithapp.problem.formulation] +# The split_fields flag must be specified, so that the PCFIELDSPLIT preconditioner +# can be used. The matrix_type must be set to aij since we lose symmetry when +# splitting. We have turned on the custom preconditioner for the fault problem. +# +split_fields = True +matrix_type = aij +use_custom_constraint_pc = True + +[pylithapp.petsc] +# The displacements are solved with algebraic multigrid (ML), and +# the fault tractions with a standard Krylov method since we do not +# explicitly form the Schur complement matrix. +# +#snes_view = true +#ksp_monitor_true_residual = true +fs_pc_type = fieldsplit +fs_pc_use_amat = +fs_pc_fieldsplit_type = multiplicative +fs_fieldsplit_displacement_pc_type = ml +fs_fieldsplit_lagrange_multiplier_pc_type = jacobi +fs_fieldsplit_displacement_ksp_type = preonly +fs_fieldsplit_lagrange_multiplier_ksp_type = preonly + + +# End of file diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg new file mode 100644 index 0000000000..4e80a5c236 --- /dev/null +++ b/examples/3d/subduction/step02.cfg @@ -0,0 +1,205 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is a viscoelastic quasistatic problem using Dirichlet +# (displacement) boundary conditions and prescribed fault slip. We +# prescribe uniform fault slip on the slab fault rupture patch with +# zero displacement on the lateral and bottom boundaries. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# This is not a self-contained simulation configuration file. This +# file only specifies parameters specific to tutorial step02. +# The general parameters are specified in the pylithapp.cfg +# file which PyLith reads by default. +# +# To run the simulation: +# pylith step02.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# Permit uknown components so that we can ignore warnings. +[pylithapp] +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 200.0*year +dt = 10.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveKin + +[pylithapp.problem.interfaces.slab] +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.UniformDB +slip.label = Final slip +slip.values = [left-lateral-slip, reverse-slip, fault-opening] +slip.data = [-1.0*m, 4.0*m, 0.0*m] + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [9.999*year] + +[pylithapp.problem.interfaces.slab.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step02-fault-slab.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We change the mantle and slab to linear Maxwell viscoelastic +# materials with depth-dependent viscosities using a CompositeDB. The +# CompsiteDB allows us to combine the density, Vp, and Vs from the +# SimpleDB from Step01 with a viscosity from a SimpleGridDB into a +# single (composite) spatial database. +[pylithapp.problem.materials] +slab = pylith.materials.MaxwellIsotropic3D +mantle = pylith.materials.MaxwellIsotropic3D + +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.mantle.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output ------------------------------------------ +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step02-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step02-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step02-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step02-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step02-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step02-mantle.h5 + + +# End of file From 8958b42d287bf838e3d0fdd1741b18a4199f7ae2 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 14:05:50 -0700 Subject: [PATCH 024/216] Improve Python ParaView scripts, use RenameSource. --- examples/3d/subduction/README | 14 +++++++------- examples/3d/subduction/plot_dispvec.py | 21 ++++++--------------- examples/3d/subduction/plot_dispwarp.py | 22 +++++++--------------- examples/3d/subduction/plot_matprops.py | 21 ++++----------------- 4 files changed, 24 insertions(+), 54 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index a328554c61..277f1abc12 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -16,8 +16,8 @@ https://pubs.usgs.gov/of/2007/1348/. Features: Spatial databases - + SimpleDB - + UniformDB + + SimpleDB [1] + + UniformDB [1] + SimpleGridDB + CompositeDB @@ -25,25 +25,25 @@ Features: - Depth profile with SimpleGridDB Dirichlet Boundary conditions - + Fixed displacement + + Fixed displacement [1] + Fixed velocity + Time history Materials - + Elastic + + Elastic [1] + Linear Maxwell viscoelastic + Powerlaw [exercise] Preconditioners - + LU + + LU [1] + AMG (ML) + AMG (ML) + custom preconditioner Uniform refinement [exercise] Output - + Output of solution - + Output of solution on ground surface + + Output of solution [1] + + Output of solution on ground surface [1] + Output of solution at points + Output of state variables diff --git a/examples/3d/subduction/plot_dispvec.py b/examples/3d/subduction/plot_dispvec.py index cb209267a9..35a60d0574 100644 --- a/examples/3d/subduction/plot_dispvec.py +++ b/examples/3d/subduction/plot_dispvec.py @@ -26,29 +26,21 @@ # Root name for simulation. SIM_NAME = "step01" -# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) -DATA_FORMAT = "hdf5" - # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 # ---------------------------------------------------------------------- -# We create sources, filters, etc using the servermanager so that we can set the -# name of the proxy shown in the pipeline using Register(registrationName=NAME). - from paraview.simple import * # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read data -if DATA_FORMAT.lower() == "vtk": - dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) -elif DATA_FORMAT.lower() == "hdf5": - dataDomain = servermanager.sources.XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) -else: - raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) -servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) +dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) +RenameSource("%s-domain" % SIM_NAME, dataDomain) + +scene = GetAnimationScene() +scene.UpdateAnimationUsingDataTimeSteps() view = GetActiveViewOrCreate('RenderView') # Show undeformed domain, colored by magnitude of displacement vector. @@ -66,8 +58,7 @@ # Add arrows to show displacement vectors. -glyph = servermanager.filters.Glyph(Input=dataDomain, GlyphType="Arrow") -servermanager.Register(glyph, registrationName="%s-domain-glyph" % SIM_NAME) +glyph = Glyph(Input=dataDomain, GlyphType="Arrow") glyph.Vectors = ["POINTS", "displacement"] glyph.ScaleFactor = DISPLACEMENT_SCALE glyph.ScaleMode = "vector" diff --git a/examples/3d/subduction/plot_dispwarp.py b/examples/3d/subduction/plot_dispwarp.py index d67a989952..0fe341c51a 100644 --- a/examples/3d/subduction/plot_dispwarp.py +++ b/examples/3d/subduction/plot_dispwarp.py @@ -26,28 +26,20 @@ # Root name for simulation. SIM_NAME = "step01" -# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) -DATA_FORMAT = "hdf5" - # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 # ---------------------------------------------------------------------- -# We create sources, filters, etc using the servermanager so that we can set the -# name of the proxy shown in the pipeline using Register(registrationName=NAME). - from paraview.simple import * # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read data -if DATA_FORMAT.lower() == "vtk": - dataDomain = servermanager.sources.LegacyVTKReader(FileNames=['output/%s-domain_t0000000.vtk' % SIM_NAME]) -elif DATA_FORMAT.lower() == "hdf5": - dataDomain = servermanager.sources.XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) -else: - raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) -servermanager.Register(dataDomain, registrationName="%s-domain" % SIM_NAME) +dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) +RenameSource("%s-domain" % SIM_NAME, dataDomain) + +scene = GetAnimationScene() +scene.UpdateAnimationUsingDataTimeSteps() view = GetActiveViewOrCreate('RenderView') # Gray wireframe for undeformed domain. @@ -56,8 +48,7 @@ domainDisplay.AmbientColor = [0.5, 0.5, 0.5] # Warp domain to show deformation -warp = servermanager.filters.WarpByVector(Input=dataDomain) -servermanager.Register(warp, registrationName="%s-domain-warp" % SIM_NAME) +warp = WarpByVector(Input=dataDomain) warp.Vectors = ['POINTS', 'displacement'] warp.ScaleFactor = DISPLACEMENT_SCALE @@ -74,6 +65,7 @@ UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) view.ResetCamera() +view.Update() Render() diff --git a/examples/3d/subduction/plot_matprops.py b/examples/3d/subduction/plot_matprops.py index ac13915b90..87d0e11bfb 100644 --- a/examples/3d/subduction/plot_matprops.py +++ b/examples/3d/subduction/plot_matprops.py @@ -25,39 +25,26 @@ # Root name for simulation. SIM_NAME = "step01" -# Format of simulation output (choices=["vtk", "hdf5"], case insentitive) -DATA_FORMAT = "hdf5" - # Material property and materials to plot. INFO_FIELD = "mu" MATERIALS = ["crust", "mantle", "wedge", "slab"] # ---------------------------------------------------------------------- -# We create sources, filters, etc using the servermanager so that we can set the -# name of the proxy shown in the pipeline using Register(registrationName=NAME). - from paraview.simple import * # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() dataAll = [] +# Read data for material in MATERIALS: - - # Read data - if DATA_FORMAT.lower() == "vtk": - pass - elif DATA_FORMAT.lower() == "hdf5": - dataMaterial = servermanager.sources.XDMFReader(FileNames=["output/%s-%s_info.xmf" % (SIM_NAME, material)]) - else: - raise ValueError("Unknown file format '%s' when choosing reader in Python script." % DATA_FORMAT) - servermanager.Register(dataMaterial, registrationName="%s-%s" % (SIM_NAME, material)) + dataMaterial = XDMFReader(FileNames=["output/%s-%s_info.xmf" % (SIM_NAME, material)]) + RenameSource("%s-%s" % (SIM_NAME, material), dataMaterial) dataAll.append(dataMaterial) +groupMaterials = GroupDatasets(Input=dataAll) view = GetActiveViewOrCreate('RenderView') -groupMaterials = GroupDatasets(Input=dataAll) - # Show domain, colored by magnitude of displacement vector. materialDisplay = Show(groupMaterials, view) ColorBy(materialDisplay, ("CELLS", INFO_FIELD)) From 37b9ebe54d633ec94a9c3d5a72cfeb44b593349e Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 14:21:01 -0700 Subject: [PATCH 025/216] Move visualization files to viz directory. --- examples/3d/subduction/{ => viz}/plot_dispvec.py | 0 examples/3d/subduction/{ => viz}/plot_dispwarp.py | 0 examples/3d/subduction/{ => viz}/plot_faultslip.py | 0 examples/3d/subduction/{ => viz}/plot_matprops.py | 0 4 files changed, 0 insertions(+), 0 deletions(-) rename examples/3d/subduction/{ => viz}/plot_dispvec.py (100%) rename examples/3d/subduction/{ => viz}/plot_dispwarp.py (100%) rename examples/3d/subduction/{ => viz}/plot_faultslip.py (100%) rename examples/3d/subduction/{ => viz}/plot_matprops.py (100%) diff --git a/examples/3d/subduction/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py similarity index 100% rename from examples/3d/subduction/plot_dispvec.py rename to examples/3d/subduction/viz/plot_dispvec.py diff --git a/examples/3d/subduction/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py similarity index 100% rename from examples/3d/subduction/plot_dispwarp.py rename to examples/3d/subduction/viz/plot_dispwarp.py diff --git a/examples/3d/subduction/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py similarity index 100% rename from examples/3d/subduction/plot_faultslip.py rename to examples/3d/subduction/viz/plot_faultslip.py diff --git a/examples/3d/subduction/plot_matprops.py b/examples/3d/subduction/viz/plot_matprops.py similarity index 100% rename from examples/3d/subduction/plot_matprops.py rename to examples/3d/subduction/viz/plot_matprops.py From 90c7419899810acbb400cf166d8bb253cd95591a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 14:31:22 -0700 Subject: [PATCH 026/216] Added missing viscosity file. --- .../spatialdb/mat_viscosity.spatialdb | 29 +++++++++++++++++++ 1 file changed, 29 insertions(+) create mode 100644 examples/3d/subduction/spatialdb/mat_viscosity.spatialdb diff --git a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb new file mode 100644 index 0000000000..d978671c3a --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb @@ -0,0 +1,29 @@ +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 1 + num-z = 4 + num-values = 1 + space-dim = 3 + value-names = viscosity + value-units = Pa*s + cs-data = cartesian { + space-dim = 3 + to-meters = 1.0e+3 + } +} + +// x coordinate +0.0 + +// y coordinate +0.0 + +// z coordinates +0.0 -50.0 -100.0 -400.0 + +// z viscosity +0.0 0.0 0.0 1.0e+22 +0.0 0.0 -50.0 8.0e+21 +0.0 0.0 -100.0 2.0e+20 +0.0 0.0 -400.0 1.0e+20 From d3d63ce2a75a515d5be2ab642ba201cb9c41b575 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 15 Jun 2017 10:21:17 +1200 Subject: [PATCH 027/216] Moved files to create coastline to viz subdirectory. --- examples/3d/subduction/{ => viz}/get_coast.sh | 0 examples/3d/subduction/{ => viz}/seg2vtk.py | 0 2 files changed, 0 insertions(+), 0 deletions(-) rename examples/3d/subduction/{ => viz}/get_coast.sh (100%) rename examples/3d/subduction/{ => viz}/seg2vtk.py (100%) diff --git a/examples/3d/subduction/get_coast.sh b/examples/3d/subduction/viz/get_coast.sh similarity index 100% rename from examples/3d/subduction/get_coast.sh rename to examples/3d/subduction/viz/get_coast.sh diff --git a/examples/3d/subduction/seg2vtk.py b/examples/3d/subduction/viz/seg2vtk.py similarity index 100% rename from examples/3d/subduction/seg2vtk.py rename to examples/3d/subduction/viz/seg2vtk.py From 4da454652d3dad398888182bab626f41c38747f6 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 15 Jun 2017 10:25:17 +1200 Subject: [PATCH 028/216] Reduced resolution to low, and included coastline VTK file. --- examples/3d/subduction/viz/cascadia_tm.vtk | 1371 ++++++++++++++++++++ examples/3d/subduction/viz/get_coast.sh | 2 +- 2 files changed, 1372 insertions(+), 1 deletion(-) create mode 100644 examples/3d/subduction/viz/cascadia_tm.vtk diff --git a/examples/3d/subduction/viz/cascadia_tm.vtk b/examples/3d/subduction/viz/cascadia_tm.vtk new file mode 100644 index 0000000000..76c3207de1 --- /dev/null +++ b/examples/3d/subduction/viz/cascadia_tm.vtk @@ -0,0 +1,1371 @@ +# vtk DataFile Version 2.0 +Coastline segments. +ASCII +DATASET POLYDATA +POINTS 1158 double +-90946.0500000000 498339.4400000000 0.1000000000 +-92871.1100000000 497082.7400000000 0.1000000000 +-85466.7700000000 489357.3800000000 0.1000000000 +-91492.2600000000 473233.8200000000 0.1000000000 +-83623.0500000000 463332.5000000000 0.1000000000 +-74961.7100000000 474268.7100000000 0.1000000000 +-81569.0400000000 456429.1600000000 0.1000000000 +-61279.5800000000 465018.8900000000 0.1000000000 +-80490.9100000000 454054.5600000000 0.1000000000 +-78182.7600000000 440446.9900000000 0.1000000000 +-88026.5100000000 467406.8400000000 0.1000000000 +-96297.5200000000 471230.0700000000 0.1000000000 +-100877.3500000000 458484.3900000000 0.1000000000 +-93607.7000000000 444168.2600000000 0.1000000000 +-61225.5400000000 429575.9100000000 0.1000000000 +-59005.4100000000 444379.6300000000 0.1000000000 +-35651.9400000000 463534.1300000000 0.1000000000 +-44993.5500000000 427705.0800000000 0.1000000000 +-25787.3600000000 419896.3400000000 0.1000000000 +-42843.1000000000 416491.2300000000 0.1000000000 +-34702.9700000000 409936.6200000000 0.1000000000 +-43142.5600000000 409436.4000000000 0.1000000000 +-34780.7900000000 406408.6200000000 0.1000000000 +-37944.7300000000 400746.5700000000 0.1000000000 +-29113.3800000000 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1027 1028 1029 1030 1031 + 8 1032 1033 1034 1035 1036 1037 1038 1039 + 4 1040 1041 1042 1043 + 4 1044 1045 1046 1047 + 31 1048 1049 1050 1051 1052 1053 1054 1055 1056 1057 1058 1059 1060 1061 1062 1063 1064 1065 1066 1067 1068 1069 1070 1071 1072 1073 1074 1075 1076 1077 1078 + 31 1079 1080 1081 1082 1083 1084 1085 1086 1087 1088 1089 1090 1091 1092 1093 1094 1095 1096 1097 1098 1099 1100 1101 1102 1103 1104 1105 1106 1107 1108 1109 + 4 1110 1111 1112 1113 + 4 1114 1115 1116 1117 + 12 1118 1119 1120 1121 1122 1123 1124 1125 1126 1127 1128 1129 + 12 1130 1131 1132 1133 1134 1135 1136 1137 1138 1139 1140 1141 + 3 1142 1143 1144 + 3 1145 1146 1147 + 2 1148 1149 + 2 1150 1151 + 2 1152 1153 + 2 1154 1155 + 2 1156 1157 diff --git a/examples/3d/subduction/viz/get_coast.sh b/examples/3d/subduction/viz/get_coast.sh index 77d0811b22..1462645cf3 100755 --- a/examples/3d/subduction/viz/get_coast.sh +++ b/examples/3d/subduction/viz/get_coast.sh @@ -13,7 +13,7 @@ vtktm="cascadia_tm.vtk" region="-R-129/-117/41/50" # Resolution: (f)ull, (h)igh, (i)ntermediate, (l)ow, or (c)rude. -reso="-Dh" +reso="-Dl" # Draw rivers option. # rivers="-Ia" From 300c4dbf2d59f278f955b50cdb203251fcdecbec Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 16:48:24 -0700 Subject: [PATCH 029/216] Add note. --- examples/3d/subduction/README | 4 ++++ 1 file changed, 4 insertions(+) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 277f1abc12..479c581c97 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -1,6 +1,10 @@ +TODO + Set coordinate system to projected geographic coordinate system. + Directory structure: mesh (mesh related files) spatialdb (spatial database related files) + viz Elastic properties loosely based on From d033e447cb31867c448a70db87cd4f9cd223fdec Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 16:48:35 -0700 Subject: [PATCH 030/216] Relaxed ksp_atol. --- examples/3d/subduction/pylithapp.cfg | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 7cf0bed62b..798c618c4f 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -131,7 +131,7 @@ pc_type = lu # Convergence parameters. ksp_rtol = 1.0e-10 -ksp_atol = 1.0e-20 +ksp_atol = 1.0e-11 ksp_max_it = 500 ksp_gmres_restart = 50 From ae59907b8b8007623c02394123a23debd3fb2c08 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 16:48:48 -0700 Subject: [PATCH 031/216] Added comments to viscosity spatial database. --- .../3d/subduction/spatialdb/mat_viscosity.spatialdb | 10 ++++++++++ 1 file changed, 10 insertions(+) diff --git a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb index d978671c3a..8ba7c26ab4 100644 --- a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb @@ -1,3 +1,13 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies a depth distribution of viscosity. +// +// The rough variation of Maxwell relaxation time with depth is +// 0 km: 10,000 years (essentially elastic) +// -50 km: 5,000 years (essentially elastic) +// -100 km: 100 years +// -400 km: 50 years +// #SPATIAL_GRID.ascii 1 SimpleGridDB { num-x = 1 From 3ea05d924cdec4c30448927822f3a188f323ab2a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 16:49:10 -0700 Subject: [PATCH 032/216] Set filename for progress and parameter output files. --- examples/3d/subduction/step01.cfg | 14 ++++++++++---- examples/3d/subduction/step02.cfg | 30 +++++++++++++++++++++--------- 2 files changed, 31 insertions(+), 13 deletions(-) diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index 92263e3af8..e6b603d0bb 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -30,16 +30,22 @@ # RUNNING THE SIMULATON # ---------------------------------------------------------------------- # -# This is not a self-contained simulation configuration file. This -# file only specifies parameters specific to tutorial step01. -# The general parameters are specified in the pylithapp.cfg -# file which PyLith reads by default. +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step01.cfg (main parameter file for step01) # # To run the simulation: # pylith step01.cfg # # Output will be directed to the "output" directory.. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step01-parameters.json +problem.progress_monitor.filename = output/step01-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index 4e80a5c236..cd8db31365 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -16,27 +16,39 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is a viscoelastic quasistatic problem using Dirichlet -# (displacement) boundary conditions and prescribed fault slip. We -# prescribe uniform fault slip on the slab fault rupture patch with -# zero displacement on the lateral and bottom boundaries. +# This problem focuses on viscoelastic relaxation from coseismic slip +# on a patch in the middle of the top of the slab. We prescribe +# uniform fault slip on the slab fault rupture patch with zero +# displacement on the lateral and bottom boundaries. # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- # -# This is not a self-contained simulation configuration file. This -# file only specifies parameters specific to tutorial step02. -# The general parameters are specified in the pylithapp.cfg -# file which PyLith reads by default. +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step02.cfg (main parameter file for step02) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. # # To run the simulation: # pylith step02.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. -# Permit uknown components so that we can ignore warnings. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- [pylithapp] +dump_parameters.filename = output/step02-parameters.json +problem.progress_monitor.filename = output/step02-progress.txt + +# Permit unknown components so that we can override components and +# ignore warnings. typos = strict # ---------------------------------------------------------------------- From 9c679fd8a70ea2f67b4ad8c0d36dd935c3c872d4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 16:49:25 -0700 Subject: [PATCH 033/216] Added step03. --- .../spatialdb/fault_slabtop_creep.spatialdb | 43 +++ examples/3d/subduction/step03.cfg | 254 ++++++++++++++++++ 2 files changed, 297 insertions(+) create mode 100644 examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb create mode 100644 examples/3d/subduction/step03.cfg diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb new file mode 100644 index 0000000000..6e34b09eda --- /dev/null +++ b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb @@ -0,0 +1,43 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify a uniform creep rate below a depth of 50 km, tapering to +// 0 at a depth of 30 km. +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 1 + num-z = 4 + num-values = 3 + value-names = left-lateral-slip reverse-slip fault-opening + value-units = cm/year cm/year cm/year + space-dim = 3 + cs-data = cartesian { + to-meters = 1.0e+3 // Specify coordinates in km for convenience. + space-dim = 3 + } // cs-data +} // SimpleDB +// x coordinate +0.0 + +// y coordinate +0.0 + +// z coordinate +99.0 -30.0 -50.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) left-laterial-slip (cm/yr) +// (5) reverse-slip (cm/yr) +// (6) fault-opening (cm/yr) +0.0 0.0 99.0 0.0 0.0 0.0 +0.0 0.0 -30.0 0.0 0.0 0.0 +0.0 0.0 -50.0 -2.0 +4.0 0.0 +0.0 0.0 -999.0 -2.0 +4.0 0.0 diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg new file mode 100644 index 0000000000..e718e32d84 --- /dev/null +++ b/examples/3d/subduction/step03.cfg @@ -0,0 +1,254 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This problem focuses on interseismic deformation with viscoelastic +# relaxation combined with aseismic slip. We use both Dirichlet +# boundary conditions to constrain the displacements on the lateral +# and bottom boundaries. The subducting slab uses prescribed slip with +# a constant slip rate time function. +# +# We use the same material properties as step02. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step03.cfg (main parameter file for step03) +# - solver_fieldsplit.cfg (field split solver settings) +# +# To run the simulation: +# pylith step03.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step03-parameters.json +problem.progress_monitor.filename = output/step03-progress.txt + +# Permit unknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 200.0*year +dt = 10.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. Because the +# slab intersects the boundaries of the domain, and PyLith does not +# permit overlap between the fault interfaces and Dirichlet boundary +# conditions, for the Dirichlet boundary conditions we use the +# nodesets which exclude vertices on the fault. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg_nofault +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg_nofault +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos_nofault +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab_top, slab_bottom] + +[pylithapp.problem.interfaces] +slab_top = pylith.faults.FaultCohesiveKin +slab_bottom = pylith.faults.FaultCohesiveKin + +# Slab top ------------------------------------------------------------- +[pylithapp.problem.interfaces.slab_top] +id = 100 +label = fault_slabtop +edge = fault_slabtop_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_top.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.SimpleGridDB +slip_rate.label = Slab top slip rate. +slip_rate.filename = spatialdb/fault_slabtop_creep.spatialdb +slip_rate.query_type = linear + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +[pylithapp.problem.interfaces.slab_top.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step03-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# Slab bottom ---------------------------------------------------------- +[pylithapp.problem.interfaces.slab_bottom] +id = 101 +label = fault_slabbot +edge = fault_slabbot_edge +up_dir = [+0.1,0,1] + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slab bottom slip rate. +slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] +slip_rate.data = [+2.0*cm/year, -4.0*cm/year, 0.0*cm/year] + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +[pylithapp.problem.interfaces.slab_bottom.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step03-fault-slabbot.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We use the same material properties as step02, with linear Maxwell +# viscoelastic models for the mantle and slab. +[pylithapp.problem.materials] +slab = pylith.materials.MaxwellIsotropic3D +mantle = pylith.materials.MaxwellIsotropic3D + +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.mantle.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output ------------------------------------------ +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step03-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step03-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step03-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step03-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step03-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step03-mantle.h5 + + +# End of file From 561db2c1f4e5281101ed86cca952d3551e3f28c5 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 21:11:34 -0700 Subject: [PATCH 034/216] Fixed fault orientation and slip directions. --- .../3d/subduction/spatialdb/fault_slabtop_creep.spatialdb | 6 +++--- examples/3d/subduction/step03.cfg | 2 +- 2 files changed, 4 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb index 6e34b09eda..9918db10a3 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb @@ -28,7 +28,7 @@ SimpleGridDB { 0.0 // z coordinate -99.0 -30.0 -50.0 -999.0 +99.0 -45.0 -60.0 -999.0 // Columns are // (1) x coordinate (km) @@ -38,6 +38,6 @@ SimpleGridDB { // (5) reverse-slip (cm/yr) // (6) fault-opening (cm/yr) 0.0 0.0 99.0 0.0 0.0 0.0 -0.0 0.0 -30.0 0.0 0.0 0.0 -0.0 0.0 -50.0 -2.0 +4.0 0.0 +0.0 0.0 -45.0 0.0 0.0 0.0 +0.0 0.0 -60.0 -2.0 +4.0 0.0 0.0 0.0 -999.0 -2.0 +4.0 0.0 diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index e718e32d84..a1a30f24f5 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -154,7 +154,7 @@ vertex_info_fields = [normal_dir, strike_dir, dip_dir] id = 101 label = fault_slabbot edge = fault_slabbot_edge -up_dir = [+0.1,0,1] +up_dir = [-0.1,0,0.9] # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). From e28a5a89b98fd3c6c2b57423a1e21b0f29cc955c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 14 Jun 2017 21:14:12 -0700 Subject: [PATCH 035/216] Updated README. --- examples/3d/subduction/README | 26 +++++++++++++------------- 1 file changed, 13 insertions(+), 13 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 479c581c97..5929795405 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -21,33 +21,33 @@ Features: Spatial databases + SimpleDB [1] - + UniformDB [1] - + SimpleGridDB - + CompositeDB + + UniformDB [1,2,3] + + SimpleGridDB [2,3] + + CompositeDB [2,3] - Geographic coordinates with SimpleGridDB - - Depth profile with SimpleGridDB + - Depth profile with SimpleGridDB [2,3] Dirichlet Boundary conditions - + Fixed displacement [1] + + Fixed displacement [1,2,3] + Fixed velocity + Time history Materials - + Elastic [1] - + Linear Maxwell viscoelastic + + Elastic [1,2,3] + + Linear Maxwell viscoelastic [2,3] + Powerlaw [exercise] Preconditioners + LU [1] + AMG (ML) - + AMG (ML) + custom preconditioner + + AMG (ML) + custom preconditioner [2,3] Uniform refinement [exercise] Output - + Output of solution [1] - + Output of solution on ground surface [1] + + Output of solution [1,2,3] + + Output of solution on ground surface [1,2,3] + Output of solution at points + Output of state variables @@ -58,10 +58,10 @@ Features: Generation of spatial databases via Python Faults - + Buried edges + + Buried edges [2,3] + Intersecting - + Multiple faults - + Prescribed slip + + Multiple faults [3] + + Prescribed slip [2,3] + Prescribed slip w/multiple ruptures + Fault friction From d8d10866855b652c76d39ae63a21e7c76b3f9f2a Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 15 Jun 2017 17:05:53 +1200 Subject: [PATCH 036/216] Added files for step06 example and updated everything to use geoprojected coordinates. --- examples/3d/subduction/cgps_sites.txt | 41 ++++ examples/3d/subduction/pylithapp.cfg | 12 +- .../spatialdb/mat_crust_elastic.spatialdb | 16 +- .../spatialdb/mat_mantle_elastic.spatialdb | 16 +- .../spatialdb/mat_slab_elastic.spatialdb | 16 +- .../spatialdb/mat_viscosity.spatialdb | 16 +- .../spatialdb/mat_wedge_elastic.spatialdb | 16 +- examples/3d/subduction/step06.cfg | 212 ++++++++++++++++++ examples/3d/subduction/synth_sse.cfg | 16 +- examples/3d/subduction/viz/get_coast.sh | 4 +- 10 files changed, 339 insertions(+), 26 deletions(-) create mode 100644 examples/3d/subduction/cgps_sites.txt create mode 100644 examples/3d/subduction/step06.cfg diff --git a/examples/3d/subduction/cgps_sites.txt b/examples/3d/subduction/cgps_sites.txt new file mode 100644 index 0000000000..d60a287803 --- /dev/null +++ b/examples/3d/subduction/cgps_sites.txt @@ -0,0 +1,41 @@ +#Site X Y Z +s000 -121.612982 47.628687 -1.000000 +s001 -127.983489 44.365155 -1.000000 +s002 -127.749628 45.735429 -1.000000 +s003 -123.350223 46.129591 -1.000000 +s004 -124.722886 47.256591 -1.000000 +s005 -121.634109 47.461605 -1.000000 +s006 -119.890760 42.130634 -1.000000 +s007 -123.609386 45.133983 -1.000000 +s008 -123.989470 47.989057 -1.000000 +s009 -120.697530 44.556228 -1.000000 +s010 -127.218005 42.400906 -1.000000 +s011 -127.230149 48.346912 -1.000000 +s012 -123.107849 42.474276 -1.000000 +s013 -126.918171 45.114353 -1.000000 +s014 -123.113671 45.375199 -1.000000 +s015 -120.224643 44.503446 -1.000000 +s016 -123.265162 45.245698 -1.000000 +s017 -122.907728 45.528426 -1.000000 +s018 -120.072297 45.355367 -1.000000 +s019 -119.991950 45.271641 -1.000000 +s020 -119.883980 44.221339 -1.000000 +s021 -127.644257 47.561659 -1.000000 +s022 -124.718673 44.112431 -1.000000 +s023 -123.051358 42.060991 -1.000000 +s024 -124.097409 43.878245 -1.000000 +s025 -124.638054 46.705427 -1.000000 +s026 -127.885885 44.327479 -1.000000 +s027 -127.435121 47.243404 -1.000000 +s028 -121.607208 42.203630 -1.000000 +s029 -119.613277 44.077366 -1.000000 +s030 -122.754429 47.486098 -1.000000 +s031 -126.657327 43.880605 -1.000000 +s032 -121.108323 47.970235 -1.000000 +s033 -120.247282 44.706072 -1.000000 +s034 -120.238278 43.404986 -1.000000 +s035 -121.963700 45.975030 -1.000000 +s036 -123.738534 47.216044 -1.000000 +s037 -120.506943 44.778731 -1.000000 +s038 -125.929533 46.173138 -1.000000 +s039 -120.736087 44.841103 -1.000000 diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 7cf0bed62b..400568c0ca 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -35,6 +35,16 @@ reader.filename = mesh/mesh_tet.exo # Cuthill-KcKee algorithm. reorder_mesh = True +# Our mesh uses a local Transverse Mercator geographic projection, +# which must be specified. +[pylithapp.mesh_generator.reader] +coordsys = spatialdata.geocoords.CSGeoProj +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level +coordsys.projector.projection = tmerc +coordsys.projector.proj_options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + # ---------------------------------------------------------------------- # materials # ---------------------------------------------------------------------- @@ -155,4 +165,4 @@ snes_error_if_not_converged = true log_view = true -# End of file \ No newline at end of file +# End of file diff --git a/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb index 2af855ab9c..8fe010cd83 100644 --- a/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_crust_elastic.spatialdb @@ -11,9 +11,19 @@ SimpleDB { num-locs = 1 // number of locations data-dim = 0 space-dim = 3 - cs-data = cartesian { - to-meters = 1.0 - space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } } } // Columns are diff --git a/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb index a22038c63e..95a552b006 100644 --- a/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_mantle_elastic.spatialdb @@ -11,9 +11,19 @@ SimpleDB { num-locs = 1 // number of locations data-dim = 0 space-dim = 3 - cs-data = cartesian { - to-meters = 1.0 - space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } } } // Columns are diff --git a/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb index 98d4cff36c..956736a654 100644 --- a/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_slab_elastic.spatialdb @@ -11,9 +11,19 @@ SimpleDB { num-locs = 1 // number of locations data-dim = 0 space-dim = 3 - cs-data = cartesian { - to-meters = 1.0 - space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } } } // Columns are diff --git a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb index d978671c3a..f151d15e19 100644 --- a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb @@ -7,9 +7,19 @@ SimpleGridDB { space-dim = 3 value-names = viscosity value-units = Pa*s - cs-data = cartesian { - space-dim = 3 - to-meters = 1.0e+3 + cs-data = geo-projected { + to-meters = 1.0e3 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } } } diff --git a/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb index 59e1f7cb9d..135fa3b252 100644 --- a/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_wedge_elastic.spatialdb @@ -11,9 +11,19 @@ SimpleDB { num-locs = 1 // number of locations data-dim = 0 space-dim = 3 - cs-data = cartesian { - to-meters = 1.0 - space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } } } // Columns are diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg new file mode 100644 index 0000000000..c079e961d5 --- /dev/null +++ b/examples/3d/subduction/step06.cfg @@ -0,0 +1,212 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions and prescribed fault slip to +# simulate a slow slip event (SSE). The slip occurs over a time +# period of one year, with fault slip specified by both a spatialdb +# (to provide an approximately Gaussian slip distribution) and a +# temporal database to control the slip amplitude as a function of +# time. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# This is not a self-contained simulation configuration file. This +# file only specifies parameters specific to tutorial step06. +# The general parameters are specified in the pylithapp.cfg +# file which PyLith reads by default. +# +# To run the simulation: +# pylith step06.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# Permit uknown components so that we can ignore warnings. +[pylithapp] +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 1.0*year +dt = 0.1*year + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# For this problem, we want output over the entire domain, for the +# ground surface, and at simulated cGPS locations. +[pylithapp.problem.implicit] +output = [domain, subdomain, cgps_sites] + +# Default output is for the entire domain. +# We need to set the type of output for the subdomain and points. +output.subdomain = pylith.meshio.OutputSolnSubset +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveKin + +[pylithapp.problem.interfaces.slab] +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# We use a time history slip function. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture] +slip_function = pylith.faults.TimeHistorySlipFn + +# The slip is defined in a spatial database. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +slip.label = Gaussian slip distribution for SSE +slip.filename = spatialdb/sse_slip.spatialdb + +# Use linear interpolation. +slip.query_type = linear + +# We use a UniformDB to specify the slip initiation time. +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +# We use a temporal database to provide the slip time history. +time_history.label = Time history of slip +time_history.filename = spatialdb/sse_slip.timedb + +# Output fault results to HDF5 file. +[pylithapp.problem.interfaces.slab.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slab.h5 + +# We want both orientation and slip information in the information file. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We keep the default elastic materials for this problem, so no changes +# are necessary. + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain, subdomain, and points output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +# Name of nodeset for top surface. +label = boundary_zpos +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-groundsurf.h5 + +# Specify output type, coordinate system, and station file for cgps_sites. +[pylithapp.problem.formulation.output.cgps_sites] +# We will use a geographic coordinate system for the cGPS sites file. +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level + +# Use HDF5 output. +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-cgps_sites.h5 + +# Simulated cGPS station file. +reader.filename = cgps_sites.txt + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step06-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step06-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step06-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step06-mantle.h5 + + +# End of file diff --git a/examples/3d/subduction/synth_sse.cfg b/examples/3d/subduction/synth_sse.cfg index 69e4d3554a..d231a742ff 100644 --- a/examples/3d/subduction/synth_sse.cfg +++ b/examples/3d/subduction/synth_sse.cfg @@ -1,16 +1,16 @@ [synth_sse] rake = 45.0 -slip_center = [-122.6765, 45.5231] -slip_radius = 0.5 +slip_center = [-124.5, 45.5] +slip_radius = 0.7 slip_max = 5.0 -slip_sigma_lon = 0.2 -slip_sigma_lat = 0.2 +slip_sigma_lon = 0.3 +slip_sigma_lat = 0.3 -slip_times = [0.0, 0.2, 0.4, 0.6, 0.8, 1.0] -slip_amplitudes = [0.0, 0.2, 0.5, 0.8, 0.9, 1.0] +slip_times = [0.0, 0.2, 0.4, 0.6, 0.8, 1.0, 1.2] +slip_amplitudes = [0.0, 0.2, 0.5, 0.8, 0.9, 1.0, 1.0] -grid_lon_range = [-123.0, -122.0] -grid_lat_range = [45.0, 46.0] +grid_lon_range = [-126.2, -123.0] +grid_lat_range = [44.4, 46.4] grid_incr = 0.04 time_db_filename = spatialdb/sse_slip.timedb diff --git a/examples/3d/subduction/viz/get_coast.sh b/examples/3d/subduction/viz/get_coast.sh index 1462645cf3..3037fdf528 100755 --- a/examples/3d/subduction/viz/get_coast.sh +++ b/examples/3d/subduction/viz/get_coast.sh @@ -10,7 +10,7 @@ txttm="cascadia_tm.txt" vtktm="cascadia_tm.vtk" # Region. -region="-R-129/-117/41/50" +region="-R-128/-118/41/50" # Resolution: (f)ull, (h)igh, (i)ntermediate, (l)ow, or (c)rude. reso="-Dl" @@ -31,4 +31,4 @@ cs2cs +proj=lonlat +ellps=WGS84 +datum=WGS84 +to +proj=tmerc +lon_0=-122.6765 +l # Run seg2vtk.py script to convert pscoast info to VTK file. ./seg2vtk.py --in_file=$txttm --out_file=$vtktm --elevation=0.1 -/bin/rm $txtwgs84 $txttm +# /bin/rm $txtwgs84 $txttm From 9ea62797bcae42561582098c1f47be60d0065cde Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 15 Jun 2017 17:16:31 +1200 Subject: [PATCH 037/216] Updated comments for consistency, and added dump_parameters and progress_monitor filenames. --- examples/3d/subduction/step06.cfg | 39 ++++++++++++++++++++----------- 1 file changed, 26 insertions(+), 13 deletions(-) diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index c079e961d5..6d90972fb0 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -28,18 +28,30 @@ # RUNNING THE SIMULATON # ---------------------------------------------------------------------- # -# This is not a self-contained simulation configuration file. This -# file only specifies parameters specific to tutorial step06. -# The general parameters are specified in the pylithapp.cfg -# file which PyLith reads by default. +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step06.cfg (main parameter file for step06) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. # # To run the simulation: # pylith step06.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. -# Permit uknown components so that we can ignore warnings. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- [pylithapp] +dump_parameters.filename = output/step06-parameters.json +problem.progress_monitor.filename = output/step06-progress.txt + +# Permit uknown components so that we can override components and +# ignore warnings. typos = strict # ---------------------------------------------------------------------- @@ -151,14 +163,6 @@ slip_time.data = [0.0*year] time_history.label = Time history of slip time_history.filename = spatialdb/sse_slip.timedb -# Output fault results to HDF5 file. -[pylithapp.problem.interfaces.slab.output] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step06-fault-slab.h5 - -# We want both orientation and slip information in the information file. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] - # ---------------------------------------------------------------------- # materials # ---------------------------------------------------------------------- @@ -195,6 +199,15 @@ writer.filename = output/step06-cgps_sites.h5 # Simulated cGPS station file. reader.filename = cgps_sites.txt +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +# Output fault results to HDF5 file. +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slab.h5 + +# We want both orientation and slip information in the information file. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] writer.filename = output/step06-slab.h5 From 840a0fe76d6c80c62ef2faf85c26c75ecf3e1f3b Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 15 Jun 2017 17:18:19 +1200 Subject: [PATCH 038/216] Uncommented line to delete scratch files. --- examples/3d/subduction/viz/get_coast.sh | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/viz/get_coast.sh b/examples/3d/subduction/viz/get_coast.sh index 3037fdf528..47249ceed7 100755 --- a/examples/3d/subduction/viz/get_coast.sh +++ b/examples/3d/subduction/viz/get_coast.sh @@ -31,4 +31,4 @@ cs2cs +proj=lonlat +ellps=WGS84 +datum=WGS84 +to +proj=tmerc +lon_0=-122.6765 +l # Run seg2vtk.py script to convert pscoast info to VTK file. ./seg2vtk.py --in_file=$txttm --out_file=$vtktm --elevation=0.1 -# /bin/rm $txtwgs84 $txttm +/bin/rm $txtwgs84 $txttm From 58750a44895ff3d51cae0bb8af2c5fd495112e8a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 09:44:45 -0700 Subject: [PATCH 039/216] Added more to coordinate system comment. --- examples/3d/subduction/pylithapp.cfg | 6 ++++-- 1 file changed, 4 insertions(+), 2 deletions(-) diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index e9ac223d6b..1eb73d367b 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -35,8 +35,10 @@ reader.filename = mesh/mesh_tet.exo # Cuthill-KcKee algorithm. reorder_mesh = True -# Our mesh uses a local Transverse Mercator geographic projection, -# which must be specified. +# Our mesh uses a local transverse Mercator geographic projection. By +# specifying the projection, we can use other georeferenced coordinate +# systems in spatial databases and the code will automatically +# transform coordinates as necessary. [pylithapp.mesh_generator.reader] coordsys = spatialdata.geocoords.CSGeoProj coordsys.space_dim = 3 From 351d605201a9db402abf89bcc9b84869f9896859 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 09:45:31 -0700 Subject: [PATCH 040/216] Added command line arguments to set paramters in ParaView Python scripts if running outside GUI. --- examples/3d/subduction/viz/plot_dispvec.py | 108 +++++++++++------ examples/3d/subduction/viz/plot_dispwarp.py | 113 ++++++++++------- examples/3d/subduction/viz/plot_faultslip.py | 121 ++++++++++++------- examples/3d/subduction/viz/plot_matprops.py | 90 +++++++++----- 4 files changed, 275 insertions(+), 157 deletions(-) mode change 100644 => 100755 examples/3d/subduction/viz/plot_dispvec.py mode change 100644 => 100755 examples/3d/subduction/viz/plot_dispwarp.py mode change 100644 => 100755 examples/3d/subduction/viz/plot_faultslip.py mode change 100644 => 100755 examples/3d/subduction/viz/plot_matprops.py diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py old mode 100644 new mode 100755 index 35a60d0574..01336a38d4 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -21,58 +21,88 @@ # This Python script runs using pvpython or within the ParaView Python # shell. + # User-specified parameters +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. # Root name for simulation. SIM_NAME = "step01" -# Scale used to exaggerate deformation. +# Scale used for displacement vectors. DISPLACEMENT_SCALE = 10.0e+3 # ---------------------------------------------------------------------- from paraview.simple import * -# Disable automatic camera reset on "Show" -paraview.simple._DisableFirstRenderCameraReset() - -# Read data -dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) -RenameSource("%s-domain" % SIM_NAME, dataDomain) - -scene = GetAnimationScene() -scene.UpdateAnimationUsingDataTimeSteps() -view = GetActiveViewOrCreate('RenderView') - -# Show undeformed domain, colored by magnitude of displacement vector. -domainDisplay = Show(dataDomain, view) -ColorBy(domainDisplay, ("POINTS", "displacement", "Magnitude")) -domainDisplay.RescaleTransferFunctionToDataRange(True) -domainDisplay.SetScalarBarVisibility(view, True) -domainDisplay.SetRepresentationType("Surface With Edges") -# Rescale color and/or opacity maps used to exactly fit the current data range -displacementLUT = GetColorTransferFunction('displacement') -domainDisplay.RescaleTransferFunctionToDataRange(False, False) -# Update scalar bar component title. -UpdateScalarBarsComponentTitle(displacementLUT, domainDisplay) +def visualize(sim, dispScale): + + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read data + dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) + RenameSource("%s-domain" % SIM_NAME, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Show undeformed domain, colored by magnitude of displacement vector. + domainDisplay = Show(dataDomain, view) + ColorBy(domainDisplay, ("POINTS", "displacement", "Magnitude")) + domainDisplay.RescaleTransferFunctionToDataRange(True) + domainDisplay.SetScalarBarVisibility(view, True) + domainDisplay.SetRepresentationType("Surface With Edges") + + # Rescale color and/or opacity maps used to exactly fit the current data range + displacementLUT = GetColorTransferFunction('displacement') + domainDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update scalar bar component title. + UpdateScalarBarsComponentTitle(displacementLUT, domainDisplay) + + + # Add arrows to show displacement vectors. + glyph = Glyph(Input=dataDomain, GlyphType="Arrow") + glyph.Vectors = ["POINTS", "displacement"] + glyph.ScaleFactor = DISPLACEMENT_SCALE + glyph.ScaleMode = "vector" + glyph.GlyphMode = "All Points" + + glyphDisplay = Show(glyph, view) + glyphDisplay.Representation = "Surface" + + view.ResetCamera() + + Render() -# Add arrows to show displacement vectors. -glyph = Glyph(Input=dataDomain, GlyphType="Arrow") -glyph.Vectors = ["POINTS", "displacement"] -glyph.ScaleFactor = DISPLACEMENT_SCALE -glyph.ScaleMode = "vector" -glyph.GlyphMode = "All Points" - -glyphDisplay = Show(glyph, view) -glyphDisplay.Representation = "Surface" - -view.ResetCamera() - -Render() - -# Uncomment if running from shell outside ParaView. -#Interact() +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--vector-scale", action="store", type=float, dest="scale") + args = parser.parse_args() + + sim = args.sim + scale = args.scale + if sim is None: + sim = SIM_NAME + if scale is None: + scale = DISPLACEMENT_SCALE + visualize(sim, scale) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, DISPLACEMENT_SCALE) # End of file diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py old mode 100644 new mode 100755 index 0fe341c51a..d40273c641 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -17,11 +17,13 @@ # Plot the undeformed domain as a gray wireframe and then the deformed # domain, colored by the value of the x-displacemenet. -# -# This Python script runs using pvpython or within the ParaView Python -# shell. -# User-specified parameters + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. # Root name for simulation. SIM_NAME = "step01" @@ -31,46 +33,69 @@ # ---------------------------------------------------------------------- from paraview.simple import * -# Disable automatic camera reset on "Show" -paraview.simple._DisableFirstRenderCameraReset() - -# Read data -dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) -RenameSource("%s-domain" % SIM_NAME, dataDomain) - -scene = GetAnimationScene() -scene.UpdateAnimationUsingDataTimeSteps() -view = GetActiveViewOrCreate('RenderView') - -# Gray wireframe for undeformed domain. -domainDisplay = Show(dataDomain, view) -domainDisplay.Representation = 'Wireframe' -domainDisplay.AmbientColor = [0.5, 0.5, 0.5] - -# Warp domain to show deformation -warp = WarpByVector(Input=dataDomain) -warp.Vectors = ['POINTS', 'displacement'] -warp.ScaleFactor = DISPLACEMENT_SCALE - -warpDisplay = Show(warp, view) -ColorBy(warpDisplay, ('POINTS', 'displacement', 'X')) -warpDisplay.RescaleTransferFunctionToDataRange(True) -warpDisplay.SetScalarBarVisibility(view, True) -warpDisplay.SetRepresentationType('Surface With Edges') - -# Rescale color and/or opacity maps used to exactly fit the current data range -displacementLUT = GetColorTransferFunction('displacement') -warpDisplay.RescaleTransferFunctionToDataRange(False, False) -# Update a scalar bar component title. -UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) - -view.ResetCamera() -view.Update() - -Render() - -# Uncomment if running from shell outside ParaView. -#Interact() + +def visualize(sim, exaggeration): + + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read data + dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % sim]) + RenameSource("%s-domain" % sim, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Gray wireframe for undeformed domain. + domainDisplay = Show(dataDomain, view) + domainDisplay.Representation = 'Wireframe' + domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + + # Warp domain to show deformation + warp = WarpByVector(Input=dataDomain) + warp.Vectors = ['POINTS', 'displacement'] + warp.ScaleFactor = exaggeration + + warpDisplay = Show(warp, view) + ColorBy(warpDisplay, ('POINTS', 'displacement', 'X')) + warpDisplay.RescaleTransferFunctionToDataRange(True) + warpDisplay.SetScalarBarVisibility(view, True) + warpDisplay.SetRepresentationType('Surface With Edges') + + # Rescale color and/or opacity maps used to exactly fit the current data range + displacementLUT = GetColorTransferFunction('displacement') + warpDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update a scalar bar component title. + UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration") + args = parser.parse_args() + + sim = args.sim + exaggeration = args.exaggeration + if sim is None: + sim = SIM_NAME + if exaggeration is None: + exaggeration = DISPLACEMENT_SCALE + visualize(sim, exaggeration) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, DISPLACEMENT_SCALE) # End of file diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py old mode 100644 new mode 100755 index 3f23f54a0a..700733a4a9 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -21,7 +21,11 @@ # This Python script runs using pvpython or within the ParaView Python # shell. -# User-specified parameters +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. # Root name for simulation. SIM_NAME = "step02" @@ -31,50 +35,77 @@ # ---------------------------------------------------------------------- from paraview.simple import * -# Disable automatic camera reset on "Show" -paraview.simple._DisableFirstRenderCameraReset() - -# Read domain data -dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) -RenameSource("%s-domain" % SIM_NAME, dataDomain) - -scene = GetAnimationScene() -scene.UpdateAnimationUsingDataTimeSteps() -view = GetActiveViewOrCreate('RenderView') - -# Gray wireframe for undeformed domain. -domainDisplay = Show(dataDomain, view) -domainDisplay.Representation = 'Wireframe' -domainDisplay.AmbientColor = [0.5, 0.5, 0.5] - -# Read fault data -dataFaults = [] -for fault in FAULTS: - data = XDMFReader(FileNames=["output/%s-%s.xmf" % (SIM_NAME, fault)]) - RenameSource("%s-%s" % (SIM_NAME, fault), data) - dataFaults.append(data) - -groupFaults = GroupDatasets(Input=dataFaults) - -faultDisplay = Show(groupFaults, view) -ColorBy(faultDisplay, ('POINTS', 'slip', 'Magnitude')) -faultDisplay.RescaleTransferFunctionToDataRange(True) -faultDisplay.SetScalarBarVisibility(view, True) -faultDisplay.SetRepresentationType('Surface With Edges') - -# Rescale color and/or opacity maps used to exactly fit the current data range -slipLUT = GetColorTransferFunction('slip') -faultDisplay.RescaleTransferFunctionToDataRange(False, False) -# Update a scalar bar component title. -UpdateScalarBarsComponentTitle(slipLUT, faultDisplay) - -view.ResetCamera() -view.Update() - -Render() - -# Uncomment if running from shell outside ParaView. -#Interact() + +def visualize(sim, faults): + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read domain data + dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) + RenameSource("%s-domain" % SIM_NAME, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Gray wireframe for undeformed domain. + domainDisplay = Show(dataDomain, view) + domainDisplay.Representation = 'Wireframe' + domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + + # Read fault data + dataFaults = [] + for fault in faults: + data = XDMFReader(FileNames=["output/%s-%s.xmf" % (SIM_NAME, fault)]) + RenameSource("%s-%s" % (SIM_NAME, fault), data) + dataFaults.append(data) + + groupFaults = GroupDatasets(Input=dataFaults) + + faultDisplay = Show(groupFaults, view) + ColorBy(faultDisplay, ('POINTS', 'slip', 'Magnitude')) + faultDisplay.RescaleTransferFunctionToDataRange(True) + faultDisplay.SetScalarBarVisibility(view, True) + faultDisplay.SetRepresentationType('Surface With Edges') + + # Rescale color and/or opacity maps used to exactly fit the current data range + slipLUT = GetColorTransferFunction('slip') + faultDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update a scalar bar component title. + UpdateScalarBarsComponentTitle(slipLUT, faultDisplay) + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--faults", action="store", dest="faults") + args = parser.parse_args() + + sim = args.sim + if args.faults: + faults = args.faults.split(",") + else: + faults = None + + if sim is None: + sim = SIM_NAME + if faults is None: + faults = FAULTS + + visualize(sim, faults) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, FAULTS) # End of file diff --git a/examples/3d/subduction/viz/plot_matprops.py b/examples/3d/subduction/viz/plot_matprops.py old mode 100644 new mode 100755 index 87d0e11bfb..116583ba00 --- a/examples/3d/subduction/viz/plot_matprops.py +++ b/examples/3d/subduction/viz/plot_matprops.py @@ -16,11 +16,13 @@ # ---------------------------------------------------------------------- # Plot the domain, colored by material properties. -# -# This Python script runs using pvpython or within the ParaView Python -# shell. -# User-specified parameters + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. # Root name for simulation. SIM_NAME = "step01" @@ -31,40 +33,70 @@ # ---------------------------------------------------------------------- from paraview.simple import * -# Disable automatic camera reset on "Show" -paraview.simple._DisableFirstRenderCameraReset() +def visualize(sim, field, materials): -dataAll = [] -# Read data -for material in MATERIALS: - dataMaterial = XDMFReader(FileNames=["output/%s-%s_info.xmf" % (SIM_NAME, material)]) - RenameSource("%s-%s" % (SIM_NAME, material), dataMaterial) - dataAll.append(dataMaterial) -groupMaterials = GroupDatasets(Input=dataAll) + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() -view = GetActiveViewOrCreate('RenderView') -# Show domain, colored by magnitude of displacement vector. -materialDisplay = Show(groupMaterials, view) -ColorBy(materialDisplay, ("CELLS", INFO_FIELD)) -materialDisplay.RescaleTransferFunctionToDataRange(True) -materialDisplay.SetScalarBarVisibility(view, True) -materialDisplay.SetRepresentationType("Surface With Edges") + dataAll = [] + # Read data + for material in materials: + dataMaterial = XDMFReader(FileNames=["output/%s-%s_info.xmf" % (sim, material)]) + RenameSource("%s-%s" % (sim, material), dataMaterial) + dataAll.append(dataMaterial) + groupMaterials = GroupDatasets(Input=dataAll) -# Rescale color and/or opacity maps used to exactly fit the current data range -materialLUT = GetColorTransferFunction(INFO_FIELD) -materialDisplay.RescaleTransferFunctionToDataRange(False, False) -# Update scalar bar component title. -UpdateScalarBarsComponentTitle(materialLUT, materialDisplay) + view = GetActiveViewOrCreate('RenderView') + # Show domain, colored by magnitude of displacement vector. + materialDisplay = Show(groupMaterials, view) + ColorBy(materialDisplay, ("CELLS", field)) + materialDisplay.RescaleTransferFunctionToDataRange(True) + materialDisplay.SetScalarBarVisibility(view, True) + materialDisplay.SetRepresentationType("Surface With Edges") -view.ResetCamera() + # Rescale color and/or opacity maps used to exactly fit the current data range + materialLUT = GetColorTransferFunction(INFO_FIELD) + materialDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update scalar bar component title. + UpdateScalarBarsComponentTitle(materialLUT, materialDisplay) -Render() + view.ResetCamera() + Render() -# Uncomment if running from shell outside ParaView. -#Interact() +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--field", action="store", dest="field") + parser.add_argument("--materials", action="store", dest="materials") + args = parser.parse_args() + + sim = args.sim + field = args.field + if args.materials: + materials = args.materials.split(",") + else: + materials = None + + if sim is None: + sim = SIM_NAME + if field is None: + field = INFO_FIELD + if materials is None: + materials = MATERIALS + visualize(sim, field, materials) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, INFO_FIELD, MATERIALS) # End of file From a35bee1de58026039ac10ad049cfedb5e61afee7 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 12:58:10 -0700 Subject: [PATCH 041/216] Update coordinate system to geographic projection. --- .../spatialdb/fault_slabtop_creep.spatialdb | 17 ++++++++++++++--- 1 file changed, 14 insertions(+), 3 deletions(-) diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb index 9918db10a3..3eca673370 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_creep.spatialdb @@ -16,11 +16,22 @@ SimpleGridDB { value-names = left-lateral-slip reverse-slip fault-opening value-units = cm/year cm/year cm/year space-dim = 3 - cs-data = cartesian { + cs-data = geo-projected { to-meters = 1.0e+3 // Specify coordinates in km for convenience. - space-dim = 3 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } // projector } // cs-data -} // SimpleDB +} // SimpleGridDB + // x coordinate 0.0 From b7a1883811b226249ebe4b91e8240e091ac5df1f Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 16 Jun 2017 10:00:05 +1200 Subject: [PATCH 042/216] Changed name of Python script to generate fault slip spatialdb, and added option of not generating a timedb. --- examples/3d/subduction/{synth_sse.cfg => synth_gaussian.cfg} | 0 examples/3d/subduction/{synth_sse.py => synth_gaussian.py} | 0 2 files changed, 0 insertions(+), 0 deletions(-) rename examples/3d/subduction/{synth_sse.cfg => synth_gaussian.cfg} (100%) rename examples/3d/subduction/{synth_sse.py => synth_gaussian.py} (100%) diff --git a/examples/3d/subduction/synth_sse.cfg b/examples/3d/subduction/synth_gaussian.cfg similarity index 100% rename from examples/3d/subduction/synth_sse.cfg rename to examples/3d/subduction/synth_gaussian.cfg diff --git a/examples/3d/subduction/synth_sse.py b/examples/3d/subduction/synth_gaussian.py similarity index 100% rename from examples/3d/subduction/synth_sse.py rename to examples/3d/subduction/synth_gaussian.py From d736cb1d50ceed29322381d3d4da038cefdc5534 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 16 Jun 2017 10:01:45 +1200 Subject: [PATCH 043/216] Changes for timedb that didn't get committed earlier. --- examples/3d/subduction/synth_gaussian.cfg | 6 +++--- examples/3d/subduction/synth_gaussian.py | 15 +++++++++------ 2 files changed, 12 insertions(+), 9 deletions(-) diff --git a/examples/3d/subduction/synth_gaussian.cfg b/examples/3d/subduction/synth_gaussian.cfg index d231a742ff..9dae5f678c 100644 --- a/examples/3d/subduction/synth_gaussian.cfg +++ b/examples/3d/subduction/synth_gaussian.cfg @@ -1,4 +1,4 @@ -[synth_sse] +[synth_gaussian] rake = 45.0 slip_center = [-124.5, 45.5] slip_radius = 0.7 @@ -18,10 +18,10 @@ time_db_filename = spatialdb/sse_slip.timedb coordsys = spatialdata.geocoords.CSGeo iohandler = spatialdata.spatialdb.SimpleGridAscii -[synth_sse.coordsys] +[synth_gaussian.coordsys] space_dim = 3 datum_horiz = WGS84 datum_vert = mean sea level -[synth_sse.iohandler] +[synth_gaussian.iohandler] filename = spatialdb/sse_slip.spatialdb diff --git a/examples/3d/subduction/synth_gaussian.py b/examples/3d/subduction/synth_gaussian.py index 288e521b3c..2f392218e5 100755 --- a/examples/3d/subduction/synth_gaussian.py +++ b/examples/3d/subduction/synth_gaussian.py @@ -1,9 +1,9 @@ #!/usr/bin/env python -## @file synth_sse.py +## @file synth_gaussian.py ## @brief Python application to create spatial databases for a synthetic -## SSE with time-varying circular slip. +## event with time-varying Gaussian slip. # import pdb import math @@ -15,14 +15,14 @@ from pyre.applications.Script import Script as Application -class SynthSse(Application): +class SynthGaussian(Application): """ Python application to create spatial databases for a synthetic SSE with time-varying Gaussian slip. """ import pyre.inventory - ## Python object for managing SynthSse facilities and properties. + ## Python object for managing SynthGaussian facilities and properties. ## ## \b Properties ## @li \b rake Rake of fault slip (degrees). @@ -95,7 +95,7 @@ class SynthSse(Application): # PUBLIC METHODS ///////////////////////////////////////////////////// - def __init__(self, name="synth_sse"): + def __init__(self, name="synth_gaussian"): Application.__init__(self, name) self.lon = None @@ -229,6 +229,9 @@ def _writeTemporaldb(self): Write temporal database with time variation of fault slip. """ + if (len(self.slipTimes) == 1): + return + time = [float(i) for i in self.slipTimes] timeArr = numpy.array(time, dtype=numpy.float64) @@ -243,7 +246,7 @@ def _writeTemporaldb(self): # ---------------------------------------------------------------------- if __name__ == '__main__': - app = SynthSse() + app = SynthGaussian() app.run() # End of file From 2a9bba5dfbdd00dc364d458fe13deb514b65ac29 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 15:13:37 -0700 Subject: [PATCH 044/216] Added step04 with earthquake cycle example. --- examples/3d/subduction/TODO | 2 + .../fault_slabtop_coseismic.spatialdb | 54 +++ examples/3d/subduction/step04.cfg | 325 ++++++++++++++++++ 3 files changed, 381 insertions(+) create mode 100644 examples/3d/subduction/TODO create mode 100644 examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb create mode 100644 examples/3d/subduction/step04.cfg diff --git a/examples/3d/subduction/TODO b/examples/3d/subduction/TODO new file mode 100644 index 0000000000..bcd38ff460 --- /dev/null +++ b/examples/3d/subduction/TODO @@ -0,0 +1,2 @@ +ParaView Python script to plot fault normal_dir, dip_dir, strike_dir + diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb new file mode 100644 index 0000000000..5abf15ecfb --- /dev/null +++ b/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb @@ -0,0 +1,54 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify a uniform creep rate below a depth of 50 km, tapering to +// 0 at a depth of 30 km. +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 1 + num-z = 4 + num-values = 3 + value-names = left-lateral-slip reverse-slip fault-opening + value-units = m m m + space-dim = 3 + cs-data = geo-projected { + to-meters = 1.0e+3 // Specify coordinates in km for convenience. + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } // projector + } // cs-data +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +0.0 + +// z coordinate +99.0 -45.0 -60.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) left-laterial-slip (m) +// (5) reverse-slip (m) +// (6) fault-opening (m) +0.0 0.0 99.0 -2.0 +4.0 0.0 +0.0 0.0 -45.0 -2.0 +4.0 0.0 +0.0 0.0 -60.0 0.0 0.0 0.0 +0.0 0.0 -999.0 0.0 0.0 0.0 diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg new file mode 100644 index 0000000000..6365978d07 --- /dev/null +++ b/examples/3d/subduction/step04.cfg @@ -0,0 +1,325 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# We combine the interseismic deformation in Step03 with coseismic +# slip to model two earthquake cycles. The coseismic slip exactly +# complements the aseismic slip at depth; we also include an +# earthquake with coseismic slip on the splay fault. +# +# We use both Dirichlet boundary conditions to constrain the +# displacements on the lateral and bottom boundaries. +# +# We use the same material properties as in Step03. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step04.cfg (main parameter file for step04) +# - solver_fieldsplit.cfg (field split solver settings) +# +# To run the simulation: +# pylith step04.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step04-parameters.json +problem.progress_monitor.filename = output/step04-progress.txt + +# Permit unknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 300.0*year +dt = 10.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. Because the +# slab intersects the boundaries of the domain, and PyLith does not +# permit overlap between the fault interfaces and Dirichlet boundary +# conditions, for the Dirichlet boundary conditions we use the +# nodesets which exclude vertices on the fault. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg_nofault +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg_nofault +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos_nofault +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab_top, slab_bottom, splay] + +[pylithapp.problem.interfaces] +slab_top = pylith.faults.FaultCohesiveKin +slab_bottom = pylith.faults.FaultCohesiveKin +splay = pylith.faults.FaultCohesiveKin + +# Slab top ------------------------------------------------------------- +[pylithapp.problem.interfaces.slab_top] +id = 100 +label = fault_slabtop +edge = fault_slabtop_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Use multiple earthquake sources for the top of the slab to model the +# earthquake cycle: +# - creep +# - eq1 +# - eq2 +eq_srcs = [creep, eq1, eq2] +eq_srcs.creep.origin_time = 0.0*year +eq_srcs.eq1.origin_time = 99.999*year +eq_srcs.eq2.origin_time = 199.999*year + +# Use the constant slip rate time function for the creep earthquake source. +eq_srcs.creep.slip_function = pylith.faults.ConstRateSlipFn + +# Creep +[pylithapp.problem.interfaces.slab_top.eq_srcs.creep.slip_function] +slip_rate = spatialdata.spatialdb.SimpleGridDB +slip_rate.label = Slab top slip rate. +slip_rate.filename = spatialdb/fault_slabtop_creep.spatialdb +slip_rate.query_type = linear + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] ; Slip time is relative to origin time + +# Earthquake 1 +[pylithapp.problem.interfaces.slab_top.eq_srcs.eq1.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +slip.label = Slab top slip rate. +slip.filename = spatialdb/fault_slabtop_coseismic.spatialdb +slip.query_type = linear + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] ; Slip time is relative to origin time. + +# Earthquake 2 (same as earthquake 1) +[pylithapp.problem.interfaces.slab_top.eq_srcs.eq2.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +slip.label = Slab top slip rate. +slip.filename = spatialdb/fault_slabtop_coseismic.spatialdb +slip.query_type = linear + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] ; Slip time is relative to origin time. + +# Output +[pylithapp.problem.interfaces.slab_top.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step04-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# Slab bottom ---------------------------------------------------------- +[pylithapp.problem.interfaces.slab_bottom] +id = 101 +label = fault_slabbot +edge = fault_slabbot_edge +up_dir = [-0.1,0,0.9] + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slab bottom slip rate. +slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] +slip_rate.data = [+2.0*cm/year, -4.0*cm/year, 0.0*cm/year] + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +# Output +[pylithapp.problem.interfaces.slab_bottom.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step04-fault-slabbot.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# Splay ---------------------------------------------------------------- +[pylithapp.problem.interfaces.splay] +id = 102 +label = fault_splay +edge = fault_splay_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Origin time for splay fault earthquake. +eq_srcs.rupture.origin_time = 249.999*year + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.splay.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.UniformDB +slip.label = Splay fault slip. +slip.values = [left-lateral-slip, reverse-slip, fault-opening] +slip.data = [-1.0*m, 2.0*m, 0.0*m] + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] ; Relative to the origin time + +# Output +[pylithapp.problem.interfaces.splay.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step04-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We use the same material properties as step02, with linear Maxwell +# viscoelastic models for the mantle and slab. +[pylithapp.problem.materials] +slab = pylith.materials.MaxwellIsotropic3D +mantle = pylith.materials.MaxwellIsotropic3D + +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.mantle.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output ------------------------------------------ +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step04-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step04-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step04-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step04-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step04-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step04-mantle.h5 + + +# End of file From db0fea8926251df1e64312afbcb8be65e870861f Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 15:13:53 -0700 Subject: [PATCH 045/216] Add more comments to README. --- examples/3d/subduction/README | 10 ++++++---- 1 file changed, 6 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 5929795405..031033bd5d 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -1,6 +1,3 @@ -TODO - Set coordinate system to projected geographic coordinate system. - Directory structure: mesh (mesh related files) spatialdb (spatial database related files) @@ -40,7 +37,7 @@ Features: Preconditioners + LU [1] - + AMG (ML) + + AMG (ML) [1ex] + AMG (ML) + custom preconditioner [2,3] Uniform refinement [exercise] @@ -101,6 +98,11 @@ Step03: Interseismic [tutorial] Step04: Earthquake cycle [exercise] Interseismic + coseismic + Exercise: Make lower slab + splay fault the primary fault surface + and the upper slab (trench side of the splay fault) the secondary + fault surface. Hint: You will need to create a nodesets in CUBIT + that correspond to the primary and secondary fault surfaces. + Step05: Compression with frictional interface [tutorial] Interseismic + rate- and state-friction Quasistatic From 2d7e9ac18eee275e4be9a28459b5f78419ca584b Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 16 Jun 2017 11:01:10 +1200 Subject: [PATCH 046/216] Added step07a.cfg to generate synthetic data, and .cfg file to provide spatialdb for slip. --- examples/3d/subduction/ss_coseismic.cfg | 27 +++ examples/3d/subduction/step07a.cfg | 218 ++++++++++++++++++++++++ 2 files changed, 245 insertions(+) create mode 100644 examples/3d/subduction/ss_coseismic.cfg create mode 100644 examples/3d/subduction/step07a.cfg diff --git a/examples/3d/subduction/ss_coseismic.cfg b/examples/3d/subduction/ss_coseismic.cfg new file mode 100644 index 0000000000..d2ce6ba56d --- /dev/null +++ b/examples/3d/subduction/ss_coseismic.cfg @@ -0,0 +1,27 @@ +[synth_gaussian] +rake = 45.0 +slip_center = [-124.0, 45.5] +slip_radius = 0.6 +slip_max = 8.0 +slip_sigma_lon = 0.3 +slip_sigma_lat = 0.3 + +slip_times = [0.0] +slip_amplitudes = [1.0] + +grid_lon_range = [-126.2, -123.0] +grid_lat_range = [44.4, 46.4] +grid_incr = 0.04 + +time_db_filename = spatialdb/coseismic_slab_slip.timedb + +coordsys = spatialdata.geocoords.CSGeo +iohandler = spatialdata.spatialdb.SimpleGridAscii + +[synth_gaussian.coordsys] +space_dim = 3 +datum_horiz = WGS84 +datum_vert = mean sea level + +[synth_gaussian.iohandler] +filename = spatialdb/coseismic_slab_slip.spatialdb diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg new file mode 100644 index 0000000000..c71f57cefd --- /dev/null +++ b/examples/3d/subduction/step07a.cfg @@ -0,0 +1,218 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions and prescribed fault slip to +# simulate a coseismic event on the subductin interface. Fault slip +# is specified with a spatialdb to provide an approximately Gaussian +# slip distribution. This problem is used to generate synthetic +# data at cGPS locations. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step07a.cfg (main parameter file for step07a) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. +# +# To run the simulation: +# pylith step07a.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step07a-parameters.json +problem.progress_monitor.filename = output/step07a-progress.txt + +# Permit uknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation.time_step] +# This is a static problem so there is only a single time step. +total_time = 0.0*year + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# For this problem, we want output over the entire domain, for the +# ground surface, and at simulated cGPS locations. +[pylithapp.problem.implicit] +output = [domain, subdomain, cgps_sites] + +# Default output is for the entire domain. +# We need to set the type of output for the subdomain and points. +output.subdomain = pylith.meshio.OutputSolnSubset +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveKin + +[pylithapp.problem.interfaces.slab] +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# We use the default step-function slip time function. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture] + +# The slip is defined in a SimpleGridDB spatial database. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +slip.label = Gaussian slip distribution for earthquake +slip.filename = spatialdb/coseismic_slab_slip.spatialdb + +# Use linear interpolation. +slip.query_type = linear + +# We use a UniformDB to specify the slip initiation time. +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We keep the default elastic materials for this problem, so no changes +# are necessary. + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain, subdomain, and points output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +# Name of nodeset for top surface. +label = boundary_zpos +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-groundsurf.h5 + +# Specify output type, coordinate system, and station file for cgps_sites. +[pylithapp.problem.formulation.output.cgps_sites] +# We will use a geographic coordinate system for the cGPS sites file. +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level + +# Use HDF5 output. +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-cgps_sites.h5 + +# Simulated cGPS station file. +reader.filename = cgps_sites.txt + +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +# Output fault results to HDF5 file. +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-fault-slab.h5 + +# We want both orientation and slip information in the information file. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step07a-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step07a-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step07a-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step07a-mantle.h5 + + +# End of file From 2242407410f753b1e5e95660b5a3ee5db27d99f1 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 15 Jun 2017 16:58:14 -0700 Subject: [PATCH 047/216] Added step05. Improve comments in step03 and step04. --- examples/3d/subduction/TODO | 2 + examples/3d/subduction/pylithapp.cfg | 2 +- .../fault_slabtop_coseismic.spatialdb | 4 +- .../fault_slabtop_slipweakening.spatialdb | 58 ++++ .../fault_slabtop_tractions.spatialdb | 57 ++++ examples/3d/subduction/step03.cfg | 2 +- examples/3d/subduction/step04.cfg | 2 +- examples/3d/subduction/step05.cfg | 279 ++++++++++++++++++ 8 files changed, 401 insertions(+), 5 deletions(-) create mode 100644 examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb create mode 100644 examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb create mode 100644 examples/3d/subduction/step05.cfg diff --git a/examples/3d/subduction/TODO b/examples/3d/subduction/TODO index bcd38ff460..633f2e3f83 100644 --- a/examples/3d/subduction/TODO +++ b/examples/3d/subduction/TODO @@ -1,2 +1,4 @@ +ParaView Python script to plot slip contours and shear traction / normal traction. + ParaView Python script to plot fault normal_dir, dip_dir, strike_dir diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 1eb73d367b..f66b8875a2 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -18,7 +18,7 @@ solverlinear = 1 meshiocubit = 1 implicitelasticity = 1 faultcohesivekin = 1 -fiatlagrange = 1 +faultcohesivedyn = 1 materials = 1 mesh_distributor = 1 diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb index 5abf15ecfb..8c6be61281 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_coseismic.spatialdb @@ -4,8 +4,8 @@ // associated with aseismic creep on the interface between the mantle // and the subducting oceanic crust. // -// We specify a uniform creep rate below a depth of 50 km, tapering to -// 0 at a depth of 30 km. +// We specify uniform slip above a depth of 45 km, tapering to +// 0 at a depth of 60 km. // #SPATIAL_GRID.ascii 1 SimpleGridDB { diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb new file mode 100644 index 0000000000..92b231bb6b --- /dev/null +++ b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb @@ -0,0 +1,58 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify depth-dependent frictional properties with stable +// sliding (equal dynamic and static coefficients of friction) above +// and below the seismogenic zone (elevations of -5 km to -45 km). +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 1 + num-z = 6 + num-values = 4 + value-names = static-coefficient dynamic-coefficient slip-weakening-parameter cohesion + value-units = none none m Pa + space-dim = 3 + cs-data = geo-projected { + to-meters = 1.0e+3 // Specify coordinates in km for convenience. + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } // projector + } // cs-data +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +0.0 + +// z coordinate +99.0 -5.0 -15.0 -35.0 -45.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) static-coefficient +// (5) dynamic-coefficient +// (6) slip-weakening-parameter (m) +// (7) cohesion (Pa) +0.0 0.0 99.0 0.6 0.6 1.0 0.0 +0.0 0.0 -5.0 0.6 0.6 1.0 0.0 +0.0 0.0 -15.0 0.6 0.2 1.0 0.0 +0.0 0.0 -30.0 0.6 0.2 1.0 0.0 +0.0 0.0 -45.0 0.6 0.6 1.0 0.0 +0.0 0.0 -999.0 0.6 0.6 1.0 0.0 diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb new file mode 100644 index 0000000000..aaf168b835 --- /dev/null +++ b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb @@ -0,0 +1,57 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify depth-dependent fault tractions with higher values in +// the stable sliding regions consistent with residual stresses in +// those regions. +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 1 + num-z = 6 + num-values = 3 + value-names = traction-shear-leftlateral traction-shear-updip traction-normal + value-units = MPa MPa MPa + space-dim = 3 + cs-data = geo-projected { + to-meters = 1.0e+3 // Specify coordinates in km for convenience. + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } // projector + } // cs-data +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +0.0 + +// z coordinate +99.0 -5.0 -15.0 -35.0 -45.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) left-lateral shear traction (MPa) +// (5) reverse shear traction (MPa) +// (6) normal traction (MPa) +0.0 0.0 99.0 0.0 10.0 -20.0 +0.0 0.0 -5.0 0.6 10.0 -20.0 +0.0 0.0 -15.0 0.6 0.0 -20.0 +0.0 0.0 -30.0 0.6 0.0 -20.0 +0.0 0.0 -45.0 0.6 10.0 -20.0 +0.0 0.0 -999.0 0.6 10.0 -20.0 diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index a1a30f24f5..1dd85f81ba 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -111,7 +111,7 @@ db_initial.label = Dirichlet BC on -z # faults # ---------------------------------------------------------------------- [pylithapp.problem] -# We prescribe slip on the slab fault patch. +# We prescribe slip on the top and bottom of the slab. interfaces = [slab_top, slab_bottom] [pylithapp.problem.interfaces] diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index 6365978d07..efa97d3fec 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -113,7 +113,7 @@ db_initial.label = Dirichlet BC on -z # faults # ---------------------------------------------------------------------- [pylithapp.problem] -# We prescribe slip on the slab fault patch. +# We prescribe slip on the top and bottom of the slab and on the splay fault. interfaces = [slab_top, slab_bottom, splay] [pylithapp.problem.interfaces] diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg new file mode 100644 index 0000000000..221e382048 --- /dev/null +++ b/examples/3d/subduction/step05.cfg @@ -0,0 +1,279 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This problem drives spontaneous rupture on the subduction zone +# interface (top of the slab) via interseismic deformation. +# +# We include viscoelastic relaxation and prescribed aseismic slip on +# the bottom of the slab. We use Dirichlet boundary conditions to +# constrain the displacements on the lateral and bottom boundaries. +# +# We use the same material properties as step02. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step05.cfg (main parameter file for step05) +# - solver_fieldsplit.cfg (field split solver settings) +# +# To run the simulation: +# pylith step05.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step05-parameters.json +problem.progress_monitor.filename = output/step05-progress.txt + +# Permit unknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +# Fault friction is a nonlinear problem so we need to use the +# nonlinear solver. +solver = pylith.problems.SolverNonlinear + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 200.0*year +dt = 10.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. Because the +# slab intersects the boundaries of the domain, and PyLith does not +# permit overlap between the fault interfaces and Dirichlet boundary +# conditions, for the Dirichlet boundary conditions we use the +# nodesets which exclude vertices on the fault. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg_nofault +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg_nofault +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos_nofault +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the bottom of the slab with spontaneous rupture +# on the top of the slab. +interfaces = [slab_top, slab_bottom] + +[pylithapp.problem.interfaces] +slab_top = pylith.faults.FaultCohesiveDyn +slab_bottom = pylith.faults.FaultCohesiveKin + +# Slab top ------------------------------------------------------------- +[pylithapp.problem.interfaces.slab_top] +id = 100 +label = fault_slabtop +edge = fault_slabtop_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Friction +friction = pylith.friction.SlipWeakening +friction.label = Slip weakening +# Force healing after each time step, so weakening is confined to each +# time step and does not carry over into subsequent time steps. +friction.force_healing = True + +# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. +zero_tolerance = 1.0e-10 + +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +friction.db_properties.label = Slip weakening +friction.db_properties.filename = spatialdb/fault_slabtop_slipweakening.spatialdb + +# Initial fault tractions +traction_perturbation = pylith.faults.TractPerturbation +traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB +traction_perturbation.db_initial.label = Initial fault tractions +traction_perturbation.db_initial.filename = spatialdb/fault_slabtop_tractions.spatialdb + +[pylithapp.problem.interfaces.slab_top.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step05-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# Slab bottom ---------------------------------------------------------- +[pylithapp.problem.interfaces.slab_bottom] +id = 101 +label = fault_slabbot +edge = fault_slabbot_edge +up_dir = [-0.1,0,0.9] + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slab bottom slip rate. +slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] +slip_rate.data = [0.0*cm/year, -4.0*cm/year, 0.0*cm/year] + +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip initiation time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +[pylithapp.problem.interfaces.slab_bottom.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step05-fault-slabbot.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir] + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We use the same material properties as step02, with linear Maxwell +# viscoelastic models for the mantle and slab. +[pylithapp.problem.materials] +slab = pylith.materials.MaxwellIsotropic3D +mantle = pylith.materials.MaxwellIsotropic3D + +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.CompositeDB +db_properties.db_A = spatialdata.spatialdb.SimpleDB +db_properties.db_B = spatialdata.spatialdb.SimpleGridDB + +[pylithapp.timedependent.materials.mantle.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output ------------------------------------------ +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step05-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step05-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step05-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step05-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step05-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step05-mantle.h5 + + +# ---------------------------------------------------------------------- +# PETSc +# ---------------------------------------------------------------------- +[pylithapp.petsc] +malloc_dump = + +# Convergence parameters. +ksp_rtol = 1.0e-20 +ksp_atol = 1.0e-11 + +snes_rtol = 1.0e-20 +snes_atol = 1.0e-9 + +# End of file From c5b513c067f6cb4a551cb076d36aab8c837e03a4 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 16 Jun 2017 13:16:04 +1200 Subject: [PATCH 048/216] Added Green's function generation for slab. Problem: at present, the pylithapp.cfg settings for output seem to be overriding everything else, so I've had to comment them out. --- examples/3d/subduction/greensfns.cfg | 45 +++++ examples/3d/subduction/pylithapp.cfg | 16 +- .../spatialdb/impulse_amplitude.spatialdb | 34 ++++ examples/3d/subduction/step07b.cfg | 180 +++++++++++++++++ examples/3d/subduction/step07c.cfg | 181 ++++++++++++++++++ 5 files changed, 448 insertions(+), 8 deletions(-) create mode 100644 examples/3d/subduction/greensfns.cfg create mode 100644 examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb create mode 100644 examples/3d/subduction/step07b.cfg create mode 100644 examples/3d/subduction/step07c.cfg diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg new file mode 100644 index 0000000000..3e0d15fb16 --- /dev/null +++ b/examples/3d/subduction/greensfns.cfg @@ -0,0 +1,45 @@ +[greensfns] + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[greensfns] +fault_id = 100 + +[greensfns.formulation.time_step] +total_time = 0.0*s ; total time of simulation +dt = 1.0*year + +[greensfns] +interfaces = [fault] + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# Define output managers for state variables output. +[greensfns.materials.slab.output] +cell_info_fields = [density,mu,lambda] +cell_data_fields = [] +writer = pylith.meshio.DataWriterHDF5 +skip = 500000 + +[greensfns.materials.wedge.output] +cell_info_fields = [density,mu,lambda] +cell_data_fields = [] +writer = pylith.meshio.DataWriterHDF5 +skip = 500000 + +[greensfns.materials.crust.output] +cell_info_fields = [density,mu,lambda] +cell_data_fields = [] +writer = pylith.meshio.DataWriterHDF5 +skip = 500000 + +[greensfns.materials.mantle.output] +cell_info_fields = [density,mu,lambda] +cell_data_fields = [] +writer = pylith.meshio.DataWriterHDF5 +skip = 500000 + +# End of file + diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index f66b8875a2..4210667e32 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -117,19 +117,19 @@ output.writer = pylith.meshio.DataWriterHDF5 # # We write the output using HDF5/Xdmf files. -[pylithapp.problem.implicit] -output = [domain, subdomain] +# [pylithapp.problem.implicit] +# output = [domain, subdomain] # Set subdomain component to OutputSolnSubset (boundary of the domain). -output.subdomain = pylith.meshio.OutputSolnSubset +# output.subdomain = pylith.meshio.OutputSolnSubset -[pylithapp.problem.formulation.output.domain] -writer = pylith.meshio.DataWriterHDF5 +# [pylithapp.problem.formulation.output.domain] +# writer = pylith.meshio.DataWriterHDF5 -[pylithapp.problem.formulation.output.subdomain] +# [pylithapp.problem.formulation.output.subdomain] # Name of nodeset for top surface. -label = boundary_zpos -writer = pylith.meshio.DataWriterHDF5 +# label = boundary_zpos +# writer = pylith.meshio.DataWriterHDF5 # ---------------------------------------------------------------------- # PETSc diff --git a/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb b/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb new file mode 100644 index 0000000000..e1b7343795 --- /dev/null +++ b/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb @@ -0,0 +1,34 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the impulse amplitudes for +// generating Green's functions. They are all set to 1. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 1 // number of material property values + value-names = slip + value-units = m + num-locs = 1 + data-dim = 0 + space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) slip (m) +0.0 0.0 0.0 1.0 diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg new file mode 100644 index 0000000000..554a9fe030 --- /dev/null +++ b/examples/3d/subduction/step07b.cfg @@ -0,0 +1,180 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions to generate Green's functions +# for a patch on the subduction interface. Responses are computed +# at simulated cGPS locations. +# Note that we change the default problem type from TimeDependent to +# GreensFns. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - greensfns.cfg (greensfns paramters, read by default) +# - step07b.cfg (main parameter file for step07b) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. +# +# To run the simulation: +# pylith step07b.cfg solver_fieldsplit.cfg --problem=pylith.problems.GreensFns +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step07b-parameters.json +problem.progress_monitor.filename = output/step07b-progress.txt + +# Permit uknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# Problem. +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +output = [cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveImpulses + +[pylithapp.problem.interfaces.slab] +id = 100 +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Label and query type for fault slip. +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.query_type = nearest + +# Spatialdb for impulses. +impulse_dof = [0] +db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb + + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We keep the default elastic materials for this problem, so no changes +# are necessary. + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# cGPS sites output --------------------------------- +[pylithapp.problem.formulation.output.cgps_sites] +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level +writer = pylith.meshio.DataWriterHDF5 +reader.filename = cgps_sites.txt + +writer.filename = output/step07b-cgps_sites.h5 + +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07b-fault-slab.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step07b-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step07b-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step07b-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step07b-mantle.h5 + + +# End of file diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg new file mode 100644 index 0000000000..75160bbb51 --- /dev/null +++ b/examples/3d/subduction/step07c.cfg @@ -0,0 +1,181 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions to generate Green's functions +# for a patch on the subduction interface. Responses are computed +# at simulated cGPS locations. This problem computes the responses +# to updip slip. +# Note that we change the default problem type from TimeDependent to +# GreensFns. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - greensfns.cfg (greensfns paramters, read by default) +# - step07c.cfg (main parameter file for step07c) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. +# +# To run the simulation: +# pylith step07c.cfg solver_fieldsplit.cfg --problem=pylith.problems.GreensFns +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step07c-parameters.json +problem.progress_monitor.filename = output/step07c-progress.txt + +# Permit uknown components so that we can override components and +# ignore warnings. +typos = strict + +# ---------------------------------------------------------------------- +# Problem. +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +output = [cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We constrain the DOF normal to each of the boundaries. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveImpulses + +[pylithapp.problem.interfaces.slab] +id = 100 +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Label and query type for fault slip. +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.query_type = nearest + +# Spatialdb for impulses. +impulse_dof = [1] +db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb + + +# ---------------------------------------------------------------------- +# materials +# ---------------------------------------------------------------------- +# We keep the default elastic materials for this problem, so no changes +# are necessary. + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# cGPS sites output --------------------------------- +[pylithapp.problem.formulation.output.cgps_sites] +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level +writer = pylith.meshio.DataWriterHDF5 +reader.filename = cgps_sites.txt + +writer.filename = output/step07c-cgps_sites.h5 + +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07c-fault-slab.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step07c-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step07c-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step07c-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step07c-mantle.h5 + + +# End of file From 06783939298eb9f64b44664ba3643e0d9dabaa71 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 16 Jun 2017 16:44:22 +1200 Subject: [PATCH 049/216] Added script to create synthetic data from PyLith results. Need to add .cfg file and test script. --- examples/3d/subduction/make_synth_data.py | 143 ++++++++++++++++++++++ 1 file changed, 143 insertions(+) create mode 100755 examples/3d/subduction/make_synth_data.py diff --git a/examples/3d/subduction/make_synth_data.py b/examples/3d/subduction/make_synth_data.py new file mode 100755 index 0000000000..a64475b3ea --- /dev/null +++ b/examples/3d/subduction/make_synth_data.py @@ -0,0 +1,143 @@ +#!/usr/bin/env python + +## @file make_synth_data.py + +## @brief Python application to create synthetic data from PyLith points output. + +import pdb +import math +import numpy +import h5py + +from pyre.applications.Script import Script as Application + +class MakeSynthData(Application): + """ + Python application to create synthetic data from PyLith points output. + """ + + import pyre.inventory + ## Python object for managing MakeSynthData facilities and properties. + ## + ## \b Properties + ## @li \b point_input_file HDF5 input file generated by PyLith. + ## @li \b sigma_east Sigma value for east displacements. + ## @li \b sigma_north Sigma value for north displacements. + ## @li \b sigma_up Sigma value for up displacements. + ## @li \b output_file Name of ASCII output file. + ## + + pointInputFile = pyre.inventory.str("point_input_file", + default="cascadia-cgps_points.h5") + pointInputFile.meta['tip'] = "HDF5 point output file from PyLith." + + sigmaEast = pyre.inventory.float("sigma_east", default=0.0005) + sigmaEast.meta['tip'] = "Sigma value for East displacements." + + sigmaNorth = pyre.inventory.float("sigma_north", default=0.0005) + sigmaNorth.meta['tip'] = "Sigma value for North displacements." + + sigmaUp = pyre.inventory.float("sigma_up", default=0.001) + sigmaUp.meta['tip'] = "Sigma value for Up displacements." + + outputFile = pyre.inventory.str("output_file", + default="cascadia-cgps_displ.txt") + outputFile.meta['tip'] = "Name of ASCII output file." + + + # PUBLIC METHODS ///////////////////////////////////////////////////// + + def __init__(self, name="make_synth_data"): + Application.__init__(self, name) + + self.coords = None + self.stations = None + self.dispRaw = None + self.dispNoise = None + + self.numStations = 0 + + return + + + def main(self): + pdb.set_trace() + + self._readHDF5() + self._addNoise() + self._writeOutput() + + return + + + # PRIVATE METHODS ///////////////////////////////////////////////////// + + + def _configure(self): + """ + Setup members using inventory. + """ + Application._configure(self) + + return + + + def _readHDF5(self): + """ + Function to read HDF5 file from PyLith. + """ + + h5File = h5py.File(self.pointInputFile, 'r') + self.coords = h5File['geometry/vertices'][:] + self.stations = h5File['stations'][:] + self.dispRaw = h5File['vertex_fields/displacement'][0,:,:] + self.numStations = self.coords.shape[0] + + return + + + def _addNoise(self): + """ + Function to add noise to computed displacements. + """ + + self.dispNoise[:,0] = self.dispRaw[:,0] + \ + self.sigmaEast * numpy.random.randn(self.numStations) + self.dispNoise[:,1] = self.dispRaw[:,1] + \ + self.sigmaNorth * numpy.random.randn(self.numStations) + self.dispNoise[:,2] = self.dispRaw[:,2] + \ + self.sigmaUp * numpy.random.randn(self.numStations) + + return + + + def _writeOutput(self): + """ + Function to write output file with noisy data and uncertainties. + """ + head = "Station\tX\tY\tZ\tUEast\tUNorth\tUUp\tSigEast\tSigNorth\tSigUp\n" + outFmt = "%s" + 9 * "\t%g" + "\n" + + f = open(self.outputFile, 'w') + f.write(head) + + for stationNum in range(self.numStations): + outLine = outFmt % (self.coords[stationNum,0], self.coords[stationNum,1], + self.coords[stationNum,2], + self.dispNoise[stationNum,0], + self.dispNoise[stationNum,1], + self.dispNoise[stationNum,2], + self.sigmaEast, self.sigmaNorth, self.sigmaUp) + f.write(outLine) + + f.close() + + return + + +# ---------------------------------------------------------------------- +if __name__ == '__main__': + app = MakeSynthData() + app.run() + +# End of file From bdd499aa74bc8085cb196b55d04c34b2ae05c492 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 16 Jun 2017 12:03:06 -0700 Subject: [PATCH 050/216] Fix output settings for Green's functions. --- examples/3d/subduction/greensfns.cfg | 20 +------------------- examples/3d/subduction/pylithapp.cfg | 16 ++++++++-------- examples/3d/subduction/step07b.cfg | 18 +++++++----------- 3 files changed, 16 insertions(+), 38 deletions(-) diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg index 3e0d15fb16..536ddfe6cc 100644 --- a/examples/3d/subduction/greensfns.cfg +++ b/examples/3d/subduction/greensfns.cfg @@ -5,41 +5,23 @@ # ---------------------------------------------------------------------- [greensfns] fault_id = 100 - -[greensfns.formulation.time_step] -total_time = 0.0*s ; total time of simulation -dt = 1.0*year - -[greensfns] interfaces = [fault] # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- -# Define output managers for state variables output. +# Turn off output of state variables for materials. [greensfns.materials.slab.output] -cell_info_fields = [density,mu,lambda] cell_data_fields = [] -writer = pylith.meshio.DataWriterHDF5 -skip = 500000 [greensfns.materials.wedge.output] -cell_info_fields = [density,mu,lambda] cell_data_fields = [] -writer = pylith.meshio.DataWriterHDF5 -skip = 500000 [greensfns.materials.crust.output] -cell_info_fields = [density,mu,lambda] cell_data_fields = [] -writer = pylith.meshio.DataWriterHDF5 -skip = 500000 [greensfns.materials.mantle.output] -cell_info_fields = [density,mu,lambda] cell_data_fields = [] -writer = pylith.meshio.DataWriterHDF5 -skip = 500000 # End of file diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 4210667e32..6f36872f9a 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -117,19 +117,19 @@ output.writer = pylith.meshio.DataWriterHDF5 # # We write the output using HDF5/Xdmf files. -# [pylithapp.problem.implicit] -# output = [domain, subdomain] +[pylithapp.problem.formulation] +output = [domain, subdomain] # Set subdomain component to OutputSolnSubset (boundary of the domain). -# output.subdomain = pylith.meshio.OutputSolnSubset +output.subdomain = pylith.meshio.OutputSolnSubset -# [pylithapp.problem.formulation.output.domain] -# writer = pylith.meshio.DataWriterHDF5 +[pylithapp.problem.formulation.output.domain] +writer = pylith.meshio.DataWriterHDF5 -# [pylithapp.problem.formulation.output.subdomain] +[pylithapp.problem.formulation.output.subdomain] # Name of nodeset for top surface. -# label = boundary_zpos -# writer = pylith.meshio.DataWriterHDF5 +label = boundary_zpos +writer = pylith.meshio.DataWriterHDF5 # ---------------------------------------------------------------------- # PETSc diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 554a9fe030..6e55fe50f7 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -50,17 +50,6 @@ dump_parameters.filename = output/step07b-parameters.json problem.progress_monitor.filename = output/step07b-progress.txt -# Permit uknown components so that we can override components and -# ignore warnings. -typos = strict - -# ---------------------------------------------------------------------- -# Problem. -# ---------------------------------------------------------------------- -[pylithapp.problem.formulation] -output = [cgps_sites] -output.cgps_sites = pylith.meshio.OutputSolnPoints - # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- @@ -145,6 +134,13 @@ db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +output = [domain, subdomain, cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# Turn off output for domain and subdomain. +#output.domain.vertex_data_fields = [] +#output.subdomain.vertex_data_fields = [] # cGPS sites output --------------------------------- [pylithapp.problem.formulation.output.cgps_sites] From d216cc00f92a053b8d548fee3f8e12502fe67c9e Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 17 Jun 2017 15:04:08 -0700 Subject: [PATCH 051/216] Clean up of step07a. --- ...ynth_data.py => make_synthetic_gpsdisp.py} | 32 ++++------ .../generate_slowslip.cfg} | 10 +-- .../generate_slowslip.py} | 19 ++---- examples/3d/subduction/step07a.cfg | 61 ++++++++----------- 4 files changed, 50 insertions(+), 72 deletions(-) rename examples/3d/subduction/{make_synth_data.py => make_synthetic_gpsdisp.py} (75%) rename examples/3d/subduction/{synth_gaussian.cfg => spatialdb/generate_slowslip.cfg} (72%) rename examples/3d/subduction/{synth_gaussian.py => spatialdb/generate_slowslip.py} (93%) diff --git a/examples/3d/subduction/make_synth_data.py b/examples/3d/subduction/make_synthetic_gpsdisp.py similarity index 75% rename from examples/3d/subduction/make_synth_data.py rename to examples/3d/subduction/make_synthetic_gpsdisp.py index a64475b3ea..1a4412d9fb 100755 --- a/examples/3d/subduction/make_synth_data.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -4,7 +4,6 @@ ## @brief Python application to create synthetic data from PyLith points output. -import pdb import math import numpy import h5py @@ -27,8 +26,7 @@ class MakeSynthData(Application): ## @li \b output_file Name of ASCII output file. ## - pointInputFile = pyre.inventory.str("point_input_file", - default="cascadia-cgps_points.h5") + pointInputFile = pyre.inventory.str("point_input_file", default="cascadia-cgps_points.h5") pointInputFile.meta['tip'] = "HDF5 point output file from PyLith." sigmaEast = pyre.inventory.float("sigma_east", default=0.0005) @@ -40,14 +38,13 @@ class MakeSynthData(Application): sigmaUp = pyre.inventory.float("sigma_up", default=0.001) sigmaUp.meta['tip'] = "Sigma value for Up displacements." - outputFile = pyre.inventory.str("output_file", - default="cascadia-cgps_displ.txt") + outputFile = pyre.inventory.str("output_file", default="cascadia-cgps_disp.txt") outputFile.meta['tip'] = "Name of ASCII output file." # PUBLIC METHODS ///////////////////////////////////////////////////// - def __init__(self, name="make_synth_data"): + def __init__(self, name="make_synthetic_gpsdisp"): Application.__init__(self, name) self.coords = None @@ -61,8 +58,6 @@ def __init__(self, name="make_synth_data"): def main(self): - pdb.set_trace() - self._readHDF5() self._addNoise() self._writeOutput() @@ -87,10 +82,12 @@ def _readHDF5(self): Function to read HDF5 file from PyLith. """ - h5File = h5py.File(self.pointInputFile, 'r') - self.coords = h5File['geometry/vertices'][:] - self.stations = h5File['stations'][:] - self.dispRaw = h5File['vertex_fields/displacement'][0,:,:] + h5 = h5py.File(self.pointInputFile, 'r') + self.coords = h5['geometry/vertices'][:] + self.stations = h5['stations'][:] + self.dispRaw = h5['vertex_fields/displacement'][0,:,:] + hf.close() + self.numStations = self.coords.shape[0] return @@ -100,14 +97,9 @@ def _addNoise(self): """ Function to add noise to computed displacements. """ - - self.dispNoise[:,0] = self.dispRaw[:,0] + \ - self.sigmaEast * numpy.random.randn(self.numStations) - self.dispNoise[:,1] = self.dispRaw[:,1] + \ - self.sigmaNorth * numpy.random.randn(self.numStations) - self.dispNoise[:,2] = self.dispRaw[:,2] + \ - self.sigmaUp * numpy.random.randn(self.numStations) - + self.dispNoise[:,0] = self.dispRaw[:,0] + self.sigmaEast * numpy.random.randn(self.numStations) + self.dispNoise[:,1] = self.dispRaw[:,1] + self.sigmaNorth * numpy.random.randn(self.numStations) + self.dispNoise[:,2] = self.dispRaw[:,2] + self.sigmaUp * numpy.random.randn(self.numStations) return diff --git a/examples/3d/subduction/synth_gaussian.cfg b/examples/3d/subduction/spatialdb/generate_slowslip.cfg similarity index 72% rename from examples/3d/subduction/synth_gaussian.cfg rename to examples/3d/subduction/spatialdb/generate_slowslip.cfg index 9dae5f678c..002e27797f 100644 --- a/examples/3d/subduction/synth_gaussian.cfg +++ b/examples/3d/subduction/spatialdb/generate_slowslip.cfg @@ -1,4 +1,4 @@ -[synth_gaussian] +[generate_slowslip] rake = 45.0 slip_center = [-124.5, 45.5] slip_radius = 0.7 @@ -13,15 +13,15 @@ grid_lon_range = [-126.2, -123.0] grid_lat_range = [44.4, 46.4] grid_incr = 0.04 -time_db_filename = spatialdb/sse_slip.timedb +time_db_filename = fault_slabtop_slowslip.timedb coordsys = spatialdata.geocoords.CSGeo iohandler = spatialdata.spatialdb.SimpleGridAscii -[synth_gaussian.coordsys] +[generate_slowslip.coordsys] space_dim = 3 datum_horiz = WGS84 datum_vert = mean sea level -[synth_gaussian.iohandler] -filename = spatialdb/sse_slip.spatialdb +[generate_slowslip.iohandler] +filename = fault_slabtop_slowslip.spatialdb diff --git a/examples/3d/subduction/synth_gaussian.py b/examples/3d/subduction/spatialdb/generate_slowslip.py similarity index 93% rename from examples/3d/subduction/synth_gaussian.py rename to examples/3d/subduction/spatialdb/generate_slowslip.py index 2f392218e5..78ba080830 100755 --- a/examples/3d/subduction/synth_gaussian.py +++ b/examples/3d/subduction/spatialdb/generate_slowslip.py @@ -1,6 +1,6 @@ #!/usr/bin/env python -## @file synth_gaussian.py +## @file generate_slowslip.py ## @brief Python application to create spatial databases for a synthetic ## event with time-varying Gaussian slip. @@ -67,8 +67,7 @@ class SynthGaussian(Application): slipTimeUnits = pyre.inventory.str("slip_time_units", default="year") slipTimeUnits.meta['tip'] = "Units used for slip times." - slipAmplitudes = pyre.inventory.list("slip_amplitudes", - default=[0.0, 0.5, 1.0]) + slipAmplitudes = pyre.inventory.list("slip_amplitudes", default=[0.0, 0.5, 1.0]) slipAmplitudes.meta['tip'] = "List of slip amplitudes." gridLonRange = pyre.inventory.list("grid_lon_range", default=[-123.0, -124.0]) @@ -83,19 +82,16 @@ class SynthGaussian(Application): timeDbFilename = pyre.inventory.str("time_db_filename", default="slip.timedb") timeDbFilename.meta['tip'] = "Filename of temporal DB output file." - coordsys = pyre.inventory.facility("coordsys", - family="coordsys", - factory=CSGeo) + coordsys = pyre.inventory.facility("coordsys", family="coordsys", factory=CSGeo) coordsys.meta['tip'] = "Coordinate system for output database." - iohandler = pyre.inventory.facility("iohandler", family="simplegrid_io", - factory=SimpleGridAscii) + iohandler = pyre.inventory.facility("iohandler", family="simplegrid_io", factory=SimpleGridAscii) iohandler.meta['tip'] = "Object for writing spatial database." # PUBLIC METHODS ///////////////////////////////////////////////////// - def __init__(self, name="synth_gaussian"): + def __init__(self, name="generate_slowslip"): Application.__init__(self, name) self.lon = None @@ -193,10 +189,7 @@ def _writeSpatialdb(self): """ Write spatial database with fault slip. """ - - print "Writing spatial database:" - - llSlipInfo = {'name': "left-lateral-slip", + llSlipInfo = {'name': "left-lateral-slip", 'units': "m", 'data': self.faultSlip[:,0]} diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index c71f57cefd..bf694e09b9 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -49,29 +49,14 @@ dump_parameters.filename = output/step07a-parameters.json problem.progress_monitor.filename = output/step07a-progress.txt -# Permit uknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- [pylithapp.problem.formulation.time_step] # This is a static problem so there is only a single time step. -total_time = 0.0*year - -# ---------------------------------------------------------------------- -# output -# ---------------------------------------------------------------------- -# For this problem, we want output over the entire domain, for the -# ground surface, and at simulated cGPS locations. -[pylithapp.problem.implicit] -output = [domain, subdomain, cgps_sites] - -# Default output is for the entire domain. -# We need to set the type of output for the subdomain and points. -output.subdomain = pylith.meshio.OutputSolnSubset -output.cgps_sites = pylith.meshio.OutputSolnPoints +# Define the total time for the simulation and the time step size. +total_time = 1.0*year +dt = 0.05*year # ---------------------------------------------------------------------- # boundary conditions @@ -140,14 +125,14 @@ quadrature.cell.dimension = 2 # We use the default step-function slip time function. [pylithapp.problem.interfaces.slab.eq_srcs.rupture] +slip_function = pylith.faults.TimeHistorySlipFn + # The slip is defined in a SimpleGridDB spatial database. [pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] slip = spatialdata.spatialdb.SimpleGridDB slip.label = Gaussian slip distribution for earthquake -slip.filename = spatialdb/coseismic_slab_slip.spatialdb - -# Use linear interpolation. +slip.filename = spatialdb/fault_slabtop_slowslip.spatialdb slip.query_type = linear # We use a UniformDB to specify the slip initiation time. @@ -156,6 +141,18 @@ slip_time.label = Slip initiation time slip_time.values = [slip-time] slip_time.data = [0.0*year] +# User time history slip function +time_history.label = Slow slip time history function +time_history.filename = spatialdb/fault_slabtop_slowslip.timedb + +# Output +[pylithapp.problem.interfaces.slab.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-fault-slab.h5 + +# We want both orientation and slip information in the information file. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + # ---------------------------------------------------------------------- # materials # ---------------------------------------------------------------------- @@ -165,16 +162,21 @@ slip_time.data = [0.0*year] # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +# For this problem, we want output over the entire domain, for the +# ground surface, and at simulated cGPS locations. +[pylithapp.problem.implicit] +output = [domain, subdomain, cgps_sites] + +# Default output is for the entire domain. +# We need to set the type of output for the subdomain and points. +output.subdomain = pylith.meshio.OutputSolnSubset +output.cgps_sites = pylith.meshio.OutputSolnPoints # Domain, subdomain, and points output --------------------------------- [pylithapp.problem.formulation.output.domain] -writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step07a-domain.h5 [pylithapp.problem.formulation.output.subdomain] -# Name of nodeset for top surface. -label = boundary_zpos -writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step07a-groundsurf.h5 # Specify output type, coordinate system, and station file for cgps_sites. @@ -192,15 +194,6 @@ writer.filename = output/step07a-cgps_sites.h5 # Simulated cGPS station file. reader.filename = cgps_sites.txt -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.slab.output] -# Output fault results to HDF5 file. -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07a-fault-slab.h5 - -# We want both orientation and slip information in the information file. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] - # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] writer.filename = output/step07a-slab.h5 From a037060510320f4cb68e22142c0261a5997069d9 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 17 Jun 2017 15:54:13 -0700 Subject: [PATCH 052/216] Added check to make sure file exists. Small fixes. --- examples/3d/subduction/viz/plot_dispvec.py | 11 +++++++---- examples/3d/subduction/viz/plot_dispwarp.py | 6 +++++- examples/3d/subduction/viz/plot_faultslip.py | 17 ++++++++++++----- examples/3d/subduction/viz/plot_matprops.py | 6 +++++- 4 files changed, 29 insertions(+), 11 deletions(-) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 01336a38d4..5868c05310 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -37,7 +37,7 @@ # ---------------------------------------------------------------------- from paraview.simple import * - +import os def visualize(sim, dispScale): @@ -45,8 +45,11 @@ def visualize(sim, dispScale): paraview.simple._DisableFirstRenderCameraReset() # Read data - dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) - RenameSource("%s-domain" % SIM_NAME, dataDomain) + filename = "output/%s-domain.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[sim]) + RenameSource("%s-domain" % sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() @@ -69,7 +72,7 @@ def visualize(sim, dispScale): # Add arrows to show displacement vectors. glyph = Glyph(Input=dataDomain, GlyphType="Arrow") glyph.Vectors = ["POINTS", "displacement"] - glyph.ScaleFactor = DISPLACEMENT_SCALE + glyph.ScaleFactor = dispScale glyph.ScaleMode = "vector" glyph.GlyphMode = "All Points" diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index d40273c641..160bfb7b50 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -33,6 +33,7 @@ # ---------------------------------------------------------------------- from paraview.simple import * +import os def visualize(sim, exaggeration): @@ -40,7 +41,10 @@ def visualize(sim, exaggeration): paraview.simple._DisableFirstRenderCameraReset() # Read data - dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % sim]) + filename = "output/%s-domain.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[filename]) RenameSource("%s-domain" % sim, dataDomain) scene = GetAnimationScene() diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py index 700733a4a9..99d4fea610 100755 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -28,21 +28,25 @@ # pvpython. # Root name for simulation. -SIM_NAME = "step02" +SIM_NAME = "step07a" # Names of faults for output files. FAULTS = ["fault-slab"] # ---------------------------------------------------------------------- from paraview.simple import * +import os def visualize(sim, faults): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read domain data - dataDomain = XDMFReader(FileNames=["output/%s-domain.xmf" % SIM_NAME]) - RenameSource("%s-domain" % SIM_NAME, dataDomain) + filename = "output/%s-domain.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[filename]) + RenameSource("%s-domain" % sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() @@ -56,8 +60,11 @@ def visualize(sim, faults): # Read fault data dataFaults = [] for fault in faults: - data = XDMFReader(FileNames=["output/%s-%s.xmf" % (SIM_NAME, fault)]) - RenameSource("%s-%s" % (SIM_NAME, fault), data) + filename = "output/%s-%s.xmf" % (sim, fault) + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + data = XDMFReader(FileNames=[filename]) + RenameSource("%s-%s" % (sim, fault), data) dataFaults.append(data) groupFaults = GroupDatasets(Input=dataFaults) diff --git a/examples/3d/subduction/viz/plot_matprops.py b/examples/3d/subduction/viz/plot_matprops.py index 116583ba00..3e47a6cc0c 100755 --- a/examples/3d/subduction/viz/plot_matprops.py +++ b/examples/3d/subduction/viz/plot_matprops.py @@ -33,6 +33,7 @@ # ---------------------------------------------------------------------- from paraview.simple import * +import os def visualize(sim, field, materials): @@ -43,7 +44,10 @@ def visualize(sim, field, materials): dataAll = [] # Read data for material in materials: - dataMaterial = XDMFReader(FileNames=["output/%s-%s_info.xmf" % (sim, material)]) + filename = "output/%s-%s_info.xmf" % (sim, material) + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataMaterial = XDMFReader(FileNames=[filename]) RenameSource("%s-%s" % (sim, material), dataMaterial) dataAll.append(dataMaterial) groupMaterials = GroupDatasets(Input=dataAll) From 37fd53216958fdb0bec37dedea5946182d413c8c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 17 Jun 2017 16:09:43 -0700 Subject: [PATCH 053/216] Cleanup of step07 parameters. --- .gitignore | 2 ++ examples/3d/subduction/ss_coseismic.cfg | 27 ------------------ examples/3d/subduction/step07a.cfg | 2 ++ examples/3d/subduction/step07b.cfg | 12 +++++--- examples/3d/subduction/step07c.cfg | 37 ++++++++++++------------- 5 files changed, 30 insertions(+), 50 deletions(-) delete mode 100644 examples/3d/subduction/ss_coseismic.cfg diff --git a/.gitignore b/.gitignore index 4766c64016..c1ed835a57 100644 --- a/.gitignore +++ b/.gitignore @@ -34,3 +34,5 @@ examples/3d/subduction/output examples/3d/subduction/mesh/geometry_surfs.jou examples/3d/subduction/mesh/*.exo examples/3d/subduction/mesh/*.sat +examples/3d/subduction/spatialdb/fault_slabtop_slowslip.spatialdb +examples/3d/subduction/spatialdb/fault_slabtop_slowslip.timedb diff --git a/examples/3d/subduction/ss_coseismic.cfg b/examples/3d/subduction/ss_coseismic.cfg deleted file mode 100644 index d2ce6ba56d..0000000000 --- a/examples/3d/subduction/ss_coseismic.cfg +++ /dev/null @@ -1,27 +0,0 @@ -[synth_gaussian] -rake = 45.0 -slip_center = [-124.0, 45.5] -slip_radius = 0.6 -slip_max = 8.0 -slip_sigma_lon = 0.3 -slip_sigma_lat = 0.3 - -slip_times = [0.0] -slip_amplitudes = [1.0] - -grid_lon_range = [-126.2, -123.0] -grid_lat_range = [44.4, 46.4] -grid_incr = 0.04 - -time_db_filename = spatialdb/coseismic_slab_slip.timedb - -coordsys = spatialdata.geocoords.CSGeo -iohandler = spatialdata.spatialdb.SimpleGridAscii - -[synth_gaussian.coordsys] -space_dim = 3 -datum_horiz = WGS84 -datum_vert = mean sea level - -[synth_gaussian.iohandler] -filename = spatialdb/coseismic_slab_slip.spatialdb diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index bf694e09b9..a3542735ea 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -175,6 +175,8 @@ output.cgps_sites = pylith.meshio.OutputSolnPoints # Domain, subdomain, and points output --------------------------------- [pylithapp.problem.formulation.output.domain] writer.filename = output/step07a-domain.h5 +# Turn off data fields. +vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] writer.filename = output/step07a-groundsurf.h5 diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 6e55fe50f7..a4cd65e7d9 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -138,11 +138,15 @@ db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb output = [domain, subdomain, cgps_sites] output.cgps_sites = pylith.meshio.OutputSolnPoints -# Turn off output for domain and subdomain. -#output.domain.vertex_data_fields = [] -#output.subdomain.vertex_data_fields = [] +# Domain, subdomain, and points output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step07b-domain.h5 +# Turn off data fields. +vertex_data_fields = [] + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step07b-groundsurf.h5 -# cGPS sites output --------------------------------- [pylithapp.problem.formulation.output.cgps_sites] coordsys = spatialdata.geocoords.CSGeo coordsys.space_dim = 3 diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg index 75160bbb51..de8e0058c6 100644 --- a/examples/3d/subduction/step07c.cfg +++ b/examples/3d/subduction/step07c.cfg @@ -51,17 +51,6 @@ dump_parameters.filename = output/step07c-parameters.json problem.progress_monitor.filename = output/step07c-progress.txt -# Permit uknown components so that we can override components and -# ignore warnings. -typos = strict - -# ---------------------------------------------------------------------- -# Problem. -# ---------------------------------------------------------------------- -[pylithapp.problem.formulation] -output = [cgps_sites] -output.cgps_sites = pylith.meshio.OutputSolnPoints - # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- @@ -136,6 +125,11 @@ db_impulse_amplitude.query_type = nearest impulse_dof = [1] db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb +# Output +[pylithapp.problem.interfaces.slab.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07c-fault-slab.h5 # ---------------------------------------------------------------------- # materials @@ -144,10 +138,21 @@ db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb # are necessary. # ---------------------------------------------------------------------- -# output +# Output # ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +output = [domain, subdomain, cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# Domain, subdomain, and points output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step07b-domain.h5 +# Turn off data fields. +vertex_data_fields = [] + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step07b-groundsurf.h5 -# cGPS sites output --------------------------------- [pylithapp.problem.formulation.output.cgps_sites] coordsys = spatialdata.geocoords.CSGeo coordsys.space_dim = 3 @@ -158,12 +163,6 @@ reader.filename = cgps_sites.txt writer.filename = output/step07c-cgps_sites.h5 -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.slab.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07c-fault-slab.h5 - # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] writer.filename = output/step07c-slab.h5 From e0eb39df26adf4cf35cb43a22388ffc48f134c3c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 17 Jun 2017 16:10:20 -0700 Subject: [PATCH 054/216] Small cleanup. --- pylith/meshio/OutputManager.py | 4 +--- 1 file changed, 1 insertion(+), 3 deletions(-) diff --git a/pylith/meshio/OutputManager.py b/pylith/meshio/OutputManager.py index 8d3225d277..c444d74745 100644 --- a/pylith/meshio/OutputManager.py +++ b/pylith/meshio/OutputManager.py @@ -240,9 +240,7 @@ def writeData(self, t, fields): logEvent = "%swriteData" % self._loggingPrefix self._eventLogger.eventBegin(logEvent) - if self._checkWrite(t) and \ - ( len(self.vertexDataFields) > 0 or \ - len(self.cellDataFields) ) > 0: + if self._checkWrite(t) and ( len(self.vertexDataFields) > 0 or len(self.cellDataFields) ) > 0: (mesh, label, labelId) = self.dataProvider().getDataMesh() self._openTimeStep(t, mesh, label, labelId) From 2f4c5a49b8270936116e06b45036881c8dfd3c68 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 17 Jun 2017 17:08:06 -0700 Subject: [PATCH 055/216] Refactor setting material models and parameters into mat_elastic.cfg and mat_viscoelastic.cfg. --- examples/3d/subduction/README | 4 +- examples/3d/subduction/mat_elastic.cfg | 48 +++++++++++++ examples/3d/subduction/mat_viscoelastic.cfg | 79 +++++++++++++++++++++ examples/3d/subduction/pylithapp.cfg | 13 +--- examples/3d/subduction/step01.cfg | 3 +- examples/3d/subduction/step02.cfg | 57 +-------------- examples/3d/subduction/step03.cfg | 54 +------------- examples/3d/subduction/step04.cfg | 54 +------------- examples/3d/subduction/step05.cfg | 54 +------------- examples/3d/subduction/step06.cfg | 15 +--- examples/3d/subduction/step07a.cfg | 9 +-- examples/3d/subduction/step07b.cfg | 9 +-- examples/3d/subduction/step07c.cfg | 11 +-- 13 files changed, 156 insertions(+), 254 deletions(-) create mode 100644 examples/3d/subduction/mat_elastic.cfg create mode 100644 examples/3d/subduction/mat_viscoelastic.cfg diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 031033bd5d..457b50ced2 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -1,7 +1,7 @@ Directory structure: mesh (mesh related files) - spatialdb (spatial database related files) - viz + spatialdb (spatial and temporal database related files) + viz (ParaView Python scripts) Elastic properties loosely based on diff --git a/examples/3d/subduction/mat_elastic.cfg b/examples/3d/subduction/mat_elastic.cfg new file mode 100644 index 0000000000..20f530c861 --- /dev/null +++ b/examples/3d/subduction/mat_elastic.cfg @@ -0,0 +1,48 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# Parameters for using linear elastic material models for the 'slab', +# 'wedge', 'mantle', and 'crust'. + +[pylithapp.problem.materials] +slab = pylith.materials.ElasticIsotropic3D +wedge = pylith.materials.ElasticIsotropic3D +crust = pylith.materials.ElasticIsotropic3D +mantle = pylith.materials.ElasticIsotropic3D + +# Slab +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for subducting slab +db_properties.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +[pylithapp.problem.materials.wedge] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for accretionary wedge +db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb + +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for mantle +db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +[pylithapp.problem.materials.crust] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for continental crust +db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb + + +# End of file diff --git a/examples/3d/subduction/mat_viscoelastic.cfg b/examples/3d/subduction/mat_viscoelastic.cfg new file mode 100644 index 0000000000..45bfe74cc3 --- /dev/null +++ b/examples/3d/subduction/mat_viscoelastic.cfg @@ -0,0 +1,79 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# Parameters for using linear elastic material models for the 'wedge' +# and 'crust" and linear Maxwell viscoelastic material models for the +# 'slab' and 'mantle'. The viscosity varies linearly with depth. +# +# We combine the density, Vp, and Vs from a SimpleDB with the +# viscosity from a SimpleGridDB using a CompositeDB. + +[pylithapp.problem.materials] +wedge = pylith.materials.ElasticIsotropic3D +crust = pylith.materials.ElasticIsotropic3D +slab = pylith.materials.MaxwellIsotropic3D +mantle = pylith.materials.MaxwellIsotropic3D + +# Slab +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A = spatialdata.spatialdb.SimpleDB +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B = spatialdata.spatialdb.SimpleGridDB +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + +# Wedge +[pylithapp.problem.materials.wedge] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for accretionary wedge +db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb + +# Mantle +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.CompositeDB + +[pylithapp.timedependent.materials.mantle.db_properties] +# Elastic properties +values_A = [density, vs, vp] +db_A = spatialdata.spatialdb.SimpleDB +db_A.label = Elastic properties +db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb + +# Viscoelastic properties +values_B = [viscosity] +db_B = spatialdata.spatialdb.SimpleGridDB +db_B.label = Linear Maxwell viscoelatic properties +db_B.filename = spatialdb/mat_viscosity.spatialdb +db_B.query_type = linear + +# Crust +[pylithapp.problem.materials.crust] +db_properties = spatialdata.spatialdb.SimpleDB +db_properties.label = Properties for continental crust +db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb + + +# End of file diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 6f36872f9a..325f9ca92d 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -58,8 +58,9 @@ coordsys.projector.proj_options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 # - mantle (block 3) # - crust (block 4) # -# We use the default material (ElasticIsotropic3D: 3-D isotropic, -# linear elastic material). +# The material model and parameters are specified in separate files to +# avoid conflicting parameters when we vary the material model from +# the default. See 'mat_elastic.cfg' and 'mat_viscoelastic.cfg'. [pylithapp.problem] materials = [slab, wedge, crust, mantle] @@ -67,8 +68,6 @@ materials = [slab, wedge, crust, mantle] [pylithapp.problem.materials.slab] label = Subducting slab id = 1 -db_properties.label = Properties for subducting slab -db_properties.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 @@ -80,8 +79,6 @@ output.writer = pylith.meshio.DataWriterHDF5 [pylithapp.problem.materials.wedge] label = Accretionary wedge id = 2 -db_properties.label = Properties for accretionary wedge -db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 @@ -91,8 +88,6 @@ output.writer = pylith.meshio.DataWriterHDF5 [pylithapp.problem.materials.mantle] label = Mantle id = 3 -db_properties.label = Properties for mantle -db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 @@ -102,8 +97,6 @@ output.writer = pylith.meshio.DataWriterHDF5 [pylithapp.problem.materials.crust] label = Continental crust id = 4 -db_properties.label = Properties for continental crust -db_properties.iohandler.filename = spatialdb/mat_crust_elastic.spatialdb quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 3 diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index e6b603d0bb..8d73b0553d 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -33,9 +33,10 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step01.cfg (main parameter file for step01) +# - mat_elastic.cfg (material models and parameters) # # To run the simulation: -# pylith step01.cfg +# pylith step01.cfg mat_elastic.cfg # # Output will be directed to the "output" directory.. diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index cd8db31365..6af0e030b8 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -28,6 +28,7 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step02.cfg (main parameter file for step02) +# - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # We use the field split preconditioner with algebraic multigrid for @@ -36,9 +37,9 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step02.cfg solver_fieldsplit.cfg +# pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -47,10 +48,6 @@ dump_parameters.filename = output/step02-parameters.json problem.progress_monitor.filename = output/step02-progress.txt -# Permit unknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -141,54 +138,6 @@ writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step02-fault-slab.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We change the mantle and slab to linear Maxwell viscoelastic -# materials with depth-dependent viscosities using a CompositeDB. The -# CompsiteDB allows us to combine the density, Vp, and Vs from the -# SimpleDB from Step01 with a viscosity from a SimpleGridDB into a -# single (composite) spatial database. -[pylithapp.problem.materials] -slab = pylith.materials.MaxwellIsotropic3D -mantle = pylith.materials.MaxwellIsotropic3D - -[pylithapp.problem.materials.slab] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.slab.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - -[pylithapp.problem.materials.mantle] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.mantle.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index 1dd85f81ba..c7e43dcf3a 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -31,12 +31,13 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step03.cfg (main parameter file for step03) +# - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # To run the simulation: -# pylith step03.cfg solver_fieldsplit.cfg +# pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -45,10 +46,6 @@ dump_parameters.filename = output/step03-parameters.json problem.progress_monitor.filename = output/step03-progress.txt -# Permit unknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -181,51 +178,6 @@ writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step03-fault-slabbot.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We use the same material properties as step02, with linear Maxwell -# viscoelastic models for the mantle and slab. -[pylithapp.problem.materials] -slab = pylith.materials.MaxwellIsotropic3D -mantle = pylith.materials.MaxwellIsotropic3D - -[pylithapp.problem.materials.slab] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.slab.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - -[pylithapp.problem.materials.mantle] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.mantle.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index efa97d3fec..966d996bc5 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -33,12 +33,13 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step04.cfg (main parameter file for step04) +# - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # To run the simulation: -# pylith step04.cfg solver_fieldsplit.cfg +# pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -47,10 +48,6 @@ dump_parameters.filename = output/step04-parameters.json problem.progress_monitor.filename = output/step04-progress.txt -# Permit unknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -252,51 +249,6 @@ writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step04-fault-slabtop.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We use the same material properties as step02, with linear Maxwell -# viscoelastic models for the mantle and slab. -[pylithapp.problem.materials] -slab = pylith.materials.MaxwellIsotropic3D -mantle = pylith.materials.MaxwellIsotropic3D - -[pylithapp.problem.materials.slab] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.slab.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - -[pylithapp.problem.materials.mantle] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.mantle.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg index 221e382048..425eabe977 100644 --- a/examples/3d/subduction/step05.cfg +++ b/examples/3d/subduction/step05.cfg @@ -32,12 +32,13 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step05.cfg (main parameter file for step05) +# - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # To run the simulation: -# pylith step05.cfg solver_fieldsplit.cfg +# pylith step05.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -46,10 +47,6 @@ dump_parameters.filename = output/step05-parameters.json problem.progress_monitor.filename = output/step05-progress.txt -# Permit unknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -193,51 +190,6 @@ writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step05-fault-slabbot.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We use the same material properties as step02, with linear Maxwell -# viscoelastic models for the mantle and slab. -[pylithapp.problem.materials] -slab = pylith.materials.MaxwellIsotropic3D -mantle = pylith.materials.MaxwellIsotropic3D - -[pylithapp.problem.materials.slab] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.slab.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - -[pylithapp.problem.materials.mantle] -db_properties = spatialdata.spatialdb.CompositeDB -db_properties.db_A = spatialdata.spatialdb.SimpleDB -db_properties.db_B = spatialdata.spatialdb.SimpleGridDB - -[pylithapp.timedependent.materials.mantle.db_properties] -# Elastic properties -values_A = [density, vs, vp] -db_A.label = Elastic properties -db_A.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb - -# Viscoelastic properties -values_B = [viscosity] -db_B.label = Linear Maxwell viscoelatic properties -db_B.filename = spatialdb/mat_viscosity.spatialdb -db_B.query_type = linear - - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 6d90972fb0..7c82da3ef4 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -31,6 +31,7 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step06.cfg (main parameter file for step06) +# - mat_elastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # We use the field split preconditioner with algebraic multigrid for @@ -39,9 +40,9 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step06.cfg solver_fieldsplit.cfg +# pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -50,10 +51,6 @@ dump_parameters.filename = output/step06-parameters.json problem.progress_monitor.filename = output/step06-progress.txt -# Permit uknown components so that we can override components and -# ignore warnings. -typos = strict - # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -163,12 +160,6 @@ slip_time.data = [0.0*year] time_history.label = Time history of slip time_history.filename = spatialdb/sse_slip.timedb -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We keep the default elastic materials for this problem, so no changes -# are necessary. - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index a3542735ea..b51df1ba44 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -30,6 +30,7 @@ # Parameter files: # - pylithapp.cfg (common paramters, read by default) # - step07a.cfg (main parameter file for step07a) +# - mat_elastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # We use the field split preconditioner with algebraic multigrid for @@ -38,7 +39,7 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step07a.cfg solver_fieldsplit.cfg +# pylith step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. @@ -153,12 +154,6 @@ writer.filename = output/step07a-fault-slab.h5 # We want both orientation and slip information in the information file. vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We keep the default elastic materials for this problem, so no changes -# are necessary. - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index a4cd65e7d9..8dc595c511 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -31,6 +31,7 @@ # - pylithapp.cfg (common paramters, read by default) # - greensfns.cfg (greensfns paramters, read by default) # - step07b.cfg (main parameter file for step07b) +# - mat_elastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # We use the field split preconditioner with algebraic multigrid for @@ -39,7 +40,7 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step07b.cfg solver_fieldsplit.cfg --problem=pylith.problems.GreensFns +# pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. @@ -125,12 +126,6 @@ impulse_dof = [0] db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We keep the default elastic materials for this problem, so no changes -# are necessary. - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg index de8e0058c6..eb832796ba 100644 --- a/examples/3d/subduction/step07c.cfg +++ b/examples/3d/subduction/step07c.cfg @@ -32,6 +32,7 @@ # - pylithapp.cfg (common paramters, read by default) # - greensfns.cfg (greensfns paramters, read by default) # - step07c.cfg (main parameter file for step07c) +# - mat_elastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # # We use the field split preconditioner with algebraic multigrid for @@ -40,9 +41,9 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step07c.cfg solver_fieldsplit.cfg --problem=pylith.problems.GreensFns +# pylith --problem=pylith.problems.GreensFns step07c.cfg mat_elastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory.. +# Output will be directed to the "output" directory. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -131,12 +132,6 @@ vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step07c-fault-slab.h5 -# ---------------------------------------------------------------------- -# materials -# ---------------------------------------------------------------------- -# We keep the default elastic materials for this problem, so no changes -# are necessary. - # ---------------------------------------------------------------------- # Output # ---------------------------------------------------------------------- From ba30afbe42cbd5c1b352c4cecb58eb4124baa53b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 18 Jun 2017 15:11:28 -0700 Subject: [PATCH 056/216] Refactored DirichletBC. pylithapp.cfg uses roller BC. --- examples/3d/subduction/pylithapp.cfg | 49 +++++++++++++++++++++++++ examples/3d/subduction/step01.cfg | 37 ++++--------------- examples/3d/subduction/step02.cfg | 54 +++++----------------------- examples/3d/subduction/step03.cfg | 47 +++++++----------------- examples/3d/subduction/step04.cfg | 48 ++++++------------------- examples/3d/subduction/step05.cfg | 47 +++++++----------------- examples/3d/subduction/step06.cfg | 46 ------------------------ examples/3d/subduction/step07a.cfg | 52 ++++----------------------- examples/3d/subduction/step07b.cfg | 52 ++++----------------------- examples/3d/subduction/step07c.cfg | 52 ++++----------------------- 10 files changed, 117 insertions(+), 367 deletions(-) diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index 325f9ca92d..ebf6958874 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -103,6 +103,55 @@ quadrature.cell.dimension = 3 output.cell_filter = pylith.meshio.CellFilterAvg output.writer = pylith.meshio.DataWriterHDF5 +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.problem] +# The generic setup is roller boundary conditions on the lateral and +# bottom boundaries. That is, we have zero displacements for the DOF +# normal to the boundary. We can use the default Dirichlet BC with its +# default spatial database (ZeroDispDB) for the boundary values. +# +# Array of boundary conditions (defaults to DirichletBC): +# x_neg (ZeroDispDB to specify zero x-displacement) +# x_pos (ZeroDispDB to specify zero x-displacement) +# y_neg (ZeroDispDB to specify zero y-displacement) +# y_pos (ZeroDispDB to specify zero y-displacement) +# z_neg (ZeroDispDB to specify zero z-displacement) +bc = [x_neg, x_pos, y_neg, y_pos, z_neg] + +# The label corresponds to the name of the nodeset in CUBIT. + +# -x face +[pylithapp.problem.bc.x_neg] +bc_dof = [0] +label = boundary_xneg +db_initial.label = Dirichlet BC on -x + +# +x face +[pylithapp.problem.bc.x_pos] +bc_dof = [0] +label = boundary_xpos +db_initial.label = Dirichlet BC on +x + +# -y face +[pylithapp.problem.bc.y_neg] +bc_dof = [1] +label = boundary_yneg +db_initial.label = Dirichlet BC on -y + +# +y face +[pylithapp.problem.bc.y_pos] +bc_dof = [1] +label = boundary_ypos +db_initial.label = Dirichlet BC on +y + +# -z face +[pylithapp.problem.bc.z_neg] +bc_dof = [2] +label = boundary_zneg +db_initial.label = Dirichlet BC on -z + # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index 8d73b0553d..2897bbc817 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -26,6 +26,12 @@ # compression. The negative z-boundary and positive and negative # y-boundaries are held fixed in the direction normal to the boundary. # +# Materials +# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -57,18 +63,7 @@ total_time = 0.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (UniformDB to specify x-displacement) -# x_pos (UniformDB to specify x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. +# We specify nonzero displacements on the -x and +x boundaries using UniformDB. # -x face [pylithapp.problem.bc.x_neg] @@ -89,24 +84,6 @@ db_initial.label = Dirichlet BC on +x db_initial.values = [displacement-x] db_initial.data = [-2.0*m] -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index 6af0e030b8..4a9861e67b 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -21,6 +21,14 @@ # uniform fault slip on the slab fault rupture patch with zero # displacement on the lateral and bottom boundaries. # +# Materials +# The 'wedge' and 'crust' blocks use the the linear, isotropic +# elastic material model, whereas the 'slab' and 'mantle' use the +# linear Maxwell viscoelastic material model (mat_viscoelastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -56,52 +64,6 @@ problem.progress_monitor.filename = output/step02-progress.txt total_time = 200.0*year dt = 10.0*year -# ---------------------------------------------------------------------- -# boundary conditions -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. - -# -x face -[pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x - -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index c7e43dcf3a..b788238757 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -22,7 +22,13 @@ # and bottom boundaries. The subducting slab uses prescribed slip with # a constant slip rate time function. # -# We use the same material properties as step02. +# Materials +# The 'wedge' and 'crust' blocks use the the linear, isotropic +# elastic material model, whereas the 'slab' and 'mantle' use the +# linear Maxwell viscoelastic material model (mat_viscoelastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -57,52 +63,23 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. Because the -# slab intersects the boundaries of the domain, and PyLith does not -# permit overlap between the fault interfaces and Dirichlet boundary -# conditions, for the Dirichlet boundary conditions we use the -# nodesets which exclude vertices on the fault. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. +# Because the slab intersects the boundaries of the domain, and PyLith +# does not permit overlap between the fault interfaces and Dirichlet +# boundary conditions, for the Dirichlet boundary conditions we use +# the nodesets which exclude vertices on the fault. We only update the +# name of the nodeset for the -x, -y, and +y boundaries. # -x face [pylithapp.problem.bc.x_neg] -bc_dof = [0] label = boundary_xneg_nofault -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x # -y face [pylithapp.problem.bc.y_neg] -bc_dof = [1] label = boundary_yneg_nofault -db_initial.label = Dirichlet BC on -y # +y face [pylithapp.problem.bc.y_pos] -bc_dof = [1] label = boundary_ypos_nofault -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z # ---------------------------------------------------------------------- # faults diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index 966d996bc5..63f690d744 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -21,10 +21,13 @@ # complements the aseismic slip at depth; we also include an # earthquake with coseismic slip on the splay fault. # -# We use both Dirichlet boundary conditions to constrain the -# displacements on the lateral and bottom boundaries. +# Materials +# The 'wedge' and 'crust' blocks use the the linear, isotropic +# elastic material model, whereas the 'slab' and 'mantle' use the +# linear Maxwell viscoelastic material model (mat_viscoelastic.cfg). # -# We use the same material properties as in Step03. +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -59,52 +62,23 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. Because the -# slab intersects the boundaries of the domain, and PyLith does not -# permit overlap between the fault interfaces and Dirichlet boundary -# conditions, for the Dirichlet boundary conditions we use the -# nodesets which exclude vertices on the fault. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. +# Because the slab intersects the boundaries of the domain, and PyLith +# does not permit overlap between the fault interfaces and Dirichlet +# boundary conditions, for the Dirichlet boundary conditions we use +# the nodesets which exclude vertices on the fault. We only update the +# name of the nodeset for the -x, -y, and +y boundaries. # -x face [pylithapp.problem.bc.x_neg] -bc_dof = [0] label = boundary_xneg_nofault -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x # -y face [pylithapp.problem.bc.y_neg] -bc_dof = [1] label = boundary_yneg_nofault -db_initial.label = Dirichlet BC on -y # +y face [pylithapp.problem.bc.y_pos] -bc_dof = [1] label = boundary_ypos_nofault -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z # ---------------------------------------------------------------------- # faults diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg index 425eabe977..976f8094b6 100644 --- a/examples/3d/subduction/step05.cfg +++ b/examples/3d/subduction/step05.cfg @@ -23,7 +23,13 @@ # the bottom of the slab. We use Dirichlet boundary conditions to # constrain the displacements on the lateral and bottom boundaries. # -# We use the same material properties as step02. +# Materials +# The 'wedge' and 'crust' blocks use the the linear, isotropic +# elastic material model, whereas the 'slab' and 'mantle' use the +# linear Maxwell viscoelastic material model (mat_viscoelastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -63,52 +69,23 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. Because the -# slab intersects the boundaries of the domain, and PyLith does not -# permit overlap between the fault interfaces and Dirichlet boundary -# conditions, for the Dirichlet boundary conditions we use the -# nodesets which exclude vertices on the fault. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. +# Because the slab intersects the boundaries of the domain, and PyLith +# does not permit overlap between the fault interfaces and Dirichlet +# boundary conditions, for the Dirichlet boundary conditions we use +# the nodesets which exclude vertices on the fault. We only update the +# name of the nodeset for the -x, -y, and +y boundaries. # -x face [pylithapp.problem.bc.x_neg] -bc_dof = [0] label = boundary_xneg_nofault -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x # -y face [pylithapp.problem.bc.y_neg] -bc_dof = [1] label = boundary_yneg_nofault -db_initial.label = Dirichlet BC on -y # +y face [pylithapp.problem.bc.y_pos] -bc_dof = [1] label = boundary_ypos_nofault -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z # ---------------------------------------------------------------------- # faults diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 7c82da3ef4..52c3a8975c 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -72,52 +72,6 @@ output = [domain, subdomain, cgps_sites] output.subdomain = pylith.meshio.OutputSolnSubset output.cgps_sites = pylith.meshio.OutputSolnPoints -# ---------------------------------------------------------------------- -# boundary conditions -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. - -# -x face -[pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x - -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index b51df1ba44..6ae3e089d0 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -23,6 +23,12 @@ # slip distribution. This problem is used to generate synthetic # data at cGPS locations. # +# Materials +# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -59,52 +65,6 @@ problem.progress_monitor.filename = output/step07a-progress.txt total_time = 1.0*year dt = 0.05*year -# ---------------------------------------------------------------------- -# boundary conditions -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. - -# -x face -[pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x - -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 8dc595c511..46d0477d5d 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -23,6 +23,12 @@ # Note that we change the default problem type from TimeDependent to # GreensFns. # +# Materials +# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -51,52 +57,6 @@ dump_parameters.filename = output/step07b-parameters.json problem.progress_monitor.filename = output/step07b-progress.txt -# ---------------------------------------------------------------------- -# boundary conditions -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. - -# -x face -[pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x - -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg index eb832796ba..13b57d8bd8 100644 --- a/examples/3d/subduction/step07c.cfg +++ b/examples/3d/subduction/step07c.cfg @@ -24,6 +24,12 @@ # Note that we change the default problem type from TimeDependent to # GreensFns. # +# Materials +# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -52,52 +58,6 @@ dump_parameters.filename = output/step07c-parameters.json problem.progress_monitor.filename = output/step07c-progress.txt -# ---------------------------------------------------------------------- -# boundary conditions -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We constrain the DOF normal to each of the boundaries. -# -# Array of boundary conditions (defaults to DirichletBC): -# x_neg (ZeroDispDB to specify zero x-displacement) -# x_pos (ZeroDispDB to specify zero x-displacement) -# y_neg (ZeroDispDB to specify zero y-displacement) -# y_pos (ZeroDispDB to specify zero y-displacement) -# z_neg (ZeroDispDB to specify zero z-displacement) -bc = [x_neg, x_pos, y_neg, y_pos, z_neg] - -# The label corresponds to the name of the nodeset in CUBIT. - -# -x face -[pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -db_initial.label = Dirichlet BC on -x - -# +x face -[pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos -db_initial.label = Dirichlet BC on +x - -# -y face -[pylithapp.problem.bc.y_neg] -bc_dof = [1] -label = boundary_yneg -db_initial.label = Dirichlet BC on -y - -# +y face -[pylithapp.problem.bc.y_pos] -bc_dof = [1] -label = boundary_ypos -db_initial.label = Dirichlet BC on +y - -# -z face -[pylithapp.problem.bc.z_neg] -bc_dof = [2] -label = boundary_zneg -db_initial.label = Dirichlet BC on -z - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- From c6db2fc115a183b48aa29e5bf1b7c39eec9d26a3 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 19 Jun 2017 10:34:31 +1200 Subject: [PATCH 057/216] Changed settings to provide a SSE more suitable for inversion. --- examples/3d/subduction/spatialdb/generate_slowslip.cfg | 4 ++-- examples/3d/subduction/spatialdb/generate_slowslip.py | 6 +++--- 2 files changed, 5 insertions(+), 5 deletions(-) diff --git a/examples/3d/subduction/spatialdb/generate_slowslip.cfg b/examples/3d/subduction/spatialdb/generate_slowslip.cfg index 002e27797f..6c3539da1d 100644 --- a/examples/3d/subduction/spatialdb/generate_slowslip.cfg +++ b/examples/3d/subduction/spatialdb/generate_slowslip.cfg @@ -1,8 +1,8 @@ [generate_slowslip] rake = 45.0 -slip_center = [-124.5, 45.5] +slip_center = [-124.0, 45.5] slip_radius = 0.7 -slip_max = 5.0 +slip_max = 8.0 slip_sigma_lon = 0.3 slip_sigma_lat = 0.3 diff --git a/examples/3d/subduction/spatialdb/generate_slowslip.py b/examples/3d/subduction/spatialdb/generate_slowslip.py index 78ba080830..c4c87503c6 100755 --- a/examples/3d/subduction/spatialdb/generate_slowslip.py +++ b/examples/3d/subduction/spatialdb/generate_slowslip.py @@ -15,14 +15,14 @@ from pyre.applications.Script import Script as Application -class SynthGaussian(Application): +class GenerateSlowslip(Application): """ Python application to create spatial databases for a synthetic SSE with time-varying Gaussian slip. """ import pyre.inventory - ## Python object for managing SynthGaussian facilities and properties. + ## Python object for managing GenerateSlowslip facilities and properties. ## ## \b Properties ## @li \b rake Rake of fault slip (degrees). @@ -239,7 +239,7 @@ def _writeTemporaldb(self): # ---------------------------------------------------------------------- if __name__ == '__main__': - app = SynthGaussian() + app = GenerateSlowslip() app.run() # End of file From 74debfcd22598c4dfe9d2913c247a4a68aa526a1 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 19 Jun 2017 11:11:22 +1200 Subject: [PATCH 058/216] Updated script to use user-defined time step and added .cfg file. Updated step06.cfg for new spatial database filenames. --- .../3d/subduction/make_synthetic_gpsdisp.cfg | 7 +++++ .../3d/subduction/make_synthetic_gpsdisp.py | 26 ++++++++++++------- examples/3d/subduction/step06.cfg | 4 +-- 3 files changed, 26 insertions(+), 11 deletions(-) create mode 100644 examples/3d/subduction/make_synthetic_gpsdisp.cfg diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.cfg b/examples/3d/subduction/make_synthetic_gpsdisp.cfg new file mode 100644 index 0000000000..b3164b9907 --- /dev/null +++ b/examples/3d/subduction/make_synthetic_gpsdisp.cfg @@ -0,0 +1,7 @@ +[make_synthetic_gpsdisp] +point_input_file = output/step06-cgps_sites.h5 +time_step = 11 +sigma_east = 0.0005 +sigma_north = 0.0005 +sigma_up = 0.001 +output_file = cgps_synthetic_displacement.txt diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index 1a4412d9fb..ae2a46e538 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -7,19 +7,21 @@ import math import numpy import h5py +# import pdb from pyre.applications.Script import Script as Application -class MakeSynthData(Application): +class MakeSyntheticGpsdisp(Application): """ Python application to create synthetic data from PyLith points output. """ import pyre.inventory - ## Python object for managing MakeSynthData facilities and properties. + ## Python object for managing MakeSyntheticGpsdisp facilities and properties. ## ## \b Properties ## @li \b point_input_file HDF5 input file generated by PyLith. + ## @li \b time_step Time step to use for data generation. ## @li \b sigma_east Sigma value for east displacements. ## @li \b sigma_north Sigma value for north displacements. ## @li \b sigma_up Sigma value for up displacements. @@ -29,6 +31,9 @@ class MakeSynthData(Application): pointInputFile = pyre.inventory.str("point_input_file", default="cascadia-cgps_points.h5") pointInputFile.meta['tip'] = "HDF5 point output file from PyLith." + timeStep = pyre.inventory.int("time_step", default=0) + timeStep.meta['tip'] = "Time step to use for data generation." + sigmaEast = pyre.inventory.float("sigma_east", default=0.0005) sigmaEast.meta['tip'] = "Sigma value for East displacements." @@ -58,6 +63,7 @@ def __init__(self, name="make_synthetic_gpsdisp"): def main(self): + # pdb.set_trace() self._readHDF5() self._addNoise() self._writeOutput() @@ -85,8 +91,8 @@ def _readHDF5(self): h5 = h5py.File(self.pointInputFile, 'r') self.coords = h5['geometry/vertices'][:] self.stations = h5['stations'][:] - self.dispRaw = h5['vertex_fields/displacement'][0,:,:] - hf.close() + self.dispRaw = h5['vertex_fields/displacement'][self.timeStep,:,:] + h5.close() self.numStations = self.coords.shape[0] @@ -97,9 +103,10 @@ def _addNoise(self): """ Function to add noise to computed displacements. """ - self.dispNoise[:,0] = self.dispRaw[:,0] + self.sigmaEast * numpy.random.randn(self.numStations) - self.dispNoise[:,1] = self.dispRaw[:,1] + self.sigmaNorth * numpy.random.randn(self.numStations) - self.dispNoise[:,2] = self.dispRaw[:,2] + self.sigmaUp * numpy.random.randn(self.numStations) + self.dispNoise = self.dispRaw.copy() + self.dispNoise[:,0] += self.sigmaEast * numpy.random.randn(self.numStations) + self.dispNoise[:,1] += self.sigmaNorth * numpy.random.randn(self.numStations) + self.dispNoise[:,2] += self.sigmaUp * numpy.random.randn(self.numStations) return @@ -114,7 +121,8 @@ def _writeOutput(self): f.write(head) for stationNum in range(self.numStations): - outLine = outFmt % (self.coords[stationNum,0], self.coords[stationNum,1], + outLine = outFmt % (self.stations[stationNum], + self.coords[stationNum,0], self.coords[stationNum,1], self.coords[stationNum,2], self.dispNoise[stationNum,0], self.dispNoise[stationNum,1], @@ -129,7 +137,7 @@ def _writeOutput(self): # ---------------------------------------------------------------------- if __name__ == '__main__': - app = MakeSynthData() + app = MakeSyntheticGpsdisp() app.run() # End of file diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 52c3a8975c..a54caf59d4 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -99,7 +99,7 @@ slip_function = pylith.faults.TimeHistorySlipFn [pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] slip = spatialdata.spatialdb.SimpleGridDB slip.label = Gaussian slip distribution for SSE -slip.filename = spatialdb/sse_slip.spatialdb +slip.filename = spatialdb/fault_slabtop_slowslip.spatialdb # Use linear interpolation. slip.query_type = linear @@ -112,7 +112,7 @@ slip_time.data = [0.0*year] # We use a temporal database to provide the slip time history. time_history.label = Time history of slip -time_history.filename = spatialdb/sse_slip.timedb +time_history.filename = spatialdb/fault_slabtop_slowslip.timedb # ---------------------------------------------------------------------- # output From 0046624f9b63738cadc8d103904ba305518b1055 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 19 Jun 2017 11:45:21 +1200 Subject: [PATCH 059/216] Modified step07 files so that we are only generating GF, and modified filenames accordingly. --- examples/3d/subduction/step07a.cfg | 94 +++++++------------ examples/3d/subduction/step07b.cfg | 23 +++-- examples/3d/subduction/step07c.cfg | 57 ++++++----- examples/3d/subduction/step07d.cfg | 146 +++++++++++++++++++++++++++++ 4 files changed, 233 insertions(+), 87 deletions(-) create mode 100644 examples/3d/subduction/step07d.cfg diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 6ae3e089d0..8fadafb216 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -16,12 +16,22 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions and prescribed fault slip to -# simulate a coseismic event on the subductin interface. Fault slip -# is specified with a spatialdb to provide an approximately Gaussian -# slip distribution. This problem is used to generate synthetic -# data at cGPS locations. +# In this problem we generate Green's functions that will be used +# to invert synthetic data generated from step06. There are four +# different sub-problems: +# step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# step07b: Generate Green's functions corresponding to updip +# slip on the subduction interface (slab top). +# step07c: Generate Green's functions corresponding to left-lateral +# slip on the splay fault. +# step07d: Generate Green's functions corresponding to updip +# slip on the splay fault. +# +# Responses (Green's functions) are computed at simulated cGPS +# locations defined in the file cgps_sites.txt. +# Note that we change the default problem type from TimeDependent to +# GreensFns. # # Materials # All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). @@ -35,6 +45,7 @@ # # Parameter files: # - pylithapp.cfg (common paramters, read by default) +# - greensfns.cfg (greensfns paramters, read by default) # - step07a.cfg (main parameter file for step07a) # - mat_elastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) @@ -45,7 +56,7 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg +# pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. @@ -56,15 +67,6 @@ dump_parameters.filename = output/step07a-parameters.json problem.progress_monitor.filename = output/step07a-progress.txt -# ---------------------------------------------------------------------- -# problem -# ---------------------------------------------------------------------- -[pylithapp.problem.formulation.time_step] -# This is a static problem so there is only a single time step. -# Define the total time for the simulation and the time step size. -total_time = 1.0*year -dt = 0.05*year - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- @@ -73,9 +75,10 @@ dt = 0.05*year interfaces = [slab] [pylithapp.problem.interfaces] -slab = pylith.faults.FaultCohesiveKin +slab = pylith.faults.FaultCohesiveImpulses [pylithapp.problem.interfaces.slab] +id = 100 label = fault_slabtop_patch edge = fault_slabtop_patch_edge @@ -84,47 +87,19 @@ edge = fault_slabtop_patch_edge quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 2 -# We use the default step-function slip time function. -[pylithapp.problem.interfaces.slab.eq_srcs.rupture] -slip_function = pylith.faults.TimeHistorySlipFn - - -# The slip is defined in a SimpleGridDB spatial database. -[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] -slip = spatialdata.spatialdb.SimpleGridDB -slip.label = Gaussian slip distribution for earthquake -slip.filename = spatialdb/fault_slabtop_slowslip.spatialdb -slip.query_type = linear - -# We use a UniformDB to specify the slip initiation time. -slip_time = spatialdata.spatialdb.UniformDB -slip_time.label = Slip initiation time -slip_time.values = [slip-time] -slip_time.data = [0.0*year] - -# User time history slip function -time_history.label = Slow slip time history function -time_history.filename = spatialdb/fault_slabtop_slowslip.timedb - -# Output -[pylithapp.problem.interfaces.slab.output] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07a-fault-slab.h5 +# Label and query type for fault slip. +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.query_type = nearest -# We want both orientation and slip information in the information file. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] +# Spatialdb for impulses. +impulse_dof = [0] +db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- -# For this problem, we want output over the entire domain, for the -# ground surface, and at simulated cGPS locations. -[pylithapp.problem.implicit] +[pylithapp.problem.formulation] output = [domain, subdomain, cgps_sites] - -# Default output is for the entire domain. -# We need to set the type of output for the subdomain and points. -output.subdomain = pylith.meshio.OutputSolnSubset output.cgps_sites = pylith.meshio.OutputSolnPoints # Domain, subdomain, and points output --------------------------------- @@ -135,21 +110,24 @@ vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] writer.filename = output/step07a-groundsurf.h5 +# Turn off data fields. +vertex_data_fields = [] -# Specify output type, coordinate system, and station file for cgps_sites. [pylithapp.problem.formulation.output.cgps_sites] -# We will use a geographic coordinate system for the cGPS sites file. coordsys = spatialdata.geocoords.CSGeo coordsys.space_dim = 3 coordsys.datum_horiz = WGS84 coordsys.datum_vert = mean sea level - -# Use HDF5 output. writer = pylith.meshio.DataWriterHDF5 +reader.filename = cgps_sites.txt + writer.filename = output/step07a-cgps_sites.h5 -# Simulated cGPS station file. -reader.filename = cgps_sites.txt +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-fault-slab.h5 # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 46d0477d5d..60fb6186b7 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -16,10 +16,20 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions to generate Green's functions -# for a patch on the subduction interface. Responses are computed -# at simulated cGPS locations. +# In this problem we generate Green's functions that will be used +# to invert synthetic data generated from step06. There are four +# different sub-problems: +# step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# step07b: Generate Green's functions corresponding to updip +# slip on the subduction interface (slab top). +# step07c: Generate Green's functions corresponding to left-lateral +# slip on the splay fault. +# step07d: Generate Green's functions corresponding to updip +# slip on the splay fault. +# +# Responses (Green's functions) are computed at simulated cGPS +# locations defined in the file cgps_sites.txt. # Note that we change the default problem type from TimeDependent to # GreensFns. # @@ -82,10 +92,9 @@ db_impulse_amplitude.label = Amplitude of fault slip impulses db_impulse_amplitude.query_type = nearest # Spatialdb for impulses. -impulse_dof = [0] +impulse_dof = [1] db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- @@ -101,6 +110,8 @@ vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] writer.filename = output/step07b-groundsurf.h5 +# Turn off data fields. +vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] coordsys = spatialdata.geocoords.CSGeo diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg index 13b57d8bd8..30a99a7b36 100644 --- a/examples/3d/subduction/step07c.cfg +++ b/examples/3d/subduction/step07c.cfg @@ -16,11 +16,20 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions to generate Green's functions -# for a patch on the subduction interface. Responses are computed -# at simulated cGPS locations. This problem computes the responses -# to updip slip. +# In this problem we generate Green's functions that will be used +# to invert synthetic data generated from step06. There are four +# different sub-problems: +# step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# step07b: Generate Green's functions corresponding to updip +# slip on the subduction interface (slab top). +# step07c: Generate Green's functions corresponding to left-lateral +# slip on the splay fault. +# step07d: Generate Green's functions corresponding to updip +# slip on the splay fault. +# +# Responses (Green's functions) are computed at simulated cGPS +# locations defined in the file cgps_sites.txt. # Note that we change the default problem type from TimeDependent to # GreensFns. # @@ -47,9 +56,9 @@ # simulations, so we put them in a separate file. # # To run the simulation: -# pylith --problem=pylith.problems.GreensFns step07c.cfg mat_elastic.cfg solver_fieldsplit.cfg +# pylith --problem=pylith.problems.GreensFns step07c.cfg mat_elastic.cfg solver_fieldsplit.cfg # -# Output will be directed to the "output" directory. +# Output will be directed to the "output" directory.. # ---------------------------------------------------------------------- # Output of parameters used and simulation progress. @@ -62,16 +71,16 @@ problem.progress_monitor.filename = output/step07c-progress.txt # faults # ---------------------------------------------------------------------- [pylithapp.problem] -# We prescribe slip on the slab fault patch. -interfaces = [slab] +# We prescribe slip on the splay fault patch. +interfaces = [splay] [pylithapp.problem.interfaces] -slab = pylith.faults.FaultCohesiveImpulses +splay = pylith.faults.FaultCohesiveImpulses -[pylithapp.problem.interfaces.slab] +[pylithapp.problem.interfaces.splay] id = 100 -label = fault_slabtop_patch -edge = fault_slabtop_patch_edge +label = fault_splay_patch +edge = fault_splay_patch_edge # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). @@ -83,17 +92,11 @@ db_impulse_amplitude.label = Amplitude of fault slip impulses db_impulse_amplitude.query_type = nearest # Spatialdb for impulses. -impulse_dof = [1] +impulse_dof = [0] db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb -# Output -[pylithapp.problem.interfaces.slab.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07c-fault-slab.h5 - # ---------------------------------------------------------------------- -# Output +# output # ---------------------------------------------------------------------- [pylithapp.problem.formulation] output = [domain, subdomain, cgps_sites] @@ -101,12 +104,14 @@ output.cgps_sites = pylith.meshio.OutputSolnPoints # Domain, subdomain, and points output --------------------------------- [pylithapp.problem.formulation.output.domain] -writer.filename = output/step07b-domain.h5 +writer.filename = output/step07c-domain.h5 # Turn off data fields. vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] -writer.filename = output/step07b-groundsurf.h5 +writer.filename = output/step07c-groundsurf.h5 +# Turn off data fields. +vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] coordsys = spatialdata.geocoords.CSGeo @@ -118,6 +123,12 @@ reader.filename = cgps_sites.txt writer.filename = output/step07c-cgps_sites.h5 +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.splay.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07c-fault-splay.h5 + # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] writer.filename = output/step07c-slab.h5 diff --git a/examples/3d/subduction/step07d.cfg b/examples/3d/subduction/step07d.cfg new file mode 100644 index 0000000000..d4c7fe1c6d --- /dev/null +++ b/examples/3d/subduction/step07d.cfg @@ -0,0 +1,146 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# In this problem we generate Green's functions that will be used +# to invert synthetic data generated from step06. There are four +# different sub-problems: +# step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# step07b: Generate Green's functions corresponding to updip +# slip on the subduction interface (slab top). +# step07c: Generate Green's functions corresponding to left-lateral +# slip on the splay fault. +# step07d: Generate Green's functions corresponding to updip +# slip on the splay fault. +# +# Responses (Green's functions) are computed at simulated cGPS +# locations defined in the file cgps_sites.txt. +# Note that we change the default problem type from TimeDependent to +# GreensFns. +# +# Materials +# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - greensfns.cfg (greensfns paramters, read by default) +# - step07d.cfg (main parameter file for step07d) +# - mat_elastic.cfg (material models and parameters) +# - solver_fieldsplit.cfg (field split solver settings) +# +# We use the field split preconditioner with algebraic multigrid for +# the displacement fields and the custom preconditioner for the +# Lagrange multiplier field. We use these solver settings in several +# simulations, so we put them in a separate file. +# +# To run the simulation: +# pylith --problem=pylith.problems.GreensFns step07d.cfg mat_elastic.cfg solver_fieldsplit.cfg +# +# Output will be directed to the "output" directory.. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step07d-parameters.json +problem.progress_monitor.filename = output/step07d-progress.txt + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.problem] +# We prescribe slip on the splay fault patch. +interfaces = [splay] + +[pylithapp.problem.interfaces] +splay = pylith.faults.FaultCohesiveImpulses + +[pylithapp.problem.interfaces.splay] +id = 100 +label = fault_splay_patch +edge = fault_splay_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Label and query type for fault slip. +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.query_type = nearest + +# Spatialdb for impulses. +impulse_dof = [1] +db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +output = [domain, subdomain, cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# Domain, subdomain, and points output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step07d-domain.h5 +# Turn off data fields. +vertex_data_fields = [] + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step07d-groundsurf.h5 +# Turn off data fields. +vertex_data_fields = [] + +[pylithapp.problem.formulation.output.cgps_sites] +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level +writer = pylith.meshio.DataWriterHDF5 +reader.filename = cgps_sites.txt + +writer.filename = output/step07d-cgps_sites.h5 + +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.splay.output] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07d-fault-splay.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step07d-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step07d-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step07d-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step07d-mantle.h5 + + +# End of file From 44179ac8d5408cf199eb6f80c990b83ec78c8c1d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 18 Jun 2017 17:02:05 -0700 Subject: [PATCH 060/216] Add missing label. --- examples/3d/subduction/mat_viscoelastic.cfg | 2 ++ 1 file changed, 2 insertions(+) diff --git a/examples/3d/subduction/mat_viscoelastic.cfg b/examples/3d/subduction/mat_viscoelastic.cfg index 45bfe74cc3..e34505698b 100644 --- a/examples/3d/subduction/mat_viscoelastic.cfg +++ b/examples/3d/subduction/mat_viscoelastic.cfg @@ -30,6 +30,7 @@ mantle = pylith.materials.MaxwellIsotropic3D # Slab [pylithapp.problem.materials.slab] db_properties = spatialdata.spatialdb.CompositeDB +db_properties.label = Composite spatial database for slab material properties [pylithapp.timedependent.materials.slab.db_properties] # Elastic properties @@ -54,6 +55,7 @@ db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb # Mantle [pylithapp.problem.materials.mantle] db_properties = spatialdata.spatialdb.CompositeDB +db_properties.label = Composite spatial database for mantle material properties [pylithapp.timedependent.materials.mantle.db_properties] # Elastic properties From e791c4a40c01e9a5915b53c715c90b81045d6286 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 18 Jun 2017 17:02:35 -0700 Subject: [PATCH 061/216] Added ParaView Python script for plotting fault directions (strike, dip, normal). --- examples/3d/subduction/viz/plot_faultdir.py | 124 ++++++++++++++++++++ 1 file changed, 124 insertions(+) create mode 100755 examples/3d/subduction/viz/plot_faultdir.py diff --git a/examples/3d/subduction/viz/plot_faultdir.py b/examples/3d/subduction/viz/plot_faultdir.py new file mode 100755 index 0000000000..b0e617119d --- /dev/null +++ b/examples/3d/subduction/viz/plot_faultdir.py @@ -0,0 +1,124 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the fault +# surfaces, colored by the magnitude of fault slip. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. + +# Root name for simulation. +SIM_NAME = "step02" + +# Names of faults for output files. +FAULTS = ["fault-slab"] +FIELD = "strike_dir" + +# ---------------------------------------------------------------------- +from paraview.simple import * +import os + +def visualize(sim, faults, direction): + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read domain data + filename = "output/%s-domain.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[filename]) + RenameSource("%s-domain" % sim, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Gray wireframe for undeformed domain. + domainDisplay = Show(dataDomain, view) + domainDisplay.Representation = 'Wireframe' + domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + + # Read fault data + dataFaults = [] + for fault in faults: + filename = "output/%s-%s_info.xmf" % (sim, fault) + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + data = XDMFReader(FileNames=[filename]) + RenameSource("%s-%s" % (sim, fault), data) + dataFaults.append(data) + + groupFaults = GroupDatasets(Input=dataFaults) + + faultDisplay = Show(groupFaults, view) + faultDisplay.SetRepresentationType('Surface With Edges') + faultDisplayProperties = GetDisplayProperties(groupFaults, view=view) + faultDisplayProperties.DiffuseColor = [0.25, 0.25, 1.0] + + # Add arrows to show displacement vectors. + glyph = Glyph(Input=groupFaults, GlyphType="Arrow") + glyph.Vectors = ["POINTS", direction] + glyph.GlyphMode = "All Points" + + glyphDisplay = Show(glyph, view) + glyphDisplay.Representation = "Surface" + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--faults", action="store", dest="faults") + parser.add_argument("--direction", action="store", dest="direction") + args = parser.parse_args() + + sim = args.sim + if args.faults: + faults = args.faults.split(",") + else: + faults = None + direction = args.directions + + if sim is None: + sim = SIM_NAME + if faults is None: + faults = FAULTS + if direction is None: + direction = FIELD + + visualize(sim, faults, direction) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, FAULTS, FIELD) + + +# End of file From cd97dc6ada3419ace7d928ab407616d9f3c4680a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 18 Jun 2017 21:59:40 -0700 Subject: [PATCH 062/216] Add ParaView Python script for plotting slip and ratio of shear/normal traction. --- .../subduction/viz/plot_faultslip-reltract.py | 137 ++++++++++++++++++ 1 file changed, 137 insertions(+) create mode 100644 examples/3d/subduction/viz/plot_faultslip-reltract.py diff --git a/examples/3d/subduction/viz/plot_faultslip-reltract.py b/examples/3d/subduction/viz/plot_faultslip-reltract.py new file mode 100644 index 0000000000..0c75ca68ab --- /dev/null +++ b/examples/3d/subduction/viz/plot_faultslip-reltract.py @@ -0,0 +1,137 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the fault +# surfaces, colored by the magnitude of fault slip. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. + +# Root name for simulation. +SIM_NAME = "step05" + +# Names of faults for output files. +FAULTS = ["fault-slab"] + +# ---------------------------------------------------------------------- +from paraview.simple import * +import os +import numpy + +def visualize(sim, faults): + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read domain data + filename = "output/%s-domain.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[filename]) + RenameSource("%s-domain" % sim, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Gray wireframe for undeformed domain. + domainDisplay = Show(dataDomain, view) + domainDisplay.Representation = 'Wireframe' + domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + + # Read fault data + dataFaults = [] + for fault in faults: + filename = "output/%s-%s.xmf" % (sim, fault) + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + data = XDMFReader(FileNames=[filename]) + RenameSource("%s-%s" % (sim, fault), data) + dataFaults.append(data) + + groupFaults = GroupDatasets(Input=dataFaults) + + # Ratio of shear to normal traction + calculator = Calculator(Input=groupFaults) + calculator.Function = 'mag(traction_X*iHat+traction_Y*jHat)/abs(traction_Z)' + calculator.ResultArrayName = 'shearDivNormal' + + ratioDisplay = Show(groupFaults, view) + ColorBy(ratioDisplay, ('POINTS', 'shearDivNormal')) + ratioDisplay.RescaleTransferFunctionToDataRange(True) + ratioDisplay.SetScalarBarVisibility(view, True) + ratioDisplay.SetRepresentationType('Surface With Edges') + + # Rescale color and/or opacity maps used to exactly fit the current data range + ratioLUT = GetColorTransferFunction('shearDivNormal') + ratioDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update a scalar bar component title. + UpdateScalarBarsComponentTitle(ratioLUT, ratioDisplay) + + calculator = Calculator(Input=groupFaults) + calculator.Function = 'mag(slip)' + calculator.ResultArrayName = 'slipMag' + + contour = Contour(Input=groupFaults) + contour.ContourBy = ['POINTS', 'slipMag'] + contour.Isosurfaces = numpy.arange(0.0, 4.01, 0.5) + contour.PointMergeMethod = 'Uniform Binning' + + contourDisplay = Show(contour, view) + + + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--faults", action="store", dest="faults") + args = parser.parse_args() + + sim = args.sim + if args.faults: + faults = args.faults.split(",") + else: + faults = None + + if sim is None: + sim = SIM_NAME + if faults is None: + faults = FAULTS + + visualize(sim, faults) + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, FAULTS) + + +# End of file From e2c042f2f7d4129297cb16126b273ba80680055d Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 19 Jun 2017 18:41:17 +1200 Subject: [PATCH 063/216] Removed GF for splay fault, and modified files accordingly. Write Python inversion code and corresponding .cfg file. Still need to check parameter settings. --- examples/3d/subduction/slip_invert.cfg | 13 + examples/3d/subduction/slip_invert.py | 482 +++++++++++++++++++++++++ examples/3d/subduction/step07a.cfg | 6 +- examples/3d/subduction/step07b.cfg | 6 +- examples/3d/subduction/step07c.cfg | 146 -------- examples/3d/subduction/step07d.cfg | 146 -------- 6 files changed, 497 insertions(+), 302 deletions(-) create mode 100644 examples/3d/subduction/slip_invert.cfg create mode 100755 examples/3d/subduction/slip_invert.py delete mode 100644 examples/3d/subduction/step07c.cfg delete mode 100644 examples/3d/subduction/step07d.cfg diff --git a/examples/3d/subduction/slip_invert.cfg b/examples/3d/subduction/slip_invert.cfg new file mode 100644 index 0000000000..e53ca3768a --- /dev/null +++ b/examples/3d/subduction/slip_invert.cfg @@ -0,0 +1,13 @@ +[slip_invert] +data_file = cgps_synthetic_displacement.txt +rake = 45.0*degree +gfimpulses_ll_file = output/step07a-fault-slab.h5 +gfimpulses_ud_file = output/step07b-fault-slab.h5 +gfresponses_ll_file = output/step07a-cgps_sites.h5 +gfresponses_ud_file = output/step07b-cgps_sites.h5 +a_priori_value = 0.0 +penalty_weight_vals = [1.0,2.0,5.0,10.0,20.0,50.0,100.0] +data_scale = 1.0 +result_summary_file = step07-inversion-summary.txt +slip_output_file = step07-inversion-slip.h5 +displacement_output_file = step07-inversion-displacement.h5 diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py new file mode 100755 index 0000000000..a3494a2e06 --- /dev/null +++ b/examples/3d/subduction/slip_invert.py @@ -0,0 +1,482 @@ +#!/usr/bin/env python +# -*- Python -*- (syntax highlighting) +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# Simple inversion script that uses PyLith-generated Green's functions. +# NOTE: This script assumes that you have PETSc installed, and that you +# have PETSC_DIR set as an environmental variable. +# + +import math +import numpy +import sys +import os +from pyre.units.angle import degree +import h5py + +from pyre.applications.Script import Script as Application + +class SlipInvert(Application): + """ + Python application to perform a linear inversion for slip using + PyLith-generated Green's functions. + """ + + ## \b Properties + ## @li \b data_file File with displacements, locations, and stdDev. + ## @li \b rake Assumed rake direction. + ## @li \b gfimpulses_ll_file HDF5 file with left-lateral GF impulses. + ## @li \b gfimpulses_ud_file HDF5 file with updip GF impulses. + ## @li \b gfresponses_ll_file HDF5 file with left-lateral GF responses. + ## @li \b gfresponses_ud_file HDF5 file with updip GF responses. + ## @li \b a_priori_value A priori value for parameters. + ## @li \b penalty_weight_vals List of penalty weights. + ## @li \b data_scale Scaling factor to apply to data and stdDev. + ## @li \b result_summary_file Text file summarizing inversion results. + ## @li \b slip_output_file Output file with slip results. + ## @li \b displacement_output_file Output file with inversion results. + ## + ## \b Facilities + ## @li None + + import pyre.inventory + + dataFile = pyre.inventory.str("data_file", default="data.txt") + dataFile.meta['tip'] = "File with displ., locations, and stdDev." + + rake = pyre.inventory.dimensional("rake", default=90.0*degree) + rake.meta['tip'] = "Assumed rake angle." + + gfImpulsesLlFile = pyre.inventory.str("gfimpulses_ll_file", + default="gfimpulse_ll.h5") + gfImpulsesLlFile.meta['tip'] = "HDF5 file with left-lateral GF impulses." + + gfImpulsesUdFile = pyre.inventory.str("gfimpulses_ud_file", + default="gfimpulse_ud.h5") + gfImpulsesUdFile.meta['tip'] = "HDF5 file with updip GF impulses." + + gfResponsesLlFile = pyre.inventory.str("gfresponses_ll_file", + default="gfresponse_ll.h5") + gfResponsesLlFile.meta['tip'] = "HDF5 file with left-lateral GF responses." + + gfResponsesUdFile = pyre.inventory.str("gfresponses_ud_file", + default="gfresponse_ud.h5") + gfResponsesUdFile.meta['tip'] = "HDF5 file with updip GF responses." + + aPrioriValue = pyre.inventory.float("a_priori_value", default=0.0) + aPrioriValue.meta['tip'] = "A priori value for parameters." + + penaltyWeightVals = pyre.inventory.list("penalty_weight_vals", + default=[0.1,0.5,1.0,5.0,10.0]) + penaltyWeightVals.meta['tip'] = "List of penalty weights." + + dataScale = pyre.inventory.float("data_scale", default=1.0) + dataScale.meta['tip'] = "Scaling factor to apply to data and stdDev." + + resultSummaryFile = pyre.inventory.str("result_summary_file", + default='result_summary.txt') + resultSummaryFile.meta['tip'] = "Text file summarizing inversion results." + + slipOutputFile = pyre.inventory.str("slip_output_file", + default='predicted_slip.h5') + slipOutputFile.meta['tip'] = "HDF5 file with predicted slip results." + + displacementOutputFile = pyre.inventory.str("displacement_output_file", + default='predicted_displacement.h5') + displacementOutputFile.meta['tip'] = "HDF5 file with predicted displacements." + + + # PUBLIC METHODS ///////////////////////////////////////////////////// + + def __init__(self, name="slip_invert"): + Application.__init__(self, name) + + self.dataCoords = None + self.dataVals = None + self.dataCov = None + self.dataNames = [] + self.numDataPoints = 0 + self.numDesignRows = 0 + + self.numFaultVerts = 0 + self.numFaultCells = 0 + self.faultVertCoords = None + self.faultCells = None + + self.numImpulses = 0 + self.impulseInds = None + self.impulseCoords = None + + self.summaryHead = 'Penalty-weight\tData-residual\t' + \ + 'Weighted-data-residual\tPenalty-residual\t' + \ + 'Weighted-penalty-residual\tTotal-residual\t' + \ + 'Total-weighted-residual' + self.numSummaryCols = 7 + + self.design = None + + return + + + def main(self): + import pdb + pdb.set_trace() + self.readData() + self.readGreens() + self.runInversions() + return + + + # PRIVATE METHODS //////////////////////////////////////////////////// + + def _configure(self): + """ + Setup members using inventory. + """ + Application._configure(self) + self.penaltyWeights = numpy.array(self.penaltyWeightVals, + dtype=numpy.float64) + self.numPenaltyWeights = self.penaltyWeights.shape[0] + + # Left-lateral and updip components from assumed rake. + self.llComp = math.cos(self.rake.value) + self.udComp = math.sin(self.rake.value) + + petscDir = os.environ['PETSC_DIR'] + self.genXdmfCmd = petscDir + "/bin/petsc_gen_xdmf.py " + + return + + + def runInversions(self): + """ + Function to run inversions using a range of penalty parameters. + """ + print "Running inversions:" + sys.stdout.flush() + + # Open output files. + d = h5py.File(self.displacementOutputFile, 'w') + s = h5py.File(self.slipOutputFile, 'w') + + # Write fault mesh and time info. + summaryInfo = numpy.zeros((self.numPenaltyWeights, self.numSummaryCols), + dtype=numpy.float64) + cellDimF = 2 + timesF = self.penaltyWeights.reshape(self.numPenaltyWeights, 1, 1) + vertsF = s.create_dataset('geometry/vertices', data=self.faultVertCoords) + timesF = s.create_dataset('time', data=timesF, maxshape=(None, 1, 1)) + topoF = s.create_dataset('topology/cells', data=self.faultCells, dtype='d') + topoF.attrs['cell_dim'] = numpy.int32(cellDimF) + totSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), + dtype=numpy.float64) + llSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), + dtype=numpy.float64) + udSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), + dtype=numpy.float64) + + # Write data mesh and time info. + cellDimD = 1 + topolD = numpy.arange(self.numDataPoints, + dtype=numpy.int64).reshape(self.numDataPoints, 1) + timesD = self.penaltyWeights.reshape(self.numPenaltyWeights, 1, 1) + vertsD = d.create_dataset('geometry/vertices', data=self.dataCoords) + timesD = d.create_dataset('time', data=timesD, maxshape=(None, 1, 1)) + topoD = d.create_dataset('topology/cells', data=topolD, dtype='d') + topoD.attrs['cell_dim'] = numpy.int32(cellDimD) + + dispEast = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), + dtype=numpy.float64) + dispNorth = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), + dtype=numpy.float64) + dispUp = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), + dtype=numpy.float64) + + # Indices of displacement components in solution vector. + eastBegin = 0 + eastEnd = self.numDataPoints + northBegin = eastEnd + northEnd = northBegin + self.numDataPoints + upBegin = northEnd + upEnd = northEnd + self.numDataPoints + + # Rescale equations using data standard deviations. + dataStdDev = numpy.sqrt(self.dataCov) + dataStdDevInvDiag = numpy.diag(1.0/dataStdDev) + dataScaledDesign = numpy.dot(dataStdDevInvDiag, self.design) + dataScaledVals = numpy.dot(dataStdDevInvDiag, self.dataVals) + + # Create a priori parameter vector. + paramVec = self.aPrioriValue * numpy.ones(self.numImpulses, + dtype=numpy.float64) + + summFmt = '%g' + 6 * '\t%e' + '\n' + + # Regularization array is just the identity matrix. + regArray = numpy.identity(self.numImpulses, dtype=numpy.float64) + + # Loop over inversions. + for invNum in range(self.numPenaltyWeights): + penWeight = self.penaltyWeights[invNum] + print ' Working on inversion %d, penalty weight = %g' % (invNum, + penWeight) + sys.stdout.flush() + paramScaledDesign = penWeight * regArray + paramScaledData = penWeight * paramVec + designMat = numpy.vstack((dataScaledDesign, paramScaledDesign)) + dataVec = numpy.hstack((dataScaledVals, paramScaledData)) + designMatTrans = numpy.transpose(designMat) + genInv = numpy.dot(numpy.linalg.inv(numpy.dot(designMatTrans, designMat)), + designMatTrans) + solution = numpy.dot(genInv, dataVec) + + # Compute residuals, etc. + predicted = numpy.dot(self.design, solution) + dataResidual = self.dataVals - predicted + dataWeightResidual = numpy.dot(dataStdDevInvDiag, dataResidual) + dataResidualNorm = numpy.linalg.norm(dataResidual) + dataWeightResidualNorm = numpy.linalg.norm(dataWeightResidual) + penalty = numpy.dot(regArray, solution) + penaltyResidual = paramVec - penalty + penaltyWeightResidual = penWeight * penaltyResidual + penaltyResidualNorm = numpy.linalg.norm(penaltyResidual) + penaltyWeightResidualNorm = numpy.linalg.norm(penaltyWeightResidual) + totalResidualNorm = dataResidualNorm + penaltyResidualNorm + totalWeightResidualNorm = dataWeightResidualNorm + \ + penaltyWeightResidualNorm + + summaryInfo[invNum,0] = penWeight + summaryInfo[invNum,1] = dataResidualNorm + summaryInfo[invNum,2] = dataWeightResidualNorm + summaryInfo[invNum,3] = penaltyResidualNorm + summaryInfo[invNum,4] = penaltyWeightResidualNorm + summaryInfo[invNum,5] = totalResidualNorm + summaryInfo[invNum,6] = totalWeightResidualNorm + + totSlip[invNum, self.impulseInds] = solution + llSlip[invNum, self.impulseInds] = self.llComp * solution + udSlip[invNum, self.impulseInds] = self.udComp * solution + dispEast[invNum, :] = predicted[eastBegin:eastEnd] + dispNorth[invNum, :] = predicted[northBegin:northEnd] + dispUp[invNum, :] = predicted[upBegin:upEnd] + + print ' Data residual: %e' % dataResidualNorm + print ' Weighted data residual: %e' % dataWeightResidualNorm + print ' Penalty residual: %e' % penaltyResidualNorm + print ' Weighted penalty residual: %e' % penaltyWeightResidualNorm + print ' Total residual: %e' % totalResidualNorm + print ' Weighted total residual: %e' % totalWeightResidualNorm + sys.stdout.flush() + + numpy.savetxt(self.resultSummaryFile, summaryInfo, delimiter='\t', + header=self.summaryHead) + + # Write results to HDF5 files. + slipTot = s.create_dataset('vertex_fields/total_slip', data=totSlip) + slipTot.attrs['vector_field_type'] = 'scalar' + slipLl = s.create_dataset('vertex_fields/leftlat_slip', data=llSlip) + slipLl.attrs['vector_field_type'] = 'scalar' + slipUd = s.create_dataset('vertex_fields/updip_slip', data=udSlip) + slipUd.attrs['vector_field_type'] = 'scalar' + eastDisp = d.create_dataset('vertex_fields/disp_east', data=dispEast) + eastDisp.attrs['vector_field_type'] = 'scalar' + northDisp = d.create_dataset('vertex_fields/disp_north', data=dispNorth) + northDisp.attrs['vector_field_type'] = 'scalar' + upDisp = d.create_dataset('vertex_fields/disp_ups', data=dispUp) + upDisp.attrs['vector_field_type'] = 'scalar' + + s.close() + d.close() + + os.system(self.genXdmfCmd + self.slipOutputFile) + os.system(self.genXdmfCmd + self.displacementOutputFile) + + return + + + def readGreens(self): + """ + Function to read impulse and response info from PyLith output files. + """ + print "Reading Green's functions:" + sys.stdout.flush() + + # Read impulses. + print " Reading left-lateral impulses:" + sys.stdout.flush() + impulsesLl = h5py.File(self.gfImpulsesLlFile, 'r') + self.faultVertCoords = impulsesLl['geometry/vertices'][:] + self.numFaultVerts = self.faultVertCoords.shape[0] + self.faultCells = numpy.array(impulsesLl['topology/cells'][:], + dtype=numpy.int) + self.numFaultCells = self.faultCells.shape[0] + llSlip = impulsesLl['vertex_fields/slip'][:,:,0] + llImpInds = numpy.nonzero(llSlip != 0.0) + self.impulseCoords = self.faultVertCoords[llImpInds[1]] + self.numImpulses = self.impulseCoords.shape[0] + + print " Number of fault vertices: %d" % self.numFaultVerts + print " Number of impulses: %d" % self.numImpulses + + (distances, self.impulseInds) = self.matchCoords(self.faultVertCoords, + self.impulseCoords) + impulsesLl.close() + + print " Reading updip impulses:" + sys.stdout.flush() + impulsesUd = h5py.File(self.gfImpulsesUdFile, 'r') + udCoords = impulsesUd['geometry/vertices'][:] + udSlip = impulsesUd['vertex_fields/slip'][:,:,1] + udImpInds = numpy.nonzero(udSlip != 0.0) + numUdImpulses = udImpInds[0].shape[0] + udCoordsUsed = udCoords[udImpInds[1]] + udSlipUsed = udSlip[udImpInds[0], udImpInds[1]] + (distances, udCoordInds) = self.matchCoords(udCoordsUsed, + self.impulseCoords) + udCoordsUsed = udCoordsUsed[udCoordInds,:] + impulsesUd.close() + + # Read responses. + print " Reading left-lateral responses:" + sys.stdout.flush() + responseLl = h5py.File(self.gfResponsesLlFile, 'r') + llResponseCoords = responseLl['geometry/vertices'][:] + llResponseVals = responseLl['vertex_fields/displacement'][:] + + (distances, llDataInds) = self.matchCoords(llResponseCoords, + self.dataCoords) + llResponsesEast = llResponseVals[:,llDataInds, 0] + llResponsesNorth = llResponseVals[:,llDataInds, 1] + llResponsesUp = llResponseVals[:,llDataInds, 2] + responseLl.close() + + print " Reading updip responses:" + sys.stdout.flush() + responseUd = h5py.File(self.gfResponsesUdFile, 'r') + udResponseCoords = responseUd['geometry/vertices'][:] + responseUdVals = responseUd['vertex_fields/displacement'][:] + udResponseVals = responseUdVals[udCoordInds,:,:] + + (distances, udDataInds) = self.matchCoords(udResponseCoords, + self.dataCoords) + udResponsesEast = udResponseVals[:,udDataInds, 0] + udResponsesNorth = udResponseVals[:,udDataInds, 1] + udResponsesUp = udResponseVals[:,udDataInds, 2] + responseUd.close() + + # Create design matrix. + print " Creating design matrix:" + sys.stdout.flush() + nE = self.numDataPoints + nN = self.numDataPoints + nU = self.numDataPoints + self.design = numpy.zeros((self.numDesignRows, self.numImpulses), + dtype=numpy.float64) + self.design[0:nE,:] = numpy.transpose(self.llComp * llResponsesEast + \ + self.udComp * udResponsesEast) + self.design[nE:nE + nN,:] = numpy.transpose( + self.llComp * llResponsesNorth + self.udComp * udResponsesNorth) + self.design[nE + nN:nE + nN + nU,:] = numpy.transpose( + self.llComp * llResponsesUp + self.udComp * udResponsesUp) + + return + + + def matchCoords(self, coordsRef, coords): + """ + Function to provide indices that match the given set of coordinates to a + reference set. + """ + + """ + This is a lot easier if you have scipy. + import scipy + tree = scipy.spatial.cKDTree(coordsRef) + (distances, inds) = tree.query(coords) + """ + + diff = coordsRef[:, :, None] - coords[:, :, None].transpose() + dist = numpy.linalg.norm(diff, axis=1) + inds = numpy.argmin(dist, axis=0) + distances = dist[inds].diagonal() + + return (distances, inds) + + + def readData(self): + """ + Function to read data, coordinates, and standard deviations. + """ + print "Reading data values:" + sys.stdout.flush() + + coords = [] + data = [] + cov = [] + dataE = [] + dataN = [] + dataU = [] + covE = [] + covN = [] + covU = [] + self.dataNames = [] + + f = open(self.dataFile, 'r') + lines = f.readlines() + self.numDataPoints = len(lines) - 1 + self.numDesignRows = 3 * self.numDataPoints + for line in range(1,self.numDataPoints + 1): + lineSplit = lines[line].split() + x = float(lineSplit[1]) + y = float(lineSplit[2]) + z = float(lineSplit[3]) + self.dataNames.append(lineSplit[0]) + coords.append([x, y, z]) + vE = self.dataScale * float(lineSplit[4]) + vN = self.dataScale * float(lineSplit[5]) + vU = self.dataScale * float(lineSplit[6]) + dataE.append(vE) + dataN.append(vN) + dataU.append(vU) + sigE = self.dataScale * float(lineSplit[7]) + sigN = self.dataScale * float(lineSplit[8]) + sigU = self.dataScale * float(lineSplit[9]) + covE.append(sigE*sigE) + covN.append(sigN*sigN) + covU.append(sigU*sigU) + + f.close() + + print " Number of data locations: %i" % self.numDataPoints + print " Number of rows in design matrix: %i" % self.numDesignRows + sys.stdout.flush() + + data = dataE + dataN + dataU + cov = covE + covN + covU + self.dataVals = numpy.array(data, dtype=numpy.float64) + self.dataCov = numpy.array(cov, dtype=numpy.float64) + self.dataCoords = numpy.array(coords, dtype=numpy.float64) + + return + + +# ---------------------------------------------------------------------- +if __name__ == '__main__': + app = SlipInvert() + app.run() + +# End of file diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 8fadafb216..9ecb9166ed 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -17,16 +17,12 @@ # ---------------------------------------------------------------------- # # In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are four +# to invert synthetic data generated from step06. There are two # different sub-problems: # step07a: Generate Green's functions corresponding to left-lateral # slip on the subduction interface (slab top). # step07b: Generate Green's functions corresponding to updip # slip on the subduction interface (slab top). -# step07c: Generate Green's functions corresponding to left-lateral -# slip on the splay fault. -# step07d: Generate Green's functions corresponding to updip -# slip on the splay fault. # # Responses (Green's functions) are computed at simulated cGPS # locations defined in the file cgps_sites.txt. diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 60fb6186b7..49b9a409e0 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -17,16 +17,12 @@ # ---------------------------------------------------------------------- # # In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are four +# to invert synthetic data generated from step06. There are two # different sub-problems: # step07a: Generate Green's functions corresponding to left-lateral # slip on the subduction interface (slab top). # step07b: Generate Green's functions corresponding to updip # slip on the subduction interface (slab top). -# step07c: Generate Green's functions corresponding to left-lateral -# slip on the splay fault. -# step07d: Generate Green's functions corresponding to updip -# slip on the splay fault. # # Responses (Green's functions) are computed at simulated cGPS # locations defined in the file cgps_sites.txt. diff --git a/examples/3d/subduction/step07c.cfg b/examples/3d/subduction/step07c.cfg deleted file mode 100644 index 30a99a7b36..0000000000 --- a/examples/3d/subduction/step07c.cfg +++ /dev/null @@ -1,146 +0,0 @@ -# -*- Python -*- (syntax highlighting) -# ---------------------------------------------------------------------- -# -# Brad T. Aagaard, U.S. Geological Survey -# Charles A. Williams, GNS Science -# Matthew G. Knepley, University of Chicago -# -# This code was developed as part of the Computational Infrastructure -# for Geodynamics (http://geodynamics.org). -# -# Copyright (c) 2010-2017 University of California, Davis -# -# See COPYING for license information. -# -# ---------------------------------------------------------------------- -# PROBLEM DESCRIPTION -# ---------------------------------------------------------------------- -# -# In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are four -# different sub-problems: -# step07a: Generate Green's functions corresponding to left-lateral -# slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to updip -# slip on the subduction interface (slab top). -# step07c: Generate Green's functions corresponding to left-lateral -# slip on the splay fault. -# step07d: Generate Green's functions corresponding to updip -# slip on the splay fault. -# -# Responses (Green's functions) are computed at simulated cGPS -# locations defined in the file cgps_sites.txt. -# Note that we change the default problem type from TimeDependent to -# GreensFns. -# -# Materials -# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). -# -# Boundary Conditions -# Roller boundary conditions (pylithapp.cfg). -# -# ---------------------------------------------------------------------- -# RUNNING THE SIMULATON -# ---------------------------------------------------------------------- -# -# Parameter files: -# - pylithapp.cfg (common paramters, read by default) -# - greensfns.cfg (greensfns paramters, read by default) -# - step07c.cfg (main parameter file for step07c) -# - mat_elastic.cfg (material models and parameters) -# - solver_fieldsplit.cfg (field split solver settings) -# -# We use the field split preconditioner with algebraic multigrid for -# the displacement fields and the custom preconditioner for the -# Lagrange multiplier field. We use these solver settings in several -# simulations, so we put them in a separate file. -# -# To run the simulation: -# pylith --problem=pylith.problems.GreensFns step07c.cfg mat_elastic.cfg solver_fieldsplit.cfg -# -# Output will be directed to the "output" directory.. - -# ---------------------------------------------------------------------- -# Output of parameters used and simulation progress. -# ---------------------------------------------------------------------- -[pylithapp] -dump_parameters.filename = output/step07c-parameters.json -problem.progress_monitor.filename = output/step07c-progress.txt - -# ---------------------------------------------------------------------- -# faults -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We prescribe slip on the splay fault patch. -interfaces = [splay] - -[pylithapp.problem.interfaces] -splay = pylith.faults.FaultCohesiveImpulses - -[pylithapp.problem.interfaces.splay] -id = 100 -label = fault_splay_patch -edge = fault_splay_patch_edge - -# We must define the quadrature information for fault cells. -# The fault cells are 2D (surface). -quadrature.cell = pylith.feassemble.FIATSimplex -quadrature.cell.dimension = 2 - -# Label and query type for fault slip. -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.query_type = nearest - -# Spatialdb for impulses. -impulse_dof = [0] -db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb - -# ---------------------------------------------------------------------- -# output -# ---------------------------------------------------------------------- -[pylithapp.problem.formulation] -output = [domain, subdomain, cgps_sites] -output.cgps_sites = pylith.meshio.OutputSolnPoints - -# Domain, subdomain, and points output --------------------------------- -[pylithapp.problem.formulation.output.domain] -writer.filename = output/step07c-domain.h5 -# Turn off data fields. -vertex_data_fields = [] - -[pylithapp.problem.formulation.output.subdomain] -writer.filename = output/step07c-groundsurf.h5 -# Turn off data fields. -vertex_data_fields = [] - -[pylithapp.problem.formulation.output.cgps_sites] -coordsys = spatialdata.geocoords.CSGeo -coordsys.space_dim = 3 -coordsys.datum_horiz = WGS84 -coordsys.datum_vert = mean sea level -writer = pylith.meshio.DataWriterHDF5 -reader.filename = cgps_sites.txt - -writer.filename = output/step07c-cgps_sites.h5 - -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.splay.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07c-fault-splay.h5 - -# Material output ------------------------------------------------------ -[pylithapp.problem.materials.slab.output] -writer.filename = output/step07c-slab.h5 - -[pylithapp.problem.materials.wedge.output] -writer.filename = output/step07c-wedge.h5 - -[pylithapp.problem.materials.crust.output] -writer.filename = output/step07c-crust.h5 - -[pylithapp.problem.materials.mantle.output] -writer.filename = output/step07c-mantle.h5 - - -# End of file diff --git a/examples/3d/subduction/step07d.cfg b/examples/3d/subduction/step07d.cfg deleted file mode 100644 index d4c7fe1c6d..0000000000 --- a/examples/3d/subduction/step07d.cfg +++ /dev/null @@ -1,146 +0,0 @@ -# -*- Python -*- (syntax highlighting) -# ---------------------------------------------------------------------- -# -# Brad T. Aagaard, U.S. Geological Survey -# Charles A. Williams, GNS Science -# Matthew G. Knepley, University of Chicago -# -# This code was developed as part of the Computational Infrastructure -# for Geodynamics (http://geodynamics.org). -# -# Copyright (c) 2010-2017 University of California, Davis -# -# See COPYING for license information. -# -# ---------------------------------------------------------------------- -# PROBLEM DESCRIPTION -# ---------------------------------------------------------------------- -# -# In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are four -# different sub-problems: -# step07a: Generate Green's functions corresponding to left-lateral -# slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to updip -# slip on the subduction interface (slab top). -# step07c: Generate Green's functions corresponding to left-lateral -# slip on the splay fault. -# step07d: Generate Green's functions corresponding to updip -# slip on the splay fault. -# -# Responses (Green's functions) are computed at simulated cGPS -# locations defined in the file cgps_sites.txt. -# Note that we change the default problem type from TimeDependent to -# GreensFns. -# -# Materials -# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). -# -# Boundary Conditions -# Roller boundary conditions (pylithapp.cfg). -# -# ---------------------------------------------------------------------- -# RUNNING THE SIMULATON -# ---------------------------------------------------------------------- -# -# Parameter files: -# - pylithapp.cfg (common paramters, read by default) -# - greensfns.cfg (greensfns paramters, read by default) -# - step07d.cfg (main parameter file for step07d) -# - mat_elastic.cfg (material models and parameters) -# - solver_fieldsplit.cfg (field split solver settings) -# -# We use the field split preconditioner with algebraic multigrid for -# the displacement fields and the custom preconditioner for the -# Lagrange multiplier field. We use these solver settings in several -# simulations, so we put them in a separate file. -# -# To run the simulation: -# pylith --problem=pylith.problems.GreensFns step07d.cfg mat_elastic.cfg solver_fieldsplit.cfg -# -# Output will be directed to the "output" directory.. - -# ---------------------------------------------------------------------- -# Output of parameters used and simulation progress. -# ---------------------------------------------------------------------- -[pylithapp] -dump_parameters.filename = output/step07d-parameters.json -problem.progress_monitor.filename = output/step07d-progress.txt - -# ---------------------------------------------------------------------- -# faults -# ---------------------------------------------------------------------- -[pylithapp.problem] -# We prescribe slip on the splay fault patch. -interfaces = [splay] - -[pylithapp.problem.interfaces] -splay = pylith.faults.FaultCohesiveImpulses - -[pylithapp.problem.interfaces.splay] -id = 100 -label = fault_splay_patch -edge = fault_splay_patch_edge - -# We must define the quadrature information for fault cells. -# The fault cells are 2D (surface). -quadrature.cell = pylith.feassemble.FIATSimplex -quadrature.cell.dimension = 2 - -# Label and query type for fault slip. -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.query_type = nearest - -# Spatialdb for impulses. -impulse_dof = [1] -db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb - -# ---------------------------------------------------------------------- -# output -# ---------------------------------------------------------------------- -[pylithapp.problem.formulation] -output = [domain, subdomain, cgps_sites] -output.cgps_sites = pylith.meshio.OutputSolnPoints - -# Domain, subdomain, and points output --------------------------------- -[pylithapp.problem.formulation.output.domain] -writer.filename = output/step07d-domain.h5 -# Turn off data fields. -vertex_data_fields = [] - -[pylithapp.problem.formulation.output.subdomain] -writer.filename = output/step07d-groundsurf.h5 -# Turn off data fields. -vertex_data_fields = [] - -[pylithapp.problem.formulation.output.cgps_sites] -coordsys = spatialdata.geocoords.CSGeo -coordsys.space_dim = 3 -coordsys.datum_horiz = WGS84 -coordsys.datum_vert = mean sea level -writer = pylith.meshio.DataWriterHDF5 -reader.filename = cgps_sites.txt - -writer.filename = output/step07d-cgps_sites.h5 - -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.splay.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step07d-fault-splay.h5 - -# Material output ------------------------------------------------------ -[pylithapp.problem.materials.slab.output] -writer.filename = output/step07d-slab.h5 - -[pylithapp.problem.materials.wedge.output] -writer.filename = output/step07d-wedge.h5 - -[pylithapp.problem.materials.crust.output] -writer.filename = output/step07d-crust.h5 - -[pylithapp.problem.materials.mantle.output] -writer.filename = output/step07d-mantle.h5 - - -# End of file From ce473f57a55d9eccf3f699b0ca9d7d3adb97d2a8 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 19 Jun 2017 10:27:43 -0700 Subject: [PATCH 064/216] Added solver settings for AMG as alternative in step01. --- .../subduction/solver_algebraicmultigrid.cfg | 24 +++++++++++++++++++ 1 file changed, 24 insertions(+) create mode 100644 examples/3d/subduction/solver_algebraicmultigrid.cfg diff --git a/examples/3d/subduction/solver_algebraicmultigrid.cfg b/examples/3d/subduction/solver_algebraicmultigrid.cfg new file mode 100644 index 0000000000..9257c1631c --- /dev/null +++ b/examples/3d/subduction/solver_algebraicmultigrid.cfg @@ -0,0 +1,24 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# This file provides an optimized solver using the ML algebraic +# multigrid preconditioner. It is well-suited for large production +# runs that do not include a fault. + +[pylithapp.petsc] +pc_type = ml + + +# End of file From 7f7f0c38a4178ba70dad2c2412c518399ed8c2a5 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 20 Jun 2017 09:39:22 +1200 Subject: [PATCH 065/216] Updated synthetic data script to generate VTK output. Commented out debugging statements in inversion script. Added additional parameter weighting values to inversion .cfg file. Added more description to step07a.cfg. --- .../3d/subduction/make_synthetic_gpsdisp.cfg | 1 + .../3d/subduction/make_synthetic_gpsdisp.py | 68 +++++++++++++++++-- examples/3d/subduction/slip_invert.cfg | 2 +- examples/3d/subduction/slip_invert.py | 4 +- examples/3d/subduction/step07a.cfg | 14 ++++ 5 files changed, 79 insertions(+), 10 deletions(-) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.cfg b/examples/3d/subduction/make_synthetic_gpsdisp.cfg index b3164b9907..288bf50bbd 100644 --- a/examples/3d/subduction/make_synthetic_gpsdisp.cfg +++ b/examples/3d/subduction/make_synthetic_gpsdisp.cfg @@ -5,3 +5,4 @@ sigma_east = 0.0005 sigma_north = 0.0005 sigma_up = 0.001 output_file = cgps_synthetic_displacement.txt +vtk_output_file = cgps_synthetic_displacement.vtk diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index ae2a46e538..1b09365e67 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -1,13 +1,27 @@ #!/usr/bin/env python - -## @file make_synth_data.py - -## @brief Python application to create synthetic data from PyLith points output. +# -*- Python -*- (syntax highlighting) +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# Python application to create synthetic data from PyLith points output. import math import numpy import h5py -# import pdb +import pdb from pyre.applications.Script import Script as Application @@ -26,9 +40,11 @@ class MakeSyntheticGpsdisp(Application): ## @li \b sigma_north Sigma value for north displacements. ## @li \b sigma_up Sigma value for up displacements. ## @li \b output_file Name of ASCII output file. + ## @li \b vtk_output_file Name of VTK output file. ## - pointInputFile = pyre.inventory.str("point_input_file", default="cascadia-cgps_points.h5") + pointInputFile = pyre.inventory.str("point_input_file", + default="cascadia-cgps_points.h5") pointInputFile.meta['tip'] = "HDF5 point output file from PyLith." timeStep = pyre.inventory.int("time_step", default=0) @@ -43,9 +59,14 @@ class MakeSyntheticGpsdisp(Application): sigmaUp = pyre.inventory.float("sigma_up", default=0.001) sigmaUp.meta['tip'] = "Sigma value for Up displacements." - outputFile = pyre.inventory.str("output_file", default="cascadia-cgps_disp.txt") + outputFile = pyre.inventory.str("output_file", + default="cascadia-cgps_disp.txt") outputFile.meta['tip'] = "Name of ASCII output file." + vtkOutputFile = pyre.inventory.str("vtk_output_file", + default="cascadia-cgps_disp.vtk") + vtkOutputFile.meta['tip'] = "Name of VTK output file." + # PUBLIC METHODS ///////////////////////////////////////////////////// @@ -67,6 +88,7 @@ def main(self): self._readHDF5() self._addNoise() self._writeOutput() + self._writeVTKOutput() return @@ -133,6 +155,38 @@ def _writeOutput(self): f.close() return + + + def _writeVTKOutput(self): + """ + Function to write VTK output file with noisy data and uncertainties. + """ + + sigma = numpy.ones((self.numStations, 3), dtype=numpy.float64) + sigma[:,0] *= self.sigmaEast + sigma[:,1] *= self.sigmaNorth + sigma[:,2] *= self.sigmaUp + + vtkHead = "# vtk DataFile Version 2.0\n" + \ + "Synthetic GPS stations\n" + \ + "ASCII\n" + \ + "DATASET POLYDATA\n" + \ + "POINTS " + repr(self.numStations) + " double\n" + + v = open(self.vtkOutputFile, 'w') + v.write(vtkHead) + numpy.savetxt(v, self.coords) + dispHead = "POINT_DATA " + repr(self.numStations) + "\n" + \ + "VECTORS displacement double\n" + \ + "LOOKUP_TABLE DEFAULT\n" + v.write(dispHead) + numpy.savetxt(v, self.dispNoise) + sigHead = "VECTORS uncertainty double\n" + v.write(sigHead) + numpy.savetxt(v, sigma) + v.close() + + return # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/slip_invert.cfg b/examples/3d/subduction/slip_invert.cfg index e53ca3768a..26bc8fa800 100644 --- a/examples/3d/subduction/slip_invert.cfg +++ b/examples/3d/subduction/slip_invert.cfg @@ -6,7 +6,7 @@ gfimpulses_ud_file = output/step07b-fault-slab.h5 gfresponses_ll_file = output/step07a-cgps_sites.h5 gfresponses_ud_file = output/step07b-cgps_sites.h5 a_priori_value = 0.0 -penalty_weight_vals = [1.0,2.0,5.0,10.0,20.0,50.0,100.0] +penalty_weight_vals = [0.1,0.2,0.5,1.0,2.0,5.0,10.0,20.0,50.0,100.0] data_scale = 1.0 result_summary_file = step07-inversion-summary.txt slip_output_file = step07-inversion-slip.h5 diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index a3494a2e06..aff72d0d2b 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -133,8 +133,8 @@ def __init__(self, name="slip_invert"): def main(self): - import pdb - pdb.set_trace() + # import pdb + # pdb.set_trace() self.readData() self.readGreens() self.runInversions() diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 9ecb9166ed..f6852c84ee 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -29,6 +29,20 @@ # Note that we change the default problem type from TimeDependent to # GreensFns. # +# Prior to generating the Green's functions, we first generate synthetic +# data from the output of problem step06, using the make_synthetic_gpsdisp.py +# script, with parameters defined in make_synthetic_gpsdisp.cfg: +# +# ./make_synthetic_gpsdisp.py +# +# After generating the synthetic data and Green's functions, we then +# perform a simple inversion using the slip_invert.py script, with +# parameters defined in slip_invert.cfg: +# +# ./slip_invert.py +# +# +# # Materials # All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). # From a196c77b9ca7548e62b8305a8179821750e796bc Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 20 Jun 2017 10:34:25 +1200 Subject: [PATCH 066/216] Updated descriptions in step07 .cfg files. Added Python script to plot inversion residuals. --- examples/3d/subduction/step07a.cfg | 9 +++ examples/3d/subduction/step07b.cfg | 23 ++++++ .../subduction/viz/plot_inversion_misfit.py | 74 +++++++++++++++++++ 3 files changed, 106 insertions(+) create mode 100755 examples/3d/subduction/viz/plot_inversion_misfit.py diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index f6852c84ee..8a8e281a44 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -41,6 +41,15 @@ # # ./slip_invert.py # +# This will generate two HDF files that may be viewed in Paraview: +# step07-inversion-slip.h5: The predicted fault slip. +# step07-inversion-displacement.h5: The predicted surface displacements. +# +# There is also an inversion summary file: step07-inversion-summary.txt +# If you have matplotlib installed, you can view a log-log plot of +# solution misfit by going into the viz directory and running: +# +# ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt # # # Materials diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 49b9a409e0..fe2b9f02ab 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -29,6 +29,29 @@ # Note that we change the default problem type from TimeDependent to # GreensFns. # +# Prior to generating the Green's functions, we first generate synthetic +# data from the output of problem step06, using the make_synthetic_gpsdisp.py +# script, with parameters defined in make_synthetic_gpsdisp.cfg: +# +# ./make_synthetic_gpsdisp.py +# +# After generating the synthetic data and Green's functions, we then +# perform a simple inversion using the slip_invert.py script, with +# parameters defined in slip_invert.cfg: +# +# ./slip_invert.py +# +# This will generate two HDF files that may be viewed in Paraview: +# step07-inversion-slip.h5: The predicted fault slip. +# step07-inversion-displacement.h5: The predicted surface displacements. +# +# There is also an inversion summary file: step07-inversion-summary.txt +# If you have matplotlib installed, you can view a log-log plot of +# solution misfit by going into the viz directory and running: +# +# ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt +# +# # Materials # All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). # diff --git a/examples/3d/subduction/viz/plot_inversion_misfit.py b/examples/3d/subduction/viz/plot_inversion_misfit.py new file mode 100755 index 0000000000..39cf4adb0a --- /dev/null +++ b/examples/3d/subduction/viz/plot_inversion_misfit.py @@ -0,0 +1,74 @@ +#!/usr/bin/env python +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# This script creates a log-log plot of weighted data misfit vs. penalty misfit. +# The code requires the numpy and matplotlib packages. + +import numpy +import matplotlib.pyplot as pyplot +import math + +# Define line colors and other parameters. +lineColor = "blue" + +# ---------------------------------------------------------------------- +def readInversionSummary(): + """ + Function to read inversion results from text file. + """ + + # Open inversion summary file and get misfits. + data = numpy.loadtxt(summaryFile, dtype=numpy.float64) + dataWeightResid = data[:,2] + penaltyResid = data[:,3] + + # Sort by penalty residual. + inds = numpy.argsort(penaltyResid) + dataWeightResidSort = dataWeightResid[inds] + penaltyResidSort = penaltyResid[inds] + + return (dataWeightResidSort, penaltyResidSort) + + +# ====================================================================== +# The main part of the code is below. +# Get command-line arguments. +from optparse import OptionParser +parser = OptionParser() +parser.add_option("-s", "--summary", action="store", type="string", + dest="summary_file", + help="Text file with inversion summary") + +(options, args) = parser.parse_args() + +if not options.summary_file: + parser.error("Summary input file must be specified.") + +summaryFile = options.summary_file + +# Get misfits. +(dataWeightResid, penaltyResid) = readInversionSummary() + +# Generate figure, starting with true solution. +pyplot.loglog(penaltyResid, dataWeightResid, linewidth=2, color=lineColor, + marker="o") +pyplot.xlabel("Log(Penalty Residual)") +pyplot.ylabel("Log(Weighted Data Residual)") +pyplot.xlim(left=10.0, right=30.0) + +pyplot.show() +# pyplot.savefig("reverse_inversion.pdf") From 35eccefbc1d9e207d48e26a153559f7e223ae1f9 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 20 Jun 2017 11:30:10 +1200 Subject: [PATCH 067/216] Improved VTK output. --- examples/3d/subduction/make_synthetic_gpsdisp.py | 13 +++++++++++-- 1 file changed, 11 insertions(+), 2 deletions(-) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index 1b09365e67..0a0c1dfa7e 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -176,11 +176,20 @@ def _writeVTKOutput(self): v = open(self.vtkOutputFile, 'w') v.write(vtkHead) numpy.savetxt(v, self.coords) + + numConnect = 2 * self.numStations + connectHead = "VERTICES %d %d\n" % (self.numStations, numConnect) + v.write(connectHead) + verts = numpy.arange(self.numStations, dtype=numpy.int) + sizes = numpy.ones_like(verts) + outConnect = numpy.column_stack((sizes, verts)) + numpy.savetxt(v, outConnect, fmt="%d") + dispHead = "POINT_DATA " + repr(self.numStations) + "\n" + \ - "VECTORS displacement double\n" + \ - "LOOKUP_TABLE DEFAULT\n" + "VECTORS displacement double\n" v.write(dispHead) numpy.savetxt(v, self.dispNoise) + sigHead = "VECTORS uncertainty double\n" v.write(sigHead) numpy.savetxt(v, sigma) From ae8a0cfb8a5e2f6fe3b892e36169337425c5aafd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 19 Jun 2017 17:08:33 -0700 Subject: [PATCH 068/216] Fixed some issues with plotting slip and traction ratio. --- ...n_cartoon.svg => subduction2d_cartoon.svg} | 0 ...l.pdf => subduction2d_cartoon_general.pdf} | Bin ...l.svg => subduction2d_cartoon_general.svg} | 0 ...ion_step01.pdf => subduction2d_step01.pdf} | Bin ..._soln.png => subduction2d_step01_soln.png} | Bin ...ion_step02.pdf => subduction2d_step02.pdf} | Bin ..._soln.png => subduction2d_step02_soln.png} | Bin ...ion_step03.pdf => subduction2d_step03.pdf} | Bin ..._soln.png => subduction2d_step03_soln.png} | Bin ..._soln.png => subduction2d_step04_soln.png} | Bin ...duction_tri3.png => subduction2d_tri3.png} | Bin .../{subduction.tex => subduction2d.tex} | 0 .../subduction/viz/plot_faultslip-reltract.py | 23 ++++++++++-------- 13 files changed, 13 insertions(+), 10 deletions(-) rename doc/userguide/examples/figs/{subduction_cartoon.svg => subduction2d_cartoon.svg} (100%) rename doc/userguide/examples/figs/{subduction_cartoon_general.pdf => subduction2d_cartoon_general.pdf} (100%) rename doc/userguide/examples/figs/{subduction_cartoon_general.svg => subduction2d_cartoon_general.svg} (100%) rename doc/userguide/examples/figs/{subduction_step01.pdf => subduction2d_step01.pdf} (100%) rename doc/userguide/examples/figs/{subduction_step01_soln.png => subduction2d_step01_soln.png} (100%) rename doc/userguide/examples/figs/{subduction_step02.pdf => subduction2d_step02.pdf} (100%) rename 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index 0c75ca68ab..d1054213a0 100644 --- a/examples/3d/subduction/viz/plot_faultslip-reltract.py +++ b/examples/3d/subduction/viz/plot_faultslip-reltract.py @@ -30,8 +30,8 @@ # Root name for simulation. SIM_NAME = "step05" -# Names of faults for output files. -FAULTS = ["fault-slab"] +# Names of faults (with spontaneous rupture) for output files. +FAULTS = ["fault-slabtop"] # ---------------------------------------------------------------------- from paraview.simple import * @@ -71,11 +71,11 @@ def visualize(sim, faults): groupFaults = GroupDatasets(Input=dataFaults) # Ratio of shear to normal traction - calculator = Calculator(Input=groupFaults) - calculator.Function = 'mag(traction_X*iHat+traction_Y*jHat)/abs(traction_Z)' - calculator.ResultArrayName = 'shearDivNormal' + calculatorRatio = Calculator(Input=groupFaults) + calculatorRatio.Function = 'mag(traction_X*iHat+traction_Y*jHat)/abs(traction_Z)' + calculatorRatio.ResultArrayName = 'shearDivNormal' - ratioDisplay = Show(groupFaults, view) + ratioDisplay = Show(calculatorRatio, view) ColorBy(ratioDisplay, ('POINTS', 'shearDivNormal')) ratioDisplay.RescaleTransferFunctionToDataRange(True) ratioDisplay.SetScalarBarVisibility(view, True) @@ -87,11 +87,14 @@ def visualize(sim, faults): # Update a scalar bar component title. UpdateScalarBarsComponentTitle(ratioLUT, ratioDisplay) - calculator = Calculator(Input=groupFaults) - calculator.Function = 'mag(slip)' - calculator.ResultArrayName = 'slipMag' + # Slip contours + SetActiveSource(groupFaults) + + calculatorSlip = Calculator(Input=groupFaults) + calculatorSlip.Function = 'mag(slip)' + calculatorSlip.ResultArrayName = 'slipMag' - contour = Contour(Input=groupFaults) + contour = Contour(Input=calculatorSlip) contour.ContourBy = ['POINTS', 'slipMag'] contour.Isosurfaces = numpy.arange(0.0, 4.01, 0.5) contour.PointMergeMethod = 'Uniform Binning' From f32280aee3401c46cb3ac29ea33a293e9a792dbc Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 19 Jun 2017 17:09:28 -0700 Subject: [PATCH 069/216] Fix typos in manual. --- doc/userguide/boundaryconditions/boundaryconditions.tex | 2 +- doc/userguide/runpylith/definesim.tex | 2 +- 2 files changed, 2 insertions(+), 2 deletions(-) diff --git a/doc/userguide/boundaryconditions/boundaryconditions.tex b/doc/userguide/boundaryconditions/boundaryconditions.tex index f11c8437b3..7476f0c40c 100644 --- a/doc/userguide/boundaryconditions/boundaryconditions.tex +++ b/doc/userguide/boundaryconditions/boundaryconditions.tex @@ -807,7 +807,7 @@ \subsubsection{Arrays of Kinematic Rupture Components} & \texttt{strike\_dir} & Direction of fault strike in global coordinate system\\ & \texttt{dip\_dir} & Up-dip direction on hanging wall in global coordinate system\\ & \texttt{final\_slip\_NAME} & Vector of final slip (in fault coordinate system) in meters\\ - & \texttt{slip\_time}\_\texttt{\noun{NAME}} & Time at which slip begins in seconds\\ + & \texttt{slip\_time}\_\texttt{NAME} & Time at which slip begins in seconds\\ \property{vertex\_data\_fields} & \texttt{slip} & Slip vector at time step (in fault coordinate system) in meters\\ & \texttt{traction\_change} & Change in fault tractions (in fault coordinate system) in Pa\\ \hline diff --git a/doc/userguide/runpylith/definesim.tex b/doc/userguide/runpylith/definesim.tex index 1daa2d5128..53e69a9dfa 100644 --- a/doc/userguide/runpylith/definesim.tex +++ b/doc/userguide/runpylith/definesim.tex @@ -58,7 +58,7 @@ \subsubsection{Units} \subsubsection{Using the Command Line} -The \commandline{-}-help} command line argument displays links to useful +The \commandline{-{}-help} command line argument displays links to useful resources for learning PyLith. Pyre uses the following syntax to change properties from the command From 882c9ea719cb111b31d3d6d374a235f6b906522a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 19 Jun 2017 17:09:45 -0700 Subject: [PATCH 070/216] Require spatial data v1.9.9. --- configure.ac | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/configure.ac b/configure.ac index 8528a23d8a..22d81dca35 100644 --- a/configure.ac +++ b/configure.ac @@ -213,7 +213,7 @@ AC_REQUIRE_CPP AC_LANG(C++) CIT_SPATIALDATA_HEADER CIT_SPATIALDATA_LIB -CIT_PYTHON_MODULE([spatialdata],[1.9.8]) +CIT_PYTHON_MODULE([spatialdata],[1.9.9]) # DOXYGEN if test "$enable_documentation" = "yes" ; then From 37420e7bafc316d31fe2774bb4bb57d0d87b7fe8 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 19 Jun 2017 17:11:22 -0700 Subject: [PATCH 071/216] Started work on adding 3d/subduction example to manual. --- doc/userguide/examples/examples.tex | 3 +- doc/userguide/examples/examples_info.py | 443 ++++++++++++++++++++++++ doc/userguide/examples/subduction2d.tex | 56 +-- doc/userguide/examples/subduction3d.py | 255 ++++++++++++++ doc/userguide/examples/subduction3d.tex | 198 +++++++++++ examples/3d/subduction/README | 5 + examples/3d/subduction/TODO | 4 - 7 files changed, 931 insertions(+), 33 deletions(-) create mode 100755 doc/userguide/examples/examples_info.py create mode 100644 doc/userguide/examples/subduction3d.py create mode 100644 doc/userguide/examples/subduction3d.tex diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 442be9db4e..92b4b3234e 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -46,10 +46,11 @@ \subsubsection{Input Files} \input{./examples/twotet4-geoproj.tex} \input{./examples/3dtet4.tex} \input{./examples/3dhex8.tex} -\input{./examples/subduction.tex} +\input{./examples/subduction2d.tex} \input{./examples/shearwave.tex} \input{./examples/greensfns2d.tex} \input{./examples/grav2d} +\input{./examples/subduction3d} \section{Additional Examples} diff --git a/doc/userguide/examples/examples_info.py b/doc/userguide/examples/examples_info.py new file mode 100755 index 0000000000..6008131347 --- /dev/null +++ b/doc/userguide/examples/examples_info.py @@ -0,0 +1,443 @@ +#!/usr/bin/env python +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# + +from collections import OrderedDict + +EXAMPLE_FILES = [ + "subduction3d", +] + +# ---------------------------------------------------------------------- +class Features(object): + CS_CART = "Cart" + CS_PROJ = "Proj" + + CELL_TRI = "Tri" + CELL_QUAD = "Quad" + CELL_TET = "Tet" + CELL_HEX = "Hex" + + MESH_ASCII = "ASCII" + MESH_CUBIT = "CUBIT" + MESH_LAGRIT = "LaGriT" + + REFINE_2 = "2x" + REFINE_4 = "4x" + REFINE_8 = "8x" + + PROB_TIMEDEPENDENT = "TD" + PROB_GREENSFNS = "GF" + + TIMEDEP_STATIC = "S" + TIMEDEP_QUASISTATIC = "QS" + TIMEDEP_DYNAMIC = "D" + + SOLVER_LINEAR = "L" + SOLVER_NONLINEAR = "NL" + + TS_BWDEULER = "BE" + TS_FWDEULER = "FE" + TS_RUNGEKUTTA = "RK" + + PRECOND_ILU = "ILU" + PRECOND_ASM = "ASM" + PRECOND_SCHUR = "SCHUR" + PRECOND_CUSTOM = "CUST" + PRECOND_ML = "ML" + PRECOND_GAMG = "GAMG" + PRECOND_ML_CUSTOM = "ML+CUST" + + SLIPFN_STEP = "STEP" + SLIPFN_RATE = "RATE" + SLIPFN_LIU = "LIU" + SLIPFN_BRUNE = "BRUNE" + SLIPFN_TIMEHISTORY = "USER" + + STRAINFORM_INFINITESIMAL = "Inf" + STRAINFORM_FINITE = "Fin" + + OUTPUT_VTK = "VTK" + OUTPUT_HDF5 = "H5" + OUTPUT_HDF5EXT = "H5Ext" + + from collections import OrderedDict + CATEGORIES = [ + ("General", + # Properties + OrderedDict(( + ("Dimension", { "enum": [2, 3], }), + ("Coordinate system", { "enum": [CS_CART, CS_PROJ], }), + ("Mesh generator", { "enum": [MESH_ASCII, MESH_CUBIT, MESH_LAGRIT], }), + ("Cells", { "enum": [CELL_TRI, CELL_QUAD, CELL_TET, CELL_HEX], }), + ("Refinement", { "enum": [REFINE_2, REFINE_4, REFINE_8], }), + ("Reordering", { "type": "boolean", }), + ("Problem type", { + "enum": [PROB_TIMEDEPENDENT, PROB_GREENSFNS], + "description": "%s: time dependent, %s: Green's functions" % (PROB_TIMEDEPENDENT, PROB_GREENSFNS), + }), + ("Time dependence", { + "enum": [TIMEDEP_STATIC, TIMEDEP_QUASISTATIC, TIMEDEP_DYNAMIC], + "description": "%s: static, %s: quasi-static, %s: dynamic" % (TIMEDEP_STATIC, TIMEDEP_QUASISTATIC, TIMEDEP_DYNAMIC), + }), + )), + # Required + ["Dimension", "Coordinate system", "Mesh generator", "Cells", "Problem type"], + ), + ("Solver", + # Properties + OrderedDict(( + ("Solver", { + "enum": [SOLVER_LINEAR, SOLVER_NONLINEAR], + "description": "%s: linear, %s: nonlinear" % (SOLVER_LINEAR, SOLVER_NONLINEAR), + }), + ("Preconditioner", { + "enum": [PRECOND_ILU, PRECOND_ASM, PRECOND_SCHUR, PRECOND_CUSTOM, PRECOND_ML, PRECOND_GAMG, PRECOND_ML_CUSTOM], + "description": "%s: ILU, %s: Additive Schwarz, %s: Schur complement, %s: custom, %s: ML algebraic multigrid, %s: geometric algebraic multigrid" % (PRECOND_ILU, PRECOND_ASM, PRECOND_SCHUR, PRECOND_CUSTOM, PRECOND_ML, PRECOND_GAMG), + }), + + ("Time stepping", { + #"enum": [TS_BWDEULER, TS_FWDEULER, TS_RUNGEKUTTA], + #"description": "%s: Backward Euler, %s: Forward Euler, %s: Runge-Kutta" % (TS_BWDEULER, TS_FWDEULER, TS_RUNGEKUTTA), + "enum": [TS_BWDEULER, TS_FWDEULER], + "description": "%s: Backward Euler, %s: Forward Euler" % (TS_BWDEULER, TS_FWDEULER), + }), + )), + # Required + ["Solver"], + ), + ("Boundary Condition", + # Properties + OrderedDict(( + ("Dirichlet", { "type": "integer", "minimum": 0, }), + ("Neumann", { "type": "integer", "minimum": 0, }), + ("Absorbing", { "type": "integer", "minimum": 0, }), + ("Point force", { "type": "integer", "minimum": 0, }), + )), + # Required + None, + ), + ("Fault", + # Properties + OrderedDict(( + ("Prescribed slip", { "type": "integer", "minimum": 0, }), + ("Slip time function", { "enum": [SLIPFN_STEP, SLIPFN_RATE, SLIPFN_LIU, SLIPFN_BRUNE, SLIPFN_TIMEHISTORY], }), + ("Constitutive model", { "type": "integer", "minimum": 0, }), + ("Static friction", { "type": "boolean" }), + ("Slip-weakening friction", { "type": "boolean" }), + ("Time-weakening friction", { "type": "boolean" }), + ("Rate-state friction w/ageing", { "type": "boolean" }), + ("Traction perturbation", { "type": "boolean" }), + )), + # Required + None, + ), + ("Bulk Rheology", + # Properties + OrderedDict(( + ("Linear elastic", { "type": "integer", "minimum": 0, }), + ("Linear Maxwell viscoelastic", { "type": "integer", "minimum": 0, }), + ("Generalized Maxwell viscoelastic", { "type": "integer", "minimum": 0, }), + ("Powerlaw viscoelastic", { "type": "integer", "minimum": 0, }), + ("Drucker-Prager elastoplastic", { "type": "integer", "minimum": 0, }), + #("Incompressible linear elastic", { "type": "integer", "minimum": 0, }), + #("Porous linear elastic", { "type": "integer", "minimum": 0, }), + ("Stress/strain formulation", { + "enum": [STRAINFORM_INFINITESIMAL, STRAINFORM_FINITE], + "description": "%s: infinitesimal, %s: small, finite strain" % (STRAINFORM_INFINITESIMAL, STRAINFORM_FINITE), + }), + ("Inertia", { "type": "boolean" }), + ("Reference state", { "type": "boolean" }), + ("Gravity", { "type": "boolean" }), + )), + # Required + ["Stress/strain formulation"], + ), + ("Output", + # Properties + OrderedDict(( + ("Format", { "enum": [OUTPUT_VTK, OUTPUT_HDF5, OUTPUT_HDF5EXT], }), + ("Domain output", { "type": "integer", "minimum": 0, }), + ("Surface output", { "type": "integer", "minimum": 0, }), + ("Point output", { "type": "integer", "minimum": 0, }), + ("State variable output", { "type": "integer", "minimum": 0, }), + ("ParaView", { "type": "boolean", }), + ("Matplotlib", { "type": "boolean", }), + )), + # Required + ["Format"], + ), + ("Spatial Database", + # Properties + OrderedDict(( + ("Uniform", { "type": "integer", "minimum": 0, }), + ("Simple", { "type": "integer", "minimum": 0, }), + ("Simple grid", { "type": "integer", "minimum": 0, }), + ("Composite", { "type": "integer", "minimum": 0, }), + ("Time history", { "type": "integer", "minimum": 0, }), + )), + # Required + None, + ) + ] + + SCHEMA = { + "$schema": "http://json-schema.org/schema#", + "id": "PyLith examples schema", + "title": "Example", + "type": "object", + "properties": {}, + "required": ["General", "Solver", "Boundary Condition", "Bulk Rheology", "Output", "Spatial Database"], + } + for category, properties, required in CATEGORIES: + SCHEMA["properties"][category] = { + "type": "object", + "properties": properties, + "additionalProperties": False} + if required: + SCHEMA["properties"][category]["required"] = required + + + +# ---------------------------------------------------------------------- +class Table(object): + """Object tabulating features in examples. + """ + + def __init__(self, fout, columns): + """Constructor. + + :param fout: File object for LaTeX output. + """ + self.fout = fout + self.columns = columns + return + + def writeHeader(self): + """Write table header. + """ + f = self.fout + + f.write("\\begin{table}[htbp]\n") + f.write("\\rowcolors{2}{yellow!30}{white}\n") + ctags = ["|l|%% Example"] + for category in self.columns: + cols = Features.SCHEMA["properties"][category]["properties"] + ctags.append("*{%d}c|%% %s" % (len(cols), category)) + f.write("\\resizebox{\\textwidth}{!}{%\n") + f.write("\\begin{tabular}{%s\n}\n" % "\n ".join(ctags)) + f.write("\\hline\n") + + f.write("\\rowcolor{blue!10}\n") + f.write("Example\n") + for category in self.columns: + cols = Features.SCHEMA["properties"][category]["properties"] + f.write("& \multicolumn{%d}{c|}{%s}\n" % (len(cols), category)) + f.write("\\\\ \n") + f.write("%%%%\n") + f.write("\\hline\n") + f.write("\\rowcolor{blue!10}\n") + f.write("\n") + for category in self.columns: + f.write("%% %s\n" % category) + cols = Features.SCHEMA["properties"][category]["properties"] + for m in cols.keys(): + f.write("& \\rlabel{%s}\n" % m) + f.write("\\\\\n") + f.write("\\hline\n") + return + + def writeRow(self, label, example): + """Write table row corresponding to features for a given example. + + :param label: Label for example. + :param example: Features for a given example. + """ + f = self.fout + fromBoolean = lambda v: "\yes" if v else "" + fromInt = lambda v: "x%d" % v + + f.write("%s\n" % label) + for category in self.columns: + cols = Features.SCHEMA["properties"][category]["properties"] + if not category in example: + for col in cols: + f.write("& ") + continue + for col, property in cols.items(): + if not col in example[category]: + f.write("& ") + continue + value = example[category][col] + s = str(value) + if "type" in property: + if property["type"] == "boolean": + s = fromBoolean(value) + elif property["type"] == "integer": + s = fromInt(value) + f.write("& %s " % s) + f.write("\n") + f.write("\\\\ \\hline\n") + return + + def writeFooter(self): + """Write table footer. + """ + f = self.fout + + f.write("\\end{tabular}}\n") + f.write("\\par\n") + + for category in self.columns: + cols = Features.SCHEMA["properties"][category]["properties"] + for label, col in cols.items(): + if "description" in col: + f.write("{\\bf %s} -- %s. " % (label, col["description"])) + f.write("\\\\ \n") + f.write("\\end{table}") + return + + @staticmethod + def writeDocHeader(fout): + """Write document header. + """ + fout.write("\\documentclass[10pt]{article}\n") + fout.write("\\usepackage{pifont}\n") + fout.write("\\usepackage{graphicx}\n") + fout.write("\\usepackage[table]{xcolor}\n") + fout.write("\\newcommand{\\rlabel}[1]{\\rotatebox[origin=l]{90}{#1}}\n") + fout.write("\\newcommand{\\yes}{\\ding{52}}\n") + fout.write("\n\\begin{document}\n") + return + + @staticmethod + def writeDocFooter(fout): + """Write document footer. + """ + fout.write("\\end{document}\n") + return + +# ---------------------------------------------------------------------- +class App(object): + """Application for generating information about examples. + """ + + def __init__(self): + """Constructor. + """ + self.examples = None + return + + def initialize(self): + """Initialize application. + """ + import importlib + self.examples = OrderedDict() + for filename in EXAMPLE_FILES: + m = importlib.import_module(filename) + for label, example in m.examples.items(): + self.examples[label] = example + return + + def validate(self): + """Validate using JSON schema. + """ + import jsonschema + ok = True + for label, example in self.examples.items(): + try: + jsonschema.validate(example, Features.SCHEMA) + print("Example '%s': OK" % label) + except jsonschema.exceptions.ValidationError as err: + print("Example '%s': ERROR" % label) + print(str(err)) + ok = False + return ok + + def tabulate(self, filename, standalone=False): + """Generate LaTeX table with list of features covered by each example. + + :param filename: Name of file for output with LaTeX code. + """ + tableColumns = [ + [ + "General", + "Solver", + "Spatial Database", + ], + [ + "Boundary Condition", + "Fault", + "Bulk Rheology", + "Output", + ], + ] + with open(filename, "w") as fout: + if standalone: + Table.writeDocHeader(fout) + for columns in tableColumns: + table = Table(fout, columns) + table.writeHeader() + for label, example in self.examples.items(): + table.writeRow(label, example) + table.writeFooter() + if standalone: + Table.writeDocFooter(fout) + return + + def listFeatures(self, exname): + """Generate LaTeX itemized list of features covered by a given example. + + LaTeX code for itemized list is written to stdout. + + :param exame: Name of example in examples list. + """ + features = self.examples[exname] + + print("EXAMPLE %s" % exname) + print("\\begin{itemize}") + for key, value in features.items(): + print("\\item %s %s" % (value, key)) + print("\\end{itemize}") + return + +# ====================================================================== +if __name__ == "__main__": + import argparse + + DESCRIPTION = "Application for generating LaTeX code for (1) a table of features covered in each example and (2) an itemized list of features covered in any given example." + + parser = argparse.ArgumentParser(description=DESCRIPTION) + parser.add_argument("--validate-only", action="store_true", dest="validateOnly") + parser.add_argument("--table", action="store_true", dest="table") + parser.add_argument("--table-filename", action="store", dest="tableFilename", default="example_table.tex") + parser.add_argument("--table-standalone", action="store_true", dest="tableStandalone") + parser.add_argument("--list-features", action="store", dest="features", default=None) + args = parser.parse_args() + + app = App() + app.initialize() + ok = app.validate() + if not args.validateOnly and ok: + if args.table: + app.tabulate(args.tableFilename, args.tableStandalone) + if args.features: + fexs = args.features.split(",") + for ex in fexs: + app.listFeatures(ex) + +# End of file diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index 24b2e60b5a..f080a30944 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -1,5 +1,5 @@ -\section{Example for Slip on a Subduction Zone} -\label{sec:example:subduction} +\section{Example for Slip on a 2D Subduction Zone} +\label{sec:example:subduction:2d} PyLith features discussed in this example: \begin{itemize} @@ -29,16 +29,16 @@ \section{Example for Slip on a Subduction Zone} \item Static friction \end{itemize} All of the files necessary to run the examples are contained in the -directory \filename{examples/2d/subduction.} +directory \filename{examples/2d/subduction}. \subsection{Overview} This example examines quasi-static interseismic and coseismic deformation in 2D for a subduction zone (see Figure -\vref{fig:example:subduction:overview}). It is based on the 2011 +\vref{fig:example:subduction:2d:overview}). It is based on the 2011 M9.0 Tohoku earthquake off the east coast of Japan. Figure -\vref{fig:example:subduction:steps} shows the three steps of +\vref{fig:example:subduction:2d:steps} shows the three steps of increasing complexity. Step 1 focuses on the coseismic slip, Step 2 focuses on interseismic deformation, and Step 3 combines the two into a pseudo-earthquake cycle deformation simulation. Step 4 focuses on @@ -46,21 +46,21 @@ \subsection{Overview} with afterslip controlled by frictional sliding. \begin{figure} - \includegraphics{examples/figs/subduction_cartoon_general} + \includegraphics{examples/figs/subduction2d_cartoon_general} \caption{Cartoon of subduction zone example.} - \label{fig:example:subduction:overview} + \label{fig:example:subduction:2d:overview} \end{figure} \begin{figure} \begin{tabular}{ccc} Step 1 & Step 2 & Step 3 \\ - \includegraphics[width=2in]{examples/figs/subduction_step01} & - \includegraphics[width=2in]{examples/figs/subduction_step02} & - \includegraphics[width=2in]{examples/figs/subduction_step03} \\ + \includegraphics[width=2in]{examples/figs/subduction2d_step01} & + \includegraphics[width=2in]{examples/figs/subduction2d_step02} & + \includegraphics[width=2in]{examples/figs/subduction2d_step03} \\ \end{tabular} \caption{Diagram of fault slip and boundary conditions for each step in the subduction zone example.} - \label{fig:example:subduction:steps} + \label{fig:example:subduction:2d:steps} \end{figure} @@ -98,11 +98,11 @@ \subsection{Mesh Description} \end{enumerate} \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction_tri3} + \includegraphics[width=4.5in]{examples/figs/subduction2d_tri3} \caption{Variable resolution finite-element mesh with triangular cells. The nominal cell size increases at a geometric rate of 1.2 away from the region of coseismic slip.} - \label{fig:example:subduction:mesh} + \label{fig:example:subduction:2d:mesh} \end{figure} @@ -151,7 +151,7 @@ \subsection{Step 1: Coseismic Slip Simulation} The spatial variation of slip comes from a cross-section of Gavin Hayes' finite-source model \url{earthquake.usgs.gov/earthquakes/eqinthenews/2011/usc0001xgp/finite_fault.php}. On the lateral and bottom boundaries of the domain, we fix the degrees -of freedom perpendicular to the boundary as shown in Figure \vref{fig:example:subduction:steps}. +of freedom perpendicular to the boundary as shown in Figure \vref{fig:example:subduction:2d:steps}. Parameter settings that augment those in \filename{pylithapp.cfg} are contained in the file \filename{step01.cfg}. These settings are: \begin{inventory} @@ -183,15 +183,15 @@ \subsection{Step 1: Coseismic Slip Simulation} each material (eight pairs of files), and fault parameters, slip, and traction (two pairs of files). -Figure \vref{fig:example:subduction:step01}, which was created using +Figure \vref{fig:example:subduction:2d:step01}, which was created using ParaView, displays the magnitude of the displacement field with the deformation exaggerated by a factor of 1000. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction_step01_soln} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step01_soln} \caption{Solution for Step 1. The colors indicate the magnitude of the displacement, and the deformation is exaggerated by a factor of 1000. } - \label{fig:example:subduction:step01} + \label{fig:example:subduction:2d:step01} \end{figure} @@ -202,7 +202,7 @@ \subsection{Step 2: Interseismic Deformation Simulation} into the mantle. We prescribe steady aseismic slip of 8 cm/yr along the interfaces between the oceanic crust and mantle with the interface between the oceanic crust and continental crust locked as shown in -Figure \vref{fig:example:subduction:steps}. We adjust the Dirichlet +Figure \vref{fig:example:subduction:2d:steps}. We adjust the Dirichlet boundary conditions on the lateral edges and bottom of the domain by pinning only the portions of the boundaries in the mantle and continental crust (i.e., not part of the oceanic crust). Parameter settings that @@ -228,7 +228,7 @@ \subsection{Step 2: Interseismic Deformation Simulation} \end{shell} The simulation will produce pairs of HDF5/Xdmf files with separate files for each material and fault interface. Figure -\vref{fig:example:subduction:step02}, which was created using +\vref{fig:example:subduction:2d:step02}, which was created using ParaView, displays the magnitude of the displacement field with the deformation exaggerated by a factor of 1000. Using the animation features within ParaView or Visit you can illustrate how the @@ -236,11 +236,11 @@ \subsection{Step 2: Interseismic Deformation Simulation} deformation. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction_step02_soln} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step02_soln} \caption{Solution for Step 2 at 100 years. The colors indicate the magnitude of the displacement, and the deformation is exaggerated by a factor of 1000.} - \label{fig:example:subduction:step02} + \label{fig:example:subduction:2d:step02} \end{figure} @@ -272,7 +272,7 @@ \subsection{Step 3: Pseudo-Earthquake Cycle Model} $$ pylith step03.cfg \end{shell} The simulation will produce pairs of HDF5/Xdmf files with separate -files for each material and fault interface. Figure \vref{fig:example:subduction:step03}, +files for each material and fault interface. Figure \vref{fig:example:subduction:2d:step03}, which was created using ParaView, displays the magnitude of the displacement field with the deformation exaggerated by a factor of 1000. Using the animation features within ParaView or Visit you can illustrate @@ -280,11 +280,11 @@ \subsection{Step 3: Pseudo-Earthquake Cycle Model} after subsiding during the interseismic deformation. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction_step03_soln} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step03_soln} \caption{Solution for Step 3 at 150 years (immediately following the earthquake rupture). The colors indicate the magnitude of the displacement, and the deformation is exaggerated by a factor of 1000.} - \label{fig:example:subduction:step03} + \label{fig:example:subduction:2d:step03} \end{figure} @@ -309,7 +309,7 @@ \subsection{Step 4: Frictional Afterslip Simulation} model. Slip will occur in regions where the coseismic slip increased the shear tractions by more than 2.0 MPa. On the lateral and bottom boundaries of the domain, we fix the degrees of freedom perpendicular -to the boundary as shown in Figure \vref{fig:example:subduction:steps}. +to the boundary as shown in Figure \vref{fig:example:subduction:2d:steps}. Parameter settings that augment those in \filename{pylithapp.cfg} are contained in the file \filename{step04.cfg}. These settings are: \begin{inventory} @@ -340,7 +340,7 @@ \subsection{Step 4: Frictional Afterslip Simulation} each material (eight pairs of files), and fault parameters, slip, and traction (two pairs of files). -Figure \vref{fig:example:subduction:step04}, which was created using +Figure \vref{fig:example:subduction:2d:step04}, which was created using ParaView, displays the magnitude of the displacement field with the original configuration. Slip occurs down-dip from the coseismic slip as well as in three areas with sharp gradients in slip, including @@ -349,10 +349,10 @@ \subsection{Step 4: Frictional Afterslip Simulation} field. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction_step01_soln} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step01_soln} \caption{Solution for Step 4. The colors indicate the magnitude of the displacement.} - \label{fig:example:subduction:step04} + \label{fig:example:subduction:2d:step04} \end{figure} diff --git a/doc/userguide/examples/subduction3d.py b/doc/userguide/examples/subduction3d.py new file mode 100644 index 0000000000..c5c935bc3b --- /dev/null +++ b/doc/userguide/examples/subduction3d.py @@ -0,0 +1,255 @@ +from examples_info import Features + +from collections import OrderedDict +examples = OrderedDict() + +examples["3d/subduction/step01"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_STATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Bulk Rheology": { + "Linear elastic": 4, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ILU, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 2, + "Simple": 4, + }, +} + +examples["3d/subduction/step02"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 1, + "Slip time function": Features.SLIPFN_STEP, + }, + "Bulk Rheology": { + "Linear elastic": 2, + "Linear Maxwell viscoelastic": 2, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 2, + "Simple": 3, + "Simple grid": 2, + "Composite": 2, + }, +} + +examples["3d/subduction/step03"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 2, + "Slip time function": Features.SLIPFN_RATE, + }, + "Bulk Rheology": { + "Linear elastic": 2, + "Linear Maxwell viscoelastic": 2, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 4, + "Simple": 3, + "Simple grid": 2, + "Composite": 2, + }, +} + +examples["3d/subduction/step04"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 3, + "Slip time function": Features.SLIPFN_STEP, + }, + "Bulk Rheology": { + "Linear elastic": 2, + "Linear Maxwell viscoelastic": 2, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 7, + "Simple": 3, + "Simple grid": 5, + "Composite": 2, + }, +} + +examples["3d/subduction/step05"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 1, + "Slip time function": Features.SLIPFN_RATE, + "Constitutive model": 1, + "Slip-weakening friction": True, + "Traction perturbation": True, + }, + "Bulk Rheology": { + "Linear elastic": 2, + "Linear Maxwell viscoelastic": 2, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_NONLINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 7, + "Simple": 3, + "Simple grid": 5, + "Composite": 2, + }, +} + + +examples["3d/subduction/step06"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 1, + "Slip time function": Features.SLIPFN_TIMEHISTORY, + }, + "Bulk Rheology": { + "Linear elastic": 4, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_NONLINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "Point output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 1, + "Simple": 4, + "Simple grid": 1, + "Time history": 1, + }, +} + + +# End of file diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex new file mode 100644 index 0000000000..2ca4b361f1 --- /dev/null +++ b/doc/userguide/examples/subduction3d.tex @@ -0,0 +1,198 @@ +\section{Examples for a 3D Subduction Zone} +\label{sec:example:subduction:3d} + +The files associated with this suite of examples are contained in the +directory \filename{examples/3d/subduction}. + + +\subsection{Overview} + +% Description - based on Cascadia subduction zone + +% Materials - slab, mangle, crust, and wedge + +% Faults - slab_top, slab_bot, splay + +% Coordinate system - transverse Mercator projection w/Portland as the origin + +% Use ParaView Python scripts + +% Organization of files (mesh, spatialdb, viz). + +\subsection{Features Illustrated} + +\subsection{Mesh Description} + +% mesh directory CUBIT/Trelis + +% Geometry + +% Size of domain + +% Slab - create 3D (extend up-dip, offset to depth normal to surface) + +% Splay + +% tet (hex is alternative) + +\subsection{Organization of Parameters} + +% pylithapp +% + mesh +% + materials +% + boundary conditions +% + output +% + solver + +% solver* +% production preconditioners for use with and without faults + +% mat* +% + linear, isotropic elastic material model for all materials +% + linear, isotropic elastic material model for crust, wedge, linear Maxwell viscoelastic model with depth-dependent viscosity for slab, mantle + +As in the examples discussed in previous sections of these examples, +we place parameters common to the three steps in the \filename{pylithapp.cfg} +file so that we do not have to duplicate them for each step. The settings +contained in \filename{pylithapp.cfg} for this problem consist of: +\begin{inventory} + \facilityitem{pylithapp.journal.info}{Settings that control the + verbosity of the output written to stdout for the different + components.} \facilityitem{pylithapp.mesh\_generator}{Settings + that control mesh importing, such as the importer type, the + filename, and the spatial dimension of the mesh.} + \facilityitem{pylithapp.timedependent}{Settings that control the + problem, such as the total time, time-step size, and spatial + dimension.} + \facilityitem{pylithapp.timedependent.materials}{Settings that + control the material type, specify which material IDs are to be + associated with a particular material type, and give the name of + the spatial database containing the physical properties for the + material. The quadrature information is also given.} + \facilityitem{pylithapp.problem.formulation.output}{Settings related + output of the solution over the domain and subdomain (ground + surface).} + \facilityitem{pylithapp.timedependent.materials.\textit{MATERIAL}.output}{Settings + related to output of the state variables for material + \textit{MATERIAL}.} \facilityitem{pylithapp.petsc}{PETSc settings + to use for the problem, such as the preconditioner type.} +\end{inventory} +The physical properties for each material are specified in spatial +database files. For example, the elastic properties for the +continental crust are in \filename{mat\_concrust.spatialdb}. The +provided spatial database files all use just a single point to specify +uniform physical properties within each material. A good exercise is +to alter the spatial database files with the physical properties to +match PREM. + + +\subsection{Step 1: Axial Compression} + +% big picture +% + squeeze boundaries => DirichletBC with prescribed displacements +% + elastic material properties => linear solver with single time step + + +% Squeeze + +The first example problem is earthquake rupture involving coseismic +slip along the interface between the subducting slab and the continental +crust and uppermost portion of the mantle below the continental crust. +The spatial variation of slip comes from a cross-section of Gavin +Hayes' finite-source model \url{earthquake.usgs.gov/earthquakes/eqinthenews/2011/usc0001xgp/finite_fault.php}. +On the lateral and bottom boundaries of the domain, we fix the degrees +of freedom perpendicular to the boundary as shown in Figure \vref{fig:example:subduction:2d:steps}. +Parameter settings that augment those in \filename{pylithapp.cfg} are +contained in the file \filename{step01.cfg}. These settings are: +\begin{inventory} + \facilityitem{pylithapp.timedependent.formulation.time\_step}{Adjust the total + simulation time to 0 years (static simulation).} + \facilityitem{pylithapp.timedependent}{Specifies the array of + boundary conditions.} + \facilityitem{pylithapp.timedependent.bc.\textit{BOUNDARY}}{Defines the settings + for boundary \textit{BOUNDARY}, including which degrees of freedom + are being constrained (x or y), the label (defined in\filename{ mesh\_tri3.exo}) + corresponding to the nodeset in CUBIT, and a label to the boundary + condition used in any error messages.} + \facilityitem{pylithapp.timedependent.interfaces.fault}{Specify the coseismic + slip along the interface between the oceanic crust and continental + crust with a small amount of slip penetrating into the upper mantle.} + \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the base filenames + for HDF5 output (for example, \filename{step01.h5}).} +\end{inventory} +We run this example by typing +\begin{shell} +$$ pylith step01.cfg +\end{shell} +The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 +files contain the data and the Xdmf files contain the metadata required +by ParaView and Visit (and possibly other visualization tools that +use Xdmf files) to access the mesh and data sets in the HDF5 files. +The files include the solution over the domain and ground surface +(two pairs of files), physical properties, stress, and strain within +each material (eight pairs of files), and fault parameters, slip, +and traction (two pairs of files). + +Figure \vref{fig:example:subduction:2d:step01}, which was created using +ParaView, displays the magnitude of the displacement field with the +deformation exaggerated by a factor of 1000. + +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step01_soln} + \caption{Solution for Step 1. The colors indicate the magnitude of the displacement, + and the deformation is exaggerated by a factor of 1000. } + \label{fig:example:subduction:2d:step01} +\end{figure} + + +\subsubsection{Exercises} + +% Algebraic multigrid preconditioner +% Adjust material properties (stiffer, softer, nearly incompressible) +% Pure shear instead of axial compression + +\subsection{Step 2: Postseismic Relaxation} + +\subsubsection{Exercises} + +% Change slip on slab to slip on splay fault +% Slip on lower slab and splay fault +% Slip on slab and splay fault + +\subsection{Step 3: Interseismic Deformation} + +\subsubsection{Exercises} + +\subsection{Step 4: Prescribed Earthquake Cycle} + +\subsubsection{Exercises} + +% Make lower slab + splay fault the primary fault surface and the +% upper slab (trench side of the splay fault) the secondary fault +% surface. Hint: You will need to create a nodesets in CUBIT that +% correspond to the primary and secondary fault surfaces. + + + +\subsection{Step 5: Spontaneous Rupture Driven by Subducting Slab} + +\subsubsection{Exercises} + +\subsection{Step 6: Prescribed Slow-Slip Event} + +\subsubsection{Exercises} + +% Change spatial distribution and time history of slip. + +\subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} + +\subsubsection{Exercises} + +% Move slip to splay fault in step06 and redo inversion. +% Adjust noise level +% Invert for slip at each time step + +\subsection{Step 8: Gravitational Body Forces} + + +% End of file diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 457b50ced2..59aaa57ff3 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -54,6 +54,11 @@ Features: Generation of spatial databases via Python + Coordinate systems + + + Geographic projection + + Geographic + Faults + Buried edges [2,3] + Intersecting diff --git a/examples/3d/subduction/TODO b/examples/3d/subduction/TODO index 633f2e3f83..e69de29bb2 100644 --- a/examples/3d/subduction/TODO +++ b/examples/3d/subduction/TODO @@ -1,4 +0,0 @@ -ParaView Python script to plot slip contours and shear traction / normal traction. - -ParaView Python script to plot fault normal_dir, dip_dir, strike_dir - From f46065e148ee7f9fb86dd5b96f5b5128d5708d8e Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 20 Jun 2017 15:16:15 +1200 Subject: [PATCH 072/216] Added script to generate initial stresses for step08. Added initial stress spatialdb for homogeneous properties. Added __init__.py so we can import coordsys. Added .cfg files for step08a and step08b. --- .../3d/subduction/generate_initial_stress.py | 78 ++++++++++++ examples/3d/subduction/mesh/__init__.py | 18 +++ .../initial_stress-homogeneous.spatialdb | 47 +++++++ examples/3d/subduction/step08a.cfg | 118 ++++++++++++++++++ examples/3d/subduction/step08b.cfg | 118 ++++++++++++++++++ 5 files changed, 379 insertions(+) create mode 100755 examples/3d/subduction/generate_initial_stress.py create mode 100755 examples/3d/subduction/mesh/__init__.py create mode 100644 examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb create mode 100644 examples/3d/subduction/step08a.cfg create mode 100644 examples/3d/subduction/step08b.cfg diff --git a/examples/3d/subduction/generate_initial_stress.py b/examples/3d/subduction/generate_initial_stress.py new file mode 100755 index 0000000000..284f04c21e --- /dev/null +++ b/examples/3d/subduction/generate_initial_stress.py @@ -0,0 +1,78 @@ +#!/usr/bin/env nemesis +""" +This script creates a spatial database for the initial stress using results +from a previous PyLith run. +""" + +dbPrefix = "initial_stress" +matPrefix = "step08a" +materials = ["crust","mantle","slab","wedge"] + +import numpy +import h5py +# import pdb +# pdb.set_trace() + +from spatialdata.spatialdb.SimpleIOAscii import SimpleIOAscii +from mesh.coordsys import cs_mesh +cs = cs_mesh() + +def getCellCenters(vertices, cells): + """ + Function to compute cell centers. + """ + cellCoords = vertices[cells, :] + cellCenters = numpy.mean(cellCoords, axis=1) + + return cellCenters + + +for material in materials: + + filenameH5 = "output/%s-%s.h5" % (matPrefix, material) + filenameDB = "spatialdb/%s-%s.spatialdb" % (dbPrefix, material) + + # Open HDF5 file and get coordinates, cells, and stress. + h5 = h5py.File(filenameH5, "r") + vertices = h5['geometry/vertices'][:] + cells = numpy.array(h5['topology/cells'][:], dtype=numpy.int) + stress = h5['cell_fields/stress'][0,:,:] + h5.close() + + # Compute coordinates of quadrature points. + quadCoords = getCellCenters(vertices, cells) + + ncells = cells.shape[0] + nvalues = stress.shape[1] + + # Create writer for spatial database file + writer = SimpleIOAscii() + writer.inventory.filename = filenameDB + writer._configure() + + values = [{'name': "stress-xx", + 'units': "Pa", + 'data': stress[:,0]}, + {'name': "stress-yy", + 'units': "Pa", + 'data': stress[:,1]}, + {'name': "stress-zz", + 'units': "Pa", + 'data': stress[:,2]}, + {'name': "stress-xy", + 'units': "Pa", + 'data': stress[:,3]}, + {'name': "stress-yz", + 'units': "Pa", + 'data': stress[:,4]}, + {'name': "stress-xz", + 'units': "Pa", + 'data': stress[:,5]}, + ] + + writer.write({'points': quadCoords, + 'coordsys': cs, + 'data_dim': 3, + 'values': values}) + +# End of file diff --git a/examples/3d/subduction/mesh/__init__.py b/examples/3d/subduction/mesh/__init__.py new file mode 100755 index 0000000000..15c9df3a48 --- /dev/null +++ b/examples/3d/subduction/mesh/__init__.py @@ -0,0 +1,18 @@ +#!/usr/bin/env python +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# End of file diff --git a/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb b/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb new file mode 100644 index 0000000000..442d0b9ed8 --- /dev/null +++ b/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb @@ -0,0 +1,47 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies the initial stresses for the model +// The stresses increase linearly with depth assuming densities +// corresponding to mantle material. +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 6 // number of stress components + + // names of the stress components + value-names = stress-xx stress-yy stress-zz stress-xy stress-yz stress-xz + + value-units = Pa Pa Pa Pa Pa Pa // units + + num-locs = 2 // number of locations: 1 value each at the upper and lower + // surfaces. Linear interpolation should be used. + + data-dim = 1 + space-dim = 3 + cs-data = geo-projected { + to-meters = 1 + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } + } +} +// Columns are +// (1) x coordinate (m) +// (2) y coordinate (m) +// (3) z coordinate (m) +// (4) stress-xx (Pa) +// (5) stress-yy (Pa) +// (6) stress-zz (Pa) +// (7) stress-xy (Pa) +// (8) stress-yz (Pa) +// (9) stress-xz (Pa) +0.0 0.0 -4000000.0 -12944778000.0 -12944778000.0 -12944778000.0 0.0 0.0 0.0 +0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg new file mode 100644 index 0000000000..988b86c04b --- /dev/null +++ b/examples/3d/subduction/step08a.cfg @@ -0,0 +1,118 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions and gravity. The gravitational +# stresses are computed using the properties in mat_elastic.cfg, but +# we balance them using initial stresses consistent with uniform +# properties corresponding to the mantle. This means that the stresses +# will not balance and we should see deformation as a result of the +# out-of-balance stresses. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step08a.cfg (main parameter file for step08a) +# - mat_elastic.cfg (material models and parameters) +# +# This problem does not include a fault, so we use the default +# solver settings in pylithapp.cfg. +# +# To run the simulation: +# pylith step08a.cfg mat_elastic.cfg +# +# Output will be directed to the "output" directory. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step08a-parameters.json +problem.progress_monitor.filename = output/step08a-progress.txt + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +# Set gravity field (default is None). +gravity_field = spatialdata.spatialdb.GravityField + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 0.0*year +dt = 0.1*year + +# ---------------------------------------------------------------------- +# initial stresses +# ---------------------------------------------------------------------- +# We must specify initial stresses for each material. +# We provide a filename for the spatial database that gives the stresses, +# and we change the query_type from the default 'nearest' to 'linear'. +[pylithapp.problem.materials.slab] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the slab +db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.query_type = linear + +[pylithapp.problem.materials.wedge] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the wedge +db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.query_type = linear + +[pylithapp.problem.materials.mantle] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the mantle +db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.query_type = linear + +[pylithapp.problem.materials.crust] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the crust +db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.query_type = linear + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step08a-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step08a-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step08a-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step08a-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step08a-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step08a-mantle.h5 + + +# End of file diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg new file mode 100644 index 0000000000..61a89a23b6 --- /dev/null +++ b/examples/3d/subduction/step08b.cfg @@ -0,0 +1,118 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is an elastic quasistatic problem using Dirichlet +# (displacement) boundary conditions and gravity. The gravitational +# stresses are computed using the properties in mat_elastic.cfg. In +# this case, we balance them with initial stresses computed from +# step08a.cfg, so the stresses should balance and we should see no +# deformation. After running step08a, generate the initial stresses: +# +# ./generate_initial_stress.py +# +# This will generate the initial stress database needed for this simulation. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step08b.cfg (main parameter file for step08b) +# - mat_elastic.cfg (material models and parameters) +# +# This problem does not include a fault, so we use the default +# solver settings in pylithapp.cfg. +# +# To run the simulation: +# pylith step08b.cfg mat_elastic.cfg +# +# Output will be directed to the "output" directory. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step08b-parameters.json +problem.progress_monitor.filename = output/step08b-progress.txt + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +# Set gravity field (default is None). +gravity_field = spatialdata.spatialdb.GravityField + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 0.0*year +dt = 0.1*year + +# ---------------------------------------------------------------------- +# initial stresses +# ---------------------------------------------------------------------- +# We must specify initial stresses for each material. +# We provide a filename for the spatial database that gives the stresses. +# Since there is a point in the database corresponding to each cell +# center, we keep the default query_type of 'nearest'. +[pylithapp.problem.materials.slab] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the slab +db_initial_stress.iohandler.filename = spatialdb/initial_stress-slab.spatialdb + +[pylithapp.problem.materials.wedge] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the wedge +db_initial_stress.iohandler.filename = spatialdb/initial_stress-wedge.spatialdb + +[pylithapp.problem.materials.mantle] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the mantle +db_initial_stress.iohandler.filename = spatialdb/initial_stress-mantle.spatialdb + +[pylithapp.problem.materials.crust] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the crust +db_initial_stress.iohandler.filename = spatialdb/initial_stress-crust.spatialdb + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step08b-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step08b-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step08b-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step08b-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step08b-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step08b-mantle.h5 + + +# End of file From c219283925444268407e876ac1e55854592ba66e Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 20 Jun 2017 15:51:00 +1200 Subject: [PATCH 073/216] Updated to use algebraic multigrid solver. Added step08c: viscoelastic with finite strain. --- examples/3d/subduction/step08a.cfg | 7 +- examples/3d/subduction/step08b.cfg | 7 +- examples/3d/subduction/step08c.cfg | 120 +++++++++++++++++++++++++++++ 3 files changed, 128 insertions(+), 6 deletions(-) create mode 100644 examples/3d/subduction/step08c.cfg diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg index 988b86c04b..a020b74fb2 100644 --- a/examples/3d/subduction/step08a.cfg +++ b/examples/3d/subduction/step08a.cfg @@ -32,12 +32,13 @@ # - pylithapp.cfg (common paramters, read by default) # - step08a.cfg (main parameter file for step08a) # - mat_elastic.cfg (material models and parameters) +# - solver_algebraicmultigrid.cfg (algebraic multigrid solver settings) # -# This problem does not include a fault, so we use the default -# solver settings in pylithapp.cfg. +# This problem does not include a fault, so we use the algebraic +# multigrid settings in solver_algebraicmultigrid.cfg. # # To run the simulation: -# pylith step08a.cfg mat_elastic.cfg +# pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg index 61a89a23b6..3e82d37e64 100644 --- a/examples/3d/subduction/step08b.cfg +++ b/examples/3d/subduction/step08b.cfg @@ -35,12 +35,13 @@ # - pylithapp.cfg (common paramters, read by default) # - step08b.cfg (main parameter file for step08b) # - mat_elastic.cfg (material models and parameters) +# - solver_algebraicmultigrid.cfg (algebraic multigrid solver settings) # -# This problem does not include a fault, so we use the default -# solver settings in pylithapp.cfg. +# This problem does not include a fault, so we use the algebraic +# multigrid settings in solver_algebraicmultigrid.cfg. # # To run the simulation: -# pylith step08b.cfg mat_elastic.cfg +# pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step08c.cfg b/examples/3d/subduction/step08c.cfg new file mode 100644 index 0000000000..3cf2a2d362 --- /dev/null +++ b/examples/3d/subduction/step08c.cfg @@ -0,0 +1,120 @@ +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This is a viscoelastic quasistatic problem using Dirichlet +# (displacement) boundary conditions, gravity, and finite strain. +# The gravitational stresses are computed using the properties in +# mat_elastic.cfg, and we balance them with initial stresses computed from +# step08a.cfg, just as we did for step08b. In this problem we use +# viscoelastic materials and the small strain formulation, such that the +# stresses are recomputed for the deformed configuration. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# Parameter files: +# - pylithapp.cfg (common paramters, read by default) +# - step08c.cfg (main parameter file for step08c) +# - mat_viscoelastic.cfg (material models and parameters) +# - solver_algebraicmultigrid.cfg (algebraic multigrid solver settings) +# +# This problem does not include a fault, so we use the algebraic +# multigrid settings in solver_algebraicmultigrid.cfg. +# +# To run the simulation: +# pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg +# +# Output will be directed to the "output" directory. + +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step08c-parameters.json +problem.progress_monitor.filename = output/step08c-progress.txt + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +# Turn on the small strain formulation, which automatically runs the +# simulation as a nonlinear problem. +formulation = pylith.problems.ImplicitLgDeform + +# Set gravity field (default is None). +gravity_field = spatialdata.spatialdb.GravityField + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +total_time = 100.0*year +dt = 10.0*year + +# ---------------------------------------------------------------------- +# initial stresses +# ---------------------------------------------------------------------- +# We must specify initial stresses for each material. +# We provide a filename for the spatial database that gives the stresses. +# Since there is a point in the database corresponding to each cell +# center, we keep the default query_type of 'nearest'. +[pylithapp.problem.materials.slab] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the slab +db_initial_stress.iohandler.filename = spatialdb/initial_stress-slab.spatialdb + +[pylithapp.problem.materials.wedge] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the wedge +db_initial_stress.iohandler.filename = spatialdb/initial_stress-wedge.spatialdb + +[pylithapp.problem.materials.mantle] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the mantle +db_initial_stress.iohandler.filename = spatialdb/initial_stress-mantle.spatialdb + +[pylithapp.problem.materials.crust] +db_initial_stress = spatialdata.spatialdb.SimpleDB +db_initial_stress.label = Initial stress in the crust +db_initial_stress.iohandler.filename = spatialdb/initial_stress-crust.spatialdb + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- + +# Domain and subdomain output --------------------------------- +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step08c-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step08c-groundsurf.h5 + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +writer.filename = output/step08c-slab.h5 + +[pylithapp.problem.materials.wedge.output] +writer.filename = output/step08c-wedge.h5 + +[pylithapp.problem.materials.crust.output] +writer.filename = output/step08c-crust.h5 + +[pylithapp.problem.materials.mantle.output] +writer.filename = output/step08c-mantle.h5 + + +# End of file From 9c74ca1e9d2f25d2664dcc14d388b1c14153bf9e Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 11:52:12 -0700 Subject: [PATCH 074/216] Adjust lines in slow slip Python script. --- examples/3d/subduction/spatialdb/generate_slowslip.py | 10 ++++++---- 1 file changed, 6 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/spatialdb/generate_slowslip.py b/examples/3d/subduction/spatialdb/generate_slowslip.py index c4c87503c6..98dd99c2be 100755 --- a/examples/3d/subduction/spatialdb/generate_slowslip.py +++ b/examples/3d/subduction/spatialdb/generate_slowslip.py @@ -149,8 +149,11 @@ def _makeGrid(self): lonGrid, latGrid = numpy.meshgrid(self.lon, self.lat) zGrid = numpy.zeros_like(lonGrid) - self.grid = numpy.column_stack((lonGrid.flatten(), latGrid.flatten(), - zGrid.flatten())) + self.grid = numpy.column_stack(( + lonGrid.flatten(), + latGrid.flatten(), + zGrid.flatten(), + )) return @@ -231,8 +234,7 @@ def _writeTemporaldb(self): amplitude = [float(i) for i in self.slipAmplitudes] amplitudeArr = numpy.array(amplitude, dtype=numpy.float64) - TimeHistoryIO.write(timeArr, amplitudeArr, self.slipTimeUnits, - self.timeDbFilename) + TimeHistoryIO.write(timeArr, amplitudeArr, self.slipTimeUnits, self.timeDbFilename) return From bec21143ae8ca58acbc0a1b5d41bed01e86ba2c6 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 11:53:46 -0700 Subject: [PATCH 075/216] Cleanup descriptions of steps. --- examples/3d/subduction/step01.cfg | 20 ++++++------ examples/3d/subduction/step02.cfg | 13 ++++---- examples/3d/subduction/step03.cfg | 16 +++++----- examples/3d/subduction/step04.cfg | 17 +++++++---- examples/3d/subduction/step05.cfg | 27 ++++++++++++---- examples/3d/subduction/step06.cfg | 35 +++++++++++++++------ examples/3d/subduction/step07a.cfg | 49 +++++++++--------------------- examples/3d/subduction/step07b.cfg | 44 ++++++++------------------- 8 files changed, 110 insertions(+), 111 deletions(-) diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index 2897bbc817..8884f78f2b 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -18,19 +18,17 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# -# This is a purely elastic static problem using only Dirichlet -# (displacement) boundary conditions. -# -# The positive and negative x-boundaries yield 4 m of axial -# compression. The negative z-boundary and positive and negative -# y-boundaries are held fixed in the direction normal to the boundary. +# We simulate axial compression in the east-west direction using +# Dirichlet (displacement) boundary conditions. # # Materials -# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). # # Boundary Conditions -# Roller boundary conditions (pylithapp.cfg). +# Roller boundary conditions (pylithapp.cfg); on the positive and +# negative x-boundaries we prescribe 2.0 m of displacement yielding +# 4 m of axial compression. # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -41,8 +39,8 @@ # - step01.cfg (main parameter file for step01) # - mat_elastic.cfg (material models and parameters) # -# To run the simulation: -# pylith step01.cfg mat_elastic.cfg +# TO RUN THE SIMULATION: +# pylith step01.cfg mat_elastic.cfg # # Output will be directed to the "output" directory.. diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index 4a9861e67b..9caf057961 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -16,10 +16,8 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This problem focuses on viscoelastic relaxation from coseismic slip -# on a patch in the middle of the top of the slab. We prescribe -# uniform fault slip on the slab fault rupture patch with zero -# displacement on the lateral and bottom boundaries. +# We simulate postseismic viscoelastic relaxation from coseismic slip +# on a patch in the middle of the top of the slab. # # Materials # The 'wedge' and 'crust' blocks use the the linear, isotropic @@ -29,6 +27,9 @@ # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# Uniform oblique slip on the slab fault rupture patch. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -44,8 +45,8 @@ # Lagrange multiplier field. We use these solver settings in several # simulations, so we put them in a separate file. # -# To run the simulation: -# pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +# TO RUN THE SIMULATION: +# pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index b788238757..e44f14e210 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -16,11 +16,9 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This problem focuses on interseismic deformation with viscoelastic -# relaxation combined with aseismic slip. We use both Dirichlet -# boundary conditions to constrain the displacements on the lateral -# and bottom boundaries. The subducting slab uses prescribed slip with -# a constant slip rate time function. +# We simulate interseismic deformation, combining aseismic slip on the +# top and bottom of the subducting slab with viscoelastic relaxation +# in the mantle and the deep part of the slab. # # Materials # The 'wedge' and 'crust' blocks use the the linear, isotropic @@ -30,6 +28,10 @@ # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# Uniform creep on the bottom of the slab. +# Uniform creep on the deeper portion of the top of the slab. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -40,8 +42,8 @@ # - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # -# To run the simulation: -# pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +# TO RUN THE SIMULATION: +# pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index 63f690d744..3f3bbe3f49 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -16,10 +16,9 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# We combine the interseismic deformation in Step03 with coseismic -# slip to model two earthquake cycles. The coseismic slip exactly -# complements the aseismic slip at depth; we also include an -# earthquake with coseismic slip on the splay fault. +# We simulate a simple earthquake cycle by superimposing coseismic +# slip on the top of the slab and splay fault with interseismic +# deformation matchnig that in Step03. # # Materials # The 'wedge' and 'crust' blocks use the the linear, isotropic @@ -29,6 +28,12 @@ # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# + Uniform creep on the bottom of the slab. +# + Uniform creep on the deeper portion of the top of the slab. +# + Coseismic slip on the shallow portion of the top of the slab. +# + Coseismic slip on the splay fault. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -39,8 +44,8 @@ # - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # -# To run the simulation: -# pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +# TO RUN THE SIMULATION: +# pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg index 976f8094b6..8644897708 100644 --- a/examples/3d/subduction/step05.cfg +++ b/examples/3d/subduction/step05.cfg @@ -19,10 +19,6 @@ # This problem drives spontaneous rupture on the subduction zone # interface (top of the slab) via interseismic deformation. # -# We include viscoelastic relaxation and prescribed aseismic slip on -# the bottom of the slab. We use Dirichlet boundary conditions to -# constrain the displacements on the lateral and bottom boundaries. -# # Materials # The 'wedge' and 'crust' blocks use the the linear, isotropic # elastic material model, whereas the 'slab' and 'mantle' use the @@ -31,6 +27,11 @@ # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# + Uniform creep on the bottom of the slab. +# + Spontaneous rupture (slip-weakening friction) on the top of the +# slab with stable sliding on the shallow and deeper portions. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -41,8 +42,8 @@ # - mat_viscoelastic.cfg (material models and parameters) # - solver_fieldsplit.cfg (field split solver settings) # -# To run the simulation: -# pylith step05.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +# TO RUN THE SIMULATION: +# pylith step05.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory. @@ -205,4 +206,18 @@ ksp_atol = 1.0e-11 snes_rtol = 1.0e-20 snes_atol = 1.0e-9 +# Friction sensitivity solve used to compute the increment in slip +# associated with changes in the Lagrange multiplier imposed by the +# fault constitutive model. +friction_pc_type = asm +friction_sub_pc_factor_shift_type = nonzero +friction_ksp_max_it = 25 +friction_ksp_gmres_restart = 30 +friction_ksp_error_if_not_converged = true + +# Uncomment to view details of friction sensitivity solve. +#friction_ksp_monitor = true +#friction_ksp_view = true +#friction_ksp_converged_reason = true + # End of file diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index a54caf59d4..46c776567f 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -16,13 +16,23 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions and prescribed fault slip to -# simulate a slow slip event (SSE). The slip occurs over a time -# period of one year, with fault slip specified by both a spatialdb -# (to provide an approximately Gaussian slip distribution) and a -# temporal database to control the slip amplitude as a function of -# time. +# We simulate a slow-slip event (SSE) on a patch in the middle of the +# top of the slab. +# +# Materials +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). +# +# Fault +# Uniform oblique slip with a duration of one month on the slab +# fault rupture patch. +# +# Output +# We output the displacements for the slip impulses on the ground +# surface ang at the fake cGPS locations defined by cgps_sites.txt. # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -39,8 +49,15 @@ # Lagrange multiplier field. We use these solver settings in several # simulations, so we put them in a separate file. # -# To run the simulation: -# pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg +# BEFORE RUNNING THE SIMULATION, run the Python script that generates +# the spatial database with the final slip distribution and the +# temporal database with the slip time function. +# +# cd spatialdb && generate_slowslip.py +# +# TO RUN THE SIMULATION: +# +# pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory. diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 8a8e281a44..cdc73142b2 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -16,48 +16,29 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are two +# In this problem we generate Green's functions that will be used to +# invert synthetic data generated from step06. There are two # different sub-problems: +# # step07a: Generate Green's functions corresponding to left-lateral # slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to updip +# step07b: Generate Green's functions corresponding to reverse # slip on the subduction interface (slab top). # -# Responses (Green's functions) are computed at simulated cGPS -# locations defined in the file cgps_sites.txt. -# Note that we change the default problem type from TimeDependent to -# GreensFns. -# -# Prior to generating the Green's functions, we first generate synthetic -# data from the output of problem step06, using the make_synthetic_gpsdisp.py -# script, with parameters defined in make_synthetic_gpsdisp.cfg: -# -# ./make_synthetic_gpsdisp.py -# -# After generating the synthetic data and Green's functions, we then -# perform a simple inversion using the slip_invert.py script, with -# parameters defined in slip_invert.cfg: -# -# ./slip_invert.py -# -# This will generate two HDF files that may be viewed in Paraview: -# step07-inversion-slip.h5: The predicted fault slip. -# step07-inversion-displacement.h5: The predicted surface displacements. -# -# There is also an inversion summary file: step07-inversion-summary.txt -# If you have matplotlib installed, you can view a log-log plot of -# solution misfit by going into the viz directory and running: -# -# ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt -# -# # Materials -# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). # # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# Slip impulses for left-lateral slip on the suduction interface (slab top). +# +# Output +# We output the displacements for the slip impulses on the ground +# surface at at the fake cGPS locations defined by cgps_sites.txt. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -74,8 +55,8 @@ # Lagrange multiplier field. We use these solver settings in several # simulations, so we put them in a separate file. # -# To run the simulation: -# pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg +# TO RUN THE SIMULATION: +# pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index fe2b9f02ab..a4e3febd9e 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -16,48 +16,28 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# In this problem we generate Green's functions that will be used -# to invert synthetic data generated from step06. There are two +# In this problem we generate Green's functions that will be used to +# invert synthetic data generated from step06. There are two # different sub-problems: +# # step07a: Generate Green's functions corresponding to left-lateral # slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to updip +# step07b: Generate Green's functions corresponding to reverse # slip on the subduction interface (slab top). # -# Responses (Green's functions) are computed at simulated cGPS -# locations defined in the file cgps_sites.txt. -# Note that we change the default problem type from TimeDependent to -# GreensFns. -# -# Prior to generating the Green's functions, we first generate synthetic -# data from the output of problem step06, using the make_synthetic_gpsdisp.py -# script, with parameters defined in make_synthetic_gpsdisp.cfg: -# -# ./make_synthetic_gpsdisp.py -# -# After generating the synthetic data and Green's functions, we then -# perform a simple inversion using the slip_invert.py script, with -# parameters defined in slip_invert.cfg: -# -# ./slip_invert.py -# -# This will generate two HDF files that may be viewed in Paraview: -# step07-inversion-slip.h5: The predicted fault slip. -# step07-inversion-displacement.h5: The predicted surface displacements. -# -# There is also an inversion summary file: step07-inversion-summary.txt -# If you have matplotlib installed, you can view a log-log plot of -# solution misfit by going into the viz directory and running: -# -# ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt -# -# # Materials # All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). # # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). # +# Fault +# Slip impulses for reverse slip on the suduction interface (slab top). +# +# Output +# We output the displacements for the slip impulses on the ground +# surface at at the fake cGPS locations defined by cgps_sites.txt. +# # ---------------------------------------------------------------------- # RUNNING THE SIMULATON # ---------------------------------------------------------------------- @@ -74,7 +54,7 @@ # Lagrange multiplier field. We use these solver settings in several # simulations, so we put them in a separate file. # -# To run the simulation: +# TO RUN THE SIMULATION: # pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. From 4efe39c1264ed24984f54aa23b6ed99f3f7287ec Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 11:54:18 -0700 Subject: [PATCH 076/216] Consolidate lines. --- examples/3d/subduction/make_synthetic_gpsdisp.py | 9 +++------ 1 file changed, 3 insertions(+), 6 deletions(-) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index 0a0c1dfa7e..596c477e59 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -43,8 +43,7 @@ class MakeSyntheticGpsdisp(Application): ## @li \b vtk_output_file Name of VTK output file. ## - pointInputFile = pyre.inventory.str("point_input_file", - default="cascadia-cgps_points.h5") + pointInputFile = pyre.inventory.str("point_input_file", default="cascadia-cgps_points.h5") pointInputFile.meta['tip'] = "HDF5 point output file from PyLith." timeStep = pyre.inventory.int("time_step", default=0) @@ -59,12 +58,10 @@ class MakeSyntheticGpsdisp(Application): sigmaUp = pyre.inventory.float("sigma_up", default=0.001) sigmaUp.meta['tip'] = "Sigma value for Up displacements." - outputFile = pyre.inventory.str("output_file", - default="cascadia-cgps_disp.txt") + outputFile = pyre.inventory.str("output_file", default="cascadia-cgps_disp.txt") outputFile.meta['tip'] = "Name of ASCII output file." - vtkOutputFile = pyre.inventory.str("vtk_output_file", - default="cascadia-cgps_disp.vtk") + vtkOutputFile = pyre.inventory.str("vtk_output_file", default="cascadia-cgps_disp.vtk") vtkOutputFile.meta['tip'] = "Name of VTK output file." From 97a34a91253be279bf90d4a852c8a65f9f2948e4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 11:56:49 -0700 Subject: [PATCH 077/216] Added overview and mesh information to manual. --- doc/userguide/examples/examples_info.py | 4 +- .../examples/figs/subduction3d_cascadia.png | Bin 0 -> 134857 bytes .../figs/subduction3d_conceptualmodel.png | Bin 0 -> 13860 bytes doc/userguide/examples/subduction3d.tex | 189 +++++++++++++++--- .../examples/subduction3d_features.tex | 164 +++++++++++++++ doc/userguide/pylithdoc.cls | 1 + doc/userguide/userguide.tex | 16 +- 7 files changed, 347 insertions(+), 27 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_cascadia.png create mode 100644 doc/userguide/examples/figs/subduction3d_conceptualmodel.png create mode 100644 doc/userguide/examples/subduction3d_features.tex diff --git a/doc/userguide/examples/examples_info.py b/doc/userguide/examples/examples_info.py index 6008131347..3630662fc9 100755 --- a/doc/userguide/examples/examples_info.py +++ b/doc/userguide/examples/examples_info.py @@ -232,7 +232,7 @@ def writeHeader(self): """ f = self.fout - f.write("\\begin{table}[htbp]\n") + #f.write("\\begin{table}[htbp]\n") f.write("\\rowcolors{2}{yellow!30}{white}\n") ctags = ["|l|%% Example"] for category in self.columns: @@ -308,7 +308,7 @@ def writeFooter(self): if "description" in col: f.write("{\\bf %s} -- %s. " % (label, col["description"])) f.write("\\\\ \n") - f.write("\\end{table}") + #f.write("\\end{table}") return @staticmethod diff --git a/doc/userguide/examples/figs/subduction3d_cascadia.png b/doc/userguide/examples/figs/subduction3d_cascadia.png new file mode 100644 index 0000000000000000000000000000000000000000..e78e33e41e7960952b0c9ce697f63556497dbfb9 GIT binary patch literal 134857 zcmXtfRa9L~7vw>L%f;O<8VK(0?(PyGxVr@R;O-6qg1dXL5bVP(xV!t@e`d|oS*zdr z^zN?ORkfp3l%!FS2$28)K$Vq|Py+zyS^$75K!ApkHg0J22jCaL2l?r3js;ot^{yI7dIS(uZ1TDw`1OUo*% zXa}L;0RTB5D8C&6E$nH0*3GD!^f2z?A%@uy$TCi6h`lnahUDLs)`Bfp z7*ew+RyYk+`b$lV{u4B8!|29flyuiaf`z_sJpU$H63K`&@oGI*=Gw(bXmN2B|6jo! z-|tx4-lPa1a*;p)3i`{}0`@~A`(yI7jTbZ|yRQYEA`Fw98yE%Az8bag0DQMgnrmM9#h(PsK zebu#hI%m)EzU2KZEqK6#M&!}c_}8f>MB1(WrgtlfB;ap4*O=09`~_}5U9lChaAwVp zG%4pjDSmLl%me^EO}ED`oCL1WpsVS05H~dq>Vqr$6eY2}J2pOHn1peTx!?;04T~_U zBT=kcySO^N#Iv&m2&g+Wb#_Xt*!S7*g zn#H#T!6|%2QElx9mE|;bH5CJ)BlSDCmiLq4^6>1$!Q4> 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zSh@7d#AXwAPttrVA2>o$en`Z;Gz1w*Acg}I1fQ#n>9l7(tX)lHg=7))nEOTxB-u;JG^)3*NNkC?94 z`k7@0!<}9o9~Q2qhK$^fk3fKklJo!bC8wi12NdzRPxoI6pY8=;=YrIfwUx4O-hc7` E0Ek*~asU7T literal 0 HcmV?d00001 diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 2ca4b361f1..a7f75ac78f 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1,39 +1,144 @@ \section{Examples for a 3D Subduction Zone} \label{sec:example:subduction:3d} -The files associated with this suite of examples are contained in the -directory \filename{examples/3d/subduction}. - - \subsection{Overview} -% Description - based on Cascadia subduction zone - -% Materials - slab, mangle, crust, and wedge - -% Faults - slab_top, slab_bot, splay +This suite of examples demonstrates use of a wide variety of features +and the general workflow often used in research simulations. We base +the model on the Cascadia subduction zone +(Figure~\ref{fig:example:subduction:3d:cascadia}). These examples will +focus on modeling the deformation associated with the the subducting +slab, including interseismic deformation with aseismic slip (creep) +and viscoelastic relaxation, coseismic slip on the slab interface and +a splay fault, and slow slip events on the top slab interface. We want +to account for the 3-D material properties associated with different +elastic properties for the subducting slab, mantle, continental crust, +and an accretionary wedge. To keep the computation time in these +examples short, we limit our model to an 800 km $\times$ 800 km +$\times$ 400 km domain and we will use a relatively coarse +discretization. For simplicity and to reduce comlexity in constructing +the mesh, we use a flat top surface (elevation of 0 with respect +to mean sea level). + +\begin{figure}[htbp] + \includegraphics[width=4.5in]{examples/figs/subduction3d_cascadia} + \caption{Cartoon of the Cascadia Subduction Zone showing the + subduction of the Juan de Fuca Plate under the North American + Plate. Source: + \href{https://pubs.usgs.gov/fs/2000/fs060-00/}{U.S. Geological + Survey Fact Sheet 060-00}} + \label{fig:example:subduction:3d:cascadia} +\end{figure} -% Coordinate system - transverse Mercator projection w/Portland as the origin +Figure~\ref{fig:example:subduction:3d:concept} shows our conceptual +model with a slab, mantle, continental crust, and accretionary +wedge. We cut off the slab at a depth of 100 km. We use a transverse +geographic projection coordinate system with Portland, Oregon, as the +origin in order to georeference our model. In order to model the +motion of the slab, we include a fault on the top of the slab at the +interface between the mantle, crust, and wedge, as well as a fault +between the bottom of the slab and the mantle. + +\begin{figure}[htbp] + \includegraphics[width=4.5in]{examples/figs/subduction3d_conceptualmodel} + \caption{Conceptual model based on the Cascadia Subduction Zone. The + model includes the subduction slab (white), the mantle (green), + continental crust (blue), and an acrretionary wedge (red).} + \label{fig:example:subduction:3d:concept} +\end{figure} -% Use ParaView Python scripts +The files associated with this suite of examples are contained in the +directory \filename{examples/3d/subduction}. This directory contains +several subdirectories: +\begin{description} +\item[\filename{mesh}] Files used to construct the finite-element mesh using + CUBIT/Trelis. +\item[\filename{spatialdb}] Files associated with the spatial + and temporal databases. +\item[\filename{viz}] ParaView + Python scripts and other files for visualizing results. +\item[\filename{output}] Directory containing simulation + output. It is created automatically when running the + simulations. +\end{description} -% Organization of files (mesh, spatialdb, viz). \subsection{Features Illustrated} -\subsection{Mesh Description} - -% mesh directory CUBIT/Trelis - -% Geometry +Table~\ref{tab:example:subduction:3d:features} lists the features +discussed in each of these 3-D subduction zone examples. With the +intent of illustrating features used in research simulations, we use +HDF5 output and, we make extensive use the most efficient +implementations of spatial databases (UniformDB and SimpleGridDB). We +also use ParaView Python scripts for visualizing the output. These +scripts can be run within the ParaView GUI or outside the ParaView +GUI, although the interaction is limited to rotating, translating, and +zooming when run outside the ParaView GUI. + +\begin{table}[htbp] + \caption{PyLith features covered in the suite of 3-D subduction zone examples.} + \label{tab:example:subduction:3d:features} + \input{examples/subduction3d_features} +\end{table} + +\subsection{Generating the Finite-Element Mesh} + +We use CUBIT/Trelis to generate the finite-element mesh. Due to its +size, we do not include the finite-element mesh in the PyLith source +or binary distributions. If you do not have CUBIT/Trelis, you can +download the mesh from +\url{https://wiki.geodynamics.org/software:pylith:examples:files} and +skip generating the mesh. + +We use contours of the Cascadia Subduction Zone from Slab v1.0 +\ref{Hayes:etal:2012} for the geometry of the top of the slab. In +order to make use of these contours from within CUBIT/Trelis, we use a +Python script (\filename{generate\_surfjou.py}) to read the contours +file and create a CUBIT/Trelis journal file +(\filename{generate\_surfs.jou}) that adds additional contours west of +the trench and then constructs the top and bottom surfaces of the +slab. The Python script also constructs a splay fault but copying a +contour to a depth below the slab and above the ground surface. + +\tip{We define the coordinate systems we use in the simulations in the + the Python script \filename{coordsys.py} to make it easier to + convert to/from various georeference coordinate systems in the pre- + and post-processing. PyLith will automatically convert among + compatible coordinate systems during the simulation.} -% Size of domain - -% Slab - create 3D (extend up-dip, offset to depth normal to surface) - -% Splay +\begin{shell} +# Make sure you are in the 'mesh' directory and then run the Python +# script to generate the journal file 'generate_surfs.jou'. +$$ ./generate_surfjou.py +\end{shell} -% tet (hex is alternative) +The next step is to use CUBIT/Trelis to run the +\filename{generate\_surfs.jou} journal file to generate the spline +surfaces for the slab and splay fault and save them as ACIS +surfaces. + +Currently we discretize the domain using a uniform, coarse resolution +of 25 km. This allows the simulations to run relatively quickly and +fit on a laptop. In a real research problem, we would tailor the +resolution to match the length scales we want to capture and use a +finer resolution. We provide journal files for both a mesh with +tetrahedral cells (\filename{mesh\_tet.jou}) and a mesh with +hexahedral cells (\filename{mesh\_tet.jou}). In the following +examples, we will focus exclusively on the mesh with tetrahedral cells +because the mesh with hexahedral cells contains cells that are +significantly distorted; this illustrates how it is often difficult to +generate high quality meshes with hexahedral cells for domains with +complex 3-D geometry. + +After you generate the ACIS surface files, run the +\filename{mesh\_tet.jou} journal file to construct the geometry, and +generate the mesh. In the end you will have an Exodus-II file +\filename{mesh\_tet.exo}, which is a NetCDF file, in the +\filename{mesh} directory. You can load this file into ParaView. + +\tip{We recommend carefully examining the \filename{geometry.jou} + journal file to understand how we assemble the 3-D slab and cut the + rectangular into pieces.} \subsection{Organization of Parameters} @@ -186,6 +291,44 @@ \subsubsection{Exercises} \subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} + %% In this problem we generate Green's functions that will be used + %% to invert synthetic data generated from step06. There are two + %% different sub-problems: + + %% step07a: Generate Green's functions corresponding to left-lateral + %% slip on the subduction interface (slab top). + %% step07b: Generate Green's functions corresponding to updip + %% slip on the subduction interface (slab top). + + %% Responses (Green's functions) are computed at simulated cGPS + %% locations defined in the file cgps_sites.txt. + %% Note that we change the default problem type from TimeDependent to + %% GreensFns. + + %% Prior to generating the Green's functions, we first generate synthetic + %% data from the output of problem step06, using the make_synthetic_gpsdisp.py + %% script, with parameters defined in make_synthetic_gpsdisp.cfg: + + %% ./make_synthetic_gpsdisp.py + + %% After generating the synthetic data and Green's functions, we then + %% perform a simple inversion using the slip_invert.py script, with + %% parameters defined in slip_invert.cfg: + + %% ./slip_invert.py + + %% This will generate two HDF files that may be viewed in Paraview: + %% step07-inversion-slip.h5: The predicted fault slip. + %% step07-inversion-displacement.h5: The predicted surface displacements. + + %% There is also an inversion summary file: step07-inversion-summary.txt + %% If you have matplotlib installed, you can view a log-log plot of + %% solution misfit by going into the viz directory and running: + + %% ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt + + + \subsubsection{Exercises} % Move slip to splay fault in step06 and redo inversion. diff --git a/doc/userguide/examples/subduction3d_features.tex b/doc/userguide/examples/subduction3d_features.tex new file mode 100644 index 0000000000..9e2c4a9ebf --- /dev/null +++ b/doc/userguide/examples/subduction3d_features.tex @@ -0,0 +1,164 @@ +\rowcolors{2}{yellow!30}{white} +\resizebox{\textwidth}{!}{% +\begin{tabular}{|l|%% Example + *{8}c|% General + *{3}c|% Solver + *{5}c|% Spatial Database +} +\hline +\rowcolor{blue!10} +Example +& \multicolumn{8}{c|}{General} +& \multicolumn{3}{c|}{Solver} +& \multicolumn{5}{c|}{Spatial Database} +\\ +%%%% +\hline +\rowcolor{blue!10} + +% General +& \rlabel{Dimension} +& \rlabel{Coordinate system} +& \rlabel{Mesh generator} +& \rlabel{Cells} +& \rlabel{Refinement} +& \rlabel{Reordering} +& \rlabel{Problem type} +& \rlabel{Time dependence} +% Solver +& \rlabel{Solver} +& \rlabel{Preconditioner} +& \rlabel{Time stepping} +% Spatial Database +& \rlabel{Uniform} +& \rlabel{Simple} +& \rlabel{Simple grid} +& \rlabel{Composite} +& \rlabel{Time history} +\\ +\hline +3d/subduction/step01 +& 3 & Proj & CUBIT & Tet & & \yes & TD & S +& L & ILU & +& x2 & x4 & & & +\\ \hline +3d/subduction/step02 +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& L & ML+CUST & BE +& x2 & x3 & x2 & x2 & +\\ \hline +3d/subduction/step03 +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& L & ML+CUST & BE +& x4 & x3 & x2 & x2 & +\\ \hline +3d/subduction/step04 +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& L & ML+CUST & BE +& x7 & x3 & x5 & x2 & +\\ \hline +3d/subduction/step05 +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& NL & ML+CUST & BE +& x7 & x3 & x5 & x2 & +\\ \hline +3d/subduction/step06 +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& NL & ML+CUST & BE +& x1 & x4 & x1 & & x1 +\\ \hline +\end{tabular}} +\par +{\bf Problem type} -- TD: time dependent, GF: Green's functions. {\bf Time dependence} -- S: static, QS: quasi-static, D: dynamic. {\bf Solver} -- L: linear, NL: nonlinear. {\bf Preconditioner} -- ILU: ILU, ASM: Additive Schwarz, SCHUR: Schur complement, CUST: custom, ML: ML algebraic multigrid, GAMG: geometric algebraic multigrid. {\bf Time stepping} -- BE: Backward Euler, FE: Forward Euler. \\ +\rowcolors{2}{yellow!30}{white} +\resizebox{\textwidth}{!}{% +\begin{tabular}{|l|%% Example + *{4}c|% Boundary Condition + *{8}c|% Fault + *{9}c|% Bulk Rheology + *{7}c|% Output +} +\hline +\rowcolor{blue!10} +Example +& \multicolumn{4}{c|}{Boundary Condition} +& \multicolumn{8}{c|}{Fault} +& \multicolumn{9}{c|}{Bulk Rheology} +& \multicolumn{7}{c|}{Output} +\\ +%%%% +\hline +\rowcolor{blue!10} + +% Boundary Condition +& \rlabel{Dirichlet} +& \rlabel{Neumann} +& \rlabel{Absorbing} +& \rlabel{Point force} +% Fault +& \rlabel{Prescribed slip} +& \rlabel{Slip time function} +& \rlabel{Constitutive model} +& \rlabel{Static friction} +& \rlabel{Slip-weakening friction} +& \rlabel{Time-weakening friction} +& \rlabel{Rate-state friction w/ageing} +& \rlabel{Traction perturbation} +% Bulk Rheology +& \rlabel{Linear elastic} +& \rlabel{Linear Maxwell viscoelastic} +& \rlabel{Generalized Maxwell viscoelastic} +& \rlabel{Powerlaw viscoelastic} +& \rlabel{Drucker-Prager elastoplastic} +& \rlabel{Stress/strain formulation} +& \rlabel{Inertia} +& \rlabel{Reference state} +& \rlabel{Gravity} +% Output +& \rlabel{Format} +& \rlabel{Domain output} +& \rlabel{Surface output} +& \rlabel{Point output} +& \rlabel{State variable output} +& \rlabel{ParaView} +& \rlabel{Matplotlib} +\\ +\hline +3d/subduction/step01 +& x5 & & & +& & & & & & & & & x4 & & & & & Inf & & & +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step02 +& x5 & & & +& x1 & STEP & & & & & & +& x2 & x2 & & & & Inf & & & +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step03 +& x5 & & & +& x2 & RATE & & & & & & +& x2 & x2 & & & & Inf & & & +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step04 +& x5 & & & +& x3 & STEP & & & & & & +& x2 & x2 & & & & Inf & & & +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step05 +& x5 & & & +& x1 & RATE & x1 & & \yes & & & \yes +& x2 & x2 & & & & Inf & & & +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step06 +& x5 & & & +& x1 & USER & & & & & & +& x4 & & & & & Inf & & & +& H5 & x1 & x1 & x1 & x4 & \yes & +\\ \hline +\end{tabular}} +\par +{\bf Stress/strain formulation} -- Inf: infinitesimal, Fin: small, finite strain. \\ diff --git a/doc/userguide/pylithdoc.cls b/doc/userguide/pylithdoc.cls index 66ac496329..b9e52b0901 100644 --- a/doc/userguide/pylithdoc.cls +++ b/doc/userguide/pylithdoc.cls @@ -31,6 +31,7 @@ \RequirePackage{listings} \RequirePackage{pifont} \RequirePackage{calc} +\RequirePackage[table]{xcolor} \RequirePackage{tikz} %\RequirePackage{url} diff --git a/doc/userguide/userguide.tex b/doc/userguide/userguide.tex index af2df5aec9..5ee27ca309 100644 --- a/doc/userguide/userguide.tex +++ b/doc/userguide/userguide.tex @@ -24,7 +24,12 @@ \usepackage{array} \usepackage{setspace} % remove -\renewcommand{\pylithVersionNumber}{2.2.0} +\usepackage{pifont} +\newcommand{\yes}{\ding{52}} +\newcommand{\rlabel}[1]{\rotatebox[origin=l]{90}{#1}} + + +\renewcommand{\pylithVersionNumber}{2.2.1} \renewcommand{\pylithDOI}{10.5281/zenodo.438705} % Update install/install.tex (version number within verbatim environment) @@ -189,6 +194,13 @@ \bibitem[Zienkiewicz and Taylor, 2000]{Zienkiewicz:Taylor:2000}Zienkiewicz, O.C. and R.L. Taylor (2000), \textit{The Finite Element Method, Fifth Edition, Volume 2: Solid Mechanics}, Butterworth-Heinemann, Oxford, -459 pp.125\end{thebibliography} +459 pp.125 + +\bibitem[Hayes et al., 2012]{Hayes:etal:2012}Hayes, G. P., D. J. Wald, + and R. L. Johnson (2012), Slab1.0: A three-dimensional model of + global subduction zone geometries, J. Geophys. Res., 117, B01302, + doi:10.1029/2011JB008524. + +\end{thebibliography} \end{document} From 3f0f5e8855e4023d2332af581f8237600d416ca4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 12:25:19 -0700 Subject: [PATCH 078/216] Added more comments to journal files. --- examples/3d/subduction/mesh/README | 6 --- .../3d/subduction/mesh/generate_surfjou.py | 7 ++- examples/3d/subduction/mesh/geometry.jou | 46 +++++++++++-------- 3 files changed, 32 insertions(+), 27 deletions(-) delete mode 100644 examples/3d/subduction/mesh/README diff --git a/examples/3d/subduction/mesh/README b/examples/3d/subduction/mesh/README deleted file mode 100644 index 09f121c1f2..0000000000 --- a/examples/3d/subduction/mesh/README +++ /dev/null @@ -1,6 +0,0 @@ -./generate_slabtop.py --slab-filename=cas_contours_dep.in.txt --journal-filename=slabtop_surf.jou --stride=10 - - - - -CUBIT> surface 16 Scheme TriMesh geometry approximation angle 90.0 \ No newline at end of file diff --git a/examples/3d/subduction/mesh/generate_surfjou.py b/examples/3d/subduction/mesh/generate_surfjou.py index fae7069721..48be3c69bd 100755 --- a/examples/3d/subduction/mesh/generate_surfjou.py +++ b/examples/3d/subduction/mesh/generate_surfjou.py @@ -22,8 +22,11 @@ # complexity of the slab geometry so that the mesh generation is # faster. # -# The Slab contours can be downloaded from: -# https://earthquake.usgs.gov/data/slab/models.php +# The Slab contours (cas_contours_dep.in.txt) can be downloaded from: +# https://earthquake.usgs.gov/data/slab/models.php. Note that we have +# gzipped the file to reduce its size in the Git repository and we +# uncompress it on the fly in this script using the gzip Python +# module. # # The reference for the Slab 1.0 model is: # diff --git a/examples/3d/subduction/mesh/geometry.jou b/examples/3d/subduction/mesh/geometry.jou index d4f9e236d2..a3efdaea52 100644 --- a/examples/3d/subduction/mesh/geometry.jou +++ b/examples/3d/subduction/mesh/geometry.jou @@ -14,16 +14,17 @@ # # ---------------------------------------------------------------------- # -# This file is called from the mesh file (mesh_tet.jou or mesh_hex.jou). +# This file is called from the mesh file (mesh_tet.jou or +# mesh_hex.jou). You can also run this file separately to examine how +# the geometry is constructed. # -# CUBIT/Trelis journal file with geometry for example showing how to import -# several surfaces (topography, subduction interface, splay fault), and -# mesh the resulting volumes. -# -# We also use the CUBIT/Trelis support for APREPRO (the expressions in +# We use the CUBIT/Trelis support for APREPRO (the expressions in # braces), which includes units and mathematical functions. See the -# APREPRO section in the appendix of the CUBIT/Trelis documentation for more -# information. +# APREPRO section in the appendix of the CUBIT/Trelis documentation +# for more information. +# +# We use the Id() APPREPRO function to get the id of various objects +# and rename them for future reference. # # ---------------------------------------------------------------------- # Set units to SI. @@ -38,6 +39,7 @@ reset # ---------------------------------------------------------------------- # Import slab surfaces and construct slab. # ---------------------------------------------------------------------- +# We name the surface, volume, and body for future reference. import Acis "surf_slabtop.sat" ${idSurf=Id("surface")} surface {idSurf} name "s_slabtop" @@ -61,7 +63,7 @@ volume {idVol} name "v_slab" delete body b_slabbot # ---------------------------------------------------------------------- -# Create block +# Create block for domain. # ---------------------------------------------------------------------- # Block is 800 km x 800 km x 400 km ${blockLength=800.0*km} @@ -72,7 +74,8 @@ brick x {blockLength} y {blockWidth} z {blockHeight} ${idVol=Id("volume")} volume {idVol} name "v_domain" -# Translate block so top is a z=0. +# Translate block so the top is at z=0 and the domain is roughly +# centered on the subduction zone. ${moveX=-60.0*km} ${moveY=0.0*km} volume v_domain move x {moveX} y {moveY} z {-0.5*blockHeight} @@ -83,7 +86,7 @@ volume v_domain move x {moveX} y {moveY} z {-0.5*blockHeight} chop volume v_domain with volume v_slab # ---------------------------------------------------------------------- -# Create planar surface for continental crust/mantle boundary. +# Create planar horizontal surface for continental crust/mantle boundary. # ---------------------------------------------------------------------- create planar surface with plane zplane offset {-40.0*km} ${idSurf=Id("surface")} @@ -93,7 +96,7 @@ webcut volume v_domain@A with plane surface s_moho delete surface s_moho # ---------------------------------------------------------------------- -# Import splay surface and cut volume. +# Import splay fault surface and cut the crust volume. # ---------------------------------------------------------------------- import Acis "surf_splay.sat" ${idSurf=Id("surface")} @@ -108,14 +111,24 @@ webcut volume v_domain@A with sheet surface s_splay # ---------------------------------------------------------------------- # Create fault patch # ---------------------------------------------------------------------- -# Create block to create rupture patch. +# In order to make it easier to specify slip on a subset 200 km +# along-strike section of the subduction interface, we inscribe curves +# on the sheet body corresponding to the subducting slab. This allows +# us to imprint this patch on the domain volumes, resulting in +# splitting the subduction interface into multiple pieces. + +# Create block with horizontal dimensions matching the desired rupture +# patch. The x and z dimensions are set to exceed the dimensions of +# the subducting interface so that the fault patch reaches the trench +# and extends to the bottom of the crust. ${patchLength=200.0*km} brick x {400.0*km} y {patchLength} z {100.0*km} ${idVol=Id("volume")} volume {idVol} name "v_patchblock" move volume v_patchblock x {-100*km} y 0 z 0 -# Scribe rupture patch onto surface geometry (volumes of sheet bodies). +# Enscribe the rupture patch onto the geometry of the subducting slab +# surface (volumes of sheet bodies). chop volume v_slabtop with volume v_patchblock keep chop volume v_splay with volume v_patchblock @@ -135,8 +148,3 @@ imprint all with volume all merge all # End of file - - - - - From fc1602b8d6e1ee173489662b0ced1c3749db8a86 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 12:28:10 -0700 Subject: [PATCH 079/216] Added more comments to bc.jou --- examples/3d/subduction/mesh/bc.jou | 4 ++++ 1 file changed, 4 insertions(+) diff --git a/examples/3d/subduction/mesh/bc.jou b/examples/3d/subduction/mesh/bc.jou index 6a5ac80169..b701ffcd56 100644 --- a/examples/3d/subduction/mesh/bc.jou +++ b/examples/3d/subduction/mesh/bc.jou @@ -23,6 +23,10 @@ # ---------------------------------------------------------------------- # Create blocks for materials # ---------------------------------------------------------------------- +# We create a block for each material in the PyLith simulations. In +# the PyLith parameters, we will set the material 'id' to the block +# 'id' here to indcate which cells correspond to a given material. + block 1 volume v_domain block 1 name "slab" From 0d8fc103ac0f0401275330a27d7cac25d123f939 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 12:33:37 -0700 Subject: [PATCH 080/216] Added note about naming conventions. --- doc/userguide/examples/subduction3d.tex | 15 +++++++++++++++ 1 file changed, 15 insertions(+) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index a7f75ac78f..67ccd5bb39 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -117,6 +117,19 @@ \subsection{Generating the Finite-Element Mesh} surfaces for the slab and splay fault and save them as ACIS surfaces. +\important{The CUBIT/Trelis journal files name objects and then later + reference them by name. When objects are cut, a suffix of + \object{@LETTER} is appended to the original name (for example, + \object{domain} becomes \object{domain} and + \object{domain@A}). However, which one retains the original name and + which ones gets the suffix is ambiguous. In general, the names are + consistent across versions of CUBIT/Trelis with the same version of + the underlying ACIS library. {\bf As a result, you may need to + update the ids in the references to previously named objects that + have been split (for example \object{domain@A} may need to be changed to + \object{domain@B}, etc) in order to account for differences in how + your version of CUBIT/Trelis has named split objects.}} + Currently we discretize the domain using a uniform, coarse resolution of 25 km. This allows the simulations to run relatively quickly and fit on a laptop. In a real research problem, we would tailor the @@ -142,6 +155,8 @@ \subsection{Generating the Finite-Element Mesh} \subsection{Organization of Parameters} + + % pylithapp % + mesh % + materials From efc452c19530bc77c88c7eb5a2f10ea768e34493 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 14:25:27 -0700 Subject: [PATCH 081/216] Fix typo. --- examples/3d/subduction/viz/plot_dispvec.py | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 5868c05310..64740b1d84 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -48,7 +48,7 @@ def visualize(sim, dispScale): filename = "output/%s-domain.xmf" % sim if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) - dataDomain = XDMFReader(FileNames=[sim]) + dataDomain = XDMFReader(FileNames=[filename]) RenameSource("%s-domain" % sim, dataDomain) scene = GetAnimationScene() From c79836ae85576dc90613a796582d5dcfc2364a94 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 10:01:30 +1200 Subject: [PATCH 082/216] Changed rake angle and time period for slow slip example. --- examples/3d/subduction/slip_invert.cfg | 2 +- examples/3d/subduction/spatialdb/generate_slowslip.cfg | 10 ++++++---- examples/3d/subduction/step06.cfg | 4 ++-- 3 files changed, 9 insertions(+), 7 deletions(-) diff --git a/examples/3d/subduction/slip_invert.cfg b/examples/3d/subduction/slip_invert.cfg index 26bc8fa800..e1bf24ce99 100644 --- a/examples/3d/subduction/slip_invert.cfg +++ b/examples/3d/subduction/slip_invert.cfg @@ -1,6 +1,6 @@ [slip_invert] data_file = cgps_synthetic_displacement.txt -rake = 45.0*degree +rake = 110.0*degree gfimpulses_ll_file = output/step07a-fault-slab.h5 gfimpulses_ud_file = output/step07b-fault-slab.h5 gfresponses_ll_file = output/step07a-cgps_sites.h5 diff --git a/examples/3d/subduction/spatialdb/generate_slowslip.cfg b/examples/3d/subduction/spatialdb/generate_slowslip.cfg index 6c3539da1d..e39173a890 100644 --- a/examples/3d/subduction/spatialdb/generate_slowslip.cfg +++ b/examples/3d/subduction/spatialdb/generate_slowslip.cfg @@ -1,20 +1,22 @@ [generate_slowslip] -rake = 45.0 +rake = 110.0 slip_center = [-124.0, 45.5] slip_radius = 0.7 slip_max = 8.0 slip_sigma_lon = 0.3 slip_sigma_lat = 0.3 -slip_times = [0.0, 0.2, 0.4, 0.6, 0.8, 1.0, 1.2] -slip_amplitudes = [0.0, 0.2, 0.5, 0.8, 0.9, 1.0, 1.0] - grid_lon_range = [-126.2, -123.0] grid_lat_range = [44.4, 46.4] grid_incr = 0.04 time_db_filename = fault_slabtop_slowslip.timedb +slip_times = [0.0, 6.0, 12.0, 18.0, 24.0, 30.0, 36.0] +slip_amplitudes = [0.0, 0.2, 0.5, 0.8, 0.9, 1.0, 1.0] + +slip_time_units = day + coordsys = spatialdata.geocoords.CSGeo iohandler = spatialdata.spatialdb.SimpleGridAscii diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 46c776567f..06265738c4 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -73,8 +73,8 @@ problem.progress_monitor.filename = output/step06-progress.txt # ---------------------------------------------------------------------- [pylithapp.problem.formulation.time_step] # Define the total time for the simulation and the time step size. -total_time = 1.0*year -dt = 0.1*year +total_time = 30.0*day +dt = 2.0*day # ---------------------------------------------------------------------- # output From d0750aeab43f366c0b5293a7f3d56ae9369e4c12 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 10:35:17 +1200 Subject: [PATCH 083/216] Changes for different rake angle and number of time steps. --- examples/3d/subduction/make_synthetic_gpsdisp.cfg | 2 +- examples/3d/subduction/slip_invert.cfg | 6 +++--- 2 files changed, 4 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.cfg b/examples/3d/subduction/make_synthetic_gpsdisp.cfg index 288bf50bbd..65dc3fbf11 100644 --- a/examples/3d/subduction/make_synthetic_gpsdisp.cfg +++ b/examples/3d/subduction/make_synthetic_gpsdisp.cfg @@ -1,6 +1,6 @@ [make_synthetic_gpsdisp] point_input_file = output/step06-cgps_sites.h5 -time_step = 11 +time_step = 15 sigma_east = 0.0005 sigma_north = 0.0005 sigma_up = 0.001 diff --git a/examples/3d/subduction/slip_invert.cfg b/examples/3d/subduction/slip_invert.cfg index e1bf24ce99..f7668fe7c9 100644 --- a/examples/3d/subduction/slip_invert.cfg +++ b/examples/3d/subduction/slip_invert.cfg @@ -8,6 +8,6 @@ gfresponses_ud_file = output/step07b-cgps_sites.h5 a_priori_value = 0.0 penalty_weight_vals = [0.1,0.2,0.5,1.0,2.0,5.0,10.0,20.0,50.0,100.0] data_scale = 1.0 -result_summary_file = step07-inversion-summary.txt -slip_output_file = step07-inversion-slip.h5 -displacement_output_file = step07-inversion-displacement.h5 +result_summary_file = output/step07-inversion-summary.txt +slip_output_file = output/step07-inversion-slip.h5 +displacement_output_file = output/step07-inversion-displacement.h5 From 68c05aaf53b222522e04b430e5384cc1fe790b77 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 11:06:02 +1200 Subject: [PATCH 084/216] Added more comments in script and in .cfg file. --- examples/3d/subduction/make_synthetic_gpsdisp.cfg | 12 ++++++++++++ examples/3d/subduction/make_synthetic_gpsdisp.py | 5 +++++ 2 files changed, 17 insertions(+) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.cfg b/examples/3d/subduction/make_synthetic_gpsdisp.cfg index 65dc3fbf11..ad2c188237 100644 --- a/examples/3d/subduction/make_synthetic_gpsdisp.cfg +++ b/examples/3d/subduction/make_synthetic_gpsdisp.cfg @@ -1,8 +1,20 @@ [make_synthetic_gpsdisp] +# This file defines the parameters used in generating synthetic data for +# the inversion in example step07. It reads the output from example step06, +# adds noise to the displacements, and then outputs the results to a text +# file and a VTK file (for visualization). + +# Output file from step06. point_input_file = output/step06-cgps_sites.h5 + +# We select the last time step for this problem. time_step = 15 + +# We assume data uncertainties of 0.5 mm horizontal and 1 mm vertical. sigma_east = 0.0005 sigma_north = 0.0005 sigma_up = 0.001 + +# Synthetic data files. output_file = cgps_synthetic_displacement.txt vtk_output_file = cgps_synthetic_displacement.vtk diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index 596c477e59..fc07e205e3 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -17,6 +17,11 @@ # ---------------------------------------------------------------------- # # Python application to create synthetic data from PyLith points output. +# This script is meant to be used with example step07. It reads the +# slow slip displacements at synthetic cGPS stations from example +# step06, adds noise to the displacements, and then generates text and +# VTK files with the synthetic data. The parameters are defined in +# the make_synthetic_gpsdisp.cfg file. import math import numpy From ba103447ecbcd83ca57faf0c9063c58f188cd9eb Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 11:18:47 +1200 Subject: [PATCH 085/216] Added more comments. --- .../3d/subduction/make_synthetic_gpsdisp.py | 3 +++ examples/3d/subduction/slip_invert.cfg | 24 ++++++++++++++++++- examples/3d/subduction/slip_invert.py | 10 ++++++++ 3 files changed, 36 insertions(+), 1 deletion(-) diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index fc07e205e3..15e5002584 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -22,6 +22,9 @@ # step06, adds noise to the displacements, and then generates text and # VTK files with the synthetic data. The parameters are defined in # the make_synthetic_gpsdisp.cfg file. +# Run this script as follows: +# ./make_synthetic_gpsdisp.py +# import math import numpy diff --git a/examples/3d/subduction/slip_invert.cfg b/examples/3d/subduction/slip_invert.cfg index f7668fe7c9..fddae83475 100644 --- a/examples/3d/subduction/slip_invert.cfg +++ b/examples/3d/subduction/slip_invert.cfg @@ -1,13 +1,35 @@ [slip_invert] +# This .cfg file defines the parameters controlling the inversion in +# example step07. This performs a set of linear inversions with the given +# set of penalty parameters. Inversion solutions and predicted displacements +# are output to HDF5 files, and an inversion summary is saved to a text +# file. + +# This file contains the synthetic geodetic observations. data_file = cgps_synthetic_displacement.txt + +# If we wanted to scale the data and uncertainties in the above file, we +# would change this value. +data_scale = 1.0 + +# We assume that we know the rake angle and that it is constant. rake = 110.0*degree + +# These are the Green's function files generated by examples step07a and +# step07b. gfimpulses_ll_file = output/step07a-fault-slab.h5 gfimpulses_ud_file = output/step07b-fault-slab.h5 gfresponses_ll_file = output/step07a-cgps_sites.h5 gfresponses_ud_file = output/step07b-cgps_sites.h5 + +# Regularization is minimum moment, where we assume an a priori value of +# zero for the fault slip. a_priori_value = 0.0 + +# This is a list of weights assigned to the regularization. penalty_weight_vals = [0.1,0.2,0.5,1.0,2.0,5.0,10.0,20.0,50.0,100.0] -data_scale = 1.0 + +# Output file names. result_summary_file = output/step07-inversion-summary.txt slip_output_file = output/step07-inversion-slip.h5 displacement_output_file = output/step07-inversion-displacement.h5 diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index aff72d0d2b..b71dacce17 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -19,6 +19,16 @@ # Simple inversion script that uses PyLith-generated Green's functions. # NOTE: This script assumes that you have PETSc installed, and that you # have PETSC_DIR set as an environmental variable. +# This script is used as part of example step07. To perform the inversion you +# must have already: +# 1. Run example step06. +# 2. Run the make_synthetic_gpsdisp.py script to generate synthetic data. +# 3. Generated the step07 Green's functions (step07a and step07b). +# +# Once you have performed the steps above, you can run this script. The +# parameters are defined in slip_invert.cfg. +# Run this script as follows: +# ./slip_invert.py # import math From 179ebff36750be0853b00c24d3db94e8658b2ce1 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 11:25:49 +1200 Subject: [PATCH 086/216] Moved file to spatialdb, changed import, and added some comments. --- .../{ => spatialdb}/generate_initial_stress.py | 11 ++++++++--- 1 file changed, 8 insertions(+), 3 deletions(-) rename examples/3d/subduction/{ => spatialdb}/generate_initial_stress.py (84%) diff --git a/examples/3d/subduction/generate_initial_stress.py b/examples/3d/subduction/spatialdb/generate_initial_stress.py similarity index 84% rename from examples/3d/subduction/generate_initial_stress.py rename to examples/3d/subduction/spatialdb/generate_initial_stress.py index 284f04c21e..d0483ba681 100755 --- a/examples/3d/subduction/generate_initial_stress.py +++ b/examples/3d/subduction/spatialdb/generate_initial_stress.py @@ -2,6 +2,9 @@ """ This script creates a spatial database for the initial stress using results from a previous PyLith run. +It is used in step08 to read stresses from example step08a, and then create a +spatial database of initial stresses that is used by examples step08b and +step08c. """ dbPrefix = "initial_stress" @@ -10,11 +13,13 @@ import numpy import h5py +import sys +sys.path.append('../mesh') # import pdb # pdb.set_trace() from spatialdata.spatialdb.SimpleIOAscii import SimpleIOAscii -from mesh.coordsys import cs_mesh +from coordsys import cs_mesh cs = cs_mesh() def getCellCenters(vertices, cells): @@ -29,8 +34,8 @@ def getCellCenters(vertices, cells): for material in materials: - filenameH5 = "output/%s-%s.h5" % (matPrefix, material) - filenameDB = "spatialdb/%s-%s.spatialdb" % (dbPrefix, material) + filenameH5 = "../output/%s-%s.h5" % (matPrefix, material) + filenameDB = "%s-%s.spatialdb" % (dbPrefix, material) # Open HDF5 file and get coordinates, cells, and stress. h5 = h5py.File(filenameH5, "r") From 4c76a2973b5dd4b4dee792a93e9583e4b6846256 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:10:53 -0700 Subject: [PATCH 087/216] Clean up spatial database stuff for Step07 and Step08. --- .../spatialdb/generate_initial_stress.py | 143 ++++++++++-------- .../spatialdb/impulse_amplitude.spatialdb | 34 ----- .../initial_stress-homogeneous.spatialdb | 47 ------ .../mat_initial_stress_grav.spatialdb | 42 +++++ examples/3d/subduction/step07a.cfg | 21 +-- examples/3d/subduction/step07b.cfg | 26 ++-- examples/3d/subduction/step08a.cfg | 49 +++--- examples/3d/subduction/step08b.cfg | 50 +++--- examples/3d/subduction/step08c.cfg | 55 +++++-- 9 files changed, 251 insertions(+), 216 deletions(-) delete mode 100644 examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb delete mode 100644 examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb create mode 100644 examples/3d/subduction/spatialdb/mat_initial_stress_grav.spatialdb diff --git a/examples/3d/subduction/spatialdb/generate_initial_stress.py b/examples/3d/subduction/spatialdb/generate_initial_stress.py index d0483ba681..1b96b3fdab 100755 --- a/examples/3d/subduction/spatialdb/generate_initial_stress.py +++ b/examples/3d/subduction/spatialdb/generate_initial_stress.py @@ -1,83 +1,104 @@ #!/usr/bin/env nemesis -""" -This script creates a spatial database for the initial stress using results -from a previous PyLith run. -It is used in step08 to read stresses from example step08a, and then create a -spatial database of initial stresses that is used by examples step08b and -step08c. -""" - -dbPrefix = "initial_stress" -matPrefix = "step08a" -materials = ["crust","mantle","slab","wedge"] +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# This script creates a spatial database with initial stresses for +# Step08b and Step08c using the PyLith output from Step08a. + import numpy import h5py import sys sys.path.append('../mesh') -# import pdb -# pdb.set_trace() from spatialdata.spatialdb.SimpleIOAscii import SimpleIOAscii from coordsys import cs_mesh cs = cs_mesh() def getCellCenters(vertices, cells): - """ - Function to compute cell centers. - """ - cellCoords = vertices[cells, :] - cellCenters = numpy.mean(cellCoords, axis=1) + """ + Function to compute cell centers. + """ + cellCoords = vertices[cells, :] + cellCenters = numpy.mean(cellCoords, axis=1) + return cellCenters - return cellCenters +def generate(sim, fileRoot, materials): + for material in materials: -for material in materials: + filenameH5 = "../output/%s-%s.h5" % (sim, material) + filenameDB = "%s-%s.spatialdb" % (fileRoot, material) - filenameH5 = "../output/%s-%s.h5" % (matPrefix, material) - filenameDB = "%s-%s.spatialdb" % (dbPrefix, material) + # Open HDF5 file and get coordinates, cells, and stress. + h5 = h5py.File(filenameH5, "r") + vertices = h5['geometry/vertices'][:] + cells = numpy.array(h5['topology/cells'][:], dtype=numpy.int) - # Open HDF5 file and get coordinates, cells, and stress. - h5 = h5py.File(filenameH5, "r") - vertices = h5['geometry/vertices'][:] - cells = numpy.array(h5['topology/cells'][:], dtype=numpy.int) - stress = h5['cell_fields/stress'][0,:,:] - h5.close() - - # Compute coordinates of quadrature points. - quadCoords = getCellCenters(vertices, cells) - - ncells = cells.shape[0] - nvalues = stress.shape[1] + # Get stresses from final time step. + stress = h5['cell_fields/stress'][-1,:,:] + h5.close() - # Create writer for spatial database file - writer = SimpleIOAscii() - writer.inventory.filename = filenameDB - writer._configure() + # Compute coordinates of quadrature points. + quadCoords = getCellCenters(vertices, cells) + + # Create writer for spatial database file + writer = SimpleIOAscii() + writer.inventory.filename = filenameDB + writer._configure() - values = [{'name': "stress-xx", - 'units': "Pa", - 'data': stress[:,0]}, - {'name': "stress-yy", - 'units': "Pa", - 'data': stress[:,1]}, - {'name': "stress-zz", - 'units': "Pa", - 'data': stress[:,2]}, - {'name': "stress-xy", - 'units': "Pa", - 'data': stress[:,3]}, - {'name': "stress-yz", - 'units': "Pa", - 'data': stress[:,4]}, - {'name': "stress-xz", - 'units': "Pa", - 'data': stress[:,5]}, - ] + values = [{'name': "stress-xx", + 'units': "Pa", + 'data': stress[:,0]}, + {'name': "stress-yy", + 'units': "Pa", + 'data': stress[:,1]}, + {'name': "stress-zz", + 'units': "Pa", + 'data': stress[:,2]}, + {'name': "stress-xy", + 'units': "Pa", + 'data': stress[:,3]}, + {'name': "stress-yz", + 'units': "Pa", + 'data': stress[:,4]}, + {'name': "stress-xz", + 'units': "Pa", + 'data': stress[:,5]}, + ] - writer.write({'points': quadCoords, - 'coordsys': cs, - 'data_dim': 3, - 'values': values}) + writer.write({'points': quadCoords, + 'coordsys': cs, + 'data_dim': 3, + 'values': values}) + + return + + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim", default="step08a") + parser.add_argument("--file-root", action="store", dest="fileRoot", default="mat_initial_stress_grav") + parser.add_argument("--materials", action="store", dest="materials", default="crust,mantle,slab,wedge") + args = parser.parse_args() + + materials = args.materials.split(",") + generate(args.sim, args.fileRoot, materials) + # End of file diff --git a/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb b/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb deleted file mode 100644 index e1b7343795..0000000000 --- a/examples/3d/subduction/spatialdb/impulse_amplitude.spatialdb +++ /dev/null @@ -1,34 +0,0 @@ -// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) -// -// This spatial database specifies the impulse amplitudes for -// generating Green's functions. They are all set to 1. -// -#SPATIAL.ascii 1 -SimpleDB { - num-values = 1 // number of material property values - value-names = slip - value-units = m - num-locs = 1 - data-dim = 0 - space-dim = 3 - cs-data = geo-projected { - to-meters = 1 - ellipsoid = WGS84 - datum-horiz = WGS84 - datum-vert = mean sea level - origin-lon = 0 - origin-lat = 0 - rotation-angle = 0 - projector = projector { - projection = tmerc - units = m - proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 - } - } -} -// Columns are -// (1) x coordinate (m) -// (2) y coordinate (m) -// (3) z coordinate (m) -// (4) slip (m) -0.0 0.0 0.0 1.0 diff --git a/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb b/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb deleted file mode 100644 index 442d0b9ed8..0000000000 --- a/examples/3d/subduction/spatialdb/initial_stress-homogeneous.spatialdb +++ /dev/null @@ -1,47 +0,0 @@ -// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) -// -// This spatial database specifies the initial stresses for the model -// The stresses increase linearly with depth assuming densities -// corresponding to mantle material. -// -#SPATIAL.ascii 1 -SimpleDB { - num-values = 6 // number of stress components - - // names of the stress components - value-names = stress-xx stress-yy stress-zz stress-xy stress-yz stress-xz - - value-units = Pa Pa Pa Pa Pa Pa // units - - num-locs = 2 // number of locations: 1 value each at the upper and lower - // surfaces. Linear interpolation should be used. - - data-dim = 1 - space-dim = 3 - cs-data = geo-projected { - to-meters = 1 - ellipsoid = WGS84 - datum-horiz = WGS84 - datum-vert = mean sea level - origin-lon = 0 - origin-lat = 0 - rotation-angle = 0 - projector = projector { - projection = tmerc - units = m - proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 - } - } -} -// Columns are -// (1) x coordinate (m) -// (2) y coordinate (m) -// (3) z coordinate (m) -// (4) stress-xx (Pa) -// (5) stress-yy (Pa) -// (6) stress-zz (Pa) -// (7) stress-xy (Pa) -// (8) stress-yz (Pa) -// (9) stress-xz (Pa) -0.0 0.0 -4000000.0 -12944778000.0 -12944778000.0 -12944778000.0 0.0 0.0 0.0 -0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 diff --git a/examples/3d/subduction/spatialdb/mat_initial_stress_grav.spatialdb b/examples/3d/subduction/spatialdb/mat_initial_stress_grav.spatialdb new file mode 100644 index 0000000000..d539ff3e34 --- /dev/null +++ b/examples/3d/subduction/spatialdb/mat_initial_stress_grav.spatialdb @@ -0,0 +1,42 @@ +// -*- C++ -*- (tell Emacs to use C++ mode for syntax highlighting) +// +// This spatial database specifies initial stresses that increase with +// depth corresponding to the overburden pressure for gravitational +// body forces acting on a material with a uniform density of 3300 +// kg/m**3 (mantle). +// +#SPATIAL.ascii 1 +SimpleDB { + num-values = 6 // number of stress components + value-names = stress-xx stress-yy stress-zz stress-xy stress-yz stress-xz + value-units = GPa GPa GPa GPa GPa GPa // units + num-locs = 2 // z=0 and z=-400*km + data-dim = 1 // points on a (vertical) line + space-dim = 3 + cs-data = geo-projected { + to-meters = 1.0e+3 // Specify coordinates in km for convenience. + ellipsoid = WGS84 + datum-horiz = WGS84 + datum-vert = mean sea level + origin-lon = 0 + origin-lat = 0 + rotation-angle = 0 + projector = projector { + projection = tmerc + units = m + proj-options = +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 + } + } +} +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) stress-xx (GPa) +// (5) stress-yy (GPa) +// (6) stress-zz (GPa) +// (7) stress-xy (GPa) +// (8) stress-yz (GPa) +// (9) stress-xz (GPa) +0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 +0.0 0.0 -400.0 -12.944778 -12.944778 -12.944778 0.0 0.0 0.0 diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index cdc73142b2..8edb026eee 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -20,10 +20,10 @@ # invert synthetic data generated from step06. There are two # different sub-problems: # -# step07a: Generate Green's functions corresponding to left-lateral -# slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to reverse -# slip on the subduction interface (slab top). +# Step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# Step07b: Generate Green's functions corresponding to reverse +# slip on the subduction interface (slab top). # # Materials # All four blocks use the linear, isotropic elastic material model @@ -87,13 +87,14 @@ edge = fault_slabtop_patch_edge quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 2 -# Label and query type for fault slip. -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.query_type = nearest - -# Spatialdb for impulses. +# Impulses for left-lateral slip. impulse_dof = [0] -db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb + +# Spatial database for slip impulse amplitude. +db_impulse_amplitude = spatialdata.spatialdb.UniformDB +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.values = [slip] +db_impulse_amplitude.data = [1.0] # ---------------------------------------------------------------------- # output diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index a4e3febd9e..988e87f198 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -20,13 +20,14 @@ # invert synthetic data generated from step06. There are two # different sub-problems: # -# step07a: Generate Green's functions corresponding to left-lateral -# slip on the subduction interface (slab top). -# step07b: Generate Green's functions corresponding to reverse -# slip on the subduction interface (slab top). +# Step07a: Generate Green's functions corresponding to left-lateral +# slip on the subduction interface (slab top). +# Step07b: Generate Green's functions corresponding to reverse +# slip on the subduction interface (slab top). # # Materials -# All four blocks use the linear, isotropic elastic material model (mat_elastic.cfg). +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). # # Boundary Conditions # Roller boundary conditions (pylithapp.cfg). @@ -55,7 +56,7 @@ # simulations, so we put them in a separate file. # # TO RUN THE SIMULATION: -# pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg +# pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg # # Output will be directed to the "output" directory.. @@ -86,13 +87,14 @@ edge = fault_slabtop_patch_edge quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 2 -# Label and query type for fault slip. -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.query_type = nearest - -# Spatialdb for impulses. +# Impulses for reverse slip. impulse_dof = [1] -db_impulse_amplitude.iohandler.filename = spatialdb/impulse_amplitude.spatialdb + +# Spatial database for slip impulse amplitude. +db_impulse_amplitude = spatialdata.spatialdb.UniformDB +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.values = [slip] +db_impulse_amplitude.data = [1.0] # ---------------------------------------------------------------------- # output diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg index a020b74fb2..550a2e93e6 100644 --- a/examples/3d/subduction/step08a.cfg +++ b/examples/3d/subduction/step08a.cfg @@ -16,13 +16,27 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions and gravity. The gravitational -# stresses are computed using the properties in mat_elastic.cfg, but -# we balance them using initial stresses consistent with uniform -# properties corresponding to the mantle. This means that the stresses -# will not balance and we should see deformation as a result of the -# out-of-balance stresses. +# We compute an estimate of the overburden stresses due to +# gravitational body forces and 3-D density variations assuming purely +# linearly, isotropic elastic materials. We minimize the deformation +# by using initial stresses equal to the overburden with uniform +# properties corresponding to the mantle. +# +# Step08a: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses for a uniform density. +# Step08b: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses from Step08a (initial stresses +# satisfy equilibrium, so there is no deformation). +# Step08c: Gravitational body forces with 3-D density variations in elastic +# and viscoelastic materials and initial stresses from Step08a +# (does not reach a steady-state solution). +# +# Materials +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -37,8 +51,8 @@ # This problem does not include a fault, so we use the algebraic # multigrid settings in solver_algebraicmultigrid.cfg. # -# To run the simulation: -# pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +# TO RUN THE SIMULATION: +# pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg # # Output will be directed to the "output" directory. @@ -57,38 +71,35 @@ problem.progress_monitor.filename = output/step08a-progress.txt gravity_field = spatialdata.spatialdb.GravityField [pylithapp.problem.formulation.time_step] -# Define the total time for the simulation and the time step size. +# Define the total time for the simulation. total_time = 0.0*year -dt = 0.1*year # ---------------------------------------------------------------------- -# initial stresses +# materials # ---------------------------------------------------------------------- -# We must specify initial stresses for each material. -# We provide a filename for the spatial database that gives the stresses, -# and we change the query_type from the default 'nearest' to 'linear'. +# We specify initial stresses for each material via a SimpleDB and linear interpolation. [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the slab -db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav.spatialdb db_initial_stress.query_type = linear [pylithapp.problem.materials.wedge] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the wedge -db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav.spatialdb db_initial_stress.query_type = linear [pylithapp.problem.materials.mantle] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the mantle -db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav.spatialdb db_initial_stress.query_type = linear [pylithapp.problem.materials.crust] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the crust -db_initial_stress.iohandler.filename = spatialdb/initial_stress-homogeneous.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav.spatialdb db_initial_stress.query_type = linear # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg index 3e82d37e64..fff8fd9b3b 100644 --- a/examples/3d/subduction/step08b.cfg +++ b/examples/3d/subduction/step08b.cfg @@ -16,16 +16,27 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is an elastic quasistatic problem using Dirichlet -# (displacement) boundary conditions and gravity. The gravitational -# stresses are computed using the properties in mat_elastic.cfg. In -# this case, we balance them with initial stresses computed from -# step08a.cfg, so the stresses should balance and we should see no -# deformation. After running step08a, generate the initial stresses: +# We compute an estimate of the overburden stresses due to +# gravitational body forces and 3-D density variations assuming purely +# linearly, isotropic elastic materials. We use the output of the +# stresses from Step08a as the initial stresses; the initial stresses +# satisfy equilibrium so there is no deformation. # -# ./generate_initial_stress.py +# Step08a: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses for a uniform density. +# Step08b: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses from Step08a (initial stresses +# satisfy equilibrium, so there is no deformation). +# Step08c: Gravitational body forces with 3-D density variations in elastic +# and viscoelastic materials and initial stresses from Step08a +# (does not reach a steady-state solution). # -# This will generate the initial stress database needed for this simulation. +# Materials +# All four blocks use the linear, isotropic elastic material model +# (mat_elastic.cfg). +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -40,8 +51,14 @@ # This problem does not include a fault, so we use the algebraic # multigrid settings in solver_algebraicmultigrid.cfg. # -# To run the simulation: -# pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +# BEFORE RUNNING THE SIMULATION, run the Python script that generates +# the spatial database with the initial stresses corresponding to the +# output from Step08a. +# +# cd spatialdb && generate_initial_stress.py +# +# TO RUN THE SIMULATION: +# pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg # # Output will be directed to the "output" directory. @@ -65,31 +82,30 @@ total_time = 0.0*year dt = 0.1*year # ---------------------------------------------------------------------- -# initial stresses +# materials # ---------------------------------------------------------------------- -# We must specify initial stresses for each material. -# We provide a filename for the spatial database that gives the stresses. +# We specify initial stresses for each material via a SimpleDB. # Since there is a point in the database corresponding to each cell # center, we keep the default query_type of 'nearest'. [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the slab -db_initial_stress.iohandler.filename = spatialdb/initial_stress-slab.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-slab.spatialdb [pylithapp.problem.materials.wedge] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the wedge -db_initial_stress.iohandler.filename = spatialdb/initial_stress-wedge.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-wedge.spatialdb [pylithapp.problem.materials.mantle] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the mantle -db_initial_stress.iohandler.filename = spatialdb/initial_stress-mantle.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-mantle.spatialdb [pylithapp.problem.materials.crust] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the crust -db_initial_stress.iohandler.filename = spatialdb/initial_stress-crust.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-crust.spatialdb # ---------------------------------------------------------------------- # output diff --git a/examples/3d/subduction/step08c.cfg b/examples/3d/subduction/step08c.cfg index 3cf2a2d362..566866177b 100644 --- a/examples/3d/subduction/step08c.cfg +++ b/examples/3d/subduction/step08c.cfg @@ -16,13 +16,31 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This is a viscoelastic quasistatic problem using Dirichlet -# (displacement) boundary conditions, gravity, and finite strain. -# The gravitational stresses are computed using the properties in -# mat_elastic.cfg, and we balance them with initial stresses computed from -# step08a.cfg, just as we did for step08b. In this problem we use -# viscoelastic materials and the small strain formulation, such that the -# stresses are recomputed for the deformed configuration. +# This example demonstrates the difficulty in finding a steady-state +# solution for the stress state arising from gravitational body forces +# with lateral density variations and viscoelastic materials. Compared +# with Step08b, this is a time-dependent simulation using viscoelastic +# materials and the small strain formulation, in which the stresses +# are recomputed for the deformed configuration.. +# +# Step08a: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses for a uniform density. +# Step08b: Gravitational body forces with 3-D density variations in elastic +# materials and initial stresses from Step08a (initial stresses +# satisfy equilibrium, so there is no deformation). +# Step08c: Gravitational body forces with 3-D density variations in elastic +# and viscoelastic materials and initial stresses from Step08a +# (does not reach a steady-state solution). +# +# Materials +# The 'wedge' and 'crust' blocks use the the linear, isotropic +# elastic material model, whereas the 'slab' and 'mantle' use the +# linear Maxwell viscoelastic material model (mat_viscoelastic.cfg). +# +# We also use the small-strain elasticity formulation. +# +# Boundary Conditions +# Roller boundary conditions (pylithapp.cfg). # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -37,8 +55,14 @@ # This problem does not include a fault, so we use the algebraic # multigrid settings in solver_algebraicmultigrid.cfg. # -# To run the simulation: -# pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg +# BEFORE RUNNING THE SIMULATION, run the Python script that generates +# the spatial database with the initial stresses corresponding to the +# output from Step08a if you have not already done so. +# +# cd spatialdb && generate_initial_stress.py +# +# TO RUN THE SIMULATION: +# pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg # # Output will be directed to the "output" directory. @@ -66,31 +90,30 @@ total_time = 100.0*year dt = 10.0*year # ---------------------------------------------------------------------- -# initial stresses +# materials # ---------------------------------------------------------------------- -# We must specify initial stresses for each material. -# We provide a filename for the spatial database that gives the stresses. +# We specify initial stresses for each material via a SimpleDB. # Since there is a point in the database corresponding to each cell # center, we keep the default query_type of 'nearest'. [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the slab -db_initial_stress.iohandler.filename = spatialdb/initial_stress-slab.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-slab.spatialdb [pylithapp.problem.materials.wedge] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the wedge -db_initial_stress.iohandler.filename = spatialdb/initial_stress-wedge.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-wedge.spatialdb [pylithapp.problem.materials.mantle] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the mantle -db_initial_stress.iohandler.filename = spatialdb/initial_stress-mantle.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-mantle.spatialdb [pylithapp.problem.materials.crust] db_initial_stress = spatialdata.spatialdb.SimpleDB db_initial_stress.label = Initial stress in the crust -db_initial_stress.iohandler.filename = spatialdb/initial_stress-crust.spatialdb +db_initial_stress.iohandler.filename = spatialdb/mat_initial_stress_grav-crust.spatialdb # ---------------------------------------------------------------------- # output From ffc40e1e687beb947fec48620280e81e392c6dd0 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:11:23 -0700 Subject: [PATCH 088/216] Add more comments to spatial database description. --- examples/3d/subduction/mat_elastic.cfg | 5 +++++ 1 file changed, 5 insertions(+) diff --git a/examples/3d/subduction/mat_elastic.cfg b/examples/3d/subduction/mat_elastic.cfg index 20f530c861..9035e3082f 100644 --- a/examples/3d/subduction/mat_elastic.cfg +++ b/examples/3d/subduction/mat_elastic.cfg @@ -16,6 +16,11 @@ # # Parameters for using linear elastic material models for the 'slab', # 'wedge', 'mantle', and 'crust'. +# +# We use a SimpleDB with a single point for each material. We could +# have used a UniformDB, but this makes it easier to adjust the +# spatial database file should we want to add in a spatial variation +# to the material properties. [pylithapp.problem.materials] slab = pylith.materials.ElasticIsotropic3D From d8e7086d6f897178ccfaf7d4daf3c85eb0f8d680 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:11:39 -0700 Subject: [PATCH 089/216] Small tweak to comment. --- examples/3d/subduction/step01.cfg | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index 8884f78f2b..c12bdc0e14 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -55,7 +55,7 @@ problem.progress_monitor.filename = output/step01-progress.txt # problem # ---------------------------------------------------------------------- [pylithapp.problem.formulation.time_step] -# Define the total time for the simulation and the default time step size. +# Define the total time for the simulation. total_time = 0.0*year # ---------------------------------------------------------------------- From 6a019a1b0efeae167fb3ba6879b529d9d6a27088 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:13:15 -0700 Subject: [PATCH 090/216] Ignore more generated spatial databases. --- .gitignore | 1 + 1 file changed, 1 insertion(+) diff --git a/.gitignore b/.gitignore index c1ed835a57..d454cb13e1 100644 --- a/.gitignore +++ b/.gitignore @@ -36,3 +36,4 @@ examples/3d/subduction/mesh/*.exo examples/3d/subduction/mesh/*.sat examples/3d/subduction/spatialdb/fault_slabtop_slowslip.spatialdb examples/3d/subduction/spatialdb/fault_slabtop_slowslip.timedb +examples/3d/subduction/spatialdb/mat_initial_stress_grav-*.spatialdb From 49fd2b4b38c4a919d2f26eb13625748f318ef46c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:23:33 -0700 Subject: [PATCH 091/216] Clean up defaults for ParaView Python script. --- examples/3d/subduction/viz/plot_dispvec.py | 12 +++--------- examples/3d/subduction/viz/plot_dispwarp.py | 12 +++--------- examples/3d/subduction/viz/plot_faultdir.py | 16 +++------------- .../3d/subduction/viz/plot_faultslip-reltract.py | 11 ++--------- examples/3d/subduction/viz/plot_faultslip.py | 13 +++---------- examples/3d/subduction/viz/plot_matprops.py | 16 ++++------------ 6 files changed, 18 insertions(+), 62 deletions(-) mode change 100644 => 100755 examples/3d/subduction/viz/plot_faultslip-reltract.py diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 64740b1d84..131ec51bb4 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -89,17 +89,11 @@ def visualize(sim, dispScale): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") - parser.add_argument("--vector-scale", action="store", type=float, dest="scale") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--vector-scale", action="store", type=float, dest="scale", default=DISPLACEMENT_SCALE) args = parser.parse_args() - sim = args.sim - scale = args.scale - if sim is None: - sim = SIM_NAME - if scale is None: - scale = DISPLACEMENT_SCALE - visualize(sim, scale) + visualize(args.sim, args.scale) Interact() else: diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index 160bfb7b50..e14ce67cf6 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -83,17 +83,11 @@ def visualize(sim, exaggeration): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") - parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) args = parser.parse_args() - sim = args.sim - exaggeration = args.exaggeration - if sim is None: - sim = SIM_NAME - if exaggeration is None: - exaggeration = DISPLACEMENT_SCALE - visualize(sim, exaggeration) + visualize(args.sim, args.exaggeration) Interact() else: diff --git a/examples/3d/subduction/viz/plot_faultdir.py b/examples/3d/subduction/viz/plot_faultdir.py index b0e617119d..83adff3263 100755 --- a/examples/3d/subduction/viz/plot_faultdir.py +++ b/examples/3d/subduction/viz/plot_faultdir.py @@ -93,26 +93,16 @@ def visualize(sim, faults, direction): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--faults", action="store", dest="faults") - parser.add_argument("--direction", action="store", dest="direction") + parser.add_argument("--direction", action="store", dest="direction", default=FIELD) args = parser.parse_args() - sim = args.sim if args.faults: faults = args.faults.split(",") else: - faults = None - direction = args.directions - - if sim is None: - sim = SIM_NAME - if faults is None: faults = FAULTS - if direction is None: - direction = FIELD - - visualize(sim, faults, direction) + visualize(args.sim, faults, args.direction) Interact() else: diff --git a/examples/3d/subduction/viz/plot_faultslip-reltract.py b/examples/3d/subduction/viz/plot_faultslip-reltract.py old mode 100644 new mode 100755 index d1054213a0..8824df70da --- a/examples/3d/subduction/viz/plot_faultslip-reltract.py +++ b/examples/3d/subduction/viz/plot_faultslip-reltract.py @@ -113,22 +113,15 @@ def visualize(sim, faults): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--faults", action="store", dest="faults") args = parser.parse_args() - sim = args.sim if args.faults: faults = args.faults.split(",") else: - faults = None - - if sim is None: - sim = SIM_NAME - if faults is None: faults = FAULTS - - visualize(sim, faults) + visualize(args.sim, faults) Interact() else: diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py index 99d4fea610..2d82c32eb6 100755 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -28,7 +28,7 @@ # pvpython. # Root name for simulation. -SIM_NAME = "step07a" +SIM_NAME = "step06" # Names of faults for output files. FAULTS = ["fault-slab"] @@ -91,22 +91,15 @@ def visualize(sim, faults): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--faults", action="store", dest="faults") args = parser.parse_args() - sim = args.sim if args.faults: faults = args.faults.split(",") else: - faults = None - - if sim is None: - sim = SIM_NAME - if faults is None: faults = FAULTS - - visualize(sim, faults) + visualize(args.sim, faults) Interact() else: diff --git a/examples/3d/subduction/viz/plot_matprops.py b/examples/3d/subduction/viz/plot_matprops.py index 3e47a6cc0c..4a67580a39 100755 --- a/examples/3d/subduction/viz/plot_matprops.py +++ b/examples/3d/subduction/viz/plot_matprops.py @@ -76,25 +76,17 @@ def visualize(sim, field, materials): import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim") - parser.add_argument("--field", action="store", dest="field") + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--field", action="store", dest="field", default=INFO_FIELD) parser.add_argument("--materials", action="store", dest="materials") args = parser.parse_args() - sim = args.sim - field = args.field if args.materials: materials = args.materials.split(",") else: - materials = None - - if sim is None: - sim = SIM_NAME - if field is None: - field = INFO_FIELD - if materials is None: materials = MATERIALS - visualize(sim, field, materials) + + visualize(args.sim, args.field, materials) Interact() else: From e438c9697d12e187218c42544bd2067ec114089b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 20 Jun 2017 17:23:57 -0700 Subject: [PATCH 092/216] More work on adding example to manual. --- .../examples/figs/subduction3d_geometry.png | Bin 0 -> 31218 bytes doc/userguide/examples/subduction3d.tex | 120 +++++++++++------- 2 files 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z2BRiJp~83#J_>-K6z`ga0YD)g>BAmnQUocp@Yc4FUr|=fk@G?-2NsCZ1%K7WWWxOUys+%Z(QK+L`av(8 zmOzESwB7ucA~i&!F^cQ;?$Qyf=yZRW!&>zn)k5*K*2Q=FvGR+7|DI7`9({G#SzYC! z1x2X+GLG5g*nja5Pn%usIOTRU@ADT9HWR($g%rLQ?c1KiGDIvcY5#k0umj3vtXhE0 zdLB`j4sJn>1_1`mDY^U?3%6XaGILX4r?&y(;0^_JqTgnJL>saqCIY`4d1A=@INJ zp)&3}xN7=KDVQJ%dnEsU&`>&a@Mm)Um&Xgrh$`jymPZ4!wo@s(M>XG`6DZF}$9KXA z;_vDyrV`u0G7Pgsoas1%q>JfFHX(1jvxfyx+dm`b;Oz;=Gk+EC%{=Ux{I_10!>C&J z&_8(lPuE`8&)uIt_cnj-{jA=q<{wtgcKeX+mi@H6|AU<41Ym~bG}?@c%$tXs!)N}2 z_eu1%i%UPR?i(H5TN<4o9i3kiTvfJGRk3=Oo&D^hnQ8!#`EfU|vG3dD;pED>qP&=Q z+pY)tN>q?&Z~wm?$9Ma6lLf0uU)OFu`WLzL`>XSBUSeqG;h4vRy%YTm(DP3#>>3*! z0TPGXE4|we_qKoc?)<1eFl(ITTjJ-HrM linear solver with single time step -% Squeeze +\begin{figure}[htbp] + \begin{tikzpicture} + \tikzstyle{annotation} = [black]; + \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + \node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; + \draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); + \node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; + \draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); + \end{scope} + \end{tikzpicture} + \caption{Diagram of axial compression example. This static + simulation uses Dirichlet boundary conditions with axial + compression in the east-west (x-direction) and purely elastic + properties.} + \label{fig:example:subduction:3d:step01:diagram} +\end{figure} The first example problem is earthquake rupture involving coseismic slip along the interface between the subducting slab and the continental @@ -304,6 +329,9 @@ \subsubsection{Exercises} % Change spatial distribution and time history of slip. +% Add propagation of the slow slip (spatial variation of slip starting +% time, change rise time) + \subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} %% In this problem we generate Green's functions that will be used @@ -315,6 +343,8 @@ \subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} %% step07b: Generate Green's functions corresponding to updip %% slip on the subduction interface (slab top). + %% Allows trivial parallel. + %% Responses (Green's functions) are computed at simulated cGPS %% locations defined in the file cgps_sites.txt. %% Note that we change the default problem type from TimeDependent to From ed80cd164228361041c2748e8b9e0de0d41e146c Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 18:39:11 +1200 Subject: [PATCH 093/216] Added some more for examples 6 and 7. --- doc/userguide/examples/subduction3d.tex | 151 ++++++++++++++++++++---- 1 file changed, 125 insertions(+), 26 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index d04dd23ba9..1141ec5ec2 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -16,7 +16,7 @@ \subsection{Overview} and an accretionary wedge. To keep the computation time in these examples short, we limit our model to an 800 km $\times$ 800 km $\times$ 400 km domain and we will use a relatively coarse -discretization. For simplicity and to reduce comlexity in constructing +discretization. For simplicity and to reduce complexity in constructing the mesh, we use a flat top surface (elevation of 0 with respect to mean sea level). @@ -97,7 +97,7 @@ \subsection{Generating the Finite-Element Mesh} file and create a CUBIT/Trelis journal file (\filename{generate\_surfs.jou}) that adds additional contours west of the trench and then constructs the top and bottom surfaces of the -slab. The Python script also constructs a splay fault but copying a +slab. The Python script also constructs a splay fault by copying a contour to a depth below the slab and above the ground surface. \tip{We define the coordinate systems we use in the simulations in the @@ -325,36 +325,136 @@ \subsubsection{Exercises} \subsection{Step 6: Prescribed Slow-Slip Event} -\subsubsection{Exercises} - -% Change spatial distribution and time history of slip. - -% Add propagation of the slow slip (spatial variation of slip starting -% time, change rise time) +This example simulates a simple slow slip event (SSE) that remains +fixed spatially but increases its amplitude with time. We assume a +constant rake angle of 110 degrees, and a time duration of 30 +days. This problem requres the use of both a spatial database to +provide the spatial distribution of slip, and a temporal database to +describe the time evolution of slip. To create these databases we +provide the \filename{generate\_slowslip.py} script, which is in the +\filename{spatialdb} directory. Once you are in the +\filename{spatialdb} directory, run the script as follows: +\begin{shell} +$$ ./generate_slowslip.py +\end{shell} +This script reads parameters from \filename{generate\_slowslip.cfg} to +generate a Gaussian slip distribution in geographic coordinates, along +with a temporal database providing the slip amplitudes at different +times. The files created are: +\begin{itemize} +\item \filename{fault\_slabtop\_slowslip.spatialdb}: Spatial database +\item \filename{fault\_slabtop\_slowslip.timedb}: Temporal database +\end{itemize} + +Once the database files have been generated, it is possible to run the +example. Parameter settings that augment those in pylithapp.cfg are +contained in the file \filename{step06.cfg}. These settings are: +\begin{inventory} + \facilityitem{pylithapp.timedependent.formulation.time\_step}{Adjust + the total simulation time to 30 days with a time step size of 2 days.} + \facilityitem{pylithapp.timedependent.formulation}{Specify output + for the domain, for the ground surface, and for a set of + simulated cGPS sites.} + \facilityitem{pylithapp.timedependent.interfaces.slab}{Specify the + spatial distribution of slip and the temporal evolution of slip on + the slab interface. We change the slip function from the default + to a time history slip function to make use of the temporal database.} + \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the + base filenames for HDF5 output for all output types (for example, + \filename{step06-domain.h5}). Note that for cGPS output we need to + provide coordinate system information as well as the name of a + text file providing cGPS site locations.} +\end{inventory} +We use elastic properties for all materials, and custom solver +settings appropriate for a problem with a fault. We run the example by typing +\begin{shell} +$$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg +\end{shell} +The problem will produce 13 pairs of HDF5/Xdmf files. In the data +files (those without a \filename{\_info} before the file suffix) there +are field values representing 15 time steps. The additional HDF5 file +that was not present in previous examples is +\filename{step06-cgps\_sites.h5}, which contains the displacements at +the simulated cGPS sites. + +Figure \vref{fig:example:subduction:3d:step06}, which was created +using ParaView, shows the surface vertical displacement along with +horizontal displacement vectors at the cGPS sites, superimposed on +contours of the applied slip at t = 24 days. -\subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} + \caption{Solution for Step 6. The colors indicate the vertical + displacement, the vectors represent the horizontal displacements + at simulated cGPS sites, and the contours represent the applied + slip at t = 24 days. } + \label{fig:example:subduction:3d:step06} +\end{figure} - %% In this problem we generate Green's functions that will be used - %% to invert synthetic data generated from step06. There are two - %% different sub-problems: - %% step07a: Generate Green's functions corresponding to left-lateral - %% slip on the subduction interface (slab top). - %% step07b: Generate Green's functions corresponding to updip - %% slip on the subduction interface (slab top). +\subsubsection{Exercises} - %% Allows trivial parallel. +\begin{itemize} +\item Change spatial distribution and time history of slip. + \begin{itemize} + \item Edit \filename{generate\_slowslip.cfg} to change spatial and + temporal distributions, and edit \filename{step06.cfg} to change the + time duration and/or time step size. + \end{itemize} +\item Add propagation of the slow slip (spatial variation of slip + initiation time). + \begin{itemize} + \item Either alter Python script to produce a spatial database of + slip initiation times, or write a new script. + \end{itemize} +\end{itemize} - %% Responses (Green's functions) are computed at simulated cGPS - %% locations defined in the file cgps_sites.txt. - %% Note that we change the default problem type from TimeDependent to - %% GreensFns. +\subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} - %% Prior to generating the Green's functions, we first generate synthetic - %% data from the output of problem step06, using the make_synthetic_gpsdisp.py - %% script, with parameters defined in make_synthetic_gpsdisp.cfg: +This example is essentially a three-dimensional analog of +{sec:example:greensfns2d}, and is a more realistic example of how +PyLith can be used to perform geodetic inversions. We use the output +of example step06 to create synthetic data. Once we have done this we +generate Green's functions to represent the geodetic responses at a +set of synthetic cGPS stations. Finally, we use the synthetic data and +Green's functions to perform an inversion, using the same generalized +inverse approach described in {sec:example:greensfns2d}. + +We first generate the synthetic data by using the script +\filename{make_synthetic_gpsdisp.py} in the top-level directory. This +script reads the parameters in \filename{make_synthetic_gpsdisp.cfg} +to generate synthetic data from the selected time step with a +specified amount of noise. Run this script as: +\begin{shell} +$$ ./make_synthetic_gpsdisp.py +\end{shell} +This will create the following files: +\begin{itemize} +\item \filename{cgps_synthetic_displacement.txt}: Read by the + inversion script. +\item \filename{cgps_synthetic_displacement.vtk}: For visualization. +\end{itemize} + +After we generate the synthetic data, we generate the Green's +functions. We divide the Green's function generation into two sub-problems: +\begin{itemize} + \item step07a: Generate Green's functions corresponding to + left-lateral slip on the subduction interface (slab top). + \item step07b: Generate Green's functions corresponding to + updip slip on the subduction interface (slab top). +\end{itemize} +Note that the Green's functions could all be generated at the same +time; however, for real problems it is generally preferable to +separate the problems to improve runtimes (e.g., both problems can be +run simultaneously). + +To generate the Green's functions we change the problem type from the +default \facility{timedependent} to \facility{greensfns}. We do this +on the command line. When we change the problem type to +\facility{greensfns}, PyLith automatically reads the file +\filename{greensfns.cfg}. We use this file to augment the settings in +\filename{pylithapp.cfg}: - %% ./make_synthetic_gpsdisp.py %% After generating the synthetic data and Green's functions, we then %% perform a simple inversion using the slip_invert.py script, with @@ -373,7 +473,6 @@ \subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} %% ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt - \subsubsection{Exercises} % Move slip to splay fault in step06 and redo inversion. From 369eeaf9b9e61aa62438c34b19730cea97b0dbce Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Wed, 21 Jun 2017 18:39:57 +1200 Subject: [PATCH 094/216] Moved some stuff out of the step07.cfg files into greensfns.cfg. --- examples/3d/subduction/greensfns.cfg | 20 +++++++++++++++++++- examples/3d/subduction/step07a.cfg | 22 ---------------------- examples/3d/subduction/step07b.cfg | 22 ---------------------- 3 files changed, 19 insertions(+), 45 deletions(-) diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg index 536ddfe6cc..5d04b8b913 100644 --- a/examples/3d/subduction/greensfns.cfg +++ b/examples/3d/subduction/greensfns.cfg @@ -4,8 +4,26 @@ # problem # ---------------------------------------------------------------------- [greensfns] +interfaces = [slab] fault_id = 100 -interfaces = [fault] + +[greensfns.interfaces] +slab = pylith.faults.FaultCohesiveImpulses + +[greensfns.interfaces.slab] +label = fault_slabtop_patch +edge = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 2 + +# Spatial database for slip impulse amplitude. +db_impulse_amplitude = spatialdata.spatialdb.UniformDB +db_impulse_amplitude.label = Amplitude of fault slip impulses +db_impulse_amplitude.values = [slip] +db_impulse_amplitude.data = [1.0] # ---------------------------------------------------------------------- # output diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 8edb026eee..6a49f552d1 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -70,32 +70,10 @@ problem.progress_monitor.filename = output/step07a-progress.txt # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- -[pylithapp.problem] -# We prescribe slip on the slab fault patch. -interfaces = [slab] - -[pylithapp.problem.interfaces] -slab = pylith.faults.FaultCohesiveImpulses - [pylithapp.problem.interfaces.slab] -id = 100 -label = fault_slabtop_patch -edge = fault_slabtop_patch_edge - -# We must define the quadrature information for fault cells. -# The fault cells are 2D (surface). -quadrature.cell = pylith.feassemble.FIATSimplex -quadrature.cell.dimension = 2 - # Impulses for left-lateral slip. impulse_dof = [0] -# Spatial database for slip impulse amplitude. -db_impulse_amplitude = spatialdata.spatialdb.UniformDB -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.values = [slip] -db_impulse_amplitude.data = [1.0] - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 988e87f198..ed9e42dd01 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -70,32 +70,10 @@ problem.progress_monitor.filename = output/step07b-progress.txt # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- -[pylithapp.problem] -# We prescribe slip on the slab fault patch. -interfaces = [slab] - -[pylithapp.problem.interfaces] -slab = pylith.faults.FaultCohesiveImpulses - [pylithapp.problem.interfaces.slab] -id = 100 -label = fault_slabtop_patch -edge = fault_slabtop_patch_edge - -# We must define the quadrature information for fault cells. -# The fault cells are 2D (surface). -quadrature.cell = pylith.feassemble.FIATSimplex -quadrature.cell.dimension = 2 - # Impulses for reverse slip. impulse_dof = [1] -# Spatial database for slip impulse amplitude. -db_impulse_amplitude = spatialdata.spatialdb.UniformDB -db_impulse_amplitude.label = Amplitude of fault slip impulses -db_impulse_amplitude.values = [slip] -db_impulse_amplitude.data = [1.0] - # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- From 86cdc314eed084f4c424df78a6b1ca4a3761d838 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:10:23 -0700 Subject: [PATCH 095/216] Update list of references. --- doc/userguide/userguide.tex | 190 ++++++++++++++++++++---------------- 1 file changed, 104 insertions(+), 86 deletions(-) diff --git a/doc/userguide/userguide.tex b/doc/userguide/userguide.tex index 5ee27ca309..9ca04bf210 100644 --- a/doc/userguide/userguide.tex +++ b/doc/userguide/userguide.tex @@ -71,135 +71,153 @@ \input{license.tex} \begin{thebibliography}{Bibliography} + \bibitem[Aagaard et al., 2001a]{Aagaard:etal:2001a}Aagaard, B.T., -J.F. 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Knepley (2007), PyLith: A finite-element code for -modeling quasi-static and dynamic crustal deformation, \emph{Eos Trans. -AGU, 88}(52), Fall Meet. Suppl., Abstract T21B-0592. + Williams, and M. Knepley (2007), PyLith: A finite-element code for + modeling quasi-static and dynamic crustal deformation, \emph{Eos + Trans. AGU, 88}(52), Fall Meet. Suppl., Abstract T21B-0592. \bibitem[Aagaard et al., 2008]{Aagaard:etal:2008}Aagaard, B., C. -Williams, and M. Knepley (2008), PyLith: A finite-element code for -modeling quasi-static and dynamic crustal deformation, \emph{Eos Trans. -AGU}, \emph{89(}53), Fall Meet. Suppl., Abstract T41A-1925. + Williams, and M. Knepley (2008), PyLith: A finite-element code for + modeling quasi-static and dynamic crustal deformation, \emph{Eos + Trans. AGU}, \emph{89(}53), Fall Meet. Suppl., Abstract + T41A-1925. -\bibitem[Bathe, 1995]{Bathe:1995}Bathe, K.-J. 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Ely + (2002), Effct of a shallow weak zone on fault rupture: Numerical + simulation of scale-model experiments, + \textit{Bull. Seismol. Soc. Am.}, 92(8), 3022-3041, doi: + 10.1785/0120010273. \bibitem[Drucker and Prager, 1952]{Drucker:Prager:1952}Drucker, D. -C. and Prager, W. (1952). Soil mechanics and plastic analysis for -limit design, \textit{Quarterly of Applied Mathematics}, \textit{10}, -157\textendash{}165. + C. and Prager, W. (1952). Soil mechanics and plastic analysis for + limit design, \textit{Quarterly of Applied Mathematics}, + \textit{10}, 157\textendash{}165. + +\bibitem[Hayes et al., 2012]{Hayes:etal:2012}Hayes, G. P., D. J. Wald, + and R. L. Johnson (2012), Slab1.0: A three-dimensional model of + global subduction zone geometries, J. Geophys. Res., 117, B01302, + doi:10.1029/2011JB008524. \bibitem[Liu et al., 2006]{Liu:etal:2006}Liu, P., R.J. Archuleta, -S.H. Hartzell (2006), Prediction of broadband ground-motion time histories: -Hybrid low/high-frequency method with correlated random source parameters, -\textit{Bull. Seismol. Soc. Am., 96}, 2118-2130. + S.H. Hartzell (2006), Prediction of broadband ground-motion time + histories: Hybrid low/high-frequency method with correlated random + source parameters, \textit{Bull. Seismol. Soc. Am., 96}, 2118-2130. \bibitem[Kaneko et al., 2008]{Kaneko:etal:2008}Kaneko, Y., N. Lapusta, -and J.-P. Ampuero (2008), Spectral element modeling of spontaneous -earthquake rupture on rate and state faults: Effect of velocity-strengthening -friction at shallow depths, \textit{Journal of Geophysical Research},\textit{ -113}, B09317, doi:10.1029/2007JB005553. - -\bibitem[Kaus et al., 2010]{Kaus:etal:2010}Kaus, B. J. P., H. Muhlhaus, -and D. A. May (2010), A stabilization algorithm for geodynamic numerical -simulations with a free surface, \textit{Physics of the Earth and -Planetary Interiors}, \textit{181}, 12-20, doi:10.1016/j.pepi.2010.04.007. + and J.-P. Ampuero (2008), Spectral element modeling of spontaneous + earthquake rupture on rate and state faults: Effect of + velocity-strengthening friction at shallow depths, \textit{Journal + of Geophysical Research},\textit{ 113}, B09317, + doi:10.1029/2007JB005553. + +\bibitem[Kaus et al., 2010]{Kaus:etal:2010}Kaus, B. J. P., + H. Muhlhaus, and D. A. May (2010), A stabilization algorithm for + geodynamic numerical simulations with a free surface, + \textit{Physics of the Earth and Planetary Interiors}, \textit{181}, + 12-20, doi:10.1016/j.pepi.2010.04.007. \bibitem[Kirby and Kronenberg, 1987]{Kirby:Kronenberg:1987}Kirby, -S. H. and A. K. Kronenberg (1987), Rheology of the lithosphere: Selected -topics, \textit{Reviews of Geophysics, 25}, 1219-1244. + S. H. and A. K. Kronenberg (1987), Rheology of the lithosphere: + Selected topics, \textit{Reviews of Geophysics, 25}, 1219-1244. \bibitem[Knopoff and Ni, 2001]{Knopoff:Ni:2001}Knopoff, L. and X.X. -Ni (2001), Numerical instability at the edge of a dynamic fracture, -\emph{Geophysical Journal International,}\textit{\emph{ }}\textit{147}(3), -1-6, doi: 10.1046/j.1365-246x.2001.01567.x. + Ni (2001), Numerical instability at the edge of a dynamic fracture, + \emph{Geophysical Journal International,}\textit{\emph{ + }}\textit{147}(3), 1-6, doi: 10.1046/j.1365-246x.2001.01567.x. \bibitem[Kojic and Bathe, 1987]{Kojic:Bathe:1987}Kojic, M. and K.-J. -Bathe (1987), The `Effective Stress-Function' Algorithm for Thermo-Elasto-Plasticity -and Creep, \emph{Int. J. Num. Meth. Eng}.\emph{, 24}, 1509-1532. + Bathe (1987), The `Effective Stress-Function' Algorithm for + Thermo-Elasto-Plasticity and Creep, + \emph{Int. J. Num. Meth. Eng}.\emph{, 24}, 1509-1532. -\bibitem[McGarr, 1988]{McGarr:1988}McGarr, A. (1988), On the state -of lithospheric stress in the absence of applied tectonic forces, -\textit{Journal of Geophysical Research}, \textit{93}, 13,609-13,617. +\bibitem[McGarr, 1988]{McGarr:1988}McGarr, A. (1988), On the state of + lithospheric stress in the absence of applied tectonic forces, + \textit{Journal of Geophysical Research}, \textit{93}, + 13,609-13,617. \bibitem[Menke, 1984]{Menke:1984}Menke, W. (1984), \textit{Geophysical -Data Analysis: Discrete Inverse Theory}, Academic Press, Inc., Orlando, -260 pp. + Data Analysis: Discrete Inverse Theory}, Academic Press, Inc., + Orlando, 260 pp. -\bibitem[Okada, 1992]{Okada:1992}Okada, Y., Internal deformation -due to shear and tensile faults in a half-space (1992), \textit{Bull. -Seismol. Soc. Am.}, \textit{83}, 1018-1040. +\bibitem[Okada, 1992]{Okada:1992}Okada, Y., Internal deformation due + to shear and tensile faults in a half-space (1992), \textit{Bull. + Seismol. Soc. Am.}, \textit{83}, 1018-1040. \bibitem[Paterson, 1994]{Paterson:1994}Paterson, W. S. B. (1994), -\textit{The Physics of Glaciers, Third Edition}, Elsevier Science -Ltd., Oxford, 480 pp. + \textit{The Physics of Glaciers, Third Edition}, Elsevier Science + Ltd., Oxford, 480 pp. -\bibitem[Prentice, 1968]{Prentice:1968}Prentice, J. H, (1968), Dimensional -problem of the power law in rheology, \textit{Nature}, \textit{217}, -157. +\bibitem[Prentice, 1968]{Prentice:1968}Prentice, J. H, (1968), + Dimensional problem of the power law in rheology, \textit{Nature}, + \textit{217}, 157. \bibitem[Savage and Prescott, 1978]{Savage:Prescott:1978}Savage, -J. C. and W. H. Prescott (1978), Asthenosphere readjustment and the -earthquake cycle, \textit{Journal of Geophysical} \textit{Research}\emph{, -83}, 3369-3376. + J. C. and W. H. Prescott (1978), Asthenosphere readjustment and the + earthquake cycle, \textit{Journal of Geophysical} + \textit{Research}\emph{, 83}, 3369-3376. + +\bibitem[Stephenson, 2007]{Stephenson:2007}Stephenson, W.J. (2007), + Velocity and density models incorporating the Cascadia subduction + zone for 3D earthquake ground motion simulations, Version 1.3: + U.S. Geological Survey, Earthquake Hazards Ground Motion + Investigations, Open-File Report 2007–1348, 24 pages, + https://pubs.usgs.gov/of/2007/1348/. \bibitem[Taylor, 2003]{Taylor:2003}Taylor, R.L. (2003), `FEAP--A -Finite Element Analysis Program', \textit{Version 7.5 Theory Manual}, -154 pp. + Finite Element Analysis Program', \textit{Version 7.5 Theory + Manual}, 154 pp. -\bibitem[Timoshenko and Goodier, 1987]{Timoshenko:Goodier:1987}Timoshenko, -S.P. and J.N. Goodier (1987), \textit{Theory of Elasticity, Third -Edition}, McGraw-Hill, New York, 567 pp. +\bibitem[Timoshenko and Goodier, + 1987]{Timoshenko:Goodier:1987}Timoshenko, S.P. and J.N. Goodier + (1987), \textit{Theory of Elasticity, Third Edition}, McGraw-Hill, + New York, 567 pp. \bibitem[Williams et al., 2005]{Williams:etal:2005}Williams, C.A., -B. Aagaard, and M.G. Knepley (2005), Development of software for studying -earthquakes across multiple spatial and temporal scales by coupling -quasi-static and dynamic simulations, \emph{Eos Trans. AGU, 86}(52), -Fall Meet. Suppl., Abstract S53A-1072. + B. Aagaard, and M.G. Knepley (2005), Development of software for + studying earthquakes across multiple spatial and temporal scales by + coupling quasi-static and dynamic simulations, \emph{Eos Trans. AGU, + 86}(52), Fall Meet. Suppl., Abstract S53A-1072. -\bibitem[Williams, 2006]{Williams:2006}Williams, C.A. (2006), Development -of a package for modeling stress in the lithosphere, \emph{Eos Trans. -AGU,} \emph{87}(36), Jt. Assem. Suppl., Abstract T24A-01 Invited. +\bibitem[Williams, 2006]{Williams:2006}Williams, C.A. (2006), + Development of a package for modeling stress in the lithosphere, + \emph{Eos Trans. AGU,} \emph{87}(36), Jt. Assem. Suppl., Abstract + T24A-01 Invited. -\bibitem[Zienkiewicz and Taylor, 2000]{Zienkiewicz:Taylor:2000}Zienkiewicz, -O.C. and R.L. Taylor (2000), \textit{The Finite Element Method, Fifth -Edition, Volume 2: Solid Mechanics}, Butterworth-Heinemann, Oxford, -459 pp.125 +\bibitem[Zienkiewicz and Taylor, + 2000]{Zienkiewicz:Taylor:2000}Zienkiewicz, O.C. and R.L. Taylor + (2000), \textit{The Finite Element Method, Fifth Edition, Volume 2: + Solid Mechanics}, Butterworth-Heinemann, Oxford, 459 pp.125 -\bibitem[Hayes et al., 2012]{Hayes:etal:2012}Hayes, G. P., D. J. Wald, - and R. L. Johnson (2012), Slab1.0: A three-dimensional model of - global subduction zone geometries, J. Geophys. Res., 117, B01302, - doi:10.1029/2011JB008524. \end{thebibliography} From a47bb1722f53e650ed3cd2727a991e8f772ce707 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:10:31 -0700 Subject: [PATCH 096/216] Fix typo. --- examples/3d/hex8/README | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/hex8/README b/examples/3d/hex8/README index 1bf265b89f..10388ad775 100644 --- a/examples/3d/hex8/README +++ b/examples/3d/hex8/README @@ -1,4 +1,4 @@ -The examples in this directory form a step-by-step sequence of 20 problems, +The examples in this directory form a step-by-step sequence of 21 problems, each building on the one before (for the most part). All of the examples use the same mesh, which was created by Cubit. The mesh is 6 km x 6 km x 4 km with linear hexahedral cells that have edges 1.0 km long. From 877b840672012b7a3cbb19d03ecc612addd1c058 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:17:04 -0700 Subject: [PATCH 097/216] Followed Charles' lead and moved a couple more things from step07a,b.cfg to greensfns.cfg. --- examples/3d/subduction/greensfns.cfg | 27 +++++++++++++++++++++++++-- examples/3d/subduction/step07a.cfg | 17 +++++++++-------- examples/3d/subduction/step07b.cfg | 17 +++++++++-------- 3 files changed, 43 insertions(+), 18 deletions(-) diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg index 5d04b8b913..0b13bc422f 100644 --- a/examples/3d/subduction/greensfns.cfg +++ b/examples/3d/subduction/greensfns.cfg @@ -1,5 +1,23 @@ -[greensfns] - +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# +# This is not a self-contained simulation configuration file. This +# file only specifies the general parameters common to the Green's +# function simulations. +# # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- @@ -28,6 +46,11 @@ db_impulse_amplitude.data = [1.0] # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +[greensfns.interfaces.slab.output] +# Add impulse amplitude to fault info output. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 + # Turn off output of state variables for materials. [greensfns.materials.slab.output] cell_data_fields = [] diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 6a49f552d1..8a234f2c82 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -77,11 +77,12 @@ impulse_dof = [0] # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +# Add cggs_sites to solution output. [pylithapp.problem.formulation] output = [domain, subdomain, cgps_sites] output.cgps_sites = pylith.meshio.OutputSolnPoints -# Domain, subdomain, and points output --------------------------------- +# Domain, subdomain, and cgs_sites [pylithapp.problem.formulation.output.domain] writer.filename = output/step07a-domain.h5 # Turn off data fields. @@ -93,22 +94,22 @@ writer.filename = output/step07a-groundsurf.h5 vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07a-cgps_sites.h5 + +# Set coordinate system associated with file with cGPS sites +reader.filename = cgps_sites.txt coordsys = spatialdata.geocoords.CSGeo coordsys.space_dim = 3 coordsys.datum_horiz = WGS84 coordsys.datum_vert = mean sea level -writer = pylith.meshio.DataWriterHDF5 -reader.filename = cgps_sites.txt -writer.filename = output/step07a-cgps_sites.h5 -# Fault output ------------------------------------------------------ +# Fault [pylithapp.problem.interfaces.slab.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step07a-fault-slab.h5 -# Material output ------------------------------------------------------ +# Materials [pylithapp.problem.materials.slab.output] writer.filename = output/step07a-slab.h5 diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index ed9e42dd01..5de988cb81 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -77,11 +77,12 @@ impulse_dof = [1] # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +# Add cggs_sites to solution output. [pylithapp.problem.formulation] output = [domain, subdomain, cgps_sites] output.cgps_sites = pylith.meshio.OutputSolnPoints -# Domain, subdomain, and points output --------------------------------- +# Domain, subdomain, and cgs_sites [pylithapp.problem.formulation.output.domain] writer.filename = output/step07b-domain.h5 # Turn off data fields. @@ -93,22 +94,22 @@ writer.filename = output/step07b-groundsurf.h5 vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step07b-cgps_sites.h5 + +# Set coordinate system associated with file with cGPS sites +reader.filename = cgps_sites.txt coordsys = spatialdata.geocoords.CSGeo coordsys.space_dim = 3 coordsys.datum_horiz = WGS84 coordsys.datum_vert = mean sea level -writer = pylith.meshio.DataWriterHDF5 -reader.filename = cgps_sites.txt -writer.filename = output/step07b-cgps_sites.h5 -# Fault output ------------------------------------------------------ +# Fault [pylithapp.problem.interfaces.slab.output] -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step07b-fault-slab.h5 -# Material output ------------------------------------------------------ +# Materials [pylithapp.problem.materials.slab.output] writer.filename = output/step07b-slab.h5 From d78a15f3508e4f5e8484373c86139ff4cbc5a9a8 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:17:53 -0700 Subject: [PATCH 098/216] Small cleanup. --- examples/3d/subduction/mat_elastic.cfg | 11 ++++++++--- examples/3d/subduction/mat_viscoelastic.cfg | 4 ++++ examples/3d/subduction/pylithapp.cfg | 21 +++++++++++++++++---- examples/3d/subduction/step01.cfg | 5 ----- 4 files changed, 29 insertions(+), 12 deletions(-) diff --git a/examples/3d/subduction/mat_elastic.cfg b/examples/3d/subduction/mat_elastic.cfg index 9035e3082f..2e3c4623c1 100644 --- a/examples/3d/subduction/mat_elastic.cfg +++ b/examples/3d/subduction/mat_elastic.cfg @@ -18,9 +18,11 @@ # 'wedge', 'mantle', and 'crust'. # # We use a SimpleDB with a single point for each material. We could -# have used a UniformDB, but this makes it easier to adjust the -# spatial database file should we want to add in a spatial variation -# to the material properties. +# have used a UniformDB, but we will reuse some of these spatial +# databases for the elastic properties when we specify the properties +# for the linear Maxwell viscoelastic models. Additionally, using +# SimpleDB makes it easier to adjust the spatial database file should +# we want to add in a spatial variation to the material properties. [pylithapp.problem.materials] slab = pylith.materials.ElasticIsotropic3D @@ -34,16 +36,19 @@ db_properties = spatialdata.spatialdb.SimpleDB db_properties.label = Properties for subducting slab db_properties.iohandler.filename = spatialdb/mat_slab_elastic.spatialdb +# Wedge [pylithapp.problem.materials.wedge] db_properties = spatialdata.spatialdb.SimpleDB db_properties.label = Properties for accretionary wedge db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb +# Mantle [pylithapp.problem.materials.mantle] db_properties = spatialdata.spatialdb.SimpleDB db_properties.label = Properties for mantle db_properties.iohandler.filename = spatialdb/mat_mantle_elastic.spatialdb +# Crust [pylithapp.problem.materials.crust] db_properties = spatialdata.spatialdb.SimpleDB db_properties.label = Properties for continental crust diff --git a/examples/3d/subduction/mat_viscoelastic.cfg b/examples/3d/subduction/mat_viscoelastic.cfg index e34505698b..8b58619729 100644 --- a/examples/3d/subduction/mat_viscoelastic.cfg +++ b/examples/3d/subduction/mat_viscoelastic.cfg @@ -27,6 +27,7 @@ crust = pylith.materials.ElasticIsotropic3D slab = pylith.materials.MaxwellIsotropic3D mantle = pylith.materials.MaxwellIsotropic3D + # Slab [pylithapp.problem.materials.slab] db_properties = spatialdata.spatialdb.CompositeDB @@ -46,12 +47,14 @@ db_B.label = Linear Maxwell viscoelatic properties db_B.filename = spatialdb/mat_viscosity.spatialdb db_B.query_type = linear + # Wedge [pylithapp.problem.materials.wedge] db_properties = spatialdata.spatialdb.SimpleDB db_properties.label = Properties for accretionary wedge db_properties.iohandler.filename = spatialdb/mat_wedge_elastic.spatialdb + # Mantle [pylithapp.problem.materials.mantle] db_properties = spatialdata.spatialdb.CompositeDB @@ -71,6 +74,7 @@ db_B.label = Linear Maxwell viscoelatic properties db_B.filename = spatialdb/mat_viscosity.spatialdb db_B.query_type = linear + # Crust [pylithapp.problem.materials.crust] db_properties = spatialdata.spatialdb.SimpleDB diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index ebf6958874..d24176268d 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -1,9 +1,23 @@ -[pylithapp] - +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# # This is not a self-contained simulation configuration file. This # file only specifies the general parameters common to the simulations # in this directory. - +# # ---------------------------------------------------------------------- # journal # ---------------------------------------------------------------------- @@ -176,7 +190,6 @@ writer = pylith.meshio.DataWriterHDF5 # ---------------------------------------------------------------------- # PETSc # ---------------------------------------------------------------------- -# Set the solver options. [pylithapp.petsc] malloc_dump = diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index c12bdc0e14..e298499139 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -65,9 +65,6 @@ total_time = 0.0*year # -x face [pylithapp.problem.bc.x_neg] -bc_dof = [0] -label = boundary_xneg -# Use a UniformDB db_initial = spatialdata.spatialdb.UniformDB db_initial.label = Dirichlet BC on -x db_initial.values = [displacement-x] @@ -75,8 +72,6 @@ db_initial.data = [+2.0*m] # +x face [pylithapp.problem.bc.x_pos] -bc_dof = [0] -label = boundary_xpos db_initial = spatialdata.spatialdb.UniformDB db_initial.label = Dirichlet BC on +x db_initial.values = [displacement-x] From a5ad3927733957292f69992bb40c431bf352994d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:18:42 -0700 Subject: [PATCH 099/216] Rewrite README for users, removing temporary comments. --- examples/3d/subduction/README | 150 +++++----------------------------- 1 file changed, 21 insertions(+), 129 deletions(-) diff --git a/examples/3d/subduction/README b/examples/3d/subduction/README index 59aaa57ff3..f1bfde0419 100644 --- a/examples/3d/subduction/README +++ b/examples/3d/subduction/README @@ -1,131 +1,23 @@ -Directory structure: - mesh (mesh related files) - spatialdb (spatial and temporal database related files) - viz (ParaView Python scripts) - - -Elastic properties loosely based on - -Stephenson, W.J., 2007, Velocity and density models incorporating the -Cascadia subduction zone for 3D earthquake ground motion simulations, -Version 1.3: U.S. Geological Survey, Earthquake Hazards Ground Motion -Investigations, Open-File Report 2007–1348, 24 pages, -https://pubs.usgs.gov/of/2007/1348/. - - - -Features: - - Spatial databases - + SimpleDB [1] - + UniformDB [1,2,3] - + SimpleGridDB [2,3] - + CompositeDB [2,3] - - - Geographic coordinates with SimpleGridDB - - Depth profile with SimpleGridDB [2,3] - - Dirichlet Boundary conditions - + Fixed displacement [1,2,3] - + Fixed velocity - + Time history - - Materials - + Elastic [1,2,3] - + Linear Maxwell viscoelastic [2,3] - + Powerlaw [exercise] - - Preconditioners - + LU [1] - + AMG (ML) [1ex] - + AMG (ML) + custom preconditioner [2,3] - - Uniform refinement [exercise] - - Output - + Output of solution [1,2,3] - + Output of solution on ground surface [1,2,3] - + Output of solution at points - + Output of state variables - - + HDF5 - - Visualization with ParaView Python scripts - - Generation of spatial databases via Python +The examples in this directory form a step-by-step sequence of 8 +problems involving a 3-D subduction zone. In general, each example +builds on the previous one. All of the examples use the same mesh, +generated using CUBIT/Trelis. - Coordinate systems - - + Geographic projection - + Geographic - - Faults - + Buried edges [2,3] - + Intersecting - + Multiple faults [3] - + Prescribed slip [2,3] - + Prescribed slip w/multiple ruptures - + Fault friction - -Step01: Axial compression [tutorial] - Dirichlet BC with initial values (UniformDB) - SimpleDB with properties for each material - Static - LU preconditioner - - ParaView - Python script to view displacement field - Python script to view material properties (shear modulus) - - Exercise: Shear instead of axial compression - -Step02: Coseismic [exercise] - DirichletBC constraining normal displacement on lateral and bottom boundaries - Prescribed uniform slip (UniformDB) on slab fault patch with viscoelastic relaxation - Viscosity via CompositeDB (single SimpleGridDB with viscosity as a fn of depth) - Quasistatic - field split + custom preconditioner - - ParaView - Python script to view prescribed slip - Python script to view relaxation of shear stress - - Exercise: Change slip on slab to slip on splay fault - Exercise: Slip on lower slab and splay fault - Exercise: Slip on slab and splay fault - -Step03: Interseismic [tutorial] - DirichletBC with constant velocity (compression) - Prescribed fault slip with constant slip rate (UniformDB) [lower slab] - Prescribed fault slip with constant slip rate at depth (SimpleGridDB) [top slab] - Quasistatic - -Step04: Earthquake cycle [exercise] - Interseismic + coseismic - - Exercise: Make lower slab + splay fault the primary fault surface - and the upper slab (trench side of the splay fault) the secondary - fault surface. Hint: You will need to create a nodesets in CUBIT - that correspond to the primary and secondary fault surfaces. - -Step05: Compression with frictional interface [tutorial] - Interseismic + rate- and state-friction - Quasistatic - -Step06: Slow slip event [tutorial] - DirichletBC constraining normal displacement on lateral and bottom boundaries - Prescribed slow slip on slab fault patch (SimpleGridDB 2-D in geo coordinates) - Time history slip-time function - Quasistatic - OutputSolnPoints - -Step07: Green's functions [tutorial] - Generate Green's functions (slab patch + splay patch?) - Simple inversion of GPS data (slip on slab or splay?) - OutputSolnPoints - -Step08: Gravity - uniform density (SimpleDB), demonstrate initial stresses to compensate gravity - variable density (match Step01), initial stress matches avg desnity, elastic: demonstrate deviation - variable density, elastic+viscoelastic: demonstrate problems +See the PyLith User Manual for a detailed discussion of these examples. +Directory structure: + * mesh (mesh related files) + * output (simulation output files, created automatically by PyLith) + * spatialdb (spatial and temporal database related files) + * (viz (ParaView Python scripts) + +List of examples + +step01: Axial compression +step02: Prescribed coseismic slip and postseismic relaxation +step03: Prescribed aseismic creep and interseismic deformation +step04: Prescribed earthquake cycle +step05: Spontaneous rupture driven by subducting slab +step06: Prescribed slow-slip event +step07a,b: Inversion of slow-slip event using 3-D Green's functions +step08a,b,c: Stress field due to gravitational body forces From bc6ce1c723ac8ac776d372077035e3562e19d583 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:19:08 -0700 Subject: [PATCH 100/216] Add more overview material and finish step01. --- .../figs/subduction3d_step01_soln.jpg | Bin 0 -> 202037 bytes doc/userguide/examples/subduction3d.tex | 335 ++++++++++++++---- 2 files 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coordsys

.space_dim = 3 +

coordsys

.datum_horiz = WGS84 +

coordsys.datum_vert

= mean sea level +

coordsys.projector.projection

= tmerc +

coordsys.projector.proj_options

= +lon_0=-122.6765 +lat_0=45.5231 +k=0.9996 +\end{cfg} + +\subsubsection{Materials} + +The finite-element mesh marks cells for each material and the type of +cell determines the type of basis functions we use in the +discretization. This means we can specify this information in the +\filename{pylithapp.cfg} file and avoid duplicating it in each +simulation parameter file. For eacmple for the slab, the parameters include +\begin{cfg} +[pylithapp.problem.materials.slab] +

label

= Subducting slab ; Label for informative error messages +

id

= 1 ; Block id in ExodusII file from CUBIT/Trelis +quadrature.cell = pylith.feassemble.FIATSimplex ; Tetrahedral cells +

quadrature.cell.dimension

= 3 + +# Average cell output over quadrature points, yielding one point per cell +output.cell_filter = pylith.meshio.CellFilterAvg +output.writer = pylith.meshio.DataWriterHDF5 ; Output using HDF5 +\end{cfg} + In this set of examples, we will consider cases in which all materials are linear, isotropic elastic and cases where the crust and wedge are linear, isotropic elastic but the slab and mantle are linear Maxwell @@ -200,15 +241,70 @@ \subsection{Organization of Simulation Parameters} the case with purely elastic models and \filename{mat\_viscoelastic.cfg} for the case with a mix of elastic and viscoelastic models. Each of these files specifies the bulk -constitutive model and spatial database to use for each material. - -Similarly, we group solver parameters into a few different files to -handle different cases. The \filename{pylithapp.cfg} file uses a -direct solver, which is suitable for debugging and test problems that -do not include a fault; a direct solver is not well-suited for -production runs because it does not scale well and uses a lot of -memory. The \filename{solver\_algebraicmultigrid.cfg} provides more -optimal settings for simulations without a fault by using an algebraic +constitutive model and spatial database to use for the properties for +each material. The values for the material properties are loosely +based on a 3-D seismic velocity model for the Pacific Northwest +\cite{Stephenson:2007}. + +\subsubsection{Boundary Conditions} + +For the Dirichlet boundary conditions, we specify the degree of +freedom constrained, the name of the nodeset in the ExodusII file from +CUBIT/Trelis that defines the boundary, and a label for the spatial +database (required for informative error messages). These settings +constrain the y-displacement on the north (+y) boundary: +\begin{cfg} +[pylithapp.problem.bc.y_pos] +

bc_dof

= [1] ; Degree of freedoms are: x=0, y=1, and z=2 +

label

= boundary_ypos ; nodeset in ExodusII file form CUBIT/Trelis +

db_initial.label

= Dirichlet BC on +y ; label for informative error messages +\end{cfg} + +\subsubsection{Solver Parameters} + +We group solver parameters into a few different files to handle +different cases. The \filename{pylithapp.cfg} contains tolerance +values for the linear and nonlinear solvers and turns on some simple +diagnostic information. The file also directs PyLith to use a direct +solver, which is suitable for debugging and test problems that do not +include a fault; a direct solver is not well-suited for production +runs because it does not scale well and uses a lot of memory. +\begin{cfg} +[pylithapp.petsc] +

malloc_dump

= ; Dump information about PETSc memory not deallocated. + +# Use LU preconditioner (helful for learning and debugging, not production simulations) +

pc_type

= lu + +# Convergence parameters. +

ksp_rtol

= 1.0e-10 ; Converge if residual norm decreases by this amount +

ksp_atol

= 1.0e-11 ; Converge if residual norm drops below this value +

ksp_max_it

= 500 ; Maximum number of iterations in linear solve +

ksp_gmres_restart

= 50 ; Restart orthogonalization in GMRES after this number of iterations + +# Linear solver monitoring options. +

ksp_monitor

= true ; Show residual norm at each iteration +#ksp_view = true ; Show solver parameters (commented out) +

ksp_converged_reason

= true ; Show reason linear solve converged +

ksp_error_if_not_converged

= true ; Generate an error if linear solve fails to converge + +# Nonlinear solver monitoring options. +

snes_rtol

= 1.0e-10 ; Converge if nonlinear residual norm decreases by this amount +

snes_atol

= 1.0e-9 ; Converge if nonlinear residual norm drops below this value +

snes_max_it

= 100 ; Maximum number of iterations in nonlinear solve +

snes_monitor

= true ; Show nonlinear residual norm at each iteration +

snes_linesearch_monitor

= true ; Show nonlinear solver line search information +#snes_view = true ; Show nolinear solver parameters (commented out) +

snes_converged_reason

= true ; Show reason nonlinear solve converged +

snes_error_if_not_converged

= true ; Generate an error if nonlinear solve fails to converge + +# PETSc summary -- useful for performance information. +

log_view

= true +\end{cfg} + +The +\filename{solver\_algebraicmultigrid.cfg} provides more optimal +settings for simulations without a fault by using an algebraic multigrid preconditioner. Similarly, for simulations with a fault \filename{solver\_fieldsplit.cfg} provides settings for applying the algebraic multigrid preconditioner to the elasticity portion of the @@ -216,11 +312,17 @@ \subsection{Organization of Simulation Parameters} Lagrange multiplier portion. \subsection{Step 1: Axial Compression} - -% big picture -% + squeeze boundaries => DirichletBC with prescribed displacements -% + elastic material properties => linear solver with single time step - +\label{sec:example:subduction:3d:step01} + +We start with a very simple example of axial compression in the +east-west direction with purely elastic material properties, and no +faults (Figure~\ref{fig:example:subduction:3d:step01:diagram}). We +impose axial compression using Dirichlet boundary conditions on the +east (+x) and west (-x) boundaries and confine the domain in the +north-south direction via zero displacement Dirichlet boundary +conditions on the north (+y) and south (-y) boundaries. We constrain +the vertical displacement by imposing zero displacement boundary +conditions on the bottom (-z) boundary. \begin{figure}[htbp] \begin{tikzpicture} @@ -235,68 +337,144 @@ \subsection{Step 1: Axial Compression} \end{tikzpicture} \caption{Diagram of axial compression example. This static simulation uses Dirichlet boundary conditions with axial - compression in the east-west (x-direction) and purely elastic - properties.} + compression in the east-west (x-direction), roller boundary + conditions on the north, south, and bottom boundaries, and purely + elastic properties.} \label{fig:example:subduction:3d:step01:diagram} \end{figure} -The first example problem is earthquake rupture involving coseismic -slip along the interface between the subducting slab and the continental -crust and uppermost portion of the mantle below the continental crust. -The spatial variation of slip comes from a cross-section of Gavin -Hayes' finite-source model \url{earthquake.usgs.gov/earthquakes/eqinthenews/2011/usc0001xgp/finite_fault.php}. -On the lateral and bottom boundaries of the domain, we fix the degrees -of freedom perpendicular to the boundary as shown in Figure \vref{fig:example:subduction:2d:steps}. -Parameter settings that augment those in \filename{pylithapp.cfg} are -contained in the file \filename{step01.cfg}. These settings are: -\begin{inventory} - \facilityitem{pylithapp.timedependent.formulation.time\_step}{Adjust the total - simulation time to 0 years (static simulation).} - \facilityitem{pylithapp.timedependent}{Specifies the array of - boundary conditions.} - \facilityitem{pylithapp.timedependent.bc.\textit{BOUNDARY}}{Defines the settings - for boundary \textit{BOUNDARY}, including which degrees of freedom - are being constrained (x or y), the label (defined in\filename{ mesh\_tri3.exo}) - corresponding to the nodeset in CUBIT, and a label to the boundary - condition used in any error messages.} - \facilityitem{pylithapp.timedependent.interfaces.fault}{Specify the coseismic - slip along the interface between the oceanic crust and continental - crust with a small amount of slip penetrating into the upper mantle.} - \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the base filenames - for HDF5 output (for example, \filename{step01.h5}).} -\end{inventory} +The \filename{pylithapp.cfg} file creates an array of five boundary +conditions, which impose zero displacements by default. We overwrite +this behavior in the \filename{step01.cfg} file for the -x and +x +boundaries using spatial databases with a single uniform displacement +value to create the axial compression: +\begin{cfg} +# -x face +[pylithapp.problem.bc.x_neg] +db_initial = spatialdata.spatialdb.UniformDB +

db_initial.label

= Dirichlet BC on -x +

db_initial.values

= [displacement-x] +

db_initial.data

= [+2.0*m] + +# +x face +[pylithapp.problem.bc.x_pos] +db_initial = spatialdata.spatialdb.UniformDB +

db_initial.label

= Dirichlet BC on +x +

db_initial.values

= [displacement-x] +

db_initial.data

= [-2.0*m] +\end{cfg} + +As discussed in Section~\ref{sec:example:subduction:3d:organization}, +we use \filename{mat\_elastic.cfg} to specify the parameters +associated with linear, isotropic elastic bulk constitutive models for +all of the materials for convenient reuse across several different +simulations. +\begin{cfg} +[pylithapp.problem.materials] +slab = pylith.materials.ElasticIsotropic3D +wedge = pylith.materials.ElasticIsotropic3D +crust = pylith.materials.ElasticIsotropic3D +mantle = pylith.materials.ElasticIsotropic3D + +# Slab +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.SimpleDB +

db_properties.label

= Properties for subducting slab +

db_properties.iohandler

.filename = spatialdb/mat_slab_elastic.spatialdb + +# Wedge +[pylithapp.problem.materials.wedge] +db_properties = spatialdata.spatialdb.SimpleDB +

db_properties.label

= Properties for accretionary wedge +

db_properties.iohandler.filename

= spatialdb/mat_wedge_elastic.spatialdb + +# Mantle +[pylithapp.problem.materials.mantle] +db_properties = spatialdata.spatialdb.SimpleDB +

db_properties.label

= Properties for mantle +

db_properties.iohandler.filename

= spatialdb/mat_mantle_elastic.spatialdb + +# Crust +[pylithapp.problem.materials.crust] +db_properties = spatialdata.spatialdb.SimpleDB +

db_properties.label

= Properties for continental crust +

db_properties.iohandler.filename

= spatialdb/mat_crust_elastic.spatialdb +\end{cfg} +We specify different elastic properties for each material +(slab, wedge, mantle, and crust) using \object{SimpleDB} spatial +databases with a single point to specify uniform properties within a +material. We choose \object{SimpleDB} rather than \object{UniformDB}, +because we will reuse some of these spatial databases for the elastic +properties when we use linear Maxwell viscoelastic constitutive model. + +The remaining parameters in the \filename{step01.cfg} file are mostly +associated with setting filenames for all of the various output, +including all of the parameters used and version information in a JSON +file, a file reporting the progress of the simulation and estimated +time of completion, and the filenames for the HDF5 files (the +corresponding Xdmf files will use the same filename with the +\filename{.xmf} suffix). + We run this example by typing \begin{shell} -$$ pylith step01.cfg +$$ pylith step01.cfg mat_elastic.cfg \end{shell} -The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 +The problem will produce ten pairs of HDF5/Xdmf files. The HDF5 files contain the data and the Xdmf files contain the metadata required -by ParaView and Visit (and possibly other visualization tools that +by ParaView and Visit (and other visualization tools that use Xdmf files) to access the mesh and data sets in the HDF5 files. The files include the solution over the domain and ground surface -(two pairs of files), physical properties, stress, and strain within -each material (eight pairs of files), and fault parameters, slip, -and traction (two pairs of files). +(two pairs of files), and physical properties, stress, and strain within +each material (eight pairs of files). -Figure \vref{fig:example:subduction:2d:step01}, which was created using +Figure \vref{fig:example:subduction:3d:step01}, which was created using ParaView, displays the magnitude of the displacement field with the deformation exaggerated by a factor of 1000. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction2d_step01_soln} - \caption{Solution for Step 1. The colors indicate the magnitude of the displacement, - and the deformation is exaggerated by a factor of 1000. } - \label{fig:example:subduction:2d:step01} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step01_soln} + \caption{Solution over the domain for Step 1. The colors indicate + the magnitude of the displacement and the arrows indicate the + direction with the length of each arrow equal to 10,000 times the + magnitude of the displacement.} + \label{fig:example:subduction:3d:step01} \end{figure} \subsubsection{Exercises} -% Algebraic multigrid preconditioner -% Adjust material properties (stiffer, softer, nearly incompressible) -% Pure shear instead of axial compression -\subsection{Step 2: Postseismic Relaxation} +\begin{itemize} +\item Run PyLith again and add + \filename{solver\_algebraicmultigrid.cfg} as an argument on the + command line to switch to the + algebraic multigrid preconditioner. + \begin{itemize} + \item Using the PETSc log summary to compare the runtime and + memory use between the original LU preconditiner and the ML + algebraic multigrid preconditioner. Hint: The algebraic + multigrid preconditioner is faster. + \item Run the simulation again with the algebraic multigrid + preconditioner using multiple cores via the + \commandline{-{}-nodes=NCORES} argument, replacing + \commandline{NCORES} with 2 or up to the number of cores on your + machine. Examine the PETSc log summary for the various runs to + see how the time spent at varies stages changes with the number + of cores. Make a plot of runtime versus the number of + cores. + \end{itemize} +\item Adjust the material properties in the spatial databases so that the slab is stiffer and + the wedge is more compliant. What happens to the solution if you make the + materials nearly incompressible? Does this also affect the rate of + convergence of the linear solve? +\item Change the Dirichlet boundary conditions to impose pure shear + instead of axial compression. Hint: You will need to change the + boundary conditions on the east, west, north, and south + boundaries. +\end{itemize} + + +\subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \subsubsection{Exercises} @@ -304,7 +482,7 @@ \subsubsection{Exercises} % Slip on lower slab and splay fault % Slip on slab and splay fault -\subsection{Step 3: Interseismic Deformation} +\subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \subsubsection{Exercises} @@ -383,7 +561,8 @@ \subsection{Step 6: Prescribed Slow-Slip Event} contours of the applied slip at t = 24 days. \begin{figure} - \includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} + %\includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} + ADD FIGURE HERE \caption{Solution for Step 6. The colors indicate the vertical displacement, the vectors represent the horizontal displacements at simulated cGPS sites, and the contours represent the applied @@ -409,7 +588,7 @@ \subsubsection{Exercises} \end{itemize} \end{itemize} -\subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} +\subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} This example is essentially a three-dimensional analog of {sec:example:greensfns2d}, and is a more realistic example of how @@ -421,19 +600,19 @@ \subsection{Step 7: Inversion of Slow-Slip using 3D Green's Functions} inverse approach described in {sec:example:greensfns2d}. We first generate the synthetic data by using the script -\filename{make_synthetic_gpsdisp.py} in the top-level directory. This -script reads the parameters in \filename{make_synthetic_gpsdisp.cfg} +\filename{make\_synthetic\_gpsdisp.py} in the top-level directory. This +script reads the parameters in \filename{make\_synthetic\_gpsdisp.cfg} to generate synthetic data from the selected time step with a specified amount of noise. Run this script as: \begin{shell} $$ ./make_synthetic_gpsdisp.py \end{shell} This will create the following files: -\begin{itemize} -\item \filename{cgps_synthetic_displacement.txt}: Read by the +\begin{description} +\item[\filename{cgps\_synthetic\_displacement.txt}] read by the inversion script. -\item \filename{cgps_synthetic_displacement.vtk}: For visualization. -\end{itemize} +\item[\filename{cgps\_synthetic\_displacement.vtk}] for visualization. +\end{description} After we generate the synthetic data, we generate the Green's functions. We divide the Green's function generation into two sub-problems: @@ -479,7 +658,7 @@ \subsubsection{Exercises} % Adjust noise level % Invert for slip at each time step -\subsection{Step 8: Gravitational Body Forces} +\subsection{Step 8: Stress Field Due to Gravitational Body Forces} % End of file From 0b2fa82aedc07faf4fb9c1d6b3733775ce4ee55d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 10:19:46 -0700 Subject: [PATCH 101/216] Improve display of vectors in plot_dispvec and add ability to save screenshot. --- examples/3d/subduction/viz/plot_dispvec.py | 20 ++++++++++++++++++++ 1 file changed, 20 insertions(+) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 131ec51bb4..46e5e2b28e 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -75,11 +75,18 @@ def visualize(sim, dispScale): glyph.ScaleFactor = dispScale glyph.ScaleMode = "vector" glyph.GlyphMode = "All Points" + glyph.GlyphType.TipRadius = 0.2 + glyph.GlyphType.ShaftRadius = 0.05 glyphDisplay = Show(glyph, view) glyphDisplay.Representation = "Surface" view.ResetCamera() + + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.ViewSize = [960, 540] Render() @@ -91,9 +98,19 @@ def visualize(sim, dispScale): parser = argparse.ArgumentParser() parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--vector-scale", action="store", type=float, dest="scale", default=DISPLACEMENT_SCALE) + parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() visualize(args.sim, args.scale) + + view = GetRenderView() + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.ViewSize = [960, 540] + if args.screenshot: + WriteImage(args.screenshot) + Interact() else: @@ -101,5 +118,8 @@ def visualize(sim, dispScale): visualize(SIM_NAME, DISPLACEMENT_SCALE) + Render() + + # End of file From 539f659e5b86b576eaa89eb1e7b8fc64276966b7 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 11:09:18 -0700 Subject: [PATCH 102/216] Small cleanup of plot_dispvec.py script. --- examples/3d/subduction/viz/plot_dispvec.py | 8 -------- 1 file changed, 8 deletions(-) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 46e5e2b28e..5c420ceb8e 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -82,12 +82,6 @@ def visualize(sim, dispScale): glyphDisplay.Representation = "Surface" view.ResetCamera() - - view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] - view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] - view.CameraViewUp = [0.0, 0.0, 1.0] - view.ViewSize = [960, 540] - Render() # ---------------------------------------------------------------------- @@ -118,8 +112,6 @@ def visualize(sim, dispScale): visualize(SIM_NAME, DISPLACEMENT_SCALE) - Render() - # End of file From 8a52959e4ad8bb9386c3c651787f6e975deca143 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 11:09:35 -0700 Subject: [PATCH 103/216] Add information on ParaView Python script. --- doc/userguide/examples/subduction3d.tex | 66 ++++++++++++++++++++++--- 1 file changed, 58 insertions(+), 8 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index b54ac83a0f..fd806c46f4 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -6,7 +6,7 @@ \subsection{Overview} This suite of examples demonstrates use of a wide variety of features and the general workflow often used in research simulations. We base the model on the Cascadia subduction zone -(Figure~\ref{fig:example:subduction:3d:cascadia}). These examples will +(Figure~\vref{fig:example:subduction:3d:cascadia}). These examples will focus on modeling the deformation associated with the the subducting slab, including interseismic deformation with aseismic slip (creep) and viscoelastic relaxation, coseismic slip on the slab interface and @@ -30,7 +30,7 @@ \subsection{Overview} \label{fig:example:subduction:3d:cascadia} \end{figure} -Figure~\ref{fig:example:subduction:3d:concept} shows our conceptual +Figure~\vref{fig:example:subduction:3d:concept} shows our conceptual model with a slab, mantle, continental crust, and accretionary wedge. We cut off the slab at a depth of 100 km. We use a transverse geographic projection coordinate system with Portland, Oregon, as the @@ -65,7 +65,7 @@ \subsection{Overview} \subsection{Features Illustrated} -Table~\ref{tab:example:subduction:3d:features} lists the features +Table~\vref{tab:example:subduction:3d:features} lists the features discussed in each of these 3-D subduction zone examples. With the intent of illustrating features used in research simulations, we use HDF5 output and, we make extensive use the most efficient @@ -316,7 +316,7 @@ \subsection{Step 1: Axial Compression} We start with a very simple example of axial compression in the east-west direction with purely elastic material properties, and no -faults (Figure~\ref{fig:example:subduction:3d:step01:diagram}). We +faults (Figure~\vref{fig:example:subduction:3d:step01:diagram}). We impose axial compression using Dirichlet boundary conditions on the east (+x) and west (-x) boundaries and confine the domain in the north-south direction via zero displacement Dirichlet boundary @@ -364,7 +364,7 @@ \subsection{Step 1: Axial Compression}

db_initial.data

= [-2.0*m] \end{cfg} -As discussed in Section~\ref{sec:example:subduction:3d:organization}, +As discussed in Section~\vref{sec:example:subduction:3d:organization}, we use \filename{mat\_elastic.cfg} to specify the parameters associated with linear, isotropic elastic bulk constitutive models for all of the materials for convenient reuse across several different @@ -427,9 +427,14 @@ \subsection{Step 1: Axial Compression} (two pairs of files), and physical properties, stress, and strain within each material (eight pairs of files). -Figure \vref{fig:example:subduction:3d:step01}, which was created using -ParaView, displays the magnitude of the displacement field with the -deformation exaggerated by a factor of 1000. +Figure \vref{fig:example:subduction:3d:step01}, which was created +using the ParaView Python script \filename{plot\_dispvec.py}, displays +the magnitude of the displacement field arrows showing the direction +and magnitude of the deformation. Material properties with a positive +Poisson's ratio result in vertical deformation along with the axial +compression. The variations in material properties among the +properties result in local spatial variations that are most evident in +the horizontal displacement components. \begin{figure} \includegraphics[width=5.0in]{examples/figs/subduction3d_step01_soln} @@ -441,6 +446,51 @@ \subsection{Step 1: Axial Compression} \end{figure} +There are three different ways you can run this Python script to view +the solution: +\begin{enumerate} +\item From a shell (terminal window) start ParaView via the command line from the + \filename{examples/3d/subduction} directory. Within the ParaView GUI, select + \object{Tools}$\rightarrow$\object{Python Shell}, click on the + \object{Run Script} button, and navigate to the \filename{viz} + directory and select the \filename{plot\_dispvec.py} file. + +\item From a shell (terminal window) start ParaView via the command line from the + \filename{examples/3d/subduction} directory adding the + \filename{-{}-script=viz/plot\_dispvec.py} command line argument. +\begin{shell} +# Make sure you are in the examples/3d/subduction directory. +$$ PATH_TO_PARAVIEW/paraview --script=viz/plot_dispvec.py +\end{shell} +\item Run the ParaView Python script directly from a shell (terminal + window) via the command line. You can use command line arguments to + set user-specified parameters. +\begin{shell} +# Make sure you are in the examples/3d/subduction directory. +# We show the optional command line arguments in square brackets. +$$ ./viz/plot_dispvec.py [--vector-scale=10.0e+4] [--sim=step01.cfg} [--screenshot=FILE] +\end{shell} +\end{enumerate} + +\tip{Running the ParaView Python script from within the ParaView GUI + allows further manipulation of the data, which is not possible when + running the ParaView Python script outside the ParaView + GUI.} + +\tip{In order to change the user-specified parameters in the ParaView + Python scripts when running them from within the ParaView GUI, you + must edit the file in an external text editor before running the + script. If you are running these script from outside the ParaView + GUI, you can simply use command line argument to change the + user-specified parameters.} + +\important{The ParaView Python scripts run Python via + \filename{pvpython}, which is a customized version of the Python + interpreter included in the ParaView distribution. This is different + from Python provided with your operating system and the one included + in the PyLith distribution.} + + \subsubsection{Exercises} From 124a194b25a5882eddfeef2a60c56691f54d783f Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 09:09:16 +1200 Subject: [PATCH 104/216] Added figure for step06. --- .../examples/figs/subduction3d_step06_soln.png | Bin 0 -> 69240 bytes 1 file changed, 0 insertions(+), 0 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_step06_soln.png diff --git a/doc/userguide/examples/figs/subduction3d_step06_soln.png b/doc/userguide/examples/figs/subduction3d_step06_soln.png new file mode 100644 index 0000000000000000000000000000000000000000..59c7795b45eb84481e75bfba28e361546f036f68 GIT binary patch literal 69240 zcmY(qWl&sQ+cY{zU~rey9a^=ch}&0cJAl>ew?bQ zp=xT_v)9^}bobROLPbd$1(5&|1OlPR%1EezK(HJj5VS5B8u&!u=&E?hKzs8$I zRHV?qFy*^+a=mC!y5oCb*1g?Hn8GJzdcH}LfhxO?zRBc9Em2~~Ru~hgCEW6L!d>7G 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zRF%V+5si{zmX_(pd1~eEOXjD>@>cOIlVxy()@bL48v;!gFh7ntg!jZ0TWXuTYK~ ze-Z%`qLH=d`Im7V5gaZv|3hoyI~e)nY12r??6@=#$it+A?PLqUwkZLiu%3evYJtbW zf+V0HWPn`h)g{hmL}y&}JOPvpE^!0{$QS$SupsI=oX57V;HT!dc4Sn`3lg*xDuSWX z%harct2!1K^AVQ^M&W=a>RG;E0m=N^0u{jjqMm`=$DHWwj$br?_zDBW$F1kczTqJA zhoZD8pz}k*phIJa%@$GDEWo0Semcd?EQM;iH>+>v(94mPz^g9|+slCa;|XOm$$xqK zoQJtP9`H)V{Z-7~FBvx7l7vewka>3Wwc~m^)i))>(0E0oWUvV)AwRatCY0~x z6AJ*vgyiz&W{<_)jzWs7pT_){9zJ)U+7xiSFdk!$#c3FGi?`ed3`G<;o2Y^Nzf~dt z@dp9Rm9PT+x5}G|A$LJ6@t6LB9e`!%4447w$KTkMpPloox5g_0!`FlgD)*6x6a+%! zQoI7u;up2wT#60)eiJg?L=|E&z_6XzViS3TbpPi^XP6#rJ#G6R6d?8GVs`j?Zo$oe ba~6QDh#fEg(kOie?gPQ36eJ5I^!@)on>F7U literal 0 HcmV?d00001 From 6a9083ca831f48f8bcf9fdcf335f836b0a939f69 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 14:13:42 -0700 Subject: [PATCH 105/216] Started work on documentation for Step 2. --- doc/userguide/examples/subduction3d.tex | 172 +++++++++++++++++++++++- 1 file changed, 170 insertions(+), 2 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index fd806c46f4..52295dda67 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1,6 +1,7 @@ \section{Examples for a 3D Subduction Zone} \label{sec:example:subduction:3d} +% ---------------------------------------------------------------------- \subsection{Overview} This suite of examples demonstrates use of a wide variety of features @@ -63,6 +64,7 @@ \subsection{Overview} \end{description} +% ---------------------------------------------------------------------- \subsection{Features Illustrated} Table~\vref{tab:example:subduction:3d:features} lists the features @@ -81,6 +83,7 @@ \subsection{Features Illustrated} \input{examples/subduction3d_features} \end{table} +% ---------------------------------------------------------------------- \subsection{Generating the Finite-Element Mesh} We use CUBIT/Trelis to generate the finite-element mesh. Due to its @@ -220,8 +223,14 @@ \subsubsection{Materials} cell determines the type of basis functions we use in the discretization. This means we can specify this information in the \filename{pylithapp.cfg} file and avoid duplicating it in each -simulation parameter file. For eacmple for the slab, the parameters include +simulation parameter file. To set up the materials, we first create an +aray of materials that defines the name for each material component. +For example, we create the array of four materials and then set the +parameters for the slab: \begin{cfg} +[pylithapp.problem] +materials = [slab, wedge, crust, mantle] + [pylithapp.problem.materials.slab]

label

= Subducting slab ; Label for informative error messages

id

= 1 ; Block id in ExodusII file from CUBIT/Trelis @@ -311,6 +320,7 @@ \subsubsection{Solver Parameters} system Jacobian matrix and our custom fault preconditioner to the Lagrange multiplier portion. +% ---------------------------------------------------------------------- \subsection{Step 1: Axial Compression} \label{sec:example:subduction:3d:step01} @@ -335,7 +345,7 @@ \subsection{Step 1: Axial Compression} \draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); \end{scope} \end{tikzpicture} - \caption{Diagram of axial compression example. This static + \caption{Diagram of Step 1: Axial compression. This static simulation uses Dirichlet boundary conditions with axial compression in the east-west (x-direction), roller boundary conditions on the north, south, and bottom boundaries, and purely @@ -524,7 +534,151 @@ \subsubsection{Exercises} \end{itemize} +% ---------------------------------------------------------------------- \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} +\label{sec:example:subduction:3d:step02} + +In this example we model the postseismic relaxation of the deep slab +and mantle resulting from coseismic slip on a fault patch in the +central portion of the subduction (top of the slab) interface. For +simplicity we will prescribed uniform slip on the fault patch and use +a linear Maxwell viscoelastic constitutive models for the slab and +mantle. As the lateral and bottom boundaries are far from the +earthquake source, we use roller boundary conditions on these +boundaries. We do not expect significant relaxation of stresses on the +shallow part of the slab, so we impose a depth-dependent +viscosity. Figure~\ref{fig:example:subduction:3d:step02:diagram} +summarizes the problem description. + +\todo{brad}{Add annotation to figure.} +\begin{figure}[htbp] + \begin{tikzpicture} + \tikzstyle{annotation} = [black]; + \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; + %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); + %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); + \end{scope} + \end{tikzpicture} + \caption{Diagram of Step 2: Prescribed coseismic slip and + postseismic relaxation. This quasistatic simulation prescribes + uniform slip on the central rupture patch on the top of the slab, + depth-dependent viscoelastic relaxation in the slab and mantle, + and roller boundary conditions on the lateral (north, south, east, + and west) and bottom boundaries.} + \label{fig:example:subduction:3d:step02:diagram} +\end{figure} + +The \filename{pylithapp.cfg} completely specifies the Dirichlet roller +boundary conditions on the five boundaries, so we do not include any +boundary condition information in \filename{step02.cfg}. As discussed +in Section~\vref{sec:example:subduction:3d:organization}, we bundle +the parameters for specification of an elastic crust and wedge and +viscoelastic slab and mantle in \filename{mat\_viscoelastic.cfg}. + +% Materials +We describe the properties of the linear, isotropic Maxwell +viscoelastic constitutive model using viscosity in addition to the Vp, +Vs, and density used to describe purely linear, isotropic elastic +models. Rather than create a database with all four of these +parameters, we leverage the \object{SimpldDB} spatial databases used +by \filename{mat\_elastic.cfg} for the elastic properties and simply +create a single new spatial database with the depth-dependent +viscosity for the slab and mantle. We use the \object{CompositeDB} +spatial database to combine these two spatial databases into a single +spatial database with the material properties. Rather than using a +\object{SimpleDB} for the depth-dependent viscosity, we use a +\object{SimpleGridDB} spatial database +(\filename{spatialdb/mat\_viscosity}), which provides faster +interpolation using a bilinear search algorithm along each coordinate +direction. We use a very large viscosity at depths above 20 km to give +behavior that is essentially elastic and decrease it so the Maxwell +relaxation time (viscosity divided by the shear modulus) is +approximately 200 years at a depth of 30 km, 100 years at a depth of +100 km, and 50 years at a depth of 400 km. Using linear interpolation +results in a piecewise linear variation in the viscosity with depth. + +\tip{The \object{SimpleGridDB} should be used whenever the points in a + spatial database can be described with a logically rectangular + grid. The grid points along each direction do not need to be + uniformly spaced.} + +In setting the parameters for the \object{CompositeDB} in +\filename{mat\_viscoelastic.cfg}, we specify which properties are +contained in each of the two spatial databases in the composite +database and the type and parameters for each of those spatial +databases. For the slab we have: +\begin{cfg} +[pylithapp.problem.materials.slab] +db_properties = spatialdata.spatialdb.CompositeDB +

db_properties.label

= Composite spatial database for slab material properties + +[pylithapp.timedependent.materials.slab.db_properties] +# Elastic properties +

values_A

= [density, vs, vp] +db_A = spatialdata.spatialdb.SimpleDB +

db_A.label

= Elastic properties +

db_A.iohandler.filename

= spatialdb/mat_slab_elastic.spatialdb + +# Viscoelastic properties +

values_B

= [viscosity] +db_B = spatialdata.spatialdb.SimpleGridDB +

db_B.label

= Linear Maxwell viscoelatic properties +

db_B.filename

= spatialdb/mat_viscosity.spatialdb +

db_B.query_type

= linear +\end{cfg} + +In the simulation specific parameter file \filename{step02.cfg}, we +specify the parameters for the quasistatic time stepping, the +coesismic rupture, and the filenames for output. By default, PyLith +will use implicit time stepping with uniform time steps, so we need +only specify the duration and time step size. +\begin{cfg} +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +

total_time

= 200.0*year +

dt

= 10.0*year +\end{cfg} + +In prescribing coseismic slip, we need to create an array of one fault +interface and then set its parameters. Because the central fault patch +contains edges of the fault buried within the domain, we need to +specify the nodeset that corresponds to the entire fault surface as +well as the nodeset that corresponds to the buried edges. This ensures +that PyLith inserts the cohesive cells and properly terminates the +fault surface at the edges. We must also set the discretization +information for the fault. +\begin{cfg} +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveKin ; Default + +[pylithapp.problem.interfaces.slab] +

label

= fault_slabtop_patch ; Nodeset for entire fault surface +

edge

= fault_slabtop_patch_edge ; Nodeset for buried edges + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

quadrature.cell.dimension

= 2 +\end{cfg} +Just as we do for the boundary conditions and materials, we create an +array of components (in this case an array of one fault, +\facility{slab}, and then refer to those components by name, for +example \facility{pylithapp.problem.interfaces.slab}. + + +We run this example by typing +\begin{shell} +$$ pylith step02.cfg mat_viscoelastic.cfg +\end{shell} + \subsubsection{Exercises} @@ -532,10 +686,20 @@ \subsubsection{Exercises} % Slip on lower slab and splay fault % Slip on slab and splay fault +\begin{itemize} +\item +\end{itemize} + + + + + +% ---------------------------------------------------------------------- \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \subsubsection{Exercises} +% ---------------------------------------------------------------------- \subsection{Step 4: Prescribed Earthquake Cycle} \subsubsection{Exercises} @@ -547,10 +711,12 @@ \subsubsection{Exercises} +% ---------------------------------------------------------------------- \subsection{Step 5: Spontaneous Rupture Driven by Subducting Slab} \subsubsection{Exercises} +% ---------------------------------------------------------------------- \subsection{Step 6: Prescribed Slow-Slip Event} This example simulates a simple slow slip event (SSE) that remains @@ -638,6 +804,7 @@ \subsubsection{Exercises} \end{itemize} \end{itemize} +% ---------------------------------------------------------------------- \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} This example is essentially a three-dimensional analog of @@ -708,6 +875,7 @@ \subsubsection{Exercises} % Adjust noise level % Invert for slip at each time step +% ---------------------------------------------------------------------- \subsection{Step 8: Stress Field Due to Gravitational Body Forces} From e07243d47b1f9b32a46beb72d521df82642d0e7b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 16:10:18 -0700 Subject: [PATCH 106/216] Add time annotation to ParaView Python scripts. --- examples/3d/subduction/viz/plot_dispvec.py | 18 ++++++++++-- examples/3d/subduction/viz/plot_dispwarp.py | 28 ++++++++++++++++-- .../subduction/viz/plot_faultslip-reltract.py | 17 ++++++++++- examples/3d/subduction/viz/plot_faultslip.py | 29 +++++++++++++++++-- 4 files changed, 84 insertions(+), 8 deletions(-) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 5c420ceb8e..2e3176d946 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -39,7 +39,7 @@ from paraview.simple import * import os -def visualize(sim, dispScale): +def visualize(sim, dispScale, showFinalTimeStep=False): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -53,6 +53,8 @@ def visualize(sim, dispScale): scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() + if showFinalTimeStep: + scene.GoToLast() view = GetActiveViewOrCreate('RenderView') # Show undeformed domain, colored by magnitude of displacement vector. @@ -80,8 +82,18 @@ def visualize(sim, dispScale): glyphDisplay = Show(glyph, view) glyphDisplay.Representation = "Surface" + + # Annotate time + tstamp = AnnotateTimeFilter(dataDomain) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 view.ResetCamera() + view.Update() Render() # ---------------------------------------------------------------------- @@ -95,13 +107,15 @@ def visualize(sim, dispScale): parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.scale) + visualize(args.sim, args.scale, showFinalTimeStep=True) view = GetRenderView() view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] view.CameraViewUp = [0.0, 0.0, 1.0] view.ViewSize = [960, 540] + view.Update() + if args.screenshot: WriteImage(args.screenshot) diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index e14ce67cf6..8714b97024 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -35,7 +35,7 @@ from paraview.simple import * import os -def visualize(sim, exaggeration): +def visualize(sim, exaggeration, showFinalTimeStep=False): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -49,6 +49,9 @@ def visualize(sim, exaggeration): scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() + if showFinalTimeStep: + scene.GoToLast() + view = GetActiveViewOrCreate('RenderView') # Gray wireframe for undeformed domain. @@ -73,6 +76,15 @@ def visualize(sim, exaggeration): # Update a scalar bar component title. UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) + # Annotate time + tstamp = AnnotateTimeFilter(warp) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 + view.ResetCamera() view.Update() Render() @@ -85,9 +97,21 @@ def visualize(sim, exaggeration): parser = argparse.ArgumentParser() parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) + parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.exaggeration) + visualize(args.sim, args.exaggeration, showFinalTimeStep=True) + + view = GetRenderView() + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.ViewSize = [960, 540] + view.Update() + + if args.screenshot: + WriteImage(args.screenshot) + Interact() else: diff --git a/examples/3d/subduction/viz/plot_faultslip-reltract.py b/examples/3d/subduction/viz/plot_faultslip-reltract.py index 8824df70da..92f9855fc3 100755 --- a/examples/3d/subduction/viz/plot_faultslip-reltract.py +++ b/examples/3d/subduction/viz/plot_faultslip-reltract.py @@ -101,7 +101,14 @@ def visualize(sim, faults): contourDisplay = Show(contour, view) - + # Annotate time + tstamp = AnnotateTimeFilter(dataDomain) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 view.ResetCamera() view.Update() @@ -122,6 +129,14 @@ def visualize(sim, faults): else: faults = FAULTS visualize(args.sim, faults) + + view = GetRenderView() + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.ViewSize = [960, 540] + view.Update() + Interact() else: diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py index 2d82c32eb6..9fb7b9e2b9 100755 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -28,7 +28,7 @@ # pvpython. # Root name for simulation. -SIM_NAME = "step06" +SIM_NAME = "step02" # Names of faults for output files. FAULTS = ["fault-slab"] @@ -37,7 +37,7 @@ from paraview.simple import * import os -def visualize(sim, faults): +def visualize(sim, faults, showFinalTimeStep=False): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -50,6 +50,8 @@ def visualize(sim, faults): scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() + if showFinalTimeStep: + scene.GoToLast() view = GetActiveViewOrCreate('RenderView') # Gray wireframe for undeformed domain. @@ -81,6 +83,15 @@ def visualize(sim, faults): # Update a scalar bar component title. UpdateScalarBarsComponentTitle(slipLUT, faultDisplay) + # Annotate time + tstamp = AnnotateTimeFilter(dataDomain) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 + view.ResetCamera() view.Update() Render() @@ -93,13 +104,25 @@ def visualize(sim, faults): parser = argparse.ArgumentParser() parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--faults", action="store", dest="faults") + parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() if args.faults: faults = args.faults.split(",") else: faults = FAULTS - visualize(args.sim, faults) + visualize(args.sim, faults, showFinalTimeStep=True) + + view = GetRenderView() + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.ViewSize = [960, 540] + view.Update() + + if args.screenshot: + WriteImage(args.screenshot) + Interact() else: From 5de1a9838d0a47a04690cf8f0f9bb7f98537cabb Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 16:10:33 -0700 Subject: [PATCH 107/216] Add more comments to step02. --- examples/3d/subduction/step02.cfg | 8 ++++---- 1 file changed, 4 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index 9caf057961..bbeaf204f5 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -73,11 +73,11 @@ dt = 10.0*year interfaces = [slab] [pylithapp.problem.interfaces] -slab = pylith.faults.FaultCohesiveKin +slab = pylith.faults.FaultCohesiveKin ; Default [pylithapp.problem.interfaces.slab] -label = fault_slabtop_patch -edge = fault_slabtop_patch_edge +label = fault_slabtop_patch ; Nodeset for the entire fault surface +edge = fault_slabtop_patch_edge ; Nodeset for the buried edges # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). @@ -99,7 +99,7 @@ slip_time.data = [9.999*year] [pylithapp.problem.interfaces.slab.output] writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step02-fault-slab.h5 -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture, slip_time_rupture] # ---------------------------------------------------------------------- # output From 953902ddd4ffea3ea2b23ce2cc35efaaad4fd63c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 16:10:54 -0700 Subject: [PATCH 108/216] Finish adding step02. --- doc/userguide/examples/subduction3d.tex | 89 +++++++++++++++++++------ 1 file changed, 68 insertions(+), 21 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 52295dda67..0f047b5fdc 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -643,14 +643,17 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation}

dt

= 10.0*year \end{cfg} -In prescribing coseismic slip, we need to create an array of one fault -interface and then set its parameters. Because the central fault patch -contains edges of the fault buried within the domain, we need to -specify the nodeset that corresponds to the entire fault surface as -well as the nodeset that corresponds to the buried edges. This ensures -that PyLith inserts the cohesive cells and properly terminates the -fault surface at the edges. We must also set the discretization -information for the fault. +In prescribing coseismic slip on the single fault patch, we create an +array with one fault interface and then set its parameters. Because +the edges of the central fault patch are buried within the domain, we +need to specify the nodeset that corresponds to the buried edges as +well as the nodeset for the entire fault surface. This ensures that +PyLith inserts the cohesive cells and properly terminates the fault +surface at the edges. Just as we do for the boundary conditions and +materials, we create an array of components (in this case an array +with one fault interface, \facility{slab}, and then refer to those +components by name, \facility{pylithapp.problem.interfaces.slab}. We +must also set the discretization information for the fault. \begin{cfg} [pylithapp.problem] # We prescribe slip on the slab fault patch. @@ -668,30 +671,74 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} quadrature.cell = pylith.feassemble.FIATSimplex

quadrature.cell.dimension

= 2 \end{cfg} -Just as we do for the boundary conditions and materials, we create an -array of components (in this case an array of one fault, -\facility{slab}, and then refer to those components by name, for -example \facility{pylithapp.problem.interfaces.slab}. +Prescribing the coseismic slip distribution on the fault involves +specifying an origin time for the rupture (default is 0.0), and a slip +time function along with its +parameters. In this case, we treat the earthquake rupture as just the +coseismic slip happening in one time step, so we use a step function +for the slip time function (which is the default). The parameters +include the final slip and slip initiation time. Because we want +uniform slip and a uniform rise time, we use \object{UniformDB} +spatial databases for both of these. Note that we specify oblique slip +with 1.0 m of right-lateral motion and 4.0 m of reverse motion. +\begin{cfg} +[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.UniformDB +

slip.label

= Final slip +

slip.values

= [left-lateral-slip, reverse-slip, fault-opening] +

slip.data

= [-1.0*m, 4.0*m, 0.0*m] + +slip_time = spatialdata.spatialdb.UniformDB +

slip_time.label

= Slip initiation time +

slip_time.values

= [slip-time] +

slip_time.data

= [9.999*year] ; Use 10*year-small value to account for roundoff errors + +[pylithapp.problem.interfaces.slab.output] +writer = pylith.meshio.DataWriterHDF5 +

writer.filename

= output/step02-fault-slab.h5 +

vertex_info_fields

= [normal_dir, strike_dir, dip_dir, final_slip_rupture, slip_time_rupture] +\end{cfg} We run this example by typing \begin{shell} -$$ pylith step02.cfg mat_viscoelastic.cfg +$$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} +Figure \vref{fig:example:subduction:3d:step02}, which was created +using the ParaView Python script \filename{plot\_dispwarp.py}, displays +the magnitude of the displacement field exaggerated by a factor of 10,000. +The shallow fault results in deformation that is localized over a +small region. + +\begin{figure} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step02_soln} + \caption{Solution over the domain for Step 2 at t=200*yr. The colors indicate + the magnitude of the displacement and we have exaggerated the + deformation by a factor of 10,000.} + \label{fig:example:subduction:3d:step02} +\end{figure} -\subsubsection{Exercises} -% Change slip on slab to slip on splay fault -% Slip on lower slab and splay fault -% Slip on slab and splay fault +\subsubsection{Exercises} \begin{itemize} -\item +\item Change the slip from the top of the slab to the splay fault + rupture patch. Hint: Identify the nodesets for the splay fault + patch. +\item Create simulataneous rupture on the central patch for the splay + fault and top of the slab. +\item Prescribe coseismic slip on the central patch for splay fault + and the top of the slab below the intersection with the splay fault. + \begin{itemize} + \item Implement this without changing the any of the nodesets. Hint: + You will need to create two fault interfaces. What do you notice + about the slip at the intersection between the splay fault and slab? + \item Add nodesets in CUBIT/Trelis to create a uniform coseismic + slip distribution across the splay fault and on the slab interface + below the splay fault. + \end{itemize} \end{itemize} - - - % ---------------------------------------------------------------------- From c8779b28309728c40fc7a1b66ca81a48d1dfa246 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 16:11:40 -0700 Subject: [PATCH 109/216] Raise depth at which viscosity drops. --- .../3d/subduction/spatialdb/mat_viscosity.spatialdb | 12 +++++++----- 1 file changed, 7 insertions(+), 5 deletions(-) diff --git a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb index e8f7562190..2168611ea0 100644 --- a/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb +++ b/examples/3d/subduction/spatialdb/mat_viscosity.spatialdb @@ -4,7 +4,8 @@ // // The rough variation of Maxwell relaxation time with depth is // 0 km: 10,000 years (essentially elastic) -// -50 km: 5,000 years (essentially elastic) +// -20 km: 5,000 years (essentially elastic) +// -30 km: 200 years // -100 km: 100 years // -400 km: 50 years // @@ -12,13 +13,13 @@ SimpleGridDB { num-x = 1 num-y = 1 - num-z = 4 + num-z = 5 num-values = 1 space-dim = 3 value-names = viscosity value-units = Pa*s cs-data = geo-projected { - to-meters = 1.0e3 + to-meters = 1.0e+3 ellipsoid = WGS84 datum-horiz = WGS84 datum-vert = mean sea level @@ -40,10 +41,11 @@ SimpleGridDB { 0.0 // z coordinates -0.0 -50.0 -100.0 -400.0 +0.0 -20.0 -30.0 -100.0 -400.0 // z viscosity 0.0 0.0 0.0 1.0e+22 -0.0 0.0 -50.0 8.0e+21 +0.0 0.0 -20.0 1.0e+21 +0.0 0.0 -30.0 4.0e+20 0.0 0.0 -100.0 2.0e+20 0.0 0.0 -400.0 1.0e+20 From 18c98f1721dd8a49676d28c8817679be2fe809f1 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 16:11:57 -0700 Subject: [PATCH 110/216] Add figure for step02. --- 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00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 11:43:41 +1200 Subject: [PATCH 111/216] Added some more details for step06. --- doc/userguide/examples/subduction3d.tex | 181 ++++++++++++++++++++---- 1 file changed, 150 insertions(+), 31 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 52295dda67..f4413dce3e 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -719,15 +719,15 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 6: Prescribed Slow-Slip Event} -This example simulates a simple slow slip event (SSE) that remains -fixed spatially but increases its amplitude with time. We assume a -constant rake angle of 110 degrees, and a time duration of 30 -days. This problem requres the use of both a spatial database to -provide the spatial distribution of slip, and a temporal database to -describe the time evolution of slip. To create these databases we -provide the \filename{generate\_slowslip.py} script, which is in the -\filename{spatialdb} directory. Once you are in the -\filename{spatialdb} directory, run the script as follows: +This example simulates a simple slow slip event (SSE) on the +subduction interface that remains fixed spatially but increases its +amplitude with time. We assume a constant rake angle of 110 degrees, +and a time duration of 30 days. This problem requres the use of both a +spatial database to provide the spatial distribution of slip, and a +temporal database to describe the time evolution of slip. To create +these databases we provide the \filename{generate\_slowslip.py} +script, which is in the \filename{spatialdb} directory. Once you are +in the \filename{spatialdb} directory, run the script as follows: \begin{shell} $$ ./generate_slowslip.py \end{shell} @@ -740,25 +740,144 @@ \subsection{Step 6: Prescribed Slow-Slip Event} \item \filename{fault\_slabtop\_slowslip.timedb}: Temporal database \end{itemize} -Once the database files have been generated, it is possible to run the -example. Parameter settings that augment those in pylithapp.cfg are -contained in the file \filename{step06.cfg}. These settings are: -\begin{inventory} - \facilityitem{pylithapp.timedependent.formulation.time\_step}{Adjust - the total simulation time to 30 days with a time step size of 2 days.} - \facilityitem{pylithapp.timedependent.formulation}{Specify output - for the domain, for the ground surface, and for a set of - simulated cGPS sites.} - \facilityitem{pylithapp.timedependent.interfaces.slab}{Specify the - spatial distribution of slip and the temporal evolution of slip on - the slab interface. We change the slip function from the default - to a time history slip function to make use of the temporal database.} - \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the - base filenames for HDF5 output for all output types (for example, - \filename{step06-domain.h5}). Note that for cGPS output we need to - provide coordinate system information as well as the name of a - text file providing cGPS site locations.} -\end{inventory} +Note that \filename{fault\_slabtop\_slowslip.spatialdb} is a +\facility{SimpleGridDB}. This type of spatial database is very +efficient in cases where property values lie on a regular grid in 2 or +3 dimensions, since searches and interpolations reduce to a set of 1D +operations. Once the database files have been generated, it is +possible to run the example. There are a number of parameters that are +changed from or added to those in \filename{pylithapp.cfg}. We first +change the total simulation time to 30 days with a time step size of 2 +days: +\begin{cfg} +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +

    total_time

    = 30.0*day +

    dt

    = 2.0*day +\end{cfg} + +The results in this example will be used to simulate output at cGPS +stations for example step07, so we modify the output manager to +provide output at synthetic cGPS stations as well as the entire domain +and ground surface: +\begin{cfg} +# For this problem, we want output over the entire domain, for the +# ground surface, and at simulated cGPS locations. +[pylithapp.problem.implicit] +output = [domain, subdomain, cgps_sites] + +# Default output is for the entire domain. +# We need to set the type of output for the subdomain and points. +output.subdomain = pylith.meshio.OutputSolnSubset +output.cgps_sites = pylith.meshio.OutputSolnPoints +\end{cfg} + +There are a number of parameters to change/modify related to the +fault. In particular, we change the default slip function to +\facility{pylith.faults.TimeHistorySlipFn}, which allows us to change +the slip amplitude as a function of time. We also use a +\facility{SimpleGridDB} to specify fault slip and linear interpolation +for the fault slip: +\begin{cfg} +[pylithapp.problem] +# We prescribe slip on the slab fault patch. +interfaces = [slab] + +[pylithapp.problem.interfaces] +slab = pylith.faults.FaultCohesiveKin + +[pylithapp.problem.interfaces.slab] +# Nodeset corresponding to the fault patch and buried edge. +

    label

    = fault_slabtop_patch +

    edge

    = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

    quadrature.cell.dimension

    = 2 + +# We use a time history slip function. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture] +slip_function = pylith.faults.TimeHistorySlipFn + +# The slip is defined in a spatial database. +[pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +

    slip.label

    = Gaussian slip distribution for SSE +

    slip.filename

    = spatialdb/fault_slabtop_slowslip.spatialdb + +# Use linear interpolation. +

    slip.query_type

    = linear + +# We use a UniformDB to specify the slip initiation time. +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] + +# We use a temporal database to provide the slip time history. +

    time_history.label

    = Time history of slip +

    time_history.filename

    = spatialdb/fault_slabtop_slowslip.timedb +\end{cfg} + +The final set of parameters involve output. The domain and subdomain +output are similar to previous examples: +\begin{cfg} +[pylithapp.problem.formulation.output.domain] +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step06-domain.h5 + +[pylithapp.problem.formulation.output.subdomain] +# Name of nodeset for top surface. +

    label

    = boundary_zpos +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step06-groundsurf.h5 +\end{cfg} +For points output, we need to provide coordinate system information as +well as the name of the text file containing station names and +coordinates: +\begin{cfg} +# Specify output type, coordinate system, and station file for cgps_sites. +[pylithapp.problem.formulation.output.cgps_sites] +# We will use a geographic coordinate system for the cGPS sites file. +coordsys = spatialdata.geocoords.CSGeo +

    coordsys.space_dim

    = 3 +

    coordsys.datum_horiz

    = WGS84 +

    coordsys.datum_vert

    = mean sea level + +# Use HDF5 output. +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step06-cgps_sites.h5 + +# Simulated cGPS station file. +

    reader.filename

    = cgps_sites.txt +\end{cfg} +The remainder of the settings are for fault and material output, +similar to other examples: +\begin{cfg} +# Fault output ------------------------------------------------------ +[pylithapp.problem.interfaces.slab.output] +# Output fault results to HDF5 file. +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slab.h5 + +# We want both orientation and slip information in the information file. +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + +# Material output ------------------------------------------------------ +[pylithapp.problem.materials.slab.output] +

    writer.filename

    = output/step06-slab.h5 + +[pylithapp.problem.materials.wedge.output] +

    writer.filename

    = output/step06-wedge.h5 + +[pylithapp.problem.materials.crust.output] +

    writer.filename

    = output/step06-crust.h5 + +[pylithapp.problem.materials.mantle.output] +

    writer.filename

    = output/step06-mantle.h5 +\end{cfg} + We use elastic properties for all materials, and custom solver settings appropriate for a problem with a fault. We run the example by typing \begin{shell} @@ -777,8 +896,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} contours of the applied slip at t = 24 days. \begin{figure} - %\includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} - ADD FIGURE HERE + \includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} \caption{Solution for Step 6. The colors indicate the vertical displacement, the vectors represent the horizontal displacements at simulated cGPS sites, and the contours represent the applied @@ -800,7 +918,8 @@ \subsubsection{Exercises} initiation time). \begin{itemize} \item Either alter Python script to produce a spatial database of - slip initiation times, or write a new script. + slip initiation times, or write a new script. Can you produce a + more realistic-looking slow slip event? \end{itemize} \end{itemize} From b613c396594161fbe67a5d24851bc5e8d2180463 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 12:03:31 +1200 Subject: [PATCH 112/216] Added more comments. --- examples/3d/subduction/step06.cfg | 3 ++- 1 file changed, 2 insertions(+), 1 deletion(-) diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 06265738c4..2fcbbcbaad 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -100,6 +100,7 @@ interfaces = [slab] slab = pylith.faults.FaultCohesiveKin [pylithapp.problem.interfaces.slab] +# Nodeset corresponding to the fault patch and buried edge. label = fault_slabtop_patch edge = fault_slabtop_patch_edge @@ -123,7 +124,7 @@ slip.query_type = linear # We use a UniformDB to specify the slip initiation time. slip_time = spatialdata.spatialdb.UniformDB -slip_time.label = Slip initiation time +slip_time.label = Slip initiation time slip_time.values = [slip-time] slip_time.data = [0.0*year] From f3ba4262f0e906781e2451d02c060428c112345d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 17:23:58 -0700 Subject: [PATCH 113/216] Started work on Step 3. --- doc/userguide/examples/subduction3d.tex | 163 +++++++++++++++++++++++- 1 file changed, 159 insertions(+), 4 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 0f047b5fdc..c2b9fd59a3 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -77,6 +77,7 @@ \subsection{Features Illustrated} GUI, although the interaction is limited to rotating, translating, and zooming when run outside the ParaView GUI. +\todo{brad}{Complete filling in table.} \begin{table}[htbp] \caption{PyLith features covered in the suite of 3-D subduction zone examples.} \label{tab:example:subduction:3d:features} @@ -706,10 +707,10 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \end{shell} Figure \vref{fig:example:subduction:3d:step02}, which was created -using the ParaView Python script \filename{plot\_dispwarp.py}, displays -the magnitude of the displacement field exaggerated by a factor of 10,000. -The shallow fault results in deformation that is localized over a -small region. +using the ParaView Python script \filename{plot\_dispwarp.py}, +displays the magnitude of the displacement field exaggerated by a +factor of 10,000 at the final time step (t=200*yr).. The shallow +fault results in deformation that is localized over a small region. \begin{figure} \includegraphics[width=5.0in]{examples/figs/subduction3d_step02_soln} @@ -743,9 +744,163 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} +\label{sec:example:subduction:3d:step03} + +We now increase the complexity of our fault model by simulating the +interseismic deformation associated with the subducting slab. We +approximate the motion of the Juan de Fuca Plate subducting under the +North American Plate by introducing aseismic slip (creep) on the +bottom of the slab and the deeper portion of the top of the slab; we +keep the interface between the top of the slab and the accretionary +wedge and shallow crust locked. As in Step 2, we will use the linear +Maxwell viscoelastic constitutive model for the slab and mantle. +Figure~\ref{fig:example:subduction:3d:step03:diagram} summarizes the +problem description. + +\todo{brad}{Add annotation to figure.} +\begin{figure}[htbp] + \begin{tikzpicture} + \tikzstyle{annotation} = [black]; + \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; + %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); + %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); + \end{scope} + \end{tikzpicture} + \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and + interseismic deformation for the subducting slab. We precsribed + steady, uniform creep on the + bottom of the slab and deeper portion of the top of the slab. We + impose roller Dirichlet boundary conditions on the lateral and + bottom boundaries, except where they overlap with the fault + interfaces for the slab.} + \label{fig:example:subduction:3d:step03:diagram} +\end{figure} + +% Fault +With slip on the top and bottom of the slab, our fault interfaces +array contains two components, one for the top of the slab, +\facility{slab\_top}, and one for the bottom of the slab, +\facility{slab\_bottom}. We use the \object{FaultCohesiveKin} +object for each of these interfaces since we want to prescribe the +slip. +\begin{cfg} +[pylithapp.problem] +interfaces = [slab_top, slab_bottom] + +[pylithapp.problem.interfaces] +slab_top = pylith.faults.FaultCohesiveKin +slab_bottom = pylith.faults.FaultCohesiveKin +\end{cfg} + +% Bottom of slab +\todo{brad}{ADD STUFF HERE} + +\begin{cfg} +[pylithapp.problem.interfaces.slab_bottom] +

    id

    = 100 ; Must be different from ids used for materials +

    label

    = fault_slabbot ; Nodeset for the entire fault surface +

    edge

    = fault_slabbot_edge ; Nodeset for the buried edges +# Give slight westward tilt to the up_dir to avoid ambigious +# directions for the shear components on the horizontal portions of the +# fault. +

    up_dir

    = [-0.1,0,0.9] + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

    quadrature.cell.dimension

    = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +

    slip_rate.label

    = Slab bottom slip rate. +

    slip_rate.values

    = [left-lateral-slip, reverse-slip, fault-opening] +

    slip_rate.data

    = [+2.0*cm/year, -4.0*cm/year, 0.0*cm/year] + +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] + +[pylithapp.problem.interfaces.slab_bottom.output] +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step03-fault-slabbot.h5 +

    vertex_info_fields

    = [normal_dir, strike_dir, dip_dir] +\end{cfg} + + +% Top of slab +\todo{brad}{ADD STUFF HERE} + +\begin{cfg} +[pylithapp.problem.interfaces.slab_top] +

    id

    = 101 ; Must be different from ids used for materials +

    label

    = fault_slabtop ; Nodeset for the entire fault surface +

    edge

    = fault_slabtop_edge ; Nodeset for the buried edges + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

    quadrature.cell.dimension

    = 2 + +# Use the constant slip rate time function. +eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.slab_top.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.SimpleGridDB +

    slip_rate.label

    = Slab top slip rate. +

    slip_rate.filename

    = spatialdb/fault_slabtop_creep.spatialdb +

    slip_rate.query_type

    = linear + +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] + +[pylithapp.problem.interfaces.slab_top.output] +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step03-fault-slabtop.h5 +

    vertex_info_fields

    = [normal_dir, strike_dir, dip_dir] +\end{cfg} + +We run this example by typing +\begin{shell} +$$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +\end{shell} + +\todo{brad}{Update this} +Figure \vref{fig:example:subduction:3d:step03}, which was created +using the ParaView Python script \filename{plot\_dispwarp.py}, displays +the magnitude of the displacement field exaggerated by a factor of 10,000. +The shallow fault results in deformation that is localized over a +small region. + +\begin{figure} +\todo{brad}{Add figure here} + %\includegraphics[width=5.0in]{examples/figs/subduction3d_step03_soln} + \caption{Solution over the domain for Step 2 at t=200*yr. The colors indicate + the magnitude of the displacement and we have exaggerated the + deformation by a factor of 10,000.} + \label{fig:example:subduction:3d:step02} +\end{figure} + \subsubsection{Exercises} +\todo{brad}{Add stuff here} +\begin{itemize} +\item +\end{itemize} + + % ---------------------------------------------------------------------- \subsection{Step 4: Prescribed Earthquake Cycle} From d0dde1cccc7020ef2ac25973c73e27599b221635 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 17:24:21 -0700 Subject: [PATCH 114/216] Reorder some parameters for consistency with manual. --- examples/3d/subduction/step03.cfg | 64 +++++++++++++++++-------------- 1 file changed, 35 insertions(+), 29 deletions(-) diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index e44f14e210..1f9d8c363c 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -88,17 +88,24 @@ label = boundary_ypos_nofault # ---------------------------------------------------------------------- [pylithapp.problem] # We prescribe slip on the top and bottom of the slab. -interfaces = [slab_top, slab_bottom] +interfaces = [slab_bottom, slab_top] [pylithapp.problem.interfaces] -slab_top = pylith.faults.FaultCohesiveKin slab_bottom = pylith.faults.FaultCohesiveKin +slab_top = pylith.faults.FaultCohesiveKin -# Slab top ------------------------------------------------------------- -[pylithapp.problem.interfaces.slab_top] -id = 100 -label = fault_slabtop -edge = fault_slabtop_edge +# Slab bottom ---------------------------------------------------------- +[pylithapp.problem.interfaces.slab_bottom] +id = 100 ; Must be different from ids used for materials +label = fault_slabbot ; Nodeset for the entire fault surface +edge = fault_slabbot_edge ; Nodeset for the buried edges +# Some portions of the bottom of the slab are perfectly horizontal, so +# our procedure that uses the vertical direction and the fault normal +# to set the along-strike and up-dip shear components breaks down. We +# remedy this by tweaking the up_dir from being completely vertical to +# tilting slightly to the west. This will result in the desired +# along-strike and up-dip directions. +up_dir = [-0.1,0,0.9] # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). @@ -109,28 +116,27 @@ quadrature.cell.dimension = 2 eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn # The slip time and final slip are defined in spatial databases. -[pylithapp.problem.interfaces.slab_top.eq_srcs.rupture.slip_function] -slip_rate = spatialdata.spatialdb.SimpleGridDB -slip_rate.label = Slab top slip rate. -slip_rate.filename = spatialdb/fault_slabtop_creep.spatialdb -slip_rate.query_type = linear +[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slab bottom slip rate. +slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] +slip_rate.data = [+2.0*cm/year, -4.0*cm/year, 0.0*cm/year] slip_time = spatialdata.spatialdb.UniformDB slip_time.label = Slip initiation time slip_time.values = [slip-time] -slip_time.data = [0.0*year] +slip_time.data = [0.0*year] -[pylithapp.problem.interfaces.slab_top.output] +[pylithapp.problem.interfaces.slab_bottom.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step03-fault-slabtop.h5 +writer.filename = output/step03-fault-slabbot.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] -# Slab bottom ---------------------------------------------------------- -[pylithapp.problem.interfaces.slab_bottom] -id = 101 -label = fault_slabbot -edge = fault_slabbot_edge -up_dir = [-0.1,0,0.9] +# Slab top ------------------------------------------------------------- +[pylithapp.problem.interfaces.slab_top] +id = 101 ; Must be different from ids used for materials +label = fault_slabtop ; Nodeset for the entire fault surface +edge = fault_slabtop_edge ; Nodeset for the buried edges # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). @@ -141,20 +147,20 @@ quadrature.cell.dimension = 2 eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn # The slip time and final slip are defined in spatial databases. -[pylithapp.problem.interfaces.slab_bottom.eq_srcs.rupture.slip_function] -slip_rate = spatialdata.spatialdb.UniformDB -slip_rate.label = Slab bottom slip rate. -slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] -slip_rate.data = [+2.0*cm/year, -4.0*cm/year, 0.0*cm/year] +[pylithapp.problem.interfaces.slab_top.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.SimpleGridDB +slip_rate.label = Slab top slip rate. +slip_rate.filename = spatialdb/fault_slabtop_creep.spatialdb +slip_rate.query_type = linear slip_time = spatialdata.spatialdb.UniformDB slip_time.label = Slip initiation time slip_time.values = [slip-time] -slip_time.data = [0.0*year] +slip_time.data = [0.0*year] -[pylithapp.problem.interfaces.slab_bottom.output] +[pylithapp.problem.interfaces.slab_top.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step03-fault-slabbot.h5 +writer.filename = output/step03-fault-slabtop.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] # ---------------------------------------------------------------------- From 65dabbe8d823a18ceb2407a6a15f00cca3aae15c Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 13:47:02 +1200 Subject: [PATCH 115/216] Added some stuff for step07. --- doc/userguide/examples/subduction3d.tex | 17 ++++++++++------- 1 file changed, 10 insertions(+), 7 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 139c922779..f55896bc77 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -974,19 +974,22 @@ \subsubsection{Exercises} \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} This example is essentially a three-dimensional analog of -{sec:example:greensfns2d}, and is a more realistic example of how +\vref{sec:example:greensfns2d}, and is a more realistic example of how PyLith can be used to perform geodetic inversions. We use the output of example step06 to create synthetic data. Once we have done this we generate Green's functions to represent the geodetic responses at a set of synthetic cGPS stations. Finally, we use the synthetic data and Green's functions to perform an inversion, using the same generalized -inverse approach described in {sec:example:greensfns2d}. +inverse approach described in \vref{sec:example:greensfns2d:inversion}. We first generate the synthetic data by using the script -\filename{make\_synthetic\_gpsdisp.py} in the top-level directory. This -script reads the parameters in \filename{make\_synthetic\_gpsdisp.cfg} -to generate synthetic data from the selected time step with a -specified amount of noise. Run this script as: +\filename{make\_synthetic\_gpsdisp.py} in the top-level +directory. This script reads the parameters in +\filename{make\_synthetic\_gpsdisp.cfg} to generate synthetic data +from the selected time step with a specified amount of noise. The +point data output from example step06 is read, the specified time step +is selected, and the specified amount of noise is added to the +results. Run this script as: \begin{shell} $$ ./make_synthetic_gpsdisp.py \end{shell} @@ -997,7 +1000,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} \item[\filename{cgps\_synthetic\_displacement.vtk}] for visualization. \end{description} -After we generate the synthetic data, we generate the Green's +After we create the synthetic data, we generate the Green's functions. We divide the Green's function generation into two sub-problems: \begin{itemize} \item step07a: Generate Green's functions corresponding to From fa1cddcd39f66d1e233ee754666a87b92a5450d5 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 13:53:39 +1200 Subject: [PATCH 116/216] Added more comments. --- examples/3d/subduction/greensfns.cfg | 3 +++ examples/3d/subduction/step07a.cfg | 2 ++ examples/3d/subduction/step07b.cfg | 2 ++ 3 files changed, 7 insertions(+) diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg index 0b13bc422f..2f58bbc3fd 100644 --- a/examples/3d/subduction/greensfns.cfg +++ b/examples/3d/subduction/greensfns.cfg @@ -21,13 +21,16 @@ # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- +# Define the interfaces (slab) and provide a fault_id. [greensfns] interfaces = [slab] fault_id = 100 +# Switch fault to FaultCohesiveImpulses for generation of Green's functions. [greensfns.interfaces] slab = pylith.faults.FaultCohesiveImpulses +# Nodesets corresponding to the fault and its buried edge. [greensfns.interfaces.slab] label = fault_slabtop_patch edge = fault_slabtop_patch_edge diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 8a234f2c82..5bb8ec61c2 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -72,6 +72,8 @@ problem.progress_monitor.filename = output/step07a-progress.txt # ---------------------------------------------------------------------- [pylithapp.problem.interfaces.slab] # Impulses for left-lateral slip. +# Note that it is possible to apply both left-lateral and updip slip +# (impulse_dof = [0,1]), but we separate the impulses into two problems. impulse_dof = [0] # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 5de988cb81..5e0486c80c 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -72,6 +72,8 @@ problem.progress_monitor.filename = output/step07b-progress.txt # ---------------------------------------------------------------------- [pylithapp.problem.interfaces.slab] # Impulses for reverse slip. +# Note that it is possible to apply both left-lateral and updip slip +# (impulse_dof = [0,1]), but we separate the impulses into two problems. impulse_dof = [1] # ---------------------------------------------------------------------- From b6ee6d0464425104393eafced1f3677399b47df3 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 13:56:46 +1200 Subject: [PATCH 117/216] Added a label for a subsection. --- doc/userguide/examples/greensfns2d.tex | 1 + 1 file changed, 1 insertion(+) diff --git a/doc/userguide/examples/greensfns2d.tex b/doc/userguide/examples/greensfns2d.tex index 153c51d530..c87a4680a5 100644 --- a/doc/userguide/examples/greensfns2d.tex +++ b/doc/userguide/examples/greensfns2d.tex @@ -244,6 +244,7 @@ \subsection{Step 2: Generation of Green's Functions} \subsection{Step 3: Simple Inversion Using PyLith-generated Green's Functions} +\label{sec:example:greensfns2d:inversion} In the previous two steps we generated a set of synthetic data as well as a set of Green's functions. Both are stored in HDF5 files. From e8bd5cefc56848cc1f1535c8188e87e48cb6bdf7 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 21:56:00 -0700 Subject: [PATCH 118/216] Improved description of fault 'id'. --- doc/userguide/boundaryconditions/boundaryconditions.tex | 7 +++++-- 1 file changed, 5 insertions(+), 2 deletions(-) diff --git a/doc/userguide/boundaryconditions/boundaryconditions.tex b/doc/userguide/boundaryconditions/boundaryconditions.tex index 7476f0c40c..5cd48a41d9 100644 --- a/doc/userguide/boundaryconditions/boundaryconditions.tex +++ b/doc/userguide/boundaryconditions/boundaryconditions.tex @@ -590,8 +590,11 @@ \subsection{Fault Parameters} \begin{inventory} \propertyitem{id}{This is an integer identifier for the fault surface. It is used to specify the \property{material-id} of the cohesive cells in -the mesh. Material identifiers must be unique so this value cannot -be the same as any of the material models or any other fault.} +the mesh. Material identifiers must be unique across all materials and +fault interfaces. Because PyLith creates the cohesive +cells at runtime, there is no correspondence between the \property{id} +property and information in the input mesh like there +is for materials.} \propertyitem{label}{Name of group of vertices associated with the fault surface. This label is also used in error and diagnostic reports.} \propertyitem{edge}{Name of group of vertices marking the buried edges of the From 25e5b39d5379a9f980c652b6ef7feef56a10ad3c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 21 Jun 2017 21:56:27 -0700 Subject: [PATCH 119/216] Step 3 is mostly complete. --- .../figs/subduction3d_step03_soln.jpg | Bin 0 -> 185122 bytes doc/userguide/examples/subduction3d.tex | 79 +++++++++++++----- 2 files changed, 58 insertions(+), 21 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_step03_soln.jpg diff --git a/doc/userguide/examples/figs/subduction3d_step03_soln.jpg b/doc/userguide/examples/figs/subduction3d_step03_soln.jpg new file mode 100644 index 0000000000000000000000000000000000000000..52df4f30fdacde27f29a3ccc54225d9ee81d4f18 GIT binary patch literal 185122 zcmb5V1ymeQx9B@SAOs5#ELiXa5AKlQP9V&ngALB$7Bmnf!9!qhNpP4MU~q@vPLLTK zf;$AaKyLo$zH`_6&UemR_w8O?tGae|)&8}uuDz@N%>4NYAXQgZQwCsR0RUKkH^85H 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    id

    = 100 ; Must be different from ids used for materials @@ -835,10 +848,12 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation}

    vertex_info_fields

    = [normal_dir, strike_dir, dip_dir] \end{cfg} - % Top of slab -\todo{brad}{ADD STUFF HERE} - +The parameters for the top of the slab closely resemble those for the +bottom of the slab. The main difference is that we use a +\object{SimpleGridDB} to define a depth variation in the slip +rate. The fault is locked at depths above 45 km and increases linearly +to the same slip rate as the bottom of the slab at a depth of 60 km. \begin{cfg} [pylithapp.problem.interfaces.slab_top]

    id

    = 101 ; Must be different from ids used for materials @@ -871,33 +886,55 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation}

    vertex_info_fields

    = [normal_dir, strike_dir, dip_dir] \end{cfg} +% Boundary conditions +PyLith does not support an overlap between Dirichlet boundary +conditions and fault interfaces, so we use nodesets that exclude +vertices on the faults for the -x, -y, and +y boundaries rather than +the nodesets that include all vertices on those boundaries. +\begin{cfg} +# -x face +[pylithapp.problem.bc.x_neg] +

    label

    = boundary_xneg_nofault + +# -y face +[pylithapp.problem.bc.y_neg] +

    label

    = boundary_yneg_nofault + +# +y face +[pylithapp.problem.bc.y_pos] +

    label

    = boundary_ypos_nofault +\end{cfg} + We run this example by typing \begin{shell} $$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} -\todo{brad}{Update this} Figure \vref{fig:example:subduction:3d:step03}, which was created -using the ParaView Python script \filename{plot\_dispwarp.py}, displays -the magnitude of the displacement field exaggerated by a factor of 10,000. -The shallow fault results in deformation that is localized over a -small region. +using the ParaView Python script \filename{plot\_dispwarp.py}, shows +the deformation exaggerated by a factor of 5,000 at the final time +step of t=200*yr. Notice that there are some local edge effects +associated with the unconstrained degrees of freedom at the +intersection of the boundaries and fault surfaces. \begin{figure} -\todo{brad}{Add figure here} %\includegraphics[width=5.0in]{examples/figs/subduction3d_step03_soln} - \caption{Solution over the domain for Step 2 at t=200*yr. The colors indicate - the magnitude of the displacement and we have exaggerated the - deformation by a factor of 10,000.} - \label{fig:example:subduction:3d:step02} + \caption{Solution over the domain for Step 2 at $t=200 \mathrm{yr}$. The colors indicate + the x-displacement and we have exaggerated the + deformation by a factor of 5,000.} + \label{fig:example:subduction:3d:step03} \end{figure} \subsubsection{Exercises} -\todo{brad}{Add stuff here} \begin{itemize} -\item +\item Adjust the locking depth for the top of the slab. How does this + affect the spatial distribution of the change in tractions on + the fault interfaces? +\item Increase the rigidity of the slab and decrease the rigidity of + the wedge and/or crust. How do these affect the change in tractions + on the fault interfaces? \end{itemize} From d1da6600ed218dff32c78606175cc008994bb4b2 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 17:19:11 +1200 Subject: [PATCH 120/216] More updates for step07. --- .../subduction3d_step07_inverse_curve.png | Bin 0 -> 46409 bytes .../figs/subduction3d_step07_inverse_soln.png | Bin 0 -> 130183 bytes doc/userguide/examples/subduction3d.tex | 241 ++++++++++++++++-- examples/3d/subduction/step07a.cfg | 1 - examples/3d/subduction/step07b.cfg | 1 - 5 files changed, 224 insertions(+), 19 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_step07_inverse_curve.png create mode 100644 doc/userguide/examples/figs/subduction3d_step07_inverse_soln.png diff --git a/doc/userguide/examples/figs/subduction3d_step07_inverse_curve.png b/doc/userguide/examples/figs/subduction3d_step07_inverse_curve.png new file mode 100644 index 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The colors indicate the vertical displacement, the vectors represent the horizontal displacements at simulated cGPS sites, and the contours represent the applied - slip at t = 24 days. } + slip at t = 24 days.} \label{fig:example:subduction:3d:step06} \end{figure} @@ -1172,32 +1172,239 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} default \facility{timedependent} to \facility{greensfns}. We do this on the command line. When we change the problem type to \facility{greensfns}, PyLith automatically reads the file -\filename{greensfns.cfg}. We use this file to augment the settings in -\filename{pylithapp.cfg}: +\filename{greensfns.cfg}. This file contains non-default settings that +are common to both sub-problems. Note that since the problem type has +been changed from the default \facility{timedependent} to +\facility{greensfns}, the facility labels are changed. Also, since +\facility{problem} is a facility of \facility{pylithapp}, we no longer +need the \facility{pylithapp} prefix in this file. We first specify +the fault information: +\begin{cfg} +# Define the interfaces (slab) and provide a fault_id. +[greensfns] +interfaces = [slab] +

    fault_id

    = 100 + +# Switch fault to FaultCohesiveImpulses for generation of Green's functions. +[greensfns.interfaces] +slab = pylith.faults.FaultCohesiveImpulses + +# Nodesets corresponding to the fault and its buried edge. +[greensfns.interfaces.slab] +

    label

    = fault_slabtop_patch +

    edge

    = fault_slabtop_patch_edge + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

    quadrature.cell.dimension

    = 2 + +# Spatial database for slip impulse amplitude. +db_impulse_amplitude = spatialdata.spatialdb.UniformDB +

    db_impulse_amplitude.label

    = Amplitude of fault slip impulses +

    db_impulse_amplitude.values

    = [slip] +

    db_impulse_amplitude.data

    = [1.0] +\end{cfg} + +In addition to defining the fault information, we also set some output +information common to both sub-problems, writing addition info fields +for fault output, and turning off material output. If we left material +output turned on, we would end up with extremely large state variable +output files: +\begin{cfg} +[greensfns.interfaces.slab.output] +# Add impulse amplitude to fault info output. +

    vertex_info_fields

    = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +writer = pylith.meshio.DataWriterHDF5 + +# Turn off output of state variables for materials. +[greensfns.materials.slab.output] +

    cell_data_fields

    = [] + +[greensfns.materials.wedge.output] +

    cell_data_fields

    = [] +[greensfns.materials.crust.output] +

    cell_data_fields

    = [] - %% After generating the synthetic data and Green's functions, we then - %% perform a simple inversion using the slip_invert.py script, with - %% parameters defined in slip_invert.cfg: +[greensfns.materials.mantle.output] +

    cell_data_fields

    = [] +\end{cfg} - %% ./slip_invert.py +The \filename{step07a.cfg} and \filename{step07b.cfg} files are +identical, except for the impulse type specification and file +names. Here are the fault parameters in \filename{step07a.cfg}: +\begin{cfg} +[pylithapp.problem.interfaces.slab] +# Impulses for left-lateral slip. +# Note that it is possible to apply both left-lateral and updip slip +# (impulse_dof = [0,1]), but we separate the impulses into two problems. +

    impulse_dof

    = [0] +\end{cfg} - %% This will generate two HDF files that may be viewed in Paraview: - %% step07-inversion-slip.h5: The predicted fault slip. - %% step07-inversion-displacement.h5: The predicted surface displacements. +In the output settings, we turn off output for the domain and ground +surface, provide coordinate system info for the simulated cGPS output, +and provide filenames: +\begin{cfg} +# Add cggs_sites to solution output. +[pylithapp.problem.formulation] +output = [domain, subdomain, cgps_sites] +output.cgps_sites = pylith.meshio.OutputSolnPoints + +# Domain, subdomain, and cgs_sites +[pylithapp.problem.formulation.output.domain] +

    writer.filename

    = output/step07a-domain.h5 +# Turn off data fields. +

    vertex_data_fields

    = [] - %% There is also an inversion summary file: step07-inversion-summary.txt - %% If you have matplotlib installed, you can view a log-log plot of - %% solution misfit by going into the viz directory and running: +[pylithapp.problem.formulation.output.subdomain] +

    writer.filename

    = output/step07a-groundsurf.h5 +# Turn off data fields. +

    vertex_data_fields

    = [] - %% ./plot_inversion_misfit.py --summary=../step07-inversion-summary.txt +[pylithapp.problem.formulation.output.cgps_sites] +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step07a-cgps_sites.h5 +# Set coordinate system associated with file with cGPS sites +

    reader.filename

    = cgps_sites.txt +coordsys = spatialdata.geocoords.CSGeo +

    coordsys.space_dim

    = 3 +

    coordsys.datum_horiz

    = WGS84 +

    coordsys.datum_vert

    = mean sea level + +# Fault +[pylithapp.problem.interfaces.slab.output] +

    writer.filename

    = output/step07a-fault-slab.h5 + +# Materials +[pylithapp.problem.materials.slab.output] +

    writer.filename

    = output/step07a-slab.h5 + +[pylithapp.problem.materials.wedge.output] +

    writer.filename

    = output/step07a-wedge.h5 + +[pylithapp.problem.materials.crust.output] +

    writer.filename

    = output/step07a-crust.h5 + +[pylithapp.problem.materials.mantle.output] +

    writer.filename

    = output/step07a-mantle.h5 +\end{cfg} + +You can run the two sub-problems as follows: +\begin{shell} +$$ pylith --problem=pylith.problems.GreensFns step07a.cfg +mat_elastic.cfg solver_fieldsplit.cfg +$$ pylith --problem=pylith.problems.GreensFns step07b.cfg +mat_elastic.cfg solver_fieldsplit.cfg +\end{shell} +\tip{To save runtime, run the two sub-problems simultaneously in +separate terminal windows. For a problem this size, this should work +fine on a laptop. For larger problems, this approach can still be +useful. Each sub-problem could be run simultaneously on several nodes +of a cluster, for example.} + +After generating the synthetic data and Green's functions, we then +perform a simple inversion using the \filename{slip\_invert.py} script, +with parameters defined in \filename{slip\_invert.cfg}. This script +performs a set of linear inversions, in a manner similar to the +inversion in \vref{sec:example:greensfns2d:inversion}. This script is +in the top-level \filename{subduction} directory. From there, run the +script as follows: +\begin{shell} +$$ ./slip_invert.py +\end{shell} +This will create a number of files in the output directory. Note that +the HDF5 files have an associated \filename{.xmf} file to use with +ParaView: +\begin{description} +\item[\filename{step07-inversion-slip.h5}] This file may + be used to visualize the predicted slip distributions for different + values of the penalty weight. +\item[\filename{step07-inversion-displacement.h5}] This file may be used to + visualize the predicted cGPS displacements for each solution. +\item[\filename{step07-inversion-summary.txt}] This file provides a summary + of the inversion results for each value of the penalty weight. +\end{description} + +When performing an inversion such as this, one approach is to find the +corner of the 'L-curve' when plotting the log of the weighted data +residual vs. the log of the penalty residual. This is viewed as the +point of diminishing returns for reducing the penalty +weight. Further reductions provide little improvement to the +weighted data residual, while providing a solution with less +regularization. A Python script has been provided in the +\filename{viz} subdirectory to plot this curve, assuming that the user +has the numpy and matplotlib Python packages installed. From the +\filename{viz} subdirectory, run this script as: +\begin{shell} +./plot_inversion_misfit.py +--summary=../output/step07-inversion-summary.txt +\end{shell} +This will produce a curve similar to that shown in Figure +\vref{fig:example:subduction:3d:step07:curve} +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step07_inverse_curve} + \caption{Plot of the 'L-curve' for inversion in example step07. The + 'corner' of the L-curve would be about the third or fourth point + from the right of the plot, representing a penalty weight of 0.5 + or 1.0 in our example. } + \label{fig:example:subduction:3d:step07:curve} +\end{figure} + +Once we have determined the optimal solution by analyzing the L-curve, +we can then visualize the results using ParaView. Figure +\vref{fig:example:subduction:3d:step07:invresults} shows the predicted +slip, the observed and predicted displacement vectors, and the slip +applied from example step06 for a penalty weight of 1.0. The data fit +is very good, and the predicted slip distribution is very close to the +applied slip, although the magnitude is slightly underestimated. +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step07_inverse_soln} + \caption{ParaView image of the inversion solution for a penalty + weight of 1.0. 'Data' is shown with blue arrows and predicted + displacements are shown with magenta arrows. Color contours + represent the predicted slip distribution and orange line contours + show the applied slip from the forward problem.} + \label{fig:example:subduction:3d:step07:invresults} +\end{figure} \subsubsection{Exercises} -% Move slip to splay fault in step06 and redo inversion. -% Adjust noise level -% Invert for slip at each time step +\begin{itemize} +\item Investigate the effects of data noise. + \begin{itemize} + \item How do the noisy data vectors compare to the raw data vectors + from example step06? + \item Create a new simulated dataset with more noise and see how + well the solution matches the applied slip. + \end{itemize} +\item Different initial slip distribution. + \begin{itemize} + \item Move the slip distribution to a different location, vary the + amplitude, etc. This will involve running another instance of example + step06 to create a new dataset. How is the solution affected? + \item Move the slip onto the splay fault. This will involve creating + a new forward model as well as generating Green's functions for the + splay fault. + \end{itemize} +\item What happens if your material properties are incorrect? + \begin{itemize} + \item Try creating your forward model with heterogeneous properties + and your Green's functions with homogeneous properties (or + vice-versa). What happens to your solution? + \end{itemize} +\item Try inverting for slip at various time steps. +\item Try a different inversion method. + \begin{itemize} + \item If you analyze the predicted slip distribution you will find + some negative slip, which is unrealistic. To overcome this problem + you could try NNLS (non-negative least squares). If you have the + scipy package installed on your computer, you could replace the + generalized inverse solution with the NNLS package included in + \filename{scipy.optimize.nnls}. + \end{itemize} +\end{itemize} % ---------------------------------------------------------------------- \subsection{Step 8: Stress Field Due to Gravitational Body Forces} diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 5bb8ec61c2..18892a76e5 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -106,7 +106,6 @@ coordsys.space_dim = 3 coordsys.datum_horiz = WGS84 coordsys.datum_vert = mean sea level - # Fault [pylithapp.problem.interfaces.slab.output] writer.filename = output/step07a-fault-slab.h5 diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 5e0486c80c..3b867146cd 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -106,7 +106,6 @@ coordsys.space_dim = 3 coordsys.datum_horiz = WGS84 coordsys.datum_vert = mean sea level - # Fault [pylithapp.problem.interfaces.slab.output] writer.filename = output/step07b-fault-slab.h5 From 65a1df662f4fa43b2dcdbda4eb37502d1b3bb746 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Thu, 22 Jun 2017 18:33:21 +1200 Subject: [PATCH 121/216] Started documentation for step08 and added some comments to .cfg file. --- .../figs/subduction3d_step08a_soln.png | Bin 0 -> 490088 bytes doc/userguide/examples/subduction3d.tex | 92 ++++++++++++++++++ examples/3d/subduction/step08a.cfg | 19 +--- 3 files changed, 97 insertions(+), 14 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_step08a_soln.png diff --git a/doc/userguide/examples/figs/subduction3d_step08a_soln.png b/doc/userguide/examples/figs/subduction3d_step08a_soln.png new file mode 100644 index 0000000000000000000000000000000000000000..5e6c4ddd4488573555583e9abb12f9a5c60744fb GIT binary patch literal 490088 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zXfjt}dKwx%AYwJ(-{o|=s;UZTCmy)tzDZvo@XWREG-{dk-jxi!@S=;M3va&;8!^HUHT%w~gikQvk8-w%#F zW!|}aw?wzNww7H%SexBgmDv~t>1BjGcVLMIte;)|BvPG;l$2B$=nw!kLZE5aax8c*6bU$Mhw%})3dd+V|_Us&*4qp?sdoyh0WMR zVF2<-C;k5d4G`HMpm$1^+FYe>BG3Tj54wV;zX4f0Tezeh{-;CHRa}4I156*Q8(blX Wdo|o2)Q>{IbK$J{nG)k0_x=May2w`m literal 0 HcmV?d00001 diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 1848d90e47..ab71e3bd1a 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1446,5 +1446,97 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 8: Stress Field Due to Gravitational Body Forces} +This example demonstrates the use of gravitational body forces in +PyLith simulations, as well as the use of initial stresses to balance +the body forces. We also demonstrate what happens when the initial +stresses are not in balance with the gravitational stresses, and show +how viscoelastic problems with gravitational stresses will in general +will not reach a steady-state solution. We do not include faults in +this example. The example is divided into three sub-problems: +\begin{itemize} +\item Step08a: Gravitational body forces with 3-D density variations + in elastic materials and initial stresses for a uniform density. +\item Step08b: Gravitational body forces with 3-D density variations + in elastic materials and initial stresses from Step08a (initial + stresses satisfy equilibrium, so there is no deformation). +\item Step08c: Gravitational body forces with 3-D density variations + in elastic and viscoelastic materials and initial stresses from + Step08a plus finite strain formulation (does not reach a steady-state + solution). +\end{itemize} + +For the first sub-problem (step08a), we apply gravitational stresses +and attempt to balance these with analytically computed stresses +consistent with the density of the mantle. Since the densities are not +constant, the forces are out of balance and we end up with significant +deformation. We first apply gravity and set the simulation time to +zero (static problem): +\begin{cfg} +[pylithapp.timedependent] +# Set gravity field (default is None). +gravity_field = spatialdata.spatialdb.GravityField + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation. +

    total_time

    = 0.0*year +\end{cfg} +Then, for each material, we use the same spatial database for the +initial stresses. We use linear interpolation and in the database the +initial stress is simply computed as $\{rho}_mgh$, where $\{rho}_m$ is +the density of the mantle material and $h$ is the depth below the +ground surface: +\begin{cfg} +# We specify initial stresses for each material via a SimpleDB and linear interpolation. +[pylithapp.problem.materials.slab] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the slab +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav.spatialdb +

    db_initial_stress.query_type

    = linear + +[pylithapp.problem.materials.wedge] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the wedge +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav.spatialdb +

    db_initial_stress.query_type

    = linear + +[pylithapp.problem.materials.mantle] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the mantle +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav.spatialdb +

    db_initial_stress.query_type

    = linear + +[pylithapp.problem.materials.crust] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the crust +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav.spatialdb +

    db_initial_stress.query_type

    = linear +\end{cfg} + +The output parameters are simply the output filenames, since all the +other parameters are the defaults in \filename{pylithapp.cfg}. We use +the algebraic multigrid solver, which is appropriate for problems with +no fault. We run the sub-problem by doing: +\begin{shell} +$$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +\end{shell} + +When the problem has run, we see deformation that is consistent with +the mismatched densities. Figure +\vref{fig:example:subduction:3d:step08a} demonstrates the deformed +mesh visualized by running the following command from the +\filename{subduction} directory: +\begin{shell} +./viz/plot_dispwarp.py --sim=step08a --exaggeration=500.0 +--screenshot=subduction3d_step08a_soln.png +\end{shell} +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step08a_soln} + \caption{Image generated by running the \filename{plot\_dispwarp.py} + script for sub-problem step08a. The crustal material to the + east is lighter than the assumed mantle material for initial + stresses, while the slab material to the west is heavier. The + result is uplift to the east and downward movement to the west.} + \label{fig:example:subduction:3d:step08a} +\end{figure} % End of file diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg index 550a2e93e6..93286d71ae 100644 --- a/examples/3d/subduction/step08a.cfg +++ b/examples/3d/subduction/step08a.cfg @@ -16,20 +16,11 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# We compute an estimate of the overburden stresses due to -# gravitational body forces and 3-D density variations assuming purely -# linearly, isotropic elastic materials. We minimize the deformation -# by using initial stresses equal to the overburden with uniform -# properties corresponding to the mantle. -# -# Step08a: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses for a uniform density. -# Step08b: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses from Step08a (initial stresses -# satisfy equilibrium, so there is no deformation). -# Step08c: Gravitational body forces with 3-D density variations in elastic -# and viscoelastic materials and initial stresses from Step08a -# (does not reach a steady-state solution). +# We apply gravitational body forces to our model with heterogeneous +# material properties, and attempt to balance these body forces with +# material properties (density) corresponding to the mantle. In this +# case the forces do not balance and we end up with large vertical +# deformations in the elastic solution. # # Materials # All four blocks use the linear, isotropic elastic material model From a5c654b36e9a58cf6945746132b59e66630c308a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 09:09:16 -0700 Subject: [PATCH 122/216] Customize colorbars (add units). Add component command line argument in plot_dispwarp.py. --- examples/3d/subduction/viz/plot_dispvec.py | 11 ++++----- examples/3d/subduction/viz/plot_dispwarp.py | 25 +++++++++++++-------- 2 files changed, 22 insertions(+), 14 deletions(-) diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 2e3176d946..4e7333a060 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -63,13 +63,14 @@ def visualize(sim, dispScale, showFinalTimeStep=False): domainDisplay.RescaleTransferFunctionToDataRange(True) domainDisplay.SetScalarBarVisibility(view, True) domainDisplay.SetRepresentationType("Surface With Edges") - - # Rescale color and/or opacity maps used to exactly fit the current data range - displacementLUT = GetColorTransferFunction('displacement') + # Rescale color maps to exactly fit the current data range domainDisplay.RescaleTransferFunctionToDataRange(False, False) - # Update scalar bar component title. - UpdateScalarBarsComponentTitle(displacementLUT, domainDisplay) + # Customize colorbar + displacementLUT = GetColorTransferFunction('displacement') + colorbar = GetScalarBar(displacementLUT, view) + colorbar.Title = "Displacement Mag. (m)" + colorbar.ComponentTitle = "" # Add arrows to show displacement vectors. glyph = Glyph(Input=dataDomain, GlyphType="Arrow") diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index 8714b97024..cdda2035c4 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -26,16 +26,17 @@ # pvpython. # Root name for simulation. -SIM_NAME = "step01" +SIM_NAME = "step03" # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 +DISPLACEMENT_COMPONENT = "X" # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, exaggeration, showFinalTimeStep=False): +def visualize(sim, exaggeration, component, showFinalTimeStep=False): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -65,16 +66,21 @@ def visualize(sim, exaggeration, showFinalTimeStep=False): warp.ScaleFactor = exaggeration warpDisplay = Show(warp, view) - ColorBy(warpDisplay, ('POINTS', 'displacement', 'X')) + ColorBy(warpDisplay, ('POINTS', 'displacement', component)) warpDisplay.RescaleTransferFunctionToDataRange(True) warpDisplay.SetScalarBarVisibility(view, True) warpDisplay.SetRepresentationType('Surface With Edges') + # Rescale color bar to exactly fit the current data range + warpDisplay.RescaleTransferFunctionToDataRange(False, False) - # Rescale color and/or opacity maps used to exactly fit the current data range + # Customize colorbar displacementLUT = GetColorTransferFunction('displacement') - warpDisplay.RescaleTransferFunctionToDataRange(False, False) - # Update a scalar bar component title. - UpdateScalarBarsComponentTitle(displacementLUT, warpDisplay) + colorbar = GetScalarBar(displacementLUT, view) + if component.lower() == "magnitude": + colorbar.Title = "Displacement Mag. (m)" + else: + colorbar.Title = "%s-displacement (m)" % component.lower() + colorbar.ComponentTitle = "" # Annotate time tstamp = AnnotateTimeFilter(warp) @@ -97,10 +103,11 @@ def visualize(sim, exaggeration, showFinalTimeStep=False): parser = argparse.ArgumentParser() parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) + parser.add_argument("--component", action="store", dest="component", default=DISPLACEMENT_COMPONENT) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.exaggeration, showFinalTimeStep=True) + visualize(args.sim, args.exaggeration, args.component, showFinalTimeStep=True) view = GetRenderView() view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] @@ -117,7 +124,7 @@ def visualize(sim, exaggeration, showFinalTimeStep=False): else: # Running inside the ParaView GUI - visualize(SIM_NAME, DISPLACEMENT_SCALE) + visualize(SIM_NAME, DISPLACEMENT_SCALE, DISPLACEMENT_COMPONENT) # End of file From acbd8db3a6ebd9e355af0cf8eeda3e58ee893931 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 09:10:45 -0700 Subject: [PATCH 123/216] Add step04 to manual. 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U<1R8s&WQo#_7Ax85BT@#f3xlx2mk;8 literal 0 HcmV?d00001 diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index ab71e3bd1a..e6a374cd11 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -11,7 +11,7 @@ \subsection{Overview} focus on modeling the deformation associated with the the subducting slab, including interseismic deformation with aseismic slip (creep) and viscoelastic relaxation, coseismic slip on the slab interface and -a splay fault, and slow slip events on the top slab interface. We want +a splay fault, and slow slip events on the subduction interface. We want to account for the 3-D material properties associated with different elastic properties for the subducting slab, mantle, continental crust, and an accretionary wedge. To keep the computation time in these @@ -36,9 +36,10 @@ \subsection{Overview} wedge. We cut off the slab at a depth of 100 km. We use a transverse geographic projection coordinate system with Portland, Oregon, as the origin in order to georeference our model. In order to model the -motion of the slab, we include a fault on the top of the slab at the -interface between the mantle, crust, and wedge, as well as a fault -between the bottom of the slab and the mantle. +motion of the slab, we include a fault for the subduction interface +(the interface between the top of the slab and the mantle, crust, and +wedge), as well as a fault between the bottom of the slab and the +mantle. \begin{figure}[htbp] \includegraphics[width=4.5in]{examples/figs/subduction3d_conceptualmodel} @@ -95,7 +96,7 @@ \subsection{Generating the Finite-Element Mesh} skip generating the mesh. We use contours of the Cascadia Subduction Zone from Slab v1.0 -\cite{Hayes:etal:2012} for the geometry of the top of the slab. In +\cite{Hayes:etal:2012} for the geometry of the subduction interface. In order to make use of these contours from within CUBIT/Trelis, we use a Python script (\filename{generate\_surfjou.py}) to read the contours file and create a CUBIT/Trelis journal file @@ -566,7 +567,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \end{tikzpicture} \caption{Diagram of Step 2: Prescribed coseismic slip and postseismic relaxation. This quasistatic simulation prescribes - uniform slip on the central rupture patch on the top of the slab, + uniform slip on the central rupture patch on the subduction interface, depth-dependent viscoelastic relaxation in the slab and mantle, and roller boundary conditions on the lateral (north, south, east, and west) and bottom boundaries.} @@ -675,12 +676,16 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} Prescribing the coseismic slip distribution on the fault involves specifying an origin time for the rupture (default is 0.0), and a slip -time function along with its -parameters. In this case, we treat the earthquake rupture as just the -coseismic slip happening in one time step, so we use a step function -for the slip time function (which is the default). The parameters -include the final slip and slip initiation time. Because we want -uniform slip and a uniform rise time, we use \object{UniformDB} +time function along with its parameters. In this case, we treat the +earthquake rupture as just the coseismic slip happening in one time +step, so we use a step function for the slip time function (which is +the default). The parameters include the final slip and slip +initiation time. This slip initiation time is relative to the +earthquake source origin time, which is 0 by default. Thus, to specify +the time of the slip for a step function, we can either specify the +origin time or the slip initiation time; in this case, we use the slip +initiation time. In Step 4 we will use the origin time. Because we +want uniform slip and a uniform rise time, we use \object{UniformDB} spatial databases for both of these. Note that we specify oblique slip with 1.0 m of right-lateral motion and 4.0 m of reverse motion. \begin{cfg} @@ -724,19 +729,20 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \subsubsection{Exercises} \begin{itemize} -\item Change the slip from the top of the slab to the splay fault - rupture patch. Hint: Identify the nodesets for the splay fault - patch. -\item Create simulataneous rupture on the central patch for the splay - fault and top of the slab. +\item Change the slip from the subduction interface rupture patch to + the splay fault rupture patch. Hint: Identify the nodesets for the + splay fault patch. +\item Create simulataneous rupture on the subduction interface rupture + patch and the splay fault rupture patch. \item Prescribe coseismic slip on the central patch for splay fault - and the top of the slab below the intersection with the splay fault. + and the subduction interface below the intersection with the splay fault. \begin{itemize} - \item Implement this without changing the any of the nodesets. Hint: - You will need to create two fault interfaces. What do you notice - about the slip at the intersection between the splay fault and slab? + \item Implement this without changing any of the nodesets in + CUBIT/Trelis. Hint: you will need to create two fault + interfaces. What do you notice about the slip at the intersection + between the splay fault and slab? \item Add nodesets in CUBIT/Trelis to create a uniform coseismic - slip distribution across the splay fault and on the slab interface + slip distribution across the splay fault and on the subduction interface below the splay fault. \end{itemize} \end{itemize} @@ -750,12 +756,12 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} interseismic deformation associated with the subducting slab. We approximate the motion of the Juan de Fuca Plate subducting under the North American Plate by introducing aseismic slip (creep) on the -bottom of the slab and the deeper portion of the top of the slab; we -keep the interface between the top of the slab and the accretionary -wedge and shallow crust locked. As in Step 2, we will use the linear -Maxwell viscoelastic constitutive model for the slab and mantle. -Figure~\ref{fig:example:subduction:3d:step03:diagram} summarizes the -problem description. +bottom of the slab and the deeper portion of the subduction interface; +we keep the interface between the subduction interface and the +accretionary wedge and shallow crust locked. As in Step 2, we will use +the linear Maxwell viscoelastic constitutive model for the slab and +mantle. Figure~\ref{fig:example:subduction:3d:step03:diagram} +summarizes the problem description. \todo{brad}{Add annotation to figure.} \begin{figure}[htbp] @@ -772,21 +778,19 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \end{tikzpicture} \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and interseismic deformation for the subducting slab. We precsribed - steady, uniform creep on the - bottom of the slab and deeper portion of the top of the slab. We - impose roller Dirichlet boundary conditions on the lateral and - bottom boundaries, except where they overlap with the fault - interfaces for the slab.} + steady, uniform creep on the bottom of the slab and deeper portion + of the subduction interface. We impose roller Dirichlet boundary + conditions on the lateral and bottom boundaries, except where they + overlap with the fault interfaces for the slab.} \label{fig:example:subduction:3d:step03:diagram} \end{figure} % Fault With slip on the top and bottom of the slab, our fault interfaces -array contains two components, one for the top of the slab, -\facility{slab\_top}, and one for the bottom of the slab, -\facility{slab\_bottom}. We use the \object{FaultCohesiveKin} -object for each of these interfaces since we want to prescribe the -slip. +array contains two components, one for the top of the slab (subduction +interface), \facility{slab\_top}, and one for the bottom of the slab, +\facility{slab\_bottom}. We use the \object{FaultCohesiveKin} object +for each of these interfaces since we want to prescribe the slip. \begin{cfg} [pylithapp.problem] interfaces = [slab_top, slab_bottom] @@ -808,7 +812,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} tilting slightly to the west. This results in consistent along-strike and up-dip directions across the fault surface. For the aseismic slip we use a constant slip rate time function (\object{ConstRateSlipFn}) -with \object[UniformDB} spatial databases to specify the constant, +with \object{UniformDB} spatial databases to specify the constant, uniform oblique slip rate of 2.0 cm/yr of left-lateral motion and 4.0 cm/yr of normal motion. Note that slip on the bottom of the subducting slab has the opposite sense of motion as that on the top of the slab. @@ -849,9 +853,9 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \end{cfg} % Top of slab -The parameters for the top of the slab closely resemble those for the -bottom of the slab. The main difference is that we use a -\object{SimpleGridDB} to define a depth variation in the slip +The parameters for the top of the slab (subduction interface) closely +resemble those for the bottom of the slab. The main difference is that +we use a \object{SimpleGridDB} to define a depth variation in the slip rate. The fault is locked at depths above 45 km and increases linearly to the same slip rate as the bottom of the slab at a depth of 60 km. \begin{cfg} @@ -887,22 +891,25 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \end{cfg} % Boundary conditions -PyLith does not support an overlap between Dirichlet boundary -conditions and fault interfaces, so we use nodesets that exclude -vertices on the faults for the -x, -y, and +y boundaries rather than -the nodesets that include all vertices on those boundaries. +We do not want the boundaries to constrain the motion of the +subducting slab, so we use the nodesets that exclude vertices on the +subducting slab. Furthermore, PyLith does not permit overlap between +the fault interfaces and Dirichlet boundary conditions. This is why +we exclude vertices on the splay fault in these nodesets as well. We +only update the name of the nodeset for the -x, -y, and +y +boundaries. \begin{cfg} # -x face [pylithapp.problem.bc.x_neg] -

    label

    = boundary_xneg_nofault +

    label

    = boundary_xneg_noslab # -y face [pylithapp.problem.bc.y_neg] -

    label

    = boundary_yneg_nofault +

    label

    = boundary_yneg_noslab # +y face [pylithapp.problem.bc.y_pos] -

    label

    = boundary_ypos_nofault +

    label

    = boundary_ypos_noslab \end{cfg} We run this example by typing @@ -918,7 +925,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} intersection of the boundaries and fault surfaces. \begin{figure} - %\includegraphics[width=5.0in]{examples/figs/subduction3d_step03_soln} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step03_soln} \caption{Solution over the domain for Step 2 at $t=200 \mathrm{yr}$. The colors indicate the x-displacement and we have exaggerated the deformation by a factor of 5,000.} @@ -929,7 +936,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \subsubsection{Exercises} \begin{itemize} -\item Adjust the locking depth for the top of the slab. How does this +\item Adjust the locking depth for the subduction interface. How does this affect the spatial distribution of the change in tractions on the fault interfaces? \item Increase the rigidity of the slab and decrease the rigidity of @@ -941,14 +948,190 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 4: Prescribed Earthquake Cycle} -\subsubsection{Exercises} +In Step 4, We combine the interseismic deformation in Step 3 with the +coseismic slip in Step 2 to simulate two earthquake cycles. We also +include an earthquake on the splay fault. This illustrates how to +include multiple earthquake sources on a single fault. We use the same +roller Dirichlet boundary conditions and combination of elastic and +viscoelatic materials as we did in Step 3. + +\todo{brad}{Add annotation to figure.} +\begin{figure}[htbp] + \begin{tikzpicture} + \tikzstyle{annotation} = [black]; + \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; + %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); + %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; + %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); + \end{scope} + \end{tikzpicture} + \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and + interseismic deformation for the subducting slab. We precsribed + steady, uniform creep on the bottom of the slab and deeper portion + of the subduction interface. We impose roller Dirichlet boundary + conditions on the lateral and bottom boundaries, except where they + overlap with the fault interfaces for the slab.} + \label{fig:example:subduction:3d:step03:diagram} +\end{figure} + +% Faults +We create an array of three fault interfaces, one for the top of the +slab (subduction interface), one for the bottom of the slab, and one +for the splay fault. The splay fault terminates into the fault on the +top of the slab, so we must list the through-going fault on the top of +the slab first. +\begin{cfg} +# We prescribe slip on the top and bottom of the slab and on the splay fault. +[pylithapp.problem] +interfaces = [slab_top, slab_bottom, splay] + +[pylithapp.problem.interfaces] +slab_top = pylith.faults.FaultCohesiveKin +slab_bottom = pylith.faults.FaultCohesiveKin +splay = pylith.faults.FaultCohesiveKin +\end{cfg} + +\important{When including intersecting faults, the through-going fault + must be listed first in the array of fault interfaces. This ensures + its cohesive cells are created before the adjacent fault that + terminates into the through-going fault. For nonintersecting faults, + the order in the list of fault interfaces does not matter.} + +% Fault: slab_bottom and slab top +The settings for the fault interface on the bottom of the slab match +those used in Step 3. For the subduction interface, we want to +impose creep on the deeper portion and earthquakes (coseismic slip) at +specific times on the upper portion. We create an array of earthquake +sources, one for the creep and one for each of the earthquakes. We +want the earthquake to be imposed at specific times, so we set their +origin time equal to the desire rupture time (100 years and 200 years) +minus a value much smaller than the time step, so that roundoff errors +do not result in the ruptures occuring one time step later than +intended. We use the same settings as we did in Step 3 for the creep +earthquake source. For the coseismic slip, we use a +\object{SimpleGridDB} to impose a depth-dependent slip distribution +that exactly complements the depth-dependent slip distribution of the +creep. Note that the slip time within an earthquake rupture is +relative to the origin time, so we set the slip time to zero to +coincide with the specified origin time. +\begin{cfg} +[pylithapp.problem.interfaces.slab_top] +# --- Skipping lines already discussed in Step 3 --- +eq_srcs = [creep, eq1, eq2] +

    eq_srcs.creep.origin_time

    = 0.0*year +

    eq_srcs.eq1.origin_time

    = 99.999*year ; 100*yr - small value +

    eq_srcs.eq2.origin_time

    = 199.999*year l 200*yr - small value + +# Use the constant slip rate time function for the creep earthquake source. +eq_srcs.creep.slip_function = pylith.faults.ConstRateSlipFn + +# Creep +[pylithapp.problem.interfaces.slab_top.eq_srcs.creep.slip_function] +slip_rate = spatialdata.spatialdb.SimpleGridDB +

    slip_rate.label

    = Slab top slip rate. +

    slip_rate.filename

    = spatialdb/fault_slabtop_creep.spatialdb +

    slip_rate.query_type

    = linear + +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] ; Slip time is relative to origin time + +# Earthquake 1 +[pylithapp.problem.interfaces.slab_top.eq_srcs.eq1.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +

    slip.label

    = Slab top slip rate. +

    slip.filename

    = spatialdb/fault_slabtop_coseismic.spatialdb +

    slip.query_type

    = linear + +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] ; Slip time is relative to origin time. + +# Earthquake 2 (same as earthquake 1) +[pylithapp.problem.interfaces.slab_top.eq_srcs.eq2.slip_function] +slip = spatialdata.spatialdb.SimpleGridDB +

    slip.label

    = Slab top slip rate. +

    slip.filename

    = spatialdb/fault_slabtop_coseismic.spatialdb +

    slip.query_type

    = linear + +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] ; Slip time is relative to origin time. +# --- Omitting output settings already discussed --- +\end{cfg} + +The settings for the splay fault look very similar to those for the +coseismic slip on the slab rupture patch in Step 2. The primary +difference is that we specify an origin time of 250 years. + +% Fault: splay +\begin{cfg} +[pylithapp.problem.interfaces.splay] +

    id

    = 102 ; id must be unique across all materials and faults +

    label

    = fault_splay ; Nodeset for the entire fault surface +

    edge

    = fault_splay_edge ; Nodeset for the buried edges + +# We must define the quadrature information for fault cells. +# The fault cells are 2D (surface). +quadrature.cell = pylith.feassemble.FIATSimplex +

    quadrature.cell.dimension

    = 2 + +# Origin time for splay fault earthquake. +

    eq_srcs.rupture.origin_time

    = 249.999*year + +# The slip time and final slip are defined in spatial databases. +[pylithapp.problem.interfaces.splay.eq_srcs.rupture.slip_function] +slip = spatialdata.spatialdb.UniformDB +

    slip.label

    = Splay fault slip. +

    slip.values

    = [left-lateral-slip, reverse-slip, fault-opening] +

    slip.data

    = [-1.0*m, 2.0*m, 0.0*m] -% Make lower slab + splay fault the primary fault surface and the -% upper slab (trench side of the splay fault) the secondary fault -% surface. Hint: You will need to create a nodesets in CUBIT that -% correspond to the primary and secondary fault surfaces. +slip_time = spatialdata.spatialdb.UniformDB +

    slip_time.label

    = Slip initiation time +

    slip_time.values

    = [slip-time] +

    slip_time.data

    = [0.0*year] ; Relative to the origin time +# --- Omitting output settings already discussed --- +\end{cfg} +We run this example by typing +\begin{shell} +$$ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +\end{shell} +Figure \vref{fig:example:subduction:3d:step04}, which was created +using the ParaView Python script \filename{plot\_dispwarp.py}, shows +the deformation exaggerated by a factor of 5,000 at the final time +step of t=300*yr. Compared to the solution in Step 3, we see the +earthquakes have reduced the deformation in the crust and accretionary +wedge. + +\begin{figure} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step04_soln} + \caption{Solution over the domain for Step 4 at $t=300 \mathrm{yr}$. The colors indicate + the z-displacement and we have exaggerated the + deformation by a factor of 5,000.} + \label{fig:example:subduction:3d:step04} +\end{figure} + +\subsubsection{Exercises} + +\begin{itemize} + \item Adjust the timing of the earthquake rupture sequence. How does + this affect the deformation? + \item Add additional earthquakes with different depth variations in + slip, keeping the total equal to the overall slip rate. + \item Adjust the nodesets in CUBIT/Trelis so that the splay fault + and the deeper portion of the subduction interface form the + through-going fault and the upper portion of the subduction + interface is the secondary fault. How does this affect the stress + accumulation in the crust and upper mantle? +\end{itemize} % ---------------------------------------------------------------------- \subsection{Step 5: Spontaneous Rupture Driven by Subducting Slab} @@ -1482,7 +1665,7 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} \end{cfg} Then, for each material, we use the same spatial database for the initial stresses. We use linear interpolation and in the database the -initial stress is simply computed as $\{rho}_mgh$, where $\{rho}_m$ is +initial stress is simply computed as $\rho_mgh$, where $\rho_m$ is the density of the mantle material and $h$ is the depth below the ground surface: \begin{cfg} diff --git a/examples/3d/subduction/mesh/bc.jou b/examples/3d/subduction/mesh/bc.jou index b701ffcd56..b329b0df43 100644 --- a/examples/3d/subduction/mesh/bc.jou +++ b/examples/3d/subduction/mesh/bc.jou @@ -43,6 +43,10 @@ block 4 name "crust" # Create nodesets for faults and boundary conditions. # ---------------------------------------------------------------------- +# Create group for slab, so that we can easily remove the overlap with +# boundaries to prevent constraining the subduction of the slab. +group "block_slab" add node in v_domain + # ---------------------------------------------------------------------- # FAULT INTERFACES # ---------------------------------------------------------------------- @@ -140,22 +144,34 @@ group "boundary_xneg_nofault" remove node in group fault_slabbot nodeset 82 group boundary_xneg_nofault nodeset 82 name "boundary_xneg_nofault" +# -x w/o slab +group "boundary_xneg_noslab" add node in group boundary_xneg +group "boundary_xneg_noslab" remove node in group block_slab +nodeset 83 group boundary_xneg_noslab +nodeset 83 name "boundary_xneg_noslab" # +y group "boundary_ypos" add node in surface 18 group "boundary_ypos" add node in surface 45 group "boundary_ypos" add node in surface 48 group "boundary_ypos" add node in surface 39 -nodeset 83 group boundary_ypos -nodeset 83 name "boundary_ypos" +nodeset 84 group boundary_ypos +nodeset 84 name "boundary_ypos" # +y w/o fault group "boundary_ypos_nofault" add node in group boundary_ypos group "boundary_ypos_nofault" remove node in group fault_slabtop group "boundary_ypos_nofault" remove node in group fault_slabbot group "boundary_ypos_nofault" remove node in group fault_splay -nodeset 84 group boundary_ypos_nofault -nodeset 84 name "boundary_ypos_nofault" +nodeset 85 group boundary_ypos_nofault +nodeset 85 name "boundary_ypos_nofault" + +# +y w/o slab +group "boundary_ypos_noslab" add node in group boundary_ypos +group "boundary_ypos_noslab" remove node in group block_slab +group "boundary_ypos_noslab" remove node in group fault_splay +nodeset 86 group boundary_ypos_noslab +nodeset 86 name "boundary_ypos_noslab" # -y @@ -163,29 +179,35 @@ group "boundary_yneg" add node in surface 21 group "boundary_yneg" add node in surface 43 group "boundary_yneg" add node in surface 50 group "boundary_yneg" add node in surface 36 -nodeset 85 group boundary_yneg -nodeset 85 name "boundary_yneg" +nodeset 87 group boundary_yneg +nodeset 87 name "boundary_yneg" # -y w/o fault group "boundary_yneg_nofault" add node in group boundary_yneg group "boundary_yneg_nofault" remove node in group fault_slabtop group "boundary_yneg_nofault" remove node in group fault_slabbot group "boundary_yneg_nofault" remove node in group fault_splay -nodeset 86 group boundary_yneg_nofault -nodeset 86 name "boundary_yneg_nofault" +nodeset 88 group boundary_yneg_nofault +nodeset 88 name "boundary_yneg_nofault" + +# -y w/o slab +group "boundary_yneg_noslab" add node in group boundary_yneg +group "boundary_yneg_noslab" remove node in group block_slab +group "boundary_yneg_noslab" remove node in group fault_splay +nodeset 89 group boundary_yneg_noslab +nodeset 89 name "boundary_yneg_noslab" # -z group "boundary_zneg" add node in surface 10 -nodeset 87 group boundary_zneg -nodeset 87 name "boundary_zneg" +nodeset 90 group boundary_zneg +nodeset 90 name "boundary_zneg" # +z group "boundary_zpos" add node in surface 47 group "boundary_zpos" add node in surface 42 group "boundary_zpos" add node in surface 19 -nodeset 88 group boundary_zpos -nodeset 88 name "boundary_zpos" +nodeset 91 group boundary_zpos +nodeset 91 name "boundary_zpos" # End of file - diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index 1f9d8c363c..7c7a93da5c 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -65,23 +65,25 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -# Because the slab intersects the boundaries of the domain, and PyLith -# does not permit overlap between the fault interfaces and Dirichlet -# boundary conditions, for the Dirichlet boundary conditions we use -# the nodesets which exclude vertices on the fault. We only update the -# name of the nodeset for the -x, -y, and +y boundaries. +# We do not want the boundaries to constrain the motion of the +# subducting slab, so we use the nodesets that exclude vertices on the +# subducting slab. Furthermore, PyLith does not permit overlap between +# the fault interfaces and Dirichlet boundary conditions. This is why +# we exclude vertices on the splay fault in these nodesets as well. We +# only update the name of the nodeset for the -x, -y, and +y +# boundaries. # -x face [pylithapp.problem.bc.x_neg] -label = boundary_xneg_nofault +label = boundary_xneg_noslab # -y face [pylithapp.problem.bc.y_neg] -label = boundary_yneg_nofault +label = boundary_yneg_noslab # +y face [pylithapp.problem.bc.y_pos] -label = boundary_ypos_nofault +label = boundary_ypos_noslab # ---------------------------------------------------------------------- # faults diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index 3f3bbe3f49..c3dc76c25d 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -67,29 +67,34 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -# Because the slab intersects the boundaries of the domain, and PyLith -# does not permit overlap between the fault interfaces and Dirichlet -# boundary conditions, for the Dirichlet boundary conditions we use -# the nodesets which exclude vertices on the fault. We only update the -# name of the nodeset for the -x, -y, and +y boundaries. +# We do not want the boundaries to constrain the motion of the +# subducting slab, so we use the nodesets that exclude vertices on the +# subducting slab. Furthermore, PyLith does not permit overlap between +# the fault interfaces and Dirichlet boundary conditions. This is why +# we exclude vertices on the splay fault in these nodesets as well. We +# only update the name of the nodeset for the -x, -y, and +y +# boundaries. # -x face [pylithapp.problem.bc.x_neg] -label = boundary_xneg_nofault +label = boundary_xneg_noslab # -y face [pylithapp.problem.bc.y_neg] -label = boundary_yneg_nofault +label = boundary_yneg_noslab # +y face [pylithapp.problem.bc.y_pos] -label = boundary_ypos_nofault +label = boundary_ypos_noslab # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- [pylithapp.problem] -# We prescribe slip on the top and bottom of the slab and on the splay fault. +# We prescribe slip on the top and bottom of the slab and on the splay +# fault. Because the splay fault terminates into the through-going +# fault on the top of the slab, we must list the splay fault AFTER the +# fault for the top of the slab. interfaces = [slab_top, slab_bottom, splay] [pylithapp.problem.interfaces] @@ -99,9 +104,9 @@ splay = pylith.faults.FaultCohesiveKin # Slab top ------------------------------------------------------------- [pylithapp.problem.interfaces.slab_top] -id = 100 -label = fault_slabtop -edge = fault_slabtop_edge +id = 100 ; id must be unique across all materials and faults +label = fault_slabtop ; Nodeset for the entire fault surface +edge = fault_slabtop_edge ; Nodeset for the buried edges # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). @@ -165,9 +170,9 @@ vertex_info_fields = [normal_dir, strike_dir, dip_dir] # Slab bottom ---------------------------------------------------------- [pylithapp.problem.interfaces.slab_bottom] -id = 101 -label = fault_slabbot -edge = fault_slabbot_edge +id = 101 ; id must be unique across all materials and faults +label = fault_slabbot ; Nodeset for the entire fault surface +edge = fault_slabbot_edge ; Nodeset for the buried edges up_dir = [-0.1,0,0.9] # We must define the quadrature information for fault cells. @@ -198,9 +203,9 @@ vertex_info_fields = [normal_dir, strike_dir, dip_dir] # Splay ---------------------------------------------------------------- [pylithapp.problem.interfaces.splay] -id = 102 -label = fault_splay -edge = fault_splay_edge +id = 102 ; id must be unique across all materials and faults +label = fault_splay ; Nodeset for the entire fault surface +edge = fault_splay_edge ; Nodeset for the buried edges # We must define the quadrature information for fault cells. # The fault cells are 2D (surface). From 2bffad7bc7d0d59ad89304e3ed64ec46ab786301 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 09:24:22 -0700 Subject: [PATCH 124/216] Added note about conflicting Python from Anaconda, HomeBrew, etc. --- doc/userguide/install/install.tex | 4 +++- 1 file changed, 3 insertions(+), 1 deletion(-) diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index 117899ca41..00af507b9b 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -83,7 +83,9 @@ \subsection{Linux and Max OS X} Python. This means the system Python must be in your path to use the PyLith binary executable; ensure \filename{/bin} and \filename{/usr/bin} are at the beginning of the PATH environment - variable before sourcing \filename{setup.sh}.} + variable before sourcing \filename{setup.sh}. {\bf This usually + applies if you have Python installed from Anaconda, HomeBrew, + MacPorts, etc.}} \subsection{Extending PyLith and/or Integrating Other Software Into PyLith} \newfeature{v.2.2.0} From 6eb6c29392a2d2ab49d73d5a84670b0655b52429 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 12:28:41 -0700 Subject: [PATCH 125/216] Updated table of features. --- doc/userguide/examples/examples_info.py | 33 ++-- doc/userguide/examples/subduction3d.py | 152 +++++++++++++++++- .../examples/subduction3d_features.tex | 65 ++++++-- 3 files changed, 226 insertions(+), 24 deletions(-) diff --git a/doc/userguide/examples/examples_info.py b/doc/userguide/examples/examples_info.py index 3630662fc9..7702e631ef 100755 --- a/doc/userguide/examples/examples_info.py +++ b/doc/userguide/examples/examples_info.py @@ -57,16 +57,16 @@ class Features(object): PRECOND_ILU = "ILU" PRECOND_ASM = "ASM" PRECOND_SCHUR = "SCHUR" - PRECOND_CUSTOM = "CUST" + PRECOND_CUSTOM = "Cust" PRECOND_ML = "ML" PRECOND_GAMG = "GAMG" - PRECOND_ML_CUSTOM = "ML+CUST" + PRECOND_ML_CUSTOM = "ML+Cust" - SLIPFN_STEP = "STEP" - SLIPFN_RATE = "RATE" - SLIPFN_LIU = "LIU" - SLIPFN_BRUNE = "BRUNE" - SLIPFN_TIMEHISTORY = "USER" + SLIPFN_STEP = "Step" + SLIPFN_RATE = "Rate" + SLIPFN_LIU = "Liu" + SLIPFN_BRUNE = "Brune" + SLIPFN_TIMEHISTORY = "User" STRAINFORM_INFINITESIMAL = "Inf" STRAINFORM_FINITE = "Fin" @@ -81,9 +81,17 @@ class Features(object): # Properties OrderedDict(( ("Dimension", { "enum": [2, 3], }), - ("Coordinate system", { "enum": [CS_CART, CS_PROJ], }), - ("Mesh generator", { "enum": [MESH_ASCII, MESH_CUBIT, MESH_LAGRIT], }), - ("Cells", { "enum": [CELL_TRI, CELL_QUAD, CELL_TET, CELL_HEX], }), + ("Coordinate system", { + "enum": [CS_CART, CS_PROJ], + "description": "%s: Cartesian, %s: geographic projection" % (CS_CART, CS_PROJ), + }), + ("Mesh generator", { + "enum": [MESH_ASCII, MESH_CUBIT, MESH_LAGRIT], + "description": "%s: ASCII, %s: CUBIT/Trelis, %s: LaGriT" % (MESH_ASCII, MESH_CUBIT, MESH_LAGRIT), + }), + ("Cells", { + "enum": [CELL_TRI, CELL_QUAD, CELL_TET, CELL_HEX], + }), ("Refinement", { "enum": [REFINE_2, REFINE_4, REFINE_8], }), ("Reordering", { "type": "boolean", }), ("Problem type", { @@ -170,7 +178,10 @@ class Features(object): ("Output", # Properties OrderedDict(( - ("Format", { "enum": [OUTPUT_VTK, OUTPUT_HDF5, OUTPUT_HDF5EXT], }), + ("Format", { + "enum": [OUTPUT_VTK, OUTPUT_HDF5, OUTPUT_HDF5EXT], + "description": "%s: VTK, %s: HDF5, %s: HDF5 w/external datasets" % (OUTPUT_VTK, OUTPUT_HDF5, OUTPUT_HDF5EXT), + }), ("Domain output", { "type": "integer", "minimum": 0, }), ("Surface output", { "type": "integer", "minimum": 0, }), ("Point output", { "type": "integer", "minimum": 0, }), diff --git a/doc/userguide/examples/subduction3d.py b/doc/userguide/examples/subduction3d.py index c5c935bc3b..f33d7eb6c5 100644 --- a/doc/userguide/examples/subduction3d.py +++ b/doc/userguide/examples/subduction3d.py @@ -231,7 +231,7 @@ "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, }, "Solver": { - "Solver": Features.SOLVER_NONLINEAR, + "Solver": Features.SOLVER_LINEAR, "Preconditioner": Features.PRECOND_ML_CUSTOM, "Time stepping": Features.TS_BWDEULER, }, @@ -252,4 +252,154 @@ } +examples["3d/subduction/step07a,b"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_GREENSFNS, + "Time dependence": Features.TIMEDEP_STATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Fault": { + "Prescribed slip": 1, + "Slip time function": Features.SLIPFN_STEP, + }, + "Bulk Rheology": { + "Linear elastic": 4, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Surface output": 1, + "Point output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Uniform": 1, + "Simple": 4, + }, +} + + +examples["3d/subduction/step08a"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_STATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Bulk Rheology": { + "Linear elastic": 4, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + "Reference state": True, + "Gravity": True, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Simple": 4, + }, +} + + +examples["3d/subduction/step08b"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_STATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Bulk Rheology": { + "Linear elastic": 4, + "Stress/strain formulation": Features.STRAINFORM_INFINITESIMAL, + "Reference state": True, + "Gravity": True, + }, + "Solver": { + "Solver": Features.SOLVER_LINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Simple": 4, + }, +} + + +examples["3d/subduction/step08c"] = { + "General": { + "Dimension": 3, + "Coordinate system": Features.CS_PROJ, + "Mesh generator": Features.MESH_CUBIT, + "Cells": Features.CELL_TET, + "Problem type": Features.PROB_TIMEDEPENDENT, + "Time dependence": Features.TIMEDEP_QUASISTATIC, + "Reordering": True, + }, + "Boundary Condition": { + "Dirichlet": 5, + }, + "Bulk Rheology": { + "Linear elastic": 2, + "Linear Maxwell viscoelastic": 2, + "Stress/strain formulation": Features.STRAINFORM_FINITE, + "Reference state": True, + "Gravity": True, + }, + "Solver": { + "Solver": Features.SOLVER_NONLINEAR, + "Preconditioner": Features.PRECOND_ML_CUSTOM, + "Time stepping": Features.TS_BWDEULER, + }, + "Output": { + "Format": Features.OUTPUT_HDF5, + "ParaView": True, + "Domain output": 1, + "Surface output": 1, + "State variable output": 4, + }, + "Spatial Database": { + "Simple": 4, + }, +} + + # End of file diff --git a/doc/userguide/examples/subduction3d_features.tex b/doc/userguide/examples/subduction3d_features.tex index 9e2c4a9ebf..6a490d8b4f 100644 --- a/doc/userguide/examples/subduction3d_features.tex +++ b/doc/userguide/examples/subduction3d_features.tex @@ -44,32 +44,52 @@ \\ \hline 3d/subduction/step02 & 3 & Proj & CUBIT & Tet & & \yes & TD & QS -& L & ML+CUST & BE +& L & ML+Cust & BE & x2 & x3 & x2 & x2 & \\ \hline 3d/subduction/step03 & 3 & Proj & CUBIT & Tet & & \yes & TD & QS -& L & ML+CUST & BE +& L & ML+Cust & BE & x4 & x3 & x2 & x2 & \\ \hline 3d/subduction/step04 & 3 & Proj & CUBIT & Tet & & \yes & TD & QS -& L & ML+CUST & BE +& L & ML+Cust & BE & x7 & x3 & x5 & x2 & \\ \hline 3d/subduction/step05 & 3 & Proj & CUBIT & Tet & & \yes & TD & QS -& NL & ML+CUST & BE +& NL & ML+Cust & BE & x7 & x3 & x5 & x2 & \\ \hline 3d/subduction/step06 & 3 & Proj & CUBIT & Tet & & \yes & TD & QS -& NL & ML+CUST & BE +& L & ML+Cust & BE & x1 & x4 & x1 & & x1 \\ \hline +3d/subduction/step07a,b +& 3 & Proj & CUBIT & Tet & & \yes & GF & S +& L & ML+Cust & BE +& x1 & x4 & & & +\\ \hline +3d/subduction/step08a +& 3 & Proj & CUBIT & Tet & & \yes & TD & S +& L & ML+Cust & +& & x4 & & & +\\ \hline +3d/subduction/step08b +& 3 & Proj & CUBIT & Tet & & \yes & TD & S +& L & ML+Cust & +& & x4 & & & +\\ \hline +3d/subduction/step08c +& 3 & Proj & CUBIT & Tet & & \yes & TD & QS +& NL & ML+Cust & BE +& & x4 & & & +\\ \hline \end{tabular}} \par -{\bf Problem type} -- TD: time dependent, GF: Green's functions. {\bf Time dependence} -- S: static, QS: quasi-static, D: dynamic. {\bf Solver} -- L: linear, NL: nonlinear. {\bf Preconditioner} -- ILU: ILU, ASM: Additive Schwarz, SCHUR: Schur complement, CUST: custom, ML: ML algebraic multigrid, GAMG: geometric algebraic multigrid. {\bf Time stepping} -- BE: Backward Euler, FE: Forward Euler. \\ +{\bf Coordinate system} -- Cart: Cartesian, Proj: geographic projection. {\bf Mesh generator} -- ASCII: ASCII, CUBIT: CUBIT/Trelis, LaGriT: LaGriT. {\bf Problem type} -- TD: time dependent, GF: Green's functions. {\bf Time dependence} -- S: static, QS: quasi-static, D: dynamic. {\bf Solver} -- L: linear, NL: nonlinear. {\bf Preconditioner} -- ILU: ILU, ASM: Additive Schwarz, SCHUR: Schur complement, Cust: custom, ML: ML algebraic multigrid, GAMG: geometric algebraic multigrid. {\bf Time stepping} -- BE: Backward Euler, FE: Forward Euler. \\ \rowcolors{2}{yellow!30}{white} \resizebox{\textwidth}{!}{% \begin{tabular}{|l|%% Example @@ -131,34 +151,55 @@ \\ \hline 3d/subduction/step02 & x5 & & & -& x1 & STEP & & & & & & +& x1 & Step & & & & & & & x2 & x2 & & & & Inf & & & & H5 & x1 & x1 & & x4 & \yes & \\ \hline 3d/subduction/step03 & x5 & & & -& x2 & RATE & & & & & & +& x2 & Rate & & & & & & & x2 & x2 & & & & Inf & & & & H5 & x1 & x1 & & x4 & \yes & \\ \hline 3d/subduction/step04 & x5 & & & -& x3 & STEP & & & & & & +& x3 & Step & & & & & & & x2 & x2 & & & & Inf & & & & H5 & x1 & x1 & & x4 & \yes & \\ \hline 3d/subduction/step05 & x5 & & & -& x1 & RATE & x1 & & \yes & & & \yes +& x1 & Rate & x1 & & \yes & & & \yes & x2 & x2 & & & & Inf & & & & H5 & x1 & x1 & & x4 & \yes & \\ \hline 3d/subduction/step06 & x5 & & & -& x1 & USER & & & & & & +& x1 & User & & & & & & & x4 & & & & & Inf & & & & H5 & x1 & x1 & x1 & x4 & \yes & \\ \hline +3d/subduction/step07a,b +& x5 & & & +& x1 & Step & & & & & & +& x4 & & & & & Inf & & & +& H5 & & x1 & x1 & x4 & \yes & +\\ \hline +3d/subduction/step08a +& x5 & & & +& & & & & & & & & x4 & & & & & Inf & & \yes & \yes +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step08b +& x5 & & & +& & & & & & & & & x4 & & & & & Inf & & \yes & \yes +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline +3d/subduction/step08c +& x5 & & & +& & & & & & & & & x2 & x2 & & & & Fin & & \yes & \yes +& H5 & x1 & x1 & & x4 & \yes & +\\ \hline \end{tabular}} \par -{\bf Stress/strain formulation} -- Inf: infinitesimal, Fin: small, finite strain. \\ +{\bf Stress/strain formulation} -- Inf: infinitesimal, Fin: small, finite strain. {\bf Format} -- VTK: VTK, H5: HDF5, H5Ext: HDF5 w/external datasets. \\ From 9528a137afebf3b1d82aad146616a65fbaefebf1 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 13:32:33 -0700 Subject: [PATCH 126/216] Small tweaks to coments. --- examples/3d/subduction/step03.cfg | 2 +- examples/3d/subduction/step04.cfg | 4 ++-- 2 files changed, 3 insertions(+), 3 deletions(-) diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index 7c7a93da5c..add152c1cf 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -30,7 +30,7 @@ # # Fault # Uniform creep on the bottom of the slab. -# Uniform creep on the deeper portion of the top of the slab. +# Uniform creep on the deeper portion of the subduction interface. # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index c3dc76c25d..4394a9d269 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -30,8 +30,8 @@ # # Fault # + Uniform creep on the bottom of the slab. -# + Uniform creep on the deeper portion of the top of the slab. -# + Coseismic slip on the shallow portion of the top of the slab. +# + Uniform creep on the deeper portion of the subduction interface. +# + Coseismic slip on the shallow portion of the subduction interface. # + Coseismic slip on the splay fault. # # ---------------------------------------------------------------------- From bded9176a5497bbd15dfd441e4464b1afccd62bd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 13:33:47 -0700 Subject: [PATCH 127/216] Keep data fields for surface output turned on (useful for visualization). --- examples/3d/subduction/step07a.cfg | 4 ++-- examples/3d/subduction/step07b.cfg | 4 ++-- 2 files changed, 4 insertions(+), 4 deletions(-) diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 18892a76e5..391879cb0e 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -92,8 +92,8 @@ vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] writer.filename = output/step07a-groundsurf.h5 -# Turn off data fields. -vertex_data_fields = [] +# Uncomment to turn off data fields. +#vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] writer = pylith.meshio.DataWriterHDF5 diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index 3b867146cd..bdd3eee36f 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -92,8 +92,8 @@ vertex_data_fields = [] [pylithapp.problem.formulation.output.subdomain] writer.filename = output/step07b-groundsurf.h5 -# Turn off data fields. -vertex_data_fields = [] +# Uncomment to turn off data fields. +#vertex_data_fields = [] [pylithapp.problem.formulation.output.cgps_sites] writer = pylith.meshio.DataWriterHDF5 From 35dc2b4a638cf71e522664f36d3f255e093b2231 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 13:35:55 -0700 Subject: [PATCH 128/216] Added diagrams for steps 1,3,4. --- .../figs/subduction3d_step01_diagram.pdf | Bin 0 -> 44582 bytes .../figs/subduction3d_step01_diagram.tex | 27 ++++++++ .../figs/subduction3d_step03_diagram.pdf | Bin 0 -> 46158 bytes .../figs/subduction3d_step03_diagram.tex | 35 ++++++++++ .../figs/subduction3d_step04_diagram.pdf | Bin 0 -> 46271 bytes .../figs/subduction3d_step04_diagram.tex | 36 ++++++++++ doc/userguide/examples/subduction3d.tex | 62 +++++------------- 7 files changed, 115 insertions(+), 45 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_step01_diagram.pdf create mode 100644 doc/userguide/examples/figs/subduction3d_step01_diagram.tex create mode 100644 doc/userguide/examples/figs/subduction3d_step03_diagram.pdf create mode 100644 doc/userguide/examples/figs/subduction3d_step03_diagram.tex create mode 100644 doc/userguide/examples/figs/subduction3d_step04_diagram.pdf create mode 100644 doc/userguide/examples/figs/subduction3d_step04_diagram.tex diff --git a/doc/userguide/examples/figs/subduction3d_step01_diagram.pdf b/doc/userguide/examples/figs/subduction3d_step01_diagram.pdf new file mode 100644 index 0000000000000000000000000000000000000000..c4768fd789bedda1d8e19400d4aa0e164e9d3c10 GIT binary patch literal 44582 zcmce-cT|(#(l(rsPz8Y?y@h~uB=imeK>{M6q7;?hi}a$j&_R^myMO`$(h-mnK#Ft( zrS}ffI|zI?p5J-C=Uw0T$NSGYuE@%|v$OY}Ju}x_GkbDdQ}G_3z#S2y+XKUGqeQ}R zB;4NEnn+rjh+pfKgBhG(N5k0K%*2I=|FNsF%ikyW?49h0_!SiFJ>bufz<2@V-~TU& z_^&_t`z-+?{s%@bPFBDO0bm61`So95#3M6jdsinDGiSI6@Z=E@zna-g3l~ecfC&7b zf50qOwk~E)aQ=I?MlNQGW+wKgW<;{GM9wZwW=3{I9^*r#eVUwovp6993-At+*-O)Z zJ^|icZ(R(S_`f59_YG;u-}1GeU^|_k_5%-2aFWLf78*Z*%$wzJ(+N|F7Y@_ff4nM1XAb zg7PtpMMJtVPYDH`db3IPGkd^PzTm|Bw`;vJ`c{^L=UW*cA7>d{`z%A&Vch#`B^a!L zHMKl9oB8VNvXH)YMWjb$8G%oskoB<7wT7kxDJ~sux^lpeI41a);re 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100644 index 0000000000..0e03cfdda8 --- /dev/null +++ b/doc/userguide/examples/figs/subduction3d_step01_diagram.tex @@ -0,0 +1,27 @@ +\documentclass[crop,tikz]{standalone} +\usepackage{tikz} +\usetikzlibrary{shadows.blur} + +\begin{document} + +\usetikzlibrary{arrows,shapes} +\input{../../palettes/figcolors} + +\tikzstyle{annotation} = [black, font={\bf}] +\tikzstyle{arrow} = [annotation, >=latex, ->, ultra thick] +\tikzstyle{image} = [anchor=south west,inner sep=0] + + +\begin{tikzpicture} + + \node[image] (image) at (0,0) {\includegraphics[width=5.5in]{subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + \node[anchor=west, annotation] (xneg) at (-0.15,0.6) {+2.0 m}; + \draw[arrow] (xneg) -- (0.15,0.6); + \node[anchor=east, annotation] (xpos) at (+1.15,0.6) {-2.0 m}; + \draw[arrow] (xpos) -- (0.85,0.6); + \end{scope} + +\end{tikzpicture} + +\end{document} diff --git a/doc/userguide/examples/figs/subduction3d_step03_diagram.pdf 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interface (deep) + \node[anchor=east, annotation] (creep) at (0.50,0.45) {Creep}; + \draw[arrow] (creep.north) -- (0.60,0.65); + \draw[arrow] (creep.north) -- (0.60,0.55); + \draw[arrow] (creep.north) -- (0.30,0.68); + + % Subduction interface: shallow + \node[anchor=east, annotation] (locked) at (0.30,0.72) {Locked}; + \draw[arrow] (locked) -- (0.38,0.76); + + % Slab not include in BC + \node[anchor=east, annotation, text width=1.0in] (bcnote) at (0,0.90) {Exclude slab\\ from Dirichlet BCs}; + \draw[arrow] (bcnote) -- (0.10,0.85); + \end{scope} + +\end{tikzpicture} + +\end{document} diff --git a/doc/userguide/examples/figs/subduction3d_step04_diagram.pdf b/doc/userguide/examples/figs/subduction3d_step04_diagram.pdf new file mode 100644 index 0000000000000000000000000000000000000000..6b248b4f535749fcbfa93522601316e3b59954d2 GIT binary patch literal 46271 zcmZttbySpJ)IJW+Ftl`+Fm%h1(hNuph=7U`D%~xO)X=4Lw}iAb0ulpANFylS4blw) zzZ*Y3&-;AWdRgS&I#OyP#DzS$O>0d5|>Za 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[anchor=south west,inner sep=0] + + +\begin{tikzpicture} + + \node[image] (image) at (0,0) {\includegraphics[width=5.5in]{subduction3d_geometry}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + % Bottom of slab, subduction interface (deep) + \node[anchor=east, annotation] (creep) at (0.50,0.45) {Creep}; + \draw[arrow] (creep.north) -- (0.60,0.65); + \draw[arrow] (creep.north) -- (0.60,0.55); + \draw[arrow] (creep.north) -- (0.30,0.68); + + % Subduction interface: shallow + \node[anchor=east, annotation] (eqs) at (0.35,0.72) {Earthquakes}; + \draw[arrow] (eqs.east) -- (0.41,0.78); + \draw[arrow] (eqs.east) -- (0.45,0.74); + + % Slab not include in BC + \node[anchor=east, annotation, text width=1.0in] (bcnote) at (0,0.90) {Exclude slab\\ from Dirichlet BCs}; + \draw[arrow] (bcnote) -- (0.10,0.85); + \end{scope} + +\end{tikzpicture} + +\end{document} diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index e6a374cd11..f3d63f81f1 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -78,7 +78,6 @@ \subsection{Features Illustrated} GUI, although the interaction is limited to rotating, translating, and zooming when run outside the ParaView GUI. -\todo{brad}{Complete filling in table.} \begin{table}[htbp] \caption{PyLith features covered in the suite of 3-D subduction zone examples.} \label{tab:example:subduction:3d:features} @@ -337,16 +336,7 @@ \subsection{Step 1: Axial Compression} conditions on the bottom (-z) boundary. \begin{figure}[htbp] - \begin{tikzpicture} - \tikzstyle{annotation} = [black]; - \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; - \begin{scope}[x={(image.south east)},y={(image.north west)}] - \node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; - \draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); - \node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; - \draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); - \end{scope} - \end{tikzpicture} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step01_diagram} \caption{Diagram of Step 1: Axial compression. This static simulation uses Dirichlet boundary conditions with axial compression in the east-west (x-direction), roller boundary @@ -476,11 +466,14 @@ \subsection{Step 1: Axial Compression} \end{shell} \item Run the ParaView Python script directly from a shell (terminal window) via the command line. You can use command line arguments to - set user-specified parameters. + set user-specified parameters. If pvpython \begin{shell} # Make sure you are in the examples/3d/subduction directory. # We show the optional command line arguments in square brackets. $$ ./viz/plot_dispvec.py [--vector-scale=10.0e+4] [--sim=step01.cfg} [--screenshot=FILE] +# +# If pvpython is not in your PATH, then you can run the script using: +$$ PATH_TO_PVPYTHON/pvpython ./viz/plot_dispvec.py \end{shell} \end{enumerate} @@ -763,25 +756,14 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} mantle. Figure~\ref{fig:example:subduction:3d:step03:diagram} summarizes the problem description. -\todo{brad}{Add annotation to figure.} \begin{figure}[htbp] - \begin{tikzpicture} - \tikzstyle{annotation} = [black]; - \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; - \begin{scope}[x={(image.south east)},y={(image.north west)}] - \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; - %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); - %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); - \end{scope} - \end{tikzpicture} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step03_diagram} \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and - interseismic deformation for the subducting slab. We precsribed + interseismic deformation for the subducting slab. We prescribe steady, uniform creep on the bottom of the slab and deeper portion of the subduction interface. We impose roller Dirichlet boundary conditions on the lateral and bottom boundaries, except where they - overlap with the fault interfaces for the slab.} + overlap with the slab and splay fault.} \label{fig:example:subduction:3d:step03:diagram} \end{figure} @@ -955,26 +937,16 @@ \subsection{Step 4: Prescribed Earthquake Cycle} roller Dirichlet boundary conditions and combination of elastic and viscoelatic materials as we did in Step 3. -\todo{brad}{Add annotation to figure.} \begin{figure}[htbp] - \begin{tikzpicture} - \tikzstyle{annotation} = [black]; - \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; - \begin{scope}[x={(image.south east)},y={(image.north west)}] - \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; - %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); - %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); - \end{scope} - \end{tikzpicture} - \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and - interseismic deformation for the subducting slab. We precsribed - steady, uniform creep on the bottom of the slab and deeper portion - of the subduction interface. We impose roller Dirichlet boundary - conditions on the lateral and bottom boundaries, except where they - overlap with the fault interfaces for the slab.} - \label{fig:example:subduction:3d:step03:diagram} + \includegraphics[width=5.0in]{examples/figs/subduction3d_step04_diagram} + \caption{Diagram of Step 4: A simple earthquake cycle combining the + prescribed aseismic slip (creep) from Step 3 with prescribed + coseismic slip for two earthquakes on the shallow portion of the + subduction interface and one earthquake on the play fault. We + impose roller Dirichlet boundary conditions on the lateral and + bottom boundaries, except where they overlap with the slab and + splay fault.} + \label{fig:example:subduction:3d:step04:diagram} \end{figure} % Faults From bcd6461e889afd17e90cb0d164a4f28db4731196 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 14:24:48 -0700 Subject: [PATCH 129/216] Added diagram for step02. --- .../figs/subduction3d_geometry_patch.png | Bin 0 -> 28715 bytes .../figs/subduction3d_step02_diagram.pdf | Bin 0 -> 36640 bytes .../figs/subduction3d_step02_diagram.tex | 25 ++++++++++++++++++ doc/userguide/examples/subduction3d.tex | 19 +++---------- 4 files changed, 29 insertions(+), 15 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction3d_geometry_patch.png create mode 100644 doc/userguide/examples/figs/subduction3d_step02_diagram.pdf create mode 100644 doc/userguide/examples/figs/subduction3d_step02_diagram.tex diff --git a/doc/userguide/examples/figs/subduction3d_geometry_patch.png b/doc/userguide/examples/figs/subduction3d_geometry_patch.png new file mode 100644 index 0000000000000000000000000000000000000000..619c56364c19896ddeeaee218945487b3a396f62 GIT binary patch literal 28715 zcmXtf1z1$y^FDk~kj^Efq>(P^knXOf*(D{V8$^2PZjkO+N+gA4=@4lU5RvX~_$_|_ z|A&RkbDuru%$+kc@63DVMro+YV`IF=Kte*oR#cGDLPA1eM?(7V#jF1icd|?M$PpJ* zu(G@i($n+Lm(H?e#2xgH3I=XSNSK7rzsN{gIi!f2Xzq%tvS@3l!~h~x{*{<~B&0V; ziZYTq-i!O4M%8R{KC3qYGgko;0;V#j2~7%0{IW~JF&6RFiodZ?dj*pvZC?x`1yWqY zQF%y7QT{S~?|AV$+7uNJ@B10oU9WwTz5?!{99!(pSBm&eTRu4(sUS6vre>fa+FA@!edy+BBdgmldH z@8bO|I}*~T2;}DrUlK<+l1|SRQ+}ZT+*!w)j0g~ExFl&fh!nzwCCe;D6N*R6=P5Ke zMZH|c6!F*@9}*q?kq5tvTCHr&n_}D=EKU;rls{1=3RkB-eB@Mrif_bQ1tHn~DW2bO zn%lc*UD`06*t_cN`A&}0xmM5n+Q-Ofd3kwU;-PF}x$WI|ATk42ZTbt{>&f<2F=5|^ z&Q8Y>^Z?J5r|!oXP7dNHqA7#zyESjxQeN)tC@!5-HtMj6m7u<-JMExILZnZ`u3KtH z*{k>Mq-aREDDT|d&;QCF1*S*tpVTV@?gWCyZML$52qc-UdAW1Lk}IwG(fuR>y^p)a z9#+@+kiJ+^5Kano-(-6o{`w9?@+K|EUd_M%?e~PxM~e@z1!9$fSRE|PS`4NZCH1(E zmhjmL>b*gFUnROfTeJ4H>!R7{Yd9&+^U}&0VN`kw@ITgi^r=GGQxjBJa0fM+dTyk} zb&!nv)_AOQ;F$n71rimiow+7)%WWCr>$33KCN|FJuP;xuHCpXRIADEB^CqPcLH`Z< zLab*6(tKSFCbMo)vg&$r;mp7+Cq=3`<+5Z#7RAb7OiOI~1;Z#O<)p7l$yBvL_Q`+R zKiSG36V7`TDp2zHblWR2u<+meMlmcF)Zd`*e9)NU2P!=v{7+Kq2lKtB4#CU#BkGBM zURvQxoVc6c59HlGF2wh(cf#WoNLfrEObzDeVR%twig#kwl@P~4{YyV<*WG+k!Q7nN zs@3~!lE=Z-u31X#Qth=nuqg4=Th-KNUKFJ19Z;wgH$o+-3L^@_YoJse6@?wc{aikw zGwL93($UXw35nH*lB2F`zx9pTzWk)To>e4d^j-NYs8 zHWrx59*1n~KMem<-DBW%4P-H+xW6W1tj|FXG4jg~*sHMTr%!p4pXfdbv(;tRONPK5 z_6xh8mPvw+)@ZpHuS$u0q!^(LlF{`GDc0KDCm;9;8--{bP~QXopBBpF{N;XX;%XOw zO^1&#Lo*o5(q%0^Z?7G425iBDcybZ&sx$D}d#&BLvlDTJP`zcAmA8+P8Z7H%;e7epc##V+#0O)W zZdns=Nx8%NK6ktow|u`x?|}Sono-4!b}H+5$fQ-)>5xBh%$=V;z+ywDa=6`S&`I

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z%IB&|Nvop&$VkLT;6GkecH z&C>nHXu0P@JC-bIhLI2>f>P7C^gZ)ZQY#dq4HOK`W4ZK$Gpka8EH3?Ug=j+sBLzdC zSWtd`iGraCP=63ed0IYjNi~$?q7ZFkX>9K7>S|$XYU1c>>S$u=>gZ}{XlCSMZsO+R zW?^Y!r$AT<&=$y&Yy~p|XzC{-`6nkN{5XH)z)6-PXB^HPI=latex, ->, ultra thick] +\tikzstyle{image} = [anchor=south west,inner sep=0] + + +\begin{tikzpicture} + + \node[image] (image) at (0,0) {\includegraphics[width=5.5in]{subduction3d_geometry_patch}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + + \node[anchor=west, annotation] (xneg) at (0.12,0.70) {Uniform slip}; + \draw[arrow] (xneg) -- (0.35,0.77); + \end{scope} + +\end{tikzpicture} + +\end{document} diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index f3d63f81f1..d87ac8a8a8 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -336,7 +336,7 @@ \subsection{Step 1: Axial Compression} conditions on the bottom (-z) boundary. \begin{figure}[htbp] - \includegraphics[width=5.0in]{examples/figs/subduction3d_step01_diagram} + \includegraphics[scale=0.75]{examples/figs/subduction3d_step01_diagram} \caption{Diagram of Step 1: Axial compression. This static simulation uses Dirichlet boundary conditions with axial compression in the east-west (x-direction), roller boundary @@ -545,19 +545,8 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} viscosity. Figure~\ref{fig:example:subduction:3d:step02:diagram} summarizes the problem description. -\todo{brad}{Add annotation to figure.} \begin{figure}[htbp] - \begin{tikzpicture} - \tikzstyle{annotation} = [black]; - \node[anchor=south west,inner sep=0] (image) at (0,0) {\includegraphics[width=4.5in]{examples/figs/subduction3d_geometry}}; - \begin{scope}[x={(image.south east)},y={(image.north west)}] - \node at (0.5,0.5) {{\bf\LARGE ADD ANNOTATION}}; - %\node[anchor=west, annotation] (xneg) at (-0.2,0.5) {+2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xneg) -- (0.0,0.5); - %\node[anchor=east, annotation] (xpos) at (+1.2,0.5) {-2.0 m}; - %\draw[>=latex, ->, ultra thick, annotation] (xpos) -- (1.0,0.5); - \end{scope} - \end{tikzpicture} + \includegraphics[scale=0.75]{examples/figs/subduction3d_step02_diagram} \caption{Diagram of Step 2: Prescribed coseismic slip and postseismic relaxation. This quasistatic simulation prescribes uniform slip on the central rupture patch on the subduction interface, @@ -757,7 +746,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} summarizes the problem description. \begin{figure}[htbp] - \includegraphics[width=5.0in]{examples/figs/subduction3d_step03_diagram} + \includegraphics[scale=0.75]{examples/figs/subduction3d_step03_diagram} \caption{Diagram of Step 3: Prescribed aseismic slip (creep) and interseismic deformation for the subducting slab. We prescribe steady, uniform creep on the bottom of the slab and deeper portion @@ -938,7 +927,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} viscoelatic materials as we did in Step 3. \begin{figure}[htbp] - \includegraphics[width=5.0in]{examples/figs/subduction3d_step04_diagram} + \includegraphics[scale=0.75]{examples/figs/subduction3d_step04_diagram} \caption{Diagram of Step 4: A simple earthquake cycle combining the prescribed aseismic slip (creep) from Step 3 with prescribed coseismic slip for two earthquakes on the shallow portion of the From 15619a3f944399d760cf27b6f44aefe83933e5d8 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 14:27:08 -0700 Subject: [PATCH 130/216] Started work on a Python script to show mesh. --- examples/3d/subduction/viz/plot_mesh.py | 93 +++++++++++++++++++++++++ 1 file changed, 93 insertions(+) create mode 100755 examples/3d/subduction/viz/plot_mesh.py diff --git a/examples/3d/subduction/viz/plot_mesh.py b/examples/3d/subduction/viz/plot_mesh.py new file mode 100755 index 0000000000..7105e7debe --- /dev/null +++ b/examples/3d/subduction/viz/plot_mesh.py @@ -0,0 +1,93 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the domain, colored by materials. + + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. + +EXODUS_FILE = "mesh/mesh_tet.exo" + +# ---------------------------------------------------------------------- +from paraview.simple import * +import os + +def visualize(filename): + + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + if not os.path.isfile(filename): + raise IOError("Exodus file '%s' does not exist." % filename) + dataDomain = ExodusIIReader(FileName=[filename]) + RenameSource("domain", dataDomain) + + view = GetActiveViewOrCreate('RenderView') + + # Show domain, colored by block. + domainDisplay = Show(dataDomain, view) + ColorBy(domainDisplay, ("FIELD", "vtkBlockColors")) + domainDisplay.RescaleTransferFunctionToDataRange(True, False) + domainDisplay.SetScalarBarVisibility(view, False) + domainDisplay.SetRepresentationType("Surface") + domainDisplay.Opacity = 0.5 + + # Add coordinate axes + axes = Axes() + axes.ScaleFactor = 1.0e+5 + + axesDisplay = Show(axes, view) + axesDisplay.SetRepresentationType('Wireframe') + axesDisplay.LineWidth = 4.0 + axesDisplay.SetScalarBarVisibility(view, False) + axesDisplay.DataAxesGrid.GridColor = [0.0, 0.0, 0.0] + + view.ResetCamera() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--filename", action="store", dest="filename", default=EXODUS_FILE) + args = parser.parse_args() + + visualize(args.filename) + + view = GetRenderView() + #view.CameraPosition = [-80160, -1130898, 133977] + #view.CameraFocalPoint = [-55107, 446810, 283137] + view.CameraViewUp = [0.0, 0.0, 1.0] + view.CameraViewAngle = 45.0 + view.ViewSize = [960, 540] + view.Update() + + Interact() + +else: + # Running inside the ParaView GUI + + visualize(EXODUS_FILE) + + +# End of file From 5b27af6513326497b8a230cbd22bace8ae2972bd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 15:22:11 -0700 Subject: [PATCH 131/216] Cleanup of step06 (add diagram). step06 is every similar to step02 so I condensed the discussion of the problem setup to emphasize the new features discussed. --- .../figs/subduction3d_step06_diagram.pdf | Bin 0 -> 36231 bytes .../figs/subduction3d_step06_diagram.tex | 25 +++ doc/userguide/examples/subduction3d.tex | 211 ++++++++---------- examples/3d/subduction/step06.cfg | 52 ++--- 4 files 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zWlNMoF@(ve0(}Gp0og2m09{{H?wruY4$^cc`zSh*Oi%ptN7|)kq4#21pR;!s)y}6=Pc(_ zrb|)IQuHr1C|-j)#RY)8q(@yxWgp2Osknj9z7YSc-52x&txOo@}M_u&i#Oq!7uhw zpQ*#ucr$5VY1}6&M~me%^JcMOmWi`>%_o>nH}wlOZB&iibA#%Kzwmjp_r=jghl zm%0Cge=`3UE0tvp3}I+REc6YW@YMkLbSxS$v~ngc2EZ#AS|xlnI(&M3I^aE7OG`U^ zI!0iA*_Y&omcSjmfBx{}t8og_F*C9uzaQ$;A3KCU=|QyV&xNHWe{NGXJ+Nb z|9>X|O8LDT80Z#%T;YG=3wqkxHzQqbeQ&!4c?Uas>%u^V8Q#!=5rXjq4h_%LWAWR9 z&{67jFd-$w2eM&uFarQrZvh}6oy-uI{|%6>osNy2lMN6O24E}zzz`D)ND0FHA1(Ut AIsgCw literal 0 HcmV?d00001 diff --git a/doc/userguide/examples/figs/subduction3d_step06_diagram.tex b/doc/userguide/examples/figs/subduction3d_step06_diagram.tex new file mode 100644 index 0000000000..666b057422 --- /dev/null +++ b/doc/userguide/examples/figs/subduction3d_step06_diagram.tex @@ -0,0 +1,25 @@ +\documentclass[crop,tikz]{standalone} +\usepackage{tikz} + +\begin{document} + +\usetikzlibrary{arrows,shapes} +\input{../../palettes/figcolors} + +\tikzstyle{annotation} = [black, font={\bf}] +\tikzstyle{arrow} = [annotation, >=latex, ->, ultra thick] +\tikzstyle{image} = [anchor=south west,inner sep=0] + + +\begin{tikzpicture} + + \node[image] (image) at (0,0) {\includegraphics[width=5.5in]{subduction3d_geometry_patch}}; + \begin{scope}[x={(image.south east)},y={(image.north west)}] + + \node[anchor=west, annotation] (xneg) at (0.12,0.70) {Prescribed slip}; + \draw[arrow] (xneg) -- (0.35,0.77); + \end{scope} + +\end{tikzpicture} + +\end{document} diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index d87ac8a8a8..ea232c7758 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1103,49 +1103,41 @@ \subsubsection{Exercises} \subsection{Step 6: Prescribed Slow-Slip Event} This example simulates a simple slow slip event (SSE) on the -subduction interface that remains fixed spatially but increases its -amplitude with time. We assume a constant rake angle of 110 degrees, -and a time duration of 30 days. This problem requres the use of both a -spatial database to provide the spatial distribution of slip, and a -temporal database to describe the time evolution of slip. To create -these databases we provide the \filename{generate\_slowslip.py} -script, which is in the \filename{spatialdb} directory. Once you are -in the \filename{spatialdb} directory, run the script as follows: -\begin{shell} -$$ ./generate_slowslip.py -\end{shell} -This script reads parameters from \filename{generate\_slowslip.cfg} to -generate a Gaussian slip distribution in geographic coordinates, along -with a temporal database providing the slip amplitudes at different -times. The files created are: -\begin{itemize} -\item \filename{fault\_slabtop\_slowslip.spatialdb}: Spatial database -\item \filename{fault\_slabtop\_slowslip.timedb}: Temporal database -\end{itemize} +subduction interface, in which the entire patch slips simultaneously +with an amplitude that grows with time. We impose a constant rake +angle of 110 degrees, and a time duration of 30 days. The time +duration is much shorter than the Maxwell time for our viscoelastic +materials, so we use elastic material properties (as we did in Step 1). + +\begin{figure}[htbp] + \includegraphics[scale=0.75]{examples/figs/subduction3d_step06_diagram} + \caption{Diagram of Step 6: Prescribed slow-slip event on the + subduction interface. This quasistatic simulation prescribes a + Gaussian slip distribution on the central rupture patch of the + subduction interface, purely elastic material properties, and + roller boundary conditions on the lateral (north, south, east, and + west) and bottom boundaries.} + \label{fig:example:subduction:3d:step06:diagram} +\end{figure} + -Note that \filename{fault\_slabtop\_slowslip.spatialdb} is a -\facility{SimpleGridDB}. This type of spatial database is very -efficient in cases where property values lie on a regular grid in 2 or -3 dimensions, since searches and interpolations reduce to a set of 1D -operations. Once the database files have been generated, it is -possible to run the example. There are a number of parameters that are -changed from or added to those in \filename{pylithapp.cfg}. We first -change the total simulation time to 30 days with a time step size of 2 -days: +% Problem +The only time dependence in this problem is the time evolution of +slip, so we set the duration of the simulation to match the duration +of the slow slip event. We use a time step of 2.0 days to insure that +we resolve the temporal evolution of the slip. \begin{cfg} [pylithapp.problem.formulation.time_step] -# Define the total time for the simulation and the time step size.

    total_time

    = 30.0*day

    dt

    = 2.0*day \end{cfg} -The results in this example will be used to simulate output at cGPS -stations for example step07, so we modify the output manager to -provide output at synthetic cGPS stations as well as the entire domain -and ground surface: +% Output at points +The results in this example will be used to simulate output at fake +continuous GPS (cGPS) stations in Step 7, so we add an output manager +for saving the solution at specific points (\object{OutputSolnPoints}) +in addition to our output managers over the domain and top surface: \begin{cfg} -# For this problem, we want output over the entire domain, for the -# ground surface, and at simulated cGPS locations. [pylithapp.problem.implicit] output = [domain, subdomain, cgps_sites] @@ -1155,12 +1147,38 @@ \subsection{Step 6: Prescribed Slow-Slip Event} output.cgps_sites = pylith.meshio.OutputSolnPoints \end{cfg} -There are a number of parameters to change/modify related to the -fault. In particular, we change the default slip function to -\facility{pylith.faults.TimeHistorySlipFn}, which allows us to change -the slip amplitude as a function of time. We also use a -\facility{SimpleGridDB} to specify fault slip and linear interpolation -for the fault slip: +For the point output we specify the output data writer, the file +containing the list of cGPS stations and the coordinate system +associated with the station locations. The format of the station file +is whitespace separated columns of station name and then the +coordinates of the station. See Section~\vref{sec:format:PointsList} +for more information. +\begin{cfg} +[pylithapp.problem.formulation.output.cgps_sites] +writer = pylith.meshio.DataWriterHDF5 +

    writer.filename

    = output/step06-cgps_sites.h5 + +# File with coordinates of cGPS stations. +

    reader.filename

    = cgps_sites.txt + +# Specify coordinate system used in cGPS station file. +coordsys = spatialdata.geocoords.CSGeo +

    coordsys.space_dim

    = 3 +

    coordsys.datum_horiz

    = WGS84 +

    coordsys.datum_vert

    = mean sea level +\end{cfg} + +% Fault +The fault parameters are very similar to those in Step 2, in which we +also prescribed slip on the subduction interface patch. The primary +difference is that we use a user-defined slip time history function +(\object{TimeHistorySlipFn}). This slip time function requires spatial +databases for the amplitude of the final slip and slip initiation +time, and a time history file specifying the normalized amplitude as a +function of time. Additional to illustrate PyLith's ability to use +spatial databases with points in other, but compatible, georeferenced +coordinate systems, we specify the slip distribution using geographic +(longitude and latitude) coordinates. \begin{cfg} [pylithapp.problem] # We prescribe slip on the slab fault patch. @@ -1183,13 +1201,11 @@ \subsection{Step 6: Prescribed Slow-Slip Event} [pylithapp.problem.interfaces.slab.eq_srcs.rupture] slip_function = pylith.faults.TimeHistorySlipFn -# The slip is defined in a spatial database. +# The slip is defined in a SimpleGridDB spatial database with linear interpolation. [pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] slip = spatialdata.spatialdb.SimpleGridDB

    slip.label

    = Gaussian slip distribution for SSE

    slip.filename

    = spatialdb/fault_slabtop_slowslip.spatialdb - -# Use linear interpolation.

    slip.query_type

    = linear # We use a UniformDB to specify the slip initiation time. @@ -1203,86 +1219,44 @@ \subsection{Step 6: Prescribed Slow-Slip Event}

    time_history.filename

    = spatialdb/fault_slabtop_slowslip.timedb \end{cfg} -The final set of parameters involve output. The domain and subdomain -output are similar to previous examples: -\begin{cfg} -[pylithapp.problem.formulation.output.domain] -writer = pylith.meshio.DataWriterHDF5 -

    writer.filename

    = output/step06-domain.h5 - -[pylithapp.problem.formulation.output.subdomain] -# Name of nodeset for top surface. -

    label

    = boundary_zpos -writer = pylith.meshio.DataWriterHDF5 -

    writer.filename

    = output/step06-groundsurf.h5 -\end{cfg} -For points output, we need to provide coordinate system information as -well as the name of the text file containing station names and -coordinates: -\begin{cfg} -# Specify output type, coordinate system, and station file for cgps_sites. -[pylithapp.problem.formulation.output.cgps_sites] -# We will use a geographic coordinate system for the cGPS sites file. -coordsys = spatialdata.geocoords.CSGeo -

    coordsys.space_dim

    = 3 -

    coordsys.datum_horiz

    = WGS84 -

    coordsys.datum_vert

    = mean sea level - -# Use HDF5 output. -writer = pylith.meshio.DataWriterHDF5 -

    writer.filename

    = output/step06-cgps_sites.h5 - -# Simulated cGPS station file. -

    reader.filename

    = cgps_sites.txt -\end{cfg} -The remainder of the settings are for fault and material output, -similar to other examples: -\begin{cfg} -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.slab.output] -# Output fault results to HDF5 file. -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step06-fault-slab.h5 - -# We want both orientation and slip information in the information file. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] - -# Material output ------------------------------------------------------ -[pylithapp.problem.materials.slab.output] -

    writer.filename

    = output/step06-slab.h5 - -[pylithapp.problem.materials.wedge.output] -

    writer.filename

    = output/step06-wedge.h5 - -[pylithapp.problem.materials.crust.output] -

    writer.filename

    = output/step06-crust.h5 - -[pylithapp.problem.materials.mantle.output] -

    writer.filename

    = output/step06-mantle.h5 -\end{cfg} - -We use elastic properties for all materials, and custom solver -settings appropriate for a problem with a fault. We run the example by typing +You will notice that the \filename{spatialdb} does not contain the +\filename{fault\_slabtop\_slowslip.spatialdb} and +\filename{fault\_slabtop\_slowslip.timedb} files. We use the +\filename{generate\_slowslip.py} Python script to generate these files +as an illustration of how to use Python to generate more somple +spatial variations and the \object{SimpleGridAscii} object to write +spatial database files. This script reads parameters from +\filename{generate\_slowslip.cfg} to generate a Gaussian slip +distribution in geographic coordinates, along with a temporal database +providing the slip amplitudes at different times. + +To run the simulation, first run the Python script to generate the +spatial database files, and then run PyLith. \begin{shell} +# Generate the spatial database files +$$ cd spatialdb && ./generate_slowslip.py +$$ ls fault_slabtop_slowslip.* +# You should see +fault_slabtop_slowslip.spatialdb fault_slabtop_slowslip.timedb +# Change back to the subduction directory and run PyLith +$$ cd .. $$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} -The problem will produce 13 pairs of HDF5/Xdmf files. In the data -files (those without a \filename{\_info} before the file suffix) there -are field values representing 15 time steps. The additional HDF5 file -that was not present in previous examples is +The problem will produce 13 pairs of HDF5/Xdmf files. The additional +HDF5 file that was not present in previous examples is \filename{step06-cgps\_sites.h5}, which contains the displacements at -the simulated cGPS sites. +the fake cGPS sites. Figure \vref{fig:example:subduction:3d:step06}, which was created using ParaView, shows the surface vertical displacement along with horizontal displacement vectors at the cGPS sites, superimposed on -contours of the applied slip at t = 24 days. +contours of the applied slip at $t = 24 \mathrm{days}$. \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step06_soln} \caption{Solution for Step 6. The colors indicate the vertical displacement, the vectors represent the horizontal displacements - at simulated cGPS sites, and the contours represent the applied + at fake cGPS sites, and the contours represent the applied slip at t = 24 days.} \label{fig:example:subduction:3d:step06} \end{figure} @@ -1423,8 +1397,8 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions}

    impulse_dof

    = [0] \end{cfg} -In the output settings, we turn off output for the domain and ground -surface, provide coordinate system info for the simulated cGPS output, +In the output settings, we turn off output for the domain, provide the +coordinate system for the fake cGPS stations, and provide filenames: \begin{cfg} # Add cggs_sites to solution output. @@ -1479,11 +1453,12 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} $$ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} -\tip{To save runtime, run the two sub-problems simultaneously in -separate terminal windows. For a problem this size, this should work -fine on a laptop. For larger problems, this approach can still be -useful. Each sub-problem could be run simultaneously on several nodes -of a cluster, for example.} + +\tip{To save time, run the two sub-problems simultaneously in separate + shells (terminals). For a problem this size, this should work fine + on a laptop. For larger problems, this approach can still be + useful. For example, each sub-problem could be run simultaneously on + several nodes of a cluster.} After generating the synthetic data and Green's functions, we then perform a simple inversion using the \filename{slip\_invert.py} script, diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 2fcbbcbaad..8ba91ff3b8 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -76,19 +76,6 @@ problem.progress_monitor.filename = output/step06-progress.txt total_time = 30.0*day dt = 2.0*day -# ---------------------------------------------------------------------- -# output -# ---------------------------------------------------------------------- -# For this problem, we want output over the entire domain, for the -# ground surface, and at simulated cGPS locations. -[pylithapp.problem.implicit] -output = [domain, subdomain, cgps_sites] - -# Default output is for the entire domain. -# We need to set the type of output for the subdomain and points. -output.subdomain = pylith.meshio.OutputSolnSubset -output.cgps_sites = pylith.meshio.OutputSolnPoints - # ---------------------------------------------------------------------- # faults # ---------------------------------------------------------------------- @@ -132,9 +119,24 @@ slip_time.data = [0.0*year] time_history.label = Time history of slip time_history.filename = spatialdb/fault_slabtop_slowslip.timedb +# Output +[pylithapp.problem.interfaces.slab.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slab.h5 +vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] + # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- +# For this problem, we want output over the entire domain, for the +# ground surface, and at simulated cGPS locations. +[pylithapp.problem.implicit] +output = [domain, subdomain, cgps_sites] + +# Default output is for the entire domain. +# We need to set the type of output for the subdomain and points. +output.subdomain = pylith.meshio.OutputSolnSubset +output.cgps_sites = pylith.meshio.OutputSolnPoints # Domain, subdomain, and points output --------------------------------- [pylithapp.problem.formulation.output.domain] @@ -147,29 +149,19 @@ label = boundary_zpos writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step06-groundsurf.h5 -# Specify output type, coordinate system, and station file for cgps_sites. +# Specify output type, station file, and coordinate system for cgps_sites. [pylithapp.problem.formulation.output.cgps_sites] -# We will use a geographic coordinate system for the cGPS sites file. -coordsys = spatialdata.geocoords.CSGeo -coordsys.space_dim = 3 -coordsys.datum_horiz = WGS84 -coordsys.datum_vert = mean sea level - -# Use HDF5 output. writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step06-cgps_sites.h5 -# Simulated cGPS station file. +# File with coordinates of cGPS stations. reader.filename = cgps_sites.txt -# Fault output ------------------------------------------------------ -[pylithapp.problem.interfaces.slab.output] -# Output fault results to HDF5 file. -writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step06-fault-slab.h5 - -# We want both orientation and slip information in the information file. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, final_slip_rupture] +# Specify coordinate system used in cGPS station file. +coordsys = spatialdata.geocoords.CSGeo +coordsys.space_dim = 3 +coordsys.datum_horiz = WGS84 +coordsys.datum_vert = mean sea level # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] From f06c6d0a6423b1a0003977739bd9ff44f872a2c6 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 17:51:04 -0700 Subject: [PATCH 132/216] Testing addition of zeroToleranceNormal. --- .../fault_slabtop_slipweakening.spatialdb | 44 ++++ .../fault_slabtop_tractions.spatialdb | 42 ++++ examples/2d/subduction/stepXX.cfg | 228 ++++++++++++++++++ examples/2d/subduction/viz/plot_dispwarp.py | 127 ++++++++++ examples/2d/subduction/viz/plot_shearratio.py | 121 ++++++++++ examples/3d/subduction/TODO | 4 + .../fault_slabtop_slipweakening.spatialdb | 4 +- .../fault_slabtop_tractions.spatialdb | 12 +- examples/3d/subduction/step05.cfg | 20 +- libsrc/pylith/faults/FaultCohesiveDyn.cc | 17 +- libsrc/pylith/faults/FaultCohesiveDyn.hh | 3 + 11 files changed, 597 insertions(+), 25 deletions(-) create mode 100644 examples/2d/subduction/fault_slabtop_slipweakening.spatialdb create mode 100644 examples/2d/subduction/fault_slabtop_tractions.spatialdb create mode 100644 examples/2d/subduction/stepXX.cfg create mode 100755 examples/2d/subduction/viz/plot_dispwarp.py create mode 100755 examples/2d/subduction/viz/plot_shearratio.py diff --git a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb new file mode 100644 index 0000000000..266246bfa6 --- /dev/null +++ b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb @@ -0,0 +1,44 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify depth-dependent frictional properties with stable +// sliding (equal dynamic and static coefficients of friction) above +// and below the seismogenic zone (elevations of -5 km to -45 km). +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 6 + num-values = 4 + value-names = static-coefficient dynamic-coefficient slip-weakening-parameter cohesion + value-units = none none cm Pa + space-dim = 2 + cs-data = cartesian { + to-meters = 1.0e+3 + space-dim = 2 + } +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +99.0 -5.0 -15.0 -35.0 -45.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) static-coefficient +// (5) dynamic-coefficient +// (6) slip-weakening-parameter (cm) +// (7) cohesion (Pa) +0.0 99.0 0.6 0.6 1.0 0.0 +0.0 -5.0 0.6 0.6 1.0 0.0 +0.0 -15.0 0.6 0.2 1.0 0.0 +0.0 -30.0 0.6 0.2 1.0 0.0 +0.0 -45.0 0.6 0.6 1.0 0.0 +0.0 -999.0 0.6 0.6 1.0 0.0 diff --git a/examples/2d/subduction/fault_slabtop_tractions.spatialdb b/examples/2d/subduction/fault_slabtop_tractions.spatialdb new file mode 100644 index 0000000000..d59fffe1e9 --- /dev/null +++ b/examples/2d/subduction/fault_slabtop_tractions.spatialdb @@ -0,0 +1,42 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify depth-dependent fault tractions with higher values in +// the stable sliding regions consistent with residual stresses in +// those regions. +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 6 + num-values = 2 + value-names = traction-shear traction-normal + value-units = MPa MPa + space-dim = 2 + cs-data = cartesian { + to-meters = 1.0e+3 + space-dim = 2 + } +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +99.0 -5.0 -15.0 -35.0 -45.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) shear traction (MPa) +// (5) normal traction (MPa) +0.0 99.0 -11.9 -20.0 +0.0 -5.0 -11.9 -20.0 +0.0 -15.0 -10.0 -20.0 +0.0 -30.0 -10.0 -20.0 +0.0 -45.0 -11.9 -20.0 +0.0 -999.0 -11.9 -20.0 diff --git a/examples/2d/subduction/stepXX.cfg b/examples/2d/subduction/stepXX.cfg new file mode 100644 index 0000000000..37b955d526 --- /dev/null +++ b/examples/2d/subduction/stepXX.cfg @@ -0,0 +1,228 @@ +[pylithapp] + +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This simulation involves aseismic creep along the interfaces between +# the subducting oceanic crust and the mantle. The slip rate is a +# constant 8 cm/yr. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# This is not a self-contained simulation configuration file. This +# file specifies only the boundary conditions and earthquake +# parameters for the simulation. The general quasi-static and mesh +# parameters are specificed in the pylithapp.cfg file which PyLith +# reads by default. +# +# To run the simulation: +# pylith step02.cfg +# +# Output will be directed to directory output. + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +# Fault friction is a nonlinear problem so we need to use the +# nonlinear solver. +solver = pylith.problems.SolverNonlinear + +[pylithapp.timedependent.formulation.time_step] +total_time = 100.0*year +dt = 5.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +# Set bc to an array of 3 boundary conditions: +# 'boundary_east_mantle' +# 'boundary_west' +# 'boundary_bottom_mantle' +bc = [boundary_east_mantle,boundary_west,boundary_bottom_mantle] + +# For all boundaries, we fix the displacement normal to the boundary +# (roller boundary condition) by retaining the default ZeroDispDB, +# which specifies a zero value. +# +# The label corresponds to the name of the nodeset in CUBIT. + +# East boundary (mantle) +[pylithapp.timedependent.bc.boundary_east_mantle] +bc_dof = [0] +label = bndry_east_mantle +db_initial.label = Dirichlet BC on east boundary (mantle) + +# West boundary +[pylithapp.timedependent.bc.boundary_west] +bc_dof = [0,1] +label = bndry_west +db_initial.label = Dirichlet BC on west boundary + +# Bottom boundary (mantle) +[pylithapp.timedependent.bc.boundary_bottom_mantle] +bc_dof = [1] +label = bndry_bot_mantle +db_initial.label = Dirichlet BC on bottom boundary (mantle) + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +interfaces = [fault_slabtop,fault_slabbot] + +# Set the type of fault interface condition. +[pylithapp.timedependent.interfaces] +fault_slabtop = pylith.faults.FaultCohesiveDyn +fault_slabbot = pylith.faults.FaultCohesiveKin + +# Slab top -------------------- +[pylithapp.timedependent.interfaces.fault_slabtop] +# The label corresponds to the name of the nodeset in CUBIT. +label = fault_slabtop +id = 100 + +# We must define the quadrature information for fault cells. +# The fault cells are 1D (line). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 1 + + + + +# Friction +friction = pylith.friction.SlipWeakening +friction.label = Slip weakening +# Force healing after each time step, so weakening is confined to each +# time step and does not carry over into subsequent time steps. +friction.force_healing = True + +# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. +zero_tolerance = 1.0e-10 + +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +friction.db_properties.label = Slip weakening +friction.db_properties.filename = fault_slabtop_slipweakening.spatialdb + +# Initial fault tractions +traction_perturbation = pylith.faults.TractPerturbation +traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB +traction_perturbation.db_initial.label = Initial fault tractions +traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb + +[pylithapp.problem.interfaces.fault_slabtop.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/stepXX-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir] +vertex_data_fields = [slip, slip_rate, traction] + + + +# Slab bottom -------------------- +[pylithapp.timedependent.interfaces.fault_slabbot] +# The label corresponds to the name of the nodeset in CUBIT. +label = fault_slabbot +id = 101 + +# We must define the quadrature information for fault cells. +# The fault cells are 1D (line). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 1 + +# Switch to constant slip rate time function. +[pylithapp.timedependent.interfaces.fault_slabbot.eq_srcs.rupture] +slip_function = pylith.faults.ConstRateSlipFn + +# The creep rate and slip time are uniform, so use UniformDB for simplicity. +[pylithapp.timedependent.interfaces.fault_slabbot.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slip rate +slip_rate.values = [left-lateral-slip, fault-opening] +slip_rate.data = [8.0*cm/year, 0.0*cm/year] + +# Slip time is uniform, so use UniformDB for convenience +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# Domain +[pylithapp.problem.formulation.output.domain] +writer.filename = output/stepXX.h5 +time_step = 1.0*year + +# Ground surface +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/stepXX-groundsurf.h5 + +# Faults +[pylithapp.problem.interfaces.fault_slabtop.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/stepXX-fault-slabtop.h5 + +[pylithapp.problem.interfaces.fault_slabbot.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/stepXX-fault-slabbot.h5 + +# Materials +[pylithapp.timedependent.materials.continent_crust.output] +writer.filename = output/stepXX-concrust.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.continent_mantle.output] +writer.filename = output/stepXX-conmantle.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.ocean_crust.output] +writer.filename = output/stepXX-oceancrust.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.ocean_mantle.output] +writer.filename = output/stepXX-oceanmantle.h5 +cell_data_fields = [] + + +# ---------------------------------------------------------------------- +# PETSc +# ---------------------------------------------------------------------- +[pylithapp.timedependent.interfaces.fault_slabtop] +zero_tolerance = 1.0e-8 + + +[pylithapp.petsc] +malloc_dump = + +# Convergence parameters. +ksp_rtol = 1.0e-20 +ksp_atol = 1.0e-9 +ksp_max_it = 1000 +ksp_gmres_restart = 50 + +snes_rtol = 1.0e-20 +snes_atol = 1.0e-7 + +snes_max_it = 1000 + + +# Friction sensitivity solve used to compute the increment in slip +# associated with changes in the Lagrange multiplier imposed by the +# fault constitutive model. +friction_pc_type = asm +friction_sub_pc_factor_shift_type = nonzero +friction_ksp_max_it = 25 +friction_ksp_gmres_restart = 30 +friction_ksp_error_if_not_converged = true + +# Uncomment to view details of friction sensitivity solve. +#friction_ksp_monitor = true +#friction_ksp_view = true +#friction_ksp_converged_reason = true + +# End of file diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py new file mode 100755 index 0000000000..af97fc0bb3 --- /dev/null +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -0,0 +1,127 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the deformed +# domain, colored by the value of the x-displacemenet. + + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. + +# Root name for simulation. +SIM_NAME = "stepXX" + +# Scale used to exaggerate deformation. +DISPLACEMENT_SCALE = 10.0e+3 +DISPLACEMENT_COMPONENT = "X" + +# ---------------------------------------------------------------------- +from paraview.simple import * +import os + +def visualize(sim, exaggeration, component, showFinalTimeStep=False): + + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + # Read data + filename = "output/%s.xmf" % sim + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + dataDomain = XDMFReader(FileNames=[filename]) + RenameSource("%s-domain" % sim, dataDomain) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + if showFinalTimeStep: + scene.GoToLast() + + view = GetActiveViewOrCreate('RenderView') + + # Gray wireframe for undeformed domain. + domainDisplay = Show(dataDomain, view) + domainDisplay.Representation = 'Wireframe' + domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + + # Warp domain to show deformation + warp = WarpByVector(Input=dataDomain) + warp.Vectors = ['POINTS', 'displacement'] + warp.ScaleFactor = exaggeration + + warpDisplay = Show(warp, view) + ColorBy(warpDisplay, ('POINTS', 'displacement', component)) + warpDisplay.RescaleTransferFunctionToDataRange(True) + warpDisplay.SetScalarBarVisibility(view, True) + warpDisplay.SetRepresentationType('Surface With Edges') + # Rescale color bar to exactly fit the current data range + warpDisplay.RescaleTransferFunctionToDataRange(False, False) + + # Customize colorbar + displacementLUT = GetColorTransferFunction('displacement') + colorbar = GetScalarBar(displacementLUT, view) + if component.lower() == "magnitude": + colorbar.Title = "Displacement Mag. (m)" + else: + colorbar.Title = "%s-displacement (m)" % component.lower() + colorbar.ComponentTitle = "" + + # Annotate time + tstamp = AnnotateTimeFilter(warp) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) + parser.add_argument("--component", action="store", dest="component", default=DISPLACEMENT_COMPONENT) + parser.add_argument("--screenshot", action="store", dest="screenshot") + args = parser.parse_args() + + visualize(args.sim, args.exaggeration, args.component, showFinalTimeStep=True) + + view = GetRenderView() + view.ViewSize = [960, 540] + view.Update() + + if args.screenshot: + WriteImage(args.screenshot) + + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, DISPLACEMENT_SCALE, DISPLACEMENT_COMPONENT) + + +# End of file diff --git a/examples/2d/subduction/viz/plot_shearratio.py b/examples/2d/subduction/viz/plot_shearratio.py new file mode 100755 index 0000000000..aa51f2cb42 --- /dev/null +++ b/examples/2d/subduction/viz/plot_shearratio.py @@ -0,0 +1,121 @@ +#!/usr/bin/env pvpython +# -*- Python -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- + +# Plot the undeformed domain as a gray wireframe and then the fault +# surfaces, colored by the magnitude of fault slip. +# +# This Python script runs using pvpython or within the ParaView Python +# shell. + +# User-specified parameters. +# +# These are used if running from within the ParaView GUI via the +# Python shell or as defaults if running outside the ParaView GUI via +# pvpython. + +# Root name for simulation. +SIM_NAME = "stepXX" + +# Names of faults (with spontaneous rupture) for output files. +FAULTS = ["fault-slabtop"] + +# ---------------------------------------------------------------------- +from paraview.simple import * +import os +import numpy + +def visualize(sim, faults): + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + + # Read fault data + dataFaults = [] + for fault in faults: + filename = "output/%s-%s.xmf" % (sim, fault) + if not os.path.isfile(filename): + raise IOError("File '%s' does not exist." % filename) + data = XDMFReader(FileNames=[filename]) + RenameSource("%s-%s" % (sim, fault), data) + dataFaults.append(data) + + groupFaults = GroupDatasets(Input=dataFaults) + + scene = GetAnimationScene() + scene.UpdateAnimationUsingDataTimeSteps() + view = GetActiveViewOrCreate('RenderView') + + # Ratio of shear to normal traction + calculatorRatio = Calculator(Input=groupFaults) + calculatorRatio.Function = '-abs(traction_X)/traction_Y' + calculatorRatio.ResultArrayName = 'shearRatio' + + ratioDisplay = Show(calculatorRatio, view) + ColorBy(ratioDisplay, ('POINTS', 'shearRatio')) + ratioDisplay.RescaleTransferFunctionToDataRange(True) + ratioDisplay.SetScalarBarVisibility(view, True) + ratioDisplay.SetRepresentationType('Wireframe') + ratioDisplay.LineWidth = 8.0 + + # Rescale color and/or opacity maps used to exactly fit the current data range + ratioLUT = GetColorTransferFunction('shearDivNormal') + ratioDisplay.RescaleTransferFunctionToDataRange(False, False) + # Update a scalar bar component title. + UpdateScalarBarsComponentTitle(ratioLUT, ratioDisplay) + + # Annotate time + tstamp = AnnotateTimeFilter(groupFaults) + tstamp.Format = 'Time: %2.0f yr' + tstamp.Scale = 3.168808781402895e-08 # seconds to years + + tstampDisplay = Show(tstamp, view) + tstampDisplay.FontFamily = "Courier" + tstampDisplay.FontSize = 14 + + view.ResetCamera() + view.Update() + Render() + +# ---------------------------------------------------------------------- +if __name__ == "__main__": + # Running from outside the ParaView GUI via pvpython + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--faults", action="store", dest="faults") + args = parser.parse_args() + + if args.faults: + faults = args.faults.split(",") + else: + faults = FAULTS + visualize(args.sim, faults) + + view = GetRenderView() + view.ViewSize = [960, 540] + view.Update() + + Interact() + +else: + # Running inside the ParaView GUI + + visualize(SIM_NAME, FAULTS) + + +# End of file diff --git a/examples/3d/subduction/TODO b/examples/3d/subduction/TODO index e69de29bb2..efdeceedf9 100644 --- a/examples/3d/subduction/TODO +++ b/examples/3d/subduction/TODO @@ -0,0 +1,4 @@ +step05 - traction_shear/traction_normal > 0.6 after fault locks + zeroToleranceNormal?? + + diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb index 92b231bb6b..8f4878bbb2 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb @@ -15,7 +15,7 @@ SimpleGridDB { num-z = 6 num-values = 4 value-names = static-coefficient dynamic-coefficient slip-weakening-parameter cohesion - value-units = none none m Pa + value-units = none none cm Pa space-dim = 3 cs-data = geo-projected { to-meters = 1.0e+3 // Specify coordinates in km for convenience. @@ -48,7 +48,7 @@ SimpleGridDB { // (3) z coordinate (km) // (4) static-coefficient // (5) dynamic-coefficient -// (6) slip-weakening-parameter (m) +// (6) slip-weakening-parameter (cm) // (7) cohesion (Pa) 0.0 0.0 99.0 0.6 0.6 1.0 0.0 0.0 0.0 -5.0 0.6 0.6 1.0 0.0 diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb index aaf168b835..926dbda225 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb @@ -49,9 +49,9 @@ SimpleGridDB { // (4) left-lateral shear traction (MPa) // (5) reverse shear traction (MPa) // (6) normal traction (MPa) -0.0 0.0 99.0 0.0 10.0 -20.0 -0.0 0.0 -5.0 0.6 10.0 -20.0 -0.0 0.0 -15.0 0.6 0.0 -20.0 -0.0 0.0 -30.0 0.6 0.0 -20.0 -0.0 0.0 -45.0 0.6 10.0 -20.0 -0.0 0.0 -999.0 0.6 10.0 -20.0 +0.0 0.0 99.0 0.0 11.9 -20.0 +0.0 0.0 -5.0 0.0 11.9 -20.0 +0.0 0.0 -15.0 0.0 10.0 -20.0 +0.0 0.0 -30.0 0.0 10.0 -20.0 +0.0 0.0 -45.0 0.0 11.9 -20.0 +0.0 0.0 -999.0 0.0 11.9 -20.0 diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg index 8644897708..44927b7cea 100644 --- a/examples/3d/subduction/step05.cfg +++ b/examples/3d/subduction/step05.cfg @@ -70,23 +70,25 @@ dt = 10.0*year # ---------------------------------------------------------------------- # boundary conditions # ---------------------------------------------------------------------- -# Because the slab intersects the boundaries of the domain, and PyLith -# does not permit overlap between the fault interfaces and Dirichlet -# boundary conditions, for the Dirichlet boundary conditions we use -# the nodesets which exclude vertices on the fault. We only update the -# name of the nodeset for the -x, -y, and +y boundaries. +# We do not want the boundaries to constrain the motion of the +# subducting slab, so we use the nodesets that exclude vertices on the +# subducting slab. Furthermore, PyLith does not permit overlap between +# the fault interfaces and Dirichlet boundary conditions. This is why +# we exclude vertices on the splay fault in these nodesets as well. We +# only update the name of the nodeset for the -x, -y, and +y +# boundaries. # -x face [pylithapp.problem.bc.x_neg] -label = boundary_xneg_nofault +label = boundary_xneg_noslab # -y face [pylithapp.problem.bc.y_neg] -label = boundary_yneg_nofault +label = boundary_yneg_noslab # +y face [pylithapp.problem.bc.y_pos] -label = boundary_ypos_nofault +label = boundary_ypos_noslab # ---------------------------------------------------------------------- # faults @@ -156,7 +158,7 @@ eq_srcs.rupture.slip_function = pylith.faults.ConstRateSlipFn slip_rate = spatialdata.spatialdb.UniformDB slip_rate.label = Slab bottom slip rate. slip_rate.values = [left-lateral-slip, reverse-slip, fault-opening] -slip_rate.data = [0.0*cm/year, -4.0*cm/year, 0.0*cm/year] +slip_rate.data = [0.0*cm/year, -8.0*cm/year, 0.0*cm/year] slip_time = spatialdata.spatialdb.UniformDB slip_time.label = Slip initiation time diff --git a/libsrc/pylith/faults/FaultCohesiveDyn.cc b/libsrc/pylith/faults/FaultCohesiveDyn.cc index 233f3a87c7..2c92108eae 100644 --- a/libsrc/pylith/faults/FaultCohesiveDyn.cc +++ b/libsrc/pylith/faults/FaultCohesiveDyn.cc @@ -62,6 +62,7 @@ // Default constructor. pylith::faults::FaultCohesiveDyn::FaultCohesiveDyn(void) : _zeroTolerance(1.0e-10), + _zeroToleranceNormal(1.0e-8), _tractPerturbation(0), _friction(0), _jacobian(0), @@ -331,7 +332,7 @@ pylith::faults::FaultCohesiveDyn::integrateResidual(const topology::Field& resid _logger->eventEnd(computeEvent); _logger->eventBegin(updateEvent); #endif - if (slipNormal < _zeroTolerance || !_openFreeSurf) { + if (slipNormal < _zeroToleranceNormal || !_openFreeSurf) { // if no opening or flag indicates to still impose initial tractions when fault is open. // Assemble contributions into field const PetscInt rnoff = residualVisitor.sectionOffset(v_negative); @@ -631,7 +632,7 @@ pylith::faults::FaultCohesiveDyn::constrainSolnSpace(topology::SolutionFields* c slipRateVertex[d] = 0.0; } // if } // for - if (fabs(slipTpdtVertex[indexN]) < _zeroTolerance) { + if (fabs(slipTpdtVertex[indexN]) < _zeroToleranceNormal) { slipTpdtVertex[indexN] = 0.0; } // if @@ -938,7 +939,7 @@ pylith::faults::FaultCohesiveDyn::constrainSolnSpace(topology::SolutionFields* c dSlipTpdtVertex[indexN] = -slipTpdtVertex[indexN]; } // if/else - } else if (slipTpdtVertex[indexN] + dSlipTpdtVertex[indexN] > _zeroTolerance) { + } else if (slipTpdtVertex[indexN] + dSlipTpdtVertex[indexN] > _zeroToleranceNormal) { // Step 5b: Insure fault traction is zero when opening (if alpha=1 // this should be enforced already, but will not be properly // enforced when alpha < 1). @@ -2150,7 +2151,7 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpaceNorm(const PylithScalar alp slipRateVertex[d] = 0.0; } // if } // for - if (fabs(slipTpdtVertex[indexN]) < _zeroTolerance) { + if (fabs(slipTpdtVertex[indexN]) < _zeroToleranceNormal) { slipTpdtVertex[indexN] = 0.0; } // if @@ -2173,7 +2174,7 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpaceNorm(const PylithScalar alp slipTpdtVertex[indexN] = 0.0; } // if/else - } else if (slipTpdtVertex[indexN] > _zeroTolerance) { + } else if (slipTpdtVertex[indexN] > _zeroToleranceNormal) { // Step b: Ensure fault traction is zero when opening (if // alpha=1 this should be enforced already, but will not be // properly enforced when alpha < 1). @@ -2187,7 +2188,7 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpaceNorm(const PylithScalar alp slipTpdtVertex[indexN] = 0.0; } // if - if (slipTpdtVertex[indexN] > _zeroTolerance) { + if (slipTpdtVertex[indexN] > _zeroToleranceNormal) { isOpening = true; } // if @@ -2292,7 +2293,7 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpace2D(scalar_array* dTractionT const PylithScalar tractionNormal = tractionTpdt[1]; const PylithScalar tractionShearMag = fabs(tractionTpdt[0]); - if (fabs(slip[1]) < _zeroTolerance && tractionNormal < -_zeroTolerance) { + if (fabs(slip[1]) < _zeroToleranceNormal && tractionNormal < -_zeroTolerance) { // if in compression and no opening PylithScalar frictionStress = _friction->calcFriction(t, slipMag, slipRateMag, tractionNormal); @@ -2374,7 +2375,7 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpace3D(scalar_array* dTractionT const PylithScalar tractionNormal = tractionTpdt[2]; const PylithScalar tractionShearMag = sqrt(tractionTpdt[0] * tractionTpdt[0] + tractionTpdt[1] * tractionTpdt[1]); - if (fabs(slip[2]) < _zeroTolerance && tractionNormal < -_zeroTolerance) { + if (fabs(slip[2]) < _zeroToleranceNormal && tractionNormal < -_zeroTolerance) { // if in compression and no opening PylithScalar frictionStress = _friction->calcFriction(t, slipMag, slipRateMag, tractionNormal); diff --git a/libsrc/pylith/faults/FaultCohesiveDyn.hh b/libsrc/pylith/faults/FaultCohesiveDyn.hh index be0b62df2e..fdba1e9f07 100644 --- a/libsrc/pylith/faults/FaultCohesiveDyn.hh +++ b/libsrc/pylith/faults/FaultCohesiveDyn.hh @@ -282,6 +282,9 @@ private : /// Minimum resolvable value accounting for roundoff errors PylithScalar _zeroTolerance; + /// Minimum resolvable value accounting for roundoff errors + PylithScalar _zeroToleranceNormal; + /// Prescribed traction variation. 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--- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1175,7 +1175,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} (\object{TimeHistorySlipFn}). This slip time function requires spatial databases for the amplitude of the final slip and slip initiation time, and a time history file specifying the normalized amplitude as a -function of time. Additional to illustrate PyLith's ability to use +function of time. Additionally, to illustrate PyLith's ability to use spatial databases with points in other, but compatible, georeferenced coordinate systems, we specify the slip distribution using geographic (longitude and latitude) coordinates. @@ -1219,17 +1219,22 @@ \subsection{Step 6: Prescribed Slow-Slip Event}

    time_history.filename

    = spatialdb/fault_slabtop_slowslip.timedb \end{cfg} -You will notice that the \filename{spatialdb} does not contain the -\filename{fault\_slabtop\_slowslip.spatialdb} and +You will notice that the \filename{spatialdb} directory does not +contain the \filename{fault\_slabtop\_slowslip.spatialdb} and \filename{fault\_slabtop\_slowslip.timedb} files. We use the \filename{generate\_slowslip.py} Python script to generate these files -as an illustration of how to use Python to generate more somple +as an illustration of how to use Python to generate more simple spatial variations and the \object{SimpleGridAscii} object to write spatial database files. This script reads parameters from \filename{generate\_slowslip.cfg} to generate a Gaussian slip distribution in geographic coordinates, along with a temporal database providing the slip amplitudes at different times. +\tip{The \filename{generate\_slowslip.py} script is one of several + examples where we make use of the Python interface to the + spatialdata package. This provides useful methods for handling + coordinate systems and spatial databases.} + To run the simulation, first run the Python script to generate the spatial database files, and then run PyLith. \begin{shell} @@ -1362,7 +1367,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} \end{cfg} In addition to defining the fault information, we also set some output -information common to both sub-problems, writing addition info fields +information common to both sub-problems, writing additional info fields for fault output, and turning off material output. If we left material output turned on, we would end up with extremely large state variable output files: @@ -1398,8 +1403,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} \end{cfg} In the output settings, we turn off output for the domain, provide the -coordinate system for the fake cGPS stations, -and provide filenames: +coordinate system for the fake cGPS stations, and provide filenames: \begin{cfg} # Add cggs_sites to solution output. [pylithapp.problem.formulation] @@ -1570,7 +1574,7 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} the body forces. We also demonstrate what happens when the initial stresses are not in balance with the gravitational stresses, and show how viscoelastic problems with gravitational stresses will in general -will not reach a steady-state solution. We do not include faults in +not reach a steady-state solution. We do not include faults in this example. The example is divided into three sub-problems: \begin{itemize} \item Step08a: Gravitational body forces with 3-D density variations @@ -1586,10 +1590,10 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} For the first sub-problem (step08a), we apply gravitational stresses and attempt to balance these with analytically computed stresses -consistent with the density of the mantle. Since the densities are not -constant, the forces are out of balance and we end up with significant -deformation. We first apply gravity and set the simulation time to -zero (static problem): +consistent with the density of the mantle. Since the actual densities +are not constant, the forces are out of balance and we end up with +significant deformation. We first apply gravity and set the simulation +time to zero (static problem): \begin{cfg} [pylithapp.timedependent] # Set gravity field (default is None). @@ -1652,10 +1656,90 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08a_soln} \caption{Image generated by running the \filename{plot\_dispwarp.py} script for sub-problem step08a. The crustal material to the - east is lighter than the assumed mantle material for initial - stresses, while the slab material to the west is heavier. The + east is less dense than the assumed mantle material for initial + stresses, while the slab material to the west is more dense. The result is uplift to the east and downward movement to the west.} \label{fig:example:subduction:3d:step08a} \end{figure} +Sub-problem step08b is similar to step08a, but rather than +analytically computing the initial stresses, we use the stresses +computed in sub-problem step08a. Since the initial stresses are now +computed using the correct densities, the stresses balance and we end +up with no elastic deformation. To generate the initial stress spatial +database, we read the state variables output files from sub-problem +step08a. The script \filename{generate\_initial\_stress.py}, located in +the \filename{spatialdb} directory, will read these files and generate +the necessary spatial database files. Note that this script is another +instance of using the Python interface to the spatialdata package. The +script allows arguments, but the default arguments are appropriate for +this example. Once you are in the \filename{spatialdb} directory, run +the script as follows: +\begin{shell} +$$ ./generate_initial_stress.py +\end{shell} +This will create spatial databases containing initial stresses for +each of the four materials. + +Once we have generated the initial stresses, we can perform the +simulation. Other than filenames, the only difference between +\filename{.cfg} files \filename{step08a.cfg} and +\filename{step08b.cfg} is in the specification of the initial +stresses. There is a separate spatial database for each material, and +since there is an initial stress for each cell centroid, we retain the +default nearest neighbor interpolation method: +\begin{cfg} +# We specify initial stresses for each material via a SimpleDB. +# Since there is a point in the database corresponding to each cell +# center, we keep the default query_type of 'nearest'. +[pylithapp.problem.materials.slab] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the slab +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav-slab.spatialdb + +[pylithapp.problem.materials.wedge] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the wedge +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav-wedge.spatialdb + +[pylithapp.problem.materials.mantle] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the mantle +

    db_initial_stress.iohandler.filename

    = spatialdb/mat_initial_stress_grav-mantle.spatialdb + +[pylithapp.problem.materials.crust] +db_initial_stress = spatialdata.spatialdb.SimpleDB +

    db_initial_stress.label

    = Initial stress in the crust +

    db_initial_stress.iohandler.filename

    = +spatialdb/mat_initial_stress_grav-crust.spatialdb +\end{cfg} + +When we compare the resulting elastic displacements with those of +example step08a, we find that there is essentially no displacement, +as seen in Figure \vref{fig:example:subduction:3d:step08b}. This +figure was also generated with the \filename{plot\_dispwarp.py} +script, using the following command: +\begin{shell} +./viz/plot_dispwarp.py --sim=step08b --exaggeration=1000.0 +--screenshot=subduction3d_step08b_soln.png +\end{shell} +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step08b_soln} + \caption{Image generated by running the \filename{plot\_dispwarp.py} + script for sub-problem step08b. In this case the densities used to + compute the initial stresses are consistent with the actual + densities, and there is no elastic deformation.} + \label{fig:example:subduction:3d:step08b} +\end{figure} + +The final sub-problem is step08c. This problem is very similar to +step08b, but we now use viscoelastic materials, and we use the finite +strain formulation (\object{ImplicitLgDeform}). With this formulation, +the deformed configuration is taken into account, whereas in the +default \object{Implicit} infinitesimal strain formulation, +deformation is not taken into account when computing stresses. The +finite strain formulation should generally be used for viscoelastic +problems with gravity where you need accurate estimates of the +vertical deformation. + % End of file From ae2ad1d562de07421bd3fcc6d88bc73b72e226d3 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Fri, 23 Jun 2017 14:28:09 +1200 Subject: [PATCH 134/216] Finished writing manual section for step08, and added new figures. 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From the \filename{viz} subdirectory, run this script as: \begin{shell} -./plot_inversion_misfit.py +$$ ./plot_inversion_misfit.py --summary=../output/step07-inversion-summary.txt \end{shell} This will produce a curve similar to that shown in Figure @@ -1649,8 +1649,8 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} mesh visualized by running the following command from the \filename{subduction} directory: \begin{shell} -./viz/plot_dispwarp.py --sim=step08a --exaggeration=500.0 ---screenshot=subduction3d_step08a_soln.png +$$ ./viz/plot_dispwarp.py --sim=step08a --exaggeration=500.0 +--component=Z --screenshot=subduction3d_step08a_soln.png \end{shell} \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08a_soln} @@ -1720,8 +1720,8 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} figure was also generated with the \filename{plot\_dispwarp.py} script, using the following command: \begin{shell} -./viz/plot_dispwarp.py --sim=step08b --exaggeration=1000.0 ---screenshot=subduction3d_step08b_soln.png +$$ ./viz/plot_dispwarp.py --sim=step08b --exaggeration=1000.0 +--component=Z --screenshot=subduction3d_step08b_soln.png \end{shell} \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08b_soln} @@ -1742,4 +1742,73 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} problems with gravity where you need accurate estimates of the vertical deformation. +As we saw in step08b, it is possible to balance the stresses for an +elastic problem. Once we include viscoelasticity, however, this +becomes much more difficult. That is what we demonstrate in this +example. Although the stresses are in equilibrium for the elastic +solution, there are still deviatoric stresses remaining, which will +drive viscous flow. Thus, a steady-state solution is never achieved. + +The only difference between the parameters in \filename{step08b.cfg} +and \filename{step08c.cfg} is in the formulation setting and the +simulation time: +\begin{cfg} +[pylithapp.timedependent] +# Turn on the small strain formulation, which automatically runs the +# simulation as a nonlinear problem. +formulation = pylith.problems.ImplicitLgDeform + +# Set gravity field (default is None). +gravity_field = spatialdata.spatialdb.GravityField + +[pylithapp.problem.formulation.time_step] +# Define the total time for the simulation and the time step size. +

      total_time

      = 100.0*year +

      dt

      = 10.0*year +\end{cfg} +We use the material settings in \filename{mat\_viscoelastic.cfg}. We +can run the simulation and visualize the vertical deformation for the +last time step by doing: +\begin{shell} +$$ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg +$$ ./viz/plot_dispwarp.py --sim=step08c --exaggeration=300.0 +--component=Z --screenshot=subduction3d_step08c_soln.png +\end{shell} +The resulting deformation is shown in Figure +\vref{fig:example:subduction:3d:step08c}. As a result of viscous flow, +the vertical deformation is even larger than for sub-problem +step08a. If we were to run the simulation for a longer time period, +the amount of vertical deformation would continue to increase. +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction3d_step08c_soln} + \caption{Image generated by running the \filename{plot\_dispwarp.py} + script for sub-problem step08c. Although the stresses balance in + the elastic solution, viscous flow in subsequent time steps + results in large vertical deformation.} + \label{fig:example:subduction:3d:step08c} +\end{figure} + +\subsubsection{Exercises} + +\begin{itemize} +\item What happens in sub-problem step08a if we use a different + reference density to compute our initial stresses? +\item For sub-problem step08b, what happens if, for one of the + materials you use the initial stresses from sub-problem step08a? +\item For sub-problem step08c, what happens if you: + \begin{itemize} + \item Run the simulation for a longer period of time? + \item Change the viscoelastic properties? For example, reduce the + viscosity, make all materials viscoelastic, switch to a power-law + rheology, etc. + \end{itemize} +\item Is it possible to find a better initial stress state for + sub-problem step08c? + \begin{itemize} + \item What if the initial stresses were computed with nearly + incompressible materials, and all materials in the model are + viscoelastic? + \end{itemize} +\end{itemize} + % End of file diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg index fff8fd9b3b..0db3e94701 100644 --- a/examples/3d/subduction/step08b.cfg +++ b/examples/3d/subduction/step08b.cfg @@ -22,15 +22,6 @@ # stresses from Step08a as the initial stresses; the initial stresses # satisfy equilibrium so there is no deformation. # -# Step08a: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses for a uniform density. -# Step08b: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses from Step08a (initial stresses -# satisfy equilibrium, so there is no deformation). -# Step08c: Gravitational body forces with 3-D density variations in elastic -# and viscoelastic materials and initial stresses from Step08a -# (does not reach a steady-state solution). -# # Materials # All four blocks use the linear, isotropic elastic material model # (mat_elastic.cfg). diff --git a/examples/3d/subduction/step08c.cfg b/examples/3d/subduction/step08c.cfg index 566866177b..d71e4d48ea 100644 --- a/examples/3d/subduction/step08c.cfg +++ b/examples/3d/subduction/step08c.cfg @@ -23,15 +23,6 @@ # materials and the small strain formulation, in which the stresses # are recomputed for the deformed configuration.. # -# Step08a: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses for a uniform density. -# Step08b: Gravitational body forces with 3-D density variations in elastic -# materials and initial stresses from Step08a (initial stresses -# satisfy equilibrium, so there is no deformation). -# Step08c: Gravitational body forces with 3-D density variations in elastic -# and viscoelastic materials and initial stresses from Step08a -# (does not reach a steady-state solution). -# # Materials # The 'wedge' and 'crust' blocks use the the linear, isotropic # elastic material model, whereas the 'slab' and 'mantle' use the From 652e8ca3ef87996e01b2b2cc39b3cc899f4c8510 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 22:34:00 -0700 Subject: [PATCH 135/216] Fix slip-weakening parameters (small Do and 1MPa stress drop). --- .../fault_slabtop_slipweakening.spatialdb | 14 +++++++------- .../subduction/fault_slabtop_tractions.spatialdb | 4 ++-- examples/2d/subduction/stepXX.cfg | 3 ++- 3 files changed, 11 insertions(+), 10 deletions(-) diff --git a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb index 266246bfa6..9b85e7b185 100644 --- a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb +++ b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb @@ -14,7 +14,7 @@ SimpleGridDB { num-y = 6 num-values = 4 value-names = static-coefficient dynamic-coefficient slip-weakening-parameter cohesion - value-units = none none cm Pa + value-units = none none m Pa space-dim = 2 cs-data = cartesian { to-meters = 1.0e+3 @@ -36,9 +36,9 @@ SimpleGridDB { // (5) dynamic-coefficient // (6) slip-weakening-parameter (cm) // (7) cohesion (Pa) -0.0 99.0 0.6 0.6 1.0 0.0 -0.0 -5.0 0.6 0.6 1.0 0.0 -0.0 -15.0 0.6 0.2 1.0 0.0 -0.0 -30.0 0.6 0.2 1.0 0.0 -0.0 -45.0 0.6 0.6 1.0 0.0 -0.0 -999.0 0.6 0.6 1.0 0.0 +0.0 99.0 0.6 0.60 1.0e-8 0.0 +0.0 -5.0 0.6 0.60 1.0e-8 0.0 +0.0 -15.0 0.6 0.55 1.0e-8 0.0 +0.0 -30.0 0.6 0.55 1.0e-8 0.0 +0.0 -45.0 0.6 0.60 1.0e-8 0.0 +0.0 -999.0 0.6 0.60 1.0e-8 0.0 diff --git a/examples/2d/subduction/fault_slabtop_tractions.spatialdb b/examples/2d/subduction/fault_slabtop_tractions.spatialdb index d59fffe1e9..60a1de9b12 100644 --- a/examples/2d/subduction/fault_slabtop_tractions.spatialdb +++ b/examples/2d/subduction/fault_slabtop_tractions.spatialdb @@ -36,7 +36,7 @@ SimpleGridDB { // (5) normal traction (MPa) 0.0 99.0 -11.9 -20.0 0.0 -5.0 -11.9 -20.0 -0.0 -15.0 -10.0 -20.0 -0.0 -30.0 -10.0 -20.0 +0.0 -15.0 -11.0 -20.0 +0.0 -30.0 -11.0 -20.0 0.0 -45.0 -11.9 -20.0 0.0 -999.0 -11.9 -20.0 diff --git a/examples/2d/subduction/stepXX.cfg b/examples/2d/subduction/stepXX.cfg index 37b955d526..bcf7328099 100644 --- a/examples/2d/subduction/stepXX.cfg +++ b/examples/2d/subduction/stepXX.cfg @@ -96,13 +96,14 @@ quadrature.cell.dimension = 1 # Friction friction = pylith.friction.SlipWeakening +#friction = pylith.friction.StaticFriction friction.label = Slip weakening # Force healing after each time step, so weakening is confined to each # time step and does not carry over into subsequent time steps. friction.force_healing = True # Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. -zero_tolerance = 1.0e-10 +zero_tolerance = 1.0e-12 friction.db_properties = spatialdata.spatialdb.SimpleGridDB friction.db_properties.label = Slip weakening From 2645015c1569cfa842586d05cd60a6d18ba3e8f2 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 22 Jun 2017 22:34:31 -0700 Subject: [PATCH 136/216] Fix obsolete call in debugging output. --- libsrc/pylith/faults/FaultCohesiveDyn.cc | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/libsrc/pylith/faults/FaultCohesiveDyn.cc b/libsrc/pylith/faults/FaultCohesiveDyn.cc index 2c92108eae..4e12c3a6d4 100644 --- a/libsrc/pylith/faults/FaultCohesiveDyn.cc +++ b/libsrc/pylith/faults/FaultCohesiveDyn.cc @@ -769,7 +769,7 @@ pylith::faults::FaultCohesiveDyn::constrainSolnSpace(topology::SolutionFields* c break; #if 0 // DEBUGGING - const int rank = _faultMesh->sieveMesh()->commRank(); + const int rank = _faultMesh->commRank(); std::cout << "["< Date: Thu, 22 Jun 2017 22:56:15 -0700 Subject: [PATCH 137/216] Added rate-state db for testing. --- .../fault_slabtop_ratestate.spatialdb | 44 +++++++++++++++++++ 1 file changed, 44 insertions(+) create mode 100644 examples/2d/subduction/fault_slabtop_ratestate.spatialdb diff --git a/examples/2d/subduction/fault_slabtop_ratestate.spatialdb b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb new file mode 100644 index 0000000000..788daad795 --- /dev/null +++ b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb @@ -0,0 +1,44 @@ +// -*- C++ -*- (syntax highlighting) +// +// This spatial database specifies the distribution of slip rate +// associated with aseismic creep on the interface between the mantle +// and the subducting oceanic crust. +// +// We specify depth-dependent frictional properties with stable +// sliding (equal dynamic and static coefficients of friction) above +// and below the seismogenic zone (elevations of -5 km to -45 km). +// +#SPATIAL_GRID.ascii 1 +SimpleGridDB { + num-x = 1 + num-y = 6 + num-values = 6 + value-names = reference-friction-coefficient reference-slip-rate characteristic-slip-distance constitutive-parameter-a constitutive-parameter-b cohesion + value-units = none m/s m none none Pa + space-dim = 2 + cs-data = cartesian { + to-meters = 1.0e+3 + space-dim = 2 + } +} // SimpleGridDB + +// x coordinate +0.0 + +// y coordinate +99.0 -5.0 -15.0 -35.0 -45.0 -999.0 + +// Columns are +// (1) x coordinate (km) +// (2) y coordinate (km) +// (3) z coordinate (km) +// (4) static-coefficient +// (5) dynamic-coefficient +// (6) slip-weakening-parameter (cm) +// (7) cohesion (Pa) +0.0 99.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 -5.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 -15.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 -30.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 -45.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 -999.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 From 75b3f16cbe6a5f054e44457213c764d995c96d05 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 13:33:45 -0700 Subject: [PATCH 138/216] Remove unused variables. --- libsrc/pylith/faults/EqKinSrc.hh | 1 + unittests/libtests/faults/TestBruneSlipFn.cc | 2 -- unittests/libtests/faults/TestConstRateSlipFn.cc | 2 -- unittests/libtests/faults/TestLiuCosSlipFn.cc | 2 -- unittests/libtests/faults/TestStepSlipFn.cc | 2 -- unittests/libtests/faults/TestTimeHistorySlipFn.cc | 2 -- 6 files changed, 1 insertion(+), 10 deletions(-) diff --git a/libsrc/pylith/faults/EqKinSrc.hh b/libsrc/pylith/faults/EqKinSrc.hh index f5176595d1..1e955ba20a 100644 --- a/libsrc/pylith/faults/EqKinSrc.hh +++ b/libsrc/pylith/faults/EqKinSrc.hh @@ -49,6 +49,7 @@ public : EqKinSrc(void); /// Destructor. + virtual ~EqKinSrc(void); /// Deallocate PETSc and local data structures. diff --git a/unittests/libtests/faults/TestBruneSlipFn.cc b/unittests/libtests/faults/TestBruneSlipFn.cc index 35084b9aae..1adb620b3e 100644 --- a/unittests/libtests/faults/TestBruneSlipFn.cc +++ b/unittests/libtests/faults/TestBruneSlipFn.cc @@ -310,7 +310,6 @@ pylith::faults::TestBruneSlipFn::_initialize(topology::Mesh* mesh, CPPUNIT_ASSERT(mesh); CPPUNIT_ASSERT(faultMesh); CPPUNIT_ASSERT(slipfn); - PetscErrorCode err; const char* meshFilename = "data/tri3.mesh"; const char* faultLabel = "fault"; @@ -370,7 +369,6 @@ pylith::faults::TestBruneSlipFn::_testInitialize(const _TestBruneSlipFn::DataStr { // _testInitialize PYLITH_METHOD_BEGIN; - PetscErrorCode err; // Setup mesh topology::Mesh mesh; meshio::MeshIOAscii meshIO; diff --git a/unittests/libtests/faults/TestConstRateSlipFn.cc b/unittests/libtests/faults/TestConstRateSlipFn.cc index 3888309f71..19ed22bca4 100644 --- a/unittests/libtests/faults/TestConstRateSlipFn.cc +++ b/unittests/libtests/faults/TestConstRateSlipFn.cc @@ -239,7 +239,6 @@ pylith::faults::TestConstRateSlipFn::_initialize(topology::Mesh* mesh, CPPUNIT_ASSERT(mesh); CPPUNIT_ASSERT(faultMesh); CPPUNIT_ASSERT(slipfn); - PetscErrorCode err; const char* meshFilename = "data/tri3.mesh"; const char* faultLabel = "fault"; @@ -292,7 +291,6 @@ pylith::faults::TestConstRateSlipFn::_testInitialize(const _TestConstRateSlipFn: { // _testInitialize PYLITH_METHOD_BEGIN; - PetscErrorCode err; // Setup mesh topology::Mesh mesh; meshio::MeshIOAscii meshIO; diff --git a/unittests/libtests/faults/TestLiuCosSlipFn.cc b/unittests/libtests/faults/TestLiuCosSlipFn.cc index 8d46bbf05b..1ee5968e7d 100644 --- a/unittests/libtests/faults/TestLiuCosSlipFn.cc +++ b/unittests/libtests/faults/TestLiuCosSlipFn.cc @@ -303,7 +303,6 @@ pylith::faults::TestLiuCosSlipFn::_initialize(topology::Mesh* mesh, PYLITH_METHOD_BEGIN; assert(slipfn); - PetscErrorCode err; const char* meshFilename = "data/tri3.mesh"; const char* faultLabel = "fault"; @@ -363,7 +362,6 @@ pylith::faults::TestLiuCosSlipFn::_testInitialize(const _TestLiuCosSlipFn::DataS { // _testInitialize PYLITH_METHOD_BEGIN; - PetscErrorCode err; // Setup mesh topology::Mesh mesh; meshio::MeshIOAscii meshIO; diff --git a/unittests/libtests/faults/TestStepSlipFn.cc b/unittests/libtests/faults/TestStepSlipFn.cc index 5de01091ca..07ec30678e 100644 --- a/unittests/libtests/faults/TestStepSlipFn.cc +++ b/unittests/libtests/faults/TestStepSlipFn.cc @@ -235,7 +235,6 @@ pylith::faults::TestStepSlipFn::_initialize(topology::Mesh* mesh, CPPUNIT_ASSERT(mesh); CPPUNIT_ASSERT(faultMesh); CPPUNIT_ASSERT(slipfn); - PetscErrorCode err; const char* meshFilename = "data/tri3.mesh"; const char* faultLabel = "fault"; @@ -288,7 +287,6 @@ pylith::faults::TestStepSlipFn::_testInitialize(const _TestStepSlipFn::DataStruc { // _testInitialize PYLITH_METHOD_BEGIN; - PetscErrorCode err; // Setup mesh topology::Mesh mesh; meshio::MeshIOAscii meshIO; diff --git a/unittests/libtests/faults/TestTimeHistorySlipFn.cc b/unittests/libtests/faults/TestTimeHistorySlipFn.cc index f5df28fdaf..3eeb7cc2eb 100644 --- a/unittests/libtests/faults/TestTimeHistorySlipFn.cc +++ b/unittests/libtests/faults/TestTimeHistorySlipFn.cc @@ -265,7 +265,6 @@ pylith::faults::TestTimeHistorySlipFn::_initialize(topology::Mesh* mesh, PYLITH_METHOD_BEGIN; assert(slipfn); - PetscErrorCode err; const char* meshFilename = "data/tri3.mesh"; const char* faultLabel = "fault"; @@ -323,7 +322,6 @@ pylith::faults::TestTimeHistorySlipFn::_testInitialize(const _TestTimeHistorySli { // _testInitialize PYLITH_METHOD_BEGIN; - PetscErrorCode err; // Setup mesh topology::Mesh mesh; meshio::MeshIOAscii meshIO; From 872413802bd788cc7d19a3b74290732faab167b2 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:01:38 -0700 Subject: [PATCH 139/216] Add step05 and step06 to 2-D subduction example. --- examples/2d/subduction/Makefile.am | 7 +- examples/2d/subduction/README | 24 +- ...patialdb => fault_slabtop_creep.spatialdb} | 0 .../fault_slabtop_ratestate.spatialdb | 21 +- .../fault_slabtop_slipweakening.spatialdb | 5 +- examples/2d/subduction/step02.cfg | 2 +- examples/2d/subduction/step03.cfg | 2 +- .../2d/subduction/{stepXX.cfg => step05.cfg} | 43 ++-- examples/2d/subduction/step06.cfg | 236 ++++++++++++++++++ examples/2d/subduction/viz/plot_dispwarp.py | 2 +- examples/2d/subduction/viz/plot_shearratio.py | 2 +- 11 files changed, 299 insertions(+), 45 deletions(-) rename examples/2d/subduction/{fault_creep_slabtop.spatialdb => fault_slabtop_creep.spatialdb} (100%) rename examples/2d/subduction/{stepXX.cfg => step05.cfg} (88%) create mode 100644 examples/2d/subduction/step06.cfg diff --git a/examples/2d/subduction/Makefile.am b/examples/2d/subduction/Makefile.am index b5ee0077a2..c779258d82 100644 --- a/examples/2d/subduction/Makefile.am +++ b/examples/2d/subduction/Makefile.am @@ -23,12 +23,17 @@ dist_noinst_DATA = \ step02.cfg \ step03.cfg \ step04.cfg \ + step05.cfg \ + step06.cfg \ geometry.jou \ mesh_tri3.jou \ createbc.jou \ mesh_tri3.exo \ fault_slip_coseismic.spatialdb \ - fault_creep_slabtop.spatialdb \ + fault_slabtop_creep.spatialdb \ + fault_slabtop_ratestate.spatialdb \ + fault_slabtop_slipweakening.spatialdb \ + fault_slabtop_tractions.spatialdb \ mat_concrust.spatialdb \ mat_conmantle.spatialdb \ mat_oceancrust.spatialdb \ diff --git a/examples/2d/subduction/README b/examples/2d/subduction/README index a21ee87d81..256f18ecf0 100644 --- a/examples/2d/subduction/README +++ b/examples/2d/subduction/README @@ -70,7 +70,7 @@ Step 2. Interseismic deformation simulation constant 8 cm/yr. The parameters for the creep along the top of the slab are defined in - fault_creep_slabtop.spatialdb + fault_slabtop_creep.spatialdb Run the simulation via the following command: pylith step02.cfg @@ -97,6 +97,28 @@ Step 4. Friction controlled afterslip Run the simulation via the following command: pylith step04.cfg +Step 5. Earthquake cycle with slip-weakening friction + + This simulation uses drives sponaneous rupture on the subducting + interface using prescribed asesismic slip on the bottom of the + slab. We use the slip-weakening friction model on the subducting + interface. + + Run the simulation and capture the output via the following commands: + pylith step05.cfg >& step05.log & + tail -f step05.log + +Step 6. Earthquake cycle with rate-state friction + + This simulation uses drives sponaneous rupture on the subducting + interface using prescribed asesismic slip on the bottom of the + slab. We use the rate-state friction model on the subducting + interface. + + Run the simulation and capture the output via the following commands: + pylith step06.cfg >& step06.log & + tail -f step06.log + Suggestions variations The list below includes some suggested modifications to the problem diff --git a/examples/2d/subduction/fault_creep_slabtop.spatialdb b/examples/2d/subduction/fault_slabtop_creep.spatialdb similarity index 100% rename from examples/2d/subduction/fault_creep_slabtop.spatialdb rename to examples/2d/subduction/fault_slabtop_creep.spatialdb diff --git a/examples/2d/subduction/fault_slabtop_ratestate.spatialdb b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb index 788daad795..b8d912dc20 100644 --- a/examples/2d/subduction/fault_slabtop_ratestate.spatialdb +++ b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb @@ -1,8 +1,7 @@ // -*- C++ -*- (syntax highlighting) // -// This spatial database specifies the distribution of slip rate -// associated with aseismic creep on the interface between the mantle -// and the subducting oceanic crust. +// This spatial database specifies the distribution of rate and state +// friction parameters for the subducting interface. // // We specify depth-dependent frictional properties with stable // sliding (equal dynamic and static coefficients of friction) above @@ -14,7 +13,7 @@ SimpleGridDB { num-y = 6 num-values = 6 value-names = reference-friction-coefficient reference-slip-rate characteristic-slip-distance constitutive-parameter-a constitutive-parameter-b cohesion - value-units = none m/s m none none Pa + value-units = none cm/year m none none Pa space-dim = 2 cs-data = cartesian { to-meters = 1.0e+3 @@ -34,11 +33,11 @@ SimpleGridDB { // (3) z coordinate (km) // (4) static-coefficient // (5) dynamic-coefficient -// (6) slip-weakening-parameter (cm) +// (6) slip-weakening-parameter (m) // (7) cohesion (Pa) -0.0 99.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 -0.0 -5.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 -0.0 -15.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 -0.0 -30.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 -0.0 -45.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 -0.0 -999.0 0.6 1.0e-12 0.05 0.01 0.08 0.0 +0.0 99.0 0.6 1.0 0.2 0.015 0.010 0.0 +0.0 -5.0 0.6 1.0 0.2 0.015 0.010 0.0 +0.0 -15.0 0.6 1.0 0.2 0.015 0.017 0.0 +0.0 -30.0 0.6 1.0 0.2 0.015 0.017 0.0 +0.0 -45.0 0.6 1.0 0.2 0.015 0.010 0.0 +0.0 -999.0 0.6 1.0 0.2 0.015 0.010 0.0 diff --git a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb index 9b85e7b185..17d964e204 100644 --- a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb +++ b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb @@ -1,8 +1,7 @@ // -*- C++ -*- (syntax highlighting) // -// This spatial database specifies the distribution of slip rate -// associated with aseismic creep on the interface between the mantle -// and the subducting oceanic crust. +// This spatial database specifies the distribution of slip-weakening +// friction properties for the subducting interface. // // We specify depth-dependent frictional properties with stable // sliding (equal dynamic and static coefficients of friction) above diff --git a/examples/2d/subduction/step02.cfg b/examples/2d/subduction/step02.cfg index 3483aada05..417db7d6dd 100644 --- a/examples/2d/subduction/step02.cfg +++ b/examples/2d/subduction/step02.cfg @@ -92,7 +92,7 @@ slip_function = pylith.faults.ConstRateSlipFn # The slip time and final slip are defined in spatial databases. [pylithapp.timedependent.interfaces.fault_slabtop.eq_srcs.rupture.slip_function] -slip_rate.iohandler.filename = fault_creep_slabtop.spatialdb +slip_rate.iohandler.filename = fault_slabtop_creep.spatialdb slip_rate.query_type = linear slip_rate.label = Final slip diff --git a/examples/2d/subduction/step03.cfg b/examples/2d/subduction/step03.cfg index 768f09f3db..0a162a3ccc 100644 --- a/examples/2d/subduction/step03.cfg +++ b/examples/2d/subduction/step03.cfg @@ -109,7 +109,7 @@ slip_function = pylith.faults.ConstRateSlipFn # The slip time and final slip are defined in spatial databases. [pylithapp.timedependent.interfaces.fault_slabtop.eq_srcs.creep.slip_function] -slip_rate.iohandler.filename = fault_creep_slabtop.spatialdb +slip_rate.iohandler.filename = fault_slabtop_creep.spatialdb slip_rate.query_type = linear slip_rate.label = Final slip diff --git a/examples/2d/subduction/stepXX.cfg b/examples/2d/subduction/step05.cfg similarity index 88% rename from examples/2d/subduction/stepXX.cfg rename to examples/2d/subduction/step05.cfg index bcf7328099..d6185e0a8f 100644 --- a/examples/2d/subduction/stepXX.cfg +++ b/examples/2d/subduction/step05.cfg @@ -4,9 +4,10 @@ # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- # -# This simulation involves aseismic creep along the interfaces between -# the subducting oceanic crust and the mantle. The slip rate is a -# constant 8 cm/yr. +# This simulation models an earthquake cycle with spontaneous ruptures +# on the subduction interfaces using slip-weakening friction. The +# deformation is drive by aseismic creep (8 cm/yr) along the bottom +# interface between the subducting oceanic crust and the mantle. # # ---------------------------------------------------------------------- # RUNNING THE SIMULATON @@ -19,9 +20,9 @@ # reads by default. # # To run the simulation: -# pylith step02.cfg +# pylith step05.cfg # -# Output will be directed to directory output. +# Output will be directed to the 'output' directory. # ---------------------------------------------------------------------- # problem @@ -33,7 +34,7 @@ solver = pylith.problems.SolverNonlinear [pylithapp.timedependent.formulation.time_step] total_time = 100.0*year -dt = 5.0*year +dt = 2.5*year # ---------------------------------------------------------------------- # boundary conditions @@ -91,20 +92,13 @@ id = 100 quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 1 - - - # Friction friction = pylith.friction.SlipWeakening -#friction = pylith.friction.StaticFriction friction.label = Slip weakening # Force healing after each time step, so weakening is confined to each -# time step and does not carry over into subsequent time steps. +# time step and is not carried over into subsequent time steps. friction.force_healing = True -# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. -zero_tolerance = 1.0e-12 - friction.db_properties = spatialdata.spatialdb.SimpleGridDB friction.db_properties.label = Slip weakening friction.db_properties.filename = fault_slabtop_slipweakening.spatialdb @@ -117,12 +111,11 @@ traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb [pylithapp.problem.interfaces.fault_slabtop.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/stepXX-fault-slabtop.h5 +writer.filename = output/step05-fault-slabtop.h5 vertex_info_fields = [normal_dir, strike_dir] vertex_data_fields = [slip, slip_rate, traction] - # Slab bottom -------------------- [pylithapp.timedependent.interfaces.fault_slabbot] # The label corresponds to the name of the nodeset in CUBIT. @@ -156,37 +149,37 @@ slip_time.data = [0.0*year] # ---------------------------------------------------------------------- # Domain [pylithapp.problem.formulation.output.domain] -writer.filename = output/stepXX.h5 +writer.filename = output/step05.h5 time_step = 1.0*year # Ground surface [pylithapp.problem.formulation.output.subdomain] -writer.filename = output/stepXX-groundsurf.h5 +writer.filename = output/step05-groundsurf.h5 # Faults [pylithapp.problem.interfaces.fault_slabtop.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/stepXX-fault-slabtop.h5 +writer.filename = output/step05-fault-slabtop.h5 [pylithapp.problem.interfaces.fault_slabbot.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/stepXX-fault-slabbot.h5 +writer.filename = output/step05-fault-slabbot.h5 # Materials [pylithapp.timedependent.materials.continent_crust.output] -writer.filename = output/stepXX-concrust.h5 +writer.filename = output/step05-concrust.h5 cell_data_fields = [] [pylithapp.timedependent.materials.continent_mantle.output] -writer.filename = output/stepXX-conmantle.h5 +writer.filename = output/step05-conmantle.h5 cell_data_fields = [] [pylithapp.timedependent.materials.ocean_crust.output] -writer.filename = output/stepXX-oceancrust.h5 +writer.filename = output/step05-oceancrust.h5 cell_data_fields = [] [pylithapp.timedependent.materials.ocean_mantle.output] -writer.filename = output/stepXX-oceanmantle.h5 +writer.filename = output/step05-oceanmantle.h5 cell_data_fields = [] @@ -194,9 +187,9 @@ cell_data_fields = [] # PETSc # ---------------------------------------------------------------------- [pylithapp.timedependent.interfaces.fault_slabtop] +# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. zero_tolerance = 1.0e-8 - [pylithapp.petsc] malloc_dump = diff --git a/examples/2d/subduction/step06.cfg b/examples/2d/subduction/step06.cfg new file mode 100644 index 0000000000..b63e492528 --- /dev/null +++ b/examples/2d/subduction/step06.cfg @@ -0,0 +1,236 @@ +[pylithapp] + +# ---------------------------------------------------------------------- +# PROBLEM DESCRIPTION +# ---------------------------------------------------------------------- +# +# This simulation models an earthquake cycle with spontaneous ruptures +# on the subduction interfaces using rate-state friction. The +# deformation is drive by aseismic creep (8 cm/yr) along the bottom +# interface between the subducting oceanic crust and the mantle. +# +# ---------------------------------------------------------------------- +# RUNNING THE SIMULATON +# ---------------------------------------------------------------------- +# +# This is not a self-contained simulation configuration file. This +# file specifies only the boundary conditions and earthquake +# parameters for the simulation. The general quasi-static and mesh +# parameters are specificed in the pylithapp.cfg file which PyLith +# reads by default. +# +# To run the simulation: +# pylith step06.cfg +# +# Output will be directed to the 'output' directory. + +# ---------------------------------------------------------------------- +# problem +# ---------------------------------------------------------------------- +[pylithapp.problem.formulation] +# Fault friction is a nonlinear problem so we need to use the +# nonlinear solver. +solver = pylith.problems.SolverNonlinear + +[pylithapp.timedependent.formulation.time_step] +total_time = 200.0*year +dt = 1.0*year + +# ---------------------------------------------------------------------- +# boundary conditions +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +# Set bc to an array of 3 boundary conditions: +# 'boundary_east_mantle' +# 'boundary_west' +# 'boundary_bottom_mantle' +bc = [boundary_east_mantle,boundary_west,boundary_bottom_mantle] + +# For all boundaries, we fix the displacement normal to the boundary +# (roller boundary condition) by retaining the default ZeroDispDB, +# which specifies a zero value. +# +# The label corresponds to the name of the nodeset in CUBIT. + +# East boundary (mantle) +[pylithapp.timedependent.bc.boundary_east_mantle] +bc_dof = [0] +label = bndry_east_mantle +db_initial.label = Dirichlet BC on east boundary (mantle) + +# West boundary +[pylithapp.timedependent.bc.boundary_west] +bc_dof = [0,1] +label = bndry_west +db_initial.label = Dirichlet BC on west boundary + +# Bottom boundary (mantle) +[pylithapp.timedependent.bc.boundary_bottom_mantle] +bc_dof = [1] +label = bndry_bot_mantle +db_initial.label = Dirichlet BC on bottom boundary (mantle) + +# ---------------------------------------------------------------------- +# faults +# ---------------------------------------------------------------------- +[pylithapp.timedependent] +interfaces = [fault_slabtop,fault_slabbot] + +# Set the type of fault interface condition. +[pylithapp.timedependent.interfaces] +fault_slabtop = pylith.faults.FaultCohesiveDyn +fault_slabbot = pylith.faults.FaultCohesiveKin + +# Slab top -------------------- +[pylithapp.timedependent.interfaces.fault_slabtop] +# The label corresponds to the name of the nodeset in CUBIT. +label = fault_slabtop +id = 100 + +# We must define the quadrature information for fault cells. +# The fault cells are 1D (line). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 1 + +# Friction +friction = pylith.friction.RateStateAgeing +friction.label = Rate-state friction +# Nondimensional slip rate below which friction is linear +friction.linear_slip_rate = 1.0e-6 + +# Set spatial database for distribution of friction parameters +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +friction.db_properties.label = Slip weakening +friction.db_properties.filename = fault_slabtop_ratestate.spatialdb + +# Set spatial database for the initial value of the state variable. +friction.db_initial_state = spatialdata.spatialdb.UniformDB +friction.db_initial_state.label = Rate State Ageing State +friction.db_initial_state.values = [state-variable] +# theta_ss = characteristic_slip_dist / reference_slip_rate +friction.db_initial_state.data = [20.0*year] + +# Initial fault tractions +traction_perturbation = pylith.faults.TractPerturbation +#traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB +#traction_perturbation.db_initial.label = Initial fault tractions +#traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb + +traction_perturbation.db_initial = spatialdata.spatialdb.UniformDB +traction_perturbation.db_initial.label = Initial fault tractions +traction_perturbation.db_initial.values = [traction-shear, traction-normal] +traction_perturbation.db_initial.data = [-12.0*MPa, -20.0*MPa] + + +[pylithapp.problem.interfaces.fault_slabtop.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slabtop.h5 +vertex_info_fields = [normal_dir, strike_dir] +vertex_data_fields = [slip, slip_rate, traction, state_variable] + + +# Slab bottom -------------------- +[pylithapp.timedependent.interfaces.fault_slabbot] +# The label corresponds to the name of the nodeset in CUBIT. +label = fault_slabbot +id = 101 + +# We must define the quadrature information for fault cells. +# The fault cells are 1D (line). +quadrature.cell = pylith.feassemble.FIATSimplex +quadrature.cell.dimension = 1 + +# Switch to constant slip rate time function. +[pylithapp.timedependent.interfaces.fault_slabbot.eq_srcs.rupture] +slip_function = pylith.faults.ConstRateSlipFn + +# The creep rate and slip time are uniform, so use UniformDB for simplicity. +[pylithapp.timedependent.interfaces.fault_slabbot.eq_srcs.rupture.slip_function] +slip_rate = spatialdata.spatialdb.UniformDB +slip_rate.label = Slip rate +slip_rate.values = [left-lateral-slip, fault-opening] +slip_rate.data = [8.0*cm/year, 0.0*cm/year] + +# Slip time is uniform, so use UniformDB for convenience +slip_time = spatialdata.spatialdb.UniformDB +slip_time.label = Slip time +slip_time.values = [slip-time] +slip_time.data = [0.0*year] + +# ---------------------------------------------------------------------- +# output +# ---------------------------------------------------------------------- +# Domain +[pylithapp.problem.formulation.output.domain] +writer.filename = output/step06.h5 +time_step = 1.0*year + +# Ground surface +[pylithapp.problem.formulation.output.subdomain] +writer.filename = output/step06-groundsurf.h5 + +# Faults +[pylithapp.problem.interfaces.fault_slabtop.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slabtop.h5 + +[pylithapp.problem.interfaces.fault_slabbot.output] +writer = pylith.meshio.DataWriterHDF5 +writer.filename = output/step06-fault-slabbot.h5 + +# Materials +[pylithapp.timedependent.materials.continent_crust.output] +writer.filename = output/step06-concrust.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.continent_mantle.output] +writer.filename = output/step06-conmantle.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.ocean_crust.output] +writer.filename = output/step06-oceancrust.h5 +cell_data_fields = [] + +[pylithapp.timedependent.materials.ocean_mantle.output] +writer.filename = output/step06-oceanmantle.h5 +cell_data_fields = [] + + +# ---------------------------------------------------------------------- +# PETSc +# ---------------------------------------------------------------------- +[pylithapp.timedependent.interfaces.fault_slabtop] +# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. +zero_tolerance = 2.0e-9 +zero_tolerance_normal = 1.0e-8 + +[pylithapp.petsc] +malloc_dump = + +# Convergence parameters. +ksp_rtol = 1.0e-20 +ksp_atol = 1.0e-9 +ksp_max_it = 1000 +ksp_gmres_restart = 50 + +snes_rtol = 1.0e-20 +snes_atol = 1.0e-7 + +snes_max_it = 500 + + +# Friction sensitivity solve used to compute the increment in slip +# associated with changes in the Lagrange multiplier imposed by the +# fault constitutive model. +friction_pc_type = asm +friction_sub_pc_factor_shift_type = nonzero +friction_ksp_max_it = 25 +friction_ksp_gmres_restart = 30 +friction_ksp_error_if_not_converged = true + +# Uncomment to view details of friction sensitivity solve. +#friction_ksp_monitor = true +#friction_ksp_view = true +#friction_ksp_converged_reason = true + +# End of file diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py index af97fc0bb3..2b317947fe 100755 --- a/examples/2d/subduction/viz/plot_dispwarp.py +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -26,7 +26,7 @@ # pvpython. # Root name for simulation. -SIM_NAME = "stepXX" +SIM_NAME = "step05" # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 diff --git a/examples/2d/subduction/viz/plot_shearratio.py b/examples/2d/subduction/viz/plot_shearratio.py index aa51f2cb42..c5f97442e0 100755 --- a/examples/2d/subduction/viz/plot_shearratio.py +++ b/examples/2d/subduction/viz/plot_shearratio.py @@ -28,7 +28,7 @@ # pvpython. # Root name for simulation. -SIM_NAME = "stepXX" +SIM_NAME = "step05" # Names of faults (with spontaneous rupture) for output files. FAULTS = ["fault-slabtop"] From 26ba027474895a9add7b69e36f0e8b397beceac0 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:02:17 -0700 Subject: [PATCH 140/216] Add separate zero tolerance for suppressing near zero values of fault opening. --- .../boundaryconditions/boundaryconditions.tex | 37 ++++++++++++------- libsrc/pylith/faults/FaultCohesiveDyn.cc | 28 ++++++++++++-- libsrc/pylith/faults/FaultCohesiveDyn.hh | 10 ++++- modulesrc/faults/FaultCohesiveDyn.i | 6 +++ pylith/faults/FaultCohesiveDyn.py | 17 +++++---- .../libtests/faults/TestFaultCohesiveDyn.cc | 16 +++++--- .../libtests/faults/TestFaultCohesiveDyn.hh | 2 +- 7 files changed, 82 insertions(+), 34 deletions(-) diff --git a/doc/userguide/boundaryconditions/boundaryconditions.tex b/doc/userguide/boundaryconditions/boundaryconditions.tex index 5cd48a41d9..79f27a5de8 100644 --- a/doc/userguide/boundaryconditions/boundaryconditions.tex +++ b/doc/userguide/boundaryconditions/boundaryconditions.tex @@ -1199,14 +1199,20 @@ \subsubsection{Dynamic Rupture Parameters} The properties and facilities of the \object{FaultCohesiveDyn} object include \begin{inventory} -\propertyitem{open\_free\_surface}{If true, enforce traction free surface when -the fault opens, otherwise apply prescribed tractions even when the -fault opens (default is true); to mimic a dike opening, use false.} -\propertyitem{zero\_tolerance}{Tolerance for detecting zero values (default -is 1.0e-10); should be larger than absolute tolerance in KSP solves.} -\facilityitem{traction\_perturbation}{Prescribed tractions on fault surface -(generally used for nucleating earthquake ruptures; default is none).} -\facilityitem{friction}{Fault constitutive model.} + \propertyitem{open\_free\_surface}{If true, enforce traction free + surface when the fault opens, otherwise apply prescribed tractions + even when the fault opens (default is true); to mimic a dike + opening, use false.} + \propertyitem{zero\_tolerance}{Tolerance for detecting zero values + (default is 1.0e-10); should be larger than absolute tolerance in + KSP solves.} + \propertyitem{zero\_tolerance\_normal}{Tolerance for + suppressing near zero fault opening values (default is 1.0e-10); + should be larger than absolute tolerance in KSP solves.} + \facilityitem{traction\_perturbation}{Prescribed tractions on fault + surface (generally used for nucleating earthquake ruptures; + default is none).} + \facilityitem{friction}{Fault constitutive model.} \end{inventory} An example of specifying the dynamic earthquake rupture properties and components in a \filename{.cfg} file: @@ -1229,15 +1235,20 @@ \subsubsection{Dynamic Rupture Parameters} \important{The dynamic rupture implementation requires careful selection of linear and nonlinear solver tolerances. A key issue is making sure the linear solver toleance is tighter (smaller) than the - tolerance used to detect slip (fault \property{zero\_toelerance}). - As a result, the linear and solver absolute tolerances should be - used to for convergence, not the relative tolerances. The settings below - illustrates the relevant parameters and example values. The values - can be scaled to change the overall desired tolerances.} + tolerance used to detect slip (fault \property{zero\_toelerance} and + \property{zero\_toelerance\_normal}). As a result, the linear and + solver absolute tolerances should be used to for convergence, not + the relative tolerances. The settings below illustrates the relevant + parameters and example values. The values can be scaled to change + the overall desired tolerances. The separate tolerance for near zero + values of fault opening was added in v2.2.1. This provides the + solver greater flexibility to prevent fault opening with nonplanar + faults..} \begin{cfg} [pylithapp.problem.interfaces.fault]

      zero_tolerance

      = 1.0e-11 +

      zero_tolerance_normal

      = 2.0e-11 [pylithapp.petsc] # Linear solver tolerances diff --git a/libsrc/pylith/faults/FaultCohesiveDyn.cc b/libsrc/pylith/faults/FaultCohesiveDyn.cc index 4e12c3a6d4..2028504447 100644 --- a/libsrc/pylith/faults/FaultCohesiveDyn.cc +++ b/libsrc/pylith/faults/FaultCohesiveDyn.cc @@ -54,7 +54,8 @@ #include // USES std::ostringstream #include // USES std::runtime_error -#include // TEMPORARY +//#include // TEMPORARY +//#define DISABLE_SLIPRATE_TOLERANCE //#define DETAILED_EVENT_LOGGING @@ -62,7 +63,7 @@ // Default constructor. pylith::faults::FaultCohesiveDyn::FaultCohesiveDyn(void) : _zeroTolerance(1.0e-10), - _zeroToleranceNormal(1.0e-8), + _zeroToleranceNormal(1.0e-10), _tractPerturbation(0), _friction(0), _jacobian(0), @@ -126,6 +127,21 @@ pylith::faults::FaultCohesiveDyn::zeroTolerance(const PylithScalar value) _zeroTolerance = value; } // zeroTolerance +// ---------------------------------------------------------------------- +// Nondimensional tolerance for detecting near zero fault opening values. +void +pylith::faults::FaultCohesiveDyn::zeroToleranceNormal(const PylithScalar value) +{ // zeroToleranceNormal + if (value < 0.0) { + std::ostringstream msg; + msg << "Tolerance (" << value << ") for suppressing zero values for fault opening for " + "fault " << label() << " must be nonnegative."; + throw std::runtime_error(msg.str()); + } // if + + _zeroToleranceNormal = value; +} // zeroToleranceNormal + // ---------------------------------------------------------------------- // Set flag used to determine when fault is traction free when it // opens or it still imposes any initial tractions. @@ -628,9 +644,11 @@ pylith::faults::FaultCohesiveDyn::constrainSolnSpace(topology::SolutionFields* c slipRateVertex[d] += orientationArray[ooff+d*spaceDim+e] * (dispTIncrArray[dipoff+e] - dispTIncrArray[dinoff+e]) / dt; tractionTpdtVertex[d] += orientationArray[ooff+d*spaceDim+e] * (dispTArray[dtloff+e] + dispTIncrArray[diloff+e]); } // for - if (fabs(slipRateVertex[d]) < _zeroTolerance) { +#if !defined(DISABLE_SLIPRATE_TOLERANCE) // 2017-06-23 Is this really necessary? + if (fabs(slipRateVertex[d]) < _zeroTolerance / dt) { slipRateVertex[d] = 0.0; } // if +#endif } // for if (fabs(slipTpdtVertex[indexN]) < _zeroToleranceNormal) { slipTpdtVertex[indexN] = 0.0; @@ -2147,9 +2165,11 @@ pylith::faults::FaultCohesiveDyn::_constrainSolnSpaceNorm(const PylithScalar alp slipRateVertex[d] += orientationArray[ooff+d*spaceDim+e] * (dispTIncrArray[dipoff+e] - dispTIncrArray[dinoff+e] + alpha*sensDispRelArray[sdroff+e]) / dt; tractionTpdtVertex[d] += orientationArray[ooff+d*spaceDim+e] * (dispTArray[dtloff+e] + dispTIncrArray[diloff+e] + alpha*dLagrangeArray[sdloff+e]); } // for - if (fabs(slipRateVertex[d]) < _zeroTolerance) { +#if !defined(DISABLE_SLIPRATE_TOLERANCE) // 2017-06-23 Is this really necessary? + if (fabs(slipRateVertex[d]) < _zeroTolerance / dt) { slipRateVertex[d] = 0.0; } // if +#endif } // for if (fabs(slipTpdtVertex[indexN]) < _zeroToleranceNormal) { slipTpdtVertex[indexN] = 0.0; diff --git a/libsrc/pylith/faults/FaultCohesiveDyn.hh b/libsrc/pylith/faults/FaultCohesiveDyn.hh index fdba1e9f07..4f17a3972d 100644 --- a/libsrc/pylith/faults/FaultCohesiveDyn.hh +++ b/libsrc/pylith/faults/FaultCohesiveDyn.hh @@ -73,6 +73,12 @@ public : */ void zeroTolerance(const PylithScalar value); + /** Nondimensional tolerance for suppressing near zero values of fault opening. + * + * @param value Nondimensional tolerance + */ + void zeroToleranceNormal(const PylithScalar value); + /** Set flag used to determine when fault is traction free when it * opens or it still imposes any initial tractions. * @@ -279,10 +285,10 @@ private : // PRIVATE MEMBERS //////////////////////////////////////////////////// private : - /// Minimum resolvable value accounting for roundoff errors + /// Minimum resolvable value accounting for roundoff errors. PylithScalar _zeroTolerance; - /// Minimum resolvable value accounting for roundoff errors + /// Minimum resolvable value accounting for roundoff errors for fault opening. PylithScalar _zeroToleranceNormal; /// Prescribed traction variation. diff --git a/modulesrc/faults/FaultCohesiveDyn.i b/modulesrc/faults/FaultCohesiveDyn.i index 1759b9c8a6..c6557505bd 100644 --- a/modulesrc/faults/FaultCohesiveDyn.i +++ b/modulesrc/faults/FaultCohesiveDyn.i @@ -59,6 +59,12 @@ namespace pylith { */ void zeroTolerance(const PylithScalar value); + /** Nondimensional tolerance for suppressing near zero values of fault opening. + * + * @param value Nondimensional tolerance + */ + void zeroToleranceNormal(const PylithScalar value); + /** Set flag used to determine when fault is traction free when it * opens or it still imposes any initial tractions. * diff --git a/pylith/faults/FaultCohesiveDyn.py b/pylith/faults/FaultCohesiveDyn.py index 3d07513a03..8a01969595 100644 --- a/pylith/faults/FaultCohesiveDyn.py +++ b/pylith/faults/FaultCohesiveDyn.py @@ -43,6 +43,7 @@ class FaultCohesiveDyn(FaultCohesive, Integrator, ModuleFaultCohesiveDyn): \b Properties @li \b zero_tolerance Tolerance for detecting zero values. + @li \b zero_tolerance_normal Tolerance for suppressing near zero values of fault opening. @li \b open_free_surface If True, enforce traction free surface when the fault opens, otherwise use initial tractions even when the fault opens. @@ -59,26 +60,25 @@ class FaultCohesiveDyn(FaultCohesive, Integrator, ModuleFaultCohesiveDyn): import pyre.inventory - zeroTolerance = pyre.inventory.float("zero_tolerance", default=1.0e-10, - validator=pyre.inventory.greaterEqual(0.0)) + zeroTolerance = pyre.inventory.float("zero_tolerance", default=1.0e-10, validator=pyre.inventory.greater(0.0)) zeroTolerance.meta['tip'] = "Tolerance for detecting zero values." + zeroToleranceNormal = pyre.inventory.float("zero_tolerance_normal", default=1.0e-10, validator=pyre.inventory.greater(0.0)) + zeroToleranceNormal.meta['tip'] = "Tolerance for suppressing near zero values of fault opening." + openFreeSurf = pyre.inventory.bool("open_free_surface", default=True) openFreeSurf.meta['tip'] = "If True, enforce traction free surface when " \ "the fault opens, otherwise use initial tractions even when the " \ "fault opens." - tract = pyre.inventory.facility("traction_perturbation", family="traction_perturbation", - factory=NullComponent) + tract = pyre.inventory.facility("traction_perturbation", family="traction_perturbation", factory=NullComponent) tract.meta['tip'] = "Prescribed perturbation in fault tractions." from pylith.friction.StaticFriction import StaticFriction - friction = pyre.inventory.facility("friction", family="friction_model", - factory=StaticFriction) + friction = pyre.inventory.facility("friction", family="friction_model", factory=StaticFriction) from pylith.meshio.OutputFaultDyn import OutputFaultDyn - output = pyre.inventory.facility("output", family="output_manager", - factory=OutputFaultDyn) + output = pyre.inventory.facility("output", family="output_manager", factory=OutputFaultDyn) output.meta['tip'] = "Output manager associated with fault data." @@ -214,6 +214,7 @@ def _configure(self): ModuleFaultCohesiveDyn.tractPerturbation(self, self.inventory.tract) ModuleFaultCohesiveDyn.frictionModel(self, self.inventory.friction) ModuleFaultCohesiveDyn.zeroTolerance(self, self.inventory.zeroTolerance) + ModuleFaultCohesiveDyn.zeroToleranceNormal(self, self.inventory.zeroToleranceNormal) ModuleFaultCohesiveDyn.openFreeSurf(self, self.inventory.openFreeSurf) self.output = self.inventory.output return diff --git a/unittests/libtests/faults/TestFaultCohesiveDyn.cc b/unittests/libtests/faults/TestFaultCohesiveDyn.cc index 398133b85f..93e0bcdb3c 100644 --- a/unittests/libtests/faults/TestFaultCohesiveDyn.cc +++ b/unittests/libtests/faults/TestFaultCohesiveDyn.cc @@ -111,7 +111,7 @@ pylith::faults::TestFaultCohesiveDyn::testTractPerturbation(void) } // testTractPerturbation // ---------------------------------------------------------------------- -// Test zeroTolerance(). +// Test zeroTolerance() and zeroToleranceNormal(). void pylith::faults::TestFaultCohesiveDyn::testZeroTolerance(void) { // testZeroTolerance @@ -121,10 +121,16 @@ pylith::faults::TestFaultCohesiveDyn::testZeroTolerance(void) CPPUNIT_ASSERT_EQUAL(PylithScalar(1.0e-10), fault._zeroTolerance); // default - const PylithScalar value = 1.0e-20; + PylithScalar value = 1.0e-20; fault.zeroTolerance(value); CPPUNIT_ASSERT_EQUAL(value, fault._zeroTolerance); + CPPUNIT_ASSERT_EQUAL(PylithScalar(1.0e-10), fault._zeroToleranceNormal); // default + + value = 1.0e-8; + fault.zeroToleranceNormal(value); + CPPUNIT_ASSERT_EQUAL(value, fault._zeroToleranceNormal); + PYLITH_METHOD_END; } // zeroTolerance @@ -207,7 +213,7 @@ pylith::faults::TestFaultCohesiveDyn::testInitialize(void) const PylithScalar tolerance = 1.0e-06; for(PetscInt d = 0; d < spaceDim; ++d) { - CPPUNIT_ASSERT_DOUBLES_EQUAL(_data->initialTractions[iVertex * spaceDim + d], tractionArray[off+d]*_data->pressureScale, tolerance); + CPPUNIT_ASSERT_DOUBLES_EQUAL(_data->initialTractions[iVertex * spaceDim + d], tractionArray[off+d]*tractionScale, tolerance); } // for } // for } // if @@ -504,8 +510,6 @@ pylith::faults::TestFaultCohesiveDyn::testUpdateStateVars(void) topology::Jacobian jacobian(fields.solution()); _setFieldsJacobian(&mesh, &fault, &fields, &jacobian, _data->fieldIncrSlip); - const int spaceDim = _data->spaceDim; - const PylithScalar t = 2.134; const PylithScalar dt = 0.01; fault.timeStep(dt); @@ -794,7 +798,7 @@ pylith::faults::TestFaultCohesiveDyn::_isConstraintEdge(const int point) const const int numConstraintEdges = _data->numConstraintEdges; bool isFound = false; - for (int i=0; i < _data->numConstraintEdges; ++i) + for (int i=0; i < numConstraintEdges; ++i) if (_data->constraintEdges[i] == point) { isFound = true; break; diff --git a/unittests/libtests/faults/TestFaultCohesiveDyn.hh b/unittests/libtests/faults/TestFaultCohesiveDyn.hh index 98edb69cc4..2dfd8e52e5 100644 --- a/unittests/libtests/faults/TestFaultCohesiveDyn.hh +++ b/unittests/libtests/faults/TestFaultCohesiveDyn.hh @@ -91,7 +91,7 @@ public: /// Test tractPerturbation(). void testTractPerturbation(void); - /// Test zeroTolerance(). + /// Test zeroTolerance() and zeroToleranceNormal(). void testZeroTolerance(void); /// Test openFreeSurf(). From 9af5e75faff9c821aa30881ef78106a8a728007c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:03:18 -0700 Subject: [PATCH 141/216] Add time step to auto test for reasonable slip rate. --- tests_auto/2d/tri3/sheardispfriction.cfg | 1 + 1 file changed, 1 insertion(+) diff --git a/tests_auto/2d/tri3/sheardispfriction.cfg b/tests_auto/2d/tri3/sheardispfriction.cfg index 3830239bdd..923a9da4c5 100644 --- a/tests_auto/2d/tri3/sheardispfriction.cfg +++ b/tests_auto/2d/tri3/sheardispfriction.cfg @@ -41,6 +41,7 @@ formulation.solver = pylith.problems.SolverNonlinear [sheardispfriction.timedependent.formulation.time_step] total_time = 0.0*s +dt = 10.0*year # ---------------------------------------------------------------------- # materials From fa1a2f20a835f872101be06d1028adf56a60c5b2 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:31:32 -0700 Subject: [PATCH 142/216] Set correct number of digits for time stamp. --- examples/2d/subduction/viz/plot_dispwarp.py | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py index 2b317947fe..8182a6bd29 100755 --- a/examples/2d/subduction/viz/plot_dispwarp.py +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -84,12 +84,12 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): # Annotate time tstamp = AnnotateTimeFilter(warp) - tstamp.Format = 'Time: %2.0f yr' + tstamp.Format = 'Time: %5.1f yr' tstamp.Scale = 3.168808781402895e-08 # seconds to years tstampDisplay = Show(tstamp, view) tstampDisplay.FontFamily = "Courier" - tstampDisplay.FontSize = 14 + tstampDisplay.FontSize = 12 view.ResetCamera() view.Update() From ed118dffb7f439385f209a3050c842be037efa1d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:32:28 -0700 Subject: [PATCH 143/216] Updated step05 setttings. Not working yet --- .../fault_slabtop_slipweakening.spatialdb | 14 ++++++------- .../fault_slabtop_tractions.spatialdb | 9 ++++---- examples/3d/subduction/step05.cfg | 21 ++++++++++++------- 3 files changed, 24 insertions(+), 20 deletions(-) diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb index 8f4878bbb2..7e07101fd8 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_slipweakening.spatialdb @@ -15,7 +15,7 @@ SimpleGridDB { num-z = 6 num-values = 4 value-names = static-coefficient dynamic-coefficient slip-weakening-parameter cohesion - value-units = none none cm Pa + value-units = none none m Pa space-dim = 3 cs-data = geo-projected { to-meters = 1.0e+3 // Specify coordinates in km for convenience. @@ -50,9 +50,9 @@ SimpleGridDB { // (5) dynamic-coefficient // (6) slip-weakening-parameter (cm) // (7) cohesion (Pa) -0.0 0.0 99.0 0.6 0.6 1.0 0.0 -0.0 0.0 -5.0 0.6 0.6 1.0 0.0 -0.0 0.0 -15.0 0.6 0.2 1.0 0.0 -0.0 0.0 -30.0 0.6 0.2 1.0 0.0 -0.0 0.0 -45.0 0.6 0.6 1.0 0.0 -0.0 0.0 -999.0 0.6 0.6 1.0 0.0 +0.0 0.0 99.0 0.6 0.60 1.0e-8 0.0 +0.0 0.0 -5.0 0.6 0.60 1.0e-8 0.0 +0.0 0.0 -15.0 0.6 0.55 1.0e-8 0.0 +0.0 0.0 -30.0 0.6 0.55 1.0e-8 0.0 +0.0 0.0 -45.0 0.6 0.60 1.0e-8 0.0 +0.0 0.0 -999.0 0.6 0.60 1.0e-8 0.0 diff --git a/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb index 926dbda225..64cb925967 100644 --- a/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb +++ b/examples/3d/subduction/spatialdb/fault_slabtop_tractions.spatialdb @@ -1,8 +1,7 @@ // -*- C++ -*- (syntax highlighting) // -// This spatial database specifies the distribution of slip rate -// associated with aseismic creep on the interface between the mantle -// and the subducting oceanic crust. +// This spatial database specifies the distribution of initial fault +// tractions on the subducting interface. // // We specify depth-dependent fault tractions with higher values in // the stable sliding regions consistent with residual stresses in @@ -51,7 +50,7 @@ SimpleGridDB { // (6) normal traction (MPa) 0.0 0.0 99.0 0.0 11.9 -20.0 0.0 0.0 -5.0 0.0 11.9 -20.0 -0.0 0.0 -15.0 0.0 10.0 -20.0 -0.0 0.0 -30.0 0.0 10.0 -20.0 +0.0 0.0 -15.0 0.0 11.0 -20.0 +0.0 0.0 -30.0 0.0 11.0 -20.0 0.0 0.0 -45.0 0.0 11.9 -20.0 0.0 0.0 -999.0 0.0 11.9 -20.0 diff --git a/examples/3d/subduction/step05.cfg b/examples/3d/subduction/step05.cfg index 44927b7cea..27b6526dea 100644 --- a/examples/3d/subduction/step05.cfg +++ b/examples/3d/subduction/step05.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey @@ -64,8 +64,8 @@ solver = pylith.problems.SolverNonlinear [pylithapp.problem.formulation.time_step] # Define the total time for the simulation and the time step size. -total_time = 200.0*year -dt = 10.0*year +total_time = 100.0*year +dt = 2.5*year # ---------------------------------------------------------------------- # boundary conditions @@ -120,9 +120,6 @@ friction.label = Slip weakening # time step and does not carry over into subsequent time steps. friction.force_healing = True -# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. -zero_tolerance = 1.0e-10 - friction.db_properties = spatialdata.spatialdb.SimpleGridDB friction.db_properties.label = Slip weakening friction.db_properties.filename = spatialdb/fault_slabtop_slipweakening.spatialdb @@ -137,6 +134,7 @@ traction_perturbation.db_initial.filename = spatialdb/fault_slabtop_tractions.sp writer = pylith.meshio.DataWriterHDF5 writer.filename = output/step05-fault-slabtop.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] +vertex_data_fields = [slip, slip_rate, traction] # Slab bottom ---------------------------------------------------------- [pylithapp.problem.interfaces.slab_bottom] @@ -198,15 +196,22 @@ writer.filename = output/step05-mantle.h5 # ---------------------------------------------------------------------- # PETSc # ---------------------------------------------------------------------- +[pylithapp.problem.interfaces.slab_top] +# Zero tolerance for locking fault (no slip). Must be larger than ksp tolerance. +zero_tolerance = 1.0e-8 +zero_tolerance_normal = 1.0e-8 + [pylithapp.petsc] malloc_dump = # Convergence parameters. ksp_rtol = 1.0e-20 -ksp_atol = 1.0e-11 +ksp_atol = 1.0e-9 snes_rtol = 1.0e-20 -snes_atol = 1.0e-9 +snes_atol = 1.0e-7 + +snes_max_it = 300 # Friction sensitivity solve used to compute the increment in slip # associated with changes in the Lagrange multiplier imposed by the From 0cb3731f9c2e963cd19f2acb12f02fe806a901a9 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:33:00 -0700 Subject: [PATCH 144/216] Add header. --- examples/2d/subduction/step01.cfg | 16 ++++++++++++++-- examples/2d/subduction/step02.cfg | 16 ++++++++++++++-- examples/2d/subduction/step03.cfg | 16 ++++++++++++++-- examples/2d/subduction/step04.cfg | 16 ++++++++++++++-- examples/2d/subduction/step05.cfg | 18 +++++++++++++++--- examples/2d/subduction/step06.cfg | 16 ++++++++++++++-- 6 files changed, 85 insertions(+), 13 deletions(-) diff --git a/examples/2d/subduction/step01.cfg b/examples/2d/subduction/step01.cfg index dad01a1dec..1a75d1c28f 100644 --- a/examples/2d/subduction/step01.cfg +++ b/examples/2d/subduction/step01.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step02.cfg b/examples/2d/subduction/step02.cfg index 417db7d6dd..a61ca2bbd6 100644 --- a/examples/2d/subduction/step02.cfg +++ b/examples/2d/subduction/step02.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step03.cfg b/examples/2d/subduction/step03.cfg index 0a162a3ccc..a895c3477a 100644 --- a/examples/2d/subduction/step03.cfg +++ b/examples/2d/subduction/step03.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step04.cfg b/examples/2d/subduction/step04.cfg index e97975e0c6..2f061668f9 100644 --- a/examples/2d/subduction/step04.cfg +++ b/examples/2d/subduction/step04.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step05.cfg b/examples/2d/subduction/step05.cfg index d6185e0a8f..502237e16c 100644 --- a/examples/2d/subduction/step05.cfg +++ b/examples/2d/subduction/step05.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- @@ -84,8 +96,8 @@ fault_slabbot = pylith.faults.FaultCohesiveKin # Slab top -------------------- [pylithapp.timedependent.interfaces.fault_slabtop] # The label corresponds to the name of the nodeset in CUBIT. -label = fault_slabtop id = 100 +label = fault_slabtop # We must define the quadrature information for fault cells. # The fault cells are 1D (line). diff --git a/examples/2d/subduction/step06.cfg b/examples/2d/subduction/step06.cfg index b63e492528..3df951c7f4 100644 --- a/examples/2d/subduction/step06.cfg +++ b/examples/2d/subduction/step06.cfg @@ -1,5 +1,17 @@ -[pylithapp] - +# -*- Config -*- (syntax highlighting) +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# # ---------------------------------------------------------------------- # PROBLEM DESCRIPTION # ---------------------------------------------------------------------- From 773837a84c880e11b33aa367774cd4c3c0cb12aa Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:33:21 -0700 Subject: [PATCH 145/216] Fix comment in spatial database file. --- examples/2d/subduction/fault_slabtop_tractions.spatialdb | 5 ++--- 1 file changed, 2 insertions(+), 3 deletions(-) diff --git a/examples/2d/subduction/fault_slabtop_tractions.spatialdb b/examples/2d/subduction/fault_slabtop_tractions.spatialdb index 60a1de9b12..ced0b575c3 100644 --- a/examples/2d/subduction/fault_slabtop_tractions.spatialdb +++ b/examples/2d/subduction/fault_slabtop_tractions.spatialdb @@ -1,8 +1,7 @@ // -*- C++ -*- (syntax highlighting) // -// This spatial database specifies the distribution of slip rate -// associated with aseismic creep on the interface between the mantle -// and the subducting oceanic crust. +// This spatial database specifies the distribution of initial fault +// tractions on the subducting interface. // // We specify depth-dependent fault tractions with higher values in // the stable sliding regions consistent with residual stresses in From 50495bb95b56743895175c476e27bac973b7e011 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:34:33 -0700 Subject: [PATCH 146/216] Added Makefile.am for examples/3d/subduction. --- configure.ac | 1 + examples/3d/Makefile.am | 3 +- examples/3d/subduction/Makefile.am | 76 ++++++++++++++++++++++++++++++ 3 files changed, 79 insertions(+), 1 deletion(-) create mode 100644 examples/3d/subduction/Makefile.am diff --git a/configure.ac b/configure.ac index 22d81dca35..85656a7da0 100644 --- a/configure.ac +++ b/configure.ac @@ -336,6 +336,7 @@ AC_CONFIG_FILES([Makefile examples/3d/Makefile examples/3d/tet4/Makefile examples/3d/hex8/Makefile + examples/3d/subduction/Makefile examples/2d/Makefile examples/2d/subduction/Makefile examples/2d/gravity/Makefile diff --git a/examples/3d/Makefile.am b/examples/3d/Makefile.am index d6578c9e7a..58ced0bcaf 100644 --- a/examples/3d/Makefile.am +++ b/examples/3d/Makefile.am @@ -18,6 +18,7 @@ SUBDIRS = \ hex8 \ - tet4 + tet4 \ + subduction # End of file diff --git a/examples/3d/subduction/Makefile.am b/examples/3d/subduction/Makefile.am new file mode 100644 index 0000000000..875c14b4d4 --- /dev/null +++ b/examples/3d/subduction/Makefile.am @@ -0,0 +1,76 @@ +# -*- Makefile -*- +# +# ---------------------------------------------------------------------- +# +# Brad T. Aagaard, U.S. Geological Survey +# Charles A. Williams, GNS Science +# Matthew G. Knepley, University of Chicago +# +# This code was developed as part of the Computational Infrastructure +# for Geodynamics (http://geodynamics.org). +# +# Copyright (c) 2010-2017 University of California, Davis +# +# See COPYING for license information. +# +# ---------------------------------------------------------------------- +# + +dist_noinst_DATA = \ + README \ + pylithapp.cfg \ + greensfns.cfg \ + mat_elastic.cfg \ + mat_viscoelastic.cfg \ + solver_algebraicmultigrid.cfg \ + solver_fieldsplit.cfg \ + step01.cfg \ + step02.cfg \ + step03.cfg \ + step04.cfg \ + step05.cfg \ + step06.cfg \ + step07a.cfg \ + step07b.cfg \ + step08a.cfg \ + step08b.cfg \ + step08c.cfg \ + make_synthetic_gpsdisp.cfg \ + slip_invert.cfg \ + make_synthetic_gpsdisp.py \ + slip_invert.py \ + mesh/bc.jou \ + mesh/cas_contours_dep.in.txt.gz \ + mesh/coordsys.py \ + mesh/generate_surfjou.py \ + mesh/geometry.jou \ + mesh/__init__.py \ + mesh/mesh_hex.jou \ + mesh/mesh_tet.jou \ + spatialdb/mat_crust_elastic.spatialdb \ + spatialdb/mat_mantle_elastic.spatialdb \ + spatialdb/mat_slab_elastic.spatialdb \ + spatialdb/mat_wedge_elastic.spatialdb \ + spatialdb/mat_viscosity.spatialdb \ + spatialdb/mat_initial_stress_grav.spatialdb \ + spatialdb/fault_slabtop_coseismic.spatialdb \ + spatialdb/fault_slabtop_creep.spatialdb \ + spatialdb/fault_slabtop_slipweakening.spatialdb \ + spatialdb/fault_slabtop_tractions.spatialdb \ + spatialdb/generate_initial_stress.py \ + spatialdb/generate_slowslip.cfg \ + spatialdb/generate_slowslip.py \ + viz/plot_dispvec.py \ + viz/plot_dispwarp.py \ + viz/plot_faultdir.py \ + viz/plot_faultslip.py \ + viz/plot_faultslip-reltract.py \ + viz/plot_matprops.py \ + viz/plot_mesh.py \ + viz/plot_inversion_misfit.py \ + viz/get_coast.sh \ + viz/seg2vtk.py \ + viz/cascadia_tm.vtk + + +# End of file From a0c51fdaffc62591d38447bd7cabc2d67faf661c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:34:54 -0700 Subject: [PATCH 147/216] Correct file type in header. --- examples/3d/subduction/step01.cfg | 2 +- examples/3d/subduction/step02.cfg | 2 +- examples/3d/subduction/step03.cfg | 2 +- examples/3d/subduction/step04.cfg | 2 +- examples/3d/subduction/step06.cfg | 2 +- examples/3d/subduction/step07a.cfg | 2 +- examples/3d/subduction/step07b.cfg | 2 +- examples/3d/subduction/step08a.cfg | 2 +- examples/3d/subduction/step08b.cfg | 2 +- examples/3d/subduction/step08c.cfg | 2 +- 10 files changed, 10 insertions(+), 10 deletions(-) diff --git a/examples/3d/subduction/step01.cfg b/examples/3d/subduction/step01.cfg index e298499139..b8c1ac48b8 100644 --- a/examples/3d/subduction/step01.cfg +++ b/examples/3d/subduction/step01.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step02.cfg b/examples/3d/subduction/step02.cfg index bbeaf204f5..71e0785590 100644 --- a/examples/3d/subduction/step02.cfg +++ b/examples/3d/subduction/step02.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step03.cfg b/examples/3d/subduction/step03.cfg index add152c1cf..f86143e8cd 100644 --- a/examples/3d/subduction/step03.cfg +++ b/examples/3d/subduction/step03.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index 4394a9d269..b5fb19b2f5 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index 8ba91ff3b8..dee7931b2c 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step07a.cfg b/examples/3d/subduction/step07a.cfg index 391879cb0e..33b2f8a21e 100644 --- a/examples/3d/subduction/step07a.cfg +++ b/examples/3d/subduction/step07a.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step07b.cfg b/examples/3d/subduction/step07b.cfg index bdd3eee36f..aae46eebb3 100644 --- a/examples/3d/subduction/step07b.cfg +++ b/examples/3d/subduction/step07b.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg index 93286d71ae..60afc8305e 100644 --- a/examples/3d/subduction/step08a.cfg +++ b/examples/3d/subduction/step08a.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg index 0db3e94701..06ed34ab65 100644 --- a/examples/3d/subduction/step08b.cfg +++ b/examples/3d/subduction/step08b.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/step08c.cfg b/examples/3d/subduction/step08c.cfg index d71e4d48ea..01df0e50fb 100644 --- a/examples/3d/subduction/step08c.cfg +++ b/examples/3d/subduction/step08c.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey From 7002bc09b146b4a2ca5a309d2a7ad6eb54852f36 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:35:10 -0700 Subject: [PATCH 148/216] Update copyright script. --- doc/developer/update_copyright.sh | 7 ++++--- 1 file changed, 4 insertions(+), 3 deletions(-) diff --git a/doc/developer/update_copyright.sh b/doc/developer/update_copyright.sh index 1d42b4e280..05a298a58a 100644 --- a/doc/developer/update_copyright.sh +++ b/doc/developer/update_copyright.sh @@ -1,9 +1,10 @@ #!/bin/bash -for suffix in .cc .icc .hh .c .h .am .py .i .jou .odb .ac .in .dat .sh; do +for suffix in .cc .icc .hh .c .h .am .py .i .jou .odb .ac .in .dat; do for f in `find . -name "*$suffix"` aclocal.m4 COPYING ; do + sed -e "s/Copyright (c) 2010-2015 University of California, Davis/Copyright (c) 2010-2017 University of California, Davis/g" $f > tmp && mv -f tmp $f + sed -e "s/Copyright (c) 2010-2016 University of California, Davis/Copyright (c) 2010-2017 University of California, Davis/g" $f > tmp && mv -f tmp $f sed -e "s/Copyright (c) 2010-2017 University of California, Davis/Copyright (c) 2010-2017 University of California, Davis/g" $f > tmp && mv -f tmp $f - sed -e "s/Copyright (c) 2010-2017 University of California, Davis/Copyright (c) 2010-2017 University of California, Davis/g" $f > tmp && mv -f tmp $f - sed -e "s/Copyright (c) 2010-2017 University of California, Davis/Copyright (c) 2010-2017 University of California, Davis/g" $f > tmp && mv -f tmp $f + sed -e "s/Matthew G. Knepley, University of Chicago/Matthew G. Knepley, Rice University/g" $f > tmp && mv -f tmp $f done done From 0d3356abc1783fc896d7986460588287ac005570 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 16:35:35 -0700 Subject: [PATCH 149/216] Add more highlighting to note on Darwin installation. --- doc/userguide/install/install.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index 00af507b9b..fe425aee45 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -78,10 +78,10 @@ \subsection{Linux and Max OS X} (for Linux) environment variables. This will prevent most conflicts.} -\important{The PyLith binary distribution for {\bf Darwin} systems is +\warning{The PyLith binary distribution for {\bf Darwin} systems is built using the system clang compiler suite and the system - Python. This means the system Python must be in your path to use the - PyLith binary executable; ensure \filename{/bin} and + Python. {\bf This means the system Python must be in your path to use the + PyLith binary executable}; ensure \filename{/bin} and \filename{/usr/bin} are at the beginning of the PATH environment variable before sourcing \filename{setup.sh}. {\bf This usually applies if you have Python installed from Anaconda, HomeBrew, From 635efc2f29498f6adc96f8411d761f9660090577 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 21:39:18 -0700 Subject: [PATCH 150/216] Added filesnames for progress and parameters. --- examples/2d/subduction/README | 20 ++++++++----------- examples/2d/subduction/step01.cfg | 7 +++++++ examples/2d/subduction/step02.cfg | 7 +++++++ examples/2d/subduction/step03.cfg | 7 +++++++ examples/2d/subduction/step04.cfg | 7 +++++++ examples/2d/subduction/step05.cfg | 7 +++++++ examples/2d/subduction/step06.cfg | 7 +++++++ .../2d/subduction/{ => viz}/plot_faultinfo.py | 0 8 files changed, 50 insertions(+), 12 deletions(-) rename examples/2d/subduction/{ => viz}/plot_faultinfo.py (100%) diff --git a/examples/2d/subduction/README b/examples/2d/subduction/README index 256f18ecf0..780eca8598 100644 --- a/examples/2d/subduction/README +++ b/examples/2d/subduction/README @@ -4,7 +4,7 @@ M9.0 Tohoku earthquake off the east coast of Japan. The main features of this example are: - * Generating a finite-element mesh using CUBIT + * Generating a finite-element mesh using CUBIT/Trelis + Nonplanar geometry + Variable mesh resolution * Spatially variable coseismic slip and creep @@ -43,10 +43,10 @@ Mesh generation (optional) NOTE: The result of this step will overwrite the included file tri3_mesh.exo. You may want to copy/rename this file so that you have a backup copy in case you have difficulty running - CUBIT. + CUBIT/Trelis. - Start CUBIT and play the journal file "mesh_tri3.jou". We highly - recommend that you study the contents of the journal files to + Start CUBIT/Trelis and play the journal file "mesh_tri3.jou". We + highly recommend that you study the contents of the journal files to understand the mesh generation process. @@ -143,12 +143,8 @@ Suggestions variations Add points, update num-locs accordingly, and change data-dim to be 1. - * Modify the CUBIT journal files to use quad4 cells rather than tri3 - cells. This requires using the pave mesh scheme. - - * Create a simulation with multiple earthquake cycles by lengthening - the duration of the simulation and adding additional earthquake - ruptures. See examples/3d/hex8/step06.cfg for an example with - multiple earthquake ruptures. Examine spinup towards a - steady-state solution. + * Modify the CUBIT/Trelis journal files to use quad4 cells rather + than tri3 cells. This requires using the pave mesh scheme. + * Adjust the friction model parameters and examine the effects on + the deformation and the convergence of the nonlinear solve. diff --git a/examples/2d/subduction/step01.cfg b/examples/2d/subduction/step01.cfg index 1a75d1c28f..4d7709d13b 100644 --- a/examples/2d/subduction/step01.cfg +++ b/examples/2d/subduction/step01.cfg @@ -36,6 +36,13 @@ # # Output will be directed to directory output. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step01-parameters.json +problem.progress_monitor.filename = output/step01-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step02.cfg b/examples/2d/subduction/step02.cfg index a61ca2bbd6..2a11ee5acb 100644 --- a/examples/2d/subduction/step02.cfg +++ b/examples/2d/subduction/step02.cfg @@ -35,6 +35,13 @@ # # Output will be directed to directory output. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step02-parameters.json +problem.progress_monitor.filename = output/step02-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step03.cfg b/examples/2d/subduction/step03.cfg index a895c3477a..df6cee45b3 100644 --- a/examples/2d/subduction/step03.cfg +++ b/examples/2d/subduction/step03.cfg @@ -35,6 +35,13 @@ # # Output will be directed to directory output. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step03-parameters.json +problem.progress_monitor.filename = output/step03-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step04.cfg b/examples/2d/subduction/step04.cfg index 2f061668f9..07b497cfb6 100644 --- a/examples/2d/subduction/step04.cfg +++ b/examples/2d/subduction/step04.cfg @@ -37,6 +37,13 @@ # # Output will be directed to directory output. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step04-parameters.json +problem.progress_monitor.filename = output/step04-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step05.cfg b/examples/2d/subduction/step05.cfg index 502237e16c..331de42d01 100644 --- a/examples/2d/subduction/step05.cfg +++ b/examples/2d/subduction/step05.cfg @@ -36,6 +36,13 @@ # # Output will be directed to the 'output' directory. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step05-parameters.json +problem.progress_monitor.filename = output/step05-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/step06.cfg b/examples/2d/subduction/step06.cfg index 3df951c7f4..b4b0623c84 100644 --- a/examples/2d/subduction/step06.cfg +++ b/examples/2d/subduction/step06.cfg @@ -36,6 +36,13 @@ # # Output will be directed to the 'output' directory. +# ---------------------------------------------------------------------- +# Output of parameters used and simulation progress. +# ---------------------------------------------------------------------- +[pylithapp] +dump_parameters.filename = output/step06-parameters.json +problem.progress_monitor.filename = output/step06-progress.txt + # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/plot_faultinfo.py b/examples/2d/subduction/viz/plot_faultinfo.py similarity index 100% rename from examples/2d/subduction/plot_faultinfo.py rename to examples/2d/subduction/viz/plot_faultinfo.py From b8885e6bf0deede4f8c89fb9d4abe74a4a19abe3 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 21:41:42 -0700 Subject: [PATCH 151/216] Trivial code cleanup. --- examples/2d/subduction/viz/plot_faultinfo.py | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/2d/subduction/viz/plot_faultinfo.py b/examples/2d/subduction/viz/plot_faultinfo.py index ce0b9f148b..0387220627 100644 --- a/examples/2d/subduction/viz/plot_faultinfo.py +++ b/examples/2d/subduction/viz/plot_faultinfo.py @@ -26,7 +26,7 @@ def getStep01(): """ # Open solution file and get slip and coordinates. - h5 = h5py.File("output/step01-fault.h5", "r", driver='sec2') + h5 = h5py.File("output/step01-fault.h5", "r") vertices = h5['geometry/vertices'][:] slip = h5['vertex_fields/slip'][0,:,0].squeeze() traction_change = h5['vertex_fields/traction_change'][0,:,:].squeeze() From e7031cdb3b63c074709a7eebb704318b8a50fe20 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 21:58:44 -0700 Subject: [PATCH 152/216] Add note that step05 is incomplete. --- doc/userguide/examples/subduction3d.tex | 5 ++++- 1 file changed, 4 insertions(+), 1 deletion(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index a38d437b64..e3a74305d0 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1097,7 +1097,10 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 5: Spontaneous Rupture Driven by Subducting Slab} -\subsubsection{Exercises} +This example is not yet complete. The parameters need to be fine tuned +to produce the desired behavior and improve the convergence for the +nonlinear solve. See Steps 5 and 6 in Section +\vref{sec:example:subduction:2d} for a 2-D example. % ---------------------------------------------------------------------- \subsection{Step 6: Prescribed Slow-Slip Event} From 3b5ec7babe6cbdcd9af01d57242a97a3fd28ea8b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 21:59:12 -0700 Subject: [PATCH 153/216] Started work on adding step05 and step06 to 2-D subduction zone. --- doc/userguide/examples/subduction2d.tex | 21 +++++++++++++++------ 1 file changed, 15 insertions(+), 6 deletions(-) diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index f080a30944..976fefcd86 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -20,12 +20,12 @@ \section{Example for Slip on a 2D Subduction Zone} \item Plane strain linearly elastic material \item Plane Maxwell linear viscoelastic material \item Prescribed slip +\item Spontaneous rupture \item Static fault rupture \item Multiple faults \item Spatially variable coseismic slip \item Spatially variable aseismic creep \item Afterslip via fault friction -\item Static fault rupture \item Static friction \end{itemize} All of the files necessary to run the examples are contained in the @@ -43,7 +43,10 @@ \subsection{Overview} focuses on interseismic deformation, and Step 3 combines the two into a pseudo-earthquake cycle deformation simulation. Step 4 focuses on using the change in tractions from Step 1 to construct a simulation -with afterslip controlled by frictional sliding. +with afterslip controlled by frictional sliding. Steps 5 and 6 replace +the prescribed aseismic slip on the subducting slab in Step 2 with a +frictional interface, producing spontaneous earthquake ruptures and +creep. \begin{figure} \includegraphics{examples/figs/subduction2d_cartoon_general} @@ -356,6 +359,14 @@ \subsection{Step 4: Frictional Afterslip Simulation} \end{figure} +\subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} + +\todo{brad}{ADD STUFF HERE} + +\subsection{Step 5: Spontaneous Earthquakes With Rate-State Friction} + +\todo{brad}{ADD STUFF HERE} + \subsection{Suggested Variations} The list below includes some suggested modifications to the problem @@ -377,10 +388,8 @@ \subsection{Suggested Variations} and change data-dim to 1. \item Modify the CUBIT journal files to use quad4 cells rather than tri3 cells. This requires using the pave mesh scheme. -\item Create a simulation with multiple earthquake cycles by lengthening - the duration of the simulation and adding additional earthquake ruptures. - See \filename{examples/3d/hex8/step06.cfg} for an example with multiple - earthquake ruptures. Examine spinup towards a steady-state solution. +\item Adjust the friction model parameters and examine the effects on + the deformation and the convergence of the nonlinear solve. \end{itemize} From b317b3b635e830c9e0dcea2d43d2e286b1d9904a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 23 Jun 2017 22:07:08 -0700 Subject: [PATCH 154/216] Increment version number to v2.2.1. --- configure.ac | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/configure.ac b/configure.ac index 85656a7da0..4e60506ffd 100644 --- a/configure.ac +++ b/configure.ac @@ -17,7 +17,7 @@ # Process this file with autoconf to produce a configure script. AC_PREREQ(2.59) -AC_INIT([PyLith], [2.2.0], [cig-short@geodynamics.org]) +AC_INIT([PyLith], [2.2.1], [cig-short@geodynamics.org]) AC_CONFIG_AUX_DIR([./aux-config]) AC_CONFIG_HEADER([portinfo]) AC_CONFIG_MACRO_DIR([m4]) From c82dda801ef3fd294420d1da40c6459ce6aee8dd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 24 Jun 2017 09:55:25 -0700 Subject: [PATCH 155/216] Added step05 to examples/subduction2d. --- doc/userguide/examples/subduction2d.tex | 143 +++++++++++++++++++++++- 1 file changed, 137 insertions(+), 6 deletions(-) diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index 976fefcd86..3a8f8d6896 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -5,28 +5,29 @@ \section{Example for Slip on a 2D Subduction Zone} \begin{itemize} \item Static solution \item Quasi-static solution -\item CUBIT mesh generation +\item CUBIT/Trelis mesh generation w/APREPRO \item Nonplanar geometry \item Variable mesh resolution -\item APREPRO programming language \item Linear triangular cells \item HDF5 output \item Dirichlet displacement and velocity boundary conditions \item ZeroDispDB spatial database -\item SimpleDB spatial database \item UniformDB spatial database +\item SimpleDB spatial database +\item SimpleGridDB \item Multiple materials \item Nonlinear solver \item Plane strain linearly elastic material -\item Plane Maxwell linear viscoelastic material +\item Plane strain linear Maxwell viscoelastic material \item Prescribed slip \item Spontaneous rupture -\item Static fault rupture \item Multiple faults \item Spatially variable coseismic slip \item Spatially variable aseismic creep \item Afterslip via fault friction \item Static friction +\item Slip-weakening friction +\item Rate-state friction \end{itemize} All of the files necessary to run the examples are contained in the directory \filename{examples/2d/subduction}. @@ -361,7 +362,137 @@ \subsection{Step 4: Frictional Afterslip Simulation} \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} -\todo{brad}{ADD STUFF HERE} +We simulate earthquake cycles over 100 years with spontaneous rupture +using slip-weakening friction. As in Step 4 including fault friction +requires the nonlinear solver. Through trial and error we choose a +time step of 2.5 years that permits reasonable convergence of the +nonlinear solver and runtime. +\begin{cfg} +[pylithapp.problem.formulation] +# Fault friction is a nonlinear problem so we need to use the +# nonlinear solver. +solver = pylith.problems.SolverNonlinear + +[pylithapp.timedependent.formulation.time_step] +

      total_time

      = 100.0*year +

      dt

      = 2.5*year +\end{cfg} +In simulations for research purposes, we +would use a higher resolution mesh and smaller time steps and +investigate the robustness of the solution to these parameters. + +% Boundary conditions +We constrain the displacement normal to the lateral and bottom +boundaries without restraining the subducting slab. We also constrain +the vertical deformation of the west boundary to facilitate the +downward motion of the subducting slab. +\begin{cfg} +[pylithapp.timedependent.bc.boundary_west] +

      bc_dof

      = [0, 1] +

      label

      = bndry_west +

      db_initial.label

      = Dirichlet BC on west boundary +\end{cfg} + +% Faults +We replace the prescribed aseismic slip +on the subduction interface that we used in Step 2 with a friction interface with the +slip-weakening fault constitutive model. +\begin{cfg} +[pylithapp.timedependent] +interfaces = [fault_slabtop, fault_slabbot] + +# Set the type of fault interface conditions. +[pylithapp.timedependent.interfaces] +fault_slabtop = pylith.faults.FaultCohesiveDyn +fault_slabbot = pylith.faults.FaultCohesiveKin +\end{cfg} + + % Fault - slab top +In order to generate stick-slip events, we need the coefficient of +friction to decrease with slip. We choose a slip-weakening friction +model with a dynamic coefficient of friction that is less than the +static coefficient of friction to provide this behavior. In +quasistatic modeling we use time steps much longer than the slip rise +time in an earthquake, so we want the slip confined to one time step +or just a few time steps. This means the drop in the coefficient of +friction should be independent in each time step; that is, we want the +fault to fully heal between time steps. This corresponds to setting +the \property{force\_healing} property of the \object{SlipWeakening} +object. + +A common feature in numerical modeling of subduction zones is stable +sliding near the trench and below the seismogenic zone. We implement +stable sliding with the slip-weakening friction via a constant +coefficient of friction (equal values for the static and dynamic +coefficients of friction). We create a lower dynamic coefficient of +friction in the seismogenic zone, by introducing depth-dependent +variations in the dynamic coefficient of friction. using a +\object{SimpleGridDB} spatial database. As discussed in Section +\vref{sec:spatial:databases} This provides more efficient +interpolation compared to the \object[SimpleDB} implementation. +We impose initial tractions on the fault in a similar fashion as we +did in Step 4. We reduce the initial shear tractions slightly in the +seismogenic zone, consistent with a stress drop in the penultimate +earthquake followed by loading during the interseimic period. +\begin{cfg} +[pylithapp.timedependent.interfaces.fault_slabtop] +# --- Skipping general information discussed previously --- +# Friction +friction = pylith.friction.SlipWeakening +friction.label = Slip weakening +# Force healing after each time step, so weakening is confined to each +# time step and is not carried over into subsequent time steps. +friction.force_healing = True + +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +friction.db_properties.label = Slip weakening +friction.db_properties.filename = fault_slabtop_slipweakening.spatialdb + +# Initial fault tractions +traction_perturbation = pylith.faults.TractPerturbation +traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB +traction_perturbation.db_initial.label = Initial fault tractions +traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb +\end{cfg} + +% Solver +We adjust several of the solver tolerances. In general, we impose +larger tolerances to reduce runtime at the expense of a less accurate +solution. We set the zero tolerances for detecting slip and +suppressing fault opening to $1.0 \times 10^{-8}$. We want tolerances +for the linear solve to be smaller than these values, so we use an +absolute tolerance of $1.0 \times 10^{-9}$ and a very small relative +tolerance to force the residual below the absolute tolerance. We +impose an absolute tolerance for the nonlinear solver to be geater +than our zero tolerances and also force the residual to match the +absolute tolerance level by using a very small relative +tolerances. Finally, we set the parameters for the solver used to +calculate consistent values for the change in slip for a given change +in the Lagrange multipliers (which we sometimes call the friction +sensitivity solve). +\begin{cfg} +[pylithapp.timedependent.interfaces.fault_slabtop] +

      zero_tolerance

      = 1.0e-8 +

      zero_tolerance_normal

      = 1.0e-8 + +# Convergence parameters. +

      ksp_rtol

      = 1.0e-20 +

      ksp_atol

      = 1.0e-9 +

      ksp_max_it

      = 1000 + +

      snes_rtol

      = 1.0e-20 +

      snes_atol

      = 1.0e-7 +

      snes_max_it

      = 1000 + +# Friction sensitivity solve used to compute the increment in slip +# associated with changes in the Lagrange multiplier imposed by the +# fault constitutive model. +

      friction_pc_type

      = asm +

      friction_sub_pc_factor_shift_type

      = nonzero +

      friction_ksp_max_it

      = 25 +

      friction_ksp_gmres_restart

      = 30 +

      friction_ksp_error_if_not_converged

      = true +\end{cfg} \subsection{Step 5: Spontaneous Earthquakes With Rate-State Friction} From aaee4a31f2ae50b4171affdeee961591999b9a3d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 24 Jun 2017 22:02:25 -0600 Subject: [PATCH 156/216] Added step05 and step06 in manual for 2-D subduction example. --- .../figs/subduction2d_step05_slip.pdf | Bin 0 -> 23998 bytes .../figs/subduction2d_step05_soln.jpg | Bin 0 -> 164323 bytes .../figs/subduction2d_step06_slip.pdf | Bin 0 -> 117600 bytes .../figs/subduction2d_step06_soln.jpg | Bin 0 -> 161653 bytes doc/userguide/examples/subduction2d.tex | 173 ++++++++++++++++-- 5 files changed, 153 insertions(+), 20 deletions(-) create mode 100644 doc/userguide/examples/figs/subduction2d_step05_slip.pdf create mode 100644 doc/userguide/examples/figs/subduction2d_step05_soln.jpg create mode 100644 doc/userguide/examples/figs/subduction2d_step06_slip.pdf create mode 100644 doc/userguide/examples/figs/subduction2d_step06_soln.jpg diff --git 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z#Py1V=us(=GK05g7bwvjBw;?wp>5+o!w) z%P6x-b?Y?PJ!BPXdNm@3xD*v=2ln2JhcgfDKAEpM12@s9tB#vAd)Fa!ZJ8EH+C~<&X5oS6qQN}6X$$DGZxPxoRxctOdBlUa-+_Xic^ayw zVOAXhsarTxpAI&JMf-hRFM4;0r7vtyJgBBb2r$!H$`M2Wr#S|X2?i-C*lOa!$y5H+ zf7K0ydBU;Df3|aYlT&{{x{mMV;)yw=YcQicz0Jk*5?McY?nQB3W zIHFu`1-THU{{XdGhGBMxgi^>u4+5KDFvNbp z-w{@G{fJ~nHpr?XB!mWlHjxeP*2}994`Yl+BvSQA-2=0PauzEg08~7BTyW`)V>KUCC775fpQFFtm_e{>=C<{l(7z z0LsJU{NsD(y#D~UYWI=ExFG=00c|L0301D^q`UtBxX+pTjD2ixU+zEe%;}rYjD5Uy zCt36T6;$N^0E~SEDzjLcCHR2~CvX}x&AzxgMjL5EnTt;Kj#Y;IIj*P5iWri1SrQGB zvL7gqDdY$#r^opWI_pcSI^zW?gs(wE0?gt>T&WFw3Xd!Q0CxWX84N[pylithapp.timedependent.interfaces.fault_slabtop] # --- Skipping general information discussed previously --- # Friction -friction = pylith.friction.SlipWeakening -friction.label = Slip weakening +friction = pylith.friction.SlipWeakening +

      friction.label

      = Slip weakening # Force healing after each time step, so weakening is confined to each # time step and is not carried over into subsequent time steps. -friction.force_healing = True +

      friction.force_healing

      = True -friction.db_properties = spatialdata.spatialdb.SimpleGridDB -friction.db_properties.label = Slip weakening -friction.db_properties.filename = fault_slabtop_slipweakening.spatialdb +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +

      friction.db_properties.label

      = Slip weakening +

      friction.db_properties.filename

      = fault_slabtop_slipweakening.spatialdb # Initial fault tractions -traction_perturbation = pylith.faults.TractPerturbation -traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB -traction_perturbation.db_initial.label = Initial fault tractions -traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb +traction_perturbation = pylith.faults.TractPerturbation +traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB +

      traction_perturbation.db_initial.label

      = Initial fault tractions +

      traction_perturbation.db_initial.filename

      = fault_slabtop_tractions.spatialdb \end{cfg} % Solver @@ -494,15 +495,141 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction}

      friction_ksp_error_if_not_converged

      = true \end{cfg} -\subsection{Step 5: Spontaneous Earthquakes With Rate-State Friction} +We run this example by typing +\begin{shell} +$$ pylith step05.cfg +\end{shell} +The problem will produce fourteen pairs of HDF5/Xdmf files. Figure +\vref{fig:example:subduction:2d:step05}, which was created using the +ParaView Python script \filename{viz/plot\_dispwarp.py} (see +Section~\ref{sec:example:subduction:3d:step01} for a discussion of how + to run ParaView Python scripts), displays the +magnitude of the velocity field with the original configuration +exaggerated by a factor of 4000. Steady slip is largely confined to +the stable sliding regions with a sequence of ruptures in the +seismogenic zone; most have a duration of a few time steps, although +most of the slip occurs in a single time +step. Figure~\ref{fig:example:subduction:2d:step05:slip} shows the +cumulative slip as a function of time and distance down dip from the +trench. + +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step05_soln} + \caption{Solution for Step 5 at the end of the simulation. The + colors indicate the magnitude of the x-displacement component and + the deformation has been exaggerated by a factor of 10,000. } + \label{fig:example:subduction:2d:step05} +\end{figure} + +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step05_slip} + \caption{Cumulative slip as a function of time and depth in Step + 5. The red lines indicate slip every 10 time steps.} + \label{fig:example:subduction:2d:step05:slip} +\end{figure} + + +\subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction} + +In this example we replace the slip-weakening in Step 5 with rate- and +state-friction using the ageing law. We also lengthen the duration of +the simulation to 200 years and reduce the time step to 1.0 years, +which were determined through trial and error to get a couple +earthquake cycles with reasonable convergence for this relatively +coarse resolution mesh. +\begin{cfg} +[pylithapp.timedependent.formulation.time_step] +

      total_time

      = 200.0*year +dt = 1.0*year +\end{cfg} + +The specification of the parameters for the rate- and state-friction +model follow a similar pattern to the ones for the slip-weakening +friction in Step 5. Our regulatization of the coefficient of friction +for near zero slip rate values involves a transition to a linear +dependence on slip rate; in this example we specify that this +transition should occur at a nondimensional slip rate of +$1.0 \times 10^{-6}$. We impose depth variation of the friction model +parameters via a \object{SimpleGridDB} spatial database in order to +generate earthquake-like ruptures in the seismogenic zone with stable +sliding above and below. For the initial tractions, we impose uniform +values using a \object{SimpleDB} spatial database. We set the initial +state for the friction model to be roughly consistent with steady +state sliding at the reference coefficient of friction at the +reference slip rate, and include it in the state variable in the +output as a check. +\begin{cfg} +[pylithapp.timedependent.interfaces.fault_slabtop] +# --- Skipping parameters discussed in previous examples. --- +# Friction +friction = pylith.friction.RateStateAgeing +

      friction.label

      = Rate-state friction +# Nondimensional slip rate below which friction depends linearly on slip rate. +

      friction.linear_slip_rate

      = 1.0e-6 + +# Set spatial database for distribution of friction parameters +friction.db_properties = spatialdata.spatialdb.SimpleGridDB +

      friction.db_properties.label

      = Slip weakening +

      friction.db_properties.filename

      = fault_slabtop_ratestate.spatialdb + +# Set spatial database for the initial value of the state variable. +friction.db_initial_state = spatialdata.spatialdb.UniformDB +

      friction.db_initial_state.label

      = Rate State Ageing State +

      friction.db_initial_state.values

      = [state-variable] +# theta_ss = characteristic_slip_dist / reference_slip_rate +

      friction.db_initial_state.data

      = [20.0*year] + +# Initial fault tractions +traction_perturbation = pylith.faults.TractPerturbation +traction_perturbation.db_initial = spatialdata.spatialdb.UniformDB +

      traction_perturbation.db_initial.label

      = Initial fault tractions +

      traction_perturbation.db_initial.values

      = [traction-shear, traction-normal] +

      traction_perturbation.db_initial.data

      = [-12.0*MPa, -20.0*MPa] + +[pylithapp.problem.interfaces.fault_slabtop.output] +writer = pylith.meshio.DataWriterHDF5 +

      writer.filename

      = output/step06-fault-slabtop.h5 +

      vertex_info_fields

      = [normal_dir, strike_dir] +

      vertex_data_fields

      = [slip, slip_rate, traction, state_variable] +\end{cfg} + +We run this example by typing +\begin{shell} +$$ pylith step06.cfg +\end{shell} +The problem will produce fourteen pairs of HDF5/Xdmf files. Figure +\vref{fig:example:subduction:2d:step06}, which was created using the +ParaView Python script \filename{viz/plot\_dispwarp.py}, displays the +magnitude of the velocity field with the original configuration +exaggerated by a factor of 4000. Steady slip is largely confined to +the stable sliding regions with a sequence of ruptures in the +seismogenic zone; note how the rate-state friction allows a more +natural nucleation of the ruptures compared to the slip-weakening +friction. Figure~\ref{fig:example:subduction:2d:step05:slip} shows the +cumulative slip as a function of time and distance down dip from the +trench. + +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step06_soln} + \caption{Solution for Step 6 at the end of the simulation. The + colors indicate the magnitude of the x-displacement component and + the deformation has been exaggerated by a factor of 10,000.} + \label{fig:example:subduction:2d:step06} +\end{figure} + +\begin{figure} + \includegraphics[width=4.5in]{examples/figs/subduction2d_step06_slip} + \caption{Cumulative slip as a function of time and depth in Step + 6. The red lines indicate slip every 10 time steps.} + \label{fig:example:subduction:2d:step06:slip} +\end{figure} -\todo{brad}{ADD STUFF HERE} -\subsection{Suggested Variations} +\subsection{Exercises} -The list below includes some suggested modifications to the problem -that will allow you to become more familiar with PyLith while examining -some interesting physics. +The list below includes some suggested modifications to these examples +that will allow you to become more familiar with PyLith while +examining some interesting physics. \begin{itemize} \item Change the resolution of the mesh by editing the \filename{mesh\_tri3.jou} journal file. Change the resolution and bias factor. @@ -519,8 +646,14 @@ \subsection{Suggested Variations} and change data-dim to 1. \item Modify the CUBIT journal files to use quad4 cells rather than tri3 cells. This requires using the pave mesh scheme. -\item Adjust the friction model parameters and examine the effects on - the deformation and the convergence of the nonlinear solve. +\item Modify Steps 5 and 6 to use a user-defined variable time + step. Experiment with longer time steps between earthquake ruptures + and smaller time steps around the time of the earthquake + ruptures. Can you develop a simple algorithm for choosing the time step? +\item Adjust the parameters of the friction models and examine the + effects on the deformation and the convergence of the nonlinear + solve. In which cases do you need to adjust the time step to retain + reasonable convergence? \end{itemize} From cd6dbafb22cdcc2b121a4506f9e691b9ea082f4c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 24 Jun 2017 22:02:57 -0600 Subject: [PATCH 157/216] Clean up of step07 for 3-D subduction example. --- doc/userguide/examples/subduction3d.tex | 240 +++++++++--------------- 1 file changed, 90 insertions(+), 150 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index e3a74305d0..2dea6b2e9f 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1291,57 +1291,31 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} -This example is essentially a three-dimensional analog of -\vref{sec:example:greensfns2d}, and is a more realistic example of how -PyLith can be used to perform geodetic inversions. We use the output -of example step06 to create synthetic data. Once we have done this we -generate Green's functions to represent the geodetic responses at a -set of synthetic cGPS stations. Finally, we use the synthetic data and -Green's functions to perform an inversion, using the same generalized -inverse approach described in \vref{sec:example:greensfns2d:inversion}. - -We first generate the synthetic data by using the script -\filename{make\_synthetic\_gpsdisp.py} in the top-level -directory. This script reads the parameters in -\filename{make\_synthetic\_gpsdisp.cfg} to generate synthetic data -from the selected time step with a specified amount of noise. The -point data output from example step06 is read, the specified time step -is selected, and the specified amount of noise is added to the -results. Run this script as: -\begin{shell} -$$ ./make_synthetic_gpsdisp.py -\end{shell} -This will create the following files: +This example a three-dimensional analog of +\vref{sec:example:greensfns2d} and is a more realistic example of how +PyLith can be used to perform geodetic inversions. We divide +generating Green's functions for slip impulses on the central rupture +patch of the subduction interface two sub-problems: \begin{description} -\item[\filename{cgps\_synthetic\_displacement.txt}] read by the - inversion script. -\item[\filename{cgps\_synthetic\_displacement.vtk}] for visualization. + \item[step07a] Left-lateral slip component. + \item[step07b] Reverse slip component. \end{description} - -After we create the synthetic data, we generate the Green's -functions. We divide the Green's function generation into two sub-problems: -\begin{itemize} - \item step07a: Generate Green's functions corresponding to - left-lateral slip on the subduction interface (slab top). - \item step07b: Generate Green's functions corresponding to - updip slip on the subduction interface (slab top). -\end{itemize} -Note that the Green's functions could all be generated at the same -time; however, for real problems it is generally preferable to -separate the problems to improve runtimes (e.g., both problems can be -run simultaneously). - -To generate the Green's functions we change the problem type from the -default \facility{timedependent} to \facility{greensfns}. We do this -on the command line. When we change the problem type to -\facility{greensfns}, PyLith automatically reads the file -\filename{greensfns.cfg}. This file contains non-default settings that -are common to both sub-problems. Note that since the problem type has -been changed from the default \facility{timedependent} to -\facility{greensfns}, the facility labels are changed. Also, since -\facility{problem} is a facility of \facility{pylithapp}, we no longer -need the \facility{pylithapp} prefix in this file. We first specify -the fault information: +Although PyLith can generate the two components in one simulation, we +often prefer to speed up the process by running simulations for each +of the components at the same time using multiple processes on a cluster. + +To generate the Green's functions we change the problem from the +default \object{TimeDependent} to \object{GreensFns}. We do this on +the command line (as illustrated below). PyLith automatically reads +the \filename{greensfns.cfg} parameter file. This file contains +settings that are common to both sub-problems. Note that the settings +in the \filename{greensfns.cfg} only apply to parameters associated +with the \object{GreensFns} and its sub-components. For the Green's +function problem, we must specify the fault interface and the id for +the fault. We specify the amplitude of the impulses via a +\object{UniformDB} spatial database, because we want impulses over the +entire fault patch. We also request the amplitude of the impulses to +be include in the fault info file. \begin{cfg} # Define the interfaces (slab) and provide a fault_id. [greensfns] @@ -1352,8 +1326,8 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} [greensfns.interfaces] slab = pylith.faults.FaultCohesiveImpulses -# Nodesets corresponding to the fault and its buried edge. [greensfns.interfaces.slab] +# Nodesets corresponding to the fault and its buried edges.

      label

      = fault_slabtop_patch

      edge

      = fault_slabtop_patch_edge @@ -1367,19 +1341,16 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions}

      db_impulse_amplitude.label

      = Amplitude of fault slip impulses

      db_impulse_amplitude.values

      = [slip]

      db_impulse_amplitude.data

      = [1.0] -\end{cfg} -In addition to defining the fault information, we also set some output -information common to both sub-problems, writing additional info fields -for fault output, and turning off material output. If we left material -output turned on, we would end up with extremely large state variable -output files: -\begin{cfg} -[greensfns.interfaces.slab.output] # Add impulse amplitude to fault info output. -

      vertex_info_fields

      = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 +

      output.vertex_info_fields

      = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +output.writer = pylith.meshio.DataWriterHDF5 +\end{cfg} +We do not make use of the state variable output for the impulse +responses, so we turn off the data fields for all of the +materials to eliminate these large data files. +\begin{cfg} # Turn off output of state variables for materials. [greensfns.materials.slab.output]

      cell_data_fields

      = [] @@ -1396,132 +1367,101 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} The \filename{step07a.cfg} and \filename{step07b.cfg} files are identical, except for the impulse type specification and file -names. Here are the fault parameters in \filename{step07a.cfg}: +names. \begin{cfg} [pylithapp.problem.interfaces.slab] +# If we wanted to generate impulses for both the left-lateral and +# reverse components in the same simulation, we would use: +# impulse_dof = [0,1] +# # Impulses for left-lateral slip. -# Note that it is possible to apply both left-lateral and updip slip -# (impulse_dof = [0,1]), but we separate the impulses into two problems.

      impulse_dof

      = [0] \end{cfg} -In the output settings, we turn off output for the domain, provide the -coordinate system for the fake cGPS stations, and provide filenames: +In the output settings, we turn off writing the solution field for the +domain: \begin{cfg} -# Add cggs_sites to solution output. -[pylithapp.problem.formulation] -output = [domain, subdomain, cgps_sites] -output.cgps_sites = pylith.meshio.OutputSolnPoints - -# Domain, subdomain, and cgs_sites [pylithapp.problem.formulation.output.domain]

      writer.filename

      = output/step07a-domain.h5 # Turn off data fields.

      vertex_data_fields

      = [] - -[pylithapp.problem.formulation.output.subdomain] -

      writer.filename

      = output/step07a-groundsurf.h5 -# Turn off data fields. -

      vertex_data_fields

      = [] - -[pylithapp.problem.formulation.output.cgps_sites] -writer = pylith.meshio.DataWriterHDF5 -

      writer.filename

      = output/step07a-cgps_sites.h5 - -# Set coordinate system associated with file with cGPS sites -

      reader.filename

      = cgps_sites.txt -coordsys = spatialdata.geocoords.CSGeo -

      coordsys.space_dim

      = 3 -

      coordsys.datum_horiz

      = WGS84 -

      coordsys.datum_vert

      = mean sea level - -# Fault -[pylithapp.problem.interfaces.slab.output] -

      writer.filename

      = output/step07a-fault-slab.h5 - -# Materials -[pylithapp.problem.materials.slab.output] -

      writer.filename

      = output/step07a-slab.h5 - -[pylithapp.problem.materials.wedge.output] -

      writer.filename

      = output/step07a-wedge.h5 - -[pylithapp.problem.materials.crust.output] -

      writer.filename

      = output/step07a-crust.h5 - -[pylithapp.problem.materials.mantle.output] -

      writer.filename

      = output/step07a-mantle.h5 \end{cfg} You can run the two sub-problems as follows: \begin{shell} -$$ pylith --problem=pylith.problems.GreensFns step07a.cfg -mat_elastic.cfg solver_fieldsplit.cfg -$$ pylith --problem=pylith.problems.GreensFns step07b.cfg -mat_elastic.cfg solver_fieldsplit.cfg +$$ pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg +$$ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} \tip{To save time, run the two sub-problems simultaneously in separate shells (terminals). For a problem this size, this should work fine - on a laptop. For larger problems, this approach can still be - useful. For example, each sub-problem could be run simultaneously on - several nodes of a cluster.} + on a laptop. For larger problems, we would run the simulations via + separate jobs on a cluster with each job running on multiple + processes.} + +% Post-process Step 6 output +Before we can run the inversion, we post-process the output from Step +6 to create synthetic data. We use the same generalized inverse +approach described in \vref{sec:example:greensfns2d:inversion}. The +Python script \filename{make\_synthetic\_gpsdisp.py} reads the +parameters in \filename{make\_synthetic\_gpsdisp.cfg} and generates +synthetic data from the selected time step with a specified amount of +noise. Run this script by typing: +\begin{shell} +$$ ./make_synthetic_gpsdisp.py +\end{shell} +This will create the following files: +\begin{description} +\item[\filename{cgps\_synthetic\_displacement.txt}] read by the + inversion script. +\item[\filename{cgps\_synthetic\_displacement.vtk}] for visualization. +\end{description} -After generating the synthetic data and Green's functions, we then -perform a simple inversion using the \filename{slip\_invert.py} script, +% Inversion +We perform a simple inversion using the \filename{slip\_invert.py} script, with parameters defined in \filename{slip\_invert.cfg}. This script performs a set of linear inversions, in a manner similar to the -inversion in \vref{sec:example:greensfns2d:inversion}. This script is -in the top-level \filename{subduction} directory. From there, run the -script as follows: +inversion in \vref{sec:example:greensfns2d:inversion}. \begin{shell} $$ ./slip_invert.py \end{shell} -This will create a number of files in the output directory. Note that -the HDF5 files have an associated \filename{.xmf} file to use with -ParaView: +This will create a number of files in the output directory. \begin{description} -\item[\filename{step07-inversion-slip.h5}] This file may - be used to visualize the predicted slip distributions for different - values of the penalty weight. -\item[\filename{step07-inversion-displacement.h5}] This file may be used to - visualize the predicted cGPS displacements for each solution. +\item[\filename{step07-inversion-slip.h5}] This HDF5/Xdmf pair of files + may be used to visualize the predicted slip distributions for + different values of the penalty weight. +\item[\filename{step07-inversion-displacement.h5}] This HDF5/Xdmf pair + of files may be used to visualize the predicted cGPS displacements + for each solution. \item[\filename{step07-inversion-summary.txt}] This file provides a summary of the inversion results for each value of the penalty weight. \end{description} -When performing an inversion such as this, one approach is to find the -corner of the 'L-curve' when plotting the log of the weighted data -residual vs. the log of the penalty residual. This is viewed as the -point of diminishing returns for reducing the penalty -weight. Further reductions provide little improvement to the -weighted data residual, while providing a solution with less -regularization. A Python script has been provided in the -\filename{viz} subdirectory to plot this curve, assuming that the user -has the numpy and matplotlib Python packages installed. From the -\filename{viz} subdirectory, run this script as: -\begin{shell} -$$ ./plot_inversion_misfit.py ---summary=../output/step07-inversion-summary.txt -\end{shell} -This will produce a curve similar to that shown in Figure -\vref{fig:example:subduction:3d:step07:curve} +One approach to finding the optimal penalty weight is to find the +corner of the 'L-curve' for the log of the weighted data residual +versus the log of the penalty residual. This is viewed as the point of +diminishing returns for reducing the penalty weight. Further +reductions provide little improvement to the weighted data residual, +while providing a solution with less regularization. Figure +\vref{fig:example:subduction:3d:step07:optimal} shows that this +procedure suggests an optimal penalty weight of 0.1 for our inversion. + \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step07_inverse_curve} - \caption{Plot of the 'L-curve' for inversion in example step07. The + \caption{Plot of the 'L-curve' for inversion in Step 7. The 'corner' of the L-curve would be about the third or fourth point from the right of the plot, representing a penalty weight of 0.5 or 1.0 in our example. } - \label{fig:example:subduction:3d:step07:curve} + \label{fig:example:subduction:3d:step07:optimal} \end{figure} -Once we have determined the optimal solution by analyzing the L-curve, -we can then visualize the results using ParaView. Figure -\vref{fig:example:subduction:3d:step07:invresults} shows the predicted -slip, the observed and predicted displacement vectors, and the slip -applied from example step06 for a penalty weight of 1.0. The data fit -is very good, and the predicted slip distribution is very close to the -applied slip, although the magnitude is slightly underestimated. +Figure \vref{fig:example:subduction:3d:step07:soln} shows the +predicted slip, the observed and predicted displacement vectors, and +the slip applied from example step06 for a penalty weight of 1.0. The +data fit is very good, and the predicted slip distribution is very +close to the applied slip, although the magnitude is slightly +underestimated. + \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step07_inverse_soln} \caption{ParaView image of the inversion solution for a penalty @@ -1529,7 +1469,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} displacements are shown with magenta arrows. Color contours represent the predicted slip distribution and orange line contours show the applied slip from the forward problem.} - \label{fig:example:subduction:3d:step07:invresults} + \label{fig:example:subduction:3d:step07:soln} \end{figure} \subsubsection{Exercises} From 8d95aef6a3f698600b00ffcaf36f394652e74104 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 24 Jun 2017 22:04:52 -0600 Subject: [PATCH 158/216] Improved plotting routines for step05 and step06. --- examples/2d/subduction/viz/plot_dispwarp.py | 19 ++-- .../2d/subduction/viz/plot_slipprofile.py | 90 +++++++++++++++++++ 2 files changed, 102 insertions(+), 7 deletions(-) create mode 100755 examples/2d/subduction/viz/plot_slipprofile.py diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py index 8182a6bd29..fb7f32787f 100755 --- a/examples/2d/subduction/viz/plot_dispwarp.py +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -30,13 +30,14 @@ # Scale used to exaggerate deformation. DISPLACEMENT_SCALE = 10.0e+3 -DISPLACEMENT_COMPONENT = "X" +FIELD = "displacement" +FIELD_COMPONENT = "X" # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, exaggeration, component, showFinalTimeStep=False): +def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -59,6 +60,7 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): domainDisplay = Show(dataDomain, view) domainDisplay.Representation = 'Wireframe' domainDisplay.AmbientColor = [0.5, 0.5, 0.5] + Hide(dataDomain, view) # Warp domain to show deformation warp = WarpByVector(Input=dataDomain) @@ -66,7 +68,7 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): warp.ScaleFactor = exaggeration warpDisplay = Show(warp, view) - ColorBy(warpDisplay, ('POINTS', 'displacement', component)) + ColorBy(warpDisplay, ('POINTS', field, component)) warpDisplay.RescaleTransferFunctionToDataRange(True) warpDisplay.SetScalarBarVisibility(view, True) warpDisplay.SetRepresentationType('Surface With Edges') @@ -103,14 +105,17 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): parser = argparse.ArgumentParser() parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) - parser.add_argument("--component", action="store", dest="component", default=DISPLACEMENT_COMPONENT) + parser.add_argument("--field", action="store", dest="field", default=FIELD) + parser.add_argument("--component", action="store", dest="component", default=FIELD_COMPONENT) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.exaggeration, args.component, showFinalTimeStep=True) + visualize(args.sim, args.exaggeration, args.field, args.component, showFinalTimeStep=True) view = GetRenderView() - view.ViewSize = [960, 540] + view.ViewSize = [1024, 540] + view.CameraPosition = [68527.89880980579, -152111.39463431376, 1405120.1034155919] + view.CameraFocalPoint = [68527.89880980579, -152111.39463431376, -1004573.5784798338] view.Update() if args.screenshot: @@ -121,7 +126,7 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): else: # Running inside the ParaView GUI - visualize(SIM_NAME, DISPLACEMENT_SCALE, DISPLACEMENT_COMPONENT) + visualize(SIM_NAME, DISPLACEMENT_SCALE, FIELD, FIELD_COMPONENT) # End of file diff --git a/examples/2d/subduction/viz/plot_slipprofile.py b/examples/2d/subduction/viz/plot_slipprofile.py new file mode 100755 index 0000000000..f76b429f35 --- /dev/null +++ b/examples/2d/subduction/viz/plot_slipprofile.py @@ -0,0 +1,90 @@ +#!/usr/bin/env python +""" +This script generates a plot showing slip or fault tractions. +""" + +# The code requires the numpy, h5py, and matplotlib packages. +import numpy +import h5py +import matplotlib +matplotlib.use('Agg') +import matplotlib.pyplot as pyplot + + +# ---------------------------------------------------------------------- +def calcDist(vertices): + """Compute down-dip distance from the trench. + """ + dist = numpy.zeros(vertices.shape[0]) + pt0 = vertices[:-1,:] + pt1 = vertices[1:,:] + dx = ((pt1[:,0]-pt0[:,0])**2 + (pt1[:,1]-pt0[:,1])**2)**0.5 + dist[1:] = numpy.cumsum(dx) + return dist + +# ---------------------------------------------------------------------- +def getData(sim): + """Read fault information from HDF5 file. + """ + filename = "output/%s-fault-slabtop.h5" % sim + h5 = h5py.File(filename, "r") + vertices = h5['geometry/vertices'][:] + slip = h5['vertex_fields/slip'][:,:,:] + tstamps = h5["time"][:] + h5.close() + + data = { + "time": tstamps, + "vertices": vertices, + "slip": slip + } + return data + +# ---------------------------------------------------------------------- +def plot(sim): + + # Get fault data for simulation. + data = getData(sim) + + # Create sort key corresponding to increasing depth. + indices = numpy.argsort(data["vertices"][:,1])[::-1] + + # Calculate down-dip distance from trench and get sorted data. + #dist = calcDist(data["vertices"][indices,:]) + dist = -data["vertices"][indices,1] + slip = data["slip"][:,indices,:] + + figure = pyplot.figure(figsize=(5.0, 3.0), facecolor='white', dpi=150) + figure.set_facecolor('white') + + axes = figure.add_axes([0.15, 0.15, 0.80, 0.82]) + + for i,t in enumerate(data["time"]): + color = "blue" + lw = 0.5 + if i % 10 == 0: + color = "red" + lw = 1.0 + axes.plot(-slip[i,:,0], dist/1.0e+3, '-', color=color, linewidth=lw) + axes.set_xlabel("Slip (m)") + #axes.set_ylabel("Down-dip Dist. (km)") + axes.set_ylabel("Depth (km)") + axes.invert_yaxis() + + + pyplot.show() + pyplot.savefig("subduction2d_%s_slip.pdf" % sim) + return + +# ====================================================================== +if __name__ == "__main__": + + import argparse + parser = argparse.ArgumentParser() + parser.add_argument("--sim", action="store", dest="sim", default="step05") + args = parser.parse_args() + + plot(args.sim) + + +# End of file From 1cd63e9bc1d7801fb439cf1b6c210be1cfe128b6 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 24 Jun 2017 22:06:17 -0600 Subject: [PATCH 159/216] Small fixes and comments for step05 and step06. --- examples/2d/subduction/step04.cfg | 4 +++- examples/2d/subduction/step05.cfg | 2 +- examples/2d/subduction/step06.cfg | 8 ++------ examples/2d/subduction/viz/plot_faultinfo.py | 0 4 files changed, 6 insertions(+), 8 deletions(-) mode change 100644 => 100755 examples/2d/subduction/viz/plot_faultinfo.py diff --git a/examples/2d/subduction/step04.cfg b/examples/2d/subduction/step04.cfg index 07b497cfb6..a873822579 100644 --- a/examples/2d/subduction/step04.cfg +++ b/examples/2d/subduction/step04.cfg @@ -117,8 +117,10 @@ quadrature.cell = pylith.feassemble.FIATSimplex quadrature.cell.dimension = 1 # Specify zero tolerance for detecting slip. Must be larger than the -# KSP absolute tolerance. +# KSP absolute tolerance. The second tolerance suppresses fault +# opening for values less than the tolerance value. zero_tolerance = 1.0e-9 +zero_tolerance_normal = 1.0e-9 # Friction model friction = pylith.friction.StaticFriction diff --git a/examples/2d/subduction/step05.cfg b/examples/2d/subduction/step05.cfg index 331de42d01..9ce8049e1c 100644 --- a/examples/2d/subduction/step05.cfg +++ b/examples/2d/subduction/step05.cfg @@ -79,7 +79,7 @@ db_initial.label = Dirichlet BC on east boundary (mantle) # West boundary [pylithapp.timedependent.bc.boundary_west] -bc_dof = [0,1] +bc_dof = [0, 1] label = bndry_west db_initial.label = Dirichlet BC on west boundary diff --git a/examples/2d/subduction/step06.cfg b/examples/2d/subduction/step06.cfg index b4b0623c84..c307130aeb 100644 --- a/examples/2d/subduction/step06.cfg +++ b/examples/2d/subduction/step06.cfg @@ -79,7 +79,7 @@ db_initial.label = Dirichlet BC on east boundary (mantle) # West boundary [pylithapp.timedependent.bc.boundary_west] -bc_dof = [0,1] +bc_dof = [0, 1] label = bndry_west db_initial.label = Dirichlet BC on west boundary @@ -114,7 +114,7 @@ quadrature.cell.dimension = 1 # Friction friction = pylith.friction.RateStateAgeing friction.label = Rate-state friction -# Nondimensional slip rate below which friction is linear +# Nondimensional slip rate below which friction depends linearly on slip rate. friction.linear_slip_rate = 1.0e-6 # Set spatial database for distribution of friction parameters @@ -131,10 +131,6 @@ friction.db_initial_state.data = [20.0*year] # Initial fault tractions traction_perturbation = pylith.faults.TractPerturbation -#traction_perturbation.db_initial = spatialdata.spatialdb.SimpleGridDB -#traction_perturbation.db_initial.label = Initial fault tractions -#traction_perturbation.db_initial.filename = fault_slabtop_tractions.spatialdb - traction_perturbation.db_initial = spatialdata.spatialdb.UniformDB traction_perturbation.db_initial.label = Initial fault tractions traction_perturbation.db_initial.values = [traction-shear, traction-normal] diff --git a/examples/2d/subduction/viz/plot_faultinfo.py b/examples/2d/subduction/viz/plot_faultinfo.py old mode 100644 new mode 100755 From 79ac58ee4f23fd9ecf1c827ac9948b41735d6a79 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Sun, 25 Jun 2017 16:29:31 +1200 Subject: [PATCH 160/216] Fixed a few typos in step07. --- doc/userguide/examples/subduction3d.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 2dea6b2e9f..c8ca8f5f8d 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1291,7 +1291,7 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} -This example a three-dimensional analog of +This example is a three-dimensional analog of \vref{sec:example:greensfns2d} and is a more realistic example of how PyLith can be used to perform geodetic inversions. We divide generating Green's functions for slip impulses on the central rupture @@ -1315,7 +1315,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} the fault. We specify the amplitude of the impulses via a \object{UniformDB} spatial database, because we want impulses over the entire fault patch. We also request the amplitude of the impulses to -be include in the fault info file. +be included in the fault info file. \begin{cfg} # Define the interfaces (slab) and provide a fault_id. [greensfns] @@ -1444,7 +1444,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} reductions provide little improvement to the weighted data residual, while providing a solution with less regularization. Figure \vref{fig:example:subduction:3d:step07:optimal} shows that this -procedure suggests an optimal penalty weight of 0.1 for our inversion. +procedure suggests an optimal penalty weight of 1.0 for our inversion. \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step07_inverse_curve} From 95fb99115a94531d1d40888c12410da5d3e1853b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:21:09 -0600 Subject: [PATCH 161/216] Spell check and cleanup of step08a. --- doc/userguide/examples/subduction3d.tex | 253 ++++++++++++------------ 1 file changed, 126 insertions(+), 127 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 2dea6b2e9f..6d54c339e6 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -7,7 +7,7 @@ \subsection{Overview} This suite of examples demonstrates use of a wide variety of features and the general workflow often used in research simulations. We base the model on the Cascadia subduction zone -(Figure~\vref{fig:example:subduction:3d:cascadia}). These examples will +(Figure~\ref{fig:example:subduction:3d:cascadia}). These examples will focus on modeling the deformation associated with the the subducting slab, including interseismic deformation with aseismic slip (creep) and viscoelastic relaxation, coseismic slip on the slab interface and @@ -31,7 +31,7 @@ \subsection{Overview} \label{fig:example:subduction:3d:cascadia} \end{figure} -Figure~\vref{fig:example:subduction:3d:concept} shows our conceptual +Figure~\ref{fig:example:subduction:3d:concept} shows our conceptual model with a slab, mantle, continental crust, and accretionary wedge. We cut off the slab at a depth of 100 km. We use a transverse geographic projection coordinate system with Portland, Oregon, as the @@ -45,7 +45,7 @@ \subsection{Overview} \includegraphics[width=4.5in]{examples/figs/subduction3d_conceptualmodel} \caption{Conceptual model based on the Cascadia Subduction Zone. The model includes the subduction slab (white), the mantle (green), - continental crust (blue), and an acrretionary wedge (red).} + continental crust (blue), and an accretionary wedge (red).} \label{fig:example:subduction:3d:concept} \end{figure} @@ -68,7 +68,7 @@ \subsection{Overview} % ---------------------------------------------------------------------- \subsection{Features Illustrated} -Table~\vref{tab:example:subduction:3d:features} lists the features +Table~\ref{tab:example:subduction:3d:features} lists the features discussed in each of these 3-D subduction zone examples. With the intent of illustrating features used in research simulations, we use HDF5 output and, we make extensive use the most efficient @@ -225,7 +225,7 @@ \subsubsection{Materials} discretization. This means we can specify this information in the \filename{pylithapp.cfg} file and avoid duplicating it in each simulation parameter file. To set up the materials, we first create an -aray of materials that defines the name for each material component. +array of materials that defines the name for each material component. For example, we create the array of four materials and then set the parameters for the slab: \begin{cfg} @@ -283,7 +283,7 @@ \subsubsection{Solver Parameters} [pylithapp.petsc]

      malloc_dump

      = ; Dump information about PETSc memory not deallocated. -# Use LU preconditioner (helful for learning and debugging, not production simulations) +# Use LU preconditioner (helpful for learning and debugging, not production simulations)

      pc_type

      = lu # Convergence parameters. @@ -304,7 +304,7 @@ \subsubsection{Solver Parameters}

      snes_max_it

      = 100 ; Maximum number of iterations in nonlinear solve

      snes_monitor

      = true ; Show nonlinear residual norm at each iteration

      snes_linesearch_monitor

      = true ; Show nonlinear solver line search information -#snes_view = true ; Show nolinear solver parameters (commented out) +#snes_view = true ; Show nonlinear solver parameters (commented out)

      snes_converged_reason

      = true ; Show reason nonlinear solve converged

      snes_error_if_not_converged

      = true ; Generate an error if nonlinear solve fails to converge @@ -327,7 +327,7 @@ \subsection{Step 1: Axial Compression} We start with a very simple example of axial compression in the east-west direction with purely elastic material properties, and no -faults (Figure~\vref{fig:example:subduction:3d:step01:diagram}). We +faults (Figure~\ref{fig:example:subduction:3d:step01:diagram}). We impose axial compression using Dirichlet boundary conditions on the east (+x) and west (-x) boundaries and confine the domain in the north-south direction via zero displacement Dirichlet boundary @@ -429,7 +429,7 @@ \subsection{Step 1: Axial Compression} (two pairs of files), and physical properties, stress, and strain within each material (eight pairs of files). -Figure \vref{fig:example:subduction:3d:step01}, which was created +Figure \ref{fig:example:subduction:3d:step01}, which was created using the ParaView Python script \filename{plot\_dispvec.py}, displays the magnitude of the displacement field arrows showing the direction and magnitude of the deformation. Material properties with a positive @@ -506,7 +506,7 @@ \subsubsection{Exercises} algebraic multigrid preconditioner. \begin{itemize} \item Using the PETSc log summary to compare the runtime and - memory use between the original LU preconditiner and the ML + memory use between the original LU preconditioner and the ML algebraic multigrid preconditioner. Hint: The algebraic multigrid preconditioner is faster. \item Run the simulation again with the algebraic multigrid @@ -568,7 +568,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} viscoelastic constitutive model using viscosity in addition to the Vp, Vs, and density used to describe purely linear, isotropic elastic models. Rather than create a database with all four of these -parameters, we leverage the \object{SimpldDB} spatial databases used +parameters, we leverage the \object{SimpleDB} spatial databases used by \filename{mat\_elastic.cfg} for the elastic properties and simply create a single new spatial database with the depth-dependent viscosity for the slab and mantle. We use the \object{CompositeDB} @@ -610,14 +610,14 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} # Viscoelastic properties

      values_B

      = [viscosity] db_B = spatialdata.spatialdb.SimpleGridDB -

      db_B.label

      = Linear Maxwell viscoelatic properties +

      db_B.label

      = Linear Maxwell viscoelastic properties

      db_B.filename

      = spatialdb/mat_viscosity.spatialdb

      db_B.query_type

      = linear \end{cfg} In the simulation specific parameter file \filename{step02.cfg}, we specify the parameters for the quasistatic time stepping, the -coesismic rupture, and the filenames for output. By default, PyLith +coseismic rupture, and the filenames for output. By default, PyLith will use implicit time stepping with uniform time steps, so we need only specify the duration and time step size. \begin{cfg} @@ -693,7 +693,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} $$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} -Figure \vref{fig:example:subduction:3d:step02}, which was created +Figure \ref{fig:example:subduction:3d:step02}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, displays the magnitude of the displacement field exaggerated by a factor of 10,000 at the final time step (200 yr). The shallow @@ -714,7 +714,7 @@ \subsubsection{Exercises} \item Change the slip from the subduction interface rupture patch to the splay fault rupture patch. Hint: Identify the nodesets for the splay fault patch. -\item Create simulataneous rupture on the subduction interface rupture +\item Create simultaneous rupture on the subduction interface rupture patch and the splay fault rupture patch. \item Prescribe coseismic slip on the central patch for splay fault and the subduction interface below the intersection with the splay fault. @@ -792,7 +792,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation}

      id

      = 100 ; Must be different from ids used for materials

      label

      = fault_slabbot ; Nodeset for the entire fault surface

      edge

      = fault_slabbot_edge ; Nodeset for the buried edges -# Give slight westward tilt to the up_dir to avoid ambigious +# Give slight westward tilt to the up_dir to avoid ambiguous # directions for the shear components on the horizontal portions of the # fault.

      up_dir

      = [-0.1,0,0.9] @@ -888,7 +888,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} $$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} -Figure \vref{fig:example:subduction:3d:step03}, which was created +Figure \ref{fig:example:subduction:3d:step03}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, shows the deformation exaggerated by a factor of 5,000 at the final time step of t=200*yr. Notice that there are some local edge effects @@ -924,7 +924,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} include an earthquake on the splay fault. This illustrates how to include multiple earthquake sources on a single fault. We use the same roller Dirichlet boundary conditions and combination of elastic and -viscoelatic materials as we did in Step 3. +viscoelastic materials as we did in Step 3. \begin{figure}[htbp] \includegraphics[scale=0.75]{examples/figs/subduction3d_step04_diagram} @@ -970,7 +970,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} want the earthquake to be imposed at specific times, so we set their origin time equal to the desire rupture time (100 years and 200 years) minus a value much smaller than the time step, so that roundoff errors -do not result in the ruptures occuring one time step later than +do not result in the ruptures occurring one time step later than intended. We use the same settings as we did in Step 3 for the creep earthquake source. For the coseismic slip, we use a \object{SimpleGridDB} to impose a depth-dependent slip distribution @@ -1065,7 +1065,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} $$ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} -Figure \vref{fig:example:subduction:3d:step04}, which was created +Figure \ref{fig:example:subduction:3d:step04}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, shows the deformation exaggerated by a factor of 5,000 at the final time step of t=300*yr. Compared to the solution in Step 3, we see the @@ -1255,7 +1255,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} \filename{step06-cgps\_sites.h5}, which contains the displacements at the fake cGPS sites. -Figure \vref{fig:example:subduction:3d:step06}, which was created +Figure \ref{fig:example:subduction:3d:step06}, which was created using ParaView, shows the surface vertical displacement along with horizontal displacement vectors at the cGPS sites, superimposed on contours of the applied slip at $t = 24 \mathrm{days}$. @@ -1297,8 +1297,8 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} generating Green's functions for slip impulses on the central rupture patch of the subduction interface two sub-problems: \begin{description} - \item[step07a] Left-lateral slip component. - \item[step07b] Reverse slip component. + \item[Step 7a] Left-lateral slip component. + \item[Step 7b] Reverse slip component. \end{description} Although PyLith can generate the two components in one simulation, we often prefer to speed up the process by running simulations for each @@ -1443,7 +1443,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} diminishing returns for reducing the penalty weight. Further reductions provide little improvement to the weighted data residual, while providing a solution with less regularization. Figure -\vref{fig:example:subduction:3d:step07:optimal} shows that this +\ref{fig:example:subduction:3d:step07:optimal} shows that this procedure suggests an optimal penalty weight of 0.1 for our inversion. \begin{figure} @@ -1455,7 +1455,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} \label{fig:example:subduction:3d:step07:optimal} \end{figure} -Figure \vref{fig:example:subduction:3d:step07:soln} shows the +Figure \ref{fig:example:subduction:3d:step07:soln} shows the predicted slip, the observed and predicted displacement vectors, and the slip applied from example step06 for a penalty weight of 1.0. The data fit is very good, and the predicted slip distribution is very @@ -1512,33 +1512,37 @@ \subsubsection{Exercises} % ---------------------------------------------------------------------- \subsection{Step 8: Stress Field Due to Gravitational Body Forces} -This example demonstrates the use of gravitational body forces in -PyLith simulations, as well as the use of initial stresses to balance -the body forces. We also demonstrate what happens when the initial -stresses are not in balance with the gravitational stresses, and show -how viscoelastic problems with gravitational stresses will in general -not reach a steady-state solution. We do not include faults in -this example. The example is divided into three sub-problems: -\begin{itemize} -\item Step08a: Gravitational body forces with 3-D density variations +This example demonstrates the use of gravitational body forces as well +as the use of initial stresses to balance the body forces. This +involves enabling gravity within our domain with Dirichlet roller +boundary conditions on the lateral and bottom boundaries; we do not +include faults in this example. We also demonstrate what happens when +the initial stresses are not in balance with the gravitational +stresses, and show how viscoelastic problems with gravitational +stresses will in general not reach a steady-state solution. The +example is divided into three sub-problems: +\begin{description} +\item[Step 8a] Gravitational body forces with 3-D density variations in elastic materials and initial stresses for a uniform density. -\item Step08b: Gravitational body forces with 3-D density variations - in elastic materials and initial stresses from Step08a (initial - stresses satisfy equilibrium, so there is no deformation). -\item Step08c: Gravitational body forces with 3-D density variations +\item[Step 8b] Gravitational body forces with 3-D density variations + in elastic materials and initial stresses from Step 8a (initial + stresses satisfy equilibrium, so there is almost no deformation). +\item[Step 8c] Gravitational body forces with 3-D density variations in elastic and viscoelastic materials and initial stresses from - Step08a plus finite strain formulation (does not reach a steady-state + Step 8a plus finite strain formulation (does not reach a steady-state solution). -\end{itemize} +\end{description} + +\subsubsection{Step 08a} -For the first sub-problem (step08a), we apply gravitational stresses -and attempt to balance these with analytically computed stresses -consistent with the density of the mantle. Since the actual densities -are not constant, the forces are out of balance and we end up with -significant deformation. We first apply gravity and set the simulation -time to zero (static problem): +For Step 8a we apply gravitational stresses and attempt to balance +these with analytically computed stresses consistent with the density +of the mantle. Since the actual density is not uniform, the stresses +are out of balance and we end up with some deformation. In +\filename{step08a.cfg} we turn on gravity and set the total time to +zero (there is no time dependence in this model). \begin{cfg} -[pylithapp.timedependent] +[pylithapp.problem] # Set gravity field (default is None). gravity_field = spatialdata.spatialdb.GravityField @@ -1546,11 +1550,14 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} # Define the total time for the simulation.

      total_time

      = 0.0*year \end{cfg} -Then, for each material, we use the same spatial database for the -initial stresses. We use linear interpolation and in the database the -initial stress is simply computed as $\rho_mgh$, where $\rho_m$ is -the density of the mantle material and $h$ is the depth below the -ground surface: + +Our initial stress field corresponds to +$\sigma_\mathit{xx} = \sigma_\mathit{yy} = \sigma_\mathit{zz} = +\rho_\mathit{mantle} gz$ for all four materials, where $\rho_\mathit{mantle}$ is the density +of the mantle, $g$ is the acceleration due to gravity, and $z$ is +elevation. With only two control points necessary to describe this linear +variation, we use the same \object{SimpleDB} spatial database for all +four materials. \begin{cfg} # We specify initial stresses for each material via a SimpleDB and linear interpolation. [pylithapp.problem.materials.slab] @@ -1578,63 +1585,62 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces}

      db_initial_stress.query_type

      = linear \end{cfg} -The output parameters are simply the output filenames, since all the -other parameters are the defaults in \filename{pylithapp.cfg}. We use -the algebraic multigrid solver, which is appropriate for problems with -no fault. We run the sub-problem by doing: +We run the sub-problem by typing: \begin{shell} $$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} When the problem has run, we see deformation that is consistent with -the mismatched densities. Figure -\vref{fig:example:subduction:3d:step08a} demonstrates the deformed -mesh visualized by running the following command from the -\filename{subduction} directory: -\begin{shell} -$$ ./viz/plot_dispwarp.py --sim=step08a --exaggeration=500.0 ---component=Z --screenshot=subduction3d_step08a_soln.png -\end{shell} +the mismatched densities. The slab subsides while the crust undergoes +uplift due to the differences in density relative to the mantle. Figure +\ref{fig:example:subduction:3d:step08a} shows the deformed mesh +visualized with the \filename{plot\_dispwarp.py} ParaView Python +script. + \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08a_soln} - \caption{Image generated by running the \filename{plot\_dispwarp.py} - script for sub-problem step08a. The crustal material to the + \caption{Solution for Step 8a. The deformation has been exaggerated + by a factor of 500 and the colors highlight the vertical + displacement component. The crustal material in the east is less dense than the assumed mantle material for initial - stresses, while the slab material to the west is more dense. The - result is uplift to the east and downward movement to the west.} + stresses, while the slab material in the west is more dense. The + result is uplift in the east and subsidence in the west.} \label{fig:example:subduction:3d:step08a} \end{figure} -Sub-problem step08b is similar to step08a, but rather than -analytically computing the initial stresses, we use the stresses -computed in sub-problem step08a. Since the initial stresses are now -computed using the correct densities, the stresses balance and we end -up with no elastic deformation. To generate the initial stress spatial -database, we read the state variables output files from sub-problem -step08a. The script \filename{generate\_initial\_stress.py}, located in -the \filename{spatialdb} directory, will read these files and generate -the necessary spatial database files. Note that this script is another -instance of using the Python interface to the spatialdata package. The -script allows arguments, but the default arguments are appropriate for -this example. Once you are in the \filename{spatialdb} directory, run -the script as follows: +\subsubsection{Step 8b} + +Step 8b is similar to Step 8a, but we use the stresses output from Step 8a as the +initial stress rather than analytically computing +initial stresses. Because the initial stresses are consistent with the +variations in density across the materials, the initial stresses will +satisfy equilibrium and there will be essentially no deformation; the +initial stresses do not perfectly balance because in Step 8a we +average the values over the quadrature points for the output. We use +the Python script \filename{generate\_initial\_stress.py}, located in the +\filename{spatialdb} directory, to +postprocess the output from Step 8a and generate the initial stress +spatial database. Note that this script uses the Python interface to +the spatialdata package to write the spatial database; this is much +easier than writing a script to format the data to conform to the +format of the spatial database. The spatial database will contain the +stresses at each cell of our unstructured mesh, so the points are not +on a logical grid, and we must use a \object{SimpleDB}. \begin{shell} +# From the examples/3d/subduction directory, change to the spatialdb subdirectory. +$$ cd spatialdb $$ ./generate_initial_stress.py \end{shell} This will create spatial databases containing initial stresses for each of the four materials. -Once we have generated the initial stresses, we can perform the -simulation. Other than filenames, the only difference between -\filename{.cfg} files \filename{step08a.cfg} and -\filename{step08b.cfg} is in the specification of the initial -stresses. There is a separate spatial database for each material, and -since there is an initial stress for each cell centroid, we retain the -default nearest neighbor interpolation method: +In the \filename{step08b.cfg} file we specify the \object{SimpleDB} +spatial database for each material (they are now material +specific). With points at each cell centroid, we use nearest +interpolation (default) rather than linear interpolation; this is a +small approximation but it is much faster than using linear +interpolation in this unstructured set of points. \begin{cfg} -# We specify initial stresses for each material via a SimpleDB. -# Since there is a point in the database corresponding to each cell -# center, we keep the default query_type of 'nearest'. [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB

      db_initial_stress.label

      = Initial stress in the slab @@ -1658,39 +1664,34 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces} \end{cfg} When we compare the resulting elastic displacements with those of -example step08a, we find that there is essentially no displacement, -as seen in Figure \vref{fig:example:subduction:3d:step08b}. This -figure was also generated with the \filename{plot\_dispwarp.py} -script, using the following command: -\begin{shell} -$$ ./viz/plot_dispwarp.py --sim=step08b --exaggeration=1000.0 ---component=Z --screenshot=subduction3d_step08b_soln.png -\end{shell} +Step 8a, we find that there is essentially no displacement, +as seen in Figure \ref{fig:example:subduction:3d:step08b}. + \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08b_soln} - \caption{Image generated by running the \filename{plot\_dispwarp.py} - script for sub-problem step08b. In this case the densities used to - compute the initial stresses are consistent with the actual - densities, and there is no elastic deformation.} + \caption{Solution for Step 8b. In this case the initial stresses + satisfy the governing equation, so there is no deformation.} \label{fig:example:subduction:3d:step08b} \end{figure} -The final sub-problem is step08c. This problem is very similar to -step08b, but we now use viscoelastic materials, and we use the finite -strain formulation (\object{ImplicitLgDeform}). With this formulation, -the deformed configuration is taken into account, whereas in the -default \object{Implicit} infinitesimal strain formulation, -deformation is not taken into account when computing stresses. The -finite strain formulation should generally be used for viscoelastic -problems with gravity where you need accurate estimates of the -vertical deformation. - -As we saw in step08b, it is possible to balance the stresses for an -elastic problem. Once we include viscoelasticity, however, this -becomes much more difficult. That is what we demonstrate in this -example. Although the stresses are in equilibrium for the elastic -solution, there are still deviatoric stresses remaining, which will -drive viscous flow. Thus, a steady-state solution is never achieved. +\subsubsection{Step 8c} + +In this example we use linear Maxwell viscoelastic models in place of +the elastic models for the slab and mantle. We also use the small +strain formulation (\object{ImplicitLgDeform}) so that the deformed +configuration is taken into account; Steps 8a and 8b use the default +\object{Implicit} infinitesimal strain formulation. The small strain +formulation should generally be used for viscoelastic problems with +gravity where you need accurate estimates of the vertical deformation. + +\warning{The shear stress variations in the initial stresses will + cause the viscoelastic materials to drive viscous flow, resulting in + time-dependent deformation. As long as the elastic materials impose + deviatoric stresses in the viscoelastic materials through continuity + of strain, the viscoelastic materials will continue to flow. {\bf As + a result, in this case and many other simulations with + viscoelastic materials and gravitational body forces, it is + difficult to find a steady state solution.}} The only difference between the parameters in \filename{step08b.cfg} and \filename{step08c.cfg} is in the formulation setting and the @@ -1710,18 +1711,16 @@ \subsection{Step 8: Stress Field Due to Gravitational Body Forces}

      dt

      = 10.0*year \end{cfg} We use the material settings in \filename{mat\_viscoelastic.cfg}. We -can run the simulation and visualize the vertical deformation for the -last time step by doing: +can run the simulation by typing: \begin{shell} $$ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg -$$ ./viz/plot_dispwarp.py --sim=step08c --exaggeration=300.0 ---component=Z --screenshot=subduction3d_step08c_soln.png \end{shell} The resulting deformation is shown in Figure -\vref{fig:example:subduction:3d:step08c}. As a result of viscous flow, -the vertical deformation is even larger than for sub-problem -step08a. If we were to run the simulation for a longer time period, -the amount of vertical deformation would continue to increase. +\ref{fig:example:subduction:3d:step08c}. As a result of viscous flow, +the vertical deformation is even larger than that for Step 8a. If we +were to run the simulation for a longer time period, the amount of +vertical deformation would continue to increase. + \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction3d_step08c_soln} \caption{Image generated by running the \filename{plot\_dispwarp.py} From 3606499a1d99a5c0073d867caf7bbefede164d61 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:21:17 -0600 Subject: [PATCH 162/216] Spell check. --- doc/userguide/examples/subduction2d.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index b268bfb417..4f483fd933 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -434,7 +434,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} We impose initial tractions on the fault in a similar fashion as we did in Step 4. We reduce the initial shear tractions slightly in the seismogenic zone, consistent with a stress drop in the penultimate -earthquake followed by loading during the interseimic period. +earthquake followed by loading during the interseismic period. \begin{cfg} [pylithapp.timedependent.interfaces.fault_slabtop] # --- Skipping general information discussed previously --- @@ -464,7 +464,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} for the linear solve to be smaller than these values, so we use an absolute tolerance of $1.0 \times 10^{-9}$ and a very small relative tolerance to force the residual below the absolute tolerance. We -impose an absolute tolerance for the nonlinear solver to be geater +impose an absolute tolerance for the nonlinear solver to be greater than our zero tolerances and also force the residual to match the absolute tolerance level by using a very small relative tolerances. Finally, we set the parameters for the solver used to @@ -545,7 +545,7 @@ \subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction} The specification of the parameters for the rate- and state-friction model follow a similar pattern to the ones for the slip-weakening -friction in Step 5. Our regulatization of the coefficient of friction +friction in Step 5. Our regularization of the coefficient of friction for near zero slip rate values involves a transition to a linear dependence on slip rate; in this example we specify that this transition should occur at a nondimensional slip rate of From 40c0ba4ca32ccf7122334564f80bdb8b41b37952 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:21:39 -0600 Subject: [PATCH 163/216] Change vref to ref to avoid loop. --- doc/userguide/examples/grav2d.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/doc/userguide/examples/grav2d.tex b/doc/userguide/examples/grav2d.tex index 7600349a24..5648376aae 100644 --- a/doc/userguide/examples/grav2d.tex +++ b/doc/userguide/examples/grav2d.tex @@ -56,7 +56,7 @@ \subsection{Problem Description} same techniques used in the 2D subduction zone example, except that this mesh is simpler. The main driver is in the journal file \filename{mesh.jou}. It calls the journal file \filename{geometry.jou} to construct the geometry. -The mesh shown in Figure \vref{fig:examples:gravity:2d:mesh} The journal +The mesh shown in Figure \ref{fig:examples:gravity:2d:mesh} The journal files are documented and describe the various steps outlined below. \begin{enumerate} \item Create the geometry defining the domain. From be4ac4c1e61d8123496255accaefb27c11bc2840 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:26:55 -0600 Subject: [PATCH 164/216] Cleanup README. --- examples/2d/subduction/README | 29 ----------------------------- 1 file changed, 29 deletions(-) diff --git a/examples/2d/subduction/README b/examples/2d/subduction/README index 780eca8598..4fd4cd7eeb 100644 --- a/examples/2d/subduction/README +++ b/examples/2d/subduction/README @@ -119,32 +119,3 @@ Step 6. Earthquake cycle with rate-state friction pylith step06.cfg >& step06.log & tail -f step06.log -Suggestions variations - - The list below includes some suggested modifications to the problem - that will allow you to become more familiar with PyLith while - examining some interesting physics. - - * Change the resolution of the mesh by editing the mesh_tri3.jou - journal file. Change the resolution and bias factor. - - * Add depth dependent viscosity to the mantle and crust. This - requires using the linear Maxwell plane strain bulk constitutive - model in the crust as well and creating spatial databases that - include viscosity for the crust. Specifying a depth dependent - variation in the parameters will require adding points, updating - num-locs accordingly, and changing data-dim to 1. - - * Modify the spatial database files for the material properties to - use depth-dependent elastic properties based on PREM (Dziewonski - and Anderson, 1981, 10.1016/0031-9201(81)90046-7). See - http://geophysics.ou.edu/solid_earth/prem.html for a simple table - of values. - - Add points, update num-locs accordingly, and change data-dim to be 1. - - * Modify the CUBIT/Trelis journal files to use quad4 cells rather - than tri3 cells. This requires using the pave mesh scheme. - - * Adjust the friction model parameters and examine the effects on - the deformation and the convergence of the nonlinear solve. From 3eac7320f5c70c45fe540d250e2d0dd8e8b07b90 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:29:31 -0600 Subject: [PATCH 165/216] Cleanup of settings. --- examples/3d/subduction/greensfns.cfg | 13 ++++++------- 1 file changed, 6 insertions(+), 7 deletions(-) diff --git a/examples/3d/subduction/greensfns.cfg b/examples/3d/subduction/greensfns.cfg index 2f58bbc3fd..fcff13dec0 100644 --- a/examples/3d/subduction/greensfns.cfg +++ b/examples/3d/subduction/greensfns.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey @@ -30,8 +30,8 @@ fault_id = 100 [greensfns.interfaces] slab = pylith.faults.FaultCohesiveImpulses -# Nodesets corresponding to the fault and its buried edge. [greensfns.interfaces.slab] +# Nodesets corresponding to the fault and its buried edges. label = fault_slabtop_patch edge = fault_slabtop_patch_edge @@ -46,14 +46,13 @@ db_impulse_amplitude.label = Amplitude of fault slip impulses db_impulse_amplitude.values = [slip] db_impulse_amplitude.data = [1.0] +# Add impulse amplitude to fault info output. +output.vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] +output.writer = pylith.meshio.DataWriterHDF5 + # ---------------------------------------------------------------------- # output # ---------------------------------------------------------------------- -[greensfns.interfaces.slab.output] -# Add impulse amplitude to fault info output. -vertex_info_fields = [normal_dir, strike_dir, dip_dir, impulse_amplitude] -writer = pylith.meshio.DataWriterHDF5 - # Turn off output of state variables for materials. [greensfns.materials.slab.output] cell_data_fields = [] From 37b2c0c6d7c203ca784e7338c23d1e8830836b5b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:29:47 -0600 Subject: [PATCH 166/216] Fix syntax highlighting. --- examples/3d/subduction/mat_elastic.cfg | 2 +- examples/3d/subduction/mat_viscoelastic.cfg | 2 +- 2 files changed, 2 insertions(+), 2 deletions(-) diff --git a/examples/3d/subduction/mat_elastic.cfg b/examples/3d/subduction/mat_elastic.cfg index 2e3c4623c1..dfd58230c6 100644 --- a/examples/3d/subduction/mat_elastic.cfg +++ b/examples/3d/subduction/mat_elastic.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/mat_viscoelastic.cfg b/examples/3d/subduction/mat_viscoelastic.cfg index 8b58619729..5ac5e9f95a 100644 --- a/examples/3d/subduction/mat_viscoelastic.cfg +++ b/examples/3d/subduction/mat_viscoelastic.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey From 4cd2c3c8d3b9eb6c964952a889235bf966be719f Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:30:14 -0600 Subject: [PATCH 167/216] Fix parameter heading. --- examples/3d/subduction/step08a.cfg | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/step08a.cfg b/examples/3d/subduction/step08a.cfg index 60afc8305e..b235ecb7e9 100644 --- a/examples/3d/subduction/step08a.cfg +++ b/examples/3d/subduction/step08a.cfg @@ -57,7 +57,7 @@ problem.progress_monitor.filename = output/step08a-progress.txt # ---------------------------------------------------------------------- # problem # ---------------------------------------------------------------------- -[pylithapp.timedependent] +[pylithapp.problem] # Set gravity field (default is None). gravity_field = spatialdata.spatialdb.GravityField From afc7b7b9fd07b7cecda9cb424472b2add778f558 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 09:47:45 -0600 Subject: [PATCH 168/216] Set version number to 2.2.1rc1 --- configure.ac | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/configure.ac b/configure.ac index 4e60506ffd..5dbfc71513 100644 --- a/configure.ac +++ b/configure.ac @@ -17,7 +17,7 @@ # Process this file with autoconf to produce a configure script. AC_PREREQ(2.59) -AC_INIT([PyLith], [2.2.1], [cig-short@geodynamics.org]) +AC_INIT([PyLith], [2.2.1rc1], [cig-short@geodynamics.org]) AC_CONFIG_AUX_DIR([./aux-config]) AC_CONFIG_HEADER([portinfo]) AC_CONFIG_MACRO_DIR([m4]) From ed682fd12756f7926cd62f7f2bc9a63de92035db Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 10:11:59 -0600 Subject: [PATCH 169/216] Added release notes and updated CHANGES. Set version to 2.2.1rc1 in manual. --- CHANGES | 16 ++++++++++ doc/releasenotes/Makefile.am | 5 +++- doc/releasenotes/announce_v2.2.1.txt | 44 ++++++++++++++++++++++++++++ doc/userguide/install/install.tex | 6 ++-- doc/userguide/userguide.tex | 4 +-- 5 files changed, 69 insertions(+), 6 deletions(-) create mode 100644 doc/releasenotes/announce_v2.2.1.txt diff --git a/CHANGES b/CHANGES index 52d3e427f5..a4584d4713 100644 --- a/CHANGES +++ b/CHANGES @@ -8,6 +8,22 @@ MIGRATING FROM VERSION 2.1 TO 2.2 No changes are needed to parameter or other input files. The default format for pylithinfo output is now JSON. +---------------------------------------------------------------------- +Version 2.2.1 +---------------------------------------------------------------------- + +* Added new examples. + + - examples/3d/subduction: New suite of examples for a 3-D + subduction zone. + + - examples/2d/subduction: Added spontaneous rupture examples for + slip-weakening and rate- and state-friction. + +* Fixed bug in generating Xdmf files for 2-D vector output. + +* Updated PETSc to v3.7.6. + ---------------------------------------------------------------------- Version 2.2.0 ---------------------------------------------------------------------- diff --git a/doc/releasenotes/Makefile.am b/doc/releasenotes/Makefile.am index 070e1074e9..b6bdd3fe0f 100644 --- a/doc/releasenotes/Makefile.am +++ b/doc/releasenotes/Makefile.am @@ -41,7 +41,10 @@ EXTRA_DIST = \ announce_v2.0.3.txt \ announce_v2.1.0.txt \ announce_v2.1.2.txt \ - announce_v2.1.3.txt + announce_v2.1.3.txt \ + announce_v2.1.4.txt \ + announce_v2.2.0.txt \ + announce_v2.2.1.txt # End of file diff --git a/doc/releasenotes/announce_v2.2.1.txt b/doc/releasenotes/announce_v2.2.1.txt new file mode 100644 index 0000000000..c2d5b03968 --- /dev/null +++ b/doc/releasenotes/announce_v2.2.1.txt @@ -0,0 +1,44 @@ +Greetings, + +I am pleased to announce the release of PyLith 2.2.1, a finite-element +code designed to solve dynamic elastic problems and quasi-static +viscoelastic problems in tectonic deformation. + +This release provides a few new examples and bugfixes. + +You can download the source code and binaries from + + http://geodynamics.org/cig/software/pylith + +Detailed installation instructions for the binary packages are in the +User Manual with detailed building instructions for a few platforms in +the INSTALL file bundled with the PyLith Installer utility. We also +offer a Docker image +(https://wiki.geodynamics.org/software:pylith:docker) for running +PyLith within a portable, virtual Linux environment. + +====================================================================== +MIGRATING FROM VERSION 2.1 TO 2.2 +====================================================================== + +No changes are needed to parameter or other input files. The default +format for pylithinfo output is now JSON. + +====================================================================== +RELEASE NOTES +====================================================================== + +* Added new examples. + + - examples/3d/subduction: New suite of examples for a 3-D + subduction zone. + + - examples/2d/subduction: Added spontaneous rupture examples for + slip-weakening and rate- and state-friction. + +* Fixed bug in generating Xdmf files for 2-D vector output. + +* Updated PETSc to v3.7.6. + +See CHANGES in the top-level source directory for a list of changes +for each prior release. diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index fe425aee45..2381090818 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -54,11 +54,11 @@ \subsection{Linux and Max OS X} \item Unpack the tarball. \begin{shell} # Linux 32-bit -$$ tar -xzf pylith-2.2.0-linux-i686.tgz +$$ tar -xzf pylith-2.2.1-linux-i686.tgz # Linux 64-bit -$$ tar -xzf pylith-2.2.0-linux-x86_64.tgz +$$ tar -xzf pylith-2.2.1-linux-x86_64.tgz # Mac OS X -$$ tar -xzf pylith-2.2.0-darwin-10.11.6.tgz +$$ tar -xzf pylith-2.2.1-darwin-10.11.6.tgz \end{shell} \item Set environment variables. The provided \filename{setup.sh} script only works if you are using bash shell. If you are using a diff --git a/doc/userguide/userguide.tex b/doc/userguide/userguide.tex index 9ca04bf210..88908349c3 100644 --- a/doc/userguide/userguide.tex +++ b/doc/userguide/userguide.tex @@ -29,8 +29,8 @@ \newcommand{\rlabel}[1]{\rotatebox[origin=l]{90}{#1}} -\renewcommand{\pylithVersionNumber}{2.2.1} -\renewcommand{\pylithDOI}{10.5281/zenodo.438705} +\renewcommand{\pylithVersionNumber}{2.2.1rc1} +\renewcommand{\pylithDOI}{10.5281/zenodo.XXXXXX} % Update install/install.tex (version number within verbatim environment) \title{PyLith User Manual} From 940776a4ebf9b7f4bba8bae0bd28ac5cbc1c6730 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 11:50:10 -0600 Subject: [PATCH 170/216] Create directory for parameter and progress output if necessary. --- pylith/problems/ProgressMonitor.py | 12 ++++++++++++ pylith/problems/ProgressMonitorStep.py | 1 + pylith/problems/ProgressMonitorTime.py | 1 + pylith/utils/DumpParameters.py | 15 +++++++++++++++ pylith/utils/DumpParametersAscii.py | 1 + pylith/utils/DumpParametersJson.py | 1 + 6 files changed, 31 insertions(+) diff --git a/pylith/problems/ProgressMonitor.py b/pylith/problems/ProgressMonitor.py index 9fdd2a5245..67d2cc3173 100644 --- a/pylith/problems/ProgressMonitor.py +++ b/pylith/problems/ProgressMonitor.py @@ -127,6 +127,18 @@ def _close(self): def _update(self, current, start, stop, now, finished, percentComplete): return + def _createPath(self, filename): + """Create path for filename if it doesn't exist. + """ + import os + relpath = os.path.dirname(filename) + + if len(relpath) > 0 and not os.path.exists(relpath): + # Only create directory on master + if self.isMaster: + os.makedirs(relpath) + return + # FACTORIES //////////////////////////////////////////////////////////// diff --git a/pylith/problems/ProgressMonitorStep.py b/pylith/problems/ProgressMonitorStep.py index b9713a6cf0..eacdb88cef 100644 --- a/pylith/problems/ProgressMonitorStep.py +++ b/pylith/problems/ProgressMonitorStep.py @@ -78,6 +78,7 @@ def _configure(self): def _open(self): + self._createPath(self.filename) self.fout = open(self.filename, "w") self.fout.write("Timestamp Step % complete Est. completion\n") self.fout.flush() diff --git a/pylith/problems/ProgressMonitorTime.py b/pylith/problems/ProgressMonitorTime.py index c7d0873072..ea7e8c787e 100644 --- a/pylith/problems/ProgressMonitorTime.py +++ b/pylith/problems/ProgressMonitorTime.py @@ -87,6 +87,7 @@ def _open(self): uparser = pyre.units.parser() self.tSimScale = uparser.parse(self.tUnits) + self._createPath(self.filename) self.fout = open(self.filename, "w") self.fout.write("Timestamp Simulation t % complete Est. completion\n") self.fout.flush() diff --git a/pylith/utils/DumpParameters.py b/pylith/utils/DumpParameters.py index b731961a91..c8c33bad5d 100644 --- a/pylith/utils/DumpParameters.py +++ b/pylith/utils/DumpParameters.py @@ -126,6 +126,21 @@ def _getPropertiesComponents(self, obj): } return (properties, facilities) + def _createPath(self, filename): + """Create path for filename if it doesn't exist. + """ + import os + relpath = os.path.dirname(filename) + + if len(relpath) > 0 and not os.path.exists(relpath): + # Only create directory on proc 0 + from pylith.mpi.Communicator import mpi_comm_world + comm = mpi_comm_world() + if 0 == comm.rank: + os.makedirs(relpath) + return + + # FACTORIES //////////////////////////////////////////////////////////// diff --git a/pylith/utils/DumpParametersAscii.py b/pylith/utils/DumpParametersAscii.py index d5572b1c67..23ee2e1da3 100644 --- a/pylith/utils/DumpParametersAscii.py +++ b/pylith/utils/DumpParametersAscii.py @@ -76,6 +76,7 @@ def write(self, app): self.collect(app) parameters = self.info["application"] + self._createPath(self.filename) with open(self.filename, "w") as fout: from .CollectVersionInfo import CollectVersionInfo import datetime diff --git a/pylith/utils/DumpParametersJson.py b/pylith/utils/DumpParametersJson.py index d38c5cca10..e04c9aca15 100644 --- a/pylith/utils/DumpParametersJson.py +++ b/pylith/utils/DumpParametersJson.py @@ -75,6 +75,7 @@ def write(self, app): if self.info is None: self.collect(app) + self._createPath(self.filename) with open(self.filename, "w") as fout: import json if self.style == "compact": From 967695309213033b8723a21175dc57456a04ce27 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 12:43:24 -0600 Subject: [PATCH 171/216] Fix script invocation (python -> nemesis). Small cleanup. --- .gitignore | 7 +++++++ examples/3d/subduction/make_synthetic_gpsdisp.py | 2 +- examples/3d/subduction/slip_invert.py | 8 +++----- examples/3d/subduction/spatialdb/generate_slowslip.py | 2 +- examples/3d/subduction/step06.cfg | 2 +- 5 files changed, 13 insertions(+), 8 deletions(-) diff --git a/.gitignore b/.gitignore index d454cb13e1..4444cbffae 100644 --- a/.gitignore +++ b/.gitignore @@ -30,6 +30,7 @@ tests_auto/*/*/*_disp.spatialdb tests_auto/*/*/output tests_auto/*/*/output examples/3d/hex8/output +examples/2d/subduction/output examples/3d/subduction/output examples/3d/subduction/mesh/geometry_surfs.jou examples/3d/subduction/mesh/*.exo @@ -37,3 +38,9 @@ examples/3d/subduction/mesh/*.sat examples/3d/subduction/spatialdb/fault_slabtop_slowslip.spatialdb examples/3d/subduction/spatialdb/fault_slabtop_slowslip.timedb examples/3d/subduction/spatialdb/mat_initial_stress_grav-*.spatialdb +doc/userguide/userguide.toc +doc/userguide/userguide.aux +doc/userguide/userguide.lof +doc/userguide/userguide.log +doc/userguide/userguide.lot +doc/userguide/userguide.out diff --git a/examples/3d/subduction/make_synthetic_gpsdisp.py b/examples/3d/subduction/make_synthetic_gpsdisp.py index 15e5002584..98a413309b 100755 --- a/examples/3d/subduction/make_synthetic_gpsdisp.py +++ b/examples/3d/subduction/make_synthetic_gpsdisp.py @@ -1,4 +1,4 @@ -#!/usr/bin/env python +#!/usr/bin/env nemesis # -*- Python -*- (syntax highlighting) # # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index b71dacce17..c5512c08b2 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -1,4 +1,4 @@ -#!/usr/bin/env python +#!/usr/bin/env nemesis # -*- Python -*- (syntax highlighting) # # ---------------------------------------------------------------------- @@ -17,8 +17,7 @@ # ---------------------------------------------------------------------- # # Simple inversion script that uses PyLith-generated Green's functions. -# NOTE: This script assumes that you have PETSc installed, and that you -# have PETSC_DIR set as an environmental variable. +# # This script is used as part of example step07. To perform the inversion you # must have already: # 1. Run example step06. @@ -166,8 +165,7 @@ def _configure(self): self.llComp = math.cos(self.rake.value) self.udComp = math.sin(self.rake.value) - petscDir = os.environ['PETSC_DIR'] - self.genXdmfCmd = petscDir + "/bin/petsc_gen_xdmf.py " + self.genXdmfCmd = "pylith_genxdmf" return diff --git a/examples/3d/subduction/spatialdb/generate_slowslip.py b/examples/3d/subduction/spatialdb/generate_slowslip.py index 98dd99c2be..4e98c519c7 100755 --- a/examples/3d/subduction/spatialdb/generate_slowslip.py +++ b/examples/3d/subduction/spatialdb/generate_slowslip.py @@ -1,4 +1,4 @@ -#!/usr/bin/env python +#!/usr/bin/env nemesis ## @file generate_slowslip.py diff --git a/examples/3d/subduction/step06.cfg b/examples/3d/subduction/step06.cfg index dee7931b2c..7e40c3d526 100644 --- a/examples/3d/subduction/step06.cfg +++ b/examples/3d/subduction/step06.cfg @@ -53,7 +53,7 @@ # the spatial database with the final slip distribution and the # temporal database with the slip time function. # -# cd spatialdb && generate_slowslip.py +# cd spatialdb && ./generate_slowslip.py # # TO RUN THE SIMULATION: # From 85eca3a0bb82e4b34bb887483f7173c23e3a3508 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 12:43:46 -0600 Subject: [PATCH 172/216] Add missing file. --- examples/3d/subduction/Makefile.am | 1 + 1 file changed, 1 insertion(+) diff --git a/examples/3d/subduction/Makefile.am b/examples/3d/subduction/Makefile.am index 875c14b4d4..d560d25953 100644 --- a/examples/3d/subduction/Makefile.am +++ b/examples/3d/subduction/Makefile.am @@ -35,6 +35,7 @@ dist_noinst_DATA = \ step08a.cfg \ step08b.cfg \ step08c.cfg \ + cgps_sites.txt \ make_synthetic_gpsdisp.cfg \ slip_invert.cfg \ make_synthetic_gpsdisp.py \ From 976a0c681d91d840152a6d8d307715d49667d16b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 13:26:50 -0600 Subject: [PATCH 173/216] Use PETSc's Xdmf generator (more general than PyLith's). --- examples/3d/subduction/slip_invert.py | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index c5512c08b2..b0c1fa5982 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -165,7 +165,7 @@ def _configure(self): self.llComp = math.cos(self.rake.value) self.udComp = math.sin(self.rake.value) - self.genXdmfCmd = "pylith_genxdmf" + self.genXdmfCmd = "petsc_gen_xdmf.py " return From b7de33bb979965fc82f6ed55f0f2f20ec583d602 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 13:27:03 -0600 Subject: [PATCH 174/216] Fix typo in instructions. --- examples/3d/subduction/step08b.cfg | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/step08b.cfg b/examples/3d/subduction/step08b.cfg index 06ed34ab65..193ab43a9e 100644 --- a/examples/3d/subduction/step08b.cfg +++ b/examples/3d/subduction/step08b.cfg @@ -46,7 +46,7 @@ # the spatial database with the initial stresses corresponding to the # output from Step08a. # -# cd spatialdb && generate_initial_stress.py +# cd spatialdb && ./generate_initial_stress.py # # TO RUN THE SIMULATION: # pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg From bc8aef3238f8d8b3575a7d824ab145a401f75c2d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sun, 25 Jun 2017 14:07:08 -0600 Subject: [PATCH 175/216] Use https for submodules. --- .gitmodules | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/.gitmodules b/.gitmodules index b26fef0f80..d7f865af53 100644 --- a/.gitmodules +++ b/.gitmodules @@ -1,9 +1,9 @@ [submodule "m4"] path = m4 - url = git://github.com/geodynamics/autoconf_cig.git + url = https://github.com/geodynamics/autoconf_cig.git [submodule "templates/materials/m4"] path = templates/materials/m4 - url = git://github.com/geodynamics/autoconf_cig.git + url = https://github.com/geodynamics/autoconf_cig.git [submodule "templates/friction/m4"] path = templates/friction/m4 - url = git://github.com/geodynamics/autoconf_cig.git + url = https://github.com/geodynamics/autoconf_cig.git From e6d5bd6b0acda41b8eff7ed0290308a8b45624bd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 27 Jun 2017 10:09:33 -0600 Subject: [PATCH 176/216] Fix syntax highlighting. --- examples/3d/subduction/pylithapp.cfg | 2 +- examples/3d/subduction/solver_algebraicmultigrid.cfg | 2 +- examples/3d/subduction/solver_fieldsplit.cfg | 2 +- 3 files changed, 3 insertions(+), 3 deletions(-) diff --git a/examples/3d/subduction/pylithapp.cfg b/examples/3d/subduction/pylithapp.cfg index d24176268d..a4e18703d3 100644 --- a/examples/3d/subduction/pylithapp.cfg +++ b/examples/3d/subduction/pylithapp.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/solver_algebraicmultigrid.cfg b/examples/3d/subduction/solver_algebraicmultigrid.cfg index 9257c1631c..d5fcdc0631 100644 --- a/examples/3d/subduction/solver_algebraicmultigrid.cfg +++ b/examples/3d/subduction/solver_algebraicmultigrid.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey diff --git a/examples/3d/subduction/solver_fieldsplit.cfg b/examples/3d/subduction/solver_fieldsplit.cfg index bf14ee0a2c..be8f76ce9d 100644 --- a/examples/3d/subduction/solver_fieldsplit.cfg +++ b/examples/3d/subduction/solver_fieldsplit.cfg @@ -1,4 +1,4 @@ -# -*- Python -*- (syntax highlighting) +# -*- Config -*- (syntax highlighting) # ---------------------------------------------------------------------- # # Brad T. Aagaard, U.S. Geological Survey From 0c6a6636f1cbfc94d86ec62f3d8e6bb3f40c5987 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 27 Jun 2017 10:10:13 -0600 Subject: [PATCH 177/216] Fix typos in spatial database comments. --- .../2d/subduction/fault_slabtop_ratestate.spatialdb | 11 ++++++----- .../subduction/fault_slabtop_slipweakening.spatialdb | 9 ++++----- .../2d/subduction/fault_slabtop_tractions.spatialdb | 5 ++--- 3 files changed, 12 insertions(+), 13 deletions(-) diff --git a/examples/2d/subduction/fault_slabtop_ratestate.spatialdb b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb index b8d912dc20..67e12b6b02 100644 --- a/examples/2d/subduction/fault_slabtop_ratestate.spatialdb +++ b/examples/2d/subduction/fault_slabtop_ratestate.spatialdb @@ -30,11 +30,12 @@ SimpleGridDB { // Columns are // (1) x coordinate (km) // (2) y coordinate (km) -// (3) z coordinate (km) -// (4) static-coefficient -// (5) dynamic-coefficient -// (6) slip-weakening-parameter (m) -// (7) cohesion (Pa) +// (3) reference-friction-coefficient +// (4) reference-slip-rate (cm/yr) +// (5) characteristic-slip-distance (m) +// (6) constitutive-parameter-a +// (7) constitutive-parameter-b +// (8) cohesion (Pa) 0.0 99.0 0.6 1.0 0.2 0.015 0.010 0.0 0.0 -5.0 0.6 1.0 0.2 0.015 0.010 0.0 0.0 -15.0 0.6 1.0 0.2 0.015 0.017 0.0 diff --git a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb index 17d964e204..84a85a4705 100644 --- a/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb +++ b/examples/2d/subduction/fault_slabtop_slipweakening.spatialdb @@ -30,11 +30,10 @@ SimpleGridDB { // Columns are // (1) x coordinate (km) // (2) y coordinate (km) -// (3) z coordinate (km) -// (4) static-coefficient -// (5) dynamic-coefficient -// (6) slip-weakening-parameter (cm) -// (7) cohesion (Pa) +// (3) static-coefficient +// (4) dynamic-coefficient +// (5) slip-weakening-parameter (m) +// (6) cohesion (Pa) 0.0 99.0 0.6 0.60 1.0e-8 0.0 0.0 -5.0 0.6 0.60 1.0e-8 0.0 0.0 -15.0 0.6 0.55 1.0e-8 0.0 diff --git a/examples/2d/subduction/fault_slabtop_tractions.spatialdb b/examples/2d/subduction/fault_slabtop_tractions.spatialdb index ced0b575c3..ab6dbc12a1 100644 --- a/examples/2d/subduction/fault_slabtop_tractions.spatialdb +++ b/examples/2d/subduction/fault_slabtop_tractions.spatialdb @@ -30,9 +30,8 @@ SimpleGridDB { // Columns are // (1) x coordinate (km) // (2) y coordinate (km) -// (3) z coordinate (km) -// (4) shear traction (MPa) -// (5) normal traction (MPa) +// (3) shear traction (MPa) +// (4) normal traction (MPa) 0.0 99.0 -11.9 -20.0 0.0 -5.0 -11.9 -20.0 0.0 -15.0 -11.0 -20.0 From eb928be2f5fd629a2c52d6ea8c35bd21b5bdfb24 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 27 Jun 2017 10:11:17 -0600 Subject: [PATCH 178/216] Small cleanup. --- examples/2d/subduction/pylithapp.cfg | 8 -------- examples/2d/subduction/step05.cfg | 4 ++-- 2 files changed, 2 insertions(+), 10 deletions(-) diff --git a/examples/2d/subduction/pylithapp.cfg b/examples/2d/subduction/pylithapp.cfg index 4536da9a2f..aabc4a8ef7 100644 --- a/examples/2d/subduction/pylithapp.cfg +++ b/examples/2d/subduction/pylithapp.cfg @@ -61,10 +61,6 @@ ocean_crust = pylith.materials.ElasticPlaneStrain continent_mantle = pylith.materials.MaxwellPlaneStrain ocean_mantle = pylith.materials.MaxwellPlaneStrain -#continent_crust = pylith.materials.MaxwellPlaneStrain ; TEMPORARY -#ocean_crust = pylith.materials.MaxwellPlaneStrain ; TEMPORARY - - # Continental crust ----------------------------- [pylithapp.timedependent.materials.continent_crust] label = Continental crust @@ -74,7 +70,6 @@ id = 1 db_properties.label = Continental crust properties db_properties.iohandler.filename = mat_concrust.spatialdb -#db_properties.iohandler.filename = mat_conmantle.spatialdb ; TEMPORARY # We are doing 2D quadrature for a triangle. quadrature.cell = pylith.feassemble.FIATSimplex @@ -105,7 +100,6 @@ id = 3 db_properties.label = Oceanic crust properties db_properties.iohandler.filename = mat_oceancrust.spatialdb -#db_properties.iohandler.filename = mat_oceanmantle.spatialdb ; TEMPORARY # We are doing 2D quadrature for a triangle. quadrature.cell = pylith.feassemble.FIATSimplex @@ -159,7 +153,6 @@ cell_filter = pylith.meshio.CellFilterAvg output_freq = time_step time_step = 9.99999*year writer = pylith.meshio.DataWriterHDF5 -#cell_data_fields = [stress,total_strain,viscous_strain] ; TEMPORARY [pylithapp.timedependent.materials.continent_mantle.output] cell_filter = pylith.meshio.CellFilterAvg @@ -173,7 +166,6 @@ cell_filter = pylith.meshio.CellFilterAvg output_freq = time_step time_step = 9.99999*year writer = pylith.meshio.DataWriterHDF5 -#cell_data_fields = [stress,total_strain,viscous_strain] ; TEMPORARY [pylithapp.timedependent.materials.ocean_mantle.output] cell_filter = pylith.meshio.CellFilterAvg diff --git a/examples/2d/subduction/step05.cfg b/examples/2d/subduction/step05.cfg index 9ce8049e1c..87cb62b0cd 100644 --- a/examples/2d/subduction/step05.cfg +++ b/examples/2d/subduction/step05.cfg @@ -63,7 +63,7 @@ dt = 2.5*year # 'boundary_east_mantle' # 'boundary_west' # 'boundary_bottom_mantle' -bc = [boundary_east_mantle,boundary_west,boundary_bottom_mantle] +bc = [boundary_east_mantle, boundary_west, boundary_bottom_mantle] # For all boundaries, we fix the displacement normal to the boundary # (roller boundary condition) by retaining the default ZeroDispDB, @@ -93,7 +93,7 @@ db_initial.label = Dirichlet BC on bottom boundary (mantle) # faults # ---------------------------------------------------------------------- [pylithapp.timedependent] -interfaces = [fault_slabtop,fault_slabbot] +interfaces = [fault_slabtop, fault_slabbot] # Set the type of fault interface condition. [pylithapp.timedependent.interfaces] From 0eb7d02967f9d2b10c0662768c9a0e52e94ec6f2 Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Tue, 27 Jun 2017 14:42:42 -0600 Subject: [PATCH 179/216] Added additional state variables output. --- examples/3d/subduction/step08c.cfg | 4 ++++ 1 file changed, 4 insertions(+) diff --git a/examples/3d/subduction/step08c.cfg b/examples/3d/subduction/step08c.cfg index 01df0e50fb..d70fc7123e 100644 --- a/examples/3d/subduction/step08c.cfg +++ b/examples/3d/subduction/step08c.cfg @@ -119,15 +119,19 @@ writer.filename = output/step08c-groundsurf.h5 # Material output ------------------------------------------------------ [pylithapp.problem.materials.slab.output] +cell_data_fields = [stress, cauchy_stress, total_strain, viscous_strain] writer.filename = output/step08c-slab.h5 [pylithapp.problem.materials.wedge.output] +cell_data_fields = [stress, cauchy_stress, total_strain] writer.filename = output/step08c-wedge.h5 [pylithapp.problem.materials.crust.output] +cell_data_fields = [stress, cauchy_stress, total_strain] writer.filename = output/step08c-crust.h5 [pylithapp.problem.materials.mantle.output] +cell_data_fields = [stress, cauchy_stress, total_strain, viscous_strain] writer.filename = output/step08c-mantle.h5 From 54298668c3f64116eed3cf7a275b5fac67cc468d Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 4 Jul 2017 17:31:55 -0700 Subject: [PATCH 180/216] Updated ParaView Python scripts to allow overriding defaults from within Python shell. --- examples/2d/subduction/viz/plot_dispwarp.py | 76 ++++++++++++------- examples/2d/subduction/viz/plot_shearratio.py | 52 ++++++++----- examples/3d/subduction/viz/plot_dispvec.py | 74 ++++++++++++------ examples/3d/subduction/viz/plot_dispwarp.py | 70 +++++++++++------ examples/3d/subduction/viz/plot_faultdir.py | 62 +++++++++------ examples/3d/subduction/viz/plot_faultslip.py | 60 ++++++++++----- examples/3d/subduction/viz/plot_matprops.py | 60 ++++++++++----- examples/3d/subduction/viz/plot_mesh.py | 41 +++++++--- 8 files changed, 328 insertions(+), 167 deletions(-) diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py index fb7f32787f..698989c067 100755 --- a/examples/2d/subduction/viz/plot_dispwarp.py +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -21,37 +21,42 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step05" - -# Scale used to exaggerate deformation. -DISPLACEMENT_SCALE = 10.0e+3 -FIELD = "displacement" -FIELD_COMPONENT = "X" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") + +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step05", + "WARP_SCALE": 10.0e+3, + "FIELD": "displacement", + "FIELD_COMPONENT": "X", + "TIMESTEP": 0, + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read data - filename = "output/%s.xmf" % sim + filename = os.path.join(parameters.output_dir, "%s.xmf" % parameters.sim) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataDomain = XDMFReader(FileNames=[filename]) - RenameSource("%s-domain" % sim, dataDomain) + RenameSource("%s-domain" % parameters.sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() - if showFinalTimeStep: + if parameters.timestep == -1: scene.GoToLast() view = GetActiveViewOrCreate('RenderView') @@ -65,10 +70,10 @@ def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): # Warp domain to show deformation warp = WarpByVector(Input=dataDomain) warp.Vectors = ['POINTS', 'displacement'] - warp.ScaleFactor = exaggeration + warp.ScaleFactor = parameters.warp_scale warpDisplay = Show(warp, view) - ColorBy(warpDisplay, ('POINTS', field, component)) + ColorBy(warpDisplay, ('POINTS', parameters.field, parameters.field_component)) warpDisplay.RescaleTransferFunctionToDataRange(True) warpDisplay.SetScalarBarVisibility(view, True) warpDisplay.SetRepresentationType('Surface With Edges') @@ -76,12 +81,12 @@ def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): warpDisplay.RescaleTransferFunctionToDataRange(False, False) # Customize colorbar - displacementLUT = GetColorTransferFunction('displacement') + displacementLUT = GetColorTransferFunction(parameters.field) colorbar = GetScalarBar(displacementLUT, view) - if component.lower() == "magnitude": + if parameters.field_component.lower() == "magnitude": colorbar.Title = "Displacement Mag. (m)" else: - colorbar.Title = "%s-displacement (m)" % component.lower() + colorbar.Title = "%s-displacement (m)" % parameters.field_component.lower() colorbar.ComponentTitle = "" # Annotate time @@ -96,21 +101,38 @@ def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): view.ResetCamera() view.Update() Render() + return + +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "WARP_SCALE", "FIELD", "FIELD_COMPONENT", "TIMESTEP") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) - parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) - parser.add_argument("--field", action="store", dest="field", default=FIELD) - parser.add_argument("--component", action="store", dest="component", default=FIELD_COMPONENT) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) + parser.add_argument("--warp_scale", action="store", type=float, dest="warp_scale", default=DEFAULTS["WARP_SCALE"]) + parser.add_argument("--field", action="store", dest="field", default=DEFAULTS["FIELD"]) + parser.add_argument("--component", action="store", dest="field_component", default=DEFAULTS["FIELD_COMPONENT"]) + parser.add_argument("--timestep", action="store", type=int, dest="timestep", default=-1) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.exaggeration, args.field, args.component, showFinalTimeStep=True) + visualize(args) view = GetRenderView() view.ViewSize = [1024, 540] @@ -124,9 +146,7 @@ def visualize(sim, exaggeration, field, component, showFinalTimeStep=False): Interact() else: - # Running inside the ParaView GUI - - visualize(SIM_NAME, DISPLACEMENT_SCALE, FIELD, FIELD_COMPONENT) + visualize(Parameters()) # End of file diff --git a/examples/2d/subduction/viz/plot_shearratio.py b/examples/2d/subduction/viz/plot_shearratio.py index c5f97442e0..3cf1069da9 100755 --- a/examples/2d/subduction/viz/plot_shearratio.py +++ b/examples/2d/subduction/viz/plot_shearratio.py @@ -23,34 +23,39 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step05" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") -# Names of faults (with spontaneous rupture) for output files. -FAULTS = ["fault-slabtop"] +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step05", + "FAULTS": ["fault-slabtop"], + "TIMESTEP": 0, + } # ---------------------------------------------------------------------- from paraview.simple import * import os import numpy -def visualize(sim, faults): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read fault data dataFaults = [] - for fault in faults: - filename = "output/%s-%s.xmf" % (sim, fault) + for fault in parameters.faults: + filename = os.path.join(parameters.output_dir, "%s-%s.xmf" % (parameters.sim, fault)) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) data = XDMFReader(FileNames=[filename]) - RenameSource("%s-%s" % (sim, fault), data) + RenameSource("%s-%s" % (parameters.sim, fault), data) dataFaults.append(data) groupFaults = GroupDatasets(Input=dataFaults) @@ -90,21 +95,34 @@ def visualize(sim, faults): view.Update() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "FAULTS") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) parser.add_argument("--faults", action="store", dest="faults") args = parser.parse_args() if args.faults: - faults = args.faults.split(",") + args.faults = args.faults.split(",") else: - faults = FAULTS - visualize(args.sim, faults) + args.faults = DEFAULT["FAULTS"] + visualize(args.sim) view = GetRenderView() view.ViewSize = [960, 540] @@ -115,7 +133,7 @@ def visualize(sim, faults): else: # Running inside the ParaView GUI - visualize(SIM_NAME, FAULTS) + visualize(Parameters()) # End of file diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 4e7333a060..593fbaeb04 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -24,42 +24,48 @@ # User-specified parameters # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step01" - -# Scale used for displacement vectors. -DISPLACEMENT_SCALE = 10.0e+3 - +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") + +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step02", + "VECTOR_SCALE": 10.0e+3, + "FIELD": "displacement", + "FIELD_COMPONENT": "Magnitude", + "TIMESTEP": 0, + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, dispScale, showFinalTimeStep=False): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read data - filename = "output/%s-domain.xmf" % sim + filename = os.path.join(parameters.output_dir, "%s-domain.xmf" % parameters.sim) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataDomain = XDMFReader(FileNames=[filename]) - RenameSource("%s-domain" % sim, dataDomain) + RenameSource("%s-domain" % parameters.sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() - if showFinalTimeStep: + if parameters.timestep == -1: scene.GoToLast() view = GetActiveViewOrCreate('RenderView') # Show undeformed domain, colored by magnitude of displacement vector. domainDisplay = Show(dataDomain, view) - ColorBy(domainDisplay, ("POINTS", "displacement", "Magnitude")) + ColorBy(domainDisplay, ("POINTS", parameters.field, parameters.field_component)) domainDisplay.RescaleTransferFunctionToDataRange(True) domainDisplay.SetScalarBarVisibility(view, True) domainDisplay.SetRepresentationType("Surface With Edges") @@ -67,15 +73,18 @@ def visualize(sim, dispScale, showFinalTimeStep=False): domainDisplay.RescaleTransferFunctionToDataRange(False, False) # Customize colorbar - displacementLUT = GetColorTransferFunction('displacement') + displacementLUT = GetColorTransferFunction(parameters.field) colorbar = GetScalarBar(displacementLUT, view) - colorbar.Title = "Displacement Mag. (m)" + if parameters.field_component.lower() == "magnitude": + colorbar.Title = "Displacement Mag. (m)" + else: + colorbar.Title = "%s-displacement (m)" % parameters.field_component.lower() colorbar.ComponentTitle = "" - # Add arrows to show displacement vectors. + # Add arrows to show vectors. glyph = Glyph(Input=dataDomain, GlyphType="Arrow") - glyph.Vectors = ["POINTS", "displacement"] - glyph.ScaleFactor = dispScale + glyph.Vectors = ["POINTS", parameters.field] + glyph.ScaleFactor = parameters.vector_scale glyph.ScaleMode = "vector" glyph.GlyphMode = "All Points" glyph.GlyphType.TipRadius = 0.2 @@ -97,18 +106,35 @@ def visualize(sim, dispScale, showFinalTimeStep=False): view.Update() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "VECTOR_SCALE", "FIELD", "FIELD_COMPONENT", "TIMESTEP") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) - parser.add_argument("--vector-scale", action="store", type=float, dest="scale", default=DISPLACEMENT_SCALE) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) + parser.add_argument("--vector-scale", action="store", type=float, dest="vector_scale", default=DEFAULTS["VECTOR_SCALE"]) + parser.add_argument("--field", action="store", dest="field", default=DEFAULTS["FIELD"]) + parser.add_argument("--component", action="store", dest="field_component", default=DEFAULTS["FIELD_COMPONENT"]) + parser.add_argument("--timestep", action="store", type=int, dest="timestep", default=-1) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.scale, showFinalTimeStep=True) + visualize(args) view = GetRenderView() view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] @@ -125,7 +151,7 @@ def visualize(sim, dispScale, showFinalTimeStep=False): else: # Running inside the ParaView GUI - visualize(SIM_NAME, DISPLACEMENT_SCALE) + visualize(Parameters()) diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index cdda2035c4..dbb3be31de 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -21,36 +21,42 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step03" - -# Scale used to exaggerate deformation. -DISPLACEMENT_SCALE = 10.0e+3 -DISPLACEMENT_COMPONENT = "X" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") + +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step02", + "WARP_SCALE": 10.0e+3, + "FIELD": "displacement", + "FIELD_COMPONENT": "Magnitude", + "TIMESTEP": 0, + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, exaggeration, component, showFinalTimeStep=False): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read data - filename = "output/%s-domain.xmf" % sim + filename = os.path.join(parameters.output_dir, "%s-domain.xmf" % parameters.sim) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataDomain = XDMFReader(FileNames=[filename]) - RenameSource("%s-domain" % sim, dataDomain) + RenameSource("%s-domain" % parameters.sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() - if showFinalTimeStep: + if parameters.timestep == -1: scene.GoToLast() view = GetActiveViewOrCreate('RenderView') @@ -63,10 +69,10 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): # Warp domain to show deformation warp = WarpByVector(Input=dataDomain) warp.Vectors = ['POINTS', 'displacement'] - warp.ScaleFactor = exaggeration + warp.ScaleFactor = parameters.warp_scale warpDisplay = Show(warp, view) - ColorBy(warpDisplay, ('POINTS', 'displacement', component)) + ColorBy(warpDisplay, ('POINTS', parameters.field, parameters.field_component)) warpDisplay.RescaleTransferFunctionToDataRange(True) warpDisplay.SetScalarBarVisibility(view, True) warpDisplay.SetRepresentationType('Surface With Edges') @@ -74,12 +80,12 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): warpDisplay.RescaleTransferFunctionToDataRange(False, False) # Customize colorbar - displacementLUT = GetColorTransferFunction('displacement') + displacementLUT = GetColorTransferFunction(parameters.field) colorbar = GetScalarBar(displacementLUT, view) - if component.lower() == "magnitude": + if parameters.field_component.lower() == "magnitude": colorbar.Title = "Displacement Mag. (m)" else: - colorbar.Title = "%s-displacement (m)" % component.lower() + colorbar.Title = "%s-displacement (m)" % parameters.field_component.lower() colorbar.ComponentTitle = "" # Annotate time @@ -95,19 +101,35 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): view.Update() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "WARP_SCALE", "FIELD", "FIELD_COMPONENT", "TIMESTEP") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) - parser.add_argument("--exaggeration", action="store", type=float, dest="exaggeration", default=DISPLACEMENT_SCALE) - parser.add_argument("--component", action="store", dest="component", default=DISPLACEMENT_COMPONENT) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) + parser.add_argument("--warp-scale", action="store", type=float, dest="warp_scale", default=DEFAULTS["WARP_SCALE"]) + parser.add_argument("--field", action="store", dest="field", default=DEFAULTS["FIELD"]) + parser.add_argument("--component", action="store", dest="field_component", default=DEFAULTS["FIELD_COMPONENT"]) + parser.add_argument("--timestep", action="store", dest="timestep", default=-1) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() - visualize(args.sim, args.exaggeration, args.component, showFinalTimeStep=True) + visualize(args) view = GetRenderView() view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] @@ -124,7 +146,7 @@ def visualize(sim, exaggeration, component, showFinalTimeStep=False): else: # Running inside the ParaView GUI - visualize(SIM_NAME, DISPLACEMENT_SCALE, DISPLACEMENT_COMPONENT) + visualize(Parameters()) # End of file diff --git a/examples/3d/subduction/viz/plot_faultdir.py b/examples/3d/subduction/viz/plot_faultdir.py index 83adff3263..396e14c516 100755 --- a/examples/3d/subduction/viz/plot_faultdir.py +++ b/examples/3d/subduction/viz/plot_faultdir.py @@ -23,31 +23,35 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step02" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") -# Names of faults for output files. -FAULTS = ["fault-slab"] -FIELD = "strike_dir" +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step02", + "FIELD": "normal_dir", + "FAULTS": ["fault-slab"], + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, faults, direction): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read domain data - filename = "output/%s-domain.xmf" % sim + filename = os.path.join(parameters.output_dir, "%s-domain.xmf" % parameters.sim) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataDomain = XDMFReader(FileNames=[filename]) - RenameSource("%s-domain" % sim, dataDomain) + RenameSource("%s-domain" % parameters.sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() @@ -60,12 +64,12 @@ def visualize(sim, faults, direction): # Read fault data dataFaults = [] - for fault in faults: - filename = "output/%s-%s_info.xmf" % (sim, fault) + for fault in parameters.faults: + filename = os.path.join(parameters.output_dir, "%s-%s_info.xmf" % (parameters.sim, fault)) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) data = XDMFReader(FileNames=[filename]) - RenameSource("%s-%s" % (sim, fault), data) + RenameSource("%s-%s" % (parameters.sim, fault), data) dataFaults.append(data) groupFaults = GroupDatasets(Input=dataFaults) @@ -77,7 +81,7 @@ def visualize(sim, faults, direction): # Add arrows to show displacement vectors. glyph = Glyph(Input=groupFaults, GlyphType="Arrow") - glyph.Vectors = ["POINTS", direction] + glyph.Vectors = ["POINTS", parameters.field] glyph.GlyphMode = "All Points" glyphDisplay = Show(glyph, view) @@ -87,28 +91,42 @@ def visualize(sim, faults, direction): view.Update() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "FIELD", "FAULTS") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) parser.add_argument("--faults", action="store", dest="faults") - parser.add_argument("--direction", action="store", dest="direction", default=FIELD) + parser.add_argument("--field", action="store", dest="field", default=DEFAULTS["FIELD"]) args = parser.parse_args() if args.faults: - faults = args.faults.split(",") + args.faults = args.faults.split(",") else: - faults = FAULTS - visualize(args.sim, faults, args.direction) + args.faults = DEFAULTS["FAULTS"] + visualize(args) Interact() else: # Running inside the ParaView GUI - visualize(SIM_NAME, FAULTS, FIELD) + visualize(Parameters()) # End of file diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py index 9fb7b9e2b9..bca229540a 100755 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -23,34 +23,39 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step02" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") -# Names of faults for output files. -FAULTS = ["fault-slab"] +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step02", + "FAULTS": ["fault-slab"], + "TIMESTEP": 0, + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, faults, showFinalTimeStep=False): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() # Read domain data - filename = "output/%s-domain.xmf" % sim + filename = os.path.join(parameters.output_dir, "%s-domain.xmf" % parameters.sim) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataDomain = XDMFReader(FileNames=[filename]) - RenameSource("%s-domain" % sim, dataDomain) + RenameSource("%s-domain" % parameters.sim, dataDomain) scene = GetAnimationScene() scene.UpdateAnimationUsingDataTimeSteps() - if showFinalTimeStep: + if parameters.timestep == -1: scene.GoToLast() view = GetActiveViewOrCreate('RenderView') @@ -61,12 +66,12 @@ def visualize(sim, faults, showFinalTimeStep=False): # Read fault data dataFaults = [] - for fault in faults: - filename = "output/%s-%s.xmf" % (sim, fault) + for fault in parameters.faults: + filename = os.path.join(parameters.output_dir, "%s-%s.xmf" % (parameters.sim, fault)) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) data = XDMFReader(FileNames=[filename]) - RenameSource("%s-%s" % (sim, fault), data) + RenameSource("%s-%s" % (parameters.sim, fault), data) dataFaults.append(data) groupFaults = GroupDatasets(Input=dataFaults) @@ -96,22 +101,37 @@ def visualize(sim, faults, showFinalTimeStep=False): view.Update() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "FAULTS", "TIMESTEP") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) parser.add_argument("--faults", action="store", dest="faults") + parser.add_argument("--timestep", action="store", dest="timestep", default=-1) parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() if args.faults: - faults = args.faults.split(",") + args.faults = args.faults.split(",") else: - faults = FAULTS - visualize(args.sim, faults, showFinalTimeStep=True) + args.faults = DEFAULTS["FAULTS"] + visualize(args) view = GetRenderView() view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] @@ -128,7 +148,7 @@ def visualize(sim, faults, showFinalTimeStep=False): else: # Running inside the ParaView GUI - visualize(SIM_NAME, FAULTS) + visualize(Parameters()) # End of file diff --git a/examples/3d/subduction/viz/plot_matprops.py b/examples/3d/subduction/viz/plot_matprops.py index 4a67580a39..4bd32abfb6 100755 --- a/examples/3d/subduction/viz/plot_matprops.py +++ b/examples/3d/subduction/viz/plot_matprops.py @@ -20,22 +20,26 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. - -# Root name for simulation. -SIM_NAME = "step01" +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") -# Material property and materials to plot. -INFO_FIELD = "mu" -MATERIALS = ["crust", "mantle", "wedge", "slab"] +DEFAULTS = { + "OUTPUT_DIR": "output", + "SIM": "step02", + "FIELD": "mu", + "MATERIALS": ["crust", "mantle", "wedge", "slab"], + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(sim, field, materials): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() @@ -43,12 +47,12 @@ def visualize(sim, field, materials): dataAll = [] # Read data - for material in materials: - filename = "output/%s-%s_info.xmf" % (sim, material) + for material in parameters.materials: + filename = os.path.join(parameters.output_dir, "%s-%s_info.xmf" % (parameters.sim, material)) if not os.path.isfile(filename): raise IOError("File '%s' does not exist." % filename) dataMaterial = XDMFReader(FileNames=[filename]) - RenameSource("%s-%s" % (sim, material), dataMaterial) + RenameSource("%s-%s" % (parameters.sim, material), dataMaterial) dataAll.append(dataMaterial) groupMaterials = GroupDatasets(Input=dataAll) @@ -56,13 +60,13 @@ def visualize(sim, field, materials): # Show domain, colored by magnitude of displacement vector. materialDisplay = Show(groupMaterials, view) - ColorBy(materialDisplay, ("CELLS", field)) + ColorBy(materialDisplay, ("CELLS", parameters.field)) materialDisplay.RescaleTransferFunctionToDataRange(True) materialDisplay.SetScalarBarVisibility(view, True) materialDisplay.SetRepresentationType("Surface With Edges") # Rescale color and/or opacity maps used to exactly fit the current data range - materialLUT = GetColorTransferFunction(INFO_FIELD) + materialLUT = GetColorTransferFunction(parameters.field) materialDisplay.RescaleTransferFunctionToDataRange(False, False) # Update scalar bar component title. UpdateScalarBarsComponentTitle(materialLUT, materialDisplay) @@ -70,29 +74,43 @@ def visualize(sim, field, materials): view.ResetCamera() Render() +class Parameters(object): + keys = ("OUTPUT_DIR", "SIM", "FIELD", "MATERIALS") + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--sim", action="store", dest="sim", default=SIM_NAME) - parser.add_argument("--field", action="store", dest="field", default=INFO_FIELD) + parser.add_argument("--output-dir", action="store", dest="output_dir", default=DEFAULTS["OUTPUT_DIR"]) + parser.add_argument("--sim", action="store", dest="sim", default=DEFAULTS["SIM"]) + parser.add_argument("--field", action="store", dest="field", default=DEFAULTS["FIELD"]) parser.add_argument("--materials", action="store", dest="materials") args = parser.parse_args() if args.materials: - materials = args.materials.split(",") + args.materials = args.materials.split(",") else: - materials = MATERIALS + args.materials = DEFAULTS["MATERIALS"] - visualize(args.sim, args.field, materials) + visualize(args) Interact() else: # Running inside the ParaView GUI - visualize(SIM_NAME, INFO_FIELD, MATERIALS) + visualize(Parameters()) # End of file diff --git a/examples/3d/subduction/viz/plot_mesh.py b/examples/3d/subduction/viz/plot_mesh.py index 7105e7debe..2c4cbae339 100755 --- a/examples/3d/subduction/viz/plot_mesh.py +++ b/examples/3d/subduction/viz/plot_mesh.py @@ -20,24 +20,30 @@ # User-specified parameters. # -# These are used if running from within the ParaView GUI via the -# Python shell or as defaults if running outside the ParaView GUI via -# pvpython. +# Default values for parameters. To use different values, overwrite +# them in the ParaView Python shell or on the command line. For +# example, set OUTPUT_DIR to the absolute path if not starting +# ParaView from the terminal shell where you ran PyLith: +# +# import os +# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") -EXODUS_FILE = "mesh/mesh_tet.exo" +DEFAULTS = { + "EXODUS_FILE": "mesh/mesh_tet.exo", + } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(filename): +def visualize(parameters): # Disable automatic camera reset on "Show" paraview.simple._DisableFirstRenderCameraReset() - if not os.path.isfile(filename): - raise IOError("Exodus file '%s' does not exist." % filename) - dataDomain = ExodusIIReader(FileName=[filename]) + if not os.path.isfile(parameters.exodus_file): + raise IOError("Exodus file '%s' does not exist." % parameters.exodus_file) + dataDomain = ExodusIIReader(FileName=[parameters.exodus_file]) RenameSource("domain", dataDomain) view = GetActiveViewOrCreate('RenderView') @@ -63,16 +69,29 @@ def visualize(filename): view.ResetCamera() Render() +class Parameters(object): + keys = ("EXODUS_FILE",) + + def __init__(self): + globalVars = globals() + for key in Parameters.keys: + if key in globalVars.keys(): + setattr(self, key.lower(), globalVars[key]) + else: + setattr(self, key.lower(), DEFAULTS[key]) + return + + # ---------------------------------------------------------------------- if __name__ == "__main__": # Running from outside the ParaView GUI via pvpython import argparse parser = argparse.ArgumentParser() - parser.add_argument("--filename", action="store", dest="filename", default=EXODUS_FILE) + parser.add_argument("--filename", action="store", dest="exodus_file", default=DEFAULTS["EXODUS_FILE"]) args = parser.parse_args() - visualize(args.filename) + visualize(args) view = GetRenderView() #view.CameraPosition = [-80160, -1130898, 133977] @@ -87,7 +106,7 @@ def visualize(filename): else: # Running inside the ParaView GUI - visualize(EXODUS_FILE) + visualize(Parameters()) # End of file From 1e2c01628b76ad77024c0fa8b41e8c41d3d1aa13 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 13 Jul 2017 10:55:55 -0700 Subject: [PATCH 181/216] Fixed boundary_ypos* and boundary_yneg* nodesets (were reversed). --- examples/3d/subduction/mesh/bc.jou | 72 +++++++++++++++--------------- 1 file changed, 36 insertions(+), 36 deletions(-) diff --git a/examples/3d/subduction/mesh/bc.jou b/examples/3d/subduction/mesh/bc.jou index b329b0df43..d422b2dd5b 100644 --- a/examples/3d/subduction/mesh/bc.jou +++ b/examples/3d/subduction/mesh/bc.jou @@ -150,52 +150,52 @@ group "boundary_xneg_noslab" remove node in group block_slab nodeset 83 group boundary_xneg_noslab nodeset 83 name "boundary_xneg_noslab" -# +y -group "boundary_ypos" add node in surface 18 -group "boundary_ypos" add node in surface 45 -group "boundary_ypos" add node in surface 48 -group "boundary_ypos" add node in surface 39 -nodeset 84 group boundary_ypos -nodeset 84 name "boundary_ypos" - -# +y w/o fault -group "boundary_ypos_nofault" add node in group boundary_ypos -group "boundary_ypos_nofault" remove node in group fault_slabtop -group "boundary_ypos_nofault" remove node in group fault_slabbot -group "boundary_ypos_nofault" remove node in group fault_splay -nodeset 85 group boundary_ypos_nofault -nodeset 85 name "boundary_ypos_nofault" - -# +y w/o slab -group "boundary_ypos_noslab" add node in group boundary_ypos -group "boundary_ypos_noslab" remove node in group block_slab -group "boundary_ypos_noslab" remove node in group fault_splay -nodeset 86 group boundary_ypos_noslab -nodeset 86 name "boundary_ypos_noslab" - - # -y -group "boundary_yneg" add node in surface 21 -group "boundary_yneg" add node in surface 43 -group "boundary_yneg" add node in surface 50 -group "boundary_yneg" add node in surface 36 -nodeset 87 group boundary_yneg -nodeset 87 name "boundary_yneg" +group "boundary_yneg" add node in surface 18 +group "boundary_yneg" add node in surface 45 +group "boundary_yneg" add node in surface 48 +group "boundary_yneg" add node in surface 39 +nodeset 84 group boundary_yneg +nodeset 84 name "boundary_yneg" -# -y w/o fault +# +y w/o fault group "boundary_yneg_nofault" add node in group boundary_yneg group "boundary_yneg_nofault" remove node in group fault_slabtop group "boundary_yneg_nofault" remove node in group fault_slabbot group "boundary_yneg_nofault" remove node in group fault_splay -nodeset 88 group boundary_yneg_nofault -nodeset 88 name "boundary_yneg_nofault" +nodeset 85 group boundary_yneg_nofault +nodeset 85 name "boundary_yneg_nofault" -# -y w/o slab +# +y w/o slab group "boundary_yneg_noslab" add node in group boundary_yneg group "boundary_yneg_noslab" remove node in group block_slab group "boundary_yneg_noslab" remove node in group fault_splay -nodeset 89 group boundary_yneg_noslab -nodeset 89 name "boundary_yneg_noslab" +nodeset 86 group boundary_yneg_noslab +nodeset 86 name "boundary_yneg_noslab" + + +# +y +group "boundary_ypos" add node in surface 21 +group "boundary_ypos" add node in surface 43 +group "boundary_ypos" add node in surface 50 +group "boundary_ypos" add node in surface 36 +nodeset 87 group boundary_ypos +nodeset 87 name "boundary_ypos" + +# -y w/o fault +group "boundary_ypos_nofault" add node in group boundary_ypos +group "boundary_ypos_nofault" remove node in group fault_slabtop +group "boundary_ypos_nofault" remove node in group fault_slabbot +group "boundary_ypos_nofault" remove node in group fault_splay +nodeset 88 group boundary_ypos_nofault +nodeset 88 name "boundary_ypos_nofault" + +# -y w/o slab +group "boundary_ypos_noslab" add node in group boundary_ypos +group "boundary_ypos_noslab" remove node in group block_slab +group "boundary_ypos_noslab" remove node in group fault_splay +nodeset 89 group boundary_ypos_noslab +nodeset 89 name "boundary_ypos_noslab" # -z group "boundary_zneg" add node in surface 10 From ef626f66c91348646ba23147427b1ab31e420ee0 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 13 Jul 2017 10:56:33 -0700 Subject: [PATCH 182/216] Added stepping through nodesets via animation. --- examples/3d/subduction/viz/plot_mesh.py | 39 +++++++++++++++++++++++++ 1 file changed, 39 insertions(+) diff --git a/examples/3d/subduction/viz/plot_mesh.py b/examples/3d/subduction/viz/plot_mesh.py index 2c4cbae339..08450bab8d 100755 --- a/examples/3d/subduction/viz/plot_mesh.py +++ b/examples/3d/subduction/viz/plot_mesh.py @@ -46,6 +46,7 @@ def visualize(parameters): dataDomain = ExodusIIReader(FileName=[parameters.exodus_file]) RenameSource("domain", dataDomain) + view = GetActiveViewOrCreate('RenderView') # Show domain, colored by block. @@ -54,6 +55,7 @@ def visualize(parameters): domainDisplay.RescaleTransferFunctionToDataRange(True, False) domainDisplay.SetScalarBarVisibility(view, False) domainDisplay.SetRepresentationType("Surface") + domainDisplay.PointSize = 6.0 domainDisplay.Opacity = 0.5 # Add coordinate axes @@ -65,6 +67,43 @@ def visualize(parameters): axesDisplay.LineWidth = 4.0 axesDisplay.SetScalarBarVisibility(view, False) axesDisplay.DataAxesGrid.GridColor = [0.0, 0.0, 0.0] + + # Nodeset information + nodeSetInfo = dataDomain.GetProperty("NodeSetInfo").GetData() + nodeSets = nodeSetInfo[::2] + dataDomain.NodeSetArrayStatus = nodeSets[0] + numNodeSets = len(nodeSets) + + nsLabel = Text() + nsLabel.Text = "Nodeset: %s" % nodeSets[0] + RenameSource("nodeset-label") + labelDisplay = Show(nsLabel, view) + labelDisplay.FontSize = 10 + + scene = GetAnimationScene() + scene.NumberOfFrames = numNodeSets + scene.StartTime = 0 + scene.EndTime = float(numNodeSets-1) + + cue = PythonAnimationCue() + cue.Script = """ +from paraview.simple import * + +def tick(self): + scene = GetAnimationScene() + i = int(scene.TimeKeeper.Time) + + domain = FindSource("domain") + nodeSetInfo = domain.GetProperty("NodeSetInfo").GetData() + nodeSets = nodeSetInfo[::2] + nodeSet = nodeSets[i] + domain.NodeSetArrayStatus = nodeSet + + label = FindSource("nodeset-label") + label.Text = "Nodeset: %s" % nodeSet +""" + scene.Cues.append(cue) + view.ResetCamera() Render() From 43193ebc261cf6d14156c4921142f2d8c2dd65a5 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 3 Aug 2017 10:54:05 -0700 Subject: [PATCH 183/216] Added mesh quality to mesh plotting. --- examples/3d/subduction/viz/plot_mesh.py | 137 ++++++++++++++++-------- 1 file changed, 95 insertions(+), 42 deletions(-) diff --git a/examples/3d/subduction/viz/plot_mesh.py b/examples/3d/subduction/viz/plot_mesh.py index 08450bab8d..5487e12098 100755 --- a/examples/3d/subduction/viz/plot_mesh.py +++ b/examples/3d/subduction/viz/plot_mesh.py @@ -15,71 +15,49 @@ # # ---------------------------------------------------------------------- -# Plot the domain, colored by materials. - - +# Plot the domain, colored by materials. Optionally, plot nodesets and +# mesh quality. +# # User-specified parameters. # -# Default values for parameters. To use different values, overwrite -# them in the ParaView Python shell or on the command line. For -# example, set OUTPUT_DIR to the absolute path if not starting -# ParaView from the terminal shell where you ran PyLith: +# To use different values, overwrite them in the ParaView Python shell +# or on the command line. For example, set EXODUS_FILE to the absolute +# path for the Exodus file if not starting ParaView from the terminal +# shell where you ran PyLith: # # import os -# OUTPUT_DIR = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "2d", "subduction", "output") +# EXODUS_FILE = os.path.join(os.environ["HOME"], "src", "pylith", "examples", "3d", "subduction", "mesh", "mesh_tet.exo") DEFAULTS = { "EXODUS_FILE": "mesh/mesh_tet.exo", + "SHOW_NODESETS": True, + "SHOW_QUALITY": True, + "QUALITY_METRIC": "Condition", + "QUALITY_THRESHOLD": 2.0, } # ---------------------------------------------------------------------- from paraview.simple import * import os -def visualize(parameters): - - # Disable automatic camera reset on "Show" - paraview.simple._DisableFirstRenderCameraReset() - - if not os.path.isfile(parameters.exodus_file): - raise IOError("Exodus file '%s' does not exist." % parameters.exodus_file) - dataDomain = ExodusIIReader(FileName=[parameters.exodus_file]) - RenameSource("domain", dataDomain) - - - view = GetActiveViewOrCreate('RenderView') - - # Show domain, colored by block. - domainDisplay = Show(dataDomain, view) - ColorBy(domainDisplay, ("FIELD", "vtkBlockColors")) - domainDisplay.RescaleTransferFunctionToDataRange(True, False) - domainDisplay.SetScalarBarVisibility(view, False) - domainDisplay.SetRepresentationType("Surface") - domainDisplay.PointSize = 6.0 - domainDisplay.Opacity = 0.5 - - # Add coordinate axes - axes = Axes() - axes.ScaleFactor = 1.0e+5 - - axesDisplay = Show(axes, view) - axesDisplay.SetRepresentationType('Wireframe') - axesDisplay.LineWidth = 4.0 - axesDisplay.SetScalarBarVisibility(view, False) - axesDisplay.DataAxesGrid.GridColor = [0.0, 0.0, 0.0] - +def plot_nodesets(dataDomain): + """Create animation with each nodeset displayed as a different + frame. We use a Python script to set the nodeset to display. + """ # Nodeset information nodeSetInfo = dataDomain.GetProperty("NodeSetInfo").GetData() nodeSets = nodeSetInfo[::2] dataDomain.NodeSetArrayStatus = nodeSets[0] numNodeSets = len(nodeSets) + view = GetActiveViewOrCreate('RenderView') + nsLabel = Text() nsLabel.Text = "Nodeset: %s" % nodeSets[0] RenameSource("nodeset-label") labelDisplay = Show(nsLabel, view) labelDisplay.FontSize = 10 - + scene = GetAnimationScene() scene.NumberOfFrames = numNodeSets scene.StartTime = 0 @@ -103,13 +81,81 @@ def tick(self): label.Text = "Nodeset: %s" % nodeSet """ scene.Cues.append(cue) + + return + +def plot_quality(dataDomain, parameters): + """Plot the mesh quality. Only cells with a quality greater (poorer + quality) than the threshold are displayed. + """ + + quality = MeshQuality(Input=dataDomain) + quality.TriangleQualityMeasure = parameters.quality_metric + quality.QuadQualityMeasure = parameters.quality_metric + quality.TetQualityMeasure = parameters.quality_metric + + view = GetActiveViewOrCreate('RenderView') + + # Threshold + threshold = Threshold(Input=quality) + threshold.Scalars = ['CELLS', 'Quality'] + threshold.ThresholdRange = [parameters.quality_threshold, 1.0e+3] + + thresholdDisplay = Show(threshold, view) + thresholdDisplay.Representation = 'Surface' + thresholdDisplay.ColorArrayName = ['CELLS', 'Quality'] + thresholdDisplay.SetScalarBarVisibility(view, True) + + return + + +def visualize(parameters): + + # Disable automatic camera reset on "Show" + paraview.simple._DisableFirstRenderCameraReset() + + if not os.path.isfile(parameters.exodus_file): + raise IOError("Exodus file '%s' does not exist." % parameters.exodus_file) + dataDomain = ExodusIIReader(FileName=[parameters.exodus_file]) + RenameSource("domain", dataDomain) + + + view = GetActiveViewOrCreate('RenderView') + + # Show domain, colored by block. + domainDisplay = Show(dataDomain, view) + ColorBy(domainDisplay, ("FIELD", "vtkBlockColors")) + domainDisplay.RescaleTransferFunctionToDataRange(True, False) + domainDisplay.SetScalarBarVisibility(view, False) + domainDisplay.SetRepresentationType("Surface") + domainDisplay.PointSize = 6.0 + domainDisplay.Opacity = 0.5 + + # Add coordinate axes + axes = Axes() + axes.ScaleFactor = 1.0e+5 + + axesDisplay = Show(axes, view) + axesDisplay.SetRepresentationType('Wireframe') + axesDisplay.LineWidth = 4.0 + axesDisplay.SetScalarBarVisibility(view, False) + axesDisplay.DataAxesGrid.GridColor = [0.0, 0.0, 0.0] + + if parameters.show_nodesets: + plot_nodesets(dataDomain) + + if parameters.show_quality: + plot_quality(dataDomain, parameters) view.ResetCamera() Render() class Parameters(object): - keys = ("EXODUS_FILE",) + """Object for managing default values and overriding them from the + current Python shell. + """ + keys = ("EXODUS_FILE", "SHOW_NODESETS", "SHOW_QUALITY", "QUALITY_METRIC", "QUALITY_THRESHOLD",) def __init__(self): globalVars = globals() @@ -128,6 +174,13 @@ def __init__(self): import argparse parser = argparse.ArgumentParser() parser.add_argument("--filename", action="store", dest="exodus_file", default=DEFAULTS["EXODUS_FILE"]) + parser.add_argument("--hide-nodesets", action="store_false", dest="show_nodesets", default=DEFAULTS["SHOW_NODESETS"]) + parser.add_argument("--hide-quality", action="store_false", dest="show_quality", default=DEFAULTS["SHOW_QUALITY"]) + parser.add_argument("--quality-metric", action="store", dest="quality_metric", default=DEFAULTS["QUALITY_METRIC"]) + parser.add_argument("--quality-threshold", action="store", type=float, dest="quality_threshold", default=DEFAULTS["QUALITY_THRESHOLD"]) + + + args = parser.parse_args() visualize(args) From e1574f58a53101dad13ea5c057c335ce8759dbc0 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 11:09:31 -0700 Subject: [PATCH 184/216] Added \menu macro. --- doc/userguide/pylithdoc.cls | 1 + 1 file changed, 1 insertion(+) diff --git a/doc/userguide/pylithdoc.cls b/doc/userguide/pylithdoc.cls index b9e52b0901..38dd06fd60 100644 --- a/doc/userguide/pylithdoc.cls +++ b/doc/userguide/pylithdoc.cls @@ -194,6 +194,7 @@ \newcommand{\filename}[1]{{\ttfamily #1}} \newcommand{\commandline}[1]{{\ttfamily #1}} \newcommand{\object}[1]{{\sffamily #1}} +\newcommand{\menu}[1]{{\sffamily #1}} % ------------------------------------------------------------------ % Code blocks From c879546816eb0b01c22691f81a5dbddf7a8a36f7 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 11:09:52 -0700 Subject: [PATCH 185/216] Add note on impulse DOF 2 for fault opening. --- .../boundaryconditions/boundaryconditions.tex | 15 ++++++++------- 1 file changed, 8 insertions(+), 7 deletions(-) diff --git a/doc/userguide/boundaryconditions/boundaryconditions.tex b/doc/userguide/boundaryconditions/boundaryconditions.tex index 79f27a5de8..3ee573c02c 100644 --- a/doc/userguide/boundaryconditions/boundaryconditions.tex +++ b/doc/userguide/boundaryconditions/boundaryconditions.tex @@ -643,12 +643,12 @@ \subsection{Fault Parameters} \subsection{Kinematic Earthquake Rupture} -Kinematic earthquake ruptures use the FaultCohesiveKin object to specify -the slip as a function of time on the fault surface. Slip may evolve -simultaneously over the fault surface instantaneously in a single -time step (as is usually done in quasi-static simulations) or propagate -over the fault surface over hundreds and up to thousands of time steps -(as is usually done in a dynamic simulation). +Kinematic earthquake ruptures use the \object{FaultCohesiveKin} object +to specify the slip as a function of time on the fault surface. Slip +may evolve simultaneously over the fault surface instantaneously in a +single time step (as is usually done in quasi-static simulations) or +propagate over the fault surface over hundreds and up to thousands of +time steps (as is usually done in a dynamic simulation). \subsubsection{Governing Equations} @@ -1690,7 +1690,8 @@ \subsection{Slip Impulses for Green's Functions} be generated at locations on the fault where the amplitude exceeds this threshold.} \propertyitem{impulse\_dof}{Array of components associated with impulses, e.g., -[0, 1] for slip involving the lateral and up-dip components.} +[0, 1, 2] for slip involving the left-lateral, reverse, and opening +components, respectively.} \facilityitem{db\_impulse\_amplitude}{Spatial database for amplitude of slip impulse (scalar field). Default is \object{SimpleDB}.} \end{inventory} From e04a22913f9b7eecaf70528f6aa84d2bbcc99e8b Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 11:10:35 -0700 Subject: [PATCH 186/216] Improve installation instructions (flowchart, Windows 10). --- doc/userguide/install/figs/installchoices.pdf | Bin 0 -> 30715 bytes doc/userguide/install/figs/installchoices.tex | 61 ++++++ doc/userguide/install/install.tex | 189 ++++++++++++------ 3 files changed, 191 insertions(+), 59 deletions(-) create mode 100644 doc/userguide/install/figs/installchoices.pdf create mode 100644 doc/userguide/install/figs/installchoices.tex diff --git a/doc/userguide/install/figs/installchoices.pdf b/doc/userguide/install/figs/installchoices.pdf new file mode 100644 index 0000000000000000000000000000000000000000..7a99233ab6017c281396b2f5c31900d8e1c037dd GIT binary patch literal 30715 zcmce+V~j3Qlr`MEZQizRK5g6Gw{6?DZQHhO+qR9{w(;GWcP4q0@5lRVrjk?Hb@r;A z+F4nZterzDCoD?KNXG(AI=3{u2F*;sKwxWN0nN<~O|Rr`XG}n^CTn0}Z0H0{ujp*x z^q)JTwhq?N^n!x6ZUmYP|L}|q|GBiG>Hj11pKmcj)63{PIhg-LF#bdQ%m2syA40*{ z(bn0)(AbfH<=>71G`+O3jj59v0V4~+e_j8om|Hm+I}p%|TIo9(3mY5S8W}_L@xL3{zhJWzzFysYl7*2uZjPV-v0~}|FTFnJHt7`xhWQYs3WC6se_TzV4caaFc|d-d;+ssHhjhyf)tx;W_`jTxG3mNeoN`u>m&j%X` z*x^%zGmQ$>4gLx>IaeFoOwl4wQ^6busAoxTBF>9Z9Xq(0#>cR;?+ZTClBV=OSgT#5 zNk8`}$6j6|46Z-PMIo$&^|GnX8?A_OnvQVUn(p4;+rDG=3XM`I#)ORS?uqSsxsrzP z?PO)=W+S{_7+sUIy-c><;a3ccm8<*Rpag=(if$OLasOc|+=D#~i-0p$Amo9WK`4aJ z0xyie+Em>G@`0pLGY?h037JZA*XhRne!84p#lO+9ZB1R})GyQ7S+krZ$yjTToege< z>RpzR29O0S=-uJQFZO+YzTZ9#QzrIHR-jee-r~hiR+y#pY42?F!CvQH6m8YYG%tzV zt?kD`vVpQRl7f%19AH1mI&E=&u{fWHDJgR04R8WtFErHint%%6W5+Tzk*jCo)r&C#{tUpsHUu)VF?CyynX^=P2X=|q zp1L!m+U}6VTm?{^L!z-57a=!NHM8=ePky;M>t5 z&O}#-5H%%;D3lz>zsqh7yPnGXtWGM(O&aC6E7C(3+LS@LFCx7tFH~z3^#DQyOp+F| zz^DvSY-Ki{03p4J`cB$PP_vXzD#*XIhg}au-~^6soE#yRmoG&z?w?Il!koAvL{buf zdQhTVG-t14nT{mD?5GC$q$MG?TF^wJn$@}xiMNT_O`(lm*}1s6?*xsN-DnqSpiD(! z-*!cC_>*U+EVJ+75Oe4l1MVbA;U!`RW!TPw(EmrgYQSTrEX!0>>=q?XYl6}y0$>H(#^wlW`8C9j80!v&lC51_H_(c9LoADzuxm$o}M?5fIu&BSu z%-2VFqlb7G;aNdAiw-|PNuXZ_TyC_nfzbVVr}{#RLCM^7jK+8#GWPbF$Q)34CY!?7 zr?xdZ#3+AOG45D{e11-zpPqif?7moX;2~9{9>!0zd&QWN@^|*}76X0_BuInLpxhB@ zW0Z8?Mu55bdqUG;74@^HfRsDaGKy-iX#hZ90~;CaiBiGqfs5)-VQKhX+#akTBtfVp zE}@qD(e4dS!J%%&SF{)q2saafVjaxkd2ty;h_K`g<&{K z$hp!^N^$>|8mj5-mcHut{if^3kF8|Bef~1OJokP#Ht_dQnnk=1oxEse8+&{h9Rn5d zL(M-%@?uG@0=NPs8kD{5l(b5J#gDX7@R(gX_I1sS@GPPslrr4u;HD^RILM5b^CEG+ zE9U=7TUQHnDh$EW@fSJ^`L$MS6%ikFNjl`61C1id>bEBtnooB`XvS`M#V<_NBvUDn zFS{&Jw>DO7l+WXcwVh0}jM%7Ve;`S(VP*PQ#i(9=DeY>z7@tRFx?kg>G-QW`c_ir) zFHU70%?_rN;m+fAA7OYGq5Qdo2O#^3BT}~`i`w?jMlJ#=Sm^J+0VZGa(dSBopw0u z$(GxrpSiKwGA{9SzP^V^@;S9xFtk0qM(P7=gB*Znp%ywYEE2blKxB4Ow2H!2Fr|4{ zv?X<-h~k$lRq~eH#okCdS-dL(E3afh6_1Zh!h(@BJu6v9QgC-7IfvX?v`0A0v zZ8T({aZl;Mq0);??uCP8`lgQ|@c`F`P#w9p51BKI{jh3G?^QN2CKx7FqzO2#ZCAImvYGm^*N%gLBKs z75)T^k}h?foiYJsvN^v zm9y8u`P+%%)J!6^Us3y?2ZsgzfWz!&IkNKbxl`{iy0|CLu#MCp#`iP8&dx`SNKR#NX7)v5?F^yvvd`IB8Nm zN9RMvdj7cx?cN*SVo`(V#1R@ZBZ8CKYx%SIRH>+yEUiisX$9WmU_!c6)?%`gy+Xo@ z=;^yKVm7o*(ZNRvH57R#eaUIZSBd&#)n18o1y_{kzHA_5;K1WWep=cyhAO?%Q7OFZ z!@8nfKZI-FgcY0wsF!hJd$uI`>!Pk)1@FfvO9J>-(5{n~^X^jGUvs5LzOt_}J;Atx z*;nzWxoe(giMIHlIb!b53>8=WRn*U!J$`$5pyA5ssrZ`ammo1U+%eAq=l4>SW_Vq? 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Binary packages have been created for Linux and Mac -OS X platforms. You can also run PyLith inside a Docker container, -which provides a virtual Linux environment on any platform that Docker -supports, including Linux, Mac OS X, and Windows. Installation of -PyLith on other operating systems -- or installation on a cluster -- -requires building the software from the source code, which can be -difficult for inexperienced users. We have created a small utility -called PyLith Installer that makes installing PyLith and all of its -dependencies from source much easier. Help is available from both a -CIG mailing list and the GitHub issue tracking system -\url{https://github.com/geodynamics/pylith/issues}. +Figure~\ref{fig:install:choices} provides a guide to select the +appropriate method for installing PyLith. Installation of PyLith on a +desktop or laptop machine is, in most cases, very easy. Binary +packages have been created for Linux and Mac OS X (Darwin) platforms. For +Windows 10 users, we recommend installing the Windows Subsystem for +Linux and using the Linux binary (see instructions in +Section~\ref{sec:install:windows}). You can also run PyLith +inside a Docker container, which provides a virtual Linux environment +on any platform that Docker supports, including Linux, Mac OS X, and +Windows. Installation of PyLith on other operating systems -- or +installation on a cluster -- requires building the software from the +source code, which can be difficult for inexperienced users. We have +created a small utility called PyLith Installer that makes installing +PyLith and all of its dependencies from source much easier. + +\begin{figure}[htbp] + \includegraphics[scale=0.8]{install/figs/installchoices} + \caption{Guide for selecting the appropriate installation choice + based on a hardware and intended use. The installation options are + discussed in more detail in the following sections.} +\label{fig:install:choices} +\end{figure} + +Help for installing and using PyLith is available from both a CIG +mailing list and the GitHub issue tracking system +\url{https://github.com/geodynamics/pylith/issues}. See +Section~\vref{sec:help} for more information. +\section{Installation of Binary Executable} -\section{Getting Help and Reporting Bugs} -\label{sec:help} - -The CIG Short-Term Crustal Dynamics Mailing List -\url{cig-short@geodynamics.org} is dedicated to CIG issues associated -with short-term crustal dynamics, including the use of PyLith. You can -subscribe to the mailing list and view messages at cig-short Mailing -List \url{geodynamics.org/cig/lists/cig-short}. - -CIG uses \object{GitHub} for source control and bug tracking. If you -find a bug in PyLith, please submit a bug report to the GitHub issue -tracking system for PyLith \url{https://github.com/geodynamics/pylith/issues}. -Of course, it is helpful to first check to see if someone else already -submitted a report related to the issue; one of the CIG developers -may have posted a work around to the problem. You can reply to a current -issue by clicking on the issue title. To submit a new issue, click -on the \object{New Issue} button. +The binaries are intended for users running on laptops or desktop +computers (as opposed to clusters). The binaries contain the compilers +and header files, so users wishing to extend the code can still use +the binary and do not need to build PyLith and its dependencies from +source. See Chapter~\vref{cha:extending} for more information on +extending PyLith. +Binary executables are available for Linux (glibc 2.12 and later) and +Mac OS X (Intel 10.10 and later) from the PyLith web page +\url{geodynamics.org/cig/software/packages/short/pylith/}. Users +running Windows 10 build 14316 and later can install a Linux bash +environment and use the PyLith binary for Linux (see +Section~\vref{sec:install:windows} for more information). -\section{Installation of Binary Executable} +\tip{On Linux systems you can check which version of glibc you have by + running \filename{ldd --version}}. -Binary executables are available for Linux and Mac OS X (Intel 10.10+) -from the PyLith web page -\url{geodynamics.org/cig/software/packages/short/pylith/}. +\tip{On Darwin systems running OS X, you can check the operating + system version by clicking on the Apple icon and \menu{About this Mac}.} -\subsection{Linux and Max OS X} +\subsection{Linux and Max OS X (Darwin)} \begin{enumerate} \item Open a terminal window and change to the directory where you want to place the distribution. @@ -49,8 +60,9 @@ \subsection{Linux and Max OS X} $$ mkdir pylith $$ cd pylith \end{shell} -\item Download the Linux or Mac OS X tarball from the PyLith web page \url{geodynamics.org/cig/software/packages/short/pylith/}, -and save it to the desired location, e.g., \filename{\$HOME/pylith}. +\item Download the Linux or Mac OS X (Darwin) tarball from the PyLith + web page \url{geodynamics.org/cig/software/packages/short/pylith/}, + and save it to the desired location, e.g., \filename{\$HOME/pylith}. \item Unpack the tarball. \begin{shell} # Linux 32-bit @@ -80,12 +92,42 @@ \subsection{Linux and Max OS X} \warning{The PyLith binary distribution for {\bf Darwin} systems is built using the system clang compiler suite and the system - Python. {\bf This means the system Python must be in your path to use the - PyLith binary executable}; ensure \filename{/bin} and + Python. {\bf This means the system Python must be in your path to + use the PyLith binary executable}; ensure \filename{/bin} and \filename{/usr/bin} are at the beginning of the PATH environment - variable before sourcing \filename{setup.sh}. {\bf This usually - applies if you have Python installed from Anaconda, HomeBrew, - MacPorts, etc.}} + variable, which is done automatically if you use the + \filename{setup.sh} script. {\bf This condition is often violated if + you have Python installed from Anaconda, HomeBrew, MacPorts, + etc. and set the PATH variable in your bash configuration file.}} + +\subsection{Windows 10} +\label{sec:install:windows} + +PyLith is developed within the Unix/Linux framework, and we do not +provide a native PyLith binary distribution for Windows. The preferred +approach to installing PyLith on a computer running Windows 10 is to +enable use of a Linux subsystem. This permits use of the PyLith Linux +x86\_64 binary within the bash environment. + +To enable the Linux subsystem on Windows 10 build 14316 and later +(users running an earlier Windows build should use the PyLith Docker +container): +\begin{enumerate} +\item Go to \menu{Settings} $\rightarrow$ \menu{Security}. +\item Under \menu{For developers} select \menu{Developer mode}. This + step should not be required for Windows build 16215 and later. +\item Go to \menu{Control Panel} $\rightarrow$ \menu{Programs} + $\rightarrow$ \menu{Turn Windows Features On or Off}. +\item Enable \menu{Windows Subsystem for Linux} and click \menu{OK}. +\item Restart the computer. +\item Go to \menu{Start} $\rightarrow$ \menu{bash}. You will be + prompted to download "Bash on Ubuntu on Windows" from the Windows + Store. Create a user account and password for the bash environment. +\item Install the PyLith Linux x86 binary within the bash environment + following the instructions for installing the PyLith binary for + Linux. You will run PyLith within the bash environment just like you + would for a Linux operating system. +\end{enumerate} \subsection{Extending PyLith and/or Integrating Other Software Into PyLith} \newfeature{v.2.2.0} @@ -109,11 +151,20 @@ \subsection{Extending PyLith and/or Integrating Other Software Into PyLith} \section{Installation of PyLith Docker Container} -Docker containers provide a self-contained virtual environment that -are a smaller, simpler alternative to a virtual machine. The PyLith -Docker container provides a Debian Linux environment with a pre-built -PyLith executable, vim text editor, iceweasel (GNU version of Firefox) -web-browser, and the matplotlib Python module. +As an alternative to installing a binary package, we provide a Docker +container for running PyLith in a self-contained virtual +environment. Docker containers provide a self-contained virtual +environment that are a smaller, simpler alternative to a virtual +machine. The PyLith Docker container provides a Debian Linux +environment with a pre-built PyLith executable, vim text editor, +iceweasel (GNU version of Firefox) web-browser, and the matplotlib +Python module. + +\tip{In nearly all cases, installing a PyLith binary provides easier + integration with mesh generation and post-processing tools, so + binaries are the preferred approach to using the PyLith Docker + container. This installation method targets users running Windows + versions earlier than Windows 10 build 14316.} \subsection{Setup (first time only)} @@ -156,7 +207,7 @@ \subsection{Run Unix shell within Docker to use PyLith.} \end{shell} In addition to a minimalist Debian Linux distribution and PyLith and -all of its depenencies, the container includes the following useful +all of its dependencies, the container includes the following useful utilities: \begin{description} \item[vim] Lightweight text editor @@ -220,17 +271,17 @@ \section{Installation from Source} \vref{fig:pylith-dependencies}). This complicates building the software from the source code. In many cases some of the packages required by PyLith are available as binary packages. On the one hand, -using the binary packages removes the burden of configuring, building, -and installing these packages, but that can come with its own host of -complications if consistent compiler and configuration settings are -not used across all of the packages on which PyLith depends. This is -usually not an issue with Linux distributions, such as Fedora, Ubuntu, -and Debian that have good quality control; it can be an issue with -Darwin package managers, such as Fink, MacPorts, and Homebrew, where -there is limited enforcement of consistency across -packages. Nevertheless, PyLith can be built on most systems provided -the instructions are followed carefully. PyLith is developed and -tested on Linux and Mac OS X. +using the binary packages for the dependencies removes the burden of +configuring, building, and installing these dependencies, but that can +come with its own host of complications if consistent compiler and +configuration settings are not used across all of the packages on +which PyLith depends. This is usually not an issue with Linux +distributions, such as Fedora, Ubuntu, and Debian that have good +quality control; it can be an issue with Darwin package managers, such +as Fink, MacPorts, and Homebrew, where there is limited enforcement of +consistency across packages. Nevertheless, PyLith can be built on most +systems provided the instructions are followed carefully. PyLith is +developed and tested on Linux and Mac OS X. A small utility, PyLith Installer, removes most of the obstacles in building PyLith and its dependencies from source. For each package @@ -350,7 +401,7 @@ \subsection{Running without a Batch System} On a cluster without a batch system, you need to explicitly specify the machines on which the job will run. Supposing the machines on your -cluster are named n001, n002, \ldots{}, etc., but you want to run the +cluster are named n001, n002, \ldots, etc., but you want to run the job on machines n001, n003, n004, and n005 (maybe n002 is down for the moment). To run an example, create a file named \filename{mymachines.cfg} which specifies the machines to use: @@ -448,4 +499,24 @@ \subsubsection{PBS Batch System} For most PBS batch systems you can specify N processes per compute node via the command line argument \commandline{-{}-scheduler.ppn=N}. +\section{Getting Help and Reporting Bugs} +\label{sec:help} + +The CIG Short-Term +Crustal Dynamics Mailing List \url{cig-short@geodynamics.org} is +dedicated to CIG issues associated with short-term crustal dynamics, +including the use of PyLith. You can subscribe to the mailing list and +view messages at cig-short Mailing List +\url{geodynamics.org/cig/lists/cig-short}. + +CIG uses \object{GitHub} for source control and bug tracking. If you +find a bug in PyLith, please submit a bug report to the GitHub issue +tracking system for PyLith \url{https://github.com/geodynamics/pylith/issues}. +Of course, it is helpful to first check to see if someone else already +submitted a report related to the issue; one of the CIG developers +may have posted a work around to the problem. You can reply to a current +issue by clicking on the issue title. To submit a new issue, click +on the \object{New Issue} button. + + % End of file From 57d6cb952c5abaec2c3c7983e38d161c86521fc5 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 20:18:55 -0700 Subject: [PATCH 187/216] Add python listing environment. --- doc/userguide/pylithdoc.cls | 9 +++++++++ 1 file changed, 9 insertions(+) diff --git a/doc/userguide/pylithdoc.cls b/doc/userguide/pylithdoc.cls index 38dd06fd60..f7356c1022 100644 --- a/doc/userguide/pylithdoc.cls +++ b/doc/userguide/pylithdoc.cls @@ -218,6 +218,15 @@ morekeywords={$$},% commentstyle=\itshape\color{orange}, }}{} +% +% python +\lstnewenvironment{python}{\lstset{% + language=python,% + frame=single,% + basicstyle=\small\ttfamily,% + morekeywords={>>>},% + commentstyle=\itshape\color{orange}, +}}{} % ------------------------------------------------------------------ % Lists From 115dc41610490001d8e58c2082e949c0e97b70bc Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 20:19:29 -0700 Subject: [PATCH 188/216] Added section on ParaView Python scripts. --- doc/userguide/examples/examples.tex | 73 +++++++++++++++++++++++++++++ 1 file changed, 73 insertions(+) diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 92b4b3234e..6988467025 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -39,6 +39,79 @@ \subsubsection{Input Files} mesh generation software to create the meshes. All of the files used in the example problems are extensively documented with comments. +\subsection{Organization of Examples} + +\todo{brad}{ADD STUFF HERE} + +\section{ParaView Python Scripts} +\label{sec:ParaView:Python:scripts} +\newfeature{v2.2.1} + +In some of the examples (currently only the 2D and 3D subduction zone +examples) we provide ParaView Python scripts for visualizing the input +finite-element mesh and the PyLith simulation results. Some of these +scripts are very generic and are easily reused; others are more +specific to the examples. The primary advantage of the ParaView Python +scripts is that they make it easy to replicate visualizations, whether +they are produced by the developers and regenerated by users. + +There are several different ways to run the ParaView Python scripts: +\begin{itemize} +\item Within the ParaView GUI, select + \menu{Tools}$\rightarrow$\menu{Python Shell}. Override the default + parameters as desired (which we will discuss later in this + section). Click on the \menu{Run Script} button, and navigate to the + select the script you want to run. +\item From a shell (terminal window) start ParaView from the command + line with the \filename{-{}-script=FILENAME} where + \filename{FILENAME} is the relative or absolute path to the ParaView + Python script. Note that this method does not provide a mechanism + for overriding the default parameters. +\item Run the ParaView Python script directly from a shell (terminal + window) via the command line. You can use command line arguments to + override the default values for the parameters. +\end{itemize} + +\tip{Running the ParaView Python script from within the ParaView GUI + allows further manipulation of the data, which is not possible when + running the ParaView Python script outside the ParaView GUI. When + run outside the ParaView GUI, the interaction is limited to + rotating, translating, and zooming.} + +\important{The ParaView Python scripts run Python via + \filename{pvpython}, which is a customized version of the Python + interpreter included in the ParaView distribution. This is different + from Python provided with your operating system and/or the one + included in the PyLith distribution. This means you cannot, in + general, import Python modules provided with the PyLith distribution + into ParaView.} + +\subsection{Overriding Default Parameters} + +We setup the ParaView Python scripts, so that when they are run from +the command line in the main directory for a given example, e.g., +\filename{examples/3d/subduction}, the script will produce the output +discussed in the manual. If you start ParaView from the OS X Dock or a +similar method, like a shortcut, then you will need to override at +least the default values for the data file(s). + +In order to override the default values from within the ParaView GUI, +simply set the values within the Python shell. For example, to set the +value of the variable \object{EXODUS\_FILE} to the absolute path of +the input file, +\begin{python} +>>> EXODUS_FILE = "/home/johndoe/pylith/examples/3d/subduction/mesh/mesh_tet.exo" +\end{python} +In this case, we use the Python os module to get the absolute path of +the home directory and append the path to the Exodus file with the +appropriate separators for the operating system. + +\important{In each of the ParaView Python scripts, the names of the + variables and their default values are given by the DEFAULTS + dictionary near the top of the file.} + + +% ====================================================================== \input{./examples/twotri3.tex} \input{./examples/twoquad4.tex} \input{./examples/twotet4.tex} From 504d08b59c775f442a6bf2287acdcbaa93380c1f Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 20:19:58 -0700 Subject: [PATCH 189/216] Added figure with mesh and discussion of viz/plot_mesh.py. --- 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zsWL8yvrw|1pq`;u)WY3Umx8ML>4O)bW}<>8P)$Y{{TZJrR2y@ogz literal 0 HcmV?d00001 diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index cc1427f1c8..793ddcd60c 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -157,6 +157,47 @@ \subsection{Generating the Finite-Element Mesh} journal file to understand how we assemble the 3-D slab and cut the rectangular domain into pieces.} +\subsubsection{Visualizing the Mesh} + +The Exodus-II file \filename{mesh\_tet.exo} can be viewed with +ParaView. We provide the Python script \filename{viz/pot\_mesh.py} to +visualize the nodesets and the mesh quality using the condition number +metric. As in our other Python scripts for ParaView (see +Section~\vref{sec:ParaView:Python:scripts} for a discussion of how to use +Python ParaView scripts), you can override the default +parameters by setting appropriate values in the Python shell (if +running within the ParaView GUI) or from the command line (if running +the script directly outside the GUI). When viewing the nodesets, the +animation controls allow stepping through the nodesets. When viewing +the mesh quality, only the cells with the given quality metric above +some threshold (poorer quality) are shown. The default quality metric +is condition number and the default threshold is 2.0. + +To visualize the mesh, start ParaView. Within the ParaView GUI Python shell +(\menu{Tools}$\rightarrow$\menu{Python Shell}), we override the +\filename{EXODUS\_FILE} and \filename{SHOW\_QUALITY} parameters. +\begin{python} +# Import the os module so we can get access to the HOME environment variable. +>>> import os +>>> HOME = os.environ["HOME"] +>>> EXODUS_FILE = os.path.join(HOME,"pylith","examples","3d","subduction","mesh","mesh_tet.exo") +# Turn off display of the mesh quality (show only the nodesets). +>>> SHOW_QUALITY = False +\end{python} +We then click on the \menu{Run Script} button and navigate to the +\filename{examples/3d/subduction/viz} directory and select +\filename{plot\_mesh.py}. + +\begin{figure}[htbp] + \includegraphics[width=5.0in]{examples/figs/subduction3d_mesh} + \caption{Visualization of the \object{fault\_slabtop} nodeset + (yellow dots) for the Exodus-II file \filename{mesh/mesh\_tet.exo} + using the \filename{viz/plot\_mesh.py} ParaView Python script. One + can step through the different nodesets using the animation + controls. This script can also be use to show the mesh quality.} + \label{fig:example:subduction:3d:mesh} +\end{figure} + \subsection{Organization of Simulation Parameters} \label{sec:example:subduction:3d:organization} @@ -448,6 +489,7 @@ \subsection{Step 1: Axial Compression} \end{figure} +\todo{brad}{Update this} There are three different ways you can run this Python script to view the solution: \begin{enumerate} From 1b441f738d714edd99c316b423cc8bc611e94bb5 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 18 Aug 2017 20:20:32 -0700 Subject: [PATCH 190/216] Improve camera settings. --- examples/3d/subduction/viz/plot_mesh.py | 12 ++++++------ 1 file changed, 6 insertions(+), 6 deletions(-) diff --git a/examples/3d/subduction/viz/plot_mesh.py b/examples/3d/subduction/viz/plot_mesh.py index 5487e12098..63819203ee 100755 --- a/examples/3d/subduction/viz/plot_mesh.py +++ b/examples/3d/subduction/viz/plot_mesh.py @@ -178,21 +178,21 @@ def __init__(self): parser.add_argument("--hide-quality", action="store_false", dest="show_quality", default=DEFAULTS["SHOW_QUALITY"]) parser.add_argument("--quality-metric", action="store", dest="quality_metric", default=DEFAULTS["QUALITY_METRIC"]) parser.add_argument("--quality-threshold", action="store", type=float, dest="quality_threshold", default=DEFAULTS["QUALITY_THRESHOLD"]) - - - + parser.add_argument("--screenshot", action="store", dest="screenshot") args = parser.parse_args() visualize(args) view = GetRenderView() - #view.CameraPosition = [-80160, -1130898, 133977] - #view.CameraFocalPoint = [-55107, 446810, 283137] + view.CameraPosition = [78002.89373974672, -1531813.1739094853, 595774.2094961794] + view.CameraFocalPoint = [-45014.6313325238, 149523.68421156122, -335271.271063906] view.CameraViewUp = [0.0, 0.0, 1.0] - view.CameraViewAngle = 45.0 view.ViewSize = [960, 540] view.Update() + if args.screenshot: + WriteImage(args.screenshot) + Interact() else: From 872d4536ccaabe4c4c1bbf700934399e1df056ea Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 21 Aug 2017 15:15:10 -0700 Subject: [PATCH 191/216] Add a little more info on ParaView Python scripts. --- doc/userguide/examples/examples.tex | 5 ++++- 1 file changed, 4 insertions(+), 1 deletion(-) diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 6988467025..f596f70ba2 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -69,7 +69,10 @@ \section{ParaView Python Scripts} for overriding the default parameters. \item Run the ParaView Python script directly from a shell (terminal window) via the command line. You can use command line arguments to - override the default values for the parameters. + override the default values for the parameters. If pvpython is not + in your PATH, then you can run a script called + \filename{MY\_SCRIPT.py} using: + \filename{PATH\_TO\_PVPYTHON/pvpython MY\_SCRIPT.py} \end{itemize} \tip{Running the ParaView Python script from within the ParaView GUI From adb62117fd17d434cea78a514fe5cba3fcd1e9d3 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 21 Aug 2017 15:15:19 -0700 Subject: [PATCH 192/216] Add a little more info on ParaView Python scripts. --- doc/userguide/examples/subduction2d.tex | 19 +++++++++---------- 1 file changed, 9 insertions(+), 10 deletions(-) diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index 4f483fd933..9b9b281a1e 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -502,16 +502,15 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} The problem will produce fourteen pairs of HDF5/Xdmf files. Figure \vref{fig:example:subduction:2d:step05}, which was created using the ParaView Python script \filename{viz/plot\_dispwarp.py} (see -Section~\ref{sec:example:subduction:3d:step01} for a discussion of how - to run ParaView Python scripts), displays the -magnitude of the velocity field with the original configuration -exaggerated by a factor of 4000. Steady slip is largely confined to -the stable sliding regions with a sequence of ruptures in the -seismogenic zone; most have a duration of a few time steps, although -most of the slip occurs in a single time -step. Figure~\ref{fig:example:subduction:2d:step05:slip} shows the -cumulative slip as a function of time and distance down dip from the -trench. +Section~\vref{sec:ParaView:Python:scripts} for a discussion of how to +run ParaView Python scripts), displays the magnitude of the velocity +field with the original configuration exaggerated by a factor of +4000. Steady slip is largely confined to the stable sliding regions +with a sequence of ruptures in the seismogenic zone; most have a +duration of a few time steps, although most of the slip occurs in a +single time step. Figure~\ref{fig:example:subduction:2d:step05:slip} +shows the cumulative slip as a function of time and distance down dip +from the trench. \begin{figure} \includegraphics[width=4.5in]{examples/figs/subduction2d_step05_soln} From ecbc20e82a925919968a7f58227782f507632f60 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 21 Aug 2017 15:16:01 -0700 Subject: [PATCH 193/216] Improve description of simulation output and cross-reference section on ParaView Python scripts. --- doc/userguide/examples/subduction3d.tex | 221 +++++++++++++----------- 1 file changed, 118 insertions(+), 103 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 793ddcd60c..602210677f 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -180,6 +180,7 @@ \subsubsection{Visualizing the Mesh} # Import the os module so we can get access to the HOME environment variable. >>> import os >>> HOME = os.environ["HOME"] +# You may need to adjust the next line, depending on where you installed PyLith. >>> EXODUS_FILE = os.path.join(HOME,"pylith","examples","3d","subduction","mesh","mesh_tet.exo") # Turn off display of the mesh quality (show only the nodesets). >>> SHOW_QUALITY = False @@ -453,31 +454,53 @@ \subsection{Step 1: Axial Compression} The remaining parameters in the \filename{step01.cfg} file are mostly associated with setting filenames for all of the various output, including all of the parameters used and version information in a JSON -file, a file reporting the progress of the simulation and estimated -time of completion, and the filenames for the HDF5 files (the -corresponding Xdmf files will use the same filename with the -\filename{.xmf} suffix). +file (\filename{output/step01-parameters.json}), a file reporting the +progress of the simulation and estimated time of completion +(\filename{output/step01-progress.txt}), and the filenames for the +HDF5 files (the corresponding Xdmf files will use the same filename +with the \filename{.xmf} suffix). We run this example by typing \begin{shell} $$ pylith step01.cfg mat_elastic.cfg \end{shell} -The problem will produce ten pairs of HDF5/Xdmf files. The HDF5 -files contain the data and the Xdmf files contain the metadata required -by ParaView and Visit (and other visualization tools that -use Xdmf files) to access the mesh and data sets in the HDF5 files. -The files include the solution over the domain and ground surface -(two pairs of files), and physical properties, stress, and strain within -each material (eight pairs of files). - -Figure \ref{fig:example:subduction:3d:step01}, which was created -using the ParaView Python script \filename{plot\_dispvec.py}, displays -the magnitude of the displacement field arrows showing the direction -and magnitude of the deformation. Material properties with a positive -Poisson's ratio result in vertical deformation along with the axial -compression. The variations in material properties among the -properties result in local spatial variations that are most evident in -the horizontal displacement components. +The simulation will produce ten pairs of HDF5/Xdmf files in the +\filename{output} directory: +\begin{description} +% Domain and subdomain output +\item[\filename{step01-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step01-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +% Materials +\item[\filename{step01-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step01-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step01-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step01-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step01-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step01-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step01-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step01-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. +\end{description} +The HDF5 files contain the data and the Xdmf files contain the +metadata required by ParaView and Visit (and other visualization tools +that use Xdmf files) to access the mesh and data sets in the HDF5 +files. + +Figure \ref{fig:example:subduction:3d:step01}, which was created using +the ParaView Python script \filename{plot\_dispvec.py} (see +Section~\vref{sec:ParaView:Python:scripts} for how to run ParaView +Python scripts), displays the magnitude of +the displacement field arrows showing the direction and magnitude of +the deformation. Material properties with a positive Poisson's ratio +result in vertical deformation along with the axial compression. The +variations in material properties among the properties result in local +spatial variations that are most evident in the horizontal +displacement components. \begin{figure} \includegraphics[width=5.0in]{examples/figs/subduction3d_step01_soln} @@ -488,86 +511,32 @@ \subsection{Step 1: Axial Compression} \label{fig:example:subduction:3d:step01} \end{figure} - -\todo{brad}{Update this} -There are three different ways you can run this Python script to view -the solution: -\begin{enumerate} -\item From a shell (terminal window) start ParaView via the command line from the - \filename{examples/3d/subduction} directory. Within the ParaView GUI, select - \object{Tools}$\rightarrow$\object{Python Shell}, click on the - \object{Run Script} button, and navigate to the \filename{viz} - directory and select the \filename{plot\_dispvec.py} file. - -\item From a shell (terminal window) start ParaView via the command line from the - \filename{examples/3d/subduction} directory adding the - \filename{-{}-script=viz/plot\_dispvec.py} command line argument. -\begin{shell} -# Make sure you are in the examples/3d/subduction directory. -$$ PATH_TO_PARAVIEW/paraview --script=viz/plot_dispvec.py -\end{shell} -\item Run the ParaView Python script directly from a shell (terminal - window) via the command line. You can use command line arguments to - set user-specified parameters. If pvpython -\begin{shell} -# Make sure you are in the examples/3d/subduction directory. -# We show the optional command line arguments in square brackets. -$$ ./viz/plot_dispvec.py [--vector-scale=10.0e+4] [--sim=step01.cfg} [--screenshot=FILE] -# -# If pvpython is not in your PATH, then you can run the script using: -$$ PATH_TO_PVPYTHON/pvpython ./viz/plot_dispvec.py -\end{shell} -\end{enumerate} - -\tip{Running the ParaView Python script from within the ParaView GUI - allows further manipulation of the data, which is not possible when - running the ParaView Python script outside the ParaView - GUI.} - -\tip{In order to change the user-specified parameters in the ParaView - Python scripts when running them from within the ParaView GUI, you - must edit the file in an external text editor before running the - script. If you are running these script from outside the ParaView - GUI, you can simply use command line argument to change the - user-specified parameters.} - -\important{The ParaView Python scripts run Python via - \filename{pvpython}, which is a customized version of the Python - interpreter included in the ParaView distribution. This is different - from Python provided with your operating system and the one included - in the PyLith distribution.} - - \subsubsection{Exercises} - \begin{itemize} \item Run PyLith again and add \filename{solver\_algebraicmultigrid.cfg} as an argument on the - command line to switch to the - algebraic multigrid preconditioner. + command line to switch to the algebraic multigrid preconditioner. \begin{itemize} - \item Using the PETSc log summary to compare the runtime and - memory use between the original LU preconditioner and the ML - algebraic multigrid preconditioner. Hint: The algebraic - multigrid preconditioner is faster. + \item Using the PETSc log summary to compare the runtime and memory + use between the original LU preconditioner and the ML algebraic + multigrid preconditioner. Hint: The algebraic multigrid + preconditioner is faster. \item Run the simulation again with the algebraic multigrid preconditioner using multiple cores via the \commandline{-{}-nodes=NCORES} argument, replacing \commandline{NCORES} with 2 or up to the number of cores on your - machine. Examine the PETSc log summary for the various runs to - see how the time spent at varies stages changes with the number - of cores. Make a plot of runtime versus the number of - cores. + machine. Examine the PETSc log summary for the various runs to see + how the time spent at varies stages changes with the number of + cores. Make a plot of runtime versus the number of cores. \end{itemize} -\item Adjust the material properties in the spatial databases so that the slab is stiffer and - the wedge is more compliant. What happens to the solution if you make the - materials nearly incompressible? Does this also affect the rate of - convergence of the linear solve? +\item Adjust the material properties in the spatial databases so that + the slab is stiffer and the wedge is more compliant. What happens to + the solution if you make the materials nearly incompressible? Does + this also affect the rate of convergence of the linear solve? \item Change the Dirichlet boundary conditions to impose pure shear instead of axial compression. Hint: You will need to change the - boundary conditions on the east, west, north, and south - boundaries. + boundary conditions on the east, west, north, and south boundaries. \end{itemize} @@ -734,6 +703,18 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \begin{shell} $$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} +The simulation will produce twelve pairs of HDF5/Xdmf files, beginning +with \filename{step02}, in the \filename{output} directory. In +addition to the ten pairs of HDF5/Xdmf files analogous to those +produced in Step 1, we also have two pairs of HDF5/Xdmf files +associated with the fault: +\begin{description} +% Fault +\item[\filename{step02-fault-slab\_info.h5[.xmf]}] Fault orientation + and rupture information. +\item[\filename{step02-fault-slab.h5[.xmf]}] Time series of slip and + traction changes. +\end{description} Figure \ref{fig:example:subduction:3d:step02}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, @@ -929,6 +910,11 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \begin{shell} $$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} +The simulation will produce fourteen pairs of HDF5/Xdmf files, +beginning with \filename{step03}, in the \filename{output} +directory. As in Step 2, there are two pairs of HDF5/Xdmf files for +each fault; one set for the fault orientation and rupture information +and one set for the time series of slip and change in tractions. Figure \ref{fig:example:subduction:3d:step03}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, shows @@ -1106,6 +1092,11 @@ \subsection{Step 4: Prescribed Earthquake Cycle} \begin{shell} $$ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} +The simulation will produce sixteen pairs of HDF5/Xdmf files, +beginning with \filename{step04}, in the \filename{output} +directory. The output includes the solution over the domain and ground +surface, the properties and state variables for each material, and the +the fault orientation and rupture information for each fault. Figure \ref{fig:example:subduction:3d:step04}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, shows @@ -1292,7 +1283,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} $$ cd .. $$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} -The problem will produce 13 pairs of HDF5/Xdmf files. The additional +The problem will produce thirteen pairs of HDF5/Xdmf files. The additional HDF5 file that was not present in previous examples is \filename{step06-cgps\_sites.h5}, which contains the displacements at the fake cGPS sites. @@ -1434,12 +1425,24 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} $$ pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg $$ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} +Each simulation will produce four pairs of HDF5/Xdmf files. For Step +7a these will be: +\begin{description} +\item[\filename{step07a-groundsurf.h5[.xmf]}] Solution field over the + ground surface for each slip impulse. +\item[\filename{step07a-cgps\_sites.h5[.xmf]}] Solution field at + continuous GPS sites for each slip impulse. +\item[\filename{step07a-fault-slab\_info.h5[.xmf]}] Fault orientation + and impulse information. +\item[\filename{step07a-fault-slab.h5[.xmf]}] Fault slip for each slip + impulse. +\end{description} \tip{To save time, run the two sub-problems simultaneously in separate - shells (terminals). For a problem this size, this should work fine - on a laptop. For larger problems, we would run the simulations via - separate jobs on a cluster with each job running on multiple - processes.} + shells (terminal windows or tabs). For a problem this size, this + should work fine on a laptop. For larger problems, we would run the + simulations via separate jobs on a cluster with each job running on + multiple processes.} % Post-process Step 6 output Before we can run the inversion, we post-process the output from Step @@ -1631,6 +1634,11 @@ \subsubsection{Step 08a} \begin{shell} $$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} +The simulation will generate ten pairs of HDF5/Xdmf files beginning +with \filename{step08a}. Two pairs of files include the solution over +the domain and ground surface. For each material the \filename{info} +pair of files contains the properties and the other pair of files +pairs of files contains the state variables. When the problem has run, we see deformation that is consistent with the mismatched densities. The slab subsides while the crust undergoes @@ -1652,22 +1660,22 @@ \subsubsection{Step 08a} \subsubsection{Step 8b} -Step 8b is similar to Step 8a, but we use the stresses output from Step 8a as the -initial stress rather than analytically computing +Step 8b is similar to Step 8a, but we use the stresses output from +Step 8a as the initial stress rather than analytically computing initial stresses. Because the initial stresses are consistent with the variations in density across the materials, the initial stresses will satisfy equilibrium and there will be essentially no deformation; the initial stresses do not perfectly balance because in Step 8a we average the values over the quadrature points for the output. We use -the Python script \filename{generate\_initial\_stress.py}, located in the -\filename{spatialdb} directory, to -postprocess the output from Step 8a and generate the initial stress -spatial database. Note that this script uses the Python interface to -the spatialdata package to write the spatial database; this is much -easier than writing a script to format the data to conform to the -format of the spatial database. The spatial database will contain the -stresses at each cell of our unstructured mesh, so the points are not -on a logical grid, and we must use a \object{SimpleDB}. +the Python script \filename{generate\_initial\_stress.py}, located in +the \filename{spatialdb} directory, to postprocess the output from +Step 8a and generate the initial stress spatial database. Note that +this script uses the Python interface to the spatialdata package to +write the spatial database; this is much easier than writing a script +to format the data to conform to the format of the spatial +database. The spatial database will contain the stresses at each cell +of our unstructured mesh, so the points are not on a logical grid, and +we must use a \object{SimpleDB}. \begin{shell} # From the examples/3d/subduction directory, change to the spatialdb subdirectory. $$ cd spatialdb @@ -1705,6 +1713,13 @@ \subsubsection{Step 8b} spatialdb/mat_initial_stress_grav-crust.spatialdb \end{cfg} +We run the sub-problem by typing: +\begin{shell} +$$ pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +\end{shell} +This simulation will produce files in the \filename{output} directory +analogous to Step 8a. + When we compare the resulting elastic displacements with those of Step 8a, we find that there is essentially no displacement, as seen in Figure \ref{fig:example:subduction:3d:step08b}. From 8004fcd81268a550e038f10d34176c5deefae479 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Mon, 21 Aug 2017 16:50:42 -0700 Subject: [PATCH 194/216] Fixed wording. --- doc/userguide/examples/subduction3d.tex | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 602210677f..e2e930e74f 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -1548,8 +1548,8 @@ \subsubsection{Exercises} \item If you analyze the predicted slip distribution you will find some negative slip, which is unrealistic. To overcome this problem you could try NNLS (non-negative least squares). If you have the - scipy package installed on your computer, you could replace the - generalized inverse solution with the NNLS package included in + Python scipy package installed on your computer, you could replace + the generalized inverse solution with the NNLS package included in \filename{scipy.optimize.nnls}. \end{itemize} \end{itemize} From ca229eaf1abfa6ddf4946997da4484421a5609e4 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 23 Aug 2017 13:44:35 -0700 Subject: [PATCH 195/216] Fixed typo in name of fault output file. --- examples/3d/subduction/step04.cfg | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/examples/3d/subduction/step04.cfg b/examples/3d/subduction/step04.cfg index b5fb19b2f5..3a11aa79cb 100644 --- a/examples/3d/subduction/step04.cfg +++ b/examples/3d/subduction/step04.cfg @@ -230,7 +230,7 @@ slip_time.data = [0.0*year] ; Relative to the origin time # Output [pylithapp.problem.interfaces.splay.output] writer = pylith.meshio.DataWriterHDF5 -writer.filename = output/step04-fault-slabtop.h5 +writer.filename = output/step04-fault-splay.h5 vertex_info_fields = [normal_dir, strike_dir, dip_dir] # ---------------------------------------------------------------------- From 10feea29caf8a346dd0e887e6dc6011793747f65 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 23 Aug 2017 14:24:56 -0700 Subject: [PATCH 196/216] List HDF5/Xdmf output files for examples/3d/subduction examples. --- doc/userguide/examples/subduction3d.tex | 149 +++++++++++++++++++++--- 1 file changed, 136 insertions(+), 13 deletions(-) diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index e2e930e74f..96ad8c52b6 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -703,12 +703,28 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} \begin{shell} $$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} -The simulation will produce twelve pairs of HDF5/Xdmf files, beginning -with \filename{step02}, in the \filename{output} directory. In -addition to the ten pairs of HDF5/Xdmf files analogous to those +In addition to the ten pairs of HDF5/Xdmf files analogous to those produced in Step 1, we also have two pairs of HDF5/Xdmf files associated with the fault: \begin{description} +% Domain and subdomain output +\item[\filename{step02-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step02-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +% Materials +\item[\filename{step02-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step02-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step02-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step02-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step02-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step02-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step02-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step02-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. % Fault \item[\filename{step02-fault-slab\_info.h5[.xmf]}] Fault orientation and rupture information. @@ -912,7 +928,37 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} \end{shell} The simulation will produce fourteen pairs of HDF5/Xdmf files, beginning with \filename{step03}, in the \filename{output} -directory. As in Step 2, there are two pairs of HDF5/Xdmf files for +directory: +\begin{description} +% Domain and subdomain output +\item[\filename{step03-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step03-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +% Materials +\item[\filename{step03-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step03-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step03-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step03-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step03-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step03-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step03-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step03-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. +% Fault +\item[\filename{step03-fault-slabbot\_info.h5[.xmf]}] Fault orientation + and rupture information for the bottom of the slab. +\item[\filename{step03-fault-slabbot.h5[.xmf]}] Time series of slip and + traction changes for the bottom of the slab. +\item[\filename{step03-fault-slabtop\_info.h5[.xmf]}] Fault orientation + and rupture information for the top of the slab. +\item[\filename{step03-fault-slabtop.h5[.xmf]}] Time series of slip and + traction changes for the top of the slab. +\end{description} +As in Step 2, there are two pairs of HDF5/Xdmf files for each fault; one set for the fault orientation and rupture information and one set for the time series of slip and change in tractions. @@ -1094,9 +1140,40 @@ \subsection{Step 4: Prescribed Earthquake Cycle} \end{shell} The simulation will produce sixteen pairs of HDF5/Xdmf files, beginning with \filename{step04}, in the \filename{output} -directory. The output includes the solution over the domain and ground -surface, the properties and state variables for each material, and the -the fault orientation and rupture information for each fault. +directory: +\begin{description} +% Domain and subdomain output +\item[\filename{step04-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step04-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +% Materials +\item[\filename{step04-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step04-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step04-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step04-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step04-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step04-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step04-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step04-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. +% Fault +\item[\filename{step04-fault-slabbot\_info.h5[.xmf]}] Fault orientation + and rupture information for the bottom of the slab. +\item[\filename{step04-fault-slabbot.h5[.xmf]}] Time series of slip and + traction changes for the bottom of the slab. +\item[\filename{step04-fault-slabtop\_info.h5[.xmf]}] Fault orientation + and rupture information for the top of the slab. +\item[\filename{step04-fault-slabtop.h5[.xmf]}] Time series of slip and + traction changes for the top of the slab. +\item[\filename{step04-fault-splay\_info.h5[.xmf]}] Fault orientation + and rupture information for the splay fault. +\item[\filename{step04-fault-splay.h5[.xmf]}] Time series of slip and + traction changes for the splay fault. +\end{description} Figure \ref{fig:example:subduction:3d:step04}, which was created using the ParaView Python script \filename{plot\_dispwarp.py}, shows @@ -1283,8 +1360,34 @@ \subsection{Step 6: Prescribed Slow-Slip Event} $$ cd .. $$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} -The problem will produce thirteen pairs of HDF5/Xdmf files. The additional -HDF5 file that was not present in previous examples is +The problem will produce thirteen pairs of HDF5/Xdmf files: +\begin{description} +% Domain and subdomain output +\item[\filename{step06-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step06-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +\item[\filename{step06-cgps\_sites.h5[.xmf]}] Time series of the solution field at the cGPS sites. +% Materials +\item[\filename{step06-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step06-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step06-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step06-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step06-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step06-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step06-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step06-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. +% Fault +\item[\filename{step06-fault-slab\_info.h5[.xmf]}] Fault orientation + and rupture information for the top of the slab. +\item[\filename{step06-fault-slab.h5[.xmf]}] Time series of slip and + traction changes for the top of the slab. +\end{description} +The additional HDF5 file that was not present in previous examples is \filename{step06-cgps\_sites.h5}, which contains the displacements at the fake cGPS sites. @@ -1635,10 +1738,27 @@ \subsubsection{Step 08a} $$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} The simulation will generate ten pairs of HDF5/Xdmf files beginning -with \filename{step08a}. Two pairs of files include the solution over -the domain and ground surface. For each material the \filename{info} -pair of files contains the properties and the other pair of files -pairs of files contains the state variables. +with \filename{step08a}: +\begin{description} +% Domain and subdomain output +\item[\filename{step08a-domain.h5[.xmf]}] Time series of the solution field over the domain. +\item[\filename{step08a-groundsurf.h5[.xmf]}] Time series of the solution field over the ground surface. +% Materials +\item[\filename{step08a-slab\_info.h5[.xmf]}] Properties for + the slab material. +\item[\filename{step08a-slab.h5[.xmf]}] Time series of the state variables (stress and strain) for the slab material. +\item[\filename{step08a-wedge\_info.h5[.xmf]}] Properties for + the wedge material. +\item[\filename{step08a-wedge.h5[.xmf]}] Time series of the state variables (stress and strain) for the wedge material. +\item[\filename{step08a-crust\_info.h5[.xmf]}] Properties for + the crust material. +\item[\filename{step08a-crust.h5[.xmf]}] Time series of the tate variables + (stress and strain) for the crust material. +\item[\filename{step08a-mantle\_info.h5[.xmf]}] Properties for + the mantle material. +\item[\filename{step08a-mantle.h5[.xmf]}] Time series of the state variables + (stress and strain) for the mantle material. +\end{description} When the problem has run, we see deformation that is consistent with the mismatched densities. The slab subsides while the crust undergoes @@ -1772,6 +1892,9 @@ \subsubsection{Step 8c} \begin{shell} $$ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg \end{shell} +This simulation will produce files in the \filename{output} directory +analogous to Steps 8a and 8b. + The resulting deformation is shown in Figure \ref{fig:example:subduction:3d:step08c}. As a result of viscous flow, the vertical deformation is even larger than that for Step 8a. If we From b0ee0dadbdbb2946b13b3542a3ee0cd2f164bf14 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Wed, 23 Aug 2017 14:25:15 -0700 Subject: [PATCH 197/216] Set version number to 2.2.1 (remove rc1). --- configure.ac | 2 +- doc/userguide/userguide.tex | 2 +- pylith/__init__.py | 2 +- 3 files changed, 3 insertions(+), 3 deletions(-) diff --git a/configure.ac b/configure.ac index 5dbfc71513..4e60506ffd 100644 --- a/configure.ac +++ b/configure.ac @@ -17,7 +17,7 @@ # Process this file with autoconf to produce a configure script. AC_PREREQ(2.59) -AC_INIT([PyLith], [2.2.1rc1], [cig-short@geodynamics.org]) +AC_INIT([PyLith], [2.2.1], [cig-short@geodynamics.org]) AC_CONFIG_AUX_DIR([./aux-config]) AC_CONFIG_HEADER([portinfo]) AC_CONFIG_MACRO_DIR([m4]) diff --git a/doc/userguide/userguide.tex b/doc/userguide/userguide.tex index 88908349c3..1eb84427f1 100644 --- a/doc/userguide/userguide.tex +++ b/doc/userguide/userguide.tex @@ -29,7 +29,7 @@ \newcommand{\rlabel}[1]{\rotatebox[origin=l]{90}{#1}} -\renewcommand{\pylithVersionNumber}{2.2.1rc1} +\renewcommand{\pylithVersionNumber}{2.2.1} \renewcommand{\pylithDOI}{10.5281/zenodo.XXXXXX} % Update install/install.tex (version number within verbatim environment) diff --git a/pylith/__init__.py b/pylith/__init__.py index 36dccfa7f7..ca6db8aaff 100644 --- a/pylith/__init__.py +++ b/pylith/__init__.py @@ -20,7 +20,7 @@ ## @brief Python top-level PyLith module initialization -__version__ = "2.2.0" +__version__ = "2.2.1" __all__ = ['apps', 'bc', From cdbd2abf265913ac3043e3ca797810e813c38c3e Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 24 Aug 2017 11:35:07 -0700 Subject: [PATCH 198/216] Added overview of examples. --- doc/userguide/examples/examples.tex | 37 ++++++++++++++++++++++------- 1 file changed, 29 insertions(+), 8 deletions(-) diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index f596f70ba2..295588e66c 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -3,9 +3,34 @@ \chapter{Examples} \section{Overview} -Each example is a self-contained lesson in how to use PyLith. The -examples increase in degree of complexity from one to the next. - +This chapter includes several suites of examples. Each suite includes +several ``steps'' which are examples that increase in complexity from +one ``step'' to the next. In some cases, a later step may make use of +output from an earlier step; these cases are clearly +documented. Table~\ref{tab:examples:overview} classifies the level of +difficulty of each example suite and provides a general description of +the type of problems discussed. + +\begin{table}[htbp] +\caption{Overview of example suites.} +\label{tab:examples:overview} +\begin{tabular}{lccp{4in}} +\textbf{Directory} & \textbf{Section(s)} & \textbf{Difficulty} & \textbf{Description} \\ +\hline +\filename{twocells} & \ref{sec:example:twotri3}--\ref{sec:examples:twotet4-geoproj} & novice & Toy problems with ASCII two-cell meshes. \\ +\filename{3d/hex8} & \ref{sec:example:3dhex8} & beginner & Illustration of most features using simple CUBIT box mesh. \\ +\filename{3d/tet4} & \ref{sec:example:3dtet4} & beginner & Illustration of refinement using simple LaGriT box mesh. \\ +\filename{bar\_shearwave} & \ref{sec:example:shearwave:tri3}--\ref{sec:example:shearwave:hex8} & beginner & Illustration of wave propagation using simple shear beam. \\ +\filename{2d/subduction} & \ref{sec:example:subduction:2d} & intermediate & Illustration of coseismic, postseismic, and creep deformation using a 2-D subduction zone cross-section with a CUBIT mesh. \\ +\filename{2d/greensfns} & \ref{sec:example:greensfns2d} & intermediate & Illustration of computing static Green's functions for a strike-slip and reverse fault using a CUBIT mesh. \\ +\filename{3d/subduction} & \ref{sec:example:subduction:3d} & intermediate & Illustration of most PyLith features for quasi-static deformation using a 3-D subduction zone with a CUBIT mesh. \\ +\hline +\end{tabular} +The \filename{3d/subduction} example suite is the newest and most +comprehensive. Users wanting to use PyLith in their research should +work through relevant beginner examples and then the +\filename{3d/subduction} examples. +\end{table} \subsection{Prerequisites} @@ -26,7 +51,7 @@ \subsection{Prerequisites} for which you do not have the proper software packages installed. -\subsubsection{Input Files} +\subsection{Input Files} The files needed to work through the examples are found in the \filename{examples} directory under the top-level PyLith @@ -39,10 +64,6 @@ \subsubsection{Input Files} mesh generation software to create the meshes. All of the files used in the example problems are extensively documented with comments. -\subsection{Organization of Examples} - -\todo{brad}{ADD STUFF HERE} - \section{ParaView Python Scripts} \label{sec:ParaView:Python:scripts} \newfeature{v2.2.1} From 92a8f8eda7dce3aba0de16f2008495cf3a75fa74 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 24 Aug 2017 11:52:12 -0700 Subject: [PATCH 199/216] Updated list of changes for v2.2.1. --- CHANGES | 36 ++++++++++++++++++++++++---- doc/releasenotes/announce_v2.2.1.txt | 36 ++++++++++++++++++++++++---- 2 files changed, 62 insertions(+), 10 deletions(-) diff --git a/CHANGES b/CHANGES index a4584d4713..2808eee6c3 100644 --- a/CHANGES +++ b/CHANGES @@ -15,14 +15,40 @@ Version 2.2.1 * Added new examples. - examples/3d/subduction: New suite of examples for a 3-D - subduction zone. + subduction zone. This intermediate level suite of examples + illustrates a wide range of PyLith features for quasi-static simulations. - - examples/2d/subduction: Added spontaneous rupture examples for - slip-weakening and rate- and state-friction. + - examples/2d/subduction: Added quasi-static spontaneous rupture + earthquake cycle examples for slip-weakening and rate- and + state-friction. -* Fixed bug in generating Xdmf files for 2-D vector output. + - These new examples make use of ParaView Python scripts to + facilitate using ParaView with PyLith. -* Updated PETSc to v3.7.6. +* Improved the PyLith manual + + - Added diagram to guide users on which installation method best + meets their needs. + + - Added instructions for how to use the Windows Subsystem for + Linux to install the PyLith Linux binary on systems running + Windows 10. + +* Fixed bug in generating Xdmf files for 2-D vector output. Converted + Xdmf generator from C++ to Python for more robust generation of Xdmf + files from Python scripts. + +* Updated spatialdata to v1.9.10. Improved error messages when reading + SimpleDB and SimpleGridDB files. + +* Updated PyLith parameter viewer to v1.0.1. Small fix to insure + hierarchy path listed matches the one for PyLith. + +* Updated PETSc to v3.7.6. See the PETSc documentation for a summary + of all of the changes. + +* Switched to using CentOS 6.9 for Linux binary builds to insure + compatibility with glibc 2.12 and later. ---------------------------------------------------------------------- Version 2.2.0 diff --git a/doc/releasenotes/announce_v2.2.1.txt b/doc/releasenotes/announce_v2.2.1.txt index c2d5b03968..400150e200 100644 --- a/doc/releasenotes/announce_v2.2.1.txt +++ b/doc/releasenotes/announce_v2.2.1.txt @@ -31,14 +31,40 @@ RELEASE NOTES * Added new examples. - examples/3d/subduction: New suite of examples for a 3-D - subduction zone. + subduction zone. This intermediate level suite of examples + illustrates a wide range of PyLith features for quasi-static simulations. - - examples/2d/subduction: Added spontaneous rupture examples for - slip-weakening and rate- and state-friction. + - examples/2d/subduction: Added quasi-static spontaneous rupture + earthquake cycle examples for slip-weakening and rate- and + state-friction. -* Fixed bug in generating Xdmf files for 2-D vector output. + - These new examples make use of ParaView Python scripts to + facilitate using ParaView with PyLith. -* Updated PETSc to v3.7.6. +* Improved the PyLith manual + + - Added diagram to guide users on which installation method best + meets their needs. + + - Added instructions for how to use the Windows Subsystem for + Linux to install the PyLith Linux binary on systems running + Windows 10. + +* Fixed bug in generating Xdmf files for 2-D vector output. Converted + Xdmf generator from C++ to Python for more robust generation of Xdmf + files from Python scripts. + +* Updated spatialdata to v1.9.10. Improved error messages when reading + SimpleDB and SimpleGridDB files. + +* Updated PyLith parameter viewer to v1.0.1. Small fix to insure + hierarchy path listed matches the one for PyLith. + +* Updated PETSc to v3.7.6. See the PETSc documentation for a summary + of all of the changes. + +* Switched to using CentOS 6.9 for Linux binary builds to insure + compatibility with glibc 2.12 and later. See CHANGES in the top-level source directory for a list of changes for each prior release. From e443102029fd392c0ff85ccdb25528873d7ed072 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 24 Aug 2017 11:55:22 -0700 Subject: [PATCH 200/216] Updated list of changes for v2.2.1. --- doc/userguide/intro/intro.tex | 47 +++++++++++++++++++++-------------- 1 file changed, 28 insertions(+), 19 deletions(-) diff --git a/doc/userguide/intro/intro.tex b/doc/userguide/intro/intro.tex index 7b160afbd9..7548b0e2d2 100644 --- a/doc/userguide/intro/intro.tex +++ b/doc/userguide/intro/intro.tex @@ -12,27 +12,36 @@ \section{Overview} \section{New in PyLith Version \pylithVersionNumber} \begin{itemize} -\item Added a browser-based parameter viewer for interactive viewing - of all PyLith parameters and version information. See Section - \ref{sec:pylith:parameter:viewer}. -\item Converted the user manual from Lyx to LaTeX and added syntax - highlighting of parameter and spatial database files. Fixed several - typos. -\item Fixed bug that sometimes resulted in an inconsistent fault - orientation when running in parallel. The bug appears to have been - introduced in v2.0. -\item Fixed two bugs in output of solution at points that sometimes - happened in parallel simulations. The errors include: +\item Added new examples \begin{itemize} - \item The order of the station names does not match the order of the - points. The point data is written in parallel by process order, so - the points for process 0 are written first, then those for process - 1, etc. This often results in reordering of the points. The - station names were written in the original order. - \item The output values for some points are incorrect. The wrong - cells were being used in the interpolation. + \item \filename{examples/3d/subduction}: New suite of examples for a 3-D + subduction zone. This intermediate level suite of examples + illustrates a wide range of PyLith features for quasi-static simulations. + \item \filename{examples/2d/subduction}: Added quasi-static spontaneous rupture + earthquake cycle examples for slip-weakening and rate- and + state-friction. + \item These new examples make use of ParaView Python scripts to + facilitate using ParaView with PyLith. \end{itemize} -\item Updated PETSc to v3.7.5. +\item Improved the PyLith manual + \begin{itemize} + \item Added diagram to guide users on which installation method best + meets their needs. + \item Added instructions for how to use the Windows Subsystem for + Linux to install the PyLith Linux binary on systems running + Windows 10. + \end{itemize} +\item Fixed bug in generating Xdmf files for 2-D vector + output. Converted Xdmf generator from C++ to Python for more robust + generation of Xdmf files from Python scripts. +\item Updated spatialdata to v1.9.10. Improved error messages when + reading SimpleDB and SimpleGridDB files. +\item Updated PyLith parameter viewer to v1.0.1. Small fix to insure + hierarchy path listed matches the one for PyLith. +\item Updated PETSc to v3.7.6. See the PETSc documentation for a + summary of all of the changes. +\item Switched to using CentOS 6.9 for Linux binary builds to insure + compatibility with glibc 2.12 and later. \end{itemize} The \filename{CHANGES} file in the top-level source directory contains a summary of features and bugfixes for each release. From 4fd129380ac4b2374f38ca4044dc799f8630b62f Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 24 Aug 2017 20:03:37 -0700 Subject: [PATCH 201/216] Convert slip inversion from using PETSc to PyLith Xdmf generator. --- examples/3d/subduction/slip_invert.py | 88 ++++++++++----------------- 1 file changed, 32 insertions(+), 56 deletions(-) diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index b0c1fa5982..a74fadd0f0 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -70,42 +70,34 @@ class SlipInvert(Application): rake = pyre.inventory.dimensional("rake", default=90.0*degree) rake.meta['tip'] = "Assumed rake angle." - gfImpulsesLlFile = pyre.inventory.str("gfimpulses_ll_file", - default="gfimpulse_ll.h5") + gfImpulsesLlFile = pyre.inventory.str("gfimpulses_ll_file", default="gfimpulse_ll.h5") gfImpulsesLlFile.meta['tip'] = "HDF5 file with left-lateral GF impulses." - gfImpulsesUdFile = pyre.inventory.str("gfimpulses_ud_file", - default="gfimpulse_ud.h5") + gfImpulsesUdFile = pyre.inventory.str("gfimpulses_ud_file", default="gfimpulse_ud.h5") gfImpulsesUdFile.meta['tip'] = "HDF5 file with updip GF impulses." - gfResponsesLlFile = pyre.inventory.str("gfresponses_ll_file", - default="gfresponse_ll.h5") + gfResponsesLlFile = pyre.inventory.str("gfresponses_ll_file", default="gfresponse_ll.h5") gfResponsesLlFile.meta['tip'] = "HDF5 file with left-lateral GF responses." - gfResponsesUdFile = pyre.inventory.str("gfresponses_ud_file", - default="gfresponse_ud.h5") + gfResponsesUdFile = pyre.inventory.str("gfresponses_ud_file", default="gfresponse_ud.h5") gfResponsesUdFile.meta['tip'] = "HDF5 file with updip GF responses." aPrioriValue = pyre.inventory.float("a_priori_value", default=0.0) aPrioriValue.meta['tip'] = "A priori value for parameters." - penaltyWeightVals = pyre.inventory.list("penalty_weight_vals", - default=[0.1,0.5,1.0,5.0,10.0]) + penaltyWeightVals = pyre.inventory.list("penalty_weight_vals", default=[0.1,0.5,1.0,5.0,10.0]) penaltyWeightVals.meta['tip'] = "List of penalty weights." dataScale = pyre.inventory.float("data_scale", default=1.0) dataScale.meta['tip'] = "Scaling factor to apply to data and stdDev." - resultSummaryFile = pyre.inventory.str("result_summary_file", - default='result_summary.txt') + resultSummaryFile = pyre.inventory.str("result_summary_file", default='result_summary.txt') resultSummaryFile.meta['tip'] = "Text file summarizing inversion results." - slipOutputFile = pyre.inventory.str("slip_output_file", - default='predicted_slip.h5') + slipOutputFile = pyre.inventory.str("slip_output_file", default='predicted_slip.h5') slipOutputFile.meta['tip'] = "HDF5 file with predicted slip results." - displacementOutputFile = pyre.inventory.str("displacement_output_file", - default='predicted_displacement.h5') + displacementOutputFile = pyre.inventory.str("displacement_output_file", default='predicted_displacement.h5') displacementOutputFile.meta['tip'] = "HDF5 file with predicted displacements." @@ -142,8 +134,6 @@ def __init__(self, name="slip_invert"): def main(self): - # import pdb - # pdb.set_trace() self.readData() self.readGreens() self.runInversions() @@ -157,16 +147,13 @@ def _configure(self): Setup members using inventory. """ Application._configure(self) - self.penaltyWeights = numpy.array(self.penaltyWeightVals, - dtype=numpy.float64) + self.penaltyWeights = numpy.array(self.penaltyWeightVals, dtype=numpy.float64) self.numPenaltyWeights = self.penaltyWeights.shape[0] # Left-lateral and updip components from assumed rake. self.llComp = math.cos(self.rake.value) self.udComp = math.sin(self.rake.value) - self.genXdmfCmd = "petsc_gen_xdmf.py " - return @@ -182,37 +169,29 @@ def runInversions(self): s = h5py.File(self.slipOutputFile, 'w') # Write fault mesh and time info. - summaryInfo = numpy.zeros((self.numPenaltyWeights, self.numSummaryCols), - dtype=numpy.float64) + summaryInfo = numpy.zeros((self.numPenaltyWeights, self.numSummaryCols), dtype=numpy.float64) cellDimF = 2 timesF = self.penaltyWeights.reshape(self.numPenaltyWeights, 1, 1) vertsF = s.create_dataset('geometry/vertices', data=self.faultVertCoords) timesF = s.create_dataset('time', data=timesF, maxshape=(None, 1, 1)) topoF = s.create_dataset('topology/cells', data=self.faultCells, dtype='d') topoF.attrs['cell_dim'] = numpy.int32(cellDimF) - totSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), - dtype=numpy.float64) - llSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), - dtype=numpy.float64) - udSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts), - dtype=numpy.float64) + totSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) + llSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) + udSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) # Write data mesh and time info. - cellDimD = 1 - topolD = numpy.arange(self.numDataPoints, - dtype=numpy.int64).reshape(self.numDataPoints, 1) + cellDimD = 0 + topolD = numpy.arange(self.numDataPoints, dtype=numpy.int64).reshape(self.numDataPoints, 1) timesD = self.penaltyWeights.reshape(self.numPenaltyWeights, 1, 1) vertsD = d.create_dataset('geometry/vertices', data=self.dataCoords) timesD = d.create_dataset('time', data=timesD, maxshape=(None, 1, 1)) topoD = d.create_dataset('topology/cells', data=topolD, dtype='d') topoD.attrs['cell_dim'] = numpy.int32(cellDimD) - dispEast = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), - dtype=numpy.float64) - dispNorth = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), - dtype=numpy.float64) - dispUp = numpy.zeros((self.numPenaltyWeights, self.numDataPoints), - dtype=numpy.float64) + dispEast = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) + dispNorth = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) + dispUp = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) # Indices of displacement components in solution vector. eastBegin = 0 @@ -229,8 +208,7 @@ def runInversions(self): dataScaledVals = numpy.dot(dataStdDevInvDiag, self.dataVals) # Create a priori parameter vector. - paramVec = self.aPrioriValue * numpy.ones(self.numImpulses, - dtype=numpy.float64) + paramVec = self.aPrioriValue * numpy.ones(self.numImpulses, dtype=numpy.float64) summFmt = '%g' + 6 * '\t%e' + '\n' @@ -240,16 +218,14 @@ def runInversions(self): # Loop over inversions. for invNum in range(self.numPenaltyWeights): penWeight = self.penaltyWeights[invNum] - print ' Working on inversion %d, penalty weight = %g' % (invNum, - penWeight) + print ' Working on inversion %d, penalty weight = %g' % (invNum, penWeight) sys.stdout.flush() paramScaledDesign = penWeight * regArray paramScaledData = penWeight * paramVec designMat = numpy.vstack((dataScaledDesign, paramScaledDesign)) dataVec = numpy.hstack((dataScaledVals, paramScaledData)) designMatTrans = numpy.transpose(designMat) - genInv = numpy.dot(numpy.linalg.inv(numpy.dot(designMatTrans, designMat)), - designMatTrans) + genInv = numpy.dot(numpy.linalg.inv(numpy.dot(designMatTrans, designMat)), designMatTrans) solution = numpy.dot(genInv, dataVec) # Compute residuals, etc. @@ -264,8 +240,7 @@ def runInversions(self): penaltyResidualNorm = numpy.linalg.norm(penaltyResidual) penaltyWeightResidualNorm = numpy.linalg.norm(penaltyWeightResidual) totalResidualNorm = dataResidualNorm + penaltyResidualNorm - totalWeightResidualNorm = dataWeightResidualNorm + \ - penaltyWeightResidualNorm + totalWeightResidualNorm = dataWeightResidualNorm + penaltyWeightResidualNorm summaryInfo[invNum,0] = penWeight summaryInfo[invNum,1] = dataResidualNorm @@ -275,12 +250,12 @@ def runInversions(self): summaryInfo[invNum,5] = totalResidualNorm summaryInfo[invNum,6] = totalWeightResidualNorm - totSlip[invNum, self.impulseInds] = solution - llSlip[invNum, self.impulseInds] = self.llComp * solution - udSlip[invNum, self.impulseInds] = self.udComp * solution - dispEast[invNum, :] = predicted[eastBegin:eastEnd] - dispNorth[invNum, :] = predicted[northBegin:northEnd] - dispUp[invNum, :] = predicted[upBegin:upEnd] + totSlip[invNum, self.impulseInds, 0] = solution + llSlip[invNum, self.impulseInds, 0] = self.llComp * solution + udSlip[invNum, self.impulseInds, 0] = self.udComp * solution + dispEast[invNum, :, 0] = predicted[eastBegin:eastEnd] + dispNorth[invNum, :, 0] = predicted[northBegin:northEnd] + dispUp[invNum, :, 0] = predicted[upBegin:upEnd] print ' Data residual: %e' % dataResidualNorm print ' Weighted data residual: %e' % dataWeightResidualNorm @@ -310,9 +285,10 @@ def runInversions(self): s.close() d.close() - os.system(self.genXdmfCmd + self.slipOutputFile) - os.system(self.genXdmfCmd + self.displacementOutputFile) - + from pylith.meshio.Xdmf import Xdmf + xdmfWriter = Xdmf() + xdmfWriter.write(self.slipOutputFile) + xdmfWriter.write(self.displacementOutputFile) return From 1677068ed0a3ac3d92a9507dad69fa04bfb1b8dd Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 25 Aug 2017 10:45:12 -0700 Subject: [PATCH 202/216] Added tip on using trace for ParaView Python scripts. --- doc/userguide/examples/examples.tex | 9 +++++++++ 1 file changed, 9 insertions(+) diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 295588e66c..339b27eff8 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -110,6 +110,15 @@ \section{ParaView Python Scripts} general, import Python modules provided with the PyLith distribution into ParaView.} +\tip{In creating the ParaView Python scripts, we performed the steps + within the GUI while capturing the commands using + \menu{Tools}$\rightarrow$\menu{Start Trace} and then + \menu{Tools}$\rightarrow$\menu{Start Trace}. This makes it very easy + to create the Python script. Note that we have omitted supefluous + commands in the trace when transferring the trace into a Python + script. See the ParaView documentation for additional information + about the Python API.} + \subsection{Overriding Default Parameters} We setup the ParaView Python scripts, so that when they are run from From 204225bb2a9e84d3715d83a43ab00e2fbf0f14fa Mon Sep 17 00:00:00 2001 From: Charles Williams Date: Mon, 28 Aug 2017 11:26:11 +1200 Subject: [PATCH 203/216] Updated script to use vectors rather than scalar components. --- examples/3d/subduction/slip_invert.py | 51 ++++++++++----------------- 1 file changed, 18 insertions(+), 33 deletions(-) diff --git a/examples/3d/subduction/slip_invert.py b/examples/3d/subduction/slip_invert.py index a74fadd0f0..9d4d5e10b7 100755 --- a/examples/3d/subduction/slip_invert.py +++ b/examples/3d/subduction/slip_invert.py @@ -169,16 +169,18 @@ def runInversions(self): s = h5py.File(self.slipOutputFile, 'w') # Write fault mesh and time info. - summaryInfo = numpy.zeros((self.numPenaltyWeights, self.numSummaryCols), dtype=numpy.float64) + summaryInfo = numpy.zeros((self.numPenaltyWeights, self.numSummaryCols), + dtype=numpy.float64) cellDimF = 2 timesF = self.penaltyWeights.reshape(self.numPenaltyWeights, 1, 1) vertsF = s.create_dataset('geometry/vertices', data=self.faultVertCoords) timesF = s.create_dataset('time', data=timesF, maxshape=(None, 1, 1)) topoF = s.create_dataset('topology/cells', data=self.faultCells, dtype='d') topoF.attrs['cell_dim'] = numpy.int32(cellDimF) - totSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) - llSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) - udSlip = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), dtype=numpy.float64) + slipVec = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 3), + dtype=numpy.float64) + slipAlongRake = numpy.zeros((self.numPenaltyWeights, self.numFaultVerts, 1), + dtype=numpy.float64) # Write data mesh and time info. cellDimD = 0 @@ -189,17 +191,7 @@ def runInversions(self): topoD = d.create_dataset('topology/cells', data=topolD, dtype='d') topoD.attrs['cell_dim'] = numpy.int32(cellDimD) - dispEast = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) - dispNorth = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) - dispUp = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 1), dtype=numpy.float64) - - # Indices of displacement components in solution vector. - eastBegin = 0 - eastEnd = self.numDataPoints - northBegin = eastEnd - northEnd = northBegin + self.numDataPoints - upBegin = northEnd - upEnd = northEnd + self.numDataPoints + predictedDisp = numpy.zeros((self.numPenaltyWeights, self.numDataPoints, 3), dtype=numpy.float64) # Rescale equations using data standard deviations. dataStdDev = numpy.sqrt(self.dataCov) @@ -250,12 +242,11 @@ def runInversions(self): summaryInfo[invNum,5] = totalResidualNorm summaryInfo[invNum,6] = totalWeightResidualNorm - totSlip[invNum, self.impulseInds, 0] = solution - llSlip[invNum, self.impulseInds, 0] = self.llComp * solution - udSlip[invNum, self.impulseInds, 0] = self.udComp * solution - dispEast[invNum, :, 0] = predicted[eastBegin:eastEnd] - dispNorth[invNum, :, 0] = predicted[northBegin:northEnd] - dispUp[invNum, :, 0] = predicted[upBegin:upEnd] + slipAlongRake[invNum, self.impulseInds, 0] = solution + slipVec[invNum, self.impulseInds, 0] = self.llComp * solution + slipVec[invNum, self.impulseInds, 1] = self.udComp * solution + predictedDisp[invNum, :, :] = predicted.reshape(self.numDataPoints, 3, + order='F') print ' Data residual: %e' % dataResidualNorm print ' Weighted data residual: %e' % dataWeightResidualNorm @@ -269,18 +260,12 @@ def runInversions(self): header=self.summaryHead) # Write results to HDF5 files. - slipTot = s.create_dataset('vertex_fields/total_slip', data=totSlip) - slipTot.attrs['vector_field_type'] = 'scalar' - slipLl = s.create_dataset('vertex_fields/leftlat_slip', data=llSlip) - slipLl.attrs['vector_field_type'] = 'scalar' - slipUd = s.create_dataset('vertex_fields/updip_slip', data=udSlip) - slipUd.attrs['vector_field_type'] = 'scalar' - eastDisp = d.create_dataset('vertex_fields/disp_east', data=dispEast) - eastDisp.attrs['vector_field_type'] = 'scalar' - northDisp = d.create_dataset('vertex_fields/disp_north', data=dispNorth) - northDisp.attrs['vector_field_type'] = 'scalar' - upDisp = d.create_dataset('vertex_fields/disp_ups', data=dispUp) - upDisp.attrs['vector_field_type'] = 'scalar' + rakeSlip = s.create_dataset('vertex_fields/rake_slip', data=slipAlongRake) + rakeSlip.attrs['vector_field_type'] = 'scalar' + vecSlip = s.create_dataset('vertex_fields/slip_vector', data=slipVec) + vecSlip.attrs['vector_field_type'] = 'vector' + vecDisp = d.create_dataset('vertex_fields/disp_vec', data=predictedDisp) + vecDisp.attrs['vector_field_type'] = 'vector' s.close() d.close() From 8300b5ccb35949dfdcc44c30a546ddb9da7ed506 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 29 Aug 2017 15:45:47 -0700 Subject: [PATCH 204/216] Added info on CUBIT/Trelis at beginning of examples. --- doc/userguide/examples/examples.tex | 28 +++++++++++++++------------- 1 file changed, 15 insertions(+), 13 deletions(-) diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 339b27eff8..0f924f3cb4 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -36,19 +36,21 @@ \subsection{Prerequisites} Before you begin any of the examples, you will need to install PyLith following the instructions in Chapter~\vref{cha:installation}. For -more complex examples, you will also need either CUBIT -\url{cubit.sandia.gov} or LaGriT \url{meshing.lanl.gov} mesh -generation software to create the meshes. If you do not wish to create -your own mesh at this time, the meshes are also provided as part of -the example. The ParaView \url{www.paraview.org} visualization -package may be used to view simulation results. ParaView 3 includes -built-in documentation that is accessed by clicking on the Help menu -item. Some additional documentation is available on the ParaView Wiki -site \url{paraview.org/Wiki/ParaView}. You may use other -visualization software, but some adaption from what is described here -will be necessary. Furthermore, you can complete a subset of the -example using files provided (as described below), skipping the steps -for which you do not have the proper software packages installed. +more complex examples, you will also need either Trelis (available +from \url{csimsoft.com}), CUBIT (available to US federal government +agencies from \url{cubit.sandia.gov}) or LaGriT (available form +\url{meshing.lanl.gov}) mesh generation software to create the +meshes. If you do not wish to create your own mesh at this time, the +meshes are also provided as part of the example. The ParaView +\url{www.paraview.org} visualization package may be used to view +simulation results. ParaView 3 includes built-in documentation that is +accessed by clicking on the Help menu item. Some additional +documentation is available on the ParaView Wiki site +\url{paraview.org/Wiki/ParaView}. You may use other visualization +software, but some adaption from what is described here will be +necessary. Furthermore, you can complete a subset of the example using +files provided (as described below), skipping the steps for which you +do not have the proper software packages installed. \subsection{Input Files} From 2b6315c1bbb51b7da869be02cec526a4fc009577 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 31 Aug 2017 14:54:58 -0700 Subject: [PATCH 205/216] Add comments on why we need to move files to/from the Docker container. --- doc/userguide/install/install.tex | 12 +++++++++--- 1 file changed, 9 insertions(+), 3 deletions(-) diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index fa728b6918..73a717956e 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -194,7 +194,8 @@ \subsection{Run Unix shell within Docker to use PyLith.} $$ docker run -ti --volumes-from pylith-data geodynamics/pylith \end{shell} -To run the container and allow display of windows on the host computer: +To run the container and allow display of windows on the host computer +(requires that X-Windows be installed): \begin{shell} # Darwin: Allow X connections $$ xhost +YOUR_IP_ADDRESS; DISPLAY=YOUR_IP_ADDRESS:0 @@ -217,7 +218,8 @@ \subsection{Run Unix shell within Docker to use PyLith.} \important{We do not yet include ParaView due to difficulties associated with setting up rendering on the host display outside the - container.} + container. You will need to copy the output files to your host + machine to view them in ParaView as described later.} \subsubsection{Using Docker containers} \begin{itemize} @@ -242,7 +244,11 @@ \subsubsection{Using Docker containers} \subsection{Copy data to/from persistent storage volume.} These commands are run on the local host outside the container, not -inside the Docker container. +inside the Docker container. These commands are used to move files +from your host machine into the PyLith Docker container and vice +versa. For example, you will generate your mesh on the host, copy the +mesh file into the Docker container, run PyLith within the container, +and then copy the output files to the host to display in ParaView. \begin{shell} # Copy data FROM persistent storage volume TO local host From b81f0683c60dba21a6a631c58c3d681349b108e2 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Thu, 31 Aug 2017 15:43:20 -0700 Subject: [PATCH 206/216] Add note on useful values for time step parameter in ParaView Python scripts. --- examples/2d/subduction/viz/plot_dispwarp.py | 2 +- examples/2d/subduction/viz/plot_shearratio.py | 2 +- examples/3d/subduction/viz/plot_dispvec.py | 2 +- examples/3d/subduction/viz/plot_dispwarp.py | 2 +- examples/3d/subduction/viz/plot_faultslip.py | 2 +- 5 files changed, 5 insertions(+), 5 deletions(-) diff --git a/examples/2d/subduction/viz/plot_dispwarp.py b/examples/2d/subduction/viz/plot_dispwarp.py index 698989c067..3bb4ba6ccb 100755 --- a/examples/2d/subduction/viz/plot_dispwarp.py +++ b/examples/2d/subduction/viz/plot_dispwarp.py @@ -35,7 +35,7 @@ "WARP_SCALE": 10.0e+3, "FIELD": "displacement", "FIELD_COMPONENT": "X", - "TIMESTEP": 0, + "TIMESTEP": 0, # Use 0 for first, -1 for last. } # ---------------------------------------------------------------------- diff --git a/examples/2d/subduction/viz/plot_shearratio.py b/examples/2d/subduction/viz/plot_shearratio.py index 3cf1069da9..0d59d8242c 100755 --- a/examples/2d/subduction/viz/plot_shearratio.py +++ b/examples/2d/subduction/viz/plot_shearratio.py @@ -35,7 +35,7 @@ "OUTPUT_DIR": "output", "SIM": "step05", "FAULTS": ["fault-slabtop"], - "TIMESTEP": 0, + "TIMESTEP": 0, # Use 0 for first, -1 for last. } # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/viz/plot_dispvec.py b/examples/3d/subduction/viz/plot_dispvec.py index 593fbaeb04..9cc4759fc5 100755 --- a/examples/3d/subduction/viz/plot_dispvec.py +++ b/examples/3d/subduction/viz/plot_dispvec.py @@ -38,7 +38,7 @@ "VECTOR_SCALE": 10.0e+3, "FIELD": "displacement", "FIELD_COMPONENT": "Magnitude", - "TIMESTEP": 0, + "TIMESTEP": 0, # Use 0 for first, -1 for last. } # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/viz/plot_dispwarp.py b/examples/3d/subduction/viz/plot_dispwarp.py index dbb3be31de..4053b0318c 100755 --- a/examples/3d/subduction/viz/plot_dispwarp.py +++ b/examples/3d/subduction/viz/plot_dispwarp.py @@ -35,7 +35,7 @@ "WARP_SCALE": 10.0e+3, "FIELD": "displacement", "FIELD_COMPONENT": "Magnitude", - "TIMESTEP": 0, + "TIMESTEP": 0, # Use 0 for first, -1 for last. } # ---------------------------------------------------------------------- diff --git a/examples/3d/subduction/viz/plot_faultslip.py b/examples/3d/subduction/viz/plot_faultslip.py index bca229540a..6628d1b287 100755 --- a/examples/3d/subduction/viz/plot_faultslip.py +++ b/examples/3d/subduction/viz/plot_faultslip.py @@ -35,7 +35,7 @@ "OUTPUT_DIR": "output", "SIM": "step02", "FAULTS": ["fault-slab"], - "TIMESTEP": 0, + "TIMESTEP": 0, # Use 0 for first, -1 for last. } # ---------------------------------------------------------------------- From 07f43dd3bd4c7b20c979a4c02553e402cd98812a Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 11:47:53 -0700 Subject: [PATCH 207/216] Improve display of code listings. --- doc/userguide/pylithdoc.cls | 56 ++++++++++++++++++++++++++++++------ doc/userguide/styleguide.tex | 14 +++++++++ 2 files changed, 62 insertions(+), 8 deletions(-) diff --git a/doc/userguide/pylithdoc.cls b/doc/userguide/pylithdoc.cls index f7356c1022..ffd77a4942 100644 --- a/doc/userguide/pylithdoc.cls +++ b/doc/userguide/pylithdoc.cls @@ -17,7 +17,7 @@ % % pylithdoc.cls Style file for PyLith documentation. \NeedsTeXFormat{LaTeX2e}[1994/06/01] -\ProvidesClass{pylithdoc}[2017/02/17 v0.1 PyLith Documentation class] +\ProvidesClass{pylithdoc}[2017/09/01 v0.2 PyLith Documentation class] \ProcessOptions* \LoadClass[10pt,twoside]{book} @@ -198,7 +198,25 @@ % ------------------------------------------------------------------ % Code blocks +% +% Caption +\renewcommand{\lst@makecaption}[2]{% + \if\lst@title\@empty + \else + \vskip\abovecaptionskip% + \begin{tikzpicture} + \node[draw=none, + inner sep=0.3em, + top color=\captioncolor!50, + bottom color=\captioncolor!10, + ]{#1: #2}; + \end{tikzpicture}\par\vspace{-1pt} + \fi +} +% +% % .cfg +% \lstdefinelanguage{cfg}{% basicstyle=\small\ttfamily, frame=tb,% @@ -208,24 +226,46 @@ moredelim=[is][\color{purple}\bfseries]{

      }{

      }, moredelim=[is][\color{blue}\bfseries]{}{}, } -\lstnewenvironment{cfg}{\lstset{language=cfg}}{} +\lstnewenvironment{cfg}[1][\@empty]{% + \def\captioncolor{blue} + \def\@makecaption{\lst@makecaption} + \lstset{% + language=cfg, + title={#1}, + backgroundcolor=\color{\captioncolor!10}, + rulecolor=\color{\captioncolor}, +}}{} % -% shell -\lstnewenvironment{shell}{\lstset{% +% shell +% +\lstnewenvironment{shell}[1][\@empty]{% + \def\captioncolor{green} + \def\@makecaption{\lst@makecaption} + \lstset{% language=bash,% - frame=single,% + frame=tb,% basicstyle=\small\ttfamily,% - morekeywords={$$},% + morekeywords={$},% commentstyle=\itshape\color{orange}, + title={#1}, + backgroundcolor=\color{\captioncolor!10}, + rulecolor=\color{\captioncolor}, }}{} % % python -\lstnewenvironment{python}{\lstset{% +% +\lstnewenvironment{python}[1][\@empty]{% + \def\captioncolor{purple} + \def\@makecaption{\lst@makecaption} + \lstset{% language=python,% - frame=single,% + frame=tb,% basicstyle=\small\ttfamily,% morekeywords={>>>},% commentstyle=\itshape\color{orange}, + title={#1}, + backgroundcolor=\color{\captioncolor!10}, + rulecolor=\color{\captioncolor}, }}{} % ------------------------------------------------------------------ diff --git a/doc/userguide/styleguide.tex b/doc/userguide/styleguide.tex index 4ba79a70dd..d284898832 100644 --- a/doc/userguide/styleguide.tex +++ b/doc/userguide/styleguide.tex @@ -43,6 +43,15 @@ headers, {\tt

      } and {\tt

      } to delimit properties, and {\tt } and {\tt } to delimit facilities. % Example use of cfg environment +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] +# This is a comment. +[pylithapp.problem] +

      timestep

      = 2.0*s ; Time step comment. +bc = [x_pos, x_neg] +\end{cfg} + +Example of \filename{.cfg} environment without title. +% Example use of cfg environment \begin{cfg} # This is a comment. [pylithapp.problem] @@ -61,6 +70,11 @@ \end{inventory} +\begin{python}[ParaView Python shell] +>>> EXODUS_FILE = "/home/johndoe/pylith/examples/3d/subduction/mesh/mesh_tet.exo" +\end{python} + + \section{My Feature} \newfeature{v2.1.4} From aa598fb8e26596318116710dd8685109445fbeab Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 11:48:23 -0700 Subject: [PATCH 208/216] Update code listings. --- doc/userguide/examples/3dhex8.tex | 2 +- doc/userguide/examples/3dhex8_dike.tex | 2 +- doc/userguide/examples/3dhex8_friction.tex | 2 +- doc/userguide/examples/3dhex8_gravity.tex | 2 +- doc/userguide/examples/3dhex8_greensfns.tex | 2 +- doc/userguide/examples/3dhex8_quasistatic.tex | 4 +- doc/userguide/examples/3dhex8_static.tex | 2 +- doc/userguide/examples/3dhex8_surfload.tex | 2 +- doc/userguide/examples/3dtet4.tex | 4 +- doc/userguide/examples/grav2d.tex | 20 ++--- doc/userguide/examples/greensfns2d.tex | 6 +- doc/userguide/examples/shearwave.tex | 14 ++-- doc/userguide/examples/subduction2d.tex | 14 ++-- doc/userguide/examples/subduction3d.tex | 36 ++++---- doc/userguide/examples/twohex8.tex | 6 +- doc/userguide/examples/twoquad4.tex | 8 +- doc/userguide/examples/twotet4-geoproj.tex | 2 +- doc/userguide/examples/twotet4.tex | 4 +- doc/userguide/install/install.tex | 83 +++++++++++-------- doc/userguide/preface.tex | 7 +- doc/userguide/runpylith/databases.tex | 30 +++---- doc/userguide/runpylith/definesim.tex | 47 +++++------ doc/userguide/runpylith/formulation.tex | 36 ++++---- doc/userguide/runpylith/output.tex | 24 +++--- doc/userguide/runpylith/parametersgui.tex | 18 ++-- doc/userguide/runpylith/postprocessing.tex | 4 +- doc/userguide/runpylith/tips.tex | 6 +- 27 files changed, 197 insertions(+), 190 deletions(-) diff --git a/doc/userguide/examples/3dhex8.tex b/doc/userguide/examples/3dhex8.tex index 95039c704a..d1d89e0647 100644 --- a/doc/userguide/examples/3dhex8.tex +++ b/doc/userguide/examples/3dhex8.tex @@ -97,7 +97,7 @@ \subsection{Mesh Generation and Description} If you have the \filename{ncdump} command available, you can see what is in the file by typing: \begin{shell} -$$ ncdump box_hex8_1000m.exo +$ ncdump box_hex8_1000m.exo \end{shell} \begin{figure} diff --git a/doc/userguide/examples/3dhex8_dike.tex b/doc/userguide/examples/3dhex8_dike.tex index 4050bf7acc..dac5faac02 100644 --- a/doc/userguide/examples/3dhex8_dike.tex +++ b/doc/userguide/examples/3dhex8_dike.tex @@ -17,7 +17,7 @@ \subsubsection{Overview} \filename{.cfg} file is \filename{step20.cfg}. The example may be run as follows: \begin{shell} -$$ pylith step20.cfg +$ pylith step20.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in diff --git a/doc/userguide/examples/3dhex8_friction.tex b/doc/userguide/examples/3dhex8_friction.tex index 9d1dd7a7e7..4d2a1e5416 100644 --- a/doc/userguide/examples/3dhex8_friction.tex +++ b/doc/userguide/examples/3dhex8_friction.tex @@ -25,7 +25,7 @@ \subsubsection{Overview} \filename{step11.cfg}, \filename{step12.cfg}, \filename{step13.cfg}, and \filename{step14.cfg}. Each example may be run as follows: \begin{shell} -$$ pylith stepXX.cfg +$ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in diff --git a/doc/userguide/examples/3dhex8_gravity.tex b/doc/userguide/examples/3dhex8_gravity.tex index 3632ebfc97..8428106f94 100644 --- a/doc/userguide/examples/3dhex8_gravity.tex +++ b/doc/userguide/examples/3dhex8_gravity.tex @@ -23,7 +23,7 @@ \subsubsection{Overview} \filename{step16.cfg}, and \filename{step17.cfg}. Each example may be run as follows: \begin{shell} -$$ pylith stepXX.cfg +$ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the diff --git a/doc/userguide/examples/3dhex8_greensfns.tex b/doc/userguide/examples/3dhex8_greensfns.tex index 0b50897780..3b066b9113 100644 --- a/doc/userguide/examples/3dhex8_greensfns.tex +++ b/doc/userguide/examples/3dhex8_greensfns.tex @@ -20,7 +20,7 @@ \subsubsection{Overview} \filename{.cfg} file is \filename{step21.cfg}. The example may be run as follows: \begin{shell} -$$ pylith step21.cfg --problem=pylith.problems.GreensFns +$ pylith step21.cfg --problem=pylith.problems.GreensFns \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg} and \filename{greensfns.cfg}, and then diff --git a/doc/userguide/examples/3dhex8_quasistatic.tex b/doc/userguide/examples/3dhex8_quasistatic.tex index 3ee03bf02f..1042416e7f 100644 --- a/doc/userguide/examples/3dhex8_quasistatic.tex +++ b/doc/userguide/examples/3dhex8_quasistatic.tex @@ -36,7 +36,7 @@ \subsubsection{Overview} \filename{step07.cfg}, \filename{step08.cfg}, and \filename{step09.cfg}. Each example may be run as follows: \begin{shell} -$$ pylith stepXX.cfg +$ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in @@ -558,7 +558,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende utility code can be used by simply executing it from the \filename{examples/3d/hex8/spatialdb/powerlaw} directory: \begin{shell} -$$ powerlaw_gendb.py +$ powerlaw_gendb.py \end{shell} This code will automatically read the parameters in \filename{powerlaw\_gendb.cfg} in creating the file \filename{examples/3d/hex8/spatialdb/mat\_powerlaw.spatialdb}. diff --git a/doc/userguide/examples/3dhex8_static.tex b/doc/userguide/examples/3dhex8_static.tex index 253e6beb16..84348c05e1 100644 --- a/doc/userguide/examples/3dhex8_static.tex +++ b/doc/userguide/examples/3dhex8_static.tex @@ -26,7 +26,7 @@ \subsubsection{Overview} corresponding \filename{.cfg} files are \filename{step01.cfg}, \filename{step02.cfg}, and \filename{step03.cfg}. Each example may be run as follows: \begin{shell} -$$ pylith stepXX.cfg +$ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in diff --git a/doc/userguide/examples/3dhex8_surfload.tex b/doc/userguide/examples/3dhex8_surfload.tex index 7bc4e4aa91..be18777165 100644 --- a/doc/userguide/examples/3dhex8_surfload.tex +++ b/doc/userguide/examples/3dhex8_surfload.tex @@ -21,7 +21,7 @@ \subsubsection{Overview} \filename{.cfg} files are \filename{step18.cfg} and \filename{step19.cfg}. Each example may be run as follows: \begin{shell} -$$ pylith stepXX.cfg +$ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in diff --git a/doc/userguide/examples/3dtet4.tex b/doc/userguide/examples/3dtet4.tex index bf1c53f6de..b8865fb91b 100644 --- a/doc/userguide/examples/3dtet4.tex +++ b/doc/userguide/examples/3dtet4.tex @@ -234,7 +234,7 @@ \subsection{Shear Displacement Example} \filename{fixeddisp\_shear.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith step01.cfg +$ pylith step01.cfg \end{shell} Once the problem has run, six files will be produced. The first file is named \filename{step01\_t0000000.vtk}. The \filename{t0000000} @@ -411,7 +411,7 @@ \subsection{Kinematic Fault Slip Example} provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith step03.cfg +$ pylith step03.cfg \end{shell} Once the problem has run, eight files will be produced. The first file is named \filename{step03\_t0000000.vtk}. The \filename{t0000000} diff --git a/doc/userguide/examples/grav2d.tex b/doc/userguide/examples/grav2d.tex index 5648376aae..45adf1bddd 100644 --- a/doc/userguide/examples/grav2d.tex +++ b/doc/userguide/examples/grav2d.tex @@ -140,7 +140,7 @@ \subsection{Step 1: Gravitational Body Forces and Infinitesimal Strain} We run the simulation using: \begin{shell} -$$ pylith gravity_infstrain.cfg +$ pylith gravity_infstrain.cfg \end{shell} The simulation produces HDF5 (and corresponding XDMF) files with the output of the displacements on the ground surface and the entire @@ -173,7 +173,7 @@ \subsection{Step 2: Gravitational Body Forces, Infinitesimal Strain, and Initial We run the simulation using: \begin{shell} -$$ pylith gravity_initstress.cfg gravity_isostatic.cfg +$ pylith gravity_initstress.cfg gravity_isostatic.cfg \end{shell} \subsection{Step 3: Infinitesimal Strain Simulation with Initial Stresses and @@ -218,7 +218,7 @@ \subsection{Step 3: Infinitesimal Strain Simulation with Initial Stresses and We run the simulation using: \begin{shell} -$$ pylith gravity_initstress.cfg gravity_vardensity.cfg +$ pylith gravity_initstress.cfg gravity_vardensity.cfg \end{shell} Figure \vref{fig:examples:gravity:2d:vardensity:stress} shows the shear stress field at the end of the simulation. @@ -249,7 +249,7 @@ \subsection{Step 4: Postseismic Relaxation with Infinitesimal Strain} We run the simulation using: \begin{shell} -$$ pylith postseismic.cfg nogravity.cfg postseismic_infstrain_nograv.cfg +$ pylith postseismic.cfg nogravity.cfg postseismic_infstrain_nograv.cfg \end{shell} Figure \vref{fig:examples:gravity:2d:postseismc:infstrain:disp} shows the vertical displacement field at the end of the simulation. @@ -273,7 +273,7 @@ \subsection{Step 5: Postseismic Relaxation with Finite Strain} When we use the finite strain formulation, the solver is automatically switched to the nonlinear solver. We run the simulation using: \begin{shell} -$$ pylith postseismic.cfg nogravity.cfg postseismic_finstrain_nograv.cfg +$ pylith postseismic.cfg nogravity.cfg postseismic_finstrain_nograv.cfg \end{shell} The results are nearly identical to those with infinitesimal strain. @@ -287,7 +287,7 @@ \subsection{Step 6: Postseismic Relaxation with Infinitesimal Strain and Gravita We run the simulation using: \begin{shell} -$$ pylith postseismic.cfg postseismic_infstrain.cfg +$ pylith postseismic.cfg postseismic_infstrain.cfg \end{shell} With the infinitesimal strain formulation and linearly material behavior, the initial stress state of equal axial stresses does not alter the @@ -303,7 +303,7 @@ \subsection{Step 7: Postseismic Relaxation with Finite Strain and Gravitational We run the simulation using: \begin{shell} -$$ pylith postseismic.cfg postseismic\_finstrain.cfg +$ pylith postseismic.cfg postseismic\_finstrain.cfg \end{shell} The finite strain formulation accounts for the redistribution of gravitational body forces as the domain deforms during the postseismic @@ -355,7 +355,7 @@ \subsection{Step 8: Postseismic Relaxation with Finite Strain, Gravitational \end{cfg} for both the crust and mantle. Next we rerun Step 3 using \begin{shell} -$$ pylith gravity_initstress.cfg gravity_vardensity.cfg +$ pylith gravity_initstress.cfg gravity_vardensity.cfg \end{shell} This will change how the values appear in ParaView output. Because the output data fields contain the values at multiple points within @@ -368,14 +368,14 @@ \subsection{Step 8: Postseismic Relaxation with Finite Strain, Gravitational to generate the spatial databases with the initial stresses from the output of Step 3: \begin{shell} -$$ ./generate_statedb.py +$ ./generate_statedb.py \end{shell} After generating the initial state variables, we uncomment the \texttt{cell\_filter} lines in \filename{pylithapp.cfg} to allow easier visualization of Step 8 results. Finally, we run the simulation of the postseismic deformation using \begin{shell} -$$ pylith postseismic.cfg gravity_initstress.cfg postseismic_vardensity.cfg +$ pylith postseismic.cfg gravity_initstress.cfg postseismic_vardensity.cfg \end{shell} In the 100 years before the earthquake, it is clear that there is some ongoing deformation associated with the relaxation of the mantle. diff --git a/doc/userguide/examples/greensfns2d.tex b/doc/userguide/examples/greensfns2d.tex index c87a4680a5..c03508a81a 100644 --- a/doc/userguide/examples/greensfns2d.tex +++ b/doc/userguide/examples/greensfns2d.tex @@ -149,7 +149,7 @@ \subsection{Step 1: Solution of the Forward Problem} component is nonzero. We run the forward models by typing (in the appropriate directory) \begin{shell} -$$ pylith eqsim.cfg +$ pylith eqsim.cfg \end{shell} Once the problem has run, four HDF5 files will be produced. The file named \filename{eqsim.h5} (and the associated XDMF file) contains the @@ -295,7 +295,7 @@ \subsection{Step 3: Simple Inversion Using PyLith-generated Green's Functions} in the top-level directory from each subdirectory. To run an inversion, type: \begin{shell} -$$ ../invert_slip.py --impulses=output/greensfns-fault.h5 \ +$ ../invert_slip.py --impulses=output/greensfns-fault.h5 \ --responses=output/greensfns-points.h5 --data=output/eqsim-points.h5 \ --penalty=penalty_params.txt --output=output/slip_inverted.txt \ \end{shell} @@ -313,7 +313,7 @@ \subsection{Step 4: Visualization of Estimated and True Solutions} is contained in the \filename{plot\_invresults.py} file contained within each subdirectory. To plot the results, type: \begin{shell} -$$ plot_invresults.py --solution=output/eqsim-fault.h5 --predicted=output/slip_inverted.txt +$ plot_invresults.py --solution=output/eqsim-fault.h5 --predicted=output/slip_inverted.txt \end{shell} The script will produce an interactive matplotlib window that shows the estimated solution compared to the true solution (Figure diff --git a/doc/userguide/examples/shearwave.tex b/doc/userguide/examples/shearwave.tex index 433eb68baf..5306d045e6 100644 --- a/doc/userguide/examples/shearwave.tex +++ b/doc/userguide/examples/shearwave.tex @@ -113,7 +113,7 @@ \subsection{Simulation Parameters} \end{cfg} To run the problem, simply run PyLith without any command line arguments: \begin{shell} -$$ pylith +$ pylith \end{shell} The VTK files will be written to the \filename{output} directory. The output includes the displacement and velocity fields over the entire @@ -183,7 +183,7 @@ \subsection{Kinematic Fault (Prescribed Slip)} rupture) example in \filename{prescribedrup.cfg}. To run the problem, simply run PyLith via: \begin{shell} -$$ pylith prescribedrup.cfg +$ pylith prescribedrup.cfg \end{shell} The VTK files will be written to the \filename{output} directory with the prefix \filename{prescribedrup}. The output includes the @@ -252,7 +252,7 @@ \subsubsection{Dynamic Fault with Static Friction} specific to this example are in \filename{spontaneousrup\_staticfriction.cfg}, so we run the problem via: \begin{shell} -$$ pylith spontaneousrup.cfg spontaneousrup_staticfriction.cfg +$ pylith spontaneousrup.cfg spontaneousrup_staticfriction.cfg \end{shell} The VTK files will be written to the \filename{output} directory with the prefix \filename{staticfriction}. The output includes the displacement @@ -299,7 +299,7 @@ \subsubsection{Dynamic Fault with Slip-Weakening Friction} The parameters specific to this example are in \filename{spontaneousrup\_slipweakening.cfg}, so we run the problem via: \begin{shell} -$$ pylith spontaneousrup.cfg spontaneousrup_slipweakening.cfg +$ pylith spontaneousrup.cfg spontaneousrup_slipweakening.cfg \end{shell} The VTK files will be written to the \filename{output} directory with the prefix \filename{slipweakening}. If the problem ran correctly, you @@ -342,7 +342,7 @@ \subsubsection{Dynamic Fault with Rate-State Friction} in \filename{spontaneousrup\_ratestateageing.cfg}, so we run the problem via: \begin{shell} -$$ pylith spontaneousrup.cfg spontaneousrup_ratestateageing.cfg +$ pylith spontaneousrup.cfg spontaneousrup_ratestateageing.cfg \end{shell} The VTK files will be written to the \filename{output} directory with the prefix \filename{ratestateageing}. If the problem ran correctly, @@ -410,7 +410,7 @@ \subsection{Simulation Parameters} the parameters are set in the \filename{pylithapp.cfg} file. To run the problem, simply run PyLith without any command line arguments: \begin{shell} -$$ pylith +$ pylith \end{shell} The VTK files will be written to the \filename{output} directory. The output includes the displacement and velocity fields over the entire @@ -476,7 +476,7 @@ \subsection{Simulation Parameters} All of the parameters are set in the \filename{pylithapp.cfg} file. To run the problem, simply run PyLith without any command line arguments: \begin{shell} -$$ pylith +$ pylith \end{shell} The VTK files will be written to the \filename{output} directory. The output includes the displacement and velocity fields over the entire diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index 9b9b281a1e..4f4ab7d21d 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -176,7 +176,7 @@ \subsection{Step 1: Coseismic Slip Simulation} \end{inventory} We run this example by typing \begin{shell} -$$ pylith step01.cfg +$ pylith step01.cfg \end{shell} The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 files contain the data and the Xdmf files contain the metadata required @@ -228,7 +228,7 @@ \subsection{Step 2: Interseismic Deformation Simulation} \end{inventory} We run this example by typing \begin{shell} -$$ pylith step02.cfg +$ pylith step02.cfg \end{shell} The simulation will produce pairs of HDF5/Xdmf files with separate files for each material and fault interface. Figure @@ -273,7 +273,7 @@ \subsection{Step 3: Pseudo-Earthquake Cycle Model} \end{inventory} We run this example by typing \begin{shell} -$$ pylith step03.cfg +$ pylith step03.cfg \end{shell} The simulation will produce pairs of HDF5/Xdmf files with separate files for each material and fault interface. Figure \vref{fig:example:subduction:2d:step03}, @@ -306,7 +306,7 @@ \subsection{Step 4: Frictional Afterslip Simulation} file is provided, so you do not need to run the Python script \filename{afterslip\_tractions.py}; however, you can do so by typing \begin{shell} -$$ python afterslip_tractions.py +$ python afterslip_tractions.py \end{shell} We provide 2.0 MPa of strength excess associated with the background stress field by using a cohesion of 2.0 MPa in the static friction @@ -334,7 +334,7 @@ \subsection{Step 4: Frictional Afterslip Simulation} We run this example by typing \begin{shell} -$$ pylith step04.cfg +$ pylith step04.cfg \end{shell} The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 files contain the data and the Xdmf files contain the metadata required @@ -497,7 +497,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} We run this example by typing \begin{shell} -$$ pylith step05.cfg +$ pylith step05.cfg \end{shell} The problem will produce fourteen pairs of HDF5/Xdmf files. Figure \vref{fig:example:subduction:2d:step05}, which was created using the @@ -594,7 +594,7 @@ \subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction} We run this example by typing \begin{shell} -$$ pylith step06.cfg +$ pylith step06.cfg \end{shell} The problem will produce fourteen pairs of HDF5/Xdmf files. Figure \vref{fig:example:subduction:2d:step06}, which was created using the diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 96ad8c52b6..ab28af5716 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -113,7 +113,7 @@ \subsection{Generating the Finite-Element Mesh} \begin{shell} # Make sure you are in the 'mesh' directory and then run the Python # script to generate the journal file 'generate_surfs.jou'. -$$ ./generate_surfjou.py +$ ./generate_surfjou.py \end{shell} The next step is to use CUBIT/Trelis to run the @@ -462,7 +462,7 @@ \subsection{Step 1: Axial Compression} We run this example by typing \begin{shell} -$$ pylith step01.cfg mat_elastic.cfg +$ pylith step01.cfg mat_elastic.cfg \end{shell} The simulation will produce ten pairs of HDF5/Xdmf files in the \filename{output} directory: @@ -701,7 +701,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} We run this example by typing \begin{shell} -$$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +$ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} In addition to the ten pairs of HDF5/Xdmf files analogous to those produced in Step 1, we also have two pairs of HDF5/Xdmf files @@ -924,7 +924,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} We run this example by typing \begin{shell} -$$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +$ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} The simulation will produce fourteen pairs of HDF5/Xdmf files, beginning with \filename{step03}, in the \filename{output} @@ -1136,7 +1136,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} We run this example by typing \begin{shell} -$$ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg +$ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} The simulation will produce sixteen pairs of HDF5/Xdmf files, beginning with \filename{step04}, in the \filename{output} @@ -1352,13 +1352,13 @@ \subsection{Step 6: Prescribed Slow-Slip Event} spatial database files, and then run PyLith. \begin{shell} # Generate the spatial database files -$$ cd spatialdb && ./generate_slowslip.py -$$ ls fault_slabtop_slowslip.* +$ cd spatialdb && ./generate_slowslip.py +$ ls fault_slabtop_slowslip.* # You should see fault_slabtop_slowslip.spatialdb fault_slabtop_slowslip.timedb # Change back to the subduction directory and run PyLith -$$ cd .. -$$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg +$ cd .. +$ pylith step06.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} The problem will produce thirteen pairs of HDF5/Xdmf files: \begin{description} @@ -1525,8 +1525,8 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} You can run the two sub-problems as follows: \begin{shell} -$$ pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg -$$ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg +$ pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg +$ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} Each simulation will produce four pairs of HDF5/Xdmf files. For Step 7a these will be: @@ -1556,7 +1556,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} synthetic data from the selected time step with a specified amount of noise. Run this script by typing: \begin{shell} -$$ ./make_synthetic_gpsdisp.py +$ ./make_synthetic_gpsdisp.py \end{shell} This will create the following files: \begin{description} @@ -1571,7 +1571,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} performs a set of linear inversions, in a manner similar to the inversion in \vref{sec:example:greensfns2d:inversion}. \begin{shell} -$$ ./slip_invert.py +$ ./slip_invert.py \end{shell} This will create a number of files in the output directory. \begin{description} @@ -1735,7 +1735,7 @@ \subsubsection{Step 08a} We run the sub-problem by typing: \begin{shell} -$$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +$ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} The simulation will generate ten pairs of HDF5/Xdmf files beginning with \filename{step08a}: @@ -1798,8 +1798,8 @@ \subsubsection{Step 8b} we must use a \object{SimpleDB}. \begin{shell} # From the examples/3d/subduction directory, change to the spatialdb subdirectory. -$$ cd spatialdb -$$ ./generate_initial_stress.py +$ cd spatialdb +$ ./generate_initial_stress.py \end{shell} This will create spatial databases containing initial stresses for each of the four materials. @@ -1835,7 +1835,7 @@ \subsubsection{Step 8b} We run the sub-problem by typing: \begin{shell} -$$ pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg +$ pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} This simulation will produce files in the \filename{output} directory analogous to Step 8a. @@ -1890,7 +1890,7 @@ \subsubsection{Step 8c} We use the material settings in \filename{mat\_viscoelastic.cfg}. We can run the simulation by typing: \begin{shell} -$$ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg +$ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg \end{shell} This simulation will produce files in the \filename{output} directory analogous to Steps 8a and 8b. diff --git a/doc/userguide/examples/twohex8.tex b/doc/userguide/examples/twohex8.tex index b16c4e020a..2567e4d13e 100644 --- a/doc/userguide/examples/twohex8.tex +++ b/doc/userguide/examples/twohex8.tex @@ -114,7 +114,7 @@ \subsection{Axial Displacement Example} complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith axialdisp.cfg +$ pylith axialdisp.cfg \end{shell} Once the problem has run, two sets of files will be produced, along with one additional file. The first set will have filenames such as @@ -173,7 +173,7 @@ \subsection{Shear Displacement Example} provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith sheardisp.cfg +$ pylith sheardisp.cfg \end{shell} If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:twohex8-shear}, which was generated using @@ -228,7 +228,7 @@ \subsection{Kinematic Fault Slip Example} \filename{dislocation\_sliptime.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith dislocation.cfg +$ pylith dislocation.cfg \end{shell} If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:twohex8-disloc}, which was generated using diff --git a/doc/userguide/examples/twoquad4.tex b/doc/userguide/examples/twoquad4.tex index c5eae47e07..77ca7a217e 100644 --- a/doc/userguide/examples/twoquad4.tex +++ b/doc/userguide/examples/twoquad4.tex @@ -103,7 +103,7 @@ \subsection{Axial Displacement Example} \filename{axialdisp.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith axialdisp.cfg +$ pylith axialdisp.cfg \end{shell} As in the two triangle axial displacement example, three files will be produced. If the problem ran correctly, you should be able to produce @@ -157,7 +157,7 @@ \subsection{Shear Displacement Example} \filename{sheardisp.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith sheardisp.cfg +$ pylith sheardisp.cfg \end{shell} As in the previous example, three files will be produced. If the problem ran correctly, you should be able to produce a figure such as @@ -221,7 +221,7 @@ \subsection{Kinematic Fault Slip Example} \filename{dislocation\_sliptime.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith dislocation.cfg +$ pylith dislocation.cfg \end{shell} The addition of a fault results in two additional output files (as in the two triangle fault example), @@ -294,7 +294,7 @@ \subsection{Axial Traction Example} complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith axialtract.cfg +$ pylith axialtract.cfg \end{shell} Once the problem has run, six files will be produced. This includes the five files as in the previous example plus diff --git a/doc/userguide/examples/twotet4-geoproj.tex b/doc/userguide/examples/twotet4-geoproj.tex index f343526444..8b69823d83 100644 --- a/doc/userguide/examples/twotet4-geoproj.tex +++ b/doc/userguide/examples/twotet4-geoproj.tex @@ -145,7 +145,7 @@ \subsection{Kinematic Fault Slip Example} dislocation\_sliptime.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith dislocation.cfg +$ pylith dislocation.cfg \end{shell} If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:twotet4-geoproj-disloc}, which was generated diff --git a/doc/userguide/examples/twotet4.tex b/doc/userguide/examples/twotet4.tex index 5d1a36cda3..382e9a6ba9 100644 --- a/doc/userguide/examples/twotet4.tex +++ b/doc/userguide/examples/twotet4.tex @@ -74,7 +74,7 @@ \subsection{Axial Displacement Example} \filename{axialdisp.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith axialdisp.cfg +$ pylith axialdisp.cfg \end{shell} If the problem ran correctly, you should be able to produce a figure such as Figure \vref{fig:twotet4-axial}, which was generated using @@ -127,7 +127,7 @@ \subsection{Kinematic Fault Slip Example} \filename{dislocation\_sliptime.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith dislocation.cfg +$ pylith dislocation.cfg \end{shell} If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:twotet4-disloc}, which was generated using diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index 73a717956e..a540e898da 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -56,9 +56,9 @@ \subsection{Linux and Max OS X (Darwin)} \item Open a terminal window and change to the directory where you want to place the distribution. \begin{shell} -$$ cd $HOME -$$ mkdir pylith -$$ cd pylith +$ cd $HOME +$ mkdir pylith +$ cd pylith \end{shell} \item Download the Linux or Mac OS X (Darwin) tarball from the PyLith web page \url{geodynamics.org/cig/software/packages/short/pylith/}, @@ -66,18 +66,18 @@ \subsection{Linux and Max OS X (Darwin)} \item Unpack the tarball. \begin{shell} # Linux 32-bit -$$ tar -xzf pylith-2.2.1-linux-i686.tgz +$ tar -xzf pylith-2.2.1-linux-i686.tgz # Linux 64-bit -$$ tar -xzf pylith-2.2.1-linux-x86_64.tgz +$ tar -xzf pylith-2.2.1-linux-x86_64.tgz # Mac OS X -$$ tar -xzf pylith-2.2.1-darwin-10.11.6.tgz +$ tar -xzf pylith-2.2.1-darwin-10.11.6.tgz \end{shell} \item Set environment variables. The provided \filename{setup.sh} script only works if you are using bash shell. If you are using a different shell, you will need to alter how the environment variables are set in \filename{setup.sh}. \begin{shell} -$$ source setup.sh +$ source setup.sh \end{shell} \end{enumerate} @@ -179,31 +179,32 @@ \subsection{Setup (first time only)} host computer. However, you can copy files to/from your host filesystem using ``docker cp'' (see below). \end{enumerate} -\begin{shell} +\begin{shell}[] # Create the container -$$ docker create --name pylith-data geodynamics/pylith-data +$ docker create --name pylith-data geodynamics/pylith-data # Run the docker container and copy examples to the persistent storage. -$$ docker run -ti --volumes-from pylith-data geodynamics/pylith -$$ cp -R $HOME/pylith-VERSION/examples $HOME/data +$ docker run -ti --volumes-from pylith-data geodynamics/pylith +# This next command is run WITHIN the docker container. +$ cp -R $HOME/pylith-VERSION/examples $HOME/data \end{shell} \subsection{Run Unix shell within Docker to use PyLith.} To run the container with a text only interface: \begin{shell} -$$ docker run -ti --volumes-from pylith-data geodynamics/pylith +$ docker run -ti --volumes-from pylith-data geodynamics/pylith \end{shell} To run the container and allow display of windows on the host computer (requires that X-Windows be installed): \begin{shell} # Darwin: Allow X connections -$$ xhost +YOUR_IP_ADDRESS; DISPLAY=YOUR_IP_ADDRESS:0 +$ xhost +YOUR_IP_ADDRESS; DISPLAY=YOUR_IP_ADDRESS:0 # Linux: Allow X connections -$$ xhost +local:root +$ xhost +local:root # For Linux and Darwin, continue with the follow lines. -$$ XSOCK=/tmp/.X11-unix -$$ docker run -ti --volumes-from pylith-data \ +$ XSOCK=/tmp/.X11-unix +$ docker run -ti --volumes-from pylith-data \ -e DISPLAY=$DISPLAY -v $XSOCK:$XSOCK geodynamics/pylith \end{shell} @@ -227,17 +228,17 @@ \subsubsection{Using Docker containers} \item To attach to a ``paused'' or ``running'' container. \begin{shell} # Get the container id. -$$ docker ps +$ docker ps # Attach to the container -$$ docker attach CONTAINER_ID +$ docker attach CONTAINER_ID \end{shell} \item To restart an existing container after it exited. \begin{shell} # Get the container id. -$$ docker ps -a +$ docker ps -a # Start and then attach to the container -$$ docker run CONTAINER_ID -$$ docker attach CONTAINER_ID +$ docker run CONTAINER_ID +$ docker attach CONTAINER_ID \end{shell} \end{itemize} @@ -252,24 +253,24 @@ \subsection{Copy data to/from persistent storage volume.} \begin{shell} # Copy data FROM persistent storage volume TO local host -$$ docker cp pylith-data:/data/pylith-user/PATH/FILENAME LOCAL_PATH +$ docker cp pylith-data:/data/pylith-user/PATH/FILENAME LOCAL_PATH # Copy data FROM local host TO persistent storage volume -$$ docker cp LOCAL_PATH pylith-data:/data/pylith-user/PATH/ +$ docker cp LOCAL_PATH pylith-data:/data/pylith-user/PATH/ \end{shell} \subsection{Docker Quick Reference} \begin{shell} # List local docker images. -$$ docker images +$ docker images # List all docker containers. -$$ docker ps -a +$ docker ps -a # List running docker containers. -$$ docker ps +$ docker ps # Remove docker container -$$ docker rm CONTAINER_ID +$ docker rm CONTAINER_ID # Remove docker image -$$ docker rmi IMAGE_ID +$ docker rmi IMAGE_ID \end{shell} \section{Installation from Source} @@ -313,13 +314,23 @@ \section{Verifying PyLith is Installed Correctly} for the examples. To run the example discussed in Section \vref{sec:example:3dhex8-static}: \begin{shell} -$$ cd examples/3d/hex8 -$$ pylith step01.cfg +$ cd examples/3d/hex8 +$ pylith step01.cfg +# A bunch of stuff will be written to stdout. The last few lines should be: +WARNING! There are options you set that were not used! +WARNING! could be spelling mistake, etc! +Option left: name:-snes_atol value: 1.0e-9 +Option left: name:-snes_converged_reason (no value) +Option left: name:-snes_error_if_not_converged (no value) +Option left: name:-snes_linesearch_monitor (no value) +Option left: name:-snes_max_it value: 100 +Option left: name:-snes_monitor (no value) +Option left: name:-snes_rtol value: 1.0e-10 \end{shell} If you run PyLith in a directory without any input, you will get the error message: \begin{shell} -$$ pylith +$ pylith >> {default}:: -- pyre.inventory(error) -- meshimporter.meshioascii.filename <- '' @@ -398,9 +409,9 @@ \subsection{Launchers and Schedulers} execution (the output is only meaningful if you're using a batch system). \begin{shell} # Display the bash script that would be submitted. -$$ pylith --scheduler.dry +$ pylith --scheduler.dry # Display the mpirun command. -$$ pylith --launcher.dry +$ pylith --launcher.dry \end{shell} \subsection{Running without a Batch System} @@ -423,7 +434,7 @@ \subsection{Running without a Batch System} Now, invoke the following: \begin{shell} -$$ pylith example.cfg mymachines.cfg +$ pylith example.cfg mymachines.cfg \end{shell} This strategy gives you the flexibility to create an assortment of \filename{.cfg} files (with one \filename{.cfg} file for each machine @@ -435,7 +446,7 @@ \subsection{Running without a Batch System} is read automatically). Then, you can run any simulation with no additional arguments: \begin{shell} -$$ pylith example.cfg +$ pylith example.cfg \end{shell} \warning{This assumes your machine list has enough nodes for the @@ -456,7 +467,7 @@ \subsection{Using a Batch System} nodes and number of processes per compute node, the job name, and the allotted time for the job: \begin{shell} -$$ pylith example1.cfg \ +$ pylith example1.cfg \ --job.queue=debug \ --job.name=example1 \ --job.stdout=example1.log \ diff --git a/doc/userguide/preface.tex b/doc/userguide/preface.tex index a4ffdf2698..bf27461240 100644 --- a/doc/userguide/preface.tex +++ b/doc/userguide/preface.tex @@ -41,10 +41,10 @@ \subsection{Unix Shell Commands} Commands entered into a Unix shell (i.e., terminal) are shown in a box. Comments are delimited by the \# character. We use -{\tt \$\$} to indicate the bash shell prompt. +{\tt \$} to indicate the bash shell prompt. \begin{shell} # This is a comment. -$$ ls -l +$ ls -l \end{shell} \subsection{Excerpts of cfg Files} @@ -121,4 +121,5 @@ \section{Request for Comments} Your suggestions and corrections can only improve this documentation. Please report any errors, inaccuracies, or typos to the CIG Short-Term -Tectonics email list \url{cig-short@geodynamics.org}. +Tectonics email list \url{cig-short@geodynamics.org} or create a +GitHub pull request. diff --git a/doc/userguide/runpylith/databases.tex b/doc/userguide/runpylith/databases.tex index 7896db4203..9994ce3368 100644 --- a/doc/userguide/runpylith/databases.tex +++ b/doc/userguide/runpylith/databases.tex @@ -84,8 +84,8 @@ \subsection{\object{SimpleDB} Spatial Database} so you do not need to change this setting.} \propertyitem{iohandler.filename}{Filename for the spatial database.} \end{inventory} -An example of setting these in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{SimpleDB} parameters in a \filename{.cfg} file]

      label

      = Material properties

      query_type

      = linear

      iohandler.filename

      = mydb.spatialdb @@ -108,15 +108,16 @@ \subsection{\object{UniformDB} Spatial Database} \propertyitem{data}{Array of values in spatial database.} \end{inventory} -Specify the physical properties of a linearly elastic, isotropic material -in a \filename{.cfg} file. The data values are dimensioned -with the appropriate units using Python syntax. -\begin{cfg} +\begin{cfg}[\object{UniformDB} parameters in a \filename{.cfg} file] [pylithapp.timedependent.materials.material]

      db_properties

      = spatialdata.spatialdb.UniformDB ; Set the db to a UniformDB

      db_properties.values

      = [vp, vs, density] ; Set the names of the values in the database

      db_properties.data

      = [5773.5*m/s, 3333.3*m/s, 2700.0*kg/m**3] ; Set the values in the database} \end{cfg} +This example specifies the physical properties of a linearly elastic, +isotropic material in a \filename{.cfg} file. The data values are +dimensioned with the appropriate units using Python syntax. + \subsubsection{\object{ZeroDispDB}} @@ -154,8 +155,8 @@ \subsection{\object{SimpleGridDB} Spatial Database} parameter are ``linear'' and ``nearest'' (default).} \propertyitem{filename}{Filename for the spatial database.} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{SimpleGridDB} parameters in a \filename{.cfg} file]

      label

      = Material properties

      query_type

      = linear

      filename

      = mydb_grid.spatialdb @@ -189,9 +190,7 @@ \subsection{SCEC CVM-H Spatial Database (\object{SCECCVMH})} below this elevation remains undistorted).} \end{inventory} -Specify the physical properties of a linearly elastic, isotropic material -using the SCEC CVM-H in a \filename{.cfg} file. -\begin{cfg} +\begin{cfg}[\object{SCECCVMH} parameters in a \filename{.cfg} file] [pylithapp.timedependent.materials.material]

      db_properties

      = spatialdata.spatialdb.SCECCVMH ; Set the database to the SCEC CVM-H @@ -214,8 +213,9 @@ \subsection{\object{CompositeDB} Spatial Database} to have two different spatial databases, e.g., a seismic velocity model with Vp, Vs, and density values, and another database with the inelastic physical properties. We can use the \object{CompositeDB} -spatial database for these cases. An example would be: -\begin{cfg} +spatial database for these cases. + +\begin{cfg}[\object{CompositeDB} parameters in a \filename{.cfg} file] [pylithapp.timedependent.materials.maxwell]

      label

      = Maxwell material

      id

      = 1 @@ -267,8 +267,8 @@ \subsection{\object{TimeHistory} Database} messages.} \propertyitem{filename}{Filename for the time history database.} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{TimeHistory} parameters in a \filename{.cfg} file]

      label

      = Displacement time history

      filename

      = mytimehistory.timedb \end{cfg} diff --git a/doc/userguide/runpylith/definesim.tex b/doc/userguide/runpylith/definesim.tex index 53e69a9dfa..b8ebfe6aa7 100644 --- a/doc/userguide/runpylith/definesim.tex +++ b/doc/userguide/runpylith/definesim.tex @@ -81,13 +81,16 @@ \subsubsection{Using the Command Line} component, you can run PyLith with the \commandline{-{}-COMPONENT.help-properties} flag: \begin{shell} -$$ pylith --problem.help-properties +$ pylith --problem.help-properties + # Show problem components. -$$ pylith --problem.help-components +$ pylith --problem.help-components + # Show bc components (bc is a component of problem). -$$ pylith --problem.bc.help-components +$ pylith --problem.bc.help-components + # Show bc properties. -$$ pylith --problem.bc.help-properties +$ pylith --problem.bc.help-properties \end{shell} @@ -139,7 +142,7 @@ \subsubsection{Specification and Placement of Configuration Files} Configuration files may be specified on the command line: \begin{shell} -$$ pylith example.cfg +$ pylith example.cfg \end{shell} In addition, the Pyre framework searches for configuration files named \filename{pylithapp.cfg} in several predefined locations. You may put @@ -172,7 +175,7 @@ \subsubsection{Specification and Placement of Configuration Files} to the directory \filename{examples/twocells/twohex8}, we have the following. \begin{shell} -$$ ls -1 *.cfg +$ ls -1 *.cfg axialdisp.cfg dislocation.cfg pylithapp.cfg @@ -182,19 +185,22 @@ \subsubsection{Specification and Placement of Configuration Files} settings are included by specifying one of the other files on the command-line: \begin{shell} -$$ pylith axialdisp.cfg +$ pylith axialdisp.cfg \end{shell} If you want to see what settings are being used, you can either examine the \filename{.cfg} files, or use the help flags as described above: \begin{shell} # Show components for the 'problem' facility. -$$ pylith axialdisp.cfg --problem.help-components +$ pylith axialdisp.cfg --problem.help-components + # Show properties for the 'problem' facility. -$$ pylith axialdisp.cfg --problem.help-properties +$ pylith axialdisp.cfg --problem.help-properties + # Show components for the 'bc' facility. -$$ pylith axialdisp.cfg --problem.bc.help-components +$ pylith axialdisp.cfg --problem.bc.help-components + # Show properties for the 'bc' facility. -$$ pylith axialdisp.cfg --problem.bc.help-properties +$ pylith axialdisp.cfg --problem.bc.help-properties \end{shell} This is generally a more useful way of determining problem settings, since it includes default values as well as those that have been specified @@ -208,7 +214,7 @@ \subsubsection{List of PyLith Parameters ({\ttfamily pylithinfo})} parameters to a text file or JSON file (default). The default name of the JSON is \filename{pylith\_parameters.json}. The usage synopsis is \begin{shell} -$$ pylithinfo [--verbose-false] [--format={ascii,json} [--filename=pylith_parameters.json] PYLITH_ARGS +$ pylithinfo [--verbose-false] [--format={ascii,json} [--filename=pylith_parameters.json] PYLITH_ARGS \end{shell} where \commandline{-{}-verbose-false} turns off printing the descriptions of the properties and components as well as the location where the @@ -356,9 +362,7 @@ \subsubsection{\object{Distributor}} \facilityitem{data\_writer}{Writer for partition information (default is \object{DataWriterVTK} for VTK output).} \end{inventory} -An example of setting the partitioner in a \filename{pylithapp.cfg} - file is: -\begin{cfg} +\begin{cfg}[\object{Distributor} parameters in a \filename{.cfg} file] [pylithapp.mesh_generator.distributor]

      partitioner

      = chaco ; Options are 'chaco' (default) and 'parmetis'. \end{cfg} @@ -426,9 +430,8 @@ \subsection{Problem Specification (\facility{problem})} \facilityitem{progress\_ monitor}{Show progress of running simulation.} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file for -a problem is: -\begin{cfg} + +\begin{cfg}[Problem parameters in a \filename{.cfg} file] [pylithapp.timedependent]

      dimension

      = 3 normalizer = spatialdata.units.NondimElasticQuasistatic @@ -456,9 +459,7 @@ \subsubsection{Nondimensionalization (\facility{normalizer})} \propertyitem{relaxation\_time}{Relaxation time to nondimensionalize time (default is 1.0 year).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file for -a problem is: -\begin{cfg} +\begin{cfg}[\object{NondimElasticQuasistatic} parameters in a \filename{.cfg} file] [pylithapp.timedependent.normalizer]

      length_scale

      = 1.0*km

      shear_modulus

      = 3.0e+10*Pa @@ -474,9 +475,7 @@ \subsubsection{Nondimensionalization (\facility{normalizer})} \propertyitem{wave\_period}{Period of seismic waves used to nondimensionalize time (default is 1.0 s).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file for -a problem is: -\begin{cfg} +\begin{cfg}[\object{NondimElasticDynamic} parameters in a \filename{.cfg} file] [pylithapp.timedependent.normalizer]

      shear_wave_speed

      = 3.0*km/s

      mass_density

      = 3.0e+3*kg/m**3 diff --git a/doc/userguide/runpylith/formulation.tex b/doc/userguide/runpylith/formulation.tex index 528ebfc362..0991d55f91 100644 --- a/doc/userguide/runpylith/formulation.tex +++ b/doc/userguide/runpylith/formulation.tex @@ -54,9 +54,8 @@ \section{Time-Dependent Problem (\facilityshape{formulation})} \facilityitem{formulation}{Formulation for solving the partial differential equation.} \end{inventory} -An example of setting the properties and components in a \filename{.cfg} file -is -\begin{cfg} + +\begin{cfg}[\object{TimeDependent} parameters in a \filename{.cfg} file] [pylithapp.timedependent] formulation = pylith.problems.Implicit ; default progres_monitor = pylith.problems.ProgressMonitorTime ; default @@ -87,8 +86,7 @@ \subsection{Time-Stepping Formulation} to a file for analysis (default is PETSc binary).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is -\begin{cfg} +\begin{cfg}[Time-stepping formulation parameters in a \filename{.cfg} file] [pylithapp.timedependent.formulation]

      matrix_type

      = sbaij ; Non-symmetric sparse matrix is 'aij'

      view_jacobian

      = false @@ -178,9 +176,8 @@ \subsubsection{Uniform, User-Specified Time Step (\object{TimeStepUniform})} \propertyitem{start\_time}{Start time for simulation (default is 0.0 s).} \propertyitem{dt}{Time step for simulation.} \end{inventory} -An example of setting a uniform, user-specified time step in a \filename{.cfg} -file is: -\begin{cfg} + +\begin{cfg}[\object{TimeStepUniform} parameters in a \filename{.cfg} file] [pylithapp.problem.formulation]

      time_step

      = pylith.problems.TimeStepUniform ; Default value @@ -207,9 +204,8 @@ \subsubsection{Nonuniform, User-Specified Time Step (\object{TimeStepUser})} \propertyitem{loop\_steps}{If true, cycle through time steps, otherwise keep using last time-step size for any time remaining.} \end{inventory} -An example of setting the properties for nonuniform, user-specified -time steps in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{TimeStepUser} parameters in a \filename{.cfg} file] [pylithapp.problem.formulation] time_step = pylith.problems.TimeStepUser ; Change the time step algorithm @@ -245,9 +241,8 @@ \subsubsection{Nonuniform, Automatic Time Step (\object{TimeStepAdapt})} \propertyitem{stability\_factor}{Safety factor for stable time step (default is 2.0).} \end{inventory} -An example of setting the properties for the automatic time step in -a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{TimeStepAdapt} parameters in a \filename{.cfg} file] [pylithapp.problem.formulation]

      time_step

      = pylith.problems.TimeStepAdapt ; Change the time step algorithm @@ -278,9 +273,8 @@ \section{Green's Functions Problem (\object{GreensFns})} equation.} \propertyitem{progress\_monitor}{Simple progress monitor via text file.} \end{inventory} -An example of setting the properties for the GreensFns problem in -a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{GreensFns} parameters in a \filename{.cfg} file] [pylithapp] problem = pylith.problems.GreensFns ; Change problem type from the default @@ -318,8 +312,8 @@ \subsection{\object{ProgressMonitorTime}} \propertyitem{filename}{Name of output file.} \propertyitem{t\_units}{Units for simulation time in output.} \end{inventory} -An example of setting the properties in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{ProgressMonitorTime} parameters in a \filename{.cfg} file] [pylithapp.problem.progressmonitor]

      update_percent

      = 5.0 ; default

      filename

      = progress.txt ; default @@ -337,8 +331,8 @@ \subsection{\object{ProgressMonitorStep}} \propertyitem{update\_percent}{Frequency (in percent) of progress updates.} \propertyitem{filename}{Name of output file.} \end{inventory} -An example of setting the properties in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{ProgressMonitorStep} parameters in a \filename{.cfg} file] [pylithapp.problem.progressmonitor]

      update_percent

      = 5.0 ; default

      filename

      = progress.txt ; default diff --git a/doc/userguide/runpylith/output.tex b/doc/userguide/runpylith/output.tex index bed06b4473..a4a37d3de0 100644 --- a/doc/userguide/runpylith/output.tex +++ b/doc/userguide/runpylith/output.tex @@ -60,9 +60,8 @@ \subsection{Output Manager} \facilityitem{cell\_filter}{Filter to apply to all cell fields (see Section \vref{sub:cell:field:filters}).} \end{inventory} -An example of setting the output parameters for a material in a \filename{.cfg} -file is -\begin{cfg} + +\begin{cfg}[\object{OutputManager} parameters in a \filename{.cfg} file] [pylithapp.timedependent.materials.elastic.output]

      output_freq

      = time_step

      time_step

      = 1.0*yr @@ -285,10 +284,7 @@ \subsubsection{Parameters} the same prefix).} \end{inventory} -An example of changing the writer from the default VTK writer to the -HDF5 writer with external datasets (\object{DataWriterHDF5Ext}) for -output over the domain in a \filename{.cfg} file is -\begin{cfg} +\begin{cfg}[\object{DataWriterHDF5Ext} parameters in a \filename{.cfg} file] [pylithapp.timedependent.domain.output]

      output_freq

      = time_step

      time_step

      = 1.0*yr @@ -296,6 +292,9 @@ \subsubsection{Parameters} writer = pylith.meshio.DataWriterHDF5Ext

      writer.filename

      = dislocation.h5 \end{cfg} +In this example, we change the writer from the default VTK writer to +the HDF5 writer with external datasets (\object{DataWriterHDF5Ext}) +for output over the domain. \subsubsection{HDF5 Utilities} @@ -306,13 +305,16 @@ \subsubsection{HDF5 Utilities} stdout. \begin{shell} # Dump the entire HDF5 file (not useful for large files). -$$ h5dump mydata.h5 +$ h5dump mydata.h5 + # Dump the hierarchy of an HDF5 file. -$$ h5dump -n mydata.h5 +$ h5dump -n mydata.h5 + # Dump the hierarchy with dataset dimensions and attributes. -$$ h5dump -H mydata.h5 +$ h5dump -H mydata.h5 + # Dump dataset 'vertices' in group '/geometry' to stdout. -$$ h5dump -d /geometry/vertices mydata.h5 +$ h5dump -d /geometry/vertices mydata.h5 \end{shell} We have also include a utility \filename{pylith\_genxdmf} (see Section \vref{sec:pylith:genxdmf}) that generates an appropriate Xdmf file diff --git a/doc/userguide/runpylith/parametersgui.tex b/doc/userguide/runpylith/parametersgui.tex index 851b1472cb..a8e6d27537 100644 --- a/doc/userguide/runpylith/parametersgui.tex +++ b/doc/userguide/runpylith/parametersgui.tex @@ -21,7 +21,7 @@ \section{Installation} downloading the tarball, unpack it. We recommend unpacking the tarball in the top-level PyLith directory. \begin{shell} -$$ tar -xvf pylith_parameters-1.0.0.tgz +$ tar -xvf pylith_parameters-1.1.0.tgz \end{shell} \section{Running the Parameter Viewer} @@ -45,7 +45,7 @@ \subsection{Generate the parameter JSON file} DumpParametersJSON component contains a property for the name of the file. You can set the filename on the command line \begin{shell} -$$ pylith --dump_parameters.filename=FILENAME.json +$ pylith --dump_parameters.filename=FILENAME.json \end{shell} or within a .cfg file \begin{cfg} @@ -64,8 +64,8 @@ \subsection{Start the web server} script. This will start a simple Python-based web server on your local computer. \begin{shell} -$$ cd parametersgui -$$ ./pylith\_paramviewer +$ cd parametersgui +$ ./pylith_paramviewer \end{shell} The script will instruct you to point your web browswer to a local port on your computer. The default is \url{http://127.0.0.1:9000}. @@ -86,7 +86,7 @@ \section{Using the Parameter Viewer} navigate to the desired file. \begin{figure}[htbp] - \includegraphics[width=5in]{runpylith/figs/paramgui_startup} + \fbox{\includegraphics[width=5in]{runpylith/figs/paramgui_startup}} \caption{Screenshot of PyLith Parameter Viewer in web browser upon startup.} \label{fig:parameters:gui:startup} \end{figure} @@ -103,7 +103,7 @@ \subsection{Version Information} \ref{fig:parameters:gui:version}. \begin{figure}[htbp] - \includegraphics[width=5in]{runpylith/figs/paramgui_version} + \fbox{\includegraphics[width=5in]{runpylith/figs/paramgui_version}} \caption{Screenshot of \textsf{Version} tab of the PyLith Parameter Viewer with sample JSON parameter file.} \label{fig:parameters:gui:version} @@ -125,7 +125,7 @@ \subsection{Parameter Information} \ref{fig:parameters:gui:parameters:selected}). \begin{figure}[htbp] - \includegraphics[width=5in]{runpylith/figs/paramgui_parameters} + \fbox{\includegraphics[width=5in]{runpylith/figs/paramgui_parameters}} \caption{Screenshot of \textsf{Parameters} tab of the PyLith Parameter Viewer with sample JSON parameter file before selecting a component in the left panel.} @@ -134,7 +134,7 @@ \subsection{Parameter Information} \begin{figure}[htbp] - \includegraphics[width=5in]{runpylith/figs/paramgui_detail} + \fbox{\includegraphics[width=5in]{runpylith/figs/paramgui_detail}} \caption{Screenshot of \textsf{Parameters} tab of the PyLith Parameter Viewer with sample JSON parameter file with the \facility{z\_neg} facility selected.} @@ -142,4 +142,4 @@ \subsection{Parameter Information} \end{figure} -% End of file \ No newline at end of file +% End of file diff --git a/doc/userguide/runpylith/postprocessing.tex b/doc/userguide/runpylith/postprocessing.tex index 0c955255c4..d992fe1a49 100644 --- a/doc/userguide/runpylith/postprocessing.tex +++ b/doc/userguide/runpylith/postprocessing.tex @@ -40,9 +40,9 @@ \subsection{\filename{pylith\_genxdmf}} is also useful in updating Xdmf files when users add fields to HDF5 files during post-processing. \begin{shell} -$$ pylith_genxdmf --files=FILE_OR_FILE_PATTERN +$ pylith_genxdmf --files=FILE_OR_FILE_PATTERN \end{shell} -The default value is the \filename{*.h5} file pattern. +The default value for \filename{FILE\_OR\_FILE\_PATTERN} is \filename{*.h5}. \warning{If the HDF5 files contain external datasets, then this utility should be run from the same relative path to the HDF5 files diff --git a/doc/userguide/runpylith/tips.tex b/doc/userguide/runpylith/tips.tex index d4a2e3c581..3fd370408b 100644 --- a/doc/userguide/runpylith/tips.tex +++ b/doc/userguide/runpylith/tips.tex @@ -109,7 +109,7 @@ \subsubsection{Segmentation Fault} can generate a backtrace using the debugger by using the \commandline{-{}-petsc.start\_in\_debugger} command-line argument: \begin{shell} -$$ pylith [..args..] --petsc.start_in_debugger +$ pylith [..args..] --petsc.start_in_debugger (gdb) continue (gdb) backtrace \end{shell} @@ -117,7 +117,7 @@ \subsubsection{Segmentation Fault} To use valgrind to detect the memory error, first go to your working directory and run the problem with \commandline{-{}-launcher.dry}: \begin{shell} -$$ pylith [..args..] --launcher.dry +$ pylith [..args..] --launcher.dry \end{shell} Instead of actually running the problem, this causes PyLith to dump @@ -126,7 +126,7 @@ \subsubsection{Segmentation Fault} valgrind before the full path to mpinemesis and tell valgrind to use a log file: \begin{shell} -$$ mpirun /path/to/valgrind --log-file=valgrind-log /path/to/mpinemesis --pyre-start +$ mpirun /path/to/valgrind --log-file=valgrind-log /path/to/mpinemesis --pyre-start [..lots of junk..] \end{shell} From 837de1b66c5cf42d25435c8fb76241f0253584b1 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 11:58:57 -0700 Subject: [PATCH 209/216] Updated code listings. --- doc/userguide/materials/materials.tex | 13 ++++++------- 1 file changed, 6 insertions(+), 7 deletions(-) diff --git a/doc/userguide/materials/materials.tex b/doc/userguide/materials/materials.tex index d14970e9fb..1ce8e6a960 100644 --- a/doc/userguide/materials/materials.tex +++ b/doc/userguide/materials/materials.tex @@ -74,11 +74,10 @@ \subsection{Material Parameters} \facilityitem{quadrature}{Numerical integration scheme used in integrating fields over each cell.} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file for -a problem with two material groups is: -\begin{cfg} + +\begin{cfg}[Parameters for two materials in a \filename{.cfg} file] [pylithapp.timedependent] -

      materials

      = [elastic,viscoelastic] +

      materials

      = [elastic, viscoelastic] [pylithapp.timedependent.materials.elastic]

      label

      = Elastic material @@ -232,7 +231,7 @@ \subsubsection{Specification of Initial State Variables} behavior, specify a spatial database for the initial stress, strain, and/or state variables as in the example from the example in Section \vref{sec:example:3dhex8}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{examples/3d/hex8/step16.cfg}] [pylithapp.timedependent.materials.elastic] db_initial_stress = spatialdata.spatialdb.SimpleDB

      db_initial_stress.iohandler.filename

      = initial\_stress.spatialdb @@ -1537,8 +1536,8 @@ \subsubsection{Drucker-Prager Elastoplastic With No Hardening (Perfectly Plastic otherwise an error message will occur when the model fails beyond the tensile strength (default is false).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{DruckerPrager3D} parameters in a \filename{.cfg} file] [pylithapp.timedependent]

      materials

      = [plastic] materials.plastic = pylith.materials.DruckerPrager3D From c5dacd36d162d2b31b8a77274458f51a8813885c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 12:23:08 -0700 Subject: [PATCH 210/216] Updates code listings. --- .../boundaryconditions/boundaryconditions.tex | 115 ++++++++---------- doc/userguide/examples/3dhex8.tex | 2 +- doc/userguide/examples/3dhex8_dike.tex | 4 +- doc/userguide/examples/3dhex8_friction.tex | 6 +- doc/userguide/examples/3dhex8_gravity.tex | 4 +- doc/userguide/examples/3dhex8_greensfns.tex | 8 +- doc/userguide/examples/3dhex8_quasistatic.tex | 10 +- doc/userguide/examples/3dhex8_static.tex | 4 +- doc/userguide/examples/3dhex8_surfload.tex | 4 +- doc/userguide/examples/3dtet4.tex | 10 +- doc/userguide/examples/shearwave.tex | 2 +- doc/userguide/examples/subduction3d.tex | 4 +- doc/userguide/examples/twoquad4.tex | 2 +- doc/userguide/examples/twotri3.tex | 4 +- doc/userguide/extending/extending.tex | 4 +- doc/userguide/install/install.tex | 2 +- doc/userguide/materials/materials.tex | 10 +- doc/userguide/runpylith/databases.tex | 28 ++--- doc/userguide/runpylith/definesim.tex | 34 +++--- doc/userguide/runpylith/formulation.tex | 18 +-- doc/userguide/runpylith/output.tex | 8 +- doc/userguide/runpylith/parametersgui.tex | 2 +- doc/userguide/runpylith/postprocessing.tex | 2 +- doc/userguide/runpylith/runpylith.tex | 2 +- 24 files changed, 136 insertions(+), 153 deletions(-) diff --git a/doc/userguide/boundaryconditions/boundaryconditions.tex b/doc/userguide/boundaryconditions/boundaryconditions.tex index 3ee573c02c..efbfb5c8b2 100644 --- a/doc/userguide/boundaryconditions/boundaryconditions.tex +++ b/doc/userguide/boundaryconditions/boundaryconditions.tex @@ -10,7 +10,7 @@ \section{Assigning Boundary Conditions} condition. \item Define boundary condition groups corresponding to the vertex sets. \item Set the parameters for each boundary condition group using - \filename{.cfg} files and/or command line + \filename{cfg} files and/or command line arguments. \item Specify the spatial variation in parameters for the boundary condition using a spatial database file. @@ -42,12 +42,11 @@ \subsection{Arrays of Boundary Condition Components} containers are no longer available (or necessary). The default boundary condition for each component in the array is the \object{DirichletBC} object. Other boundary conditions can be bound to the named items in the array -via a \filename{.cfg} file, \filename{.pml} file, or the command line. +via a \filename{cfg} file, \filename{pml} file, or the command line. The parameters for the boundary condition are set using the name of -the boundary condition. An example of setting the array of boundary -condition components and changing the types of boundary conditions -in a \texttt{.cfg} file: -\begin{cfg} +the boundary condition. + +\begin{cfg}[Array of boundary conditions in a \filename{cfg} file] [pylithapp.problem]

      bc

      = [x_neg, x_pos, y_pos, z_neg] ; Array of boundary conditions @@ -119,9 +118,9 @@ \subsection{Dirichlet Boundary Conditions} By default the output manager does not output any information. The specified displacements and velocities can be output by including ``displacement'' and ``velocity'' in the output manager's \property{vertex\_info\_fields} -array parameter. An example of setting the Dirichlet boundary condition -parameters in a \filename{.cfg} file is: -\begin{cfg} +array parameter. + +\begin{cfg}[\object{DirichletBC} parameters in a \filename{cfg} file] [pylithapp.problem]

      bc

      = [mybc] @@ -173,6 +172,7 @@ \subsubsection{Dirichlet Boundary Condition Spatial Database Files} \caption{Values in the spatial databases used for Dirichlet boundary conditions.} \begin{tabular}{lp{4in}} \textbf{Spatial database} & \textbf{Name in Spatial Database}\\ + \hline \facility{db\_initial} & \texttt{displacement-x, displacement-y, displacement-z}\\ \facility{db\_rate} & \texttt{displacement-rate-x, displacement-rate-y, displacement-rate-z, rate-start-time}\\ \facility{db\_change} & \texttt{displacement-x, displacement-y, displacement-z, change-start-time}\\ @@ -219,9 +219,9 @@ \subsection{Neumann Boundary Conditions} By default the output manager does not output any information. The specified tractions can be output in global coordinates by including ``tractions'' in the output manager's \property{cell\_info\_fields} -array parameter. An example of setting these parameters in a -\filename{.cfg} file is: -\begin{cfg} +array parameter. + +\begin{cfg}[\object{Neumann} parameters in a \filename{cfg} file] pylithapp.timedependent]

      bc

      = [x_neg, x_pos, y_neg] bc.x_pos = pylith.bc.Neumann ; Change BC type to Neumann @@ -314,9 +314,8 @@ \subsubsection{Point Force Parameters} \propertyitem{label}{Label of the group of vertices associated with the boundary condition.} \propertyitem{bc\_dof}{Array of degrees of freedom to which forces are applied (first degree of freedom is 0).} \end{inventory} -An example of setting the point force boundary condition parameters -in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{PointForce} parameters in a \filename{cfg} file] [pylithapp.problem]

      bc

      = [mybc] bc.mybc = pylith.bc.PointForce @@ -618,10 +617,10 @@ \subsection{Fault Parameters} The fault coordinate system is shown in Figure \vref{fig:fault:slip:motions}. The vectors in the fault coordinate system can be transformed to the global coordinate system using the direction vectors in the diagnostic -output. An example of setting these parameters in a \filename{.cfg} -file is: -\begin{cfg} - +output. + +\begin{cfg}[Fault parameters in a \filename{cfg} file] +[pylithapp.problem]

      interfaces

      = [fault] [pylithapp.problem.interfaces] @@ -786,10 +785,10 @@ \subsubsection{Arrays of Kinematic Rupture Components} associates a name (string) with each kinematic rupture. The default dynamic array contains a single earthquake rupture, ``rupture''. The \property{eq\_srcs} is the \object{FaultCohesiveKin} facility for this -dynamic array. An example of setting the array of kinematic rupture -components in a \filename{.cfg} file: -\begin{cfg} - +dynamic array. + +\begin{cfg}[Array of kinematic rupture components in a \filename{cfg} file] +[pylithapp.problem.interfaces.fault]

      eq_srcs

      = [earthquake,creep] \end{cfg} The output manager includes generic fault information (orientation) @@ -825,9 +824,8 @@ \subsubsection{Kinematic Rupture Parameters} is relative to the origin time (default is 0). This means that slip initiates at a point at a time corresponding to the sum of the kinematic rupture's origin time and the slip initiation time for that point. -An example of specifying the kinematic earthquake rupture properties -and components in a \filename{.cfg} file: -\begin{cfg} + +\begin{cfg}[\object{FaultCohesiveKin} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault]

      eq_srcs

      = [earthquake,creep] @@ -876,8 +874,8 @@ \subsubsection{Slip Time Function} \facilityitem{final\_slip}{Spatial database of slip ($D_{final})$.} \facilityitem{slip\_time}{Spatial database of slip initiation times ($t_{r}$).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{StepSlipFn} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault.eq_srcs.rupture] slip_function = pylith.faults.StepSlipFn @@ -923,8 +921,8 @@ \subsubsection{Slip Time Function} \facilityitem{slip\_rate}{Spatial database of slip rate ($V$).} \facilityitem{slip\_time}{Spatial database of slip initiation times ($t_{r}$).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{ConstRateSlipFn} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault.eq_srcs.ruptures] slip_function = pylith.faults.ConstRateSlipFn @@ -972,8 +970,8 @@ \subsubsection{Slip Time Function} \facilityitem{slip\_time}{Spatial database of slip initiation times ($t_{r}$).} \facilityitem{rise\_time}{Spatial database for rise time ($t_{\mathit{rise}}$).} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{BruneSlipFn} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault.eq_srcs.ruptures] slip_function = pylith.faults.BruneSlipFn @@ -1045,8 +1043,8 @@ \subsubsection{Slip Time Function} \facilityitem{slip\_time}{Spatial database of slip initiation times ($t_{r}$).} \facilityitem{time\_history}{Temporal database for slip evolution.} \end{inventory} -An example of setting these parameters in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{TimeHistorySlipFn} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault.eq_srcs.ruptures] slip_function = pylith.faults.TimeHistorySlipFn @@ -1171,7 +1169,7 @@ \subsubsection{Governing Equations} manner as the main solver, except we use the prefix \texttt{friction\_} in all of the settings related to the KSP solver for these two linear systems. For example, to use the recommended additive Schwarz preconditioner -in the friction sensitivity solves, the settings in a \texttt{.cfg} +in the friction sensitivity solves, the settings in a \filename{cfg} file are: \begin{cfg} [pylithapp.petsc] @@ -1214,9 +1212,8 @@ \subsubsection{Dynamic Rupture Parameters} default is none).} \facilityitem{friction}{Fault constitutive model.} \end{inventory} -An example of specifying the dynamic earthquake rupture properties -and components in a \filename{.cfg} file: -\begin{cfg} + +\begin{cfg}[\object{FaultCohesiveDyn} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault]

      open_free_surface

      = True ; default @@ -1243,9 +1240,9 @@ \subsubsection{Dynamic Rupture Parameters} the overall desired tolerances. The separate tolerance for near zero values of fault opening was added in v2.2.1. This provides the solver greater flexibility to prevent fault opening with nonplanar - faults..} + faults.} -\begin{cfg} +\begin{cfg}[Sample tolerance settings for fault friction] [pylithapp.problem.interfaces.fault]

      zero_tolerance

      = 1.0e-11

      zero_tolerance_normal

      = 2.0e-11 @@ -1406,9 +1403,8 @@ \subsubsection{Fault Constitutive Models} \propertyitem{force\_healing}{Flag indicating whether healing (cumalative slip state variable reset to zero) is forced after every time step.} \end{inventory} -An example of setting the properties for the slip-weakening friction -component in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{SlipWeakening} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault] friction = pylith.friction.SlipWeakening ; Change from the default @@ -1495,9 +1491,7 @@ \subsubsection{Fault Constitutive Models} the \texttt{force\_healing} parameter, because this friction model was developed for dynamic simulations. -An example of setting the properties for the slip- and time-weakening friction -component in a \filename{.cfg} file is: -\begin{cfg} +\begin{cfg}[\object{SlipWeakeningTime} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault] friction = pylith.friction.SlipWeakeningTime ; Change from the default \end{cfg} @@ -1562,9 +1556,7 @@ \subsubsection{Fault Constitutive Models} the \texttt{force\_healing} parameter, because this friction model was developed for dynamic simulations. -An example of setting the properties for this slip- and time-weakening friction -component in a \filename{.cfg} file is: -\begin{cfg} +\begin{cfg}[\object{SlipWeakeningTimeStable} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault] friction = pylith.friction.SlipWeakeningTimeStable ; Change from the default \end{cfg} @@ -1646,9 +1638,8 @@ \subsubsection{Fault Constitutive Models} occurs, $V_{linear}$. In quasi-static simulations it should be about one order of magnitude larger than absolute tolerance in solve.} \end{inventory} -An example of setting the properties for the rate- and state-friction -component in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{RateStateAgeing} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces.fault] friction = pylith.friction.RateStateAgeing ; Change from the default

      friction.linear_slip_rate

      = 1.0e-12 ; default value @@ -1695,9 +1686,8 @@ \subsection{Slip Impulses for Green's Functions} \facilityitem{db\_impulse\_amplitude}{Spatial database for amplitude of slip impulse (scalar field). Default is \object{SimpleDB}.} \end{inventory} -An example of setting the properties and facilities for \object{FaultCohesiveImpulses} -in a \filename{.cfg} file is: -\begin{cfg} + +\begin{cfg}[\object{FaultCohesiveImpulses} parameters in a \filename{cfg} file] [pylithapp.problem.interfaces] fault = pylith.faults.FaultCohesiveImpulses ; Change from the default @@ -1747,20 +1737,13 @@ \section{Gravitational Body Forces} the vector might be specified as (0, -1, 0). The vector still has three components, although the extra component is not used. -Gravity is turned off by default. To include gravitational effects -in a simulation, you can turn it on as follows: -\begin{cfg} +\begin{cfg}[Turning on gravitational body forces in a \filename{cfg} file] [pylithapp.timedependent] gravity_field = spatialdata.spatialdb.GravityField -\end{cfg} -By simply adding this flag, the default gravity field values will -be used and a \facility{gravity\_field} component will be assigned for -the problem. The default values may be changed by altering the properties -of \facility{gravity\_field}: -\begin{cfg} + [pylithapp.timedependent.gravity_field] -

      acceleration

      = 100.0*m*s**-2 -

      gravity_dir

      = [0, -1, 0] +

      acceleration

      = 100.0*m*s**-2 ; default is 9.80665*m*s**-2 +

      gravity_dir

      = [0, -1, 0] ; default is [0, 0, -1] \end{cfg} Examples using gravity are described in Sections \vref{sec:example:3dhex8:gravity} and \vref{sec:example:grav2d}. diff --git a/doc/userguide/examples/3dhex8.tex b/doc/userguide/examples/3dhex8.tex index d1d89e0647..38091492c1 100644 --- a/doc/userguide/examples/3dhex8.tex +++ b/doc/userguide/examples/3dhex8.tex @@ -147,7 +147,7 @@ \subsection{Additional Common Information} us to specify different material types or material variations for the upper crust and lower crust, if desired. For now, we retain the default \object{ElasticIsotropic3D} material type for both materials. -This behavior will be overridden by example-specific\filename{.cfg} +This behavior will be overridden by example-specific \filename{cfg} files in some of the examples. Although the material groups are specified in \filename{pylithapp.cfg}, the physical properties for the material models are given in \filename{spatialdb/} diff --git a/doc/userguide/examples/3dhex8_dike.tex b/doc/userguide/examples/3dhex8_dike.tex index dac5faac02..af099474db 100644 --- a/doc/userguide/examples/3dhex8_dike.tex +++ b/doc/userguide/examples/3dhex8_dike.tex @@ -14,14 +14,14 @@ \subsubsection{Overview} This set of examples describes a problem where prescribed tensile tractions are imposed on a fault to mimic a dike intrusion. The example is contained in the directory \filename{examples/3d/hex8}, and the corresponding -\filename{.cfg} file is \filename{step20.cfg}. The example may be run +\filename{cfg} file is \filename{step20.cfg}. The example may be run as follows: \begin{shell} $ pylith step20.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in -the \filename{step20.cfg} file. The \filename{.cfg} file is extensively +the \filename{step20.cfg} file. The \filename{cfg} file is extensively documented, to provide detailed information on the various parameters. diff --git a/doc/userguide/examples/3dhex8_friction.tex b/doc/userguide/examples/3dhex8_friction.tex index 4d2a1e5416..022112153e 100644 --- a/doc/userguide/examples/3dhex8_friction.tex +++ b/doc/userguide/examples/3dhex8_friction.tex @@ -21,7 +21,7 @@ \subsubsection{Overview} the fault. Otherwise, there would be no frictional resistance. Fault friction generates nonlinear behavior, so we use the nonlinear solver. All of the examples are contained in the directory \filename{examples/3d/hex8}, -and the corresponding \filename{.cfg} files are \filename{step10.cfg}, +and the corresponding \filename{cfg} files are \filename{step10.cfg}, \filename{step11.cfg}, \filename{step12.cfg}, \filename{step13.cfg}, and \filename{step14.cfg}. Each example may be run as follows: \begin{shell} @@ -29,7 +29,7 @@ \subsubsection{Overview} \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in -the \filename{stepXX.cfg} file. Each \filename{.cfg} file is extensively +the \filename{stepXX.cfg} file. Each \filename{cfg} file is extensively documented, to provide detailed information on the various parameters. @@ -105,7 +105,7 @@ \subsubsection{Step11 - Static Friction (Slip) with Static Dirichlet Boundary Co are identical. To change the amount of shear displacement, we change the spatial database for the positive and negative x-faces to a \object{UniformDB}, and apply the altered values within the -\filename{.cfg} file: +\filename{cfg} file: \begin{cfg} # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos] diff --git a/doc/userguide/examples/3dhex8_gravity.tex b/doc/userguide/examples/3dhex8_gravity.tex index 8428106f94..f2b4398ca6 100644 --- a/doc/userguide/examples/3dhex8_gravity.tex +++ b/doc/userguide/examples/3dhex8_gravity.tex @@ -19,7 +19,7 @@ \subsubsection{Overview} demonstrates the usage of a finite strain formulation, which automatically invokes the nonlinear solver. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the -corresponding \filename{.cfg} files are \filename{step15.cfg}, +corresponding \filename{cfg} files are \filename{step15.cfg}, \filename{step16.cfg}, and \filename{step17.cfg}. Each example may be run as follows: \begin{shell} @@ -28,7 +28,7 @@ \subsubsection{Overview} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in the \filename{stepXX.cfg} file. Each -\filename{.cfg} file is extensively documented, to provide detailed +\filename{cfg} file is extensively documented, to provide detailed information on the various parameters. diff --git a/doc/userguide/examples/3dhex8_greensfns.tex b/doc/userguide/examples/3dhex8_greensfns.tex index 3b066b9113..4038383e57 100644 --- a/doc/userguide/examples/3dhex8_greensfns.tex +++ b/doc/userguide/examples/3dhex8_greensfns.tex @@ -17,7 +17,7 @@ \subsubsection{Overview} This example describes a problem where we generate a set of Green's functions that could be used in an inversion. The example is contained in the directory \filename{examples/3d/hex8}, and the corresponding -\filename{.cfg} file is \filename{step21.cfg}. The example may be run +\filename{cfg} file is \filename{step21.cfg}. The example may be run as follows: \begin{shell} $ pylith step21.cfg --problem=pylith.problems.GreensFns @@ -25,19 +25,19 @@ \subsubsection{Overview} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg} and \filename{greensfns.cfg}, and then override or augment them with the additional parameters in the -\filename{step21.cfg} file. The \filename{.cfg} files are extensively +\filename{step21.cfg} file. The \filename{cfg} files are extensively documented, to provide detailed information on the various parameters. \subsubsection{Step21 - Green's Function Generation} -This problem makes use of two \filename{.cfg} files that are read by +This problem makes use of two \filename{cfg} files that are read by default -- \filename{pylithapp.cfg} and \filename{greensfns.cfg}. The \filename{greensfns.cfg} file is read automatically because we have changed the problem type to \object{GreensFns} (as opposed to the default \object{TimeDependent} problem type). The facility name then becomes \facility{greensfns}, and PyLith will therefore search for a -\filename{.cfg} file matching the name of the facility. The +\filename{cfg} file matching the name of the facility. The \filename{greensfns.cfg} file contains settings that are specific to the \object{GreensFns} problem type: \begin{cfg} diff --git a/doc/userguide/examples/3dhex8_quasistatic.tex b/doc/userguide/examples/3dhex8_quasistatic.tex index 1042416e7f..0c69d490df 100644 --- a/doc/userguide/examples/3dhex8_quasistatic.tex +++ b/doc/userguide/examples/3dhex8_quasistatic.tex @@ -31,7 +31,7 @@ \subsubsection{Overview} viscoelastic and Drucker-Prager elastoplastic). Some of the examples also demonstrate the usage of HDF5 output, which is an alternative to the default VTK output. All of the examples are contained in the -directory \filename{examples/3d/hex8}, and the corresponding \filename{.cfg} +directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step04.cfg}, \filename{step05.cfg}, \filename{step06.cfg}, \filename{step07.cfg}, \filename{step08.cfg}, and \filename{step09.cfg}. Each example may be run as follows: @@ -40,7 +40,7 @@ \subsubsection{Overview} \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in -the \filename{stepXX.cfg} file. Each \filename{.cfg} file is extensively +the \filename{stepXX.cfg} file. Each \filename{cfg} file is extensively documented, to provide detailed information on the various parameters. @@ -292,7 +292,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema Xdmf files describing the contents of the HDF5 files, which allows the files to be read easily by applications such as ParaView. Since VTK output is still the default, we must change the value from the -default. Also note that the filename suffix is \filename{.h5}: +default. Also note that the filename suffix is \filename{h5}: \begin{cfg} # Give basename for output of solution over domain. [pylithapp.problem.formulation.output.domain] @@ -400,7 +400,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema along with slip time information. When we have run the simulation, the output HDF5 and Xdmf files will be contained in \filename{examples/3d/hex8/output} (all with a prefix of \filename{step06}). To open the files in ParaView, -the Xdmf (\filename{.xmf}) files should be opened, as these files describe +the Xdmf (\filename{xmf}) files should be opened, as these files describe the HDF5 data structure. Results using ParaView are shown in Figure \vref{fig:example:3dhex8:step06:displacement}. @@ -489,7 +489,7 @@ \subsubsection{Step07 - Dirichlet Velocity Boundary Conditions with Time-Depende When we have run the simulation, the output HDF5 and Xdmf files will be contained in \filename{examples/3d/hex8/output} (all with a prefix of \filename{step07}). As for example step06, make sure to open the -\filename{.xmf} files rather than the \filename{.h5} files. Results using +\filename{xmf} files rather than the \filename{h5} files. Results using ParaView are shown in Figure \vref{fig:example:3dhex8:step07:displacement}. \begin{figure} diff --git a/doc/userguide/examples/3dhex8_static.tex b/doc/userguide/examples/3dhex8_static.tex index 84348c05e1..f9ec0492a7 100644 --- a/doc/userguide/examples/3dhex8_static.tex +++ b/doc/userguide/examples/3dhex8_static.tex @@ -23,14 +23,14 @@ \subsubsection{Overview} of different types of boundary conditions in PyLith, as well as demonstrating the use of a kinematic fault for a static problem. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the -corresponding \filename{.cfg} files are \filename{step01.cfg}, \filename{step02.cfg}, +corresponding \filename{cfg} files are \filename{step01.cfg}, \filename{step02.cfg}, and \filename{step03.cfg}. Each example may be run as follows: \begin{shell} $ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in -the \filename{stepXX.cfg} file. Each \filename{.cfg} file is extensively +the \filename{stepXX.cfg} file. Each \filename{cfg} file is extensively documented to provide detailed information on the various parameters. diff --git a/doc/userguide/examples/3dhex8_surfload.tex b/doc/userguide/examples/3dhex8_surfload.tex index be18777165..8c150a4b0b 100644 --- a/doc/userguide/examples/3dhex8_surfload.tex +++ b/doc/userguide/examples/3dhex8_surfload.tex @@ -18,14 +18,14 @@ \subsubsection{Overview} load in a quasi-static problem. The second problem also includes output of the solution at user-defined locations. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the corresponding -\filename{.cfg} files are \filename{step18.cfg} and \filename{step19.cfg}. +\filename{cfg} files are \filename{step18.cfg} and \filename{step19.cfg}. Each example may be run as follows: \begin{shell} $ pylith stepXX.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in -the \filename{stepXX.cfg} file. Each \filename{.cfg} file is extensively +the \filename{stepXX.cfg} file. Each \filename{cfg} file is extensively documented, to provide detailed information on the various parameters. diff --git a/doc/userguide/examples/3dtet4.tex b/doc/userguide/examples/3dtet4.tex index b8865fb91b..a06d21c51c 100644 --- a/doc/userguide/examples/3dtet4.tex +++ b/doc/userguide/examples/3dtet4.tex @@ -75,9 +75,9 @@ \subsection{Mesh Generation and Description} and \filename{tet4\_1000m\_binary.pset}. The ASCII files are not actually needed, but we create them so users can see what is contained in the files. These files may also be used instead of the binary versions, -if desired. The \filename{.gmv} files define the mesh information, and +if desired. The \filename{gmv} files define the mesh information, and they may be read directly by the GMV \url{laws.lanl.gov/XCM/gmv/GMVHome.html} -mesh visualization package. The \filename{.pset} files specify the vertices +mesh visualization package. The \filename{pset} files specify the vertices corresponding to each set of vertices on a surface used in the problem, including the fault as well as external boundaries to which boundary conditions are applied. @@ -97,7 +97,7 @@ \subsection{Additional Common Information} In such cases it is generally useful to create a file named \filename{pylithapp.cfg} in the run directory, since this file is read automatically every time PyLith is run. Settings specific to a particular problem may -be placed in other \filename{.cfg} files, as described later, and then +be placed in other \filename{cfg} files, as described later, and then those files are placed on the command line. The settings contained in \filename{pylithapp.cfg} for this problem consist of: \begin{inventory} @@ -261,7 +261,7 @@ \subsection{Shear Displacement Example} given for a subset of the mesh corresponding to the ground surface. Also, the cells in this file are one dimension lower than the cells described in \filename{step01\_t0000000.vtk}, so they are -triangles rather than tetrahedra. All of the \filename{.vtk} files may +triangles rather than tetrahedra. All of the \filename{vtk} files may be used with a number of visualization packages. If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:3dtet4:shear}, which was generated using ParaView. @@ -443,7 +443,7 @@ \subsection{Kinematic Fault Slip Example} for the cohesive cell. The final file, \filename{step03-fault\_info.vtk}, provides information such as the normal direction, final slip, and slip time for each vertex on the -fault. All of the \filename{.vtk} files may be used with a number of +fault. All of the \filename{vtk} files may be used with a number of visualization packages. If the problem ran correctly, you should be able to generate a figure such as Figure\vref{fig:3dtet:dislocation}, which was generated using ParaView. diff --git a/doc/userguide/examples/shearwave.tex b/doc/userguide/examples/shearwave.tex index 5306d045e6..eb1d56fc78 100644 --- a/doc/userguide/examples/shearwave.tex +++ b/doc/userguide/examples/shearwave.tex @@ -177,7 +177,7 @@ \subsection{Kinematic Fault (Prescribed Slip)} the tri3 and tet4 simulations. In contrast to the tri3, tet4, and hex8 shear wave examples which only contained a single simulation in a directory, in this example we consider several different simulations. -Consequently, we separate the parameters into multiple \filename{.cfg} +Consequently, we separate the parameters into multiple \filename{cfg} files. The common parameters are placed in \filename{pylithapp.cfg} with the parameters specific to the kinematic fault (prescribed rupture) example in \filename{prescribedrup.cfg}. To run the problem, diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index ab28af5716..8582587674 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -289,7 +289,7 @@ \subsubsection{Materials} are linear, isotropic elastic and cases where the crust and wedge are linear, isotropic elastic but the slab and mantle are linear Maxwell viscoelastic. As a result, we put the parameters for these two cases -in separate \filename{.cfg} files with \filename{mat\_elastic.cfg} for +in separate \filename{cfg} files with \filename{mat\_elastic.cfg} for the case with purely elastic models and \filename{mat\_viscoelastic.cfg} for the case with a mix of elastic and viscoelastic models. Each of these files specifies the bulk @@ -458,7 +458,7 @@ \subsection{Step 1: Axial Compression} progress of the simulation and estimated time of completion (\filename{output/step01-progress.txt}), and the filenames for the HDF5 files (the corresponding Xdmf files will use the same filename -with the \filename{.xmf} suffix). +with the \filename{xmf} suffix). We run this example by typing \begin{shell} diff --git a/doc/userguide/examples/twoquad4.tex b/doc/userguide/examples/twoquad4.tex index 77ca7a217e..620c19c020 100644 --- a/doc/userguide/examples/twoquad4.tex +++ b/doc/userguide/examples/twoquad4.tex @@ -57,7 +57,7 @@ \subsection{Additional Common Information} information. As in the previous examples, we place this information in \filename{pylithapp.cfg}, since this file is read automatically every time PyLith is run. Settings specific to a particular problem may -be placed in other \filename{.cfg} files, as described later, and then +be placed in other \filename{cfg} files, as described later, and then those files are placed on the command line. diff --git a/doc/userguide/examples/twotri3.tex b/doc/userguide/examples/twotri3.tex index 1f28c39231..31a58f73ba 100644 --- a/doc/userguide/examples/twotri3.tex +++ b/doc/userguide/examples/twotri3.tex @@ -58,7 +58,7 @@ \subsection{Additional Common Information} create a file named \filename{pylithapp.cfg} in the working directory, since this file is read automatically every time PyLith is run. Settings specific to a particular problem may be placed in other -\filename{.cfg} files, as described later, and then those files are +\filename{cfg} files, as described later, and then those files are placed on the command line. The settings contained in \filename{pylithapp.cfg} for this problem consist of: \begin{inventory} @@ -137,7 +137,7 @@ \subsection{Axial Displacement Example} and strain values for each cell. The final file (\filename{axialdisp-statevars\_info.vtk}) gives the material properties used for the problem. Since we have not specified which properties to write, the default properties (\texttt{mu}, -\texttt{lambda}, \texttt{density}) are written. All of the \filename{.vtk} +\texttt{lambda}, \texttt{density}) are written. All of the \filename{vtk} files may be used with a number of visualization packages. If the problem ran correctly, you should be able to generate a figure such as Figure \vref{fig:twotri3-axial}, which was generated using ParaView. diff --git a/doc/userguide/extending/extending.tex b/doc/userguide/extending/extending.tex index 854abebd28..870b70f986 100644 --- a/doc/userguide/extending/extending.tex +++ b/doc/userguide/extending/extending.tex @@ -20,13 +20,13 @@ \chapter{Extending PyLith} \begin{enumerate} \item Setting up the source files for the component or set of components based on the templates. -\item Edit the Python source file (\filename{.py}) for the component. +\item Edit the Python source file (\filename{py}) for the component. \begin{enumerate} \item Define the user-specified properties and facilities. \item Transfer the user-specified data from the Python object to the corresponding C++ object via calls to the SWIG interface object. \end{enumerate} -\item Edit the C++ header (\filename{.hh}) and implementation files (\filename{.cc}) +\item Edit the C++ header (\filename{hh}) and implementation files (\filename{cc}) for the component. \begin{enumerate} \item Implement the methods required to satisfy the interface definition diff --git a/doc/userguide/install/install.tex b/doc/userguide/install/install.tex index a540e898da..682b86437f 100644 --- a/doc/userguide/install/install.tex +++ b/doc/userguide/install/install.tex @@ -437,7 +437,7 @@ \subsection{Running without a Batch System} $ pylith example.cfg mymachines.cfg \end{shell} This strategy gives you the flexibility to create an assortment of -\filename{.cfg} files (with one \filename{.cfg} file for each machine +\filename{cfg} files (with one \filename{cfg} file for each machine list) which can be easily paired with different parameter files. If your machine list does not change often, you may find it more convenient diff --git a/doc/userguide/materials/materials.tex b/doc/userguide/materials/materials.tex index 1ce8e6a960..1347a94c26 100644 --- a/doc/userguide/materials/materials.tex +++ b/doc/userguide/materials/materials.tex @@ -10,7 +10,7 @@ \section{Specifying Material Properties} \item In the mesh generation process, assign a material identifier to each cell. \item Define material property groups corresponding to each material identifier. -\item Set the parameters for each material group using \filename{.cfg} and/or command-line arguments. +\item Set the parameters for each material group using \filename{cfg} and/or command-line arguments. \item Specify the spatial variation in material property parameters using a spatial database file. \end{enumerate} @@ -42,7 +42,7 @@ \subsection{Material Property Groups} arrays of components, and it was necessary to predefine these arrays. More recent versions of Pythia do support this, however, and it is now possible to define material property groups using a -\filename{.cfg} file or on the command-line. User-defined containers +\filename{cfg} file or on the command-line. User-defined containers are no longer necessary, and the predefined containers are no longer available (or necessary). If a set of material groups is not specified, a single material model is used for the entire problem. See @@ -75,7 +75,7 @@ \subsection{Material Parameters} over each cell.} \end{inventory} -\begin{cfg}[Parameters for two materials in a \filename{.cfg} file] +\begin{cfg}[Parameters for two materials in a \filename{cfg} file] [pylithapp.timedependent]

      materials

      = [elastic, viscoelastic] @@ -256,7 +256,7 @@ \subsubsection{Specification of Initial State Variables} 2D stress components ($\sigma_{xx}$, $\sigma_{yy}$, and $\sigma_{xy}$) and an additional database containing the out of plane stress and initial values for all other state variables for the given material. -The complete initial stress field may then be defined in the \filename{.cfg} +The complete initial stress field may then be defined in the \filename{cfg} file as: \begin{cfg} [pylithapp.problem.materials.powerlaw] @@ -1537,7 +1537,7 @@ \subsubsection{Drucker-Prager Elastoplastic With No Hardening (Perfectly Plastic the tensile strength (default is false).} \end{inventory} -\begin{cfg}[\object{DruckerPrager3D} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{DruckerPrager3D} parameters in a \filename{cfg} file] [pylithapp.timedependent]

      materials

      = [plastic] materials.plastic = pylith.materials.DruckerPrager3D diff --git a/doc/userguide/runpylith/databases.tex b/doc/userguide/runpylith/databases.tex index 9994ce3368..2dd41dcd76 100644 --- a/doc/userguide/runpylith/databases.tex +++ b/doc/userguide/runpylith/databases.tex @@ -7,9 +7,9 @@ \section{Databases for Boundaries, Interfaces, and Material Properties} provides labels defining sets of vertices to which boundary conditions or fault conditions will be applied, as well as cell labels that will be used to define the material type of each cell. For boundary conditions, -the \filename{.cfg} file is used to associate boundary condition types +the \filename{cfg} file is used to associate boundary condition types and spatial databases with each vertex group (see Chapter \vref{cha:boundary:interface:conditions}). -For materials, the \filename{.cfg} file is used to associate material +For materials, the \filename{cfg} file is used to associate material types and spatial databases with cells identified by the material identifier (see Figure \vref{fig:material:models}). @@ -74,7 +74,7 @@ \subsection{\object{SimpleDB} Spatial Database} \object{SimpleDB} uses a simple ASCII file to specify the variation of values (e.g., displacement field, slip field, physical properties) in space. The file format is described in Section \vref{sec:format:SimpleIOAscii}. The examples in Chapter \vref{cha:examples} use \object{SimpleDB} files to specify the values for the boundary conditions, physical properties, and fault slip. As in the other Pyre objects, spatial database objects contain parameters -that can be set from the command line or using \filename{.cfg} +that can be set from the command line or using \filename{cfg} files. The properties and facilities for a spatial database are: \begin{inventory} \propertyitem{label}{Label for the database, which is used in diagnostic messages.} @@ -85,7 +85,7 @@ \subsection{\object{SimpleDB} Spatial Database} \propertyitem{iohandler.filename}{Filename for the spatial database.} \end{inventory} -\begin{cfg}[\object{SimpleDB} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{SimpleDB} parameters in a \filename{cfg} file]

      label

      = Material properties

      query_type

      = linear

      iohandler.filename

      = mydb.spatialdb @@ -96,26 +96,26 @@ \subsection{\object{UniformDB} Spatial Database} The \object{SimpleDB} spatial database is quite general, but when the values are uniform, it is often easier to use the \object{UniformDB} spatial database instead. With the \object{UniformDB}, you specify the values directly either -on the command line or in a parameter-setting (\filename{.cfg}) file. +on the command line or in a parameter-setting (\filename{cfg}) file. On the other hand, if the values are used in more than one place, it is easier to place the values in a \object{SimpleDB} file, because they can then be referred to using the filename of the spatial database rather than having to repeatedly list all of the values on the command -line or in a parameter-setting (\filename{.cfg}) file. The properties +line or in a parameter-setting (\filename{cfg}) file. The properties for a \object{UniformDB} are: \begin{inventory} \propertyitem{values}{Array of names of values in spatial database.} \propertyitem{data}{Array of values in spatial database.} \end{inventory} -\begin{cfg}[\object{UniformDB} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{UniformDB} parameters in a \filename{cfg} file] [pylithapp.timedependent.materials.material]

      db_properties

      = spatialdata.spatialdb.UniformDB ; Set the db to a UniformDB

      db_properties.values

      = [vp, vs, density] ; Set the names of the values in the database

      db_properties.data

      = [5773.5*m/s, 3333.3*m/s, 2700.0*kg/m**3] ; Set the values in the database} \end{cfg} This example specifies the physical properties of a linearly elastic, -isotropic material in a \filename{.cfg} file. The data values are +isotropic material in a \filename{cfg} file. The data values are dimensioned with the appropriate units using Python syntax. @@ -146,7 +146,7 @@ \subsection{\object{SimpleGridDB} Spatial Database} \vref{sec:format:SimpleGridDB}. As in the other Pyre objects, spatial database objects contain parameters -that can be set from the command line or using \filename{.cfg} +that can be set from the command line or using \filename{cfg} files. The parameters for a spatial database are: \begin{inventory} \propertyitem{label}{Label for the database, which is used in @@ -156,7 +156,7 @@ \subsection{\object{SimpleGridDB} Spatial Database} \propertyitem{filename}{Filename for the spatial database.} \end{inventory} -\begin{cfg}[\object{SimpleGridDB} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{SimpleGridDB} parameters in a \filename{cfg} file]

      label

      = Material properties

      query_type

      = linear

      filename

      = mydb_grid.spatialdb @@ -190,7 +190,7 @@ \subsection{SCEC CVM-H Spatial Database (\object{SCECCVMH})} below this elevation remains undistorted).} \end{inventory} -\begin{cfg}[\object{SCECCVMH} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{SCECCVMH} parameters in a \filename{cfg} file] [pylithapp.timedependent.materials.material]

      db_properties

      = spatialdata.spatialdb.SCECCVMH ; Set the database to the SCEC CVM-H @@ -215,7 +215,7 @@ \subsection{\object{CompositeDB} Spatial Database} inelastic physical properties. We can use the \object{CompositeDB} spatial database for these cases. -\begin{cfg}[\object{CompositeDB} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{CompositeDB} parameters in a \filename{cfg} file] [pylithapp.timedependent.materials.maxwell]

      label

      = Maxwell material

      id

      = 1 @@ -260,7 +260,7 @@ \subsection{\object{TimeHistory} Database} database. The file format is described in Section \vref{sec:format:TimeHistoryIO}. As in the other Pyre objects, spatial database objects contain parameters -that can be set from the command line or using \filename{.cfg} +that can be set from the command line or using \filename{cfg} files. The parameters for a spatial database are: \begin{inventory} \propertyitem{label}{Label for the time history database, which is used in diagnostic @@ -268,7 +268,7 @@ \subsection{\object{TimeHistory} Database} \propertyitem{filename}{Filename for the time history database.} \end{inventory} -\begin{cfg}[\object{TimeHistory} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{TimeHistory} parameters in a \filename{cfg} file]

      label

      = Displacement time history

      filename

      = mytimehistory.timedb \end{cfg} diff --git a/doc/userguide/runpylith/definesim.tex b/doc/userguide/runpylith/definesim.tex index b8ebfe6aa7..2d4f6c47ec 100644 --- a/doc/userguide/runpylith/definesim.tex +++ b/doc/userguide/runpylith/definesim.tex @@ -25,7 +25,7 @@ \subsection{Setting PyLith Parameters} There are several methods for setting input parameters for the \filename{pylith} executable: via the command line or by using a text -file in \filename{.cfg} or \filename{.pml} format. Both facilities and +file in \filename{cfg} or \filename{pml} format. Both facilities and properties have default values provided, so you only need to set values when you want to deviate from the default behavior. @@ -99,7 +99,7 @@ \subsubsection{Using a {\ttfamily .cfg} File} Entering all those parameters via the command line involves the risk of typographical errors. You will generally find it easier to collect parameters into a -\filename{.cfg} file. The file is composed of one or more sections +\filename{cfg} file. The file is composed of one or more sections which are formatted as follows: \begin{cfg} [pylithapp.COMPONENT1.COMPONENT2] @@ -110,13 +110,13 @@ \subsubsection{Using a {\ttfamily .cfg} File}

      PROPERTY2

      = VALUE2 ; this is another comment \end{cfg} -\tip{We strongly recommend that you use \filename{.cfg} files for your +\tip{We strongly recommend that you use \filename{cfg} files for your work. The files are syntax-highlighted in the vim editor.} \subsubsection{Using a {\ttfamily.pml} File} -A \filename{.pml} file is an XML file that specifies parameter values +A \filename{pml} file is an XML file that specifies parameter values in a highly structured format. It is composed of nested sections which are formatted as follows: \begin{lstlisting}[basicstyle=\ttfamily,frame=tb]{language=xml} @@ -128,14 +128,14 @@ \subsubsection{Using a {\ttfamily.pml} File} \end{lstlisting} XML files are intended to be read and written by machines, not edited -manually by humans. The \filename{.pml} file format is intended for +manually by humans. The \filename{pml} file format is intended for applications in which PyLith input files are generated by another program, e.g., a GUI, web application, or a high-level structured editor. This file format will not be discussed further here, but if -you are interested in using \filename{.pml} files, note that \filename{.pml} -files and \filename{.cfg} files can be used interchangeably; in the -following discussion, a file with a \filename{.pml} extension can be -substituted anywhere a \filename{.cfg} file can be used. +you are interested in using \filename{pml} files, note that \filename{pml} +files and \filename{cfg} files can be used interchangeably; in the +following discussion, a file with a \filename{pml} extension can be +substituted anywhere a \filename{cfg} file can be used. \subsubsection{Specification and Placement of Configuration Files} @@ -157,7 +157,7 @@ \subsubsection{Specification and Placement of Configuration Files} \end{enumerate} \important{The Pyre framework will search these directories for - \filename{.cfg} files matching the names of components (for example, + \filename{cfg} files matching the names of components (for example, \filename{timedependent.cfg}, \filename{faultcohesivekin.cfg}, \filename{greensfns.cfg}, \filename{pointforce.cfg}, etc) and will attempt to assign all parameters in those files to the respective @@ -188,7 +188,7 @@ \subsubsection{Specification and Placement of Configuration Files} $ pylith axialdisp.cfg \end{shell} If you want to see what settings are being used, you can either examine -the \filename{.cfg} files, or use the help flags as described above: +the \filename{cfg} files, or use the help flags as described above: \begin{shell} # Show components for the 'problem' facility. $ pylith axialdisp.cfg --problem.help-components @@ -204,7 +204,7 @@ \subsubsection{Specification and Placement of Configuration Files} \end{shell} This is generally a more useful way of determining problem settings, since it includes default values as well as those that have been specified -in the \filename{.cfg} file. +in the \filename{cfg} file. \subsubsection{List of PyLith Parameters ({\ttfamily pylithinfo})} @@ -362,7 +362,7 @@ \subsubsection{\object{Distributor}} \facilityitem{data\_writer}{Writer for partition information (default is \object{DataWriterVTK} for VTK output).} \end{inventory} -\begin{cfg}[\object{Distributor} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{Distributor} parameters in a \filename{cfg} file] [pylithapp.mesh_generator.distributor]

      partitioner

      = chaco ; Options are 'chaco' (default) and 'parmetis'. \end{cfg} @@ -431,7 +431,7 @@ \subsection{Problem Specification (\facility{problem})} simulation.} \end{inventory} -\begin{cfg}[Problem parameters in a \filename{.cfg} file] +\begin{cfg}[Problem parameters in a \filename{cfg} file] [pylithapp.timedependent]

      dimension

      = 3 normalizer = spatialdata.units.NondimElasticQuasistatic @@ -459,7 +459,7 @@ \subsubsection{Nondimensionalization (\facility{normalizer})} \propertyitem{relaxation\_time}{Relaxation time to nondimensionalize time (default is 1.0 year).} \end{inventory} -\begin{cfg}[\object{NondimElasticQuasistatic} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{NondimElasticQuasistatic} parameters in a \filename{cfg} file] [pylithapp.timedependent.normalizer]

      length_scale

      = 1.0*km

      shear_modulus

      = 3.0e+10*Pa @@ -475,7 +475,7 @@ \subsubsection{Nondimensionalization (\facility{normalizer})} \propertyitem{wave\_period}{Period of seismic waves used to nondimensionalize time (default is 1.0 s).} \end{inventory} -\begin{cfg}[\object{NondimElasticDynamic} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{NondimElasticDynamic} parameters in a \filename{cfg} file] [pylithapp.timedependent.normalizer]

      shear_wave_speed

      = 3.0*km/s

      mass_density

      = 3.0e+3*kg/m**3 @@ -537,7 +537,7 @@ \subsection{PETSc Settings (\facility{petsc})} this permits solving the linear system with a trivial solver so we do not use a PETSc solver in this case (see Section \vref{sec:solvers}). -PETSc options can be set in \filename{.cfg} files in sections +PETSc options can be set in \filename{cfg} files in sections beginning with \texttt{[pylithapp.petsc]}. The options of primary interest in the case of PyLith are shown in Table \vref{tab:petsc:options:defaults}. PETSc options are used to control diff --git a/doc/userguide/runpylith/formulation.tex b/doc/userguide/runpylith/formulation.tex index 0991d55f91..99f997b100 100644 --- a/doc/userguide/runpylith/formulation.tex +++ b/doc/userguide/runpylith/formulation.tex @@ -55,7 +55,7 @@ \section{Time-Dependent Problem (\facilityshape{formulation})} equation.} \end{inventory} -\begin{cfg}[\object{TimeDependent} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{TimeDependent} parameters in a \filename{cfg} file] [pylithapp.timedependent] formulation = pylith.problems.Implicit ; default progres_monitor = pylith.problems.ProgressMonitorTime ; default @@ -86,7 +86,7 @@ \subsection{Time-Stepping Formulation} to a file for analysis (default is PETSc binary).} \end{inventory} -\begin{cfg}[Time-stepping formulation parameters in a \filename{.cfg} file] +\begin{cfg}[Time-stepping formulation parameters in a \filename{cfg} file] [pylithapp.timedependent.formulation]

      matrix_type

      = sbaij ; Non-symmetric sparse matrix is 'aij'

      view_jacobian

      = false @@ -117,7 +117,7 @@ \subsection{Numerical Damping in Explicit Time Stepping} artificial viscosity is 0.1. We have found values in the range 0.1-0.4 sufficiently suppress numerical noise while not excessively reducing the peak velocity. An example of setting the normalized artificial -viscosity in a \filename{.cfg} file is +viscosity in a \filename{cfg} file is \begin{cfg} [pylithapp.timedependent.formulation]

      norm_viscosity

      = 0.2 @@ -177,7 +177,7 @@ \subsubsection{Uniform, User-Specified Time Step (\object{TimeStepUniform})} \propertyitem{dt}{Time step for simulation.} \end{inventory} -\begin{cfg}[\object{TimeStepUniform} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{TimeStepUniform} parameters in a \filename{cfg} file] [pylithapp.problem.formulation]

      time_step

      = pylith.problems.TimeStepUniform ; Default value @@ -205,7 +205,7 @@ \subsubsection{Nonuniform, User-Specified Time Step (\object{TimeStepUser})} using last time-step size for any time remaining.} \end{inventory} -\begin{cfg}[\object{TimeStepUser} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{TimeStepUser} parameters in a \filename{cfg} file] [pylithapp.problem.formulation] time_step = pylith.problems.TimeStepUser ; Change the time step algorithm @@ -242,7 +242,7 @@ \subsubsection{Nonuniform, Automatic Time Step (\object{TimeStepAdapt})} is 2.0).} \end{inventory} -\begin{cfg}[\object{TimeStepAdapt} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{TimeStepAdapt} parameters in a \filename{cfg} file] [pylithapp.problem.formulation]

      time_step

      = pylith.problems.TimeStepAdapt ; Change the time step algorithm @@ -274,7 +274,7 @@ \section{Green's Functions Problem (\object{GreensFns})} \propertyitem{progress\_monitor}{Simple progress monitor via text file.} \end{inventory} -\begin{cfg}[\object{GreensFns} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{GreensFns} parameters in a \filename{cfg} file] [pylithapp] problem = pylith.problems.GreensFns ; Change problem type from the default @@ -313,7 +313,7 @@ \subsection{\object{ProgressMonitorTime}} \propertyitem{t\_units}{Units for simulation time in output.} \end{inventory} -\begin{cfg}[\object{ProgressMonitorTime} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{ProgressMonitorTime} parameters in a \filename{cfg} file] [pylithapp.problem.progressmonitor]

      update_percent

      = 5.0 ; default

      filename

      = progress.txt ; default @@ -332,7 +332,7 @@ \subsection{\object{ProgressMonitorStep}} \propertyitem{filename}{Name of output file.} \end{inventory} -\begin{cfg}[\object{ProgressMonitorStep} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{ProgressMonitorStep} parameters in a \filename{cfg} file] [pylithapp.problem.progressmonitor]

      update_percent

      = 5.0 ; default

      filename

      = progress.txt ; default diff --git a/doc/userguide/runpylith/output.tex b/doc/userguide/runpylith/output.tex index a4a37d3de0..a496e405a8 100644 --- a/doc/userguide/runpylith/output.tex +++ b/doc/userguide/runpylith/output.tex @@ -61,7 +61,7 @@ \subsection{Output Manager} \vref{sub:cell:field:filters}).} \end{inventory} -\begin{cfg}[\object{OutputManager} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{OutputManager} parameters in a \filename{cfg} file] [pylithapp.timedependent.materials.elastic.output]

      output_freq

      = time_step

      time_step

      = 1.0*yr @@ -203,7 +203,7 @@ \subsection{HDF5/Xdmf Output (\object{DataWriterHDF5}, \object{DataWriterHDF5Ext Format, \url{www.xdmf.org}) metadata file that provides this information. This file is written when PyLith closes the HDF5 file at the end of the simulation. In order to visualize the datasets in an HDF5 file, -one simply opens the corresponding Xdmf file (the extension is \filename{.xmf}) +one simply opens the corresponding Xdmf file (the extension is \filename{xmf}) in ParaView or Visit. The Xdmf file contains the relative path to the HDF5 file so the files can be moved but must be located together in the same directory. @@ -243,7 +243,7 @@ \subsection{HDF5/Xdmf Output (\object{DataWriterHDF5}, \object{DataWriterHDF5Ext that the use of external data files results in one data file per dataset in addition to the HDF5 and Xdmf files. The external data files use the name of the HDF5 file with the dataset name added to the -prefix and the \filename{.h5} suffix replaced by \filename{.dat}. The +prefix and the \filename{h5} suffix replaced by \filename{dat}. The HDF5 files include relative paths to the external data files, so these files can also be moved, but they, too, must be kept together in the same directory. This provides a more robust method of output because @@ -284,7 +284,7 @@ \subsubsection{Parameters} the same prefix).} \end{inventory} -\begin{cfg}[\object{DataWriterHDF5Ext} parameters in a \filename{.cfg} file] +\begin{cfg}[\object{DataWriterHDF5Ext} parameters in a \filename{cfg} file] [pylithapp.timedependent.domain.output]

      output_freq

      = time_step

      time_step

      = 1.0*yr diff --git a/doc/userguide/runpylith/parametersgui.tex b/doc/userguide/runpylith/parametersgui.tex index a8e6d27537..3346fc7d77 100644 --- a/doc/userguide/runpylith/parametersgui.tex +++ b/doc/userguide/runpylith/parametersgui.tex @@ -36,7 +36,7 @@ \section{Running the Parameter Viewer} \subsection{Generate the parameter JSON file} The parameter viewer uses a JSON file with all of the parameters -collected from \filename{.cfg} files, command line arguments, etc as +collected from \filename{cfg} files, command line arguments, etc as input. This file can be generated using \filename{pylithinfo} (see Section \ref{sec:pylithinfo}) and, by default, it will be generated whenever a \filename{pylith} simulation is run. When using diff --git a/doc/userguide/runpylith/postprocessing.tex b/doc/userguide/runpylith/postprocessing.tex index d992fe1a49..9fe393f122 100644 --- a/doc/userguide/runpylith/postprocessing.tex +++ b/doc/userguide/runpylith/postprocessing.tex @@ -15,7 +15,7 @@ \subsection{\filename{pylith\_eqinfo}} at the centroid of the fault cells. In the future we plan to account for lateral variations in shear modulus across the fault when calculating the seismic moment. The Python script is a Pyre application, so its -parameters can be specified using \filename{.cfg} and command line arguments +parameters can be specified using \filename{cfg} and command line arguments just like PyLith. The Pyre properties and facilities include: \begin{inventory} \propertyitem{output\_filename}{Filename for output of slip information.} diff --git a/doc/userguide/runpylith/runpylith.tex b/doc/userguide/runpylith/runpylith.tex index 52e660f8b4..e6e8791e60 100644 --- a/doc/userguide/runpylith/runpylith.tex +++ b/doc/userguide/runpylith/runpylith.tex @@ -19,7 +19,7 @@ \chapter{Running PyLith} describe the type of problem to be run, solver information, time-stepping information, boundary conditions, materials, etc. This information can be provided from the command-line or by using a - \filename{.cfg.} + \filename{cfg} file. \item Databases specifying the material property values and boundary condition values to be used. Arbitrarily complex spatial variations in boundary and fault conditions and material properties may be From d07c2629ce5a52d213d5c0673fae4c11cc8fc2a9 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 14:43:01 -0700 Subject: [PATCH 211/216] Update code listings. --- doc/userguide/examples/3dhex8.tex | 5 +- doc/userguide/examples/3dhex8_dike.tex | 2 +- doc/userguide/examples/3dhex8_friction.tex | 37 ++++--- doc/userguide/examples/3dhex8_gravity.tex | 20 ++-- doc/userguide/examples/3dhex8_greensfns.tex | 4 +- doc/userguide/examples/3dhex8_quasistatic.tex | 70 +++++++----- doc/userguide/examples/3dhex8_static.tex | 28 +++-- doc/userguide/examples/3dhex8_surfload.tex | 14 ++- doc/userguide/examples/examples.tex | 2 +- doc/userguide/examples/grav2d.tex | 46 ++++---- doc/userguide/examples/greensfns2d.tex | 14 +-- doc/userguide/examples/subduction2d.tex | 14 +-- doc/userguide/examples/subduction3d.tex | 102 ++++++++---------- doc/userguide/examples/twohex8.tex | 2 +- doc/userguide/examples/twotri3.tex | 24 ++--- 15 files changed, 207 insertions(+), 177 deletions(-) diff --git a/doc/userguide/examples/3dhex8.tex b/doc/userguide/examples/3dhex8.tex index 38091492c1..2fe2822f39 100644 --- a/doc/userguide/examples/3dhex8.tex +++ b/doc/userguide/examples/3dhex8.tex @@ -115,16 +115,17 @@ \subsection{Additional Common Information} As in previous examples, we place this information in \filename{pylithapp.cfg}. Since these examples use a mesh from CUBIT, in this file we set the importer to \object{MeshIOCubit}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.mesh_generator] reader = pylith.meshio.MeshIOCubit [pylithapp.mesh_generator.reader]

      filename

      = mesh/box_hex8_1000m.exo \end{cfg} + This example differs from some earlier examples, because we specify two material groups: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.timedependent] materials = [upper_crust, lower_crust] diff --git a/doc/userguide/examples/3dhex8_dike.tex b/doc/userguide/examples/3dhex8_dike.tex index af099474db..95cc167ac3 100644 --- a/doc/userguide/examples/3dhex8_dike.tex +++ b/doc/userguide/examples/3dhex8_dike.tex @@ -44,7 +44,7 @@ \subsubsection{Step20 - Static Dike Intrusion} open; the default behavior for fault opening is a free surface (the two sides of the fault are completely uncoupled). The most important fault parameters for prescribing the tensile fault tractions are -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step20.cfg}] [pylithapp.timedependent.interfaces.fault]

      open_free_surface

      = False traction_perturbation = pylith.faults.TractPerturbation diff --git a/doc/userguide/examples/3dhex8_friction.tex b/doc/userguide/examples/3dhex8_friction.tex index 022112153e..387b16b08d 100644 --- a/doc/userguide/examples/3dhex8_friction.tex +++ b/doc/userguide/examples/3dhex8_friction.tex @@ -23,9 +23,22 @@ \subsubsection{Overview} All of the examples are contained in the directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step10.cfg}, \filename{step11.cfg}, \filename{step12.cfg}, \filename{step13.cfg}, and -\filename{step14.cfg}. Each example may be run as follows: +\filename{step14.cfg}. Run the examples as follows: \begin{shell} -$ pylith stepXX.cfg +# Step10 +$ pylith step10.cfg + +# Step11 +$ pylith step11.cfg + +# Step12 +$ pylith step12.cfg + +# Step13 +$ pylith step13.cfg + +# Step14 +$ pylith step14.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in @@ -41,7 +54,7 @@ \subsubsection{Step10 - Static Friction (Stick) with Static Dirichlet Boundary C to cause the fault to slip, so the solution is identical to that in example step01. As in previous examples involving faults, we must first provide an array defining the fault interfaces: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step10.cfg}] [pylithapp.timedependent] # Set interfaces to an array of 1 fault: 'fault'. interfaces = [fault] @@ -52,7 +65,7 @@ \subsubsection{Step10 - Static Friction (Stick) with Static Dirichlet Boundary C \end{cfg} We need to change the fault interface from the default (\object{FaultCohesiveKin}) to \object{FaultCohesiveDyn} and we set the friction model to use: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step10.cfg}] [pylithapp.timedependent.interfaces] fault = pylith.faults.FaultCohesiveDyn ; Change to dynamic fault interface. @@ -62,7 +75,7 @@ \subsubsection{Step10 - Static Friction (Stick) with Static Dirichlet Boundary C The \object{StaticFriction} model requires values for the coefficient of friction and the cohesion (see Section \vref{sec:fault:constitutive:models}). We provide both of these using a \object{UniformDB}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step10.cfg}] [pylithapp.timedependent.interfaces.fault] # Set static friction model parameters using a uniform DB. Set the # static coefficient of friction to 0.6 and cohesion to 0.0 Pa. @@ -106,7 +119,7 @@ \subsubsection{Step11 - Static Friction (Slip) with Static Dirichlet Boundary Co the spatial database for the positive and negative x-faces to a \object{UniformDB}, and apply the altered values within the \filename{cfg} file: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step11.cfg}] # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos]

      bc_dof

      = [0, 1] @@ -149,7 +162,7 @@ \subsubsection{Step12 - Static Friction with Quasi-Static Dirichlet Boundary Con conditions and run the simulation for 200 years. Once fault friction is overcome, the fault slips at a steady rate. To prevent convergence problems we set the time step size to a constant value of 5 years: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step12.cfg}] # Change the total simulation time to 200 years, and use a constant time # step size of 5 years. [pylithapp.timedependent.implicit.time_step] @@ -160,7 +173,7 @@ \subsubsection{Step12 - Static Friction with Quasi-Static Dirichlet Boundary Con along the x-axis (to maintain a compressive stress on the fault), and we apply velocity boundary conditions that yield a left-lateral sense of motion: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step12.cfg}] # Boundary condition on +x face -- Dirichlet [pylithapp.timedependent.bc.x_pos]

      bc_dof

      = [0,1] @@ -189,7 +202,7 @@ \subsubsection{Step12 - Static Friction with Quasi-Static Dirichlet Boundary Con For this example, we keep the same coefficient of friction as examples step10 and step11, but we include a cohesion of 2 MPa: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step12.cfg}] [pylithapp.timedependent.interfaces.fault] # Set static friction model parameters using a uniform DB. Set the # static coefficient of friction to 0.6 and cohesion to 2.0 MPa. @@ -221,7 +234,7 @@ \subsubsection{Step13 - Slip-Weakening Friction with Quasi-Static Dirichlet Boun boundary conditions. We first define the friction model for the simulation: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step13.cfg}] [pylithapp.timedependent.interfaces.fault] # Use the slip-weakening friction model. friction = pylith.friction.SlipWeakening @@ -261,7 +274,7 @@ \subsubsection{Step14 - Rate-and-State Friction with Quasi-Static Dirichlet Boun intial displacement and velocity boundary conditions. We first define the friction model for the simulation: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step14.cfg}] [pylithapp.timedependent.interfaces.fault] # Use the rate-and-state aging friction model. friction = pylith.friction.RateStateAgeing @@ -283,7 +296,7 @@ \subsubsection{Step14 - Rate-and-State Friction with Quasi-Static Dirichlet Boun \end{cfg} For this model, we also want to set the initial value of the state variable: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step14.cfg}] [pylithapp.timedependent.interfaces.fault] # Set spatial database for the initial value of the state variable. friction.db_initial_state = spatialdata.spatialdb.UniformDB diff --git a/doc/userguide/examples/3dhex8_gravity.tex b/doc/userguide/examples/3dhex8_gravity.tex index f2b4398ca6..5797cac890 100644 --- a/doc/userguide/examples/3dhex8_gravity.tex +++ b/doc/userguide/examples/3dhex8_gravity.tex @@ -20,10 +20,16 @@ \subsubsection{Overview} automatically invokes the nonlinear solver. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step15.cfg}, -\filename{step16.cfg}, and \filename{step17.cfg}. Each example may be -run as follows: +\filename{step16.cfg}, and \filename{step17.cfg}. Run the examples as follows: \begin{shell} -$ pylith stepXX.cfg +# Step15 +$ pylith step15.cfg + +# Step16 +$ pylith step16.cfg + +# Step17 +$ pylith step17.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the @@ -47,7 +53,7 @@ \subsubsection{Step15 - Gravitational Body Forces} We set the gravity field, which by default has values of 9.80655 $\unitfrac{m}{s^{2}}$ for acceleration and $\left[0,0,-1\right]$ for direction and time stepping implementation: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step15.cfg}] [pylithapp.timedependent] gravity_field = spatialdata.spatialdb.GravityField ; Set gravity field @@ -68,7 +74,7 @@ \subsubsection{Step15 - Gravitational Body Forces} \vref{sec:materials:formulation:generalized:Maxwell}), and use a \object{SimpleDB} to provide the properties. We also request the relevant properties and state variables for output: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step15.cfg}] # Change material type of lower crust to generalized Maxwell viscoelastic. [pylithapp.timedependent] materials.lower_crust = pylith.materials.GenMaxwellIsotropic3D @@ -116,7 +122,7 @@ \subsubsection{Step16 - Gravitational Body Forces with Initial Stresses} crust. Since the materials have the same density, we are able to use the same \object{SimpleDB} with a linear variation for both (see file \filename{examples/3d/hex8/spatialdb/initial\_stress.spatialdb}): -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step16.cfg}] # We must specify initial stresses for each material. # We provide a filename for the spatial database that gives the stresses, # and we change the query_type from the default 'nearest' to 'linear'. @@ -170,7 +176,7 @@ \subsubsection{Step17 - Gravitational Body Forces with Small Strain} large deformation formulation is nonlinear, PyLith automatically switches the solver from the default \object{SolverLinear} to \object{SolverNonlinear}. It is thus only necessary to change the formulation: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step17.cfg}] [pylithapp.timedependent] # Set the formulation for finite strain. The default solver will # automatically be switched to the nonlinear solver. diff --git a/doc/userguide/examples/3dhex8_greensfns.tex b/doc/userguide/examples/3dhex8_greensfns.tex index 4038383e57..da926f90bf 100644 --- a/doc/userguide/examples/3dhex8_greensfns.tex +++ b/doc/userguide/examples/3dhex8_greensfns.tex @@ -40,7 +40,7 @@ \subsubsection{Step21 - Green's Function Generation} \filename{cfg} file matching the name of the facility. The \filename{greensfns.cfg} file contains settings that are specific to the \object{GreensFns} problem type: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step21.cfg}] [greensfns]

      fault_id

      = 10 @@ -76,7 +76,7 @@ \subsubsection{Step21 - Green's Function Generation} PyLith provides the ability to interpolate displacements to a specified set of points, which would generally be necessary when generating Green's functions: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step21.cfg}] [pylithapp.problem.formulation] output = [domain, points] output.points = pylith.meshio.OutputSolnPoints diff --git a/doc/userguide/examples/3dhex8_quasistatic.tex b/doc/userguide/examples/3dhex8_quasistatic.tex index 0c69d490df..10ce6b1442 100644 --- a/doc/userguide/examples/3dhex8_quasistatic.tex +++ b/doc/userguide/examples/3dhex8_quasistatic.tex @@ -34,9 +34,25 @@ \subsubsection{Overview} directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step04.cfg}, \filename{step05.cfg}, \filename{step06.cfg}, \filename{step07.cfg}, \filename{step08.cfg}, and \filename{step09.cfg}. -Each example may be run as follows: +Run the examples as follows: \begin{shell} -$ pylith stepXX.cfg +# Step04 +$ pylith step04.cfg + +# Step05 +$ pylith step05.cfg + +# Step06 +$ pylith step06.cfg + +# Step07 +$ pylith step07.cfg + +# Step08 +$ pylith step08.cfg + +# Step09 +$ pylith step09.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in @@ -56,7 +72,7 @@ \subsubsection{Step04 - Pure Dirichlet Velocity Boundary Conditions} behavior is \object{TimeStepUniform}. We retain that behavior for this problem and provide the total simulation time and the time-step size: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] # Change the total simulation time to 200 years, and use a constant time # step size of 20 years. [pylithapp.timedependent.implicit.time_step]<.h> @@ -67,7 +83,7 @@ \subsubsection{Step04 - Pure Dirichlet Velocity Boundary Conditions} database from which to obtain the material properties (using the default \object{SimpleDB}), and request additional output information for the material: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] # Change material type of lower crust to Maxwell viscoelastic. [pylithapp.timedependent] materials.lower_crust = pylith.materials.MaxwellIsotropic3D @@ -94,7 +110,7 @@ \subsubsection{Step04 - Pure Dirichlet Velocity Boundary Conditions} \facility{db\_initial}. To apply the velocity boundary conditions, we must specify \facility{db\_rate}, which is zero by default. We use a \object{UniformDB} to assign the velocities: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos]

      bc_dof

      = [0, 1] @@ -125,7 +141,7 @@ \subsubsection{Step04 - Pure Dirichlet Velocity Boundary Conditions} assign a more user-friendly format to the output file time stamp, and we request that the time stamp is in units of 1 year (rather than the default value of seconds): -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] # Give basename for VTK domain output of solution over domain. [pylithapp.problem.formulation.output.domain] # We specify that output occurs in terms of a given time frequency, and @@ -185,7 +201,7 @@ \subsubsection{Step05 - Time-Varying Dirichlet and Neumann Boundary Conditions} For the boundary conditions, we must first change the boundary condition type for the positive x-face from the default Dirichlet to Neumann: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] # +x face -- first change bc type to Neumann [pylithapp.timedependent.bc] x_pos = pylith.bc.Neumann @@ -196,7 +212,7 @@ \subsubsection{Step05 - Time-Varying Dirichlet and Neumann Boundary Conditions} for the traction rates, and use a rate of 0.01 MPa/year, so that by the end of 200 years we have completely cancelled the initial traction of -1 MPa: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.timedependent.bc.x_pos] # First specify a UniformDB for the initial tractions, along with the values. db_initial = spatialdata.spatialdb.UniformDB @@ -213,7 +229,7 @@ \subsubsection{Step05 - Time-Varying Dirichlet and Neumann Boundary Conditions} The boundary conditions on the negative x-face are analogous, but we are instead using Dirichlet boundary conditions, and the initial displacement is in the same direction as the applied velocities: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] # -x face [pylithapp.timedependent.bc.x_neg]

      bc_dof

      = [0, 1] @@ -272,7 +288,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema less than 1.0 allows time-step sizes greater than the stable time-step size, which may provide inaccurate results. The adaptive time stepping information is provided as: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] # Change time stepping algorithm from uniform time step, to adaptive # time stepping. time_step = pylith.problems.TimeStepAdapt @@ -293,7 +309,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema the files to be read easily by applications such as ParaView. Since VTK output is still the default, we must change the value from the default. Also note that the filename suffix is \filename{h5}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] # Give basename for output of solution over domain. [pylithapp.problem.formulation.output.domain] # We specify that output occurs in terms of a given time frequency, and @@ -312,7 +328,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema We also set the writer for other output as well, since it is not the default. For subdomain output we use: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] # Give basename for output of solution over ground surface. [pylithapp.problem.formulation.output.subdomain] # Name of nodeset for ground surface. @@ -340,7 +356,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema fault interface, we identify the nodeset corresponding to the fault, and we provide quadrature information for the fault. We then define an array of earthquake sources and provide an origin time for each: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.timedependent.interfaces.fault] # Set earthquake sources to an array consisting of creep and 3 ruptures. eq_srcs = [creep, one, two, three] @@ -355,7 +371,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema the ruptures has the same amount of slip, and slip occurs simultaneously for the entire rupture region, so we can use the same \object{SimpleDB} files providing slip and slip time for each rupture: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] # Define slip and origin time for first rupture. [pylithapp.timedependent.interfaces.fault.eq_srcs.one.slip_function]

      slip.iohandler.filename

      = spatialdb/finalslip_rupture.spatialdb @@ -374,7 +390,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema For the creep source, we change the slip function to \object{ConstRateSlipFn}, and we use a \object{SimpleDB} for both the slip time and the slip rate: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] # Define slip rate and origin time for fault creep. [pylithapp.timedependent.interfaces.fault.eq_srcs.creep] slip_function = pylith.faults.ConstRateSlipFn @@ -389,7 +405,7 @@ \subsubsection{Step06 - Dirichlet Boundary Conditions with Time-Dependent Kinema types, there are a number of additional fault information fields available for output. We add these additional fields' output to the fault information file: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.timedependent.interfaces.fault]

      output.vertex_info_fields

      = [normal_dir, strike_dir, dip_dir, final_slip_creep, \ final_slip_one, final_slip_two, final_slip_three, slip_time_creep, slip_time_one, \ @@ -426,7 +442,7 @@ \subsubsection{Step07 - Dirichlet Velocity Boundary Conditions with Time-Depende on the positive and negative x-faces, as well as the negative z-face. For the velocities on the positive and negative x-faces, we use a \object{UniformDB}: -\begin{cfg} +\begin{cfg}`w # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos]

      bc_dof

      = [0, 1] @@ -457,7 +473,7 @@ \subsubsection{Step07 - Dirichlet Velocity Boundary Conditions with Time-Depende size. This is more accurate than computing the velocities from the displacement field output that has been decimated in time. We can obtain this information by explicitly requesting it in \property{vertex\_data\_fields}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step07.cfg}] # Give basename for output of solution over domain. [pylithapp.problem.formulation.output.domain] # We specify that output occurs in terms of a given time frequency, and @@ -509,7 +525,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende example step07, except the the lower crust is composed of a power-law viscoelastic material. Since the material behavior is now nonlinear, we must use the nonlinear solver: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] [pylithapp.timedependent] # For this problem we must switch to a nonlinear solver. implicit.solver = pylith.problems.SolverNonlinear @@ -518,7 +534,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende note that the use of the nonlinear solver may require additional options if we wish to override the defaults. These settings are contained in \filename{pylithapp.cfg}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] [pylithapp.petsc] # Nonlinear solver monitoring options.

      snes_rtol

      = 1.0e-8 @@ -564,7 +580,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende in creating the file \filename{examples/3d/hex8/spatialdb/mat\_powerlaw.spatialdb}. We first change the material type of the lower crust to \object{PowerLaw3D}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] # Change material type of lower crust to power-law viscoelastic. [pylithapp.timedependent] materials.lower_crust = pylith.materials.PowerLaw3D @@ -575,7 +591,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende from a thermal model. In such a case we can use a \object{CompositeDB}, which allows a different spatial database to be used for a subset of the properties. We do this as follows: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] # Provide a spatial database from which to obtain property values. # In this case, we prefer to obtain the power-law properties from one # database and the elastic properties from another database, so we use @@ -587,7 +603,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende \end{cfg} We must define the properties that come from each spatial database and then provide the database parameters: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] # Provide the values to be obtained from each database and the database # name. [pylithapp.timedependent.materials.lower_crust.db_properties] @@ -602,7 +618,7 @@ \subsubsection{Step08 - Dirichlet Velocity Boundary Conditions with Time-Depende variables with respect to the default \object{ElasticIsotropic3D} material, so we request that these properties be written to the \facility{lower\_crust} material files: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08.cfg}] # Since there are additional properties and state variables for the # power-law model, we explicitly request that they be output. Properties are # named in cell_info_fields and state variables are named in @@ -637,7 +653,7 @@ \subsubsection{Step09 - Dirichlet Velocity Boundary Conditions with Time-Depende size for the material depends on the loading conditions. To avoid this, we set the maximum time-step size to 5 years rather than the value of 10 years used in example \filename{step08}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step09.cfg}] # Change the total simulation time to 700 years, and set the maximum time # step size to 5 years. [pylithapp.timedependent.implicit.time_step] @@ -664,7 +680,7 @@ \subsubsection{Step09 - Dirichlet Velocity Boundary Conditions with Time-Depende \end{cfg} As for the step08 example, we first define the properties that come from each spatial database and then provide the database filename: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step09.cfg}] # Provide the values to be obtained from each database and the database # name. [pylithapp.timedependent.materials.lower_crust.db_properties] @@ -678,7 +694,7 @@ \subsubsection{Step09 - Dirichlet Velocity Boundary Conditions with Time-Depende \end{cfg} We also request output of the properties and state variables that are unique to the \object{DruckerPrager3D} material: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step09.cfg}] # Since there are additional properties and state variables for the # Drucker-Prager model, we explicitly request that they be output. # Properties are named in cell\_info\_fields and state variables are named in diff --git a/doc/userguide/examples/3dhex8_static.tex b/doc/userguide/examples/3dhex8_static.tex index f9ec0492a7..cc04574596 100644 --- a/doc/userguide/examples/3dhex8_static.tex +++ b/doc/userguide/examples/3dhex8_static.tex @@ -24,9 +24,17 @@ \subsubsection{Overview} the use of a kinematic fault for a static problem. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step01.cfg}, \filename{step02.cfg}, -and \filename{step03.cfg}. Each example may be run as follows: +and \filename{step03.cfg}. Run the examples as follows: \begin{shell} -$ pylith stepXX.cfg +# Step01 +$ pylith step01.cfg + +# Step02 +$ pylith step02.cfg + +# Step03 +$ pylith step03.cfg + \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in @@ -46,7 +54,7 @@ \subsubsection{Step01 - Pure Dirichlet Boundary Conditions} subsequent examples we would like to output the displacement solution over a subset of the domain corresponding to the ground surface. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step01.cfg}] [pylithapp.timedependent.implicit] # Set the output to an array of 2 output managers. # We will output the solution over the domain and the ground surface. @@ -67,7 +75,7 @@ \subsubsection{Step01 - Pure Dirichlet Boundary Conditions} specify the type of spatial database is being used to describe the boundary conditions. For the x-faces, we use a \object{SimpleDB} to provide the displacements on the x-faces: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step01.cfg}] # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos]

      bc_dof

      = [0, 1] @@ -88,7 +96,7 @@ \subsubsection{Step01 - Pure Dirichlet Boundary Conditions} database for \facility{db\_initial} is \object{ZeroDispBC}, which automatically applies zero displacements to all vertices in the nodeset, and no filename is required (or needed). -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step01.cfg}] # Boundary condition on -z face [pylithapp.timedependent.bc.z_neg]

      bc_dof

      = [2] @@ -122,7 +130,7 @@ \subsubsection{Step02 - Dirichlet and Neumann Boundary Conditions} For the boundary conditions, we must first change the boundary condition type for the positive x-face from the default Dirichlet to Neumann: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] # +x face -- first change bc type to Neumann [pylithapp.timedependent.bc] x_pos = pylith.bc.Neumann @@ -136,7 +144,7 @@ \subsubsection{Step02 - Dirichlet and Neumann Boundary Conditions} integration order of 2. A lower integration order would not provide sufficient accuracy while a higher integration order would offer no benefit (while requiring more computation time and storage): -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] # Boundary condition on +x face [pylithapp.timedependent.bc.x_pos]

      label

      = face_xpos @@ -152,7 +160,7 @@ \subsubsection{Step02 - Dirichlet and Neumann Boundary Conditions} The boundary conditions on the negative x-face are simpler than they were in example step01 (zero displacements in the x and y-directions), so we can use the default \object{ZeroDispBC}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] # Boundary condition on -x face [pylithapp.timedependent.bc.x_neg]

      bc_dof

      = [0, 1] @@ -191,7 +199,7 @@ \subsubsection{Step03 - Dirichlet Boundary Conditions with Kinematic Fault Slip} a fault interface. We do this by providing an array containing a single interface. For this example we specify the fault slip, so we set the interface type to \object{FaultCohesiveKin}. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] [pylithapp.timedependent] # Set interfaces to an array of 1 fault: 'fault'. interfaces = [fault] @@ -214,7 +222,7 @@ \subsubsection{Step03 - Dirichlet Boundary Conditions with Kinematic Fault Slip} variation of fault slip, and another \object{SimpleDB} to define the spatial variation in slip initiation times (the start time is 0.0 everywhere since this is a static problem): -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] # The slip time and final slip are defined in spatial databases. [pylithapp.timedependent.interfaces.fault.eq\_srcs.rupture.slip\_function]

      slip.iohandler.filename

      = spatialdb/finalslip.spatialdb diff --git a/doc/userguide/examples/3dhex8_surfload.tex b/doc/userguide/examples/3dhex8_surfload.tex index 8c150a4b0b..dd97f5c9ee 100644 --- a/doc/userguide/examples/3dhex8_surfload.tex +++ b/doc/userguide/examples/3dhex8_surfload.tex @@ -19,9 +19,13 @@ \subsubsection{Overview} of the solution at user-defined locations. All of the examples are contained in the directory \filename{examples/3d/hex8}, and the corresponding \filename{cfg} files are \filename{step18.cfg} and \filename{step19.cfg}. -Each example may be run as follows: +Run the examples as follows: \begin{shell} -$ pylith stepXX.cfg +# Step18 +$ pylith step18.cfg + +# Step19 +$ pylith step19.cfg \end{shell} This will cause PyLith to read the default parameters in \filename{pylithapp.cfg}, and then override or augment them with the additional parameters in @@ -47,7 +51,7 @@ \subsubsection{Step18 - Static Surface Load} degree of freedom that is constrained, the name of the nodeset from CUBIT, and a label used in diagnostic output. For the Dirichlet boundary condition on the +x surface we have: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step18.cfg}] [pylithapp.timedependent.bc.x_pos]

      label

      = face_xpos

      bc_dof

      = [0] @@ -63,7 +67,7 @@ \subsubsection{Step18 - Static Surface Load} Finally, we specify a vector for the up direction because the tractions are applied to a horizontal surface, resulting in ambiguous shear directions for our default orientation convention. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step18.cfg}] [pylithapp.timedependent.bc] z_pos = pylith.bc.Neumann @@ -120,7 +124,7 @@ \subsubsection{Step19 - Time-Dependent Surface Load} Rather than specify a spatial database for the initial value of the Neumann boundary condition corresponding to the surface load, we specify a spatial database for the change in value and the temporal database: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{Step19.cfg}] [pylithapp.timedependent.bc.z_pos]

      label

      = face_zpos diff --git a/doc/userguide/examples/examples.tex b/doc/userguide/examples/examples.tex index 0f924f3cb4..1df26cbca5 100644 --- a/doc/userguide/examples/examples.tex +++ b/doc/userguide/examples/examples.tex @@ -134,7 +134,7 @@ \subsection{Overriding Default Parameters} simply set the values within the Python shell. For example, to set the value of the variable \object{EXODUS\_FILE} to the absolute path of the input file, -\begin{python} +\begin{python}[ParaView Python shell] >>> EXODUS_FILE = "/home/johndoe/pylith/examples/3d/subduction/mesh/mesh_tet.exo" \end{python} In this case, we use the Python os module to get the absolute path of diff --git a/doc/userguide/examples/grav2d.tex b/doc/userguide/examples/grav2d.tex index 45adf1bddd..f1693f71cf 100644 --- a/doc/userguide/examples/grav2d.tex +++ b/doc/userguide/examples/grav2d.tex @@ -109,13 +109,13 @@ \subsection{Additional Common Information} \end{inventory} Since we do not desire an initial elastic solution prior to beginning our time stepping for the simulations, we turn off the elastic prestep: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.timedependent]

      elastic_prestep

      = False \end{cfg} For two-dimensional problems involving gravity, we also need to change the default \property{gravity\_dir}: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.timedependent] gravity_field = spatialdata.spatialdb.GravityField

      gravity_field.gravity_dir

      = [0.0, -1.0, 0.0] @@ -138,8 +138,7 @@ \subsection{Step 1: Gravitational Body Forces and Infinitesimal Strain} look at this file during the simulation to monitor the progress and get an estimate of when the simulation will finish. -We run the simulation using: -\begin{shell} +\begin{shell}[Run Step 1 simulation] $ pylith gravity_infstrain.cfg \end{shell} The simulation produces HDF5 (and corresponding XDMF) files with the @@ -171,8 +170,7 @@ \subsection{Step 2: Gravitational Body Forces, Infinitesimal Strain, and Initial Step 1, the simulation specific parameter file contains the filenames for the output. -We run the simulation using: -\begin{shell} +\begin{shell}[Run Step 2 simulation] $ pylith gravity_initstress.cfg gravity_isostatic.cfg \end{shell} @@ -216,8 +214,7 @@ \subsection{Step 3: Infinitesimal Strain Simulation with Initial Stresses and equilibrium or steady state stress state associated with gravitational body forces and lateral density variations or topography. -We run the simulation using: -\begin{shell} +\begin{shell}[Run Step 3 simulation] $ pylith gravity_initstress.cfg gravity_vardensity.cfg \end{shell} Figure \vref{fig:examples:gravity:2d:vardensity:stress} shows the @@ -247,8 +244,7 @@ \subsection{Step 4: Postseismic Relaxation with Infinitesimal Strain} algebraic multigrid preconditioner for the elastic block and the custom fault preconditioner for the Lagrange multipliers. -We run the simulation using: -\begin{shell} +\begin{shell}[Run Step 4 simulation] $ pylith postseismic.cfg nogravity.cfg postseismic_infstrain_nograv.cfg \end{shell} Figure \vref{fig:examples:gravity:2d:postseismc:infstrain:disp} shows @@ -266,13 +262,13 @@ \subsection{Step 5: Postseismic Relaxation with Finite Strain} This simulation is the same as Step 4, but we use the finite strain formulation.: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{postseismic\_finstrain.cfg}] [pylithapp.timedependent] formulation = pylith.problems.ImplicitLgDeform \end{cfg} When we use the finite strain formulation, the solver is automatically -switched to the nonlinear solver. We run the simulation using: -\begin{shell} +switched to the nonlinear solver. +\begin{shell}[Run Step 5 simulation] $ pylith postseismic.cfg nogravity.cfg postseismic_finstrain_nograv.cfg \end{shell} The results are nearly identical to those with infinitesimal strain. @@ -285,8 +281,7 @@ \subsection{Step 6: Postseismic Relaxation with Infinitesimal Strain and Gravita equations, so our initial conditions are axial stresses equal to the overburden pressure. -We run the simulation using: -\begin{shell} +\begin{shell}[Run Step 6 simulation] $ pylith postseismic.cfg postseismic_infstrain.cfg \end{shell} With the infinitesimal strain formulation and linearly material behavior, @@ -301,9 +296,8 @@ \subsection{Step 7: Postseismic Relaxation with Finite Strain and Gravitational This simulation is the same as Step 5, but we include gravitational body forces; this is also the same as Step 6, but with finite strain. -We run the simulation using: -\begin{shell} -$ pylith postseismic.cfg postseismic\_finstrain.cfg +\begin{shell}[Run Step 7 simulation] +$ pylith postseismic.cfg postseismic_finstrain.cfg \end{shell} The finite strain formulation accounts for the redistribution of gravitational body forces as the domain deforms during the postseismic @@ -349,12 +343,11 @@ \subsection{Step 8: Postseismic Relaxation with Finite Strain, Gravitational state so that the Cauchy stresses are very close to the second Pioloa-Kirchoff stresses. Our first step is to modify the \filename{pylithapp.cfg} file by commenting out the lines with the CellFilterAvg settings: -\begin{cfg} -# If rerunning Step 3 to get initial conditions for Step 8, comment out the next line as shown. +\begin{cfg}[Modify \filename{pylithapp.cfg} when rerunning Step 3] #cell_filter = pylith.meshio.CellFilterAvg \end{cfg} -for both the crust and mantle. Next we rerun Step 3 using -\begin{shell} +for both the crust and mantle. +\begin{shell}[Rerun Step 3 after modifying \filename{pylithapp.cfg}] $ pylith gravity_initstress.cfg gravity_vardensity.cfg \end{shell} This will change how the values appear in ParaView output. Because @@ -366,15 +359,14 @@ \subsection{Step 8: Postseismic Relaxation with Finite Strain, Gravitational values 3, 4, and 5 correspond to the values at the second quadrature point, etc. We use the Python script \filename{generate\_statedb.py} to generate the spatial databases with the initial stresses from the -output of Step 3: -\begin{shell} +output of Step 3. +\begin{shell}[Generate intial stresses using output from Step 3] $ ./generate_statedb.py \end{shell} After generating the initial state variables, we uncomment the \texttt{cell\_filter} lines in \filename{pylithapp.cfg} to allow easier visualization of Step -8 results. Finally, we run the simulation of the postseismic deformation -using -\begin{shell} +8 results. +\begin{shell}[Run Step 8 simulation] $ pylith postseismic.cfg gravity_initstress.cfg postseismic_vardensity.cfg \end{shell} In the 100 years before the earthquake, it is clear that there is diff --git a/doc/userguide/examples/greensfns2d.tex b/doc/userguide/examples/greensfns2d.tex index c03508a81a..1696f729f5 100644 --- a/doc/userguide/examples/greensfns2d.tex +++ b/doc/userguide/examples/greensfns2d.tex @@ -110,7 +110,7 @@ \subsection{Additional Common Information} One aspect that has not been covered previously is the specification of output at discrete points, rather than over a mesh or sub-mesh. We do this using the \object{OutputSolnPoints} output type: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.problem.formulation] output = [domain, points] output.points = pylith.meshio.OutputSolnPoints @@ -190,7 +190,7 @@ \subsection{Step 2: Generation of Green's Functions} file \filename{greensfns.cfg} by default, in addition to \filename{pylithapp.cfg}. These additional parameter settings provide the information necessary to generate the Green's functions: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{greensfns.cfg}] [greensfns]

      fault_id

      = 100 @@ -292,9 +292,9 @@ \subsection{Step 3: Simple Inversion Using PyLith-generated Green's Functions} solution is performed for a range of values of the penalty parameter, which are contained in the file \filename{penalty\_params.txt} within each subdirectory. The inversion is performed by running the script -in the top-level directory from each subdirectory. To run an inversion, -type: -\begin{shell} +in the top-level directory from each subdirectory. + +\begin{shell}[Run the inversion] $ ../invert_slip.py --impulses=output/greensfns-fault.h5 \ --responses=output/greensfns-points.h5 --data=output/eqsim-points.h5 \ --penalty=penalty_params.txt --output=output/slip_inverted.txt \ @@ -311,8 +311,8 @@ \subsection{Step 4: Visualization of Estimated and True Solutions} PyLith binary). We also use the h5py package again to read the applied slip for the forward problem. The Python code to plot the results is contained in the \filename{plot\_invresults.py} file contained within -each subdirectory. To plot the results, type: -\begin{shell} +each subdirectory. +\begin{shell}[Plot the results (requires Matplotlib)] $ plot_invresults.py --solution=output/eqsim-fault.h5 --predicted=output/slip_inverted.txt \end{shell} The script will produce an interactive matplotlib window that shows diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index 4f4ab7d21d..ca0eb98db0 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -368,7 +368,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} requires the nonlinear solver. Through trial and error we choose a time step of 2.5 years that permits reasonable convergence of the nonlinear solver and runtime. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.problem.formulation] # Fault friction is a nonlinear problem so we need to use the # nonlinear solver. @@ -387,7 +387,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} boundaries without restraining the subducting slab. We also constrain the vertical deformation of the west boundary to facilitate the downward motion of the subducting slab. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.timedependent.bc.boundary_west]

      bc_dof

      = [0, 1]

      label

      = bndry_west @@ -398,7 +398,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} We replace the prescribed aseismic slip on the subduction interface that we used in Step 2 with a friction interface with the slip-weakening fault constitutive model. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.timedependent] interfaces = [fault_slabtop, fault_slabbot] @@ -435,7 +435,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} did in Step 4. We reduce the initial shear tractions slightly in the seismogenic zone, consistent with a stress drop in the penultimate earthquake followed by loading during the interseismic period. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.timedependent.interfaces.fault_slabtop] # --- Skipping general information discussed previously --- # Friction @@ -471,7 +471,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction} calculate consistent values for the change in slip for a given change in the Lagrange multipliers (which we sometimes call the friction sensitivity solve). -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step05.cfg}] [pylithapp.timedependent.interfaces.fault_slabtop]

      zero_tolerance

      = 1.0e-8

      zero_tolerance_normal

      = 1.0e-8 @@ -536,7 +536,7 @@ \subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction} which were determined through trial and error to get a couple earthquake cycles with reasonable convergence for this relatively coarse resolution mesh. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.timedependent.formulation.time_step]

      total_time

      = 200.0*year dt = 1.0*year @@ -557,7 +557,7 @@ \subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction} state sliding at the reference coefficient of friction at the reference slip rate, and include it in the state variable in the output as a check. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.timedependent.interfaces.fault_slabtop] # --- Skipping parameters discussed in previous examples. --- # Friction diff --git a/doc/userguide/examples/subduction3d.tex b/doc/userguide/examples/subduction3d.tex index 8582587674..0ba062c573 100644 --- a/doc/userguide/examples/subduction3d.tex +++ b/doc/userguide/examples/subduction3d.tex @@ -110,7 +110,7 @@ \subsection{Generating the Finite-Element Mesh} and post-processing. PyLith will automatically convert among compatible coordinate systems during the simulation.} -\begin{shell} +\begin{shell}[Generate \filename{generate\_surfs.jou}] # Make sure you are in the 'mesh' directory and then run the Python # script to generate the journal file 'generate_surfs.jou'. $ ./generate_surfjou.py @@ -176,7 +176,7 @@ \subsubsection{Visualizing the Mesh} To visualize the mesh, start ParaView. Within the ParaView GUI Python shell (\menu{Tools}$\rightarrow$\menu{Python Shell}), we override the \filename{EXODUS\_FILE} and \filename{SHOW\_QUALITY} parameters. -\begin{python} +\begin{python}[ParaView Python shell] # Import the os module so we can get access to the HOME environment variable. >>> import os >>> HOME = os.environ["HOME"] @@ -250,7 +250,7 @@ \subsubsection{Coordinate system} between compatible coordinate systems. Our spatialdata library uses Proj4 for geographic projections, so we specify the projection using Proj4 syntax in the \property{proj\_options} property: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.mesh_generator.reader] coordsys = spatialdata.geocoords.CSGeoProj

      coordsys

      .space_dim = 3 @@ -270,7 +270,7 @@ \subsubsection{Materials} array of materials that defines the name for each material component. For example, we create the array of four materials and then set the parameters for the slab: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.problem] materials = [slab, wedge, crust, mantle] @@ -305,7 +305,7 @@ \subsubsection{Boundary Conditions} CUBIT/Trelis that defines the boundary, and a label for the spatial database (required for informative error messages). These settings constrain the y-displacement on the north (+y) boundary: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.problem.bc.y_pos]

      bc_dof

      = [1] ; Degree of freedoms are: x=0, y=1, and z=2

      label

      = boundary_ypos ; nodeset in ExodusII file form CUBIT/Trelis @@ -321,7 +321,7 @@ \subsubsection{Solver Parameters} solver, which is suitable for debugging and test problems that do not include a fault; a direct solver is not well-suited for production runs because it does not scale well and uses a lot of memory. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{pylithapp.cfg}] [pylithapp.petsc]

      malloc_dump

      = ; Dump information about PETSc memory not deallocated. @@ -392,7 +392,7 @@ \subsection{Step 1: Axial Compression} this behavior in the \filename{step01.cfg} file for the -x and +x boundaries using spatial databases with a single uniform displacement value to create the axial compression: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step01.cfg}] # -x face [pylithapp.problem.bc.x_neg] db_initial = spatialdata.spatialdb.UniformDB @@ -413,7 +413,7 @@ \subsection{Step 1: Axial Compression} associated with linear, isotropic elastic bulk constitutive models for all of the materials for convenient reuse across several different simulations. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{mat\_elastic.cfg}] [pylithapp.problem.materials] slab = pylith.materials.ElasticIsotropic3D wedge = pylith.materials.ElasticIsotropic3D @@ -460,8 +460,7 @@ \subsection{Step 1: Axial Compression} HDF5 files (the corresponding Xdmf files will use the same filename with the \filename{xmf} suffix). -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 1 simulation] $ pylith step01.cfg mat_elastic.cfg \end{shell} The simulation will produce ten pairs of HDF5/Xdmf files in the @@ -606,7 +605,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} contained in each of the two spatial databases in the composite database and the type and parameters for each of those spatial databases. For the slab we have: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{mat\_viscoelastic.cfg}] [pylithapp.problem.materials.slab] db_properties = spatialdata.spatialdb.CompositeDB

      db_properties.label

      = Composite spatial database for slab material properties @@ -631,7 +630,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} coseismic rupture, and the filenames for output. By default, PyLith will use implicit time stepping with uniform time steps, so we need only specify the duration and time step size. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] [pylithapp.problem.formulation.time_step] # Define the total time for the simulation and the time step size.

      total_time

      = 200.0*year @@ -649,7 +648,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} with one fault interface, \facility{slab}, and then refer to those components by name, \facility{pylithapp.problem.interfaces.slab}. We must also set the discretization information for the fault. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] [pylithapp.problem] # We prescribe slip on the slab fault patch. interfaces = [slab] @@ -681,7 +680,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation} want uniform slip and a uniform rise time, we use \object{UniformDB} spatial databases for both of these. Note that we specify oblique slip with 1.0 m of right-lateral motion and 4.0 m of reverse motion. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step02.cfg}] [pylithapp.problem.interfaces.slab.eq_srcs.rupture.slip_function] slip = spatialdata.spatialdb.UniformDB

      slip.label

      = Final slip @@ -699,8 +698,7 @@ \subsection{Step 2: Prescribed Coseismic Slip and Postseismic Relaxation}

      vertex_info_fields

      = [normal_dir, strike_dir, dip_dir, final_slip_rupture, slip_time_rupture] \end{cfg} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 2 simulation] $ pylith step02.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} In addition to the ten pairs of HDF5/Xdmf files analogous to those @@ -801,13 +799,13 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} interface), \facility{slab\_top}, and one for the bottom of the slab, \facility{slab\_bottom}. We use the \object{FaultCohesiveKin} object for each of these interfaces since we want to prescribe the slip. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] [pylithapp.problem] -interfaces = [slab_top, slab_bottom] +interfaces = [slab_bottom, slab_top] [pylithapp.problem.interfaces] -slab_top = pylith.faults.FaultCohesiveKin slab_bottom = pylith.faults.FaultCohesiveKin +slab_top = pylith.faults.FaultCohesiveKin \end{cfg} % Bottom of slab @@ -826,7 +824,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} uniform oblique slip rate of 2.0 cm/yr of left-lateral motion and 4.0 cm/yr of normal motion. Note that slip on the bottom of the subducting slab has the opposite sense of motion as that on the top of the slab. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] [pylithapp.problem.interfaces.slab_bottom]

      id

      = 100 ; Must be different from ids used for materials

      label

      = fault_slabbot ; Nodeset for the entire fault surface @@ -868,7 +866,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} we use a \object{SimpleGridDB} to define a depth variation in the slip rate. The fault is locked at depths above 45 km and increases linearly to the same slip rate as the bottom of the slab at a depth of 60 km. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] [pylithapp.problem.interfaces.slab_top]

      id

      = 101 ; Must be different from ids used for materials

      label

      = fault_slabtop ; Nodeset for the entire fault surface @@ -908,7 +906,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation} we exclude vertices on the splay fault in these nodesets as well. We only update the name of the nodeset for the -x, -y, and +y boundaries. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step03.cfg}] # -x face [pylithapp.problem.bc.x_neg]

      label

      = boundary_xneg_noslab @@ -922,8 +920,7 @@ \subsection{Step 3: Prescribed Aseismic Creep and Interseismic Deformation}

      label

      = boundary_ypos_noslab \end{cfg} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 3 simulation] $ pylith step03.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} The simulation will produce fourteen pairs of HDF5/Xdmf files, @@ -1018,7 +1015,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} for the splay fault. The splay fault terminates into the fault on the top of the slab, so we must list the through-going fault on the top of the slab first. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] # We prescribe slip on the top and bottom of the slab and on the splay fault. [pylithapp.problem] interfaces = [slab_top, slab_bottom, splay] @@ -1052,7 +1049,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} creep. Note that the slip time within an earthquake rupture is relative to the origin time, so we set the slip time to zero to coincide with the specified origin time. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] [pylithapp.problem.interfaces.slab_top] # --- Skipping lines already discussed in Step 3 --- eq_srcs = [creep, eq1, eq2] @@ -1106,7 +1103,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} difference is that we specify an origin time of 250 years. % Fault: splay -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step04.cfg}] [pylithapp.problem.interfaces.splay]

      id

      = 102 ; id must be unique across all materials and faults

      label

      = fault_splay ; Nodeset for the entire fault surface @@ -1134,8 +1131,7 @@ \subsection{Step 4: Prescribed Earthquake Cycle} # --- Omitting output settings already discussed --- \end{cfg} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 4 simulation] $ pylith step04.cfg mat_viscoelastic.cfg solver_fieldsplit.cfg \end{shell} The simulation will produce sixteen pairs of HDF5/Xdmf files, @@ -1239,7 +1235,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} slip, so we set the duration of the simulation to match the duration of the slow slip event. We use a time step of 2.0 days to insure that we resolve the temporal evolution of the slip. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.problem.formulation.time_step]

      total_time

      = 30.0*day

      dt

      = 2.0*day @@ -1250,7 +1246,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} continuous GPS (cGPS) stations in Step 7, so we add an output manager for saving the solution at specific points (\object{OutputSolnPoints}) in addition to our output managers over the domain and top surface: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.problem.implicit] output = [domain, subdomain, cgps_sites] @@ -1266,7 +1262,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} is whitespace separated columns of station name and then the coordinates of the station. See Section~\vref{sec:format:PointsList} for more information. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.problem.formulation.output.cgps_sites] writer = pylith.meshio.DataWriterHDF5

      writer.filename

      = output/step06-cgps_sites.h5 @@ -1292,7 +1288,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} spatial databases with points in other, but compatible, georeferenced coordinate systems, we specify the slip distribution using geographic (longitude and latitude) coordinates. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step06.cfg}] [pylithapp.problem] # We prescribe slip on the slab fault patch. interfaces = [slab] @@ -1350,7 +1346,7 @@ \subsection{Step 6: Prescribed Slow-Slip Event} To run the simulation, first run the Python script to generate the spatial database files, and then run PyLith. -\begin{shell} +\begin{shell}[Run Step 4 simulation] # Generate the spatial database files $ cd spatialdb && ./generate_slowslip.py $ ls fault_slabtop_slowslip.* @@ -1452,7 +1448,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} \object{UniformDB} spatial database, because we want impulses over the entire fault patch. We also request the amplitude of the impulses to be included in the fault info file. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{greensfns.cfg}] # Define the interfaces (slab) and provide a fault_id. [greensfns] interfaces = [slab] @@ -1486,7 +1482,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} We do not make use of the state variable output for the impulse responses, so we turn off the data fields for all of the materials to eliminate these large data files. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{greensfns.cfg}] # Turn off output of state variables for materials. [greensfns.materials.slab.output]

      cell_data_fields

      = [] @@ -1504,7 +1500,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} The \filename{step07a.cfg} and \filename{step07b.cfg} files are identical, except for the impulse type specification and file names. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step07a.cfg}] [pylithapp.problem.interfaces.slab] # If we wanted to generate impulses for both the left-lateral and # reverse components in the same simulation, we would use: @@ -1516,15 +1512,14 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} In the output settings, we turn off writing the solution field for the domain: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step07a.cfg}] [pylithapp.problem.formulation.output.domain]

      writer.filename

      = output/step07a-domain.h5 # Turn off data fields.

      vertex_data_fields

      = [] \end{cfg} -You can run the two sub-problems as follows: -\begin{shell} +\begin{shell}[Run Step 7 simulations] $ pylith --problem=pylith.problems.GreensFns step07a.cfg mat_elastic.cfg solver_fieldsplit.cfg $ pylith --problem=pylith.problems.GreensFns step07b.cfg mat_elastic.cfg solver_fieldsplit.cfg \end{shell} @@ -1554,8 +1549,8 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} Python script \filename{make\_synthetic\_gpsdisp.py} reads the parameters in \filename{make\_synthetic\_gpsdisp.cfg} and generates synthetic data from the selected time step with a specified amount of -noise. Run this script by typing: -\begin{shell} +noise. +\begin{shell}[Generate synthetic GPS data] $ ./make_synthetic_gpsdisp.py \end{shell} This will create the following files: @@ -1570,7 +1565,7 @@ \subsection{Step 7: Inversion of Slow-Slip Event using 3-D Green's Functions} with parameters defined in \filename{slip\_invert.cfg}. This script performs a set of linear inversions, in a manner similar to the inversion in \vref{sec:example:greensfns2d:inversion}. -\begin{shell} +\begin{shell}[Run the inversion] $ ./slip_invert.py \end{shell} This will create a number of files in the output directory. @@ -1689,7 +1684,7 @@ \subsubsection{Step 08a} are out of balance and we end up with some deformation. In \filename{step08a.cfg} we turn on gravity and set the total time to zero (there is no time dependence in this model). -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08a.cfg}] [pylithapp.problem] # Set gravity field (default is None). gravity_field = spatialdata.spatialdb.GravityField @@ -1706,7 +1701,7 @@ \subsubsection{Step 08a} elevation. With only two control points necessary to describe this linear variation, we use the same \object{SimpleDB} spatial database for all four materials. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08a.cfg}] # We specify initial stresses for each material via a SimpleDB and linear interpolation. [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB @@ -1733,8 +1728,7 @@ \subsubsection{Step 08a}

      db_initial_stress.query_type

      = linear \end{cfg} -We run the sub-problem by typing: -\begin{shell} +\begin{shell}[Run Step 8a simulation] $ pylith step08a.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} The simulation will generate ten pairs of HDF5/Xdmf files beginning @@ -1796,7 +1790,7 @@ \subsubsection{Step 8b} database. The spatial database will contain the stresses at each cell of our unstructured mesh, so the points are not on a logical grid, and we must use a \object{SimpleDB}. -\begin{shell} +\begin{shell}[Generate the initial stresses for Step 8b] # From the examples/3d/subduction directory, change to the spatialdb subdirectory. $ cd spatialdb $ ./generate_initial_stress.py @@ -1810,7 +1804,7 @@ \subsubsection{Step 8b} interpolation (default) rather than linear interpolation; this is a small approximation but it is much faster than using linear interpolation in this unstructured set of points. -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08b.cfg}] [pylithapp.problem.materials.slab] db_initial_stress = spatialdata.spatialdb.SimpleDB

      db_initial_stress.label

      = Initial stress in the slab @@ -1833,8 +1827,7 @@ \subsubsection{Step 8b} spatialdb/mat_initial_stress_grav-crust.spatialdb \end{cfg} -We run the sub-problem by typing: -\begin{shell} +\begin{shell}[Run Step 8b simulation] $ pylith step08b.cfg mat_elastic.cfg solver_algebraicmultigrid.cfg \end{shell} This simulation will produce files in the \filename{output} directory @@ -1873,7 +1866,7 @@ \subsubsection{Step 8c} The only difference between the parameters in \filename{step08b.cfg} and \filename{step08c.cfg} is in the formulation setting and the simulation time: -\begin{cfg} +\begin{cfg}[Excerpt from \filename{step08c.cfg}] [pylithapp.timedependent] # Turn on the small strain formulation, which automatically runs the # simulation as a nonlinear problem. @@ -1887,9 +1880,8 @@ \subsubsection{Step 8c}

      total_time

      = 100.0*year

      dt

      = 10.0*year \end{cfg} -We use the material settings in \filename{mat\_viscoelastic.cfg}. We -can run the simulation by typing: -\begin{shell} +We use the material settings in \filename{mat\_viscoelastic.cfg}. +\begin{shell}[Run Step 8c simulation] $ pylith step08c.cfg mat_viscoelastic.cfg solver_algebraicmultigrid.cfg \end{shell} This simulation will produce files in the \filename{output} directory diff --git a/doc/userguide/examples/twohex8.tex b/doc/userguide/examples/twohex8.tex index 2567e4d13e..ac30d3d4ea 100644 --- a/doc/userguide/examples/twohex8.tex +++ b/doc/userguide/examples/twohex8.tex @@ -65,7 +65,7 @@ \subsection{Additional Common Information} [pylithapp.timedependent.materials.material]

      label

      = viscoelastic material

      id

      = 1 -db = spatialdata.spatialdb.UniformDB +db = spatialdata.spatialdb.UniformDB

      db.values

      = [vp, vs, density, viscosity]

      db.data

      = [5773.502691896258*m/s, 3333.333333333333*m/s, 2700.0*kg/m**3, 1.0e18*Pa*s] diff --git a/doc/userguide/examples/twotri3.tex b/doc/userguide/examples/twotri3.tex index 31a58f73ba..541b936b69 100644 --- a/doc/userguide/examples/twotri3.tex +++ b/doc/userguide/examples/twotri3.tex @@ -78,16 +78,14 @@ \subsection{Additional Common Information} the preconditioner type.} \end{inventory} All of the problems in this directory use the same material database, -as specified under -\begin{cfg} -[pylithapp.timedependent.materials] -\end{cfg} -in \filename{pylithapp.cfg}. This information is contained in the file -\filename{matprops.spatialdb}. Although the material model is specified -in \filename{pylithapp.cfg}, the values for the physical properties -of the material are given in \filename{matprops.spatialdb}. For this -example, values describing elastic plane strain material properties -are given at a single point, resulting in uniform material properties. +as specified under \object{pylithapp.timedependent.materials} in +\filename{pylithapp.cfg}. This information is contained in the file +\filename{matprops.spatialdb}. Although the material model is +specified in \filename{pylithapp.cfg}, the values for the physical +properties of the material are given in +\filename{matprops.spatialdb}. For this example, values describing +elastic plane strain material properties are given at a single point, +resulting in uniform material properties. \subsection{Axial Displacement Example} @@ -123,7 +121,7 @@ \subsection{Axial Displacement Example} \filename{axialdisp.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith axialdisp.cfg +$ pylith axialdisp.cfg \end{shell} Once the problem has run, three files will be produced. The first file is named \filename{axialdisp\_t0000000.vtk}. The \filename{t0000000} @@ -177,7 +175,7 @@ \subsection{Shear Displacement Example} \filename{sheardisp.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith sheardisp.cfg +$ pylith sheardisp.cfg \end{shell} Once the problem has run, three files will be produced as in the previous example. If the problem ran correctly, you should be able to @@ -243,7 +241,7 @@ \subsection{Kinematic Fault Slip Example} \filename{dislocation\_sliptime.spatialdb}) provide a complete description of the problem, and we can then run this example by typing \begin{shell} -$$ pylith dislocation.cfg +$ pylith dislocation.cfg \end{shell} Once the problem has run, five files are produced. In addition to the files produced in the previous two examples, this example produces two From aa3bae7d730ee83ba9e9b1c9d691cfc7c58e369f Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 15:38:31 -0700 Subject: [PATCH 212/216] Updated code listings. --- doc/userguide/examples/subduction2d.tex | 21 +++++++++------------ 1 file changed, 9 insertions(+), 12 deletions(-) diff --git a/doc/userguide/examples/subduction2d.tex b/doc/userguide/examples/subduction2d.tex index ca0eb98db0..e70ae2865a 100644 --- a/doc/userguide/examples/subduction2d.tex +++ b/doc/userguide/examples/subduction2d.tex @@ -174,8 +174,8 @@ \subsection{Step 1: Coseismic Slip Simulation} \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the base filenames for HDF5 output (for example, \filename{step01.h5}).} \end{inventory} -We run this example by typing -\begin{shell} + +\begin{shell}[Run Step 1 simulation] $ pylith step01.cfg \end{shell} The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 @@ -226,8 +226,8 @@ \subsection{Step 2: Interseismic Deformation Simulation} \facilityitem{pylithapp.problem.formulation.output.domain}{Gives the base filename for HDF5 output (for example, \filename{step02.h5}).} \end{inventory} -We run this example by typing -\begin{shell} + +\begin{shell}[Run Step 2 simulation] $ pylith step02.cfg \end{shell} The simulation will produce pairs of HDF5/Xdmf files with separate @@ -302,10 +302,10 @@ \subsection{Step 4: Frictional Afterslip Simulation} and a background stress field. The background stress field is simply normal tractions consistent with the overburden (lithostatic load) for a uniform half-space and shear tractions consistent with a coefficient -of friction of 0.6. The \texttt{afterslip\_tractions.} spatialdb +of friction of 0.6. The \texttt{afterslip\_tractions.spatialdb} file is provided, so you do not need to run the Python script \filename{afterslip\_tractions.py}; however, you can do so by typing -\begin{shell} +\begin{shell}[Optional: Generate \filename{afterslip\_tractions.spatialdb}] $ python afterslip_tractions.py \end{shell} We provide 2.0 MPa of strength excess associated with the background @@ -332,8 +332,7 @@ \subsection{Step 4: Frictional Afterslip Simulation} for HDF5 output (for example, \filename{step04.h5}).} \end{inventory} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 4 simulation] $ pylith step04.cfg \end{shell} The problem will produce twelve pairs of HDF5/Xdmf files. The HDF5 @@ -495,8 +494,7 @@ \subsection{Step 5: Spontaneous Earthquakes With Slip-Weakening Friction}

      friction_ksp_error_if_not_converged

      = true \end{cfg} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 5 simulation] $ pylith step05.cfg \end{shell} The problem will produce fourteen pairs of HDF5/Xdmf files. Figure @@ -592,8 +590,7 @@ \subsection{Step 6: Spontaneous Earthquakes With Rate-State Friction}

      vertex_data_fields

      = [slip, slip_rate, traction, state_variable] \end{cfg} -We run this example by typing -\begin{shell} +\begin{shell}[Run Step 6 simulation] $ pylith step06.cfg \end{shell} The problem will produce fourteen pairs of HDF5/Xdmf files. Figure From 5d41a5ec134d29c5e7a038490a21b4755c9a776c Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Fri, 1 Sep 2017 15:38:48 -0700 Subject: [PATCH 213/216] Improve color scheme. --- doc/userguide/pylithdoc.cls | 37 +++++++++++++++++++----------------- doc/userguide/styleguide.tex | 2 +- 2 files changed, 21 insertions(+), 18 deletions(-) diff --git a/doc/userguide/pylithdoc.cls b/doc/userguide/pylithdoc.cls index ffd77a4942..9b7f8a0e65 100644 --- a/doc/userguide/pylithdoc.cls +++ b/doc/userguide/pylithdoc.cls @@ -78,26 +78,29 @@ \renewcommand{\footnotesize}{\@setfontsize\footnotesize{8}{9.5}} % % Colors -\definecolor{yellow}{rgb}{1.0, 1.0, 0.45} % 255/255/115 -\definecolor{dkyellow}{rgb}{0.9, 0.9, 0.0} % % 230/230/0 +\definecolor{ltred}{rgb}{1.0, 0.57, 0.59} % 255/145/151 +\definecolor{red}{rgb}{0.63, 0.00, 0.06} % 161/0/16 -\definecolor{ltorange}{rgb}{1.0, 0.74, 0.41} % 255/188/105 -\definecolor{orange}{rgb}{0.96, 0.50, 0.0} % 246/127/0 +\definecolor{ltblue}{rgb}{0.57, 0.59, 1.00} % 145/151/255 +\definecolor{mdblue}{rgb}{0.28, 0.50, 0.80} % 72/128/205 +\definecolor{blue}{rgb}{0.00, 0.06, 0.63} % 0/16/161 -\definecolor{ltred}{rgb}{1.0, 0.25, 0.25} % 255/64/64 -\definecolor{red}{rgb}{0.79, 0.00, 0.01} % 201/0/3 +\definecolor{ltgreen}{rgb}{0.59, 1.00, 0.57} % 151/255/145 +\definecolor{green}{rgb}{0.06, 0.63, 0.00} % 16/161/0 -\definecolor{ltpurple}{rgb}{0.81, 0.57, 1.00} % 206/145/255 -\definecolor{purple}{rgb}{0.38, 0.00, 0.68} % 97/1/175 +\definecolor{ltpurple}{rgb}{0.62, 0.29, 0.63} % 157/75/161 +\definecolor{purple}{rgb}{0.63, 0.00, 0.54} % 131/1/138 -\definecolor{ltblue}{rgb}{0.2, 0.73, 1.0} % 51/187/255 -\definecolor{mdblue}{rgb}{0.28, 0.50, 0.80} % 72/128/205 -\definecolor{blue}{rgb}{0.12, 0.43, 0.59} % 30/110/150 +\definecolor{ltcyan}{rgb}{0.33, 0.70, 0.68} % 83/179/174 +\definecolor{cyan}{rgb}{0.00, 0.54, 0.51} % 1/138/131 + +\definecolor{ltyellow}{rgb}{1.0, 0.97, 0.46} % 255/248/118 +\definecolor{yellow}{rgb}{0.90, 0.83, 0.0} % % 230/211/0 + + +\definecolor{ltorange}{rgb}{1.0, 0.74, 0.35} % 255/189/89 +\definecolor{orange}{rgb}{0.87, 0.45, 0.0} % 222/115/0 -\definecolor{ltltgreen}{rgb}{0.7, 1.00, 0.7} % 96/204/14 -\definecolor{ltgreen}{rgb}{0.37, 0.80, 0.05} % 96/204/14 -\definecolor{green}{rgb}{0.23, 0.49, 0.03} % 59/125/8 - \definecolor{dkslate}{rgb}{0.18, 0.21, 0.28} % 47/53/72 \definecolor{mdslate}{rgb}{0.45, 0.50, 0.68} % 114/127/173 \definecolor{ltslate}{rgb}{0.85, 0.88, 0.95} % 216/225/229 @@ -227,7 +230,7 @@ moredelim=[is][\color{blue}\bfseries]{}{}, } \lstnewenvironment{cfg}[1][\@empty]{% - \def\captioncolor{blue} + \def\captioncolor{cyan} \def\@makecaption{\lst@makecaption} \lstset{% language=cfg, @@ -239,7 +242,7 @@ % shell % \lstnewenvironment{shell}[1][\@empty]{% - \def\captioncolor{green} + \def\captioncolor{mdslate} \def\@makecaption{\lst@makecaption} \lstset{% language=bash,% diff --git a/doc/userguide/styleguide.tex b/doc/userguide/styleguide.tex index d284898832..31a854d2d7 100644 --- a/doc/userguide/styleguide.tex +++ b/doc/userguide/styleguide.tex @@ -33,7 +33,7 @@ Use the {\tt shell} environment when listing commands to be run in a Unix shell. % Example use of shell environment. -\begin{shell} +\begin{shell}[Bash shell] # This is a comment. $ ls -l \end{shell} From 837ec0286ed788f65282de09d171530a5d7a4900 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Sat, 2 Sep 2017 16:06:20 -0700 Subject: [PATCH 214/216] Fix EAR grant number. --- doc/userguide/preface.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/doc/userguide/preface.tex b/doc/userguide/preface.tex index bf27461240..4cf8ee401f 100644 --- a/doc/userguide/preface.tex +++ b/doc/userguide/preface.tex @@ -103,7 +103,7 @@ \section{Support} This material is based upon work supported by the National Science Foundation under Grants No. 0313238, 0745391, 1150901, and -EAR-0949446. Any opinions, findings, and conclusions or +EAR-1550901. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation. From 85e2ddd14629c0b877d3e60148376bcf55168677 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 5 Sep 2017 09:19:09 -0700 Subject: [PATCH 215/216] Updated list of changes. --- CHANGES | 8 +++++--- doc/releasenotes/announce_v2.2.1.txt | 8 +++++--- doc/userguide/intro/intro.tex | 12 +++++++----- 3 files changed, 17 insertions(+), 11 deletions(-) diff --git a/CHANGES b/CHANGES index 2808eee6c3..dd0c075acd 100644 --- a/CHANGES +++ b/CHANGES @@ -19,8 +19,8 @@ Version 2.2.1 illustrates a wide range of PyLith features for quasi-static simulations. - examples/2d/subduction: Added quasi-static spontaneous rupture - earthquake cycle examples for slip-weakening and rate- and - state-friction. + earthquake cycle examples (Steps 5 and 6) for slip-weakening and + rate- and state-friction. - These new examples make use of ParaView Python scripts to facilitate using ParaView with PyLith. @@ -41,7 +41,9 @@ Version 2.2.1 * Updated spatialdata to v1.9.10. Improved error messages when reading SimpleDB and SimpleGridDB files. -* Updated PyLith parameter viewer to v1.0.1. Small fix to insure +* Updated PyLith parameter viewer to v1.1.0. Application and + documentation are now available on line at + https://geodynamics.github.io/pylith_parameters. Small fix to insure hierarchy path listed matches the one for PyLith. * Updated PETSc to v3.7.6. See the PETSc documentation for a summary diff --git a/doc/releasenotes/announce_v2.2.1.txt b/doc/releasenotes/announce_v2.2.1.txt index 400150e200..44d0fb22ea 100644 --- a/doc/releasenotes/announce_v2.2.1.txt +++ b/doc/releasenotes/announce_v2.2.1.txt @@ -35,8 +35,8 @@ RELEASE NOTES illustrates a wide range of PyLith features for quasi-static simulations. - examples/2d/subduction: Added quasi-static spontaneous rupture - earthquake cycle examples for slip-weakening and rate- and - state-friction. + earthquake cycle examples (Steps 5 and 6) for slip-weakening and + rate- and state-friction. - These new examples make use of ParaView Python scripts to facilitate using ParaView with PyLith. @@ -57,7 +57,9 @@ RELEASE NOTES * Updated spatialdata to v1.9.10. Improved error messages when reading SimpleDB and SimpleGridDB files. -* Updated PyLith parameter viewer to v1.0.1. Small fix to insure +* Updated PyLith parameter viewer to v1.1.0. Application and + documentation are now available on line at + https://geodynamics.github.io/pylith_parameters. Small fix to insure hierarchy path listed matches the one for PyLith. * Updated PETSc to v3.7.6. See the PETSc documentation for a summary diff --git a/doc/userguide/intro/intro.tex b/doc/userguide/intro/intro.tex index 7548b0e2d2..9b8d1664f9 100644 --- a/doc/userguide/intro/intro.tex +++ b/doc/userguide/intro/intro.tex @@ -17,9 +17,9 @@ \section{New in PyLith Version \pylithVersionNumber} \item \filename{examples/3d/subduction}: New suite of examples for a 3-D subduction zone. This intermediate level suite of examples illustrates a wide range of PyLith features for quasi-static simulations. - \item \filename{examples/2d/subduction}: Added quasi-static spontaneous rupture - earthquake cycle examples for slip-weakening and rate- and - state-friction. + \item \filename{examples/2d/subduction}: Added quasi-static + spontaneous rupture earthquake cycle examples (Steps 5 and 6) for + slip-weakening and rate- and state-friction. \item These new examples make use of ParaView Python scripts to facilitate using ParaView with PyLith. \end{itemize} @@ -36,8 +36,10 @@ \section{New in PyLith Version \pylithVersionNumber} generation of Xdmf files from Python scripts. \item Updated spatialdata to v1.9.10. Improved error messages when reading SimpleDB and SimpleGridDB files. -\item Updated PyLith parameter viewer to v1.0.1. Small fix to insure - hierarchy path listed matches the one for PyLith. +\item Updated PyLith parameter viewer to v1.1.0. Application and + documentation are now available online + (\url{https://geodynamics.github.io/pylith_parameters/}). Small fix + to insure hierarchy path listed matches the one for PyLith. \item Updated PETSc to v3.7.6. See the PETSc documentation for a summary of all of the changes. \item Switched to using CentOS 6.9 for Linux binary builds to insure From 3c4fab7d82ffbd38e6687ed512ccf3ef15298c70 Mon Sep 17 00:00:00 2001 From: Brad Aagaard Date: Tue, 5 Sep 2017 09:47:55 -0700 Subject: [PATCH 216/216] Fix typo in Makefile.am. --- libsrc/pylith/Makefile.am | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/libsrc/pylith/Makefile.am b/libsrc/pylith/Makefile.am index 697a174c48..7b64c457e3 100644 --- a/libsrc/pylith/Makefile.am +++ b/libsrc/pylith/Makefile.am @@ -166,7 +166,7 @@ if ENABLE_HDF5 libpylith_la_SOURCES += \ meshio/HDF5.cc \ meshio/DataWriterHDF5.cc \ - meshio/DataWriterHDF5Ext.cc \ + meshio/DataWriterHDF5Ext.cc libpylith_la_LIBADD += -lhdf5 endif

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