Merge branch 'modernize-testing' into 'development'
Modernize testing See merge request damask/DAMASK!289
This commit is contained in:
commit
a70c69718b
103
.gitlab-ci.yml
103
.gitlab-ci.yml
|
@ -2,14 +2,10 @@
|
|||
stages:
|
||||
- prepareAll
|
||||
- python
|
||||
- preprocessing
|
||||
- postprocessing
|
||||
- compilePETSc
|
||||
- prepareGrid
|
||||
- deprecated
|
||||
- compile
|
||||
- grid
|
||||
- compileMarc
|
||||
- marc
|
||||
- example
|
||||
- performance
|
||||
- createPackage
|
||||
- createDocumentation
|
||||
|
@ -111,71 +107,70 @@ Pytest_python:
|
|||
|
||||
###################################################################################################
|
||||
Pre_SeedGeneration:
|
||||
stage: preprocessing
|
||||
stage: deprecated
|
||||
script: PreProcessing_SeedGeneration/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Pre_GeomGeneration:
|
||||
stage: preprocessing
|
||||
stage: deprecated
|
||||
script: PreProcessing_GeomGeneration/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Pre_GeomModification:
|
||||
stage: preprocessing
|
||||
stage: deprecated
|
||||
script: PreProcessing_GeomModification/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Pre_General:
|
||||
stage: preprocessing
|
||||
stage: deprecated
|
||||
script: PreProcessing/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
Post_General:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script: PostProcessing/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Post_GeometryReconstruction:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script: spectral_geometryReconstruction/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Post_addCurl:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script: addCurl/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Post_addDivergence:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script: addDivergence/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Post_addGradient:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script: addGradient/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Post_OrientationAverageMisorientation:
|
||||
stage: postprocessing
|
||||
stage: deprecated
|
||||
script:
|
||||
- OrientationAverageMisorientation/test.py
|
||||
except:
|
||||
|
@ -183,8 +178,8 @@ Post_OrientationAverageMisorientation:
|
|||
- release
|
||||
|
||||
###################################################################################################
|
||||
grid_mech_compile_Intel:
|
||||
stage: compilePETSc
|
||||
compile_grid_Intel:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $IntelCompiler $MPICH_Intel $PETSc_MPICH_Intel
|
||||
- cd pytest
|
||||
|
@ -193,8 +188,8 @@ grid_mech_compile_Intel:
|
|||
- master
|
||||
- release
|
||||
|
||||
Compile_FEM_Intel:
|
||||
stage: compilePETSc
|
||||
compile_mesh_Intel:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $IntelCompiler $MPICH_Intel $PETSc_MPICH_Intel
|
||||
- cd pytest
|
||||
|
@ -203,8 +198,8 @@ Compile_FEM_Intel:
|
|||
- master
|
||||
- release
|
||||
|
||||
grid_mech_compile_GNU:
|
||||
stage: compilePETSc
|
||||
compile_grid_GNU:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $GNUCompiler $MPICH_GNU $PETSc_MPICH_GNU
|
||||
- cd pytest
|
||||
|
@ -213,8 +208,8 @@ grid_mech_compile_GNU:
|
|||
- master
|
||||
- release
|
||||
|
||||
Compile_FEM_GNU:
|
||||
stage: compilePETSc
|
||||
compile_mesh_GNU:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $GNUCompiler $MPICH_GNU $PETSc_MPICH_GNU
|
||||
- cd pytest
|
||||
|
@ -223,13 +218,36 @@ Compile_FEM_GNU:
|
|||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
Compile_Intel_Prepare:
|
||||
stage: prepareGrid
|
||||
compile_MARC:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $IntelMarc $HDF5Marc $MSC
|
||||
- cd pytest
|
||||
- pytest -k 'compile and Marc' --basetemp=${TESTROOT}/compile_Marc
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
setup_grid:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $IntelCompiler $MPICH_Intel $PETSc_MPICH_Intel
|
||||
- cd $DAMASKROOT
|
||||
- make clean grid processing
|
||||
- BUILD_DIR=$(mktemp -d)
|
||||
- cd ${BUILD_DIR}
|
||||
- cmake -DDAMASK_SOLVER=GRID -DCMAKE_INSTALL_PREFIX=${DAMASKROOT} ${DAMASKROOT}
|
||||
- make -j2 all install
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
setup_mesh:
|
||||
stage: compile
|
||||
script:
|
||||
- module load $IntelCompiler $MPICH_Intel $PETSc_MPICH_Intel
|
||||
- BUILD_DIR=$(mktemp -d)
|
||||
- cd ${BUILD_DIR}
|
||||
- cmake -DDAMASK_SOLVER=MESH -DCMAKE_INSTALL_PREFIX=${DAMASKROOT} ${DAMASKROOT}
|
||||
- make -j2 all install
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
@ -252,13 +270,6 @@ Thermal:
|
|||
- master
|
||||
- release
|
||||
|
||||
grid_parsingArguments:
|
||||
stage: grid
|
||||
script: grid_parsingArguments/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
Nonlocal_Damage_DetectChanges:
|
||||
stage: grid
|
||||
script: Nonlocal_Damage_DetectChanges/test.py
|
||||
|
@ -280,16 +291,6 @@ Phenopowerlaw_singleSlip:
|
|||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
Marc_compileIfort:
|
||||
stage: compileMarc
|
||||
script:
|
||||
- module load $IntelMarc $HDF5Marc $MSC
|
||||
- cd pytest
|
||||
- pytest -k 'compile and Marc' --basetemp=${TESTROOT}/compile_Marc
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
Hex_elastic:
|
||||
|
@ -337,14 +338,6 @@ Marc_elementLib:
|
|||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
grid_all_example:
|
||||
stage: example
|
||||
script: grid_all_example/test.py
|
||||
except:
|
||||
- master
|
||||
- release
|
||||
|
||||
###################################################################################################
|
||||
SpectralRuntime:
|
||||
stage: performance
|
||||
|
|
2
PRIVATE
2
PRIVATE
|
@ -1 +1 @@
|
|||
Subproject commit 8bd09b5511d1e0e0ea288b47d16ce4924d75adcd
|
||||
Subproject commit a6be226f2ab08cfa44adabf37168f4d952d6174f
|
|
@ -13,85 +13,6 @@ import damask
|
|||
scriptName = os.path.splitext(os.path.basename(__file__))[0]
|
||||
scriptID = ' '.join([scriptName,damask.version])
|
||||
|
||||
def volTetrahedron(coords):
|
||||
"""
|
||||
Return the volume of the tetrahedron with given vertices or sides.
|
||||
|
||||
If vertices are given they must be in a NumPy array with shape (4,3): the
|
||||
position vectors of the 4 vertices in 3 dimensions; if the six sides are
|
||||
given, they must be an array of length 6. If both are given, the sides
|
||||
will be used in the calculation.
|
||||
|
||||
This method implements
|
||||
Tartaglia's formula using the Cayley-Menger determinant:
|
||||
|0 1 1 1 1 |
|
||||
|1 0 s1^2 s2^2 s3^2|
|
||||
288 V^2 = |1 s1^2 0 s4^2 s5^2|
|
||||
|1 s2^2 s4^2 0 s6^2|
|
||||
|1 s3^2 s5^2 s6^2 0 |
|
||||
where s1, s2, ..., s6 are the tetrahedron side lengths.
|
||||
|
||||
from http://codereview.stackexchange.com/questions/77593/calculating-the-volume-of-a-tetrahedron
|
||||
"""
|
||||
# The indexes of rows in the vertices array corresponding to all
|
||||
# possible pairs of vertices
|
||||
vertex_pair_indexes = np.array(((0, 1), (0, 2), (0, 3),
|
||||
(1, 2), (1, 3), (2, 3)))
|
||||
|
||||
# Get all the squares of all side lengths from the differences between
|
||||
# the 6 different pairs of vertex positions
|
||||
vertices = np.concatenate((coords[0],coords[1],coords[2],coords[3])).reshape(4,3)
|
||||
vertex1, vertex2 = vertex_pair_indexes[:,0], vertex_pair_indexes[:,1]
|
||||
sides_squared = np.sum((vertices[vertex1] - vertices[vertex2])**2,axis=-1)
|
||||
|
||||
|
||||
# Set up the Cayley-Menger determinant
|
||||
M = np.zeros((5,5))
|
||||
# Fill in the upper triangle of the matrix
|
||||
M[0,1:] = 1
|
||||
# The squared-side length elements can be indexed using the vertex
|
||||
# pair indices (compare with the determinant illustrated above)
|
||||
M[tuple(zip(*(vertex_pair_indexes + 1)))] = sides_squared
|
||||
|
||||
# The matrix is symmetric, so we can fill in the lower triangle by
|
||||
# adding the transpose
|
||||
M = M + M.T
|
||||
return np.sqrt(np.linalg.det(M) / 288)
|
||||
|
||||
|
||||
def volumeMismatch(size,F,nodes):
|
||||
"""
|
||||
Calculates the volume mismatch.
|
||||
|
||||
volume mismatch is defined as the difference between volume of reconstructed
|
||||
(compatible) cube and determinant of deformation gradient at Fourier point.
|
||||
"""
|
||||
coords = np.empty([8,3])
|
||||
vMismatch = np.empty(F.shape[:3])
|
||||
|
||||
#--------------------------------------------------------------------------------------------------
|
||||
# calculate actual volume and volume resulting from deformation gradient
|
||||
for k in range(grid[0]):
|
||||
for j in range(grid[1]):
|
||||
for i in range(grid[2]):
|
||||
coords[0,0:3] = nodes[k, j, i ,0:3]
|
||||
coords[1,0:3] = nodes[k ,j, i+1,0:3]
|
||||
coords[2,0:3] = nodes[k ,j+1,i+1,0:3]
|
||||
coords[3,0:3] = nodes[k, j+1,i ,0:3]
|
||||
coords[4,0:3] = nodes[k+1,j, i ,0:3]
|
||||
coords[5,0:3] = nodes[k+1,j, i+1,0:3]
|
||||
coords[6,0:3] = nodes[k+1,j+1,i+1,0:3]
|
||||
coords[7,0:3] = nodes[k+1,j+1,i ,0:3]
|
||||
vMismatch[k,j,i] = \
|
||||
( abs(volTetrahedron([coords[6,0:3],coords[0,0:3],coords[7,0:3],coords[3,0:3]])) \
|
||||
+ abs(volTetrahedron([coords[6,0:3],coords[0,0:3],coords[7,0:3],coords[4,0:3]])) \
|
||||
+ abs(volTetrahedron([coords[6,0:3],coords[0,0:3],coords[2,0:3],coords[3,0:3]])) \
|
||||
+ abs(volTetrahedron([coords[6,0:3],coords[0,0:3],coords[2,0:3],coords[1,0:3]])) \
|
||||
+ abs(volTetrahedron([coords[6,0:3],coords[4,0:3],coords[1,0:3],coords[5,0:3]])) \
|
||||
+ abs(volTetrahedron([coords[6,0:3],coords[4,0:3],coords[1,0:3],coords[0,0:3]]))) \
|
||||
/np.linalg.det(F[k,j,i,0:3,0:3])
|
||||
return vMismatch/(size.prod()/grid.prod())
|
||||
|
||||
|
||||
def shapeMismatch(size,F,nodes,centres):
|
||||
"""
|
||||
|
@ -101,35 +22,16 @@ def shapeMismatch(size,F,nodes,centres):
|
|||
the corners of reconstructed (combatible) volume element and the vectors calculated by deforming
|
||||
the initial volume element with the current deformation gradient.
|
||||
"""
|
||||
sMismatch = np.empty(F.shape[:3])
|
||||
|
||||
#--------------------------------------------------------------------------------------------------
|
||||
# initial positions
|
||||
delta = size/grid*.5
|
||||
coordsInitial = np.vstack((delta * np.array((-1,-1,-1)),
|
||||
delta * np.array((+1,-1,-1)),
|
||||
delta * np.array((+1,+1,-1)),
|
||||
delta * np.array((-1,+1,-1)),
|
||||
delta * np.array((-1,-1,+1)),
|
||||
delta * np.array((+1,-1,+1)),
|
||||
delta * np.array((+1,+1,+1)),
|
||||
delta * np.array((-1,+1,+1))))
|
||||
|
||||
#--------------------------------------------------------------------------------------------------
|
||||
# compare deformed original and deformed positions to actual positions
|
||||
for k in range(grid[0]):
|
||||
for j in range(grid[1]):
|
||||
for i in range(grid[2]):
|
||||
sMismatch[k,j,i] = \
|
||||
+ np.linalg.norm(nodes[k, j, i ,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[0,0:3]))\
|
||||
+ np.linalg.norm(nodes[k+1,j, i ,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[1,0:3]))\
|
||||
+ np.linalg.norm(nodes[k+1,j+1,i ,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[2,0:3]))\
|
||||
+ np.linalg.norm(nodes[k, j+1,i ,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[3,0:3]))\
|
||||
+ np.linalg.norm(nodes[k, j, i+1,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[4,0:3]))\
|
||||
+ np.linalg.norm(nodes[k+1,j, i+1,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[5,0:3]))\
|
||||
+ np.linalg.norm(nodes[k+1,j+1,i+1,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[6,0:3]))\
|
||||
+ np.linalg.norm(nodes[k ,j+1,i+1,0:3] - centres[k,j,i,0:3] - np.dot(F[k,j,i,:,:], coordsInitial[7,0:3]))
|
||||
return sMismatch
|
||||
return + np.linalg.norm(nodes[:-1,:-1,:-1] -centres - np.dot(F,delta * np.array((-1,-1,-1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[+1:,:-1,:-1] -centres - np.dot(F,delta * np.array((+1,-1,-1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[+1:,+1:,:-1] -centres - np.dot(F,delta * np.array((+1,+1,-1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[:-1,+1:,:-1] -centres - np.dot(F,delta * np.array((-1,+1,-1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[:-1,:-1,+1:] -centres - np.dot(F,delta * np.array((-1,-1,+1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[+1:,:-1,+1:] -centres - np.dot(F,delta * np.array((+1,-1,+1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[+1:,+1:,+1:] -centres - np.dot(F,delta * np.array((+1,+1,+1))),axis=-1)\
|
||||
+ np.linalg.norm(nodes[:-1,+1:,+1:] -centres - np.dot(F,delta * np.array((-1,+1,+1))),axis=-1)
|
||||
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
@ -155,10 +57,6 @@ parser.add_option('--no-shape','-s',
|
|||
dest = 'shape',
|
||||
action = 'store_false',
|
||||
help = 'omit shape mismatch')
|
||||
parser.add_option('--no-volume','-v',
|
||||
dest = 'volume',
|
||||
action = 'store_false',
|
||||
help = 'omit volume mismatch')
|
||||
parser.set_defaults(pos = 'pos',
|
||||
defgrad = 'f',
|
||||
shape = True,
|
||||
|
@ -185,10 +83,4 @@ for name in filenames:
|
|||
shapeMismatch.reshape(-1,1,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
if options.volume:
|
||||
volumeMismatch = volumeMismatch(size,F,nodes)
|
||||
table = table.add('volMismatch(({}))'.format(options.defgrad),
|
||||
volumeMismatch.reshape(-1,1,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -55,4 +55,4 @@ for name in filenames:
|
|||
curl.reshape(tuple(grid)+(-1,)).reshape(-1,np.prod(shape),order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -1,74 +0,0 @@
|
|||
#!/usr/bin/env python3
|
||||
|
||||
import os
|
||||
import sys
|
||||
from io import StringIO
|
||||
from optparse import OptionParser
|
||||
|
||||
import numpy as np
|
||||
|
||||
import damask
|
||||
|
||||
|
||||
scriptName = os.path.splitext(os.path.basename(__file__))[0]
|
||||
scriptID = ' '.join([scriptName,damask.version])
|
||||
|
||||
def derivative(coordinates,what):
|
||||
|
||||
result = np.empty_like(what)
|
||||
|
||||
# use differentiation by interpolation
|
||||
# as described in http://www2.math.umd.edu/~dlevy/classes/amsc466/lecture-notes/differentiation-chap.pdf
|
||||
|
||||
result[1:-1,:] = + what[1:-1,:] * (2.*coordinates[1:-1]-coordinates[:-2]-coordinates[2:]) / \
|
||||
((coordinates[1:-1]-coordinates[:-2])*(coordinates[1:-1]-coordinates[2:])) \
|
||||
+ what[2:,:] * (coordinates[1:-1]-coordinates[:-2]) / \
|
||||
((coordinates[2:]-coordinates[1:-1])*(coordinates[2:]-coordinates[:-2])) \
|
||||
+ what[:-2,:] * (coordinates[1:-1]-coordinates[2:]) / \
|
||||
((coordinates[:-2]-coordinates[1:-1])*(coordinates[:-2]-coordinates[2:])) \
|
||||
|
||||
result[0,:] = (what[0,:] - what[1,:]) / \
|
||||
(coordinates[0] - coordinates[1])
|
||||
result[-1,:] = (what[-1,:] - what[-2,:]) / \
|
||||
(coordinates[-1] - coordinates[-2])
|
||||
|
||||
return result
|
||||
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
# MAIN
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
parser = OptionParser(option_class=damask.extendableOption, usage='%prog options [ASCIItable(s)]', description = """
|
||||
Add column(s) containing numerical derivative of requested column(s) with respect to given coordinates.
|
||||
|
||||
""", version = scriptID)
|
||||
|
||||
parser.add_option('-c','--coordinates',
|
||||
dest = 'coordinates',
|
||||
type = 'string', metavar='string',
|
||||
help = 'heading of coordinate column')
|
||||
parser.add_option('-l','--label',
|
||||
dest = 'labels',
|
||||
action = 'extend', metavar = '<string LIST>',
|
||||
help = 'heading of column(s) to differentiate')
|
||||
|
||||
|
||||
(options,filenames) = parser.parse_args()
|
||||
if filenames == []: filenames = [None]
|
||||
|
||||
if options.coordinates is None:
|
||||
parser.error('no coordinate column specified.')
|
||||
if options.labels is None:
|
||||
parser.error('no data column specified.')
|
||||
|
||||
for name in filenames:
|
||||
damask.util.report(scriptName,name)
|
||||
|
||||
table = damask.Table.load(StringIO(''.join(sys.stdin.read())) if name is None else name)
|
||||
for label in options.labels:
|
||||
table = table.add('d({})/d({})'.format(label,options.coordinates),
|
||||
derivative(table.get(options.coordinates),table.get(label)),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
|
@ -60,7 +60,7 @@ for name in filenames:
|
|||
.add('fluct({}).{}'.format(options.f,options.pos),
|
||||
damask.grid_filters.node_displacement_fluct(size,F).reshape(-1,3,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))\
|
||||
.save((sys.stdout if name is None else os.path.splitext(name)[0]+'_nodal.txt'), legacy=True)
|
||||
.save((sys.stdout if name is None else os.path.splitext(name)[0]+'_nodal.txt'))
|
||||
else:
|
||||
table.add('avg({}).{}'.format(options.f,options.pos),
|
||||
damask.grid_filters.cell_displacement_avg(size,F).reshape(-1,3,order='F'),
|
||||
|
@ -68,4 +68,4 @@ for name in filenames:
|
|||
.add('fluct({}).{}'.format(options.f,options.pos),
|
||||
damask.grid_filters.cell_displacement_fluct(size,F).reshape(-1,3,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))\
|
||||
.save((sys.stdout if name is None else name), legacy=True)
|
||||
.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -55,4 +55,4 @@ for name in filenames:
|
|||
div.reshape(tuple(grid)+(-1,)).reshape(-1,np.prod(shape)//3,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -184,4 +184,4 @@ for name in filenames:
|
|||
distance[i,:],
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -55,4 +55,4 @@ for name in filenames:
|
|||
grad.reshape(tuple(grid)+(-1,)).reshape(-1,np.prod(shape)*3,order='F'),
|
||||
scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
|
@ -1,150 +0,0 @@
|
|||
#!/usr/bin/env python3
|
||||
|
||||
import os
|
||||
import sys
|
||||
from io import StringIO
|
||||
from optparse import OptionParser
|
||||
|
||||
import numpy as np
|
||||
|
||||
import damask
|
||||
|
||||
|
||||
scriptName = os.path.splitext(os.path.basename(__file__))[0]
|
||||
scriptID = ' '.join([scriptName,damask.version])
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
# MAIN
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
parser = OptionParser(option_class=damask.extendableOption, usage='%prog options [ASCIItable(s)]', description = """
|
||||
Add quaternion and/or Bunge Euler angle representation of crystal lattice orientation.
|
||||
Orientation is given by quaternion, Euler angles, rotation matrix, or crystal frame coordinates
|
||||
(i.e. component vectors of rotation matrix).
|
||||
Additional (globally fixed) rotations of the lab frame and/or crystal frame can be applied.
|
||||
|
||||
""", version = scriptID)
|
||||
|
||||
representations = ['quaternion', 'rodrigues', 'eulers', 'matrix', 'axisangle']
|
||||
|
||||
|
||||
parser.add_option('-o',
|
||||
'--output',
|
||||
dest = 'output',
|
||||
action = 'extend', metavar = '<string LIST>',
|
||||
help = 'output orientation formats {{{}}}'.format(', '.join(representations)))
|
||||
parser.add_option('-d',
|
||||
'--degrees',
|
||||
dest = 'degrees',
|
||||
action = 'store_true',
|
||||
help = 'all angles in degrees')
|
||||
parser.add_option('-R',
|
||||
'--labrotation',
|
||||
dest='labrotation',
|
||||
type = 'float', nargs = 4, metavar = ' '.join(['float']*4),
|
||||
help = 'axis and angle of additional lab frame rotation [%default]')
|
||||
parser.add_option('-r',
|
||||
'--crystalrotation',
|
||||
dest='crystalrotation',
|
||||
type = 'float', nargs = 4, metavar = ' '.join(['float']*4),
|
||||
help = 'axis and angle of additional crystal frame rotation [%default]')
|
||||
parser.add_option('--eulers',
|
||||
dest = 'eulers',
|
||||
metavar = 'string',
|
||||
help = 'Euler angles label')
|
||||
parser.add_option('--rodrigues',
|
||||
dest = 'rodrigues',
|
||||
metavar = 'string',
|
||||
help = 'Rodrigues vector label')
|
||||
parser.add_option('--matrix',
|
||||
dest = 'matrix',
|
||||
metavar = 'string',
|
||||
help = 'orientation matrix label')
|
||||
parser.add_option('--quaternion',
|
||||
dest = 'quaternion',
|
||||
metavar = 'string',
|
||||
help = 'quaternion label')
|
||||
parser.add_option('-x',
|
||||
dest = 'x',
|
||||
metavar = 'string',
|
||||
help = 'label of lab x vector (expressed in crystal coords)')
|
||||
parser.add_option('-y',
|
||||
dest = 'y',
|
||||
metavar = 'string',
|
||||
help = 'label of lab y vector (expressed in crystal coords)')
|
||||
parser.add_option('-z',
|
||||
dest = 'z',
|
||||
metavar = 'string',
|
||||
help = 'label of lab z vector (expressed in crystal coords)')
|
||||
parser.add_option('--lattice',
|
||||
dest = 'lattice',
|
||||
metavar = 'string',
|
||||
help = 'lattice structure to reduce rotation into fundamental zone')
|
||||
|
||||
parser.set_defaults(output = [],
|
||||
labrotation = (1.,1.,1.,0.), # no rotation about (1,1,1)
|
||||
crystalrotation = (1.,1.,1.,0.), # no rotation about (1,1,1)
|
||||
lattice = None,
|
||||
)
|
||||
|
||||
(options, filenames) = parser.parse_args()
|
||||
if filenames == []: filenames = [None]
|
||||
|
||||
if options.output == [] or (not set(options.output).issubset(set(representations))):
|
||||
parser.error('output must be chosen from {}.'.format(', '.join(representations)))
|
||||
|
||||
input = [options.eulers is not None,
|
||||
options.rodrigues is not None,
|
||||
options.x is not None and \
|
||||
options.y is not None and \
|
||||
options.z is not None,
|
||||
options.matrix is not None,
|
||||
options.quaternion is not None,
|
||||
]
|
||||
|
||||
if np.sum(input) != 1: parser.error('needs exactly one input format.')
|
||||
|
||||
r = damask.Rotation.from_axis_angle(np.array(options.crystalrotation),options.degrees,normalize=True)
|
||||
R = damask.Rotation.from_axis_angle(np.array(options.labrotation),options.degrees,normalize=True)
|
||||
|
||||
for name in filenames:
|
||||
damask.util.report(scriptName,name)
|
||||
|
||||
table = damask.Table.load(StringIO(''.join(sys.stdin.read())) if name is None else name)
|
||||
|
||||
if options.eulers is not None:
|
||||
label = options.eulers
|
||||
print(np.max(table.get(options.eulers),axis=0))
|
||||
o = damask.Rotation.from_Euler_angles(table.get(options.eulers), options.degrees)
|
||||
elif options.rodrigues is not None:
|
||||
label = options.rodrigues
|
||||
o = damask.Rotation.from_Rodrigues_vector(table.get(options.rodrigues))
|
||||
elif options.matrix is not None:
|
||||
label = options.matrix
|
||||
o = damask.Rotation.from_matrix(table.get(options.matrix).reshape(-1,3,3))
|
||||
elif options.x is not None:
|
||||
label = '<{},{},{}>'.format(options.x,options.y,options.z)
|
||||
M = np.block([table.get(options.x),table.get(options.y),table.get(options.z)]).reshape(-1,3,3)
|
||||
o = damask.Rotation.from_matrix(M/np.linalg.norm(M,axis=0))
|
||||
elif options.quaternion is not None:
|
||||
label = options.quaternion
|
||||
o = damask.Rotation.from_quaternion(table.get(options.quaternion))
|
||||
|
||||
o = r.broadcast_to(o.shape) @ o @ R.broadcast_to(o.shape)
|
||||
|
||||
#if options.lattice is not None:
|
||||
# o = damask.Orientation(rotation = o,lattice = options.lattice).reduced().rotation
|
||||
|
||||
|
||||
if 'rodrigues' in options.output:
|
||||
table = table.add('ro({})'.format(label),o.as_Rodrigues_vector(), scriptID+' '+' '.join(sys.argv[1:]))
|
||||
if 'eulers' in options.output:
|
||||
table = table.add('eu({})'.format(label),o.as_Euler_angles(options.degrees),scriptID+' '+' '.join(sys.argv[1:]))
|
||||
if 'quaternion' in options.output:
|
||||
table = table.add('qu({})'.format(label),o.as_quaternion(), scriptID+' '+' '.join(sys.argv[1:]))
|
||||
if 'matrix' in options.output:
|
||||
table = table.add('om({})'.format(label),o.as_matrix(), scriptID+' '+' '.join(sys.argv[1:]))
|
||||
if 'axisangle' in options.output:
|
||||
table = table.add('om({})'.format(label),o.as_axis_angle(options.degrees), scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
|
@ -14,84 +14,9 @@ scriptName = os.path.splitext(os.path.basename(__file__))[0]
|
|||
scriptID = ' '.join([scriptName,damask.version])
|
||||
|
||||
slipSystems = {
|
||||
'fcc':
|
||||
np.array([
|
||||
[+0,+1,-1 , +1,+1,+1],
|
||||
[-1,+0,+1 , +1,+1,+1],
|
||||
[+1,-1,+0 , +1,+1,+1],
|
||||
[+0,-1,-1 , -1,-1,+1],
|
||||
[+1,+0,+1 , -1,-1,+1],
|
||||
[-1,+1,+0 , -1,-1,+1],
|
||||
[+0,-1,+1 , +1,-1,-1],
|
||||
[-1,+0,-1 , +1,-1,-1],
|
||||
[+1,+1,+0 , +1,-1,-1],
|
||||
[+0,+1,+1 , -1,+1,-1],
|
||||
[+1,+0,-1 , -1,+1,-1],
|
||||
[-1,-1,+0 , -1,+1,-1],
|
||||
],'d'),
|
||||
'bcc':
|
||||
np.array([
|
||||
[+1,-1,+1 , +0,+1,+1],
|
||||
[-1,-1,+1 , +0,+1,+1],
|
||||
[+1,+1,+1 , +0,-1,+1],
|
||||
[-1,+1,+1 , +0,-1,+1],
|
||||
[-1,+1,+1 , +1,+0,+1],
|
||||
[-1,-1,+1 , +1,+0,+1],
|
||||
[+1,+1,+1 , -1,+0,+1],
|
||||
[+1,-1,+1 , -1,+0,+1],
|
||||
[-1,+1,+1 , +1,+1,+0],
|
||||
[-1,+1,-1 , +1,+1,+0],
|
||||
[+1,+1,+1 , -1,+1,+0],
|
||||
[+1,+1,-1 , -1,+1,+0],
|
||||
[-1,+1,+1 , +2,+1,+1],
|
||||
[+1,+1,+1 , -2,+1,+1],
|
||||
[+1,+1,-1 , +2,-1,+1],
|
||||
[+1,-1,+1 , +2,+1,-1],
|
||||
[+1,-1,+1 , +1,+2,+1],
|
||||
[+1,+1,-1 , -1,+2,+1],
|
||||
[+1,+1,+1 , +1,-2,+1],
|
||||
[-1,+1,+1 , +1,+2,-1],
|
||||
[+1,+1,-1 , +1,+1,+2],
|
||||
[+1,-1,+1 , -1,+1,+2],
|
||||
[-1,+1,+1 , +1,-1,+2],
|
||||
[+1,+1,+1 , +1,+1,-2],
|
||||
],'d'),
|
||||
'hex':
|
||||
np.array([
|
||||
[+2,-1,-1,+0 , +0,+0,+0,+1],
|
||||
[-1,+2,-1,+0 , +0,+0,+0,+1],
|
||||
[-1,-1,+2,+0 , +0,+0,+0,+1],
|
||||
[+2,-1,-1,+0 , +0,+1,-1,+0],
|
||||
[-1,+2,-1,+0 , -1,+0,+1,+0],
|
||||
[-1,-1,+2,+0 , +1,-1,+0,+0],
|
||||
[-1,+1,+0,+0 , +1,+1,-2,+0],
|
||||
[+0,-1,+1,+0 , -2,+1,+1,+0],
|
||||
[+1,+0,-1,+0 , +1,-2,+1,+0],
|
||||
[-1,+2,-1,+0 , +1,+0,-1,+1],
|
||||
[-2,+1,+1,+0 , +0,+1,-1,+1],
|
||||
[-1,-1,+2,+0 , -1,+1,+0,+1],
|
||||
[+1,-2,+1,+0 , -1,+0,+1,+1],
|
||||
[+2,-1,-1,+0 , +0,-1,+1,+1],
|
||||
[+1,+1,-2,+0 , +1,-1,+0,+1],
|
||||
[-2,+1,+1,+3 , +1,+0,-1,+1],
|
||||
[-1,-1,+2,+3 , +1,+0,-1,+1],
|
||||
[-1,-1,+2,+3 , +0,+1,-1,+1],
|
||||
[+1,-2,+1,+3 , +0,+1,-1,+1],
|
||||
[+1,-2,+1,+3 , -1,+1,+0,+1],
|
||||
[+2,-1,-1,+3 , -1,+1,+0,+1],
|
||||
[+2,-1,-1,+3 , -1,+0,+1,+1],
|
||||
[+1,+1,-2,+3 , -1,+0,+1,+1],
|
||||
[+1,+1,-2,+3 , +0,-1,+1,+1],
|
||||
[-1,+2,-1,+3 , +0,-1,+1,+1],
|
||||
[-1,+2,-1,+3 , +1,-1,+0,+1],
|
||||
[-2,+1,+1,+3 , +1,-1,+0,+1],
|
||||
[-1,-1,+2,+3 , +1,+1,-2,+2],
|
||||
[+1,-2,+1,+3 , -1,+2,-1,+2],
|
||||
[+2,-1,-1,+3 , -2,+1,+1,+2],
|
||||
[+1,+1,-2,+3 , -1,-1,+2,+2],
|
||||
[-1,+2,-1,+3 , +1,-2,+1,+2],
|
||||
[-2,+1,+1,+3 , +2,-1,-1,+2],
|
||||
],'d'),
|
||||
'fcc': damask.lattice.kinematics['cF']['slip'][:12],
|
||||
'bcc': damask.lattice.kinematics['cI']['slip'],
|
||||
'hex': damask.lattice.kinematics['hP']['slip'],
|
||||
}
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
@ -156,11 +81,11 @@ elif options.lattice == 'hex':
|
|||
# convert 4 Miller index notation of hex to orthogonal 3 Miller index notation
|
||||
for i in range(len(slip_direction)):
|
||||
slip_direction[i] = np.array([slipSystems['hex'][i,0]*1.5,
|
||||
(slipSystems['hex'][i,0] + 2.*slipSystems['hex'][i,1])*0.5*np.sqrt(3),
|
||||
(slipSystems['hex'][i,0] + 2.*slipSystems['hex'][i,1])*0.5*np.sqrt(3),
|
||||
slipSystems['hex'][i,3]*options.CoverA,
|
||||
])
|
||||
slip_normal[i] = np.array([slipSystems['hex'][i,4],
|
||||
(slipSystems['hex'][i,4] + 2.*slipSystems['hex'][i,5])/np.sqrt(3),
|
||||
(slipSystems['hex'][i,4] + 2.*slipSystems['hex'][i,5])/np.sqrt(3),
|
||||
slipSystems['hex'][i,7]/options.CoverA,
|
||||
])
|
||||
|
||||
|
@ -189,4 +114,4 @@ for name in filenames:
|
|||
for i,label in enumerate(labels):
|
||||
table = table.add(label,S[:,i],scriptID+' '+' '.join(sys.argv[1:]))
|
||||
|
||||
table.save((sys.stdout if name is None else name), legacy=True)
|
||||
table.save((sys.stdout if name is None else name))
|
||||
|
|
Loading…
Reference in New Issue