last polishing on preprocessing scripts, documentation and scripts are all up to date.
added addSchmidfactors to post processing scripts
This commit is contained in:
Martin Diehl
parent
84c43741a6
commit
e635b06270
|
|
@ -0,0 +1,369 @@
|
|||
#!/usr/bin/python
|
||||
|
||||
import os,re,sys,math
|
||||
from optparse import OptionParser
|
||||
|
||||
CoverA=1.587
|
||||
slipnormal_temp = [ # This is the real slip system information for hex aka titanium for now.
|
||||
[0,0,0,1],
|
||||
[0,0,0,1],
|
||||
[0,0,0,1],
|
||||
[0,1,-1,0],
|
||||
[-1,0,1,0],
|
||||
[1,-1,0,0],
|
||||
[0,1,-1,1],
|
||||
[-1,1,0,1],
|
||||
[-1,0,1,1],
|
||||
[0,-1,1,1],
|
||||
[1,-1,0,1],
|
||||
[1,0,-1,1],
|
||||
[0,1,-1,1],
|
||||
[0,1,-1,1],
|
||||
[-1,1,0,1],
|
||||
[-1,1,0,1],
|
||||
[-1,0,1,1],
|
||||
[-1,0,1,1],
|
||||
[0,-1,1,1],
|
||||
[0,-1,1,1],
|
||||
[1,-1,0,1],
|
||||
[1,-1,0,1],
|
||||
[1,0,-1,1],
|
||||
[1,0,-1,1],
|
||||
]
|
||||
|
||||
slipdirection_temp = [
|
||||
[2,-1,-1,0],
|
||||
[-1,2,-1,0],
|
||||
[-1,-1,2,0],
|
||||
[2,-1,-1,0],
|
||||
[-1,2,-1,0],
|
||||
[-1,-1,2,0],
|
||||
[2,-1,-1,0],
|
||||
[1,1,-2,0],
|
||||
[-1,2,-1,0],
|
||||
[-2,1,1,0],
|
||||
[-1,-1,2,0],
|
||||
[1,-2,1,0],
|
||||
[-1,2,-1,3],
|
||||
[1,1,-2,3],
|
||||
[-2,1,1,3],
|
||||
[-1,2,-1,3],
|
||||
[-1,-1,2,3],
|
||||
[-2,1,1,3],
|
||||
[1,-2,1,3],
|
||||
[-1,-1,2,3],
|
||||
[2,-1,-1,3],
|
||||
[1,-2,1,3],
|
||||
[1,1,-2,3],
|
||||
[2,-1,-1,3],
|
||||
]
|
||||
|
||||
# slip normals and directions according to cpfem implementation
|
||||
Nslipsystems = {'fcc': 12, 'bcc': 24, 'hex': 24}
|
||||
slipnormal = { \
|
||||
'fcc': [
|
||||
[1,1,1],
|
||||
[1,1,1],
|
||||
[1,1,1],
|
||||
[-1,-1,1],
|
||||
[-1,-1,1],
|
||||
[-1,-1,1],
|
||||
[1,-1,-1],
|
||||
[1,-1,-1],
|
||||
[1,-1,-1],
|
||||
[-1,1,-1],
|
||||
[-1,1,-1],
|
||||
[-1,1,-1],
|
||||
],
|
||||
'bcc': [
|
||||
[0,1,1],
|
||||
[0,1,1],
|
||||
[0,-1,1],
|
||||
[0,-1,1],
|
||||
[1,0,1],
|
||||
[1,0,1],
|
||||
[-1,0,1],
|
||||
[-1,0,1],
|
||||
[1,1,0],
|
||||
[1,1,0],
|
||||
[-1,1,0],
|
||||
[-1,1,0],
|
||||
[2,1,1],
|
||||
[-2,1,1],
|
||||
[2,-1,1],
|
||||
[2,1,-1],
|
||||
[1,2,1],
|
||||
[-1,2,1],
|
||||
[1,-2,1],
|
||||
[1,2,-1],
|
||||
[1,1,2],
|
||||
[-1,1,2],
|
||||
[1,-1,2],
|
||||
[1,1,-2],
|
||||
],
|
||||
'hex': [ # these are dummy numbers and are recalculated based on the above hex real slip systems.
|
||||
[1,1,0],
|
||||
[1,1,0],
|
||||
[1,0,1],
|
||||
[1,0,1],
|
||||
[0,1,1],
|
||||
[0,1,1],
|
||||
[1,-1,0],
|
||||
[1,-1,0],
|
||||
[-1,0,1],
|
||||
[-1,0,1],
|
||||
[0,-1,1],
|
||||
[0,-1,1],
|
||||
[2,-1,1],
|
||||
[1,-2,-1],
|
||||
[1,1,2],
|
||||
[2,1,1],
|
||||
[1,2,-1],
|
||||
[1,-1,2],
|
||||
[2,1,-1],
|
||||
[1,2,1],
|
||||
[1,-1,-2],
|
||||
[2,-1,-1],
|
||||
[1,-2,1],
|
||||
[1,1,-2],
|
||||
],
|
||||
}
|
||||
slipdirection = { \
|
||||
'fcc': [
|
||||
[0,1,-1],
|
||||
[-1,0,1],
|
||||
[1,-1,0],
|
||||
[0,-1,-1],
|
||||
[1,0,1],
|
||||
[-1,1,0],
|
||||
[0,-1,1],
|
||||
[-1,0,-1],
|
||||
[1,1,0],
|
||||
[0,1,1],
|
||||
[1,0,-1],
|
||||
[-1,-1,0],
|
||||
],
|
||||
'bcc': [
|
||||
[1,-1,1],
|
||||
[-1,-1,1],
|
||||
[1,1,1],
|
||||
[-1,1,1],
|
||||
[-1,1,1],
|
||||
[-1,-1,1],
|
||||
[1,1,1],
|
||||
[1,-1,1],
|
||||
[-1,1,1],
|
||||
[-1,1,-1],
|
||||
[1,1,1],
|
||||
[1,1,-1],
|
||||
[-1,1,1],
|
||||
[1,1,1],
|
||||
[1,1,-1],
|
||||
[1,-1,1],
|
||||
[1,-1,1],
|
||||
[1,1,-1],
|
||||
[1,1,1],
|
||||
[-1,1,1],
|
||||
[1,1,-1],
|
||||
[1,-1,1],
|
||||
[-1,1,1],
|
||||
[1,1,1],
|
||||
],
|
||||
'hex': [ # these are dummy numbers and are recalculated based on the above hex real slip systems.
|
||||
[-1,1,1],
|
||||
[1,-1,1],
|
||||
[-1,-1,1],
|
||||
[-1,1,1],
|
||||
[-1,-1,1],
|
||||
[1,-1,1],
|
||||
[1,1,1],
|
||||
[-1,-1,1],
|
||||
[1,-1,1],
|
||||
[1,1,1],
|
||||
[1,1,1],
|
||||
[-1,1,1],
|
||||
[1,1,-1],
|
||||
[1,1,-1],
|
||||
[1,1,-1],
|
||||
[1,-1,-1],
|
||||
[1,-1,-1],
|
||||
[1,-1,-1],
|
||||
[1,-1,1],
|
||||
[1,-1,1],
|
||||
[1,-1,1],
|
||||
[1,1,1],
|
||||
[1,1,1],
|
||||
[1,1,1],
|
||||
],
|
||||
}
|
||||
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
def applyEulers(phi1,Phi,phi2,x):
|
||||
""" transform x given in crystal coordinates to xbar returned in lab coordinates for Euler angles phi1,Phi,phi2 """
|
||||
|
||||
eulerRot = [[ math.cos(phi1)*math.cos(phi2) - math.cos(Phi)*math.sin(phi1)*math.sin(phi2), - math.cos(phi1)*math.sin(phi2) - math.cos(Phi)*math.cos(phi2)*math.sin(phi1), math.sin(Phi)*math.sin(phi1)], \
|
||||
[ math.cos(phi2)*math.sin(phi1) + math.cos(Phi)*math.cos(phi1)*math.sin(phi2), math.cos(Phi)*math.cos(phi1)*math.cos(phi2) - math.sin(phi1)*math.sin(phi2), -math.sin(Phi)*math.cos(phi1)], \
|
||||
[ math.sin(Phi)*math.sin(phi2), math.sin(Phi)*math.cos(phi2), math.cos(Phi)]]
|
||||
|
||||
xbar = [0,0,0]
|
||||
if len(x) == 3:
|
||||
for i in range(3):
|
||||
xbar[i] = sum([eulerRot[i][j]*x[j] for j in range(3)])
|
||||
return xbar
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
def normalize(x):
|
||||
|
||||
norm = math.sqrt(sum([x[i]*x[i] for i in range(len(x))]))
|
||||
|
||||
return [x[i]/norm for i in range(len(x))]
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
def crossproduct(x,y):
|
||||
|
||||
return [
|
||||
x[1]*y[2]-y[1]*x[2],
|
||||
x[2]*y[0]-y[2]*x[0],
|
||||
x[0]*y[1]-y[0]*x[1],
|
||||
]
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
|
||||
|
||||
|
||||
# --------------------------------------------------------------------
|
||||
# MAIN
|
||||
# --------------------------------------------------------------------
|
||||
parser = OptionParser(usage='%prog [options] [file]', description = """
|
||||
Add columns listing Schmid factors (and optional trace vector of selected system) for given Euler angles.
|
||||
Column headings need to have names 'phi1', 'Phi', 'phi2'.
|
||||
|
||||
$Id$
|
||||
""")
|
||||
|
||||
parser.add_option('-l','--lattice', dest='lattice', choices=('fcc','bcc','hex'), \
|
||||
help='key for lattice type [%default]')
|
||||
parser.add_option('-d','--forcedirection', dest='forcedirection', type='int', nargs=3, \
|
||||
help='force direction in lab coordinates [%default]')
|
||||
parser.add_option('-n','--stressnormal', dest='stressnormal', type='int', nargs=3, \
|
||||
help='stress plane normal in lab coordinates [%default]')
|
||||
parser.add_option('-t','--trace', dest='traceplane', type='int', nargs=3, \
|
||||
help="normal (in lab coordinates) of plane on which the plane trace of the Schmid factor(s) is reported [%default]")
|
||||
parser.add_option('-r','--rank', dest='rank', type='int', \
|
||||
help="report trace of r'th highest Schmid factor [%default]")
|
||||
parser.set_defaults(lattice = 'fcc')
|
||||
parser.set_defaults(forcedirection = [0, 0, 1])
|
||||
parser.set_defaults(stressnormal = None)
|
||||
parser.set_defaults(traceplane = None)
|
||||
parser.set_defaults(rank = 0)
|
||||
|
||||
(options,filename) = parser.parse_args()
|
||||
|
||||
options.forcedirection = normalize(options.forcedirection)
|
||||
if options.stressnormal:
|
||||
if abs(sum([options.forcedirection[i] * options.stressnormal[i] for i in range(3)])) < 1e-3:
|
||||
options.stressnormal = normalize(options.stressnormal)
|
||||
else:
|
||||
parser.error('stress plane normal not orthogonal to force direction')
|
||||
else:
|
||||
options.stressnormal = options.forcedirection
|
||||
if options.traceplane:
|
||||
options.traceplane = normalize(options.traceplane)
|
||||
options.rank = min(options.rank,Nslipsystems[options.lattice])
|
||||
|
||||
# read from standard input unless input file specified
|
||||
if filename == []:
|
||||
file = sys.stdin
|
||||
elif os.path.exists(filename[0]):
|
||||
file = open(filename[0])
|
||||
|
||||
# read data
|
||||
content = file.readlines()
|
||||
file.close()
|
||||
|
||||
# get labels by either read the first row, or - if keyword header is present - the last line of the header
|
||||
headerlines = 1
|
||||
m = re.search('(\d+)\s*head', content[0].lower())
|
||||
if m:
|
||||
headerlines = int(m.group(1))+1
|
||||
labels = content[headerlines-1].split()
|
||||
data = content[headerlines:]
|
||||
|
||||
# Convert 4 Miller indices notation of hex to orthogonal 3 Miller indices notation
|
||||
if options.lattice=="hex":
|
||||
for i in range(Nslipsystems[options.lattice]):
|
||||
slipnormal[options.lattice][i][0]=slipnormal_temp[i][0]
|
||||
slipnormal[options.lattice][i][1]=(slipnormal_temp[i][0]+2.0*slipnormal_temp[i][1])/math.sqrt(3.0)
|
||||
slipnormal[options.lattice][i][2]=slipnormal_temp[i][3]/CoverA
|
||||
slipdirection[options.lattice][i][0]=slipdirection_temp[i][0]*1.5 # direction [uvtw]->[3u/2 (u+2v)*sqrt(3)/2 w*(c/a)] ,
|
||||
slipdirection[options.lattice][i][1]=(slipdirection_temp[i][0]+2.0*slipdirection_temp[i][1])*(0.5*math.sqrt(3.0))
|
||||
slipdirection[options.lattice][i][2]=slipdirection_temp[i][3]*CoverA
|
||||
|
||||
for i in range(Nslipsystems[options.lattice]):
|
||||
slipnormal[options.lattice][i]=normalize(slipnormal[options.lattice][i])
|
||||
slipdirection[options.lattice][i]=normalize(slipdirection[options.lattice][i])
|
||||
|
||||
for c in range(len(labels)):
|
||||
m = re.search('.*([Pp]hi\d*).*', labels[c])
|
||||
if m:
|
||||
if m.group(1).lower() == "phi1":
|
||||
phi1Column = c
|
||||
elif m.group(1).lower() == "phi":
|
||||
PhiColumn = c
|
||||
elif m.group(1).lower() == "phi2":
|
||||
phi2Column = c
|
||||
|
||||
output = '1\theader\n' + \
|
||||
'\t'.join(map(str,labels)) + \
|
||||
'\t' + \
|
||||
'\t'.join(['(%i)S(%i %i %i)[%i %i %i]'%(i+1,
|
||||
slipnormal[options.lattice][i][0],
|
||||
slipnormal[options.lattice][i][1],
|
||||
slipnormal[options.lattice][i][2],
|
||||
slipdirection[options.lattice][i][0],
|
||||
slipdirection[options.lattice][i][1],
|
||||
slipdirection[options.lattice][i][2],
|
||||
) for i in range(Nslipsystems[options.lattice])])
|
||||
if options.traceplane:
|
||||
if options.rank > 0:
|
||||
output += '\ttrace_x\ttrace_y\ttrace_z\tsystem'
|
||||
else:
|
||||
output += '\t' + '\t'.join(['(%i)tx\tty\ttz'%(i+1) for i in range(Nslipsystems[options.lattice])])
|
||||
output += '\n'
|
||||
|
||||
for line in data:
|
||||
items = line.split()[:len(labels)]
|
||||
if items == []:
|
||||
continue
|
||||
phi1 = math.radians(float(items[phi1Column]))
|
||||
Phi = math.radians(float(items[PhiColumn]))
|
||||
phi2 = math.radians(float(items[phi2Column]))
|
||||
S = [ sum( [applyEulers(phi1,Phi,phi2,normalize( slipnormal[options.lattice][slipsystem]))[i]*options.stressnormal[i] for i in range(3)] ) * \
|
||||
sum( [applyEulers(phi1,Phi,phi2,normalize(slipdirection[options.lattice][slipsystem]))[i]*options.forcedirection[i] for i in range(3)] ) \
|
||||
for slipsystem in range(Nslipsystems[options.lattice]) ]
|
||||
output += '\t'.join(items + map(str,S))
|
||||
if options.traceplane:
|
||||
trace = [crossproduct(options.traceplane,applyEulers(phi1,Phi,phi2,normalize(slipnormal[options.lattice][slipsystem]))) \
|
||||
for slipsystem in range(Nslipsystems[options.lattice]) ]
|
||||
if options.rank == 0:
|
||||
output += '\t' + '\t'.join(map(lambda x:'%f\t%f\t%f'%(x[0],x[1],x[2]),trace))
|
||||
elif options.rank > 0:
|
||||
SabsSorted = sorted([(abs(S[i]),i) for i in range(len(S))])
|
||||
output += '\t' + '\t'.join(map(str,trace[SabsSorted[-options.rank][1]])) + '\t%i'%(1+SabsSorted[-options.rank][1])
|
||||
# for t in [normalize(crossproduct(options.traceplane,applyEulers(phi1,Phi,phi2,normalize(slipnormal[options.lattice][i])))) for i in range(12,24)]:
|
||||
# print '\t'.join(map(str,t))
|
||||
# print '\t'.join(map(lambda x: str(-x),t))
|
||||
# print '\t'.join(['0','0','0'])
|
||||
# print
|
||||
output += '\n'
|
||||
|
||||
if filename == []:
|
||||
print output
|
||||
else:
|
||||
file = open(filename[0],'w')
|
||||
file.write(output)
|
||||
file.close()
|
||||
|
|
@ -46,9 +46,9 @@ Changes the (three-dimensional) canvas of a spectral geometry description.
|
|||
parser.add_option('-g', '--grid', dest='grid', type='int', nargs = 3, \
|
||||
help='a,b,c grid of hexahedral box [unchanged]')
|
||||
parser.add_option('-o', '--offset', dest='offset', type='int', nargs = 3, \
|
||||
help='x,y,z offset from old to new origin of grid %default')
|
||||
help='a,b,c offset from old to new origin of grid %default')
|
||||
parser.add_option('-f', '--fill', dest='fill', type='int', \
|
||||
help='(background) canvas grain index [autodetect]')
|
||||
help='(background) canvas grain index. "0" selects maximum microstructure index + 1 [%default]')
|
||||
parser.add_option('-2', '--twodimensional', dest='twoD', action='store_true', \
|
||||
help='output geom file with two-dimensional data arrangement [%default]')
|
||||
|
||||
|
|
|
|||
|
|
@ -117,7 +117,7 @@ boundaries, triple lines, and quadruple points.
|
|||
|
||||
parser.add_option('-t','--type', dest='type', action='extend', type='string', \
|
||||
help='feature type (%s)'%(', '.join(map(lambda x:', '.join(x['names']),features))))
|
||||
parser.add_option('-n','--neighborhood', dest='neigborhood', action='store', type='string', \
|
||||
parser.add_option('-n','--neighborhood', dest='neigborhood', choices=neighborhoods.keys(), \
|
||||
help='type of neighborhood (%s) [neumann]'%(', '.join(neighborhoods.keys())))
|
||||
parser.add_option('-2', '--twodimensional', dest='twoD', action='store_true', \
|
||||
help='output geom file with two-dimensional data arrangement [%default]')
|
||||
|
|
@ -128,9 +128,6 @@ parser.set_defaults(twoD = False)
|
|||
|
||||
(options,filenames) = parser.parse_args()
|
||||
|
||||
options.neighborhood = options.neighborhood.lower()
|
||||
if options.neighborhood not in neighborhoods:
|
||||
parser.error('unknown neighborhood %s!'%options.neighborhood)
|
||||
|
||||
feature_list = []
|
||||
for i,feature in enumerate(features):
|
||||
|
|
|
|||
|
|
@ -40,8 +40,8 @@ Generate a geometry file of a bicontinuous structure of given type.
|
|||
""" + string.replace('$Id$','\n','\\n')
|
||||
)
|
||||
|
||||
parser.add_option('-t','--type', dest='type', type='string', \
|
||||
help='type of minimal surface (%s)'%(','.join(minimal_surfaces)))
|
||||
parser.add_option('-t','--type', dest='type', choices=minimal_surfaces, \
|
||||
help='type of minimal surface (%s) [primitive]' %(','.join(minimal_surfaces)))
|
||||
parser.add_option('-f','--threshold', dest='threshold', type='float', \
|
||||
help='threshold value defining minimal surface [%default]')
|
||||
parser.add_option('-g', '--grid', dest='grid', type='int', nargs=3, \
|
||||
|
|
@ -51,7 +51,7 @@ parser.add_option('-s', '--size', dest='size', type='float', nargs=3, \
|
|||
parser.add_option('-p', '--periods', dest='periods', type='int', \
|
||||
help='number of repetitions of unit cell [%default]')
|
||||
parser.add_option('--homogenization', dest='homogenization', type='int', \
|
||||
help='homogenization index to be used [%defaults]')
|
||||
help='homogenization index to be used [%default]')
|
||||
parser.add_option('--m', dest='microstructure', type='int', nargs = 2, \
|
||||
help='two microstructure indices to be used %default')
|
||||
parser.add_option('-2', '--twodimensional', dest='twoD', action='store_true', \
|
||||
|
|
|
|||
|
|
@ -40,7 +40,7 @@ Generate geometry description and material configuration by standard Voronoi tes
|
|||
)
|
||||
|
||||
parser.add_option('-g', '--grid', dest='grid', type='int', nargs = 3, \
|
||||
help='a,b,c grid of hexahedral box [from seed file]')
|
||||
help='a,b,c grid of hexahedral box [from seeds file]')
|
||||
parser.add_option('-s', '--size', dest='size', type='float', nargs = 3, \
|
||||
help='x,y,z size of hexahedral box [1.0 along largest grid point number]')
|
||||
parser.add_option('--homogenization', dest='homogenization', type='int', \
|
||||
|
|
|
|||
|
|
@ -48,7 +48,8 @@ i.e. within the region close to a grain/phase boundary.
|
|||
parser.add_option('-v', '--vicinity', dest='vicinity', type='int', \
|
||||
help='voxel distance checked for presence of other microstructure [%default]')
|
||||
parser.add_option('-m', '--microstructureoffset', dest='offset', type='int', \
|
||||
help='integer offset for tagged microstructure [autodetect]')
|
||||
help='offset (positive or negative) for tagged microstructure. '+
|
||||
'"0" selects maximum microstructure index [%default]')
|
||||
parser.add_option('-2', '--twodimensional', dest='twoD', action='store_true', \
|
||||
help='output geom file with two-dimensional data arrangement')
|
||||
|
||||
|
|
|
|||
|
|
@ -792,7 +792,7 @@ parser.add_option("-o", "--output", action='extend', dest='output', type='string
|
|||
help="types of output [image, mentat, procedure, spectral]")
|
||||
parser.add_option("-p", "--port", type="int",\
|
||||
dest="port",\
|
||||
help="Mentat connection port")
|
||||
help="Mentat connection port [%default]")
|
||||
parser.add_option("-2", "--twodimensional", action="store_true",\
|
||||
dest="twoD",\
|
||||
help="twodimensional model [%default]")
|
||||
|
|
@ -804,16 +804,16 @@ parser.add_option("-e", "--strain", type="float",\
|
|||
help="final strain to reach in simulation [%default]")
|
||||
parser.add_option("--rate", type="float",\
|
||||
dest="strainrate",\
|
||||
help="(engineering) strain rate to simulate")
|
||||
help="(engineering) strain rate to simulate [%default]")
|
||||
parser.add_option("-N", "--increments", type="int",\
|
||||
dest="increments",\
|
||||
help="number of increments to take")
|
||||
help="number of increments to take [%default]")
|
||||
parser.add_option("-t", "--tolerance", type="float",\
|
||||
dest="tolerance",\
|
||||
help="relative tolerance of pixel positions to be swept")
|
||||
help="relative tolerance of pixel positions to be swept [%default]")
|
||||
parser.add_option("-m", "--mesh", choices=['dt_planar_trimesh','af_planar_trimesh','af_planar_quadmesh'],\
|
||||
dest="mesh",\
|
||||
help="algorithm and element type for automeshing [%default]")
|
||||
help="algorithm and element type for automeshing (dt_planar_trimesh, af_planar_trimesh, af_planar_quadmesh) [%default]")
|
||||
parser.add_option("-x", "--xmargin", type="float",\
|
||||
dest="xmargin",\
|
||||
help="margin in x in units of patch size [%default]")
|
||||
|
|
@ -828,22 +828,23 @@ parser.add_option("-z", "--extrusion", type="int",\
|
|||
help="number of repetitions in z-direction [%default]")
|
||||
parser.add_option("-i", "--imagesize", type="int",\
|
||||
dest="imgsize",\
|
||||
help="size of PNG image")
|
||||
help="size of PNG image [%default]")
|
||||
parser.add_option("-M", "--coordtransformation", type="float", nargs=4, \
|
||||
dest="M",\
|
||||
help="2x2 transformation from rcb to Euler coords ( = M . [x_rcb,y_rcb])")
|
||||
help="2x2 transformation from rcb to Euler coords [%default]")
|
||||
parser.add_option("--scatter", type="float",\
|
||||
dest="scatter",\
|
||||
help="orientation scatter [%default]")
|
||||
help="orientation scatter %default")
|
||||
|
||||
parser.set_defaults(output = [])
|
||||
parser.set_defaults(size = 1.0)
|
||||
parser.set_defaults(port = 40007)
|
||||
parser.set_defaults(xmargin = 0.0)
|
||||
parser.set_defaults(ymargin = 0.0)
|
||||
parser.set_defaults(resolution = 64)
|
||||
parser.set_defaults(extrusion = 2)
|
||||
parser.set_defaults(imgsize = 512)
|
||||
parser.set_defaults(M = [0.0,1.0,1.0,0]) # M_11, M_12, M_21, M_22. x,y in RCB is y,x of Eulers!!
|
||||
parser.set_defaults(M = [0.0,1.0,1.0,0.0]) # M_11, M_12, M_21, M_22. x,y in RCB is y,x of Eulers!!
|
||||
parser.set_defaults(tolerance = 1.0e-3)
|
||||
parser.set_defaults(scatter = 0.0)
|
||||
parser.set_defaults(strain = 0.2)
|
||||
|
|
|
|||
|
|
@ -35,7 +35,7 @@ mappings = {
|
|||
|
||||
|
||||
parser = OptionParser(option_class=extendedOption, usage='%prog [options]', description = """
|
||||
Distribute given number of points randomly within the three-dimensional cube [0,0,0]--[1,1,1].
|
||||
Distribute given number of points randomly within the three-dimensional cube [0.0,0.0,0.0]--[1.0,1.0,1.0].
|
||||
Reports positions with random crystal orientations in seeds file format to STDOUT.
|
||||
""" + string.replace('$Id$','\n','\\n')
|
||||
)
|
||||
|
|
|
|||
|
|
@ -47,6 +47,7 @@ bin_link = { \
|
|||
'addMises.py',
|
||||
'addNorm.py',
|
||||
'addPK2.py',
|
||||
'addSchmidfactors.py',
|
||||
'addSpectralDecomposition.py',
|
||||
'addStrainTensors.py',
|
||||
'averageDown.py',
|
||||
|
|
|
|||
Loading…
Reference in New Issue