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DAMASK_EICMD
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using ordering as in DAMASK 

autogenerated by a small script from lattice.f90
This commit is contained in:
Martin Diehl 2020-05-21 15:42:05 +02:00
parent 23b1381eaf
commit 7aecc37219
1 changed files with 72 additions and 81 deletions
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153
processing/post/addSchmidfactors.py
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@ -15,91 +15,82 @@ scriptID = ' '.join([scriptName,damask.version])
slipSystems = { slipSystems = {
'fcc': 'fcc':
np.array([ np.array([
# Slip direction Plane normal [+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,-1,+0 , +1,+1,+1],
[ 1,-1, 0, 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,+1,+0 , -1,-1,+1],
[-1, 1, 0, -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,+1,+0 , +1,-1,-1],
[ 1, 1, 0, 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,-1,+0 , -1,+1,-1],
[-1,-1, 0, -1, 1,-1, ], ],'d'),
],'f'),
'bcc': 'bcc':
np.array([ np.array([
# Slip system <111>{110} [+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 , +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,+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,+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],
# Slip system <111>{112} [+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 , +2,+1,-1],
[ 1, 1,-1, 2,-1, 1, ], [+1,-1,+1 , +1,+2,+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,+2,-1],
[ 1, 1, 1, 1,-2, 1, ], [+1,+1,-1 , +1,+1,+2],
[-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,-2],
[-1, 1, 1, 1,-1, 2, ], ],'d'),
[ 1, 1, 1, 1, 1,-2, ],
],'f'),
'hex': 'hex':
np.array([ np.array([
# Basal systems <11.0>{00.1} (independent of c/a-ratio, Bravais notation (4 coordinate base)) [+2,-1,-1,+0 , +0,+0,+0,+1],
[ 2, -1, -1, 0, 0, 0, 0, 1, ], [-1,+2,-1,+0 , +0,+0,+0,+1],
[-1, 2, -1, 0, 0, 0, 0, 1, ], [-1,-1,+2,+0 , +0,+0,+0,+1],
[-1, -1, 2, 0, 0, 0, 0, 1, ], [+2,-1,-1,+0 , +0,+1,-1,+0],
# 1st type prismatic systems <11.0>{10.0} (independent of c/a-ratio) [-1,+2,-1,+0 , -1,+0,+1,+0],
[ 2, -1, -1, 0, 0, 1, -1, 0, ], [-1,-1,+2,+0 , +1,-1,+0,+0],
[-1, 2, -1, 0, -1, 0, 1, 0, ], [-1,+1,+0,+0 , +1,+1,-2,+0],
[-1, -1, 2, 0, 1, -1, 0, 0, ], [+0,-1,+1,+0 , -2,+1,+1,+0],
# 2nd type prismatic systems <10.0>{11.0} -- a slip; plane normals independent of c/a-ratio [+1,+0,-1,+0 , +1,-2,+1,+0],
[ 0, 1, -1, 0, 2, -1, -1, 0, ], [-1,+2,-1,+0 , +1,+0,-1,+1],
[-1, 0, 1, 0, -1, 2, -1, 0, ], [-2,+1,+1,+0 , +0,+1,-1,+1],
[ 1, -1, 0, 0, -1, -1, 2, 0, ], [-1,-1,+2,+0 , -1,+1,+0,+1],
# 1st type 1st order pyramidal systems <11.0>{-11.1} -- plane normals depend on the c/a-ratio [+1,-2,+1,+0 , -1,+0,+1,+1],
[ 2, -1, -1, 0, 0, 1, -1, 1, ], [+2,-1,-1,+0 , +0,-1,+1,+1],
[-1, 2, -1, 0, -1, 0, 1, 1, ], [+1,+1,-2,+0 , +1,-1,+0,+1],
[-1, -1, 2, 0, 1, -1, 0, 1, ], [-2,+1,+1,+3 , +1,+0,-1,+1],
[ 1, 1, -2, 0, -1, 1, 0, 1, ], [-1,-1,+2,+3 , +1,+0,-1,+1],
[-2, 1, 1, 0, 0, -1, 1, 1, ], [-1,-1,+2,+3 , +0,+1,-1,+1],
[ 1, -2, 1, 0, 1, 0, -1, 1, ], [+1,-2,+1,+3 , +0,+1,-1,+1],
# pyramidal system: c+a slip <11.3>{-10.1} -- plane normals depend on the c/a-ratio [+1,-2,+1,+3 , -1,+1,+0,+1],
[ 2, -1, -1, 3, -1, 1, 0, 1, ], [+2,-1,-1,+3 , -1,+1,+0,+1],
[ 1, -2, 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 , -1,+0,+1,+1],
[-2, 1, 1, 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 , +0,-1,+1,+1],
[ 1, 1, -2, 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,-1,+0,+1],
[-1, 2, -1, 3, 1, -1, 0, 1, ], [-1,-1,+2,+3 , +1,+1,-2,+2],
[ 1, 1, -2, 3, -1, 0, 1, 1, ], [+1,-2,+1,+3 , -1,+2,-1,+2],
[ 2, -1, -1, 3, -1, 0, 1, 1, ], [+2,-1,-1,+3 , -2,+1,+1,+2],
[ 1, -2, 1, 3, 0, 1, -1, 1, ], [+1,+1,-2,+3 , -1,-1,+2,+2],
[-1, -1, 2, 3, 0, 1, -1, 1, ], [-1,+2,-1,+3 , +1,-2,+1,+2],
# pyramidal system: c+a slip <11.3>{-1-1.2} -- as for hexagonal ice (Castelnau et al. 1996, similar to twin system found below) [-2,+1,+1,+3 , +2,-1,-1,+2],
[ 2, -1, -1, 3, -2, 1, 1, 2, ], # sorted according to similar twin system ],'d'),
[-1, 2, -1, 3, 1, -2, 1, 2, ], # <11.3>{-1-1.2} shear = 2((c/a)^2-2)/(3 c/a)
[-1, -1, 2, 3, 1, 1, -2, 2, ],
[-2, 1, 1, 3, 2, -1, -1, 2, ],
[ 1, -2, 1, 3, -1, 2, -1, 2, ],
[ 1, 1, -2, 3, -1, -1, 2, 2, ],
],'f'),
} }
# -------------------------------------------------------------------- # --------------------------------------------------------------------