2014-04-02 00:11:14 +05:30
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#!/usr/bin/env python
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# -*- coding: UTF-8 no BOM -*-
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2013-06-04 18:26:57 +05:30
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import os,re,sys,math
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from optparse import OptionParser
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CoverA=1.587
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slipnormal_temp = [ # This is the real slip system information for hex aka titanium for now.
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[0,0,0,1],
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[0,0,0,1],
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[0,0,0,1],
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[0,1,-1,0],
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[-1,0,1,0],
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[1,-1,0,0],
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[0,1,-1,1],
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[-1,1,0,1],
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[-1,0,1,1],
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[0,-1,1,1],
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[1,-1,0,1],
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[1,0,-1,1],
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[0,1,-1,1],
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[0,1,-1,1],
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[-1,1,0,1],
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[-1,1,0,1],
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[-1,0,1,1],
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[-1,0,1,1],
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[0,-1,1,1],
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[0,-1,1,1],
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[1,-1,0,1],
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[1,-1,0,1],
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[1,0,-1,1],
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[1,0,-1,1],
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]
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slipdirection_temp = [
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[2,-1,-1,0],
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[-1,2,-1,0],
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[-1,-1,2,0],
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[2,-1,-1,0],
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[-1,2,-1,0],
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[-1,-1,2,0],
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[2,-1,-1,0],
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[1,1,-2,0],
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[-1,2,-1,0],
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[-2,1,1,0],
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[-1,-1,2,0],
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[1,-2,1,0],
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[-1,2,-1,3],
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[1,1,-2,3],
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[-2,1,1,3],
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[-1,2,-1,3],
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[-1,-1,2,3],
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[-2,1,1,3],
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[1,-2,1,3],
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[-1,-1,2,3],
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[2,-1,-1,3],
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[1,-2,1,3],
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[1,1,-2,3],
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[2,-1,-1,3],
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]
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# slip normals and directions according to cpfem implementation
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Nslipsystems = {'fcc': 12, 'bcc': 24, 'hex': 24}
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slipnormal = { \
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'fcc': [
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[1,1,1],
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[1,1,1],
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[1,1,1],
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[-1,-1,1],
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[-1,-1,1],
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[-1,-1,1],
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[1,-1,-1],
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[1,-1,-1],
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[1,-1,-1],
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[-1,1,-1],
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[-1,1,-1],
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[-1,1,-1],
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],
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'bcc': [
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[0,1,1],
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[0,1,1],
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[0,-1,1],
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[0,-1,1],
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[1,0,1],
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[1,0,1],
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[-1,0,1],
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[-1,0,1],
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[1,1,0],
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[1,1,0],
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[-1,1,0],
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[-1,1,0],
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[2,1,1],
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[-2,1,1],
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[2,-1,1],
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[2,1,-1],
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[1,2,1],
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[-1,2,1],
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[1,-2,1],
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[1,2,-1],
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[1,1,2],
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[-1,1,2],
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[1,-1,2],
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[1,1,-2],
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],
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'hex': [ # these are dummy numbers and are recalculated based on the above hex real slip systems.
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[1,1,0],
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[1,1,0],
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[1,0,1],
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[1,0,1],
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[0,1,1],
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[0,1,1],
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[1,-1,0],
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[1,-1,0],
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[-1,0,1],
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[-1,0,1],
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[0,-1,1],
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[0,-1,1],
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[2,-1,1],
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[1,-2,-1],
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[1,1,2],
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[2,1,1],
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[1,2,-1],
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[1,-1,2],
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[2,1,-1],
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[1,2,1],
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[1,-1,-2],
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[2,-1,-1],
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[1,-2,1],
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[1,1,-2],
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],
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}
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slipdirection = { \
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'fcc': [
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[0,1,-1],
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[-1,0,1],
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[1,-1,0],
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[0,-1,-1],
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[1,0,1],
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[-1,1,0],
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[0,-1,1],
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[-1,0,-1],
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[1,1,0],
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[0,1,1],
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[1,0,-1],
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[-1,-1,0],
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],
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'bcc': [
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[1,-1,1],
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[-1,-1,1],
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[1,1,1],
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[-1,1,1],
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[-1,1,1],
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[-1,-1,1],
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[1,1,1],
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[1,-1,1],
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[-1,1,1],
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[-1,1,-1],
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[1,1,1],
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[1,1,-1],
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[-1,1,1],
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[1,1,1],
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[1,1,-1],
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[1,-1,1],
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[1,-1,1],
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[1,1,-1],
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[1,1,1],
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[-1,1,1],
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[1,1,-1],
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[1,-1,1],
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[-1,1,1],
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[1,1,1],
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],
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'hex': [ # these are dummy numbers and are recalculated based on the above hex real slip systems.
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[-1,1,1],
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[1,-1,1],
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[-1,-1,1],
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[-1,1,1],
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[-1,-1,1],
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[1,-1,1],
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[1,1,1],
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[-1,-1,1],
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[1,-1,1],
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[1,1,1],
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[1,1,1],
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[-1,1,1],
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[1,1,-1],
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[1,1,-1],
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[1,1,-1],
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[1,-1,-1],
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[1,-1,-1],
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[1,-1,-1],
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[1,-1,1],
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[1,-1,1],
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[1,-1,1],
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[1,1,1],
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[1,1,1],
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[1,1,1],
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],
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}
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# --------------------------------------------------------------------
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def applyEulers(phi1,Phi,phi2,x):
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""" transform x given in crystal coordinates to xbar returned in lab coordinates for Euler angles phi1,Phi,phi2 """
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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)], \
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[ 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)], \
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[ math.sin(Phi)*math.sin(phi2), math.sin(Phi)*math.cos(phi2), math.cos(Phi)]]
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xbar = [0,0,0]
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if len(x) == 3:
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for i in range(3):
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xbar[i] = sum([eulerRot[i][j]*x[j] for j in range(3)])
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return xbar
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# --------------------------------------------------------------------
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def normalize(x):
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norm = math.sqrt(sum([x[i]*x[i] for i in range(len(x))]))
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return [x[i]/norm for i in range(len(x))]
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# --------------------------------------------------------------------
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def crossproduct(x,y):
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return [
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x[1]*y[2]-y[1]*x[2],
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x[2]*y[0]-y[2]*x[0],
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x[0]*y[1]-y[0]*x[1],
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]
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# --------------------------------------------------------------------
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# --------------------------------------------------------------------
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# MAIN
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# --------------------------------------------------------------------
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parser = OptionParser(usage='%prog [options] [file]', description = """
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Add columns listing Schmid factors (and optional trace vector of selected system) for given Euler angles.
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Column headings need to have names 'phi1', 'Phi', 'phi2'.
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$Id$
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""")
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parser.add_option('-l','--lattice', dest='lattice', choices=('fcc','bcc','hex'), \
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help='key for lattice type [%default]')
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parser.add_option('-d','--forcedirection', dest='forcedirection', type='int', nargs=3, \
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help='force direction in lab coordinates [%default]')
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parser.add_option('-n','--stressnormal', dest='stressnormal', type='int', nargs=3, \
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help='stress plane normal in lab coordinates [%default]')
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parser.add_option('-t','--trace', dest='traceplane', type='int', nargs=3, \
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help="normal (in lab coordinates) of plane on which the plane trace of the Schmid factor(s) is reported [%default]")
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parser.add_option('-r','--rank', dest='rank', type='int', \
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help="report trace of r'th highest Schmid factor [%default]")
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parser.set_defaults(lattice = 'fcc')
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parser.set_defaults(forcedirection = [0, 0, 1])
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parser.set_defaults(stressnormal = None)
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parser.set_defaults(traceplane = None)
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parser.set_defaults(rank = 0)
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(options,filename) = parser.parse_args()
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options.forcedirection = normalize(options.forcedirection)
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if options.stressnormal:
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if abs(sum([options.forcedirection[i] * options.stressnormal[i] for i in range(3)])) < 1e-3:
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options.stressnormal = normalize(options.stressnormal)
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else:
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parser.error('stress plane normal not orthogonal to force direction')
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else:
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options.stressnormal = options.forcedirection
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if options.traceplane:
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options.traceplane = normalize(options.traceplane)
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options.rank = min(options.rank,Nslipsystems[options.lattice])
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# read from standard input unless input file specified
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if filename == []:
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file = sys.stdin
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elif os.path.exists(filename[0]):
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file = open(filename[0])
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# read data
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content = file.readlines()
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file.close()
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# get labels by either read the first row, or - if keyword header is present - the last line of the header
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headerlines = 1
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m = re.search('(\d+)\s*head', content[0].lower())
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if m:
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headerlines = int(m.group(1))+1
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labels = content[headerlines-1].split()
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data = content[headerlines:]
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# Convert 4 Miller indices notation of hex to orthogonal 3 Miller indices notation
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if options.lattice=="hex":
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for i in range(Nslipsystems[options.lattice]):
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slipnormal[options.lattice][i][0]=slipnormal_temp[i][0]
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slipnormal[options.lattice][i][1]=(slipnormal_temp[i][0]+2.0*slipnormal_temp[i][1])/math.sqrt(3.0)
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slipnormal[options.lattice][i][2]=slipnormal_temp[i][3]/CoverA
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slipdirection[options.lattice][i][0]=slipdirection_temp[i][0]*1.5 # direction [uvtw]->[3u/2 (u+2v)*sqrt(3)/2 w*(c/a)] ,
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slipdirection[options.lattice][i][1]=(slipdirection_temp[i][0]+2.0*slipdirection_temp[i][1])*(0.5*math.sqrt(3.0))
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slipdirection[options.lattice][i][2]=slipdirection_temp[i][3]*CoverA
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for i in range(Nslipsystems[options.lattice]):
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slipnormal[options.lattice][i]=normalize(slipnormal[options.lattice][i])
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slipdirection[options.lattice][i]=normalize(slipdirection[options.lattice][i])
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for c in range(len(labels)):
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m = re.search('.*([Pp]hi\d*).*', labels[c])
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if m:
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if m.group(1).lower() == "phi1":
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phi1Column = c
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elif m.group(1).lower() == "phi":
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PhiColumn = c
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elif m.group(1).lower() == "phi2":
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phi2Column = c
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output = '1\theader\n' + \
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'\t'.join(map(str,labels)) + \
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'\t' + \
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'\t'.join(['(%i)S(%i %i %i)[%i %i %i]'%(i+1,
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slipnormal[options.lattice][i][0],
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slipnormal[options.lattice][i][1],
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slipnormal[options.lattice][i][2],
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slipdirection[options.lattice][i][0],
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slipdirection[options.lattice][i][1],
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slipdirection[options.lattice][i][2],
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) for i in range(Nslipsystems[options.lattice])])
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if options.traceplane:
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if options.rank > 0:
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output += '\ttrace_x\ttrace_y\ttrace_z\tsystem'
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else:
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output += '\t' + '\t'.join(['(%i)tx\tty\ttz'%(i+1) for i in range(Nslipsystems[options.lattice])])
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output += '\n'
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for line in data:
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items = line.split()[:len(labels)]
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if items == []:
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continue
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phi1 = math.radians(float(items[phi1Column]))
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Phi = math.radians(float(items[PhiColumn]))
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phi2 = math.radians(float(items[phi2Column]))
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S = [ sum( [applyEulers(phi1,Phi,phi2,normalize( slipnormal[options.lattice][slipsystem]))[i]*options.stressnormal[i] for i in range(3)] ) * \
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sum( [applyEulers(phi1,Phi,phi2,normalize(slipdirection[options.lattice][slipsystem]))[i]*options.forcedirection[i] for i in range(3)] ) \
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for slipsystem in range(Nslipsystems[options.lattice]) ]
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output += '\t'.join(items + map(str,S))
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if options.traceplane:
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trace = [crossproduct(options.traceplane,applyEulers(phi1,Phi,phi2,normalize(slipnormal[options.lattice][slipsystem]))) \
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for slipsystem in range(Nslipsystems[options.lattice]) ]
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if options.rank == 0:
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output += '\t' + '\t'.join(map(lambda x:'%f\t%f\t%f'%(x[0],x[1],x[2]),trace))
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elif options.rank > 0:
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SabsSorted = sorted([(abs(S[i]),i) for i in range(len(S))])
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output += '\t' + '\t'.join(map(str,trace[SabsSorted[-options.rank][1]])) + '\t%i'%(1+SabsSorted[-options.rank][1])
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# for t in [normalize(crossproduct(options.traceplane,applyEulers(phi1,Phi,phi2,normalize(slipnormal[options.lattice][i])))) for i in range(12,24)]:
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# print '\t'.join(map(str,t))
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# print '\t'.join(map(lambda x: str(-x),t))
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# print '\t'.join(['0','0','0'])
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# print
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output += '\n'
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if filename == []:
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print output
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else:
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file = open(filename[0],'w')
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file.write(output)
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file.close()
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