phase depends on constituent, not integration point
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@ -954,7 +954,7 @@ subroutine crystallite_init
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do e = FEsolving_execElem(1),FEsolving_execElem(2)
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do i = FEsolving_execIP(1), FEsolving_execIP(2); do c = 1, homogenization_Nconstituents(material_homogenizationAt(e))
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p = material_phaseAt(i,e)
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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crystallite_Fp0(1:3,1:3,c,i,e) = material_orientation0(c,i,e)%asMatrix() ! Fp reflects initial orientation (see 10.1016/j.actamat.2006.01.005)
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crystallite_Fp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e) &
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@ -1031,7 +1031,7 @@ function crystallite_stress()
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elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2)
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do i = FEsolving_execIP(1),FEsolving_execIP(2); do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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homogenizationRequestsCalculation: if (crystallite_requested(c,i,e)) then
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p = material_phaseAt(i,e)
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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plasticState (material_phaseAt(c,e))%subState0( :,material_phaseMemberAt(c,i,e)) = &
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plasticState (material_phaseAt(c,e))%partitionedState0(:,material_phaseMemberAt(c,i,e))
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@ -1064,7 +1064,7 @@ function crystallite_stress()
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elementLooping3: do e = FEsolving_execElem(1),FEsolving_execElem(2)
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do i = FEsolving_execIP(1),FEsolving_execIP(2)
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do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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p = material_phaseAt(i,e)
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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!--------------------------------------------------------------------------------------------------
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! wind forward
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@ -1161,9 +1161,9 @@ subroutine crystallite_initializeRestorationPoints(i,e)
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c, & !< constituent number
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s,p, m
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p = material_phaseAt(i,e)
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do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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m = material_phaseMemberAt(c,i,e)
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e)
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crystallite_partitionedLp0(1:3,1:3,c,i,e) = crystallite_Lp0(1:3,1:3,c,i,e)
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constitutive_mech_partionedFi0(p)%data(1:3,1:3,m) = constitutive_mech_Fi0(p)%data(1:3,1:3,m)
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@ -1193,9 +1193,9 @@ subroutine crystallite_windForward(i,e)
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integer :: &
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c, & !< constituent number
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s, p, m
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p = material_phaseAt(i,e)
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do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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m = material_phaseMemberAt(c,i,e)
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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crystallite_partitionedF0 (1:3,1:3,c,i,e) = crystallite_partitionedF(1:3,1:3,c,i,e)
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crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp (1:3,1:3,c,i,e)
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crystallite_partitionedLp0(1:3,1:3,c,i,e) = crystallite_Lp (1:3,1:3,c,i,e)
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@ -1226,13 +1226,13 @@ subroutine crystallite_restore(i,e,includeL)
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includeL !< protect agains fake cutback
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integer :: &
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c, p, m !< constituent number
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p = material_phaseAt(i,e)
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do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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if (includeL) then
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crystallite_Lp(1:3,1:3,c,i,e) = crystallite_partitionedLp0(1:3,1:3,c,i,e)
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crystallite_Li(1:3,1:3,c,i,e) = crystallite_partitionedLi0(1:3,1:3,c,i,e)
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endif ! maybe protecting everything from overwriting makes more sense
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p = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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crystallite_Fp(1:3,1:3,c,i,e) = crystallite_partitionedFp0(1:3,1:3,c,i,e)
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constitutive_mech_Fi(p)%data(1:3,1:3,m) = constitutive_mech_partionedFi0(p)%data(1:3,1:3,m)
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@ -1277,7 +1277,7 @@ function crystallite_stressTangent(c,i,e) result(dPdF)
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real(pReal), dimension(9,9):: temp_99
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logical :: error
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pp = material_phaseAt(i,e)
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pp = material_phaseAt(c,e)
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m = material_phaseMemberAt(c,i,e)
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call constitutive_hooke_SandItsTangents(devNull,dSdFe,dSdFi, &
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