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phase depends on constituent, not integration point

This commit is contained in:
Martin Diehl 2020-12-21 09:48:20 +01:00
parent 07873b2409
commit 43cbe622d0
1 changed files with 9 additions and 9 deletions
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14
src/constitutive.f90
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@ -954,7 +954,7 @@ subroutine crystallite_init
do e = FEsolving_execElem(1),FEsolving_execElem(2) do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1), FEsolving_execIP(2); do c = 1, homogenization_Nconstituents(material_homogenizationAt(e)) do i = FEsolving_execIP(1), FEsolving_execIP(2); do c = 1, homogenization_Nconstituents(material_homogenizationAt(e))
p = material_phaseAt(i,e) p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
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) 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)
crystallite_Fp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e) & crystallite_Fp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e) &
@ -1031,7 +1031,7 @@ function crystallite_stress()
elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2) elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1),FEsolving_execIP(2); do c = 1,homogenization_Nconstituents(material_homogenizationAt(e)) do i = FEsolving_execIP(1),FEsolving_execIP(2); do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
homogenizationRequestsCalculation: if (crystallite_requested(c,i,e)) then homogenizationRequestsCalculation: if (crystallite_requested(c,i,e)) then
p = material_phaseAt(i,e) p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
plasticState (material_phaseAt(c,e))%subState0( :,material_phaseMemberAt(c,i,e)) = & plasticState (material_phaseAt(c,e))%subState0( :,material_phaseMemberAt(c,i,e)) = &
plasticState (material_phaseAt(c,e))%partitionedState0(:,material_phaseMemberAt(c,i,e)) plasticState (material_phaseAt(c,e))%partitionedState0(:,material_phaseMemberAt(c,i,e))
@ -1064,7 +1064,7 @@ function crystallite_stress()
elementLooping3: do e = FEsolving_execElem(1),FEsolving_execElem(2) elementLooping3: do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1),FEsolving_execIP(2) do i = FEsolving_execIP(1),FEsolving_execIP(2)
do c = 1,homogenization_Nconstituents(material_homogenizationAt(e)) do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
p = material_phaseAt(i,e) p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
!-------------------------------------------------------------------------------------------------- !--------------------------------------------------------------------------------------------------
! wind forward ! wind forward
@ -1161,8 +1161,8 @@ subroutine crystallite_initializeRestorationPoints(i,e)
c, & !< constituent number c, & !< constituent number
s,p, m s,p, m
p = material_phaseAt(i,e)
do c = 1,homogenization_Nconstituents(material_homogenizationAt(e)) do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e) crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e)
crystallite_partitionedLp0(1:3,1:3,c,i,e) = crystallite_Lp0(1:3,1:3,c,i,e) crystallite_partitionedLp0(1:3,1:3,c,i,e) = crystallite_Lp0(1:3,1:3,c,i,e)
@ -1193,8 +1193,8 @@ subroutine crystallite_windForward(i,e)
integer :: & integer :: &
c, & !< constituent number c, & !< constituent number
s, p, m s, p, m
p = material_phaseAt(i,e)
do c = 1,homogenization_Nconstituents(material_homogenizationAt(e)) do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
crystallite_partitionedF0 (1:3,1:3,c,i,e) = crystallite_partitionedF(1:3,1:3,c,i,e) crystallite_partitionedF0 (1:3,1:3,c,i,e) = crystallite_partitionedF(1:3,1:3,c,i,e)
crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp (1:3,1:3,c,i,e) crystallite_partitionedFp0(1:3,1:3,c,i,e) = crystallite_Fp (1:3,1:3,c,i,e)
@ -1226,13 +1226,13 @@ subroutine crystallite_restore(i,e,includeL)
includeL !< protect agains fake cutback includeL !< protect agains fake cutback
integer :: & integer :: &
c, p, m !< constituent number c, p, m !< constituent number
p = material_phaseAt(i,e)
do c = 1,homogenization_Nconstituents(material_homogenizationAt(e)) do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
if (includeL) then if (includeL) then
crystallite_Lp(1:3,1:3,c,i,e) = crystallite_partitionedLp0(1:3,1:3,c,i,e) crystallite_Lp(1:3,1:3,c,i,e) = crystallite_partitionedLp0(1:3,1:3,c,i,e)
crystallite_Li(1:3,1:3,c,i,e) = crystallite_partitionedLi0(1:3,1:3,c,i,e) crystallite_Li(1:3,1:3,c,i,e) = crystallite_partitionedLi0(1:3,1:3,c,i,e)
endif ! maybe protecting everything from overwriting makes more sense endif ! maybe protecting everything from overwriting makes more sense
p = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
crystallite_Fp(1:3,1:3,c,i,e) = crystallite_partitionedFp0(1:3,1:3,c,i,e) crystallite_Fp(1:3,1:3,c,i,e) = crystallite_partitionedFp0(1:3,1:3,c,i,e)
constitutive_mech_Fi(p)%data(1:3,1:3,m) = constitutive_mech_partionedFi0(p)%data(1:3,1:3,m) constitutive_mech_Fi(p)%data(1:3,1:3,m) = constitutive_mech_partionedFi0(p)%data(1:3,1:3,m)
@ -1277,7 +1277,7 @@ function crystallite_stressTangent(c,i,e) result(dPdF)
real(pReal), dimension(9,9):: temp_99 real(pReal), dimension(9,9):: temp_99
logical :: error logical :: error
pp = material_phaseAt(i,e) pp = material_phaseAt(c,e)
m = material_phaseMemberAt(c,i,e) m = material_phaseMemberAt(c,i,e)
call constitutive_hooke_SandItsTangents(devNull,dSdFe,dSdFi, & call constitutive_hooke_SandItsTangents(devNull,dSdFe,dSdFi, &