storing Lp and related fields in new structure
This commit is contained in:
Martin Diehl
parent
79a8a40e6d
commit
3719b9a52c
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@ -35,9 +35,6 @@ module constitutive
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!
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crystallite_Fe, & !< current "elastic" def grad (end of converged time step)
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!
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crystallite_Fp, & !< current plastic def grad (end of converged time step)
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crystallite_Fp0, & !< plastic def grad at start of FE inc
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crystallite_partitionedFp0,& !< plastic def grad at start of homog inc
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crystallite_subFp0,& !< plastic def grad at start of crystallite inc
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!
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crystallite_subFi0,& !< intermediate def grad at start of crystallite inc
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@ -71,7 +68,11 @@ module constitutive
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constitutive_mech_partionedFi0, &
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constitutive_mech_Li, &
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constitutive_mech_Li0, &
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constitutive_mech_partionedLi0
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constitutive_mech_partionedLi0, &
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constitutive_mech_Fp, &
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constitutive_mech_Fp0, &
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constitutive_mech_partionedFp0
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type :: tNumerics
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integer :: &
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@ -320,14 +321,13 @@ module constitutive
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end subroutine constitutive_plastic_LpAndItsTangents
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module subroutine constitutive_plastic_dependentState(F, Fp, ipc, ip, el)
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module subroutine constitutive_plastic_dependentState(F, ipc, ip, el)
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integer, intent(in) :: &
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ipc, & !< component-ID of integration point
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ip, & !< integration point
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el !< element
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real(pReal), intent(in), dimension(3,3) :: &
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F, & !< elastic deformation gradient
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Fp !< plastic deformation gradient
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F !< elastic deformation gradient
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end subroutine constitutive_plastic_dependentState
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@ -643,33 +643,22 @@ end function constitutive_damage_collectDotState
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!--------------------------------------------------------------------------------------------------
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!> @brief contains the constitutive equation for calculating the rate of change of microstructure
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!--------------------------------------------------------------------------------------------------
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function constitutive_thermal_collectDotState(S, ipc, ip, el,phase,of) result(broken)
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function constitutive_thermal_collectDotState(ph,me) result(broken)
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integer, intent(in) :: &
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ipc, & !< component-ID of integration point
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ip, & !< integration point
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el, & !< element
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phase, &
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of
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real(pReal), intent(in), dimension(3,3) :: &
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S !< 2nd Piola Kirchhoff stress (vector notation)
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integer :: &
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i !< counter in source loop
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integer, intent(in) :: ph, me
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logical :: broken
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integer :: i
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broken = .false.
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SourceLoop: do i = 1, phase_Nsources(phase)
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SourceLoop: do i = 1, phase_Nsources(ph)
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sourceType: select case (phase_source(i,phase))
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if (phase_source(i,ph) == SOURCE_thermal_externalheat_ID) &
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call source_thermal_externalheat_dotState(ph,me)
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case (SOURCE_thermal_externalheat_ID) sourceType
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call source_thermal_externalheat_dotState(phase,of)
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end select sourceType
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broken = broken .or. any(IEEE_is_NaN(sourceState(phase)%p(i)%dotState(:,of)))
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broken = broken .or. any(IEEE_is_NaN(sourceState(ph)%p(i)%dotState(:,me)))
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enddo SourceLoop
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@ -853,12 +842,12 @@ subroutine crystallite_init
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allocate(crystallite_partitionedF(3,3,cMax,iMax,eMax),source=0.0_pReal)
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allocate(crystallite_S0, &
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crystallite_F0,crystallite_Fp0,crystallite_Lp0, &
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crystallite_F0,crystallite_Lp0, &
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crystallite_partitionedS0, &
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crystallite_partitionedF0,crystallite_partitionedFp0,&
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crystallite_partitionedF0,&
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crystallite_partitionedLp0, &
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crystallite_S,crystallite_P, &
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crystallite_Fe,crystallite_Fp,crystallite_Lp, &
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crystallite_Fe,crystallite_Lp, &
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crystallite_subF,crystallite_subF0, &
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crystallite_subFp0,crystallite_subFi0, &
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source = crystallite_partitionedF)
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@ -908,6 +897,9 @@ subroutine crystallite_init
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allocate(constitutive_mech_Fi(phases%length))
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allocate(constitutive_mech_Fi0(phases%length))
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allocate(constitutive_mech_partionedFi0(phases%length))
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allocate(constitutive_mech_Fp(phases%length))
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allocate(constitutive_mech_Fp0(phases%length))
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allocate(constitutive_mech_partionedFp0(phases%length))
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allocate(constitutive_mech_Li(phases%length))
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allocate(constitutive_mech_Li0(phases%length))
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allocate(constitutive_mech_partionedLi0(phases%length))
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@ -917,6 +909,9 @@ subroutine crystallite_init
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allocate(constitutive_mech_Fi(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_Fi0(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_partionedFi0(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_Fp(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_Fp0(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_partionedFp0(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_Li(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_Li0(p)%data(3,3,Nconstituents))
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allocate(constitutive_mech_partionedLi0(p)%data(3,3,Nconstituents))
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@ -933,39 +928,38 @@ subroutine crystallite_init
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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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/ math_det33(crystallite_Fp0(1:3,1:3,c,i,e))**(1.0_pReal/3.0_pReal)
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constitutive_mech_Fp0(p)%data(1:3,1:3,m) = material_orientation0(c,i,e)%asMatrix() ! Fp reflects initial orientation (see 10.1016/j.actamat.2006.01.005)
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constitutive_mech_Fp0(p)%data(1:3,1:3,m) = constitutive_mech_Fp0(p)%data(1:3,1:3,m) &
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/ math_det33(constitutive_mech_Fp0(p)%data(1:3,1:3,m))**(1.0_pReal/3.0_pReal)
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constitutive_mech_Fi0(p)%data(1:3,1:3,m) = math_I3
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crystallite_F0(1:3,1:3,c,i,e) = math_I3
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crystallite_Fe(1:3,1:3,c,i,e) = math_inv33(matmul(constitutive_mech_Fi0(p)%data(1:3,1:3,m), &
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crystallite_Fp0(1:3,1:3,c,i,e))) ! assuming that euler angles are given in internal strain free configuration
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crystallite_Fp(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e)
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constitutive_mech_Fp0(p)%data(1:3,1:3,m))) ! assuming that euler angles are given in internal strain free configuration
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constitutive_mech_Fp(p)%data(1:3,1:3,m) = constitutive_mech_Fp0(p)%data(1:3,1:3,m)
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constitutive_mech_Fi(p)%data(1:3,1:3,m) = constitutive_mech_Fi0(p)%data(1:3,1:3,m)
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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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constitutive_mech_partionedFp0(p)%data(1:3,1:3,m) = constitutive_mech_Fp0(p)%data(1:3,1:3,m)
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crystallite_requested(c,i,e) = .true.
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enddo; enddo
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enddo
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!$OMP END PARALLEL DO
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crystallite_partitionedFp0 = crystallite_Fp0
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crystallite_partitionedF0 = crystallite_F0
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crystallite_partitionedF = crystallite_F0
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call crystallite_orientations()
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!$OMP PARALLEL DO
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!$OMP PARALLEL DO PRIVATE(p,m)
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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(c,e)
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m = material_phaseMemberAt(c,i,e)
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call constitutive_plastic_dependentState(crystallite_partitionedF0(1:3,1:3,c,i,e), &
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crystallite_partitionedFp0(1:3,1:3,c,i,e), &
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c,i,e) ! update dependent state variables to be consistent with basic states
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enddo
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enddo
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@ -1018,7 +1012,7 @@ function crystallite_stress()
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sourceState(material_phaseAt(c,e))%p(s)%subState0( :,material_phaseMemberAt(c,i,e)) = &
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sourceState(material_phaseAt(c,e))%p(s)%partitionedState0(:,material_phaseMemberAt(c,i,e))
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enddo
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crystallite_subFp0(1:3,1:3,c,i,e) = crystallite_partitionedFp0(1:3,1:3,c,i,e)
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crystallite_subFp0(1:3,1:3,c,i,e) = constitutive_mech_partionedFp0(p)%data(1:3,1:3,m)
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crystallite_subFi0(1:3,1:3,c,i,e) = constitutive_mech_partionedFi0(p)%data(1:3,1:3,m)
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crystallite_subF0(1:3,1:3,c,i,e) = crystallite_partitionedF0(1:3,1:3,c,i,e)
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subFrac(c,i,e) = 0.0_pReal
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@ -1058,7 +1052,7 @@ function crystallite_stress()
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crystallite_subF0 (1:3,1:3,c,i,e) = crystallite_subF(1:3,1:3,c,i,e)
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subLp0(1:3,1:3,c,i,e) = crystallite_Lp (1:3,1:3,c,i,e)
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subLi0(1:3,1:3,c,i,e) = constitutive_mech_Li(p)%data(1:3,1:3,m)
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crystallite_subFp0(1:3,1:3,c,i,e) = crystallite_Fp (1:3,1:3,c,i,e)
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crystallite_subFp0(1:3,1:3,c,i,e) = constitutive_mech_Fp(p)%data(1:3,1:3,m)
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crystallite_subFi0(1:3,1:3,c,i,e) = constitutive_mech_Fi(p)%data(1:3,1:3,m)
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plasticState( material_phaseAt(c,e))%subState0(:,material_phaseMemberAt(c,i,e)) &
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= plasticState(material_phaseAt(c,e))%state( :,material_phaseMemberAt(c,i,e))
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@ -1072,7 +1066,7 @@ function crystallite_stress()
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! cut back (reduced time and restore)
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else
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crystallite_subStep(c,i,e) = num%subStepSizeCryst * crystallite_subStep(c,i,e)
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crystallite_Fp (1:3,1:3,c,i,e) = crystallite_subFp0(1:3,1:3,c,i,e)
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constitutive_mech_Fp(p)%data(1:3,1:3,m) = crystallite_subFp0(1:3,1:3,c,i,e)
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constitutive_mech_Fi(p)%data(1:3,1:3,m) = crystallite_subFi0(1:3,1:3,c,i,e)
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crystallite_S (1:3,1:3,c,i,e) = crystallite_S0 (1:3,1:3,c,i,e)
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if (crystallite_subStep(c,i,e) < 1.0_pReal) then ! actual (not initial) cutback
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@ -1098,7 +1092,7 @@ function crystallite_stress()
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-crystallite_partitionedF0(1:3,1:3,c,i,e))
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crystallite_Fe(1:3,1:3,c,i,e) = matmul(crystallite_subF(1:3,1:3,c,i,e), &
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math_inv33(matmul(constitutive_mech_Fi(p)%data(1:3,1:3,m), &
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crystallite_Fp(1:3,1:3,c,i,e))))
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constitutive_mech_Fp(p)%data(1:3,1:3,m))))
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crystallite_subdt(c,i,e) = crystallite_subStep(c,i,e) * crystallite_dt(c,i,e)
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crystallite_converged(c,i,e) = .false.
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call integrateState(c,i,e)
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@ -1142,7 +1136,6 @@ subroutine constitutive_initializeRestorationPoints(i,e)
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do c = 1,homogenization_Nconstituents(material_homogenizationAt(e))
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ph = material_phaseAt(c,e)
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me = 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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crystallite_partitionedF0(1:3,1:3,c,i,e) = crystallite_F0(1:3,1:3,c,i,e)
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crystallite_partitionedS0(1:3,1:3,c,i,e) = crystallite_S0(1:3,1:3,c,i,e)
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@ -1172,7 +1165,7 @@ subroutine constitutive_windForward(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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constitutive_mech_partionedFp0(p)%data(1:3,1:3,m) = constitutive_mech_Fp(p)%data(1:3,1:3,m)
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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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constitutive_mech_partionedFi0(p)%data(1:3,1:3,m) = constitutive_mech_Fi(p)%data(1:3,1:3,m)
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constitutive_mech_partionedLi0(p)%data(1:3,1:3,m) = constitutive_mech_Li(p)%data(1:3,1:3,m)
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@ -1210,7 +1203,7 @@ subroutine crystallite_restore(i,e,includeL)
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constitutive_mech_Li(p)%data(1:3,1:3,m) = constitutive_mech_partionedLi0(p)%data(1:3,1:3,m)
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endif ! maybe protecting everything from overwriting makes more sense
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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_Fp(p)%data(1:3,1:3,m) = constitutive_mech_partionedFp0(p)%data(1:3,1:3,m)
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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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crystallite_S (1:3,1:3,c,i,e) = crystallite_partitionedS0 (1:3,1:3,c,i,e)
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@ -1264,7 +1257,7 @@ function crystallite_stressTangent(c,i,e) result(dPdF)
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constitutive_mech_Fi(pp)%data(1:3,1:3,m), &
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c,i,e)
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invFp = math_inv33(crystallite_Fp(1:3,1:3,c,i,e))
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invFp = math_inv33(constitutive_mech_Fp(pp)%data(1:3,1:3,m))
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invFi = math_inv33(constitutive_mech_Fi(pp)%data(1:3,1:3,m))
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invSubFp0 = math_inv33(crystallite_subFp0(1:3,1:3,c,i,e))
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invSubFi0 = math_inv33(crystallite_subFi0(1:3,1:3,c,i,e))
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@ -1434,7 +1427,7 @@ subroutine integrateSourceState(g,i,e)
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p = material_phaseAt(g,e)
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c = material_phaseMemberAt(g,i,e)
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broken = constitutive_thermal_collectDotState(crystallite_S(1:3,1:3,g,i,e), g,i,e,p,c)
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broken = constitutive_thermal_collectDotState(p,c)
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broken = broken .or. constitutive_damage_collectDotState(crystallite_S(1:3,1:3,g,i,e), g,i,e,p,c)
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if(broken) return
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@ -1453,7 +1446,7 @@ subroutine integrateSourceState(g,i,e)
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source_dotState(1:size_so(s),1,s) = sourceState(p)%p(s)%dotState(:,c)
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enddo
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broken = constitutive_thermal_collectDotState(crystallite_S(1:3,1:3,g,i,e), g,i,e,p,c)
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broken = constitutive_thermal_collectDotState(p,c)
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broken = broken .or. constitutive_damage_collectDotState(crystallite_S(1:3,1:3,g,i,e), g,i,e,p,c)
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if(broken) exit iteration
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@ -1540,7 +1533,6 @@ subroutine crystallite_restartWrite
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fileHandle = HDF5_openFile(fileName,'a')
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call HDF5_write(fileHandle,crystallite_partitionedF,'F')
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call HDF5_write(fileHandle,crystallite_Fp, 'F_p')
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call HDF5_write(fileHandle,crystallite_Lp, 'L_p')
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call HDF5_write(fileHandle,crystallite_S, 'S')
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@ -1552,6 +1544,8 @@ subroutine crystallite_restartWrite
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call HDF5_write(groupHandle,constitutive_mech_Fi(i)%data,datasetName)
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write(datasetName,'(i0,a)') i,'_L_i'
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call HDF5_write(groupHandle,constitutive_mech_Li(i)%data,datasetName)
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write(datasetName,'(i0,a)') i,'_F_p'
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call HDF5_write(groupHandle,constitutive_mech_Fp(i)%data,datasetName)
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enddo
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call HDF5_closeGroup(groupHandle)
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@ -1583,7 +1577,6 @@ subroutine crystallite_restartRead
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fileHandle = HDF5_openFile(fileName)
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call HDF5_read(fileHandle,crystallite_F0, 'F')
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call HDF5_read(fileHandle,crystallite_Fp0,'F_p')
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call HDF5_read(fileHandle,crystallite_Lp0,'L_p')
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call HDF5_read(fileHandle,crystallite_S0, 'S')
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@ -1595,6 +1588,8 @@ subroutine crystallite_restartRead
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call HDF5_read(groupHandle,constitutive_mech_Fi0(i)%data,datasetName)
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write(datasetName,'(i0,a)') i,'_L_i'
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call HDF5_read(groupHandle,constitutive_mech_Li0(i)%data,datasetName)
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write(datasetName,'(i0,a)') i,'_F_p'
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call HDF5_read(groupHandle,constitutive_mech_Fp0(i)%data,datasetName)
|
||||
enddo
|
||||
call HDF5_closeGroup(groupHandle)
|
||||
|
||||
|
|
@ -1619,13 +1614,13 @@ subroutine crystallite_forward
|
|||
integer :: i, j
|
||||
|
||||
crystallite_F0 = crystallite_partitionedF
|
||||
crystallite_Fp0 = crystallite_Fp
|
||||
crystallite_Lp0 = crystallite_Lp
|
||||
crystallite_S0 = crystallite_S
|
||||
|
||||
do i = 1, size(plasticState)
|
||||
plasticState(i)%state0 = plasticState(i)%state
|
||||
constitutive_mech_Fi0(i) = constitutive_mech_Fi(i)
|
||||
constitutive_mech_Fp0(i) = constitutive_mech_Fp(i)
|
||||
constitutive_mech_Li0(i) = constitutive_mech_Li(i)
|
||||
enddo
|
||||
do i = 1,size(material_name_homogenization)
|
||||
|
|
|
|||
|
|
@ -462,15 +462,14 @@ end subroutine constitutive_hooke_SandItsTangents
|
|||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief calls microstructure function of the different plasticity constitutive models
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
module subroutine constitutive_plastic_dependentState(F, Fp, ipc, ip, el)
|
||||
module subroutine constitutive_plastic_dependentState(F, ipc, ip, el)
|
||||
|
||||
integer, intent(in) :: &
|
||||
ipc, & !< component-ID of integration point
|
||||
ip, & !< integration point
|
||||
el !< element
|
||||
real(pReal), intent(in), dimension(3,3) :: &
|
||||
F, & !< elastic deformation gradient
|
||||
Fp !< plastic deformation gradient
|
||||
F !< elastic deformation gradient
|
||||
|
||||
integer :: &
|
||||
ho, & !< homogenization
|
||||
|
|
@ -569,7 +568,7 @@ end subroutine constitutive_plastic_LpAndItsTangents
|
|||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief contains the constitutive equation for calculating the rate of change of microstructure
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
function mech_collectDotState(FpArray, subdt, ipc, ip, el,phase,of) result(broken)
|
||||
function mech_collectDotState(subdt, ipc, ip, el,phase,of) result(broken)
|
||||
|
||||
integer, intent(in) :: &
|
||||
ipc, & !< component-ID of integration point
|
||||
|
|
@ -579,8 +578,6 @@ function mech_collectDotState(FpArray, subdt, ipc, ip, el,phase,of) result(broke
|
|||
of
|
||||
real(pReal), intent(in) :: &
|
||||
subdt !< timestep
|
||||
real(pReal), intent(in), dimension(3,3,homogenization_maxNconstituents,discretization_nIPs,discretization_Nelems) :: &
|
||||
FpArray !< plastic deformation gradient
|
||||
real(pReal), dimension(3,3) :: &
|
||||
Mp
|
||||
integer :: &
|
||||
|
|
@ -793,8 +790,7 @@ function integrateStress(ipc,ip,el,timeFraction) result(broken)
|
|||
F = crystallite_subF(1:3,1:3,ipc,ip,el)
|
||||
endif
|
||||
|
||||
call constitutive_plastic_dependentState(crystallite_partitionedF(1:3,1:3,ipc,ip,el), &
|
||||
crystallite_Fp(1:3,1:3,ipc,ip,el),ipc,ip,el)
|
||||
call constitutive_plastic_dependentState(crystallite_partitionedF(1:3,1:3,ipc,ip,el),ipc,ip,el)
|
||||
|
||||
p = material_phaseAt(ipc,el)
|
||||
m = material_phaseMemberAt(ipc,ip,el)
|
||||
|
|
@ -936,7 +932,7 @@ function integrateStress(ipc,ip,el,timeFraction) result(broken)
|
|||
crystallite_S (1:3,1:3,ipc,ip,el) = S
|
||||
crystallite_Lp (1:3,1:3,ipc,ip,el) = Lpguess
|
||||
constitutive_mech_Li(p)%data(1:3,1:3,m) = Liguess
|
||||
crystallite_Fp (1:3,1:3,ipc,ip,el) = Fp_new / math_det33(Fp_new)**(1.0_pReal/3.0_pReal) ! regularize
|
||||
constitutive_mech_Fp(p)%data(1:3,1:3,m) = Fp_new / math_det33(Fp_new)**(1.0_pReal/3.0_pReal) ! regularize
|
||||
constitutive_mech_Fi(p)%data(1:3,1:3,m) = Fi_new
|
||||
crystallite_Fe (1:3,1:3,ipc,ip,el) = matmul(matmul(F,invFp_new),invFi_new)
|
||||
broken = .false.
|
||||
|
|
@ -975,8 +971,7 @@ module subroutine integrateStateFPI(g,i,e)
|
|||
p = material_phaseAt(g,e)
|
||||
c = material_phaseMemberAt(g,i,e)
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) return
|
||||
|
||||
size_pl = plasticState(p)%sizeDotState
|
||||
|
|
@ -993,8 +988,7 @@ module subroutine integrateStateFPI(g,i,e)
|
|||
broken = integrateStress(g,i,e)
|
||||
if(broken) exit iteration
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) exit iteration
|
||||
|
||||
zeta = damper(plasticState(p)%dotState(:,c),plastic_dotState(1:size_pl,1),&
|
||||
|
|
@ -1063,8 +1057,7 @@ subroutine integrateStateEuler(g,i,e)
|
|||
p = material_phaseAt(g,e)
|
||||
c = material_phaseMemberAt(g,i,e)
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) return
|
||||
|
||||
sizeDotState = plasticState(p)%sizeDotState
|
||||
|
|
@ -1104,8 +1097,7 @@ subroutine integrateStateAdaptiveEuler(g,i,e)
|
|||
p = material_phaseAt(g,e)
|
||||
c = material_phaseMemberAt(g,i,e)
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) return
|
||||
|
||||
sizeDotState = plasticState(p)%sizeDotState
|
||||
|
|
@ -1121,8 +1113,7 @@ subroutine integrateStateAdaptiveEuler(g,i,e)
|
|||
broken = integrateStress(g,i,e)
|
||||
if(broken) return
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) return
|
||||
|
||||
|
||||
|
|
@ -1216,8 +1207,7 @@ subroutine integrateStateRK(g,i,e,A,B,CC,DB)
|
|||
p = material_phaseAt(g,e)
|
||||
c = material_phaseMemberAt(g,i,e)
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e), g,i,e,p,c)
|
||||
if(broken) return
|
||||
|
||||
do stage = 1,size(A,1)
|
||||
|
|
@ -1239,8 +1229,7 @@ subroutine integrateStateRK(g,i,e,A,B,CC,DB)
|
|||
broken = integrateStress(g,i,e,CC(stage))
|
||||
if(broken) exit
|
||||
|
||||
broken = mech_collectDotState(crystallite_partitionedFp0, &
|
||||
crystallite_subdt(g,i,e)*CC(stage), g,i,e,p,c)
|
||||
broken = mech_collectDotState(crystallite_subdt(g,i,e)*CC(stage), g,i,e,p,c)
|
||||
if(broken) exit
|
||||
|
||||
enddo
|
||||
|
|
@ -1301,8 +1290,7 @@ subroutine crystallite_results(group,ph)
|
|||
call results_writeDataset(group//'/mechanics/',selected_tensors,output_constituent(ph)%label(ou),&
|
||||
'elastic deformation gradient','1')
|
||||
case('F_p')
|
||||
selected_tensors = select_tensors(crystallite_Fp,ph)
|
||||
call results_writeDataset(group//'/mechanics/',selected_tensors,output_constituent(ph)%label(ou),&
|
||||
call results_writeDataset(group//'/mechanics/',constitutive_mech_Fp(ph)%data,output_constituent(ph)%label(ou),&
|
||||
'plastic deformation gradient','1')
|
||||
case('F_i')
|
||||
call results_writeDataset(group//'/mechanics/',constitutive_mech_Fi(ph)%data,output_constituent(ph)%label(ou),&
|
||||
|
|
@ -1414,6 +1402,7 @@ module subroutine mech_initializeRestorationPoints(ph,me)
|
|||
|
||||
|
||||
constitutive_mech_partionedFi0(ph)%data(1:3,1:3,me) = constitutive_mech_Fi0(ph)%data(1:3,1:3,me)
|
||||
constitutive_mech_partionedFp0(ph)%data(1:3,1:3,me) = constitutive_mech_Fp0(ph)%data(1:3,1:3,me)
|
||||
constitutive_mech_partionedLi0(ph)%data(1:3,1:3,me) = constitutive_mech_Li0(ph)%data(1:3,1:3,me)
|
||||
plasticState(ph)%partitionedState0(:,me) = plasticState(ph)%state0(:,me)
|
||||
|
||||
|
|
|
|||
|
|
@ -563,6 +563,8 @@ module subroutine plastic_nonlocal_dependentState(F, instance, of, ip, el)
|
|||
el
|
||||
|
||||
integer :: &
|
||||
ph, &
|
||||
me, &
|
||||
no, & !< neighbor offset
|
||||
neighbor_el, & ! element number of neighboring material point
|
||||
neighbor_ip, & ! integration point of neighboring material point
|
||||
|
|
@ -642,8 +644,10 @@ module subroutine plastic_nonlocal_dependentState(F, instance, of, ip, el)
|
|||
|
||||
rho0 = getRho0(instance,of,ip,el)
|
||||
if (.not. phase_localPlasticity(material_phaseAt(1,el)) .and. prm%shortRangeStressCorrection) then
|
||||
invFp = math_inv33(crystallite_Fp(1:3,1:3,1,ip,el))
|
||||
invFe = matmul(crystallite_Fp(1:3,1:3,1,ip,el),math_inv33(F))
|
||||
ph = material_phaseAt(1,el)
|
||||
me = material_phaseMemberAt(1,ip,el)
|
||||
invFp = math_inv33(constitutive_mech_Fp(ph)%data(1:3,1:3,me))
|
||||
invFe = matmul(constitutive_mech_Fp(ph)%data(1:3,1:3,me),math_inv33(F))
|
||||
|
||||
rho_edg_delta = rho0(:,mob_edg_pos) - rho0(:,mob_edg_neg)
|
||||
rho_scr_delta = rho0(:,mob_scr_pos) - rho0(:,mob_scr_neg)
|
||||
|
|
@ -1290,7 +1294,7 @@ function rhoDotFlux(F,timestep, instance,of,ip,el)
|
|||
m(1:3,:,4) = prm%slip_transverse
|
||||
|
||||
my_F = F(1:3,1:3,1,ip,el)
|
||||
my_Fe = matmul(my_F, math_inv33(crystallite_Fp(1:3,1:3,1,ip,el)))
|
||||
my_Fe = matmul(my_F, math_inv33(constitutive_mech_Fp(ph)%data(1:3,1:3,of)))
|
||||
|
||||
neighbors: do n = 1,nIPneighbors
|
||||
|
||||
|
|
@ -1308,7 +1312,7 @@ function rhoDotFlux(F,timestep, instance,of,ip,el)
|
|||
if (neighbor_n > 0) then ! if neighbor exists, average deformation gradient
|
||||
neighbor_instance = phase_plasticityInstance(material_phaseAt(1,neighbor_el))
|
||||
neighbor_F = F(1:3,1:3,1,neighbor_ip,neighbor_el)
|
||||
neighbor_Fe = matmul(neighbor_F, math_inv33(crystallite_Fp(1:3,1:3,1,neighbor_ip,neighbor_el)))
|
||||
neighbor_Fe = matmul(neighbor_F, math_inv33(constitutive_mech_Fp(np)%data(1:3,1:3,no)))
|
||||
Favg = 0.5_pReal * (my_F + neighbor_F)
|
||||
else ! if no neighbor, take my value as average
|
||||
Favg = my_F
|
||||
|
|
|
|||
Loading…
Reference in New Issue