smaller, readable functions
This commit is contained in:
parent
7beed17a39
commit
d805887ef7
|
@ -119,7 +119,10 @@ module crystallite
|
|||
crystallite_results, &
|
||||
crystallite_restartWrite, &
|
||||
crystallite_restartRead, &
|
||||
crystallite_forward
|
||||
crystallite_forward, &
|
||||
crystallite_initializeRestorationPoints, &
|
||||
crystallite_windForward, &
|
||||
crystallite_restore
|
||||
|
||||
contains
|
||||
|
||||
|
@ -480,6 +483,102 @@ function crystallite_stress()
|
|||
end function crystallite_stress
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief tbd
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
subroutine crystallite_initializeRestorationPoints(i,e)
|
||||
|
||||
integer, intent(in) :: &
|
||||
i, & !< integration point number
|
||||
e !< element number
|
||||
integer :: &
|
||||
c, & !< grain number
|
||||
s
|
||||
|
||||
do c = 1,homogenization_Ngrains(material_homogenizationAt(e))
|
||||
crystallite_partionedFp0(1:3,1:3,c,i,e) = crystallite_Fp0(1:3,1:3,c,i,e)
|
||||
crystallite_partionedLp0(1:3,1:3,c,i,e) = crystallite_Lp0(1:3,1:3,c,i,e)
|
||||
crystallite_partionedFi0(1:3,1:3,c,i,e) = crystallite_Fi0(1:3,1:3,c,i,e)
|
||||
crystallite_partionedLi0(1:3,1:3,c,i,e) = crystallite_Li0(1:3,1:3,c,i,e)
|
||||
crystallite_partionedF0(1:3,1:3,c,i,e) = crystallite_F0(1:3,1:3,c,i,e)
|
||||
crystallite_partionedS0(1:3,1:3,c,i,e) = crystallite_S0(1:3,1:3,c,i,e)
|
||||
|
||||
plasticState(material_phaseAt(c,e))%partionedState0(:,material_phasememberAt(c,i,e)) = &
|
||||
plasticState(material_phaseAt(c,e))%state0( :,material_phasememberAt(c,i,e))
|
||||
do s = 1, phase_Nsources(material_phaseAt(c,e))
|
||||
sourceState(material_phaseAt(c,e))%p(s)%partionedState0(:,material_phasememberAt(c,i,e)) = &
|
||||
sourceState(material_phaseAt(c,e))%p(s)%state0( :,material_phasememberAt(c,i,e))
|
||||
enddo
|
||||
enddo
|
||||
|
||||
end subroutine crystallite_initializeRestorationPoints
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief tbd
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
subroutine crystallite_windForward(i,e)
|
||||
|
||||
integer, intent(in) :: &
|
||||
i, & !< integration point number
|
||||
e !< element number
|
||||
integer :: &
|
||||
c, & !< grain number
|
||||
s
|
||||
|
||||
do c = 1,homogenization_Ngrains(material_homogenizationAt(e))
|
||||
crystallite_partionedF0 (1:3,1:3,c,i,e) = crystallite_partionedF(1:3,1:3,c,i,e)
|
||||
crystallite_partionedFp0(1:3,1:3,c,i,e) = crystallite_Fp (1:3,1:3,c,i,e)
|
||||
crystallite_partionedLp0(1:3,1:3,c,i,e) = crystallite_Lp (1:3,1:3,c,i,e)
|
||||
crystallite_partionedFi0(1:3,1:3,c,i,e) = crystallite_Fi (1:3,1:3,c,i,e)
|
||||
crystallite_partionedLi0(1:3,1:3,c,i,e) = crystallite_Li (1:3,1:3,c,i,e)
|
||||
crystallite_partionedS0 (1:3,1:3,c,i,e) = crystallite_S (1:3,1:3,c,i,e)
|
||||
|
||||
plasticState (material_phaseAt(c,e))%partionedState0(:,material_phasememberAt(c,i,e)) = &
|
||||
plasticState (material_phaseAt(c,e))%state (:,material_phasememberAt(c,i,e))
|
||||
do s = 1, phase_Nsources(material_phaseAt(c,e))
|
||||
sourceState(material_phaseAt(c,e))%p(s)%partionedState0(:,material_phasememberAt(c,i,e)) = &
|
||||
sourceState(material_phaseAt(c,e))%p(s)%state (:,material_phasememberAt(c,i,e))
|
||||
enddo
|
||||
enddo
|
||||
|
||||
end subroutine crystallite_windForward
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief tbd
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
subroutine crystallite_restore(i,e,includeL)
|
||||
|
||||
integer, intent(in) :: &
|
||||
i, & !< integration point number
|
||||
e !< element number
|
||||
logical, intent(in) :: &
|
||||
includeL !< protect agains fake cutback
|
||||
integer :: &
|
||||
c, & !< grain number
|
||||
s
|
||||
|
||||
do c = 1,homogenization_Ngrains(material_homogenizationAt(e))
|
||||
if (includeL) then
|
||||
crystallite_Lp(1:3,1:3,c,i,e) = crystallite_partionedLp0(1:3,1:3,c,i,e)
|
||||
crystallite_Li(1:3,1:3,c,i,e) = crystallite_partionedLi0(1:3,1:3,c,i,e)
|
||||
endif ! maybe protecting everything from overwriting makes more sense
|
||||
crystallite_Fp(1:3,1:3,c,i,e) = crystallite_partionedFp0(1:3,1:3,c,i,e)
|
||||
crystallite_Fi(1:3,1:3,c,i,e) = crystallite_partionedFi0(1:3,1:3,c,i,e)
|
||||
crystallite_S (1:3,1:3,c,i,e) = crystallite_partionedS0 (1:3,1:3,c,i,e)
|
||||
|
||||
plasticState (material_phaseAt(c,e))%state( :,material_phasememberAt(c,i,e)) = &
|
||||
plasticState (material_phaseAt(c,e))%partionedState0(:,material_phasememberAt(c,i,e))
|
||||
do s = 1, phase_Nsources(material_phaseAt(c,e))
|
||||
sourceState(material_phaseAt(c,e))%p(s)%state( :,material_phasememberAt(c,i,e)) = &
|
||||
sourceState(material_phaseAt(c,e))%p(s)%partionedState0(:,material_phasememberAt(c,i,e))
|
||||
enddo
|
||||
enddo
|
||||
|
||||
end subroutine crystallite_restore
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief calculate tangent (dPdF)
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
|
|
|
@ -211,10 +211,8 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
|
|||
integer :: &
|
||||
NiterationHomog, &
|
||||
NiterationMPstate, &
|
||||
g, & !< grain number
|
||||
i, & !< integration point number
|
||||
e, & !< element number
|
||||
mySource, &
|
||||
myNgrains
|
||||
real(pReal), dimension(discretization_nIP,discretization_nElem) :: &
|
||||
subFrac, &
|
||||
|
@ -225,40 +223,13 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
|
|||
logical, dimension(2,discretization_nIP,discretization_nElem) :: &
|
||||
doneAndHappy
|
||||
|
||||
#ifdef DEBUG
|
||||
|
||||
if (debugHomog%basic) then
|
||||
print'(/a,i5,1x,i2)', ' << HOMOG >> Material Point start at el ip ', debugHomog%element, debugHomog%ip
|
||||
|
||||
print'(a,/,3(12x,3(f14.9,1x)/))', ' << HOMOG >> F0', &
|
||||
transpose(materialpoint_F0(1:3,1:3,debugHomog%ip,debugHomog%element))
|
||||
print'(a,/,3(12x,3(f14.9,1x)/))', ' << HOMOG >> F', &
|
||||
transpose(materialpoint_F(1:3,1:3,debugHomog%ip,debugHomog%element))
|
||||
endif
|
||||
#endif
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
! initialize restoration points
|
||||
do e = FEsolving_execElem(1),FEsolving_execElem(2)
|
||||
myNgrains = homogenization_Ngrains(material_homogenizationAt(e))
|
||||
do i = FEsolving_execIP(1),FEsolving_execIP(2);
|
||||
do g = 1,myNgrains
|
||||
|
||||
plasticState (material_phaseAt(g,e))%partionedState0(:,material_phasememberAt(g,i,e)) = &
|
||||
plasticState (material_phaseAt(g,e))%state0( :,material_phasememberAt(g,i,e))
|
||||
do mySource = 1, phase_Nsources(material_phaseAt(g,e))
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%partionedState0(:,material_phasememberAt(g,i,e)) = &
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%state0( :,material_phasememberAt(g,i,e))
|
||||
enddo
|
||||
|
||||
crystallite_partionedFp0(1:3,1:3,g,i,e) = crystallite_Fp0(1:3,1:3,g,i,e)
|
||||
crystallite_partionedLp0(1:3,1:3,g,i,e) = crystallite_Lp0(1:3,1:3,g,i,e)
|
||||
crystallite_partionedFi0(1:3,1:3,g,i,e) = crystallite_Fi0(1:3,1:3,g,i,e)
|
||||
crystallite_partionedLi0(1:3,1:3,g,i,e) = crystallite_Li0(1:3,1:3,g,i,e)
|
||||
crystallite_partionedF0(1:3,1:3,g,i,e) = crystallite_F0(1:3,1:3,g,i,e)
|
||||
crystallite_partionedS0(1:3,1:3,g,i,e) = crystallite_S0(1:3,1:3,g,i,e)
|
||||
|
||||
enddo
|
||||
call crystallite_initializeRestorationPoints(i,e)
|
||||
|
||||
subFrac(i,e) = 0.0_pReal
|
||||
converged(i,e) = .false. ! pretend failed step ...
|
||||
|
@ -285,44 +256,19 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
|
|||
any(subStep(FEsolving_execIP(1):FEsolving_execIP(2),&
|
||||
FEsolving_execElem(1):FEsolving_execElem(2)) > num%subStepMinHomog))
|
||||
|
||||
!$OMP PARALLEL DO PRIVATE(myNgrains)
|
||||
!$OMP PARALLEL DO
|
||||
elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2)
|
||||
myNgrains = homogenization_Ngrains(material_homogenizationAt(e))
|
||||
IpLooping1: do i = FEsolving_execIP(1),FEsolving_execIP(2)
|
||||
|
||||
if (converged(i,e)) then
|
||||
#ifdef DEBUG
|
||||
if (debugHomog%extensive .and. ((e == debugHomog%element .and. i == debugHomog%ip) &
|
||||
.or. .not. debugHomog%selective)) then
|
||||
print'(a,f12.8,a,f12.8,a,i8,1x,i2/)', ' << HOMOG >> winding forward from ', &
|
||||
subFrac(i,e), ' to current subFrac ', &
|
||||
subFrac(i,e)+subStep(i,e),' in materialpoint_stressAndItsTangent at el ip ',e,i
|
||||
endif
|
||||
#endif
|
||||
|
||||
!---------------------------------------------------------------------------------------------------
|
||||
! calculate new subStep and new subFrac
|
||||
subFrac(i,e) = subFrac(i,e) + subStep(i,e)
|
||||
subStep(i,e) = min(1.0_pReal-subFrac(i,e),num%stepIncreaseHomog*subStep(i,e)) ! introduce flexibility for step increase/acceleration
|
||||
|
||||
steppingNeeded: if (subStep(i,e) > num%subStepMinHomog) then
|
||||
|
||||
! wind forward grain starting point
|
||||
crystallite_partionedF0 (1:3,1:3,1:myNgrains,i,e) = crystallite_partionedF(1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_partionedFp0(1:3,1:3,1:myNgrains,i,e) = crystallite_Fp (1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_partionedLp0(1:3,1:3,1:myNgrains,i,e) = crystallite_Lp (1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_partionedFi0(1:3,1:3,1:myNgrains,i,e) = crystallite_Fi (1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_partionedLi0(1:3,1:3,1:myNgrains,i,e) = crystallite_Li (1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_partionedS0 (1:3,1:3,1:myNgrains,i,e) = crystallite_S (1:3,1:3,1:myNgrains,i,e)
|
||||
|
||||
do g = 1,myNgrains
|
||||
plasticState (material_phaseAt(g,e))%partionedState0(:,material_phasememberAt(g,i,e)) = &
|
||||
plasticState (material_phaseAt(g,e))%state (:,material_phasememberAt(g,i,e))
|
||||
do mySource = 1, phase_Nsources(material_phaseAt(g,e))
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%partionedState0(:,material_phasememberAt(g,i,e)) = &
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%state (:,material_phasememberAt(g,i,e))
|
||||
enddo
|
||||
enddo
|
||||
call crystallite_windForward(i,e)
|
||||
|
||||
if(homogState(material_homogenizationAt(e))%sizeState > 0) &
|
||||
homogState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e)) = &
|
||||
|
@ -347,32 +293,8 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
|
|||
else ! cutback makes sense
|
||||
subStep(i,e) = num%subStepSizeHomog * subStep(i,e) ! crystallite had severe trouble, so do a significant cutback
|
||||
|
||||
#ifdef DEBUG
|
||||
if (debugHomog%extensive .and. ((e == debugHomog%element .and. i == debugHomog%ip) &
|
||||
.or. .not. debugHomog%selective)) then
|
||||
print'(a,f12.8,a,i8,1x,i2/)', &
|
||||
'<< HOMOG >> cutback step in materialpoint_stressAndItsTangent with new subStep: ',&
|
||||
subStep(i,e),' at el ip',e,i
|
||||
endif
|
||||
#endif
|
||||
call crystallite_restore(i,e,subStep(i,e) < 1.0_pReal)
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
! restore
|
||||
if (subStep(i,e) < 1.0_pReal) then ! protect against fake cutback from \Delta t = 2 to 1. Maybe that "trick" is not necessary anymore at all? I.e. start with \Delta t = 1
|
||||
crystallite_Lp(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedLp0(1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_Li(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedLi0(1:3,1:3,1:myNgrains,i,e)
|
||||
endif ! maybe protecting everything from overwriting (not only L) makes even more sense
|
||||
crystallite_Fp(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedFp0(1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_Fi(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedFi0(1:3,1:3,1:myNgrains,i,e)
|
||||
crystallite_S (1:3,1:3,1:myNgrains,i,e) = crystallite_partionedS0 (1:3,1:3,1:myNgrains,i,e)
|
||||
do g = 1, myNgrains
|
||||
plasticState (material_phaseAt(g,e))%state( :,material_phasememberAt(g,i,e)) = &
|
||||
plasticState (material_phaseAt(g,e))%partionedState0(:,material_phasememberAt(g,i,e))
|
||||
do mySource = 1, phase_Nsources(material_phaseAt(g,e))
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%state( :,material_phasememberAt(g,i,e)) = &
|
||||
sourceState(material_phaseAt(g,e))%p(mySource)%partionedState0(:,material_phasememberAt(g,i,e))
|
||||
enddo
|
||||
enddo
|
||||
if(homogState(material_homogenizationAt(e))%sizeState > 0) &
|
||||
homogState(material_homogenizationAt(e))%State( :,material_homogenizationMemberAt(i,e)) = &
|
||||
homogState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e))
|
||||
|
|
Loading…
Reference in New Issue