parent
fc171f388a
commit
dcd22ccb6a
|
@ -381,7 +381,7 @@ subroutine plastic_phenopowerlaw_init
|
|||
dot%gamma_twin => plasticState(p)%dotState(startIndex:endIndex,:)
|
||||
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolShear
|
||||
|
||||
plasticState(p)%state0 = plasticState(p)%state ! ToDo: this could be done centrally
|
||||
plasticState(p)%state0 = plasticState(p)%state ! ToDo: this could be done centrally
|
||||
dot%whole => plasticState(p)%dotState
|
||||
|
||||
end associate
|
||||
|
@ -398,7 +398,7 @@ end subroutine plastic_phenopowerlaw_init
|
|||
subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
|
||||
|
||||
implicit none
|
||||
real(pReal), dimension(3,3), intent(out) :: &
|
||||
real(pReal), dimension(3,3), intent(out) :: &
|
||||
Lp !< plastic velocity gradient
|
||||
real(pReal), dimension(3,3,3,3), intent(out) :: &
|
||||
dLp_dMp !< derivative of Lp with respect to the Mandel stress
|
||||
|
@ -420,9 +420,9 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
|
|||
Lp = 0.0_pReal
|
||||
dLp_dMp = 0.0_pReal
|
||||
|
||||
associate(prm => param(instance), stt => state(instance))
|
||||
associate(prm => param(instance))
|
||||
|
||||
call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
|
||||
call kinetics_slip(Mp,instance,of,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
|
||||
slipSystems: do i = 1_pInt, prm%totalNslip
|
||||
Lp = Lp + (gdot_slip_pos(i)+gdot_slip_neg(i))*prm%Schmid_slip(1:3,1:3,i)
|
||||
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
|
||||
|
@ -431,7 +431,7 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
|
|||
+ dgdot_dtauslip_neg(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_neg(m,n,i)
|
||||
enddo slipSystems
|
||||
|
||||
call kinetics_twin(prm,stt,of,Mp,gdot_twin,dgdot_dtautwin)
|
||||
call kinetics_twin(Mp,instance,of,gdot_twin,dgdot_dtautwin)
|
||||
twinSystems: do i = 1_pInt, prm%totalNtwin
|
||||
Lp = Lp + gdot_twin(i)*prm%Schmid_twin(1:3,1:3,i)
|
||||
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
|
||||
|
@ -452,7 +452,7 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
|
|||
implicit none
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp !< Mandel stress
|
||||
integer(pInt), intent(in) :: &
|
||||
integer(pInt), intent(in) :: &
|
||||
instance, &
|
||||
of
|
||||
|
||||
|
@ -487,9 +487,9 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
|
|||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
! shear rates
|
||||
call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg)
|
||||
call kinetics_slip(Mp,instance,of,gdot_slip_pos,gdot_slip_neg)
|
||||
dot%gamma_slip(:,of) = abs(gdot_slip_pos+gdot_slip_neg)
|
||||
call kinetics_twin(prm,stt,of,Mp,dot%gamma_twin(:,of))
|
||||
call kinetics_twin(Mp,instance,of,dot%gamma_twin(:,of))
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
! hardening
|
||||
|
@ -509,41 +509,110 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
|
|||
end subroutine plastic_phenopowerlaw_dotState
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief return array of constitutive results
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
function plastic_phenopowerlaw_postResults(Mp,instance,of) result(postResults)
|
||||
use math, only: &
|
||||
math_mul33xx33
|
||||
|
||||
implicit none
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp !< Mandel stress
|
||||
integer(pInt), intent(in) :: &
|
||||
instance, &
|
||||
of
|
||||
|
||||
real(pReal), dimension(sum(plastic_phenopowerlaw_sizePostResult(:,instance))) :: &
|
||||
postResults
|
||||
|
||||
integer(pInt) :: &
|
||||
o,c,i
|
||||
real(pReal), dimension(param(instance)%totalNslip) :: &
|
||||
gdot_slip_pos,gdot_slip_neg
|
||||
|
||||
postResults = 0.0_pReal
|
||||
c = 0_pInt
|
||||
|
||||
associate( prm => param(instance), stt => state(instance))
|
||||
|
||||
outputsLoop: do o = 1_pInt,size(prm%outputID)
|
||||
select case(prm%outputID(o))
|
||||
|
||||
case (resistance_slip_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = stt%xi_slip(1:prm%totalNslip,of)
|
||||
c = c + prm%totalNslip
|
||||
case (accumulatedshear_slip_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = stt%gamma_slip(1:prm%totalNslip,of)
|
||||
c = c + prm%totalNslip
|
||||
case (shearrate_slip_ID)
|
||||
call kinetics_slip(Mp,instance,of,gdot_slip_pos,gdot_slip_neg)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = gdot_slip_pos+gdot_slip_neg
|
||||
c = c + prm%totalNslip
|
||||
case (resolvedstress_slip_ID)
|
||||
do i = 1_pInt, prm%totalNslip
|
||||
postResults(c+i) = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,i))
|
||||
enddo
|
||||
c = c + prm%totalNslip
|
||||
|
||||
case (resistance_twin_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNtwin) = stt%xi_twin(1:prm%totalNtwin,of)
|
||||
c = c + prm%totalNtwin
|
||||
case (accumulatedshear_twin_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNtwin) = stt%gamma_twin(1:prm%totalNtwin,of)
|
||||
c = c + prm%totalNtwin
|
||||
case (shearrate_twin_ID)
|
||||
call kinetics_twin(Mp,instance,of,postResults(c+1_pInt:c+prm%totalNtwin))
|
||||
c = c + prm%totalNtwin
|
||||
case (resolvedstress_twin_ID)
|
||||
do i = 1_pInt, prm%totalNtwin
|
||||
postResults(c+i) = math_mul33xx33(Mp,prm%Schmid_twin(1:3,1:3,i))
|
||||
enddo
|
||||
c = c + prm%totalNtwin
|
||||
|
||||
end select
|
||||
enddo outputsLoop
|
||||
|
||||
end associate
|
||||
|
||||
end function plastic_phenopowerlaw_postResults
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief calculates shear rates on slip systems and derivatives with respect to resolved stress
|
||||
!> @details Shear rates are calculated only optionally.
|
||||
! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
|
||||
! have the optional arguments at the end
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
pure subroutine kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg, &
|
||||
dgdot_dtau_slip_pos,dgdot_dtau_slip_neg)
|
||||
pure subroutine kinetics_slip(Mp,instance,of, &
|
||||
gdot_slip_pos,gdot_slip_neg,dgdot_dtau_slip_pos,dgdot_dtau_slip_neg)
|
||||
use prec, only: &
|
||||
dNeq0
|
||||
use math, only: &
|
||||
math_mul33xx33
|
||||
|
||||
implicit none
|
||||
type(tParameters), intent(in) :: &
|
||||
prm
|
||||
type(tPhenopowerlawState), intent(in) :: &
|
||||
stt
|
||||
integer(pInt), intent(in) :: &
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp !< Mandel stress
|
||||
integer(pInt), intent(in) :: &
|
||||
instance, &
|
||||
of
|
||||
real(pReal), dimension(prm%totalNslip), intent(out) :: &
|
||||
|
||||
real(pReal), dimension(param(instance)%totalNslip), intent(out) :: &
|
||||
gdot_slip_pos, &
|
||||
gdot_slip_neg
|
||||
real(pReal), dimension(prm%totalNslip), optional, intent(out) :: &
|
||||
real(pReal), dimension(param(instance)%totalNslip), intent(out), optional :: &
|
||||
dgdot_dtau_slip_pos, &
|
||||
dgdot_dtau_slip_neg
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp
|
||||
|
||||
real(pReal), dimension(prm%totalNslip) :: &
|
||||
real(pReal), dimension(param(instance)%totalNslip) :: &
|
||||
tau_slip_pos, &
|
||||
tau_slip_neg
|
||||
integer(pInt) :: i
|
||||
logical :: nonSchmidActive
|
||||
|
||||
associate(prm => param(instance), stt => state(instance))
|
||||
|
||||
nonSchmidActive = size(prm%nonSchmidCoeff) > 0_pInt
|
||||
|
||||
do i = 1_pInt, prm%totalNslip
|
||||
|
@ -580,6 +649,7 @@ pure subroutine kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg, &
|
|||
dgdot_dtau_slip_neg = 0.0_pReal
|
||||
end where
|
||||
endif
|
||||
end associate
|
||||
|
||||
end subroutine kinetics_slip
|
||||
|
||||
|
@ -591,30 +661,31 @@ end subroutine kinetics_slip
|
|||
! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
|
||||
! have the optional arguments at the end.
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
pure subroutine kinetics_twin(prm,stt,of,Mp,gdot_twin,dgdot_dtau_twin)
|
||||
pure subroutine kinetics_twin(Mp,instance,of,&
|
||||
gdot_twin,dgdot_dtau_twin)
|
||||
use prec, only: &
|
||||
dNeq0
|
||||
use math, only: &
|
||||
math_mul33xx33
|
||||
|
||||
implicit none
|
||||
type(tParameters), intent(in) :: &
|
||||
prm
|
||||
type(tPhenopowerlawState), intent(in) :: &
|
||||
stt
|
||||
integer(pInt), intent(in) :: &
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp !< Mandel stress
|
||||
integer(pInt), intent(in) :: &
|
||||
instance, &
|
||||
of
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp
|
||||
real(pReal), dimension(prm%totalNtwin), intent(out) :: &
|
||||
|
||||
real(pReal), dimension(param(instance)%totalNtwin), intent(out) :: &
|
||||
gdot_twin
|
||||
real(pReal), dimension(prm%totalNtwin), optional, intent(out) :: &
|
||||
real(pReal), dimension(param(instance)%totalNtwin), intent(out), optional :: &
|
||||
dgdot_dtau_twin
|
||||
|
||||
real(pReal), dimension(prm%totalNtwin) :: &
|
||||
real(pReal), dimension(param(instance)%totalNtwin) :: &
|
||||
tau_twin
|
||||
integer(pInt) :: i
|
||||
|
||||
associate(prm => param(instance), stt => state(instance))
|
||||
|
||||
do i = 1_pInt, prm%totalNtwin
|
||||
tau_twin(i) = math_mul33xx33(Mp,prm%Schmid_twin(1:3,1:3,i))
|
||||
enddo
|
||||
|
@ -634,75 +705,8 @@ pure subroutine kinetics_twin(prm,stt,of,Mp,gdot_twin,dgdot_dtau_twin)
|
|||
end where
|
||||
endif
|
||||
|
||||
end subroutine kinetics_twin
|
||||
|
||||
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
!> @brief return array of constitutive results
|
||||
!--------------------------------------------------------------------------------------------------
|
||||
function plastic_phenopowerlaw_postResults(Mp,instance,of) result(postResults)
|
||||
use math, only: &
|
||||
math_mul33xx33
|
||||
|
||||
implicit none
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mp !< Mandel stress
|
||||
integer(pInt), intent(in) :: &
|
||||
instance, &
|
||||
of
|
||||
|
||||
real(pReal), dimension(sum(plastic_phenopowerlaw_sizePostResult(:,instance))) :: &
|
||||
postResults
|
||||
|
||||
integer(pInt) :: &
|
||||
o,c,i
|
||||
real(pReal), dimension(param(instance)%totalNslip) :: &
|
||||
gdot_slip_pos,gdot_slip_neg
|
||||
|
||||
postResults = 0.0_pReal
|
||||
c = 0_pInt
|
||||
|
||||
associate( prm => param(instance), stt => state(instance))
|
||||
|
||||
outputsLoop: do o = 1_pInt,size(prm%outputID)
|
||||
select case(prm%outputID(o))
|
||||
|
||||
case (resistance_slip_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = stt%xi_slip(1:prm%totalNslip,of)
|
||||
c = c + prm%totalNslip
|
||||
case (accumulatedshear_slip_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = stt%gamma_slip(1:prm%totalNslip,of)
|
||||
c = c + prm%totalNslip
|
||||
case (shearrate_slip_ID)
|
||||
call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg)
|
||||
postResults(c+1_pInt:c+prm%totalNslip) = gdot_slip_pos+gdot_slip_neg
|
||||
c = c + prm%totalNslip
|
||||
case (resolvedstress_slip_ID)
|
||||
do i = 1_pInt, prm%totalNslip
|
||||
postResults(c+i) = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,i))
|
||||
enddo
|
||||
c = c + prm%totalNslip
|
||||
|
||||
case (resistance_twin_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNtwin) = stt%xi_twin(1:prm%totalNtwin,of)
|
||||
c = c + prm%totalNtwin
|
||||
case (accumulatedshear_twin_ID)
|
||||
postResults(c+1_pInt:c+prm%totalNtwin) = stt%gamma_twin(1:prm%totalNtwin,of)
|
||||
c = c + prm%totalNtwin
|
||||
case (shearrate_twin_ID)
|
||||
call kinetics_twin(prm,stt,of,Mp,postResults(c+1_pInt:c+prm%totalNtwin))
|
||||
c = c + prm%totalNtwin
|
||||
case (resolvedstress_twin_ID)
|
||||
do i = 1_pInt, prm%totalNtwin
|
||||
postResults(c+i) = math_mul33xx33(Mp,prm%Schmid_twin(1:3,1:3,i))
|
||||
enddo
|
||||
c = c + prm%totalNtwin
|
||||
|
||||
end select
|
||||
enddo outputsLoop
|
||||
|
||||
end associate
|
||||
|
||||
end function plastic_phenopowerlaw_postResults
|
||||
end subroutine kinetics_twin
|
||||
|
||||
end module plastic_phenopowerlaw
|
||||
|
|
Loading…
Reference in New Issue