no need to calculate twinned volume fraction as state

This commit is contained in:
Martin Diehl 2018-11-25 16:14:46 +01:00
parent 8a253856f1
commit 7cc2892e64
1 changed files with 12 additions and 21 deletions

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@ -78,8 +78,6 @@ module plastic_phenopowerlaw
type(tParameters), dimension(:), allocatable, private :: param !< containers of constitutive parameters (len Ninstance) type(tParameters), dimension(:), allocatable, private :: param !< containers of constitutive parameters (len Ninstance)
type, private :: tPhenopowerlawState type, private :: tPhenopowerlawState
real(pReal), pointer, dimension(:) :: &
sumF ! ToDo: why not make a dependent state?
real(pReal), pointer, dimension(:,:) :: & real(pReal), pointer, dimension(:,:) :: &
xi_slip, & xi_slip, &
xi_twin, & xi_twin, &
@ -349,8 +347,7 @@ subroutine plastic_phenopowerlaw_init
! allocate state arrays ! allocate state arrays
NipcMyPhase = count(material_phase == p) ! number of IPCs containing my phase NipcMyPhase = count(material_phase == p) ! number of IPCs containing my phase
sizeState = size(['tau_slip ','gamma_slip']) * prm%TotalNslip & sizeState = size(['tau_slip ','gamma_slip']) * prm%TotalNslip &
+ size(['tau_twin ','gamma_twin']) * prm%TotalNtwin & + size(['tau_twin ','gamma_twin']) * prm%TotalNtwin
+ size(['sum(f) ']) ! ToDo: only needed if either twin or slip active!
sizeDotState = sizeState sizeDotState = sizeState
call material_allocatePlasticState(p,NipcMyPhase,sizeState,sizeDotState,0_pInt, & call material_allocatePlasticState(p,NipcMyPhase,sizeState,sizeDotState,0_pInt, &
@ -374,12 +371,6 @@ subroutine plastic_phenopowerlaw_init
dot%xi_twin => plasticState(p)%dotState(startIndex:endIndex,:) dot%xi_twin => plasticState(p)%dotState(startIndex:endIndex,:)
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolResistance plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolResistance
startIndex = endIndex + 1_pInt
endIndex = endIndex + 1_pInt
stt%sumF=>plasticState(p)%state (startIndex,:)
dot%sumF=>plasticState(p)%dotState(startIndex,:)
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolTwinFrac
startIndex = endIndex + 1_pInt startIndex = endIndex + 1_pInt
endIndex = endIndex + prm%totalNslip endIndex = endIndex + prm%totalNslip
stt%gamma_slip => plasticState(p)%state (startIndex:endIndex,:) stt%gamma_slip => plasticState(p)%state (startIndex:endIndex,:)
@ -439,7 +430,8 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg) call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
slipSystems: do i = 1_pInt, prm%totalNslip slipSystems: do i = 1_pInt, prm%totalNslip
Lp = Lp + (1.0_pReal-stt%sumF(of))*(gdot_slip_pos(i)+gdot_slip_neg(i))*prm%Schmid_slip(1:3,1:3,i) Lp = Lp + (1.0_pReal- sum(stt%gamma_twin(:,of)/prm%gamma_twin_char)) & ! only shear in untwinned volume
* (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) & forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) & dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ dgdot_dtauslip_pos(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_pos(m,n,i) & + dgdot_dtauslip_pos(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_pos(m,n,i) &
@ -475,8 +467,8 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
i i
real(pReal) :: & real(pReal) :: &
c_SlipSlip,c_TwinSlip,c_TwinTwin, & c_SlipSlip,c_TwinSlip,c_TwinTwin, &
xi_slip_sat_offset,sumGamma xi_slip_sat_offset,&
sumGamma,sumF
real(pReal), dimension(param(instance)%totalNslip) :: & real(pReal), dimension(param(instance)%totalNslip) :: &
left_SlipSlip,right_SlipSlip, & left_SlipSlip,right_SlipSlip, &
gdot_slip_pos,gdot_slip_neg gdot_slip_pos,gdot_slip_neg
@ -488,17 +480,18 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
dot%whole(:,of) = 0.0_pReal dot%whole(:,of) = 0.0_pReal
sumGamma = sum(stt%gamma_slip(:,of)) sumGamma = sum(stt%gamma_slip(:,of))
sumF = sum(stt%gamma_twin(:,of)/prm%gamma_twin_char)
!-------------------------------------------------------------------------------------------------- !--------------------------------------------------------------------------------------------------
! system-independent (nonlinear) prefactors to M_Xx (X influenced by x) matrices ! system-independent (nonlinear) prefactors to M_Xx (X influenced by x) matrices
c_SlipSlip = prm%h0_slipslip * (1.0_pReal + prm%twinC*stt%sumF(of)** prm%twinB) c_SlipSlip = prm%h0_slipslip * (1.0_pReal + prm%twinC*sumF** prm%twinB)
c_TwinSlip = prm%h0_TwinSlip * sumGamma**prm%twinE c_TwinSlip = prm%h0_TwinSlip * sumGamma**prm%twinE
c_TwinTwin = prm%h0_TwinTwin * stt%sumF(of)**prm%twinD c_TwinTwin = prm%h0_TwinTwin * sumF**prm%twinD
!-------------------------------------------------------------------------------------------------- !--------------------------------------------------------------------------------------------------
! calculate left and right vectors ! calculate left and right vectors
left_SlipSlip = 1.0_pReal + prm%H_int left_SlipSlip = 1.0_pReal + prm%H_int
xi_slip_sat_offset = prm%spr*sqrt(stt%sumF(of)) xi_slip_sat_offset = prm%spr*sqrt(sumF)
right_SlipSlip = abs(1.0_pReal-stt%xi_slip(:,of) / (prm%xi_slip_sat+xi_slip_sat_offset)) **prm%a_slip & right_SlipSlip = abs(1.0_pReal-stt%xi_slip(:,of) / (prm%xi_slip_sat+xi_slip_sat_offset)) **prm%a_slip &
* sign(1.0_pReal,1.0_pReal-stt%xi_slip(:,of) / (prm%xi_slip_sat+xi_slip_sat_offset)) * sign(1.0_pReal,1.0_pReal-stt%xi_slip(:,of) / (prm%xi_slip_sat+xi_slip_sat_offset))
@ -507,9 +500,6 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg) call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg)
dot%gamma_slip(:,of) = abs(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(prm,stt,of,Mp,dot%gamma_twin(:,of))
if (prm%totalNtwin > 0_pInt) dot%sumF(of) = merge(sum(dot%gamma_twin(:,of)/prm%gamma_twin_char), &
0.0_pReal, &
stt%sumF(of) < 0.98_pReal)
!-------------------------------------------------------------------------------------------------- !--------------------------------------------------------------------------------------------------
! hardening ! hardening
@ -605,7 +595,7 @@ end subroutine kinetics_slip
!-------------------------------------------------------------------------------------------------- !--------------------------------------------------------------------------------------------------
!> @brief calculates shear rates on twin systems and derivatives with respect to resolved stress !> @brief calculates shear rates on twin systems and derivatives with respect to resolved stress
!> @details: Shear rates are calculated only optionally. NOTE: Against the common convention, the !> @details: Derivates 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 !> 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(prm,stt,of,Mp,gdot_twin,dgdot_dtau_twin)
@ -637,7 +627,8 @@ pure subroutine kinetics_twin(prm,stt,of,Mp,gdot_twin,dgdot_dtau_twin)
enddo enddo
where(tau_twin > 0.0_pReal) where(tau_twin > 0.0_pReal)
gdot_twin = (1.0_pReal-stt%sumF(of))*prm%gdot0_twin*(abs(tau_twin)/stt%xi_twin(:,of))**prm%n_twin gdot_twin = (1.0_pReal-sum(stt%gamma_twin(:,of)/prm%gamma_twin_char)) & ! only twin in untwinned volume fraction
* prm%gdot0_twin*(abs(tau_twin)/stt%xi_twin(:,of))**prm%n_twin
else where else where
gdot_twin = 0.0_pReal gdot_twin = 0.0_pReal
end where end where