IMPORTANT Behavior change: Slip (Lp) happens in twinned volume fraction
aliases for associate do not have to be defined
This commit is contained in:
Martin Diehl
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cf4a0a69fd
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2aa6b12126
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@ -148,12 +148,6 @@ subroutine plastic_phenopowerlaw_init
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real(pReal), dimension(0), parameter :: emptyRealArray = [real(pReal)::]
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character(len=65536), dimension(0), parameter :: emptyStringArray = [character(len=65536)::]
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type(tParameters) :: &
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prm
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type(tPhenopowerlawState) :: &
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stt, &
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dot
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integer(kind(undefined_ID)) :: &
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outputID !< ID of each post result output
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@ -398,6 +392,8 @@ end subroutine plastic_phenopowerlaw_init
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates plastic velocity gradient and its tangent
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!> @details asumme that deformation by dislocation glide affects twinned and untwinned volume
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! equally (Taylor assumption). Twinning happens only in untwinned volume (
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!--------------------------------------------------------------------------------------------------
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subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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@ -421,18 +417,14 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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real(pReal), dimension(param(instance)%totalNtwin) :: &
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gdot_twin,dgdot_dtautwin
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type(tParameters) :: prm
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type(tPhenopowerlawState) :: stt
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associate(prm => param(instance), stt => state(instance))
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Lp = 0.0_pReal
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dLp_dMp = 0.0_pReal
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associate(prm => param(instance), stt => state(instance))
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call kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
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slipSystems: do i = 1_pInt, prm%totalNslip
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Lp = Lp + (1.0_pReal- sum(stt%gamma_twin(:,of)/prm%gamma_twin_char)) & ! only shear in untwinned volume
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* (gdot_slip_pos(i)+gdot_slip_neg(i))*prm%Schmid_slip(1:3,1:3,i)
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Lp = Lp + (gdot_slip_pos(i)+gdot_slip_neg(i))*prm%Schmid_slip(1:3,1:3,i)
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forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
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dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
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+ dgdot_dtauslip_pos(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_pos(m,n,i) &
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@ -446,8 +438,8 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,instance,of)
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dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
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+ dgdot_dtautwin(i)*prm%Schmid_twin(k,l,i)*prm%Schmid_twin(m,n,i)
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enddo twinSystems
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end associate
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end associate
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end subroutine plastic_phenopowerlaw_LpAndItsTangent
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@ -474,9 +466,6 @@ subroutine plastic_phenopowerlaw_dotState(Mp,instance,of)
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left_SlipSlip,right_SlipSlip, &
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gdot_slip_pos,gdot_slip_neg
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type(tParameters) :: prm
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type(tPhenopowerlawState) :: dot,stt
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associate(prm => param(instance), stt => state(instance), dot => dotState(instance))
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dot%whole(:,of) = 0.0_pReal
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@ -522,8 +511,9 @@ end subroutine plastic_phenopowerlaw_dotState
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates shear rates on slip systems and derivatives with respect to resolved stress
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!> @details: Shear rates are calculated only optionally. NOTE: Against the common convention, the
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!> result (i.e. intent(out)) variables are the last to have the optional arguments at the end
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!> @details Shear rates are calculated only optionally.
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! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
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! have the optional arguments at the end
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_slip(prm,stt,of,Mp,gdot_slip_pos,gdot_slip_neg, &
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dgdot_dtau_slip_pos,dgdot_dtau_slip_neg)
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@ -595,9 +585,11 @@ end subroutine kinetics_slip
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates shear rates on twin systems and derivatives with respect to resolved stress
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!> @details: Derivates are calculated only optionally. NOTE: Against the common convention, the
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!> result (i.e. intent(out)) variables are the last to have the optional arguments at the end
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!> @brief calculates shear rates on twin systems and derivatives with respect to resolved stress.
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! twinning is assumed to take place only in untwinned volume.
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!> @details Derivates are calculated only optionally.
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! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
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! have the optional arguments at the end.
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_twin(prm,stt,of,Mp,gdot_twin,dgdot_dtau_twin)
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use prec, only: &
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@ -667,14 +659,11 @@ function plastic_phenopowerlaw_postResults(Mp,instance,of) result(postResults)
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real(pReal), dimension(param(instance)%totalNslip) :: &
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gdot_slip_pos,gdot_slip_neg
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type(tParameters) :: prm
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type(tPhenopowerlawState) :: stt
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associate( prm => param(instance), stt => state(instance))
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postResults = 0.0_pReal
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c = 0_pInt
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associate( prm => param(instance), stt => state(instance))
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outputsLoop: do o = 1_pInt,size(prm%outputID)
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select case(prm%outputID(o))
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@ -711,6 +700,7 @@ function plastic_phenopowerlaw_postResults(Mp,instance,of) result(postResults)
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end select
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enddo outputsLoop
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end associate
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end function plastic_phenopowerlaw_postResults
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