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DAMASK_EICMD
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consistent with new naming scheme

This commit is contained in:
Martin Diehl 2021-04-25 08:06:52 +02:00
parent 7250fbb7c6
commit d0b86f54fb
12 changed files with 325 additions and 327 deletions
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4
src/DAMASK_interface.f90
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@ -51,9 +51,7 @@ subroutine DAMASK_interface_init
#include <petsc/finclude/petscsys.h>
#if PETSC_VERSION_MAJOR!=3 || PETSC_VERSION_MINOR<PETSC_MINOR_MIN || PETSC_VERSION_MINOR>PETSC_MINOR_MAX
===================================================================================================
-- WRONG PETSc VERSION --- WRONG PETSc VERSION --- WRONG PETSc VERSION --- WRONG PETSc VERSION --
===================================================================================================
-- UNSUPPORTED PETSc VERSION --- UNSUPPORTED PETSc VERSION --- UNSUPPORTED PETSc VERSION ---
#endif
character(len=pPathLen*3+pStringLen) :: &

16
src/phase.f90
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@ -161,13 +161,13 @@ module phase
real(pReal), dimension(3,3) :: P
end function phase_P
module function thermal_T(ph,me) result(T)
integer, intent(in) :: ph,me
module function thermal_T(ph,en) result(T)
integer, intent(in) :: ph,en
real(pReal) :: T
end function thermal_T
module function thermal_dot_T(ph,me) result(dot_T)
integer, intent(in) :: ph,me
module function thermal_dot_T(ph,en) result(dot_T)
integer, intent(in) :: ph,en
real(pReal) :: dot_T
end function thermal_dot_T
@ -216,10 +216,10 @@ module phase
! == cleaned:end ===================================================================================
module function thermal_stress(Delta_t,ph,me) result(converged_)
module function thermal_stress(Delta_t,ph,en) result(converged_)
real(pReal), intent(in) :: Delta_t
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
logical :: converged_
end function thermal_stress
@ -253,8 +253,8 @@ module phase
f
end function phase_f_phi
module function phase_f_T(ph,me) result(f)
integer, intent(in) :: ph, me
module function phase_f_T(ph,en) result(f)
integer, intent(in) :: ph, en
real(pReal) :: f
end function phase_f_T

78
src/phase_mechanical_plastic.f90
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@ -37,7 +37,7 @@ submodule(phase:mechanical) plastic
myPlasticity
end function plastic_nonlocal_init
module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -46,10 +46,10 @@ submodule(phase:mechanical) plastic
Mp
integer, intent(in) :: &
ph, &
me
en
end subroutine isotropic_LpAndItsTangent
pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -58,10 +58,10 @@ submodule(phase:mechanical) plastic
Mp
integer, intent(in) :: &
ph, &
me
en
end subroutine phenopowerlaw_LpAndItsTangent
pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -70,10 +70,10 @@ submodule(phase:mechanical) plastic
Mp
integer, intent(in) :: &
ph, &
me
en
end subroutine kinehardening_LpAndItsTangent
module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -85,10 +85,10 @@ submodule(phase:mechanical) plastic
T
integer, intent(in) :: &
ph, &
me
en
end subroutine dislotwin_LpAndItsTangent
pure module subroutine dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
pure module subroutine dislotungsten_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -100,11 +100,11 @@ submodule(phase:mechanical) plastic
T
integer, intent(in) :: &
ph, &
me
en
end subroutine dislotungsten_LpAndItsTangent
module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
Mp,Temperature,ph,me)
Mp,Temperature,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -116,55 +116,55 @@ submodule(phase:mechanical) plastic
Temperature
integer, intent(in) :: &
ph, &
me
en
end subroutine nonlocal_LpAndItsTangent
module subroutine isotropic_dotState(Mp,ph,me)
module subroutine isotropic_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
end subroutine isotropic_dotState
module subroutine phenopowerlaw_dotState(Mp,ph,me)
module subroutine phenopowerlaw_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
end subroutine phenopowerlaw_dotState
module subroutine plastic_kinehardening_dotState(Mp,ph,me)
module subroutine plastic_kinehardening_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
end subroutine plastic_kinehardening_dotState
module subroutine dislotwin_dotState(Mp,T,ph,me)
module subroutine dislotwin_dotState(Mp,T,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pReal), intent(in) :: &
T
integer, intent(in) :: &
ph, &
me
en
end subroutine dislotwin_dotState
module subroutine dislotungsten_dotState(Mp,T,ph,me)
module subroutine dislotungsten_dotState(Mp,T,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pReal), intent(in) :: &
T
integer, intent(in) :: &
ph, &
me
en
end subroutine dislotungsten_dotState
module subroutine nonlocal_dotState(Mp,Temperature,timestep,ph,me,ip,el)
module subroutine nonlocal_dotState(Mp,Temperature,timestep,ph,en,ip,el)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< MandelStress
real(pReal), intent(in) :: &
@ -172,47 +172,47 @@ submodule(phase:mechanical) plastic
timestep !< substepped crystallite time increment
integer, intent(in) :: &
ph, &
me, &
en, &
ip, & !< current integration point
el !< current element number
end subroutine nonlocal_dotState
module subroutine dislotwin_dependentState(T,ph,me)
module subroutine dislotwin_dependentState(T,ph,en)
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(in) :: &
T
end subroutine dislotwin_dependentState
module subroutine dislotungsten_dependentState(ph,me)
module subroutine dislotungsten_dependentState(ph,en)
integer, intent(in) :: &
ph, &
me
en
end subroutine dislotungsten_dependentState
module subroutine nonlocal_dependentState(ph, me, ip, el)
module subroutine nonlocal_dependentState(ph, en, ip, el)
integer, intent(in) :: &
ph, &
me, &
en, &
ip, & !< current integration point
el !< current element number
end subroutine nonlocal_dependentState
module subroutine plastic_kinehardening_deltaState(Mp,ph,me)
module subroutine plastic_kinehardening_deltaState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
end subroutine plastic_kinehardening_deltaState
module subroutine plastic_nonlocal_deltaState(Mp,ph,me)
module subroutine plastic_nonlocal_deltaState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp
integer, intent(in) :: &
ph, &
me
en
end subroutine plastic_nonlocal_deltaState
end interface
@ -357,22 +357,22 @@ module subroutine plastic_dependentState(co, ip, el)
integer :: &
ph, &
me
en
ph = material_phaseAt(co,el)
me = material_phasememberAt(co,ip,el)
en = material_phasememberAt(co,ip,el)
plasticType: select case (phase_plasticity(material_phaseAt(co,el)))
case (PLASTICITY_DISLOTWIN_ID) plasticType
call dislotwin_dependentState(thermal_T(ph,me),ph,me)
call dislotwin_dependentState(thermal_T(ph,en),ph,en)
case (PLASTICITY_DISLOTUNGSTEN_ID) plasticType
call dislotungsten_dependentState(ph,me)
call dislotungsten_dependentState(ph,en)
case (PLASTICITY_NONLOCAL_ID) plasticType
call nonlocal_dependentState(ph,me,ip,el)
call nonlocal_dependentState(ph,en,ip,el)
end select plasticType

62
src/phase_mechanical_plastic_dislotungsten.f90
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@ -17,7 +17,7 @@ submodule(phase:plastic) dislotungsten
D_0 = 1.0_pReal, & !< prefactor for self-diffusion coefficient
Q_cl = 1.0_pReal !< activation energy for dislocation climb
real(pReal), allocatable, dimension(:) :: &
b_sl, & !< magnitude me Burgers vector [m]
b_sl, & !< magnitude en Burgers vector [m]
D_a, &
i_sl, & !< Adj. parameter for distance between 2 forest dislocations
f_at, & !< factor to calculate atomic volume
@ -271,7 +271,7 @@ end function plastic_dislotungsten_init
!> @brief Calculate plastic velocity gradient and its tangent.
!--------------------------------------------------------------------------------------------------
pure module subroutine dislotungsten_LpAndItsTangent(Lp,dLp_dMp, &
Mp,T,ph,me)
Mp,T,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
real(pReal), dimension(3,3,3,3), intent(out) :: &
@ -283,7 +283,7 @@ pure module subroutine dislotungsten_LpAndItsTangent(Lp,dLp_dMp, &
T !< temperature
integer, intent(in) :: &
ph, &
me
en
integer :: &
i,k,l,m,n
@ -296,7 +296,7 @@ pure module subroutine dislotungsten_LpAndItsTangent(Lp,dLp_dMp, &
associate(prm => param(ph))
call kinetics(Mp,T,ph,me,dot_gamma_pos,dot_gamma_neg,ddot_gamma_dtau_pos,ddot_gamma_dtau_neg)
call kinetics(Mp,T,ph,en,dot_gamma_pos,dot_gamma_neg,ddot_gamma_dtau_pos,ddot_gamma_dtau_neg)
do i = 1, prm%sum_N_sl
Lp = Lp + (dot_gamma_pos(i)+dot_gamma_neg(i))*prm%P_sl(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -313,7 +313,7 @@ end subroutine dislotungsten_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine dislotungsten_dotState(Mp,T,ph,me)
module subroutine dislotungsten_dotState(Mp,T,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
@ -321,7 +321,7 @@ module subroutine dislotungsten_dotState(Mp,T,ph,me)
T !< temperature
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: &
VacancyDiffusion
@ -337,11 +337,11 @@ module subroutine dislotungsten_dotState(Mp,T,ph,me)
associate(prm => param(ph), stt => state(ph),&
dot => dotState(ph), dst => dependentState(ph))
call kinetics(Mp,T,ph,me,&
call kinetics(Mp,T,ph,en,&
gdot_pos,gdot_neg, &
tau_pos_out = tau_pos,tau_neg_out = tau_neg)
dot%gamma_sl(:,me) = (gdot_pos+gdot_neg) ! ToDo: needs to be abs
dot%gamma_sl(:,en) = (gdot_pos+gdot_neg) ! ToDo: needs to be abs
VacancyDiffusion = prm%D_0*exp(-prm%Q_cl/(kB*T))
where(dEq0(tau_pos)) ! ToDo: use avg of pos and neg
@ -350,20 +350,20 @@ module subroutine dislotungsten_dotState(Mp,T,ph,me)
else where
dip_distance = math_clip(3.0_pReal*prm%mu*prm%b_sl/(16.0_pReal*PI*abs(tau_pos)), &
prm%D_a, & ! lower limit
dst%Lambda_sl(:,me)) ! upper limit
dot_rho_dip_formation = merge(2.0_pReal*dip_distance* stt%rho_mob(:,me)*abs(dot%gamma_sl(:,me))/prm%b_sl, & ! ToDo: ignore region of spontaneous annihilation
dst%Lambda_sl(:,en)) ! upper limit
dot_rho_dip_formation = merge(2.0_pReal*dip_distance* stt%rho_mob(:,en)*abs(dot%gamma_sl(:,en))/prm%b_sl, & ! ToDo: ignore region of spontaneous annihilation
0.0_pReal, &
prm%dipoleformation)
v_cl = (3.0_pReal*prm%mu*VacancyDiffusion*prm%f_at/(2.0_pReal*pi*kB*T)) &
* (1.0_pReal/(dip_distance+prm%D_a))
dot_rho_dip_climb = (4.0_pReal*v_cl*stt%rho_dip(:,me))/(dip_distance-prm%D_a) ! ToDo: Discuss with Franz: Stress dependency?
dot_rho_dip_climb = (4.0_pReal*v_cl*stt%rho_dip(:,en))/(dip_distance-prm%D_a) ! ToDo: Discuss with Franz: Stress dependency?
end where
dot%rho_mob(:,me) = abs(dot%gamma_sl(:,me))/(prm%b_sl*dst%Lambda_sl(:,me)) & ! multiplication
dot%rho_mob(:,en) = abs(dot%gamma_sl(:,en))/(prm%b_sl*dst%Lambda_sl(:,en)) & ! multiplication
- dot_rho_dip_formation &
- (2.0_pReal*prm%D_a)/prm%b_sl*stt%rho_mob(:,me)*abs(dot%gamma_sl(:,me)) ! Spontaneous annihilation of 2 single edge dislocations
dot%rho_dip(:,me) = dot_rho_dip_formation &
- (2.0_pReal*prm%D_a)/prm%b_sl*stt%rho_dip(:,me)*abs(dot%gamma_sl(:,me)) & ! Spontaneous annihilation of a single edge dislocation with a dipole constituent
- (2.0_pReal*prm%D_a)/prm%b_sl*stt%rho_mob(:,en)*abs(dot%gamma_sl(:,en)) ! Spontaneous annihilation of 2 single edge dislocations
dot%rho_dip(:,en) = dot_rho_dip_formation &
- (2.0_pReal*prm%D_a)/prm%b_sl*stt%rho_dip(:,en)*abs(dot%gamma_sl(:,en)) & ! Spontaneous annihilation of a single edge dislocation with a dipole constituent
- dot_rho_dip_climb
end associate
@ -374,22 +374,22 @@ end subroutine dislotungsten_dotState
!--------------------------------------------------------------------------------------------------
!> @brief Calculate derived quantities from state.
!--------------------------------------------------------------------------------------------------
module subroutine dislotungsten_dependentState(ph,me)
module subroutine dislotungsten_dependentState(ph,en)
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_sl) :: &
dislocationSpacing
associate(prm => param(ph), stt => state(ph),dst => dependentState(ph))
dislocationSpacing = sqrt(matmul(prm%forestProjection,stt%rho_mob(:,me)+stt%rho_dip(:,me)))
dst%threshold_stress(:,me) = prm%mu*prm%b_sl &
* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,me)+stt%rho_dip(:,me)))
dislocationSpacing = sqrt(matmul(prm%forestProjection,stt%rho_mob(:,en)+stt%rho_dip(:,en)))
dst%threshold_stress(:,en) = prm%mu*prm%b_sl &
* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,en)+stt%rho_dip(:,en)))
dst%Lambda_sl(:,me) = prm%D/(1.0_pReal+prm%D*dislocationSpacing/prm%i_sl)
dst%Lambda_sl(:,en) = prm%D/(1.0_pReal+prm%D*dislocationSpacing/prm%i_sl)
end associate
@ -438,7 +438,7 @@ end subroutine plastic_dislotungsten_results
! 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(Mp,T,ph,me, &
pure subroutine kinetics(Mp,T,ph,en, &
dot_gamma_pos,dot_gamma_neg,ddot_gamma_dtau_pos,ddot_gamma_dtau_neg,tau_pos_out,tau_neg_out)
real(pReal), dimension(3,3), intent(in) :: &
@ -447,7 +447,7 @@ pure subroutine kinetics(Mp,T,ph,me, &
T !< temperature
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(out), dimension(param(ph)%sum_N_sl) :: &
dot_gamma_pos, &
@ -478,11 +478,11 @@ pure subroutine kinetics(Mp,T,ph,me, &
if (present(tau_neg_out)) tau_neg_out = tau_neg
associate(BoltzmannRatio => prm%Q_s/(kB*T), &
dot_gamma_0 => stt%rho_mob(:,me)*prm%b_sl*prm%v_0, &
effectiveLength => dst%Lambda_sl(:,me) - prm%w)
dot_gamma_0 => stt%rho_mob(:,en)*prm%b_sl*prm%v_0, &
effectiveLength => dst%Lambda_sl(:,en) - prm%w)
significantPositiveTau: where(abs(tau_pos)-dst%threshold_stress(:,me) > tol_math_check)
StressRatio = (abs(tau_pos)-dst%threshold_stress(:,me))/prm%tau_Peierls
significantPositiveTau: where(abs(tau_pos)-dst%threshold_stress(:,en) > tol_math_check)
StressRatio = (abs(tau_pos)-dst%threshold_stress(:,en))/prm%tau_Peierls
StressRatio_p = StressRatio** prm%p
StressRatio_pminus1 = StressRatio**(prm%p-1.0_pReal)
needsGoodName = exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q)
@ -498,7 +498,7 @@ pure subroutine kinetics(Mp,T,ph,me, &
end where significantPositiveTau
if (present(ddot_gamma_dtau_pos)) then
significantPositiveTau2: where(abs(tau_pos)-dst%threshold_stress(:,me) > tol_math_check)
significantPositiveTau2: where(abs(tau_pos)-dst%threshold_stress(:,en) > tol_math_check)
dtn = -1.0_pReal * t_n * BoltzmannRatio * prm%p * prm%q * (1.0_pReal-StressRatio_p)**(prm%q - 1.0_pReal) &
* (StressRatio)**(prm%p - 1.0_pReal) / prm%tau_Peierls
dtk = -1.0_pReal * t_k / tau_pos
@ -511,8 +511,8 @@ pure subroutine kinetics(Mp,T,ph,me, &
end where significantPositiveTau2
endif
significantNegativeTau: where(abs(tau_neg)-dst%threshold_stress(:,me) > tol_math_check)
StressRatio = (abs(tau_neg)-dst%threshold_stress(:,me))/prm%tau_Peierls
significantNegativeTau: where(abs(tau_neg)-dst%threshold_stress(:,en) > tol_math_check)
StressRatio = (abs(tau_neg)-dst%threshold_stress(:,en))/prm%tau_Peierls
StressRatio_p = StressRatio** prm%p
StressRatio_pminus1 = StressRatio**(prm%p-1.0_pReal)
needsGoodName = exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q)
@ -528,7 +528,7 @@ pure subroutine kinetics(Mp,T,ph,me, &
end where significantNegativeTau
if (present(ddot_gamma_dtau_neg)) then
significantNegativeTau2: where(abs(tau_neg)-dst%threshold_stress(:,me) > tol_math_check)
significantNegativeTau2: where(abs(tau_neg)-dst%threshold_stress(:,en) > tol_math_check)
dtn = -1.0_pReal * t_n * BoltzmannRatio * prm%p * prm%q * (1.0_pReal-StressRatio_p)**(prm%q - 1.0_pReal) &
* (StressRatio)**(prm%p - 1.0_pReal) / prm%tau_Peierls
dtk = -1.0_pReal * t_k / tau_neg

122
src/phase_mechanical_plastic_dislotwin.f90
View File

@ -519,12 +519,12 @@ end function plastic_dislotwin_homogenizedC
!--------------------------------------------------------------------------------------------------
!> @brief Calculate plastic velocity gradient and its tangent.
!--------------------------------------------------------------------------------------------------
module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,en)
real(pReal), dimension(3,3), intent(out) :: Lp
real(pReal), dimension(3,3,3,3), intent(out) :: dLp_dMp
real(pReal), dimension(3,3), intent(in) :: Mp
integer, intent(in) :: ph,me
integer, intent(in) :: ph,en
real(pReal), intent(in) :: T
integer :: i,k,l,m,n
@ -565,13 +565,13 @@ module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
associate(prm => param(ph), stt => state(ph))
f_unrotated = 1.0_pReal &
- sum(stt%f_tw(1:prm%sum_N_tw,me)) &
- sum(stt%f_tr(1:prm%sum_N_tr,me))
- sum(stt%f_tw(1:prm%sum_N_tw,en)) &
- sum(stt%f_tr(1:prm%sum_N_tr,en))
Lp = 0.0_pReal
dLp_dMp = 0.0_pReal
call kinetics_slip(Mp,T,ph,me,dot_gamma_sl,ddot_gamma_dtau_slip)
call kinetics_slip(Mp,T,ph,en,dot_gamma_sl,ddot_gamma_dtau_slip)
slipContribution: do i = 1, prm%sum_N_sl
Lp = Lp + dot_gamma_sl(i)*prm%P_sl(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -579,7 +579,7 @@ module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
+ ddot_gamma_dtau_slip(i) * prm%P_sl(k,l,i) * prm%P_sl(m,n,i)
enddo slipContribution
call kinetics_twin(Mp,T,dot_gamma_sl,ph,me,dot_gamma_tw,ddot_gamma_dtau_tw)
call kinetics_twin(Mp,T,dot_gamma_sl,ph,en,dot_gamma_tw,ddot_gamma_dtau_tw)
twinContibution: do i = 1, prm%sum_N_tw
Lp = Lp + dot_gamma_tw(i)*prm%P_tw(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -587,7 +587,7 @@ module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,ph,me)
+ ddot_gamma_dtau_tw(i)* prm%P_tw(k,l,i)*prm%P_tw(m,n,i)
enddo twinContibution
call kinetics_trans(Mp,T,dot_gamma_sl,ph,me,dot_gamma_tr,ddot_gamma_dtau_tr)
call kinetics_trans(Mp,T,dot_gamma_sl,ph,en,dot_gamma_tr,ddot_gamma_dtau_tr)
transContibution: do i = 1, prm%sum_N_tr
Lp = Lp + dot_gamma_tr(i)*prm%P_tr(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -632,7 +632,7 @@ end subroutine dislotwin_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine dislotwin_dotState(Mp,T,ph,me)
module subroutine dislotwin_dotState(Mp,T,ph,en)
real(pReal), dimension(3,3), intent(in):: &
Mp !< Mandel stress
@ -640,7 +640,7 @@ module subroutine dislotwin_dotState(Mp,T,ph,me)
T !< temperature at integration point
integer, intent(in) :: &
ph, &
me
en
integer :: i
real(pReal) :: &
@ -664,11 +664,11 @@ module subroutine dislotwin_dotState(Mp,T,ph,me)
dot => dotState(ph), dst => dependentState(ph))
f_unrotated = 1.0_pReal &
- sum(stt%f_tw(1:prm%sum_N_tw,me)) &
- sum(stt%f_tr(1:prm%sum_N_tr,me))
- sum(stt%f_tw(1:prm%sum_N_tw,en)) &
- sum(stt%f_tr(1:prm%sum_N_tr,en))
call kinetics_slip(Mp,T,ph,me,dot_gamma_sl)
dot%gamma_sl(:,me) = abs(dot_gamma_sl)
call kinetics_slip(Mp,T,ph,en,dot_gamma_sl)
dot%gamma_sl(:,en) = abs(dot_gamma_sl)
rho_dip_distance_min = prm%D_a*prm%b_sl
@ -680,11 +680,11 @@ module subroutine dislotwin_dotState(Mp,T,ph,me)
dot_rho_dip_climb(i) = 0.0_pReal
else significantSlipStress
rho_dip_distance = 3.0_pReal*prm%mu*prm%b_sl(i)/(16.0_pReal*PI*abs(tau))
rho_dip_distance = math_clip(rho_dip_distance, right = dst%Lambda_sl(i,me))
rho_dip_distance = math_clip(rho_dip_distance, right = dst%Lambda_sl(i,en))
rho_dip_distance = math_clip(rho_dip_distance, left = rho_dip_distance_min(i))
dot_rho_dip_formation(i) = 2.0_pReal*(rho_dip_distance-rho_dip_distance_min(i))/prm%b_sl(i) &
* stt%rho_mob(i,me)*abs(dot_gamma_sl(i))
* stt%rho_mob(i,en)*abs(dot_gamma_sl(i))
if (dEq(rho_dip_distance,rho_dip_distance_min(i))) then
dot_rho_dip_climb(i) = 0.0_pReal
@ -698,25 +698,25 @@ module subroutine dislotwin_dotState(Mp,T,ph,me)
v_cl = 2.0_pReal*prm%omega*b_d**2.0_pReal*exp(-prm%Q_cl/(kB*T)) &
* (exp(abs(sigma_cl)*prm%b_sl(i)**3.0_pReal/(kB*T)) - 1.0_pReal)
dot_rho_dip_climb(i) = 4.0_pReal*v_cl*stt%rho_dip(i,me) &
dot_rho_dip_climb(i) = 4.0_pReal*v_cl*stt%rho_dip(i,en) &
/ (rho_dip_distance-rho_dip_distance_min(i))
endif
endif significantSlipStress
enddo slipState
dot%rho_mob(:,me) = abs(dot_gamma_sl)/(prm%b_sl*dst%Lambda_sl(:,me)) &
dot%rho_mob(:,en) = abs(dot_gamma_sl)/(prm%b_sl*dst%Lambda_sl(:,en)) &
- dot_rho_dip_formation &
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_mob(:,me)*abs(dot_gamma_sl)
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_mob(:,en)*abs(dot_gamma_sl)
dot%rho_dip(:,me) = dot_rho_dip_formation &
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_dip(:,me)*abs(dot_gamma_sl) &
dot%rho_dip(:,en) = dot_rho_dip_formation &
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_dip(:,en)*abs(dot_gamma_sl) &
- dot_rho_dip_climb
call kinetics_twin(Mp,T,dot_gamma_sl,ph,me,dot_gamma_tw)
dot%f_tw(:,me) = f_unrotated*dot_gamma_tw/prm%gamma_char
call kinetics_twin(Mp,T,dot_gamma_sl,ph,en,dot_gamma_tw)
dot%f_tw(:,en) = f_unrotated*dot_gamma_tw/prm%gamma_char
call kinetics_trans(Mp,T,dot_gamma_sl,ph,me,dot_gamma_tr)
dot%f_tr(:,me) = f_unrotated*dot_gamma_tr
call kinetics_trans(Mp,T,dot_gamma_sl,ph,en,dot_gamma_tr)
dot%f_tr(:,en) = f_unrotated*dot_gamma_tr
end associate
@ -726,11 +726,11 @@ end subroutine dislotwin_dotState
!--------------------------------------------------------------------------------------------------
!> @brief Calculate derived quantities from state.
!--------------------------------------------------------------------------------------------------
module subroutine dislotwin_dependentState(T,ph,me)
module subroutine dislotwin_dependentState(T,ph,en)
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(in) :: &
T
@ -752,50 +752,50 @@ module subroutine dislotwin_dependentState(T,ph,me)
stt => state(ph),&
dst => dependentState(ph))
sumf_tw = sum(stt%f_tw(1:prm%sum_N_tw,me))
sumf_tr = sum(stt%f_tr(1:prm%sum_N_tr,me))
sumf_tw = sum(stt%f_tw(1:prm%sum_N_tw,en))
sumf_tr = sum(stt%f_tr(1:prm%sum_N_tr,en))
Gamma = prm%Gamma_sf_0K + prm%dGamma_sf_dT * T
!* rescaled volume fraction for topology
f_over_t_tw = stt%f_tw(1:prm%sum_N_tw,me)/prm%t_tw ! this is per system ...
f_over_t_tw = stt%f_tw(1:prm%sum_N_tw,en)/prm%t_tw ! this is per system ...
f_over_t_tr = sumf_tr/prm%t_tr ! but this not
! ToDo ...Physically correct, but naming could be adjusted
inv_lambda_sl = sqrt(matmul(prm%forestProjection,stt%rho_mob(:,me)+stt%rho_dip(:,me)))/prm%i_sl
inv_lambda_sl = sqrt(matmul(prm%forestProjection,stt%rho_mob(:,en)+stt%rho_dip(:,en)))/prm%i_sl
if (prm%sum_N_tw > 0 .and. prm%sum_N_sl > 0) &
inv_lambda_sl = inv_lambda_sl + matmul(prm%h_sl_tw,f_over_t_tw)/(1.0_pReal-sumf_tw)
if (prm%sum_N_tr > 0 .and. prm%sum_N_sl > 0) &
inv_lambda_sl = inv_lambda_sl + matmul(prm%h_sl_tr,f_over_t_tr)/(1.0_pReal-sumf_tr)
dst%Lambda_sl(:,me) = prm%D / (1.0_pReal+prm%D*inv_lambda_sl)
dst%Lambda_sl(:,en) = prm%D / (1.0_pReal+prm%D*inv_lambda_sl)
inv_lambda_tw_tw = matmul(prm%h_tw_tw,f_over_t_tw)/(1.0_pReal-sumf_tw)
dst%Lambda_tw(:,me) = prm%i_tw*prm%D/(1.0_pReal+prm%D*inv_lambda_tw_tw)
dst%Lambda_tw(:,en) = prm%i_tw*prm%D/(1.0_pReal+prm%D*inv_lambda_tw_tw)
inv_lambda_tr_tr = matmul(prm%h_tr_tr,f_over_t_tr)/(1.0_pReal-sumf_tr)
dst%Lambda_tr(:,me) = prm%i_tr*prm%D/(1.0_pReal+prm%D*inv_lambda_tr_tr)
dst%Lambda_tr(:,en) = prm%i_tr*prm%D/(1.0_pReal+prm%D*inv_lambda_tr_tr)
!* threshold stress for dislocation motion
dst%tau_pass(:,me) = prm%mu*prm%b_sl* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,me)+stt%rho_dip(:,me)))
dst%tau_pass(:,en) = prm%mu*prm%b_sl* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,en)+stt%rho_dip(:,en)))
!* threshold stress for growing twin/martensite
if(prm%sum_N_tw == prm%sum_N_sl) &
dst%tau_hat_tw(:,me) = Gamma/(3.0_pReal*prm%b_tw) &
dst%tau_hat_tw(:,en) = Gamma/(3.0_pReal*prm%b_tw) &
+ 3.0_pReal*prm%b_tw*prm%mu/(prm%L_tw*prm%b_sl) ! slip Burgers here correct?
if(prm%sum_N_tr == prm%sum_N_sl) &
dst%tau_hat_tr(:,me) = Gamma/(3.0_pReal*prm%b_tr) &
dst%tau_hat_tr(:,en) = Gamma/(3.0_pReal*prm%b_tr) &
+ 3.0_pReal*prm%b_tr*prm%mu/(prm%L_tr*prm%b_sl) & ! slip Burgers here correct?
+ prm%h*prm%delta_G/ (3.0_pReal*prm%b_tr)
dst%V_tw(:,me) = (PI/4.0_pReal)*prm%t_tw*dst%Lambda_tw(:,me)**2.0_pReal
dst%V_tr(:,me) = (PI/4.0_pReal)*prm%t_tr*dst%Lambda_tr(:,me)**2.0_pReal
dst%V_tw(:,en) = (PI/4.0_pReal)*prm%t_tw*dst%Lambda_tw(:,en)**2.0_pReal
dst%V_tr(:,en) = (PI/4.0_pReal)*prm%t_tr*dst%Lambda_tr(:,en)**2.0_pReal
x0 = prm%mu*prm%b_tw**2.0_pReal/(Gamma*8.0_pReal*PI)*(2.0_pReal+prm%nu)/(1.0_pReal-prm%nu) ! ToDo: In the paper, this is the Burgers vector for slip and is the same for twin and trans
dst%tau_r_tw(:,me) = prm%mu*prm%b_tw/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%x_c_tw)+cos(pi/3.0_pReal)/x0)
dst%tau_r_tw(:,en) = prm%mu*prm%b_tw/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%x_c_tw)+cos(pi/3.0_pReal)/x0)
x0 = prm%mu*prm%b_tr**2.0_pReal/(Gamma*8.0_pReal*PI)*(2.0_pReal+prm%nu)/(1.0_pReal-prm%nu) ! ToDo: In the paper, this is the Burgers vector for slip
dst%tau_r_tr(:,me) = prm%mu*prm%b_tr/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%x_c_tr)+cos(pi/3.0_pReal)/x0)
dst%tau_r_tr(:,en) = prm%mu*prm%b_tr/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%x_c_tr)+cos(pi/3.0_pReal)/x0)
end associate
@ -860,7 +860,7 @@ end subroutine plastic_dislotwin_results
! 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(Mp,T,ph,me, &
pure subroutine kinetics_slip(Mp,T,ph,en, &
dot_gamma_sl,ddot_gamma_dtau_slip,tau_slip)
real(pReal), dimension(3,3), intent(in) :: &
@ -869,7 +869,7 @@ pure subroutine kinetics_slip(Mp,T,ph,me, &
T !< temperature
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_sl), intent(out) :: &
dot_gamma_sl
@ -898,7 +898,7 @@ pure subroutine kinetics_slip(Mp,T,ph,me, &
tau(i) = math_tensordot(Mp,prm%P_sl(1:3,1:3,i))
enddo
tau_eff = abs(tau)-dst%tau_pass(:,me)
tau_eff = abs(tau)-dst%tau_pass(:,en)
significantStress: where(tau_eff > tol_math_check)
stressRatio = tau_eff/prm%tau_0
@ -907,7 +907,7 @@ pure subroutine kinetics_slip(Mp,T,ph,me, &
v_wait_inverse = prm%v_0**(-1.0_pReal) * exp(BoltzmannRatio*(1.0_pReal-StressRatio_p)** prm%q)
v_run_inverse = prm%B/(tau_eff*prm%b_sl)
dot_gamma_sl = sign(stt%rho_mob(:,me)*prm%b_sl/(v_wait_inverse+v_run_inverse),tau)
dot_gamma_sl = sign(stt%rho_mob(:,en)*prm%b_sl/(v_wait_inverse+v_run_inverse),tau)
dV_wait_inverse_dTau = -1.0_pReal * v_wait_inverse * prm%p * prm%q * BoltzmannRatio &
* (stressRatio**(prm%p-1.0_pReal)) &
@ -916,7 +916,7 @@ pure subroutine kinetics_slip(Mp,T,ph,me, &
dV_run_inverse_dTau = -1.0_pReal * v_run_inverse/tau_eff
dV_dTau = -1.0_pReal * (dV_wait_inverse_dTau+dV_run_inverse_dTau) &
/ (v_wait_inverse+v_run_inverse)**2.0_pReal
ddot_gamma_dtau = dV_dTau*stt%rho_mob(:,me)*prm%b_sl
ddot_gamma_dtau = dV_dTau*stt%rho_mob(:,en)*prm%b_sl
else where significantStress
dot_gamma_sl = 0.0_pReal
ddot_gamma_dtau = 0.0_pReal
@ -937,7 +937,7 @@ 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(Mp,T,dot_gamma_sl,ph,me,&
pure subroutine kinetics_twin(Mp,T,dot_gamma_sl,ph,en,&
dot_gamma_tw,ddot_gamma_dtau_tw)
real(pReal), dimension(3,3), intent(in) :: &
@ -946,7 +946,7 @@ pure subroutine kinetics_twin(Mp,T,dot_gamma_sl,ph,me,&
T !< temperature
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_sl), intent(in) :: &
dot_gamma_sl
@ -970,11 +970,11 @@ pure subroutine kinetics_twin(Mp,T,dot_gamma_sl,ph,me,&
isFCC: if (prm%fccTwinTransNucleation) then
s1=prm%fcc_twinNucleationSlipPair(1,i)
s2=prm%fcc_twinNucleationSlipPair(2,i)
if (tau(i) < dst%tau_r_tw(i,me)) then ! ToDo: correct?
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,me)+stt%rho_dip(s2,me))+&
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,me)+stt%rho_dip(s1,me)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
if (tau(i) < dst%tau_r_tw(i,en)) then ! ToDo: correct?
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,en)+stt%rho_dip(s2,en))+&
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,en)+stt%rho_dip(s1,en)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
(prm%L_tw*prm%b_sl(i))*&
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tw(i,me)-tau(i)))) ! P_ncs
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tw(i,en)-tau(i)))) ! P_ncs
else
Ndot0=0.0_pReal
end if
@ -984,8 +984,8 @@ pure subroutine kinetics_twin(Mp,T,dot_gamma_sl,ph,me,&
enddo
significantStress: where(tau > tol_math_check)
StressRatio_r = (dst%tau_hat_tw(:,me)/tau)**prm%r
dot_gamma_tw = prm%gamma_char * dst%V_tw(:,me) * Ndot0*exp(-StressRatio_r)
StressRatio_r = (dst%tau_hat_tw(:,en)/tau)**prm%r
dot_gamma_tw = prm%gamma_char * dst%V_tw(:,en) * Ndot0*exp(-StressRatio_r)
ddot_gamma_dtau = (dot_gamma_tw*prm%r/tau)*StressRatio_r
else where significantStress
dot_gamma_tw = 0.0_pReal
@ -1006,7 +1006,7 @@ end subroutine kinetics_twin
! 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_trans(Mp,T,dot_gamma_sl,ph,me,&
pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,ph,en,&
dot_gamma_tr,ddot_gamma_dtau_tr)
real(pReal), dimension(3,3), intent(in) :: &
@ -1015,7 +1015,7 @@ pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,ph,me,&
T !< temperature
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_sl), intent(in) :: &
dot_gamma_sl
@ -1038,11 +1038,11 @@ pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,ph,me,&
isFCC: if (prm%fccTwinTransNucleation) then
s1=prm%fcc_twinNucleationSlipPair(1,i)
s2=prm%fcc_twinNucleationSlipPair(2,i)
if (tau(i) < dst%tau_r_tr(i,me)) then ! ToDo: correct?
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,me)+stt%rho_dip(s2,me))+&
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,me)+stt%rho_dip(s1,me)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
if (tau(i) < dst%tau_r_tr(i,en)) then ! ToDo: correct?
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,en)+stt%rho_dip(s2,en))+&
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,en)+stt%rho_dip(s1,en)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
(prm%L_tr*prm%b_sl(i))*&
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tr(i,me)-tau(i)))) ! P_ncs
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tr(i,en)-tau(i)))) ! P_ncs
else
Ndot0=0.0_pReal
end if
@ -1052,8 +1052,8 @@ pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,ph,me,&
enddo
significantStress: where(tau > tol_math_check)
StressRatio_s = (dst%tau_hat_tr(:,me)/tau)**prm%s
dot_gamma_tr = dst%V_tr(:,me) * Ndot0*exp(-StressRatio_s)
StressRatio_s = (dst%tau_hat_tr(:,en)/tau)**prm%s
dot_gamma_tr = dst%V_tr(:,en) * Ndot0*exp(-StressRatio_s)
ddot_gamma_dtau = (dot_gamma_tr*prm%s/tau)*StressRatio_s
else where significantStress
dot_gamma_tr = 0.0_pReal

22
src/phase_mechanical_plastic_isotropic.f90
View File

@ -156,7 +156,7 @@ end function plastic_isotropic_init
!--------------------------------------------------------------------------------------------------
!> @brief Calculate plastic velocity gradient and its tangent.
!--------------------------------------------------------------------------------------------------
module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
@ -167,7 +167,7 @@ module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(3,3) :: &
Mp_dev !< deviatoric part of the Mandel stress
@ -185,7 +185,7 @@ module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
norm_Mp_dev = sqrt(squarenorm_Mp_dev)
if (norm_Mp_dev > 0.0_pReal) then
dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp_dev/(prm%M*stt%xi(me))) **prm%n
dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp_dev/(prm%M*stt%xi(en))) **prm%n
Lp = dot_gamma/prm%M * Mp_dev/norm_Mp_dev
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -248,13 +248,13 @@ module subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,ph,en)
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine isotropic_dotState(Mp,ph,me)
module subroutine isotropic_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: &
dot_gamma, & !< strainrate
@ -270,7 +270,7 @@ module subroutine isotropic_dotState(Mp,ph,me)
norm_Mp = sqrt(math_tensordot(math_deviatoric33(Mp),math_deviatoric33(Mp)))
endif
dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp /(prm%M*stt%xi(me))) **prm%n
dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp /(prm%M*stt%xi(en))) **prm%n
if (dot_gamma > 1e-12_pReal) then
if (dEq0(prm%c_1)) then
@ -280,15 +280,15 @@ module subroutine isotropic_dotState(Mp,ph,me)
+ asinh( (dot_gamma / prm%c_1)**(1.0_pReal / prm%c_2))**(1.0_pReal / prm%c_3) &
/ prm%c_4 * (dot_gamma / prm%dot_gamma_0)**(1.0_pReal / prm%n)
endif
dot%xi(me) = dot_gamma &
dot%xi(en) = dot_gamma &
* ( prm%h_0 + prm%h_ln * log(dot_gamma) ) &
* abs( 1.0_pReal - stt%xi(me)/xi_inf_star )**prm%a &
* sign(1.0_pReal, 1.0_pReal - stt%xi(me)/xi_inf_star)
* abs( 1.0_pReal - stt%xi(en)/xi_inf_star )**prm%a &
* sign(1.0_pReal, 1.0_pReal - stt%xi(en)/xi_inf_star)
else
dot%xi(me) = 0.0_pReal
dot%xi(en) = 0.0_pReal
endif
dot%gamma(me) = dot_gamma ! ToDo: not really used
dot%gamma(en) = dot_gamma ! ToDo: not really used
end associate

60
src/phase_mechanical_plastic_kinehardening.f90
View File

@ -230,7 +230,7 @@ end function plastic_kinehardening_init
!--------------------------------------------------------------------------------------------------
!> @brief Calculate plastic velocity gradient and its tangent.
!--------------------------------------------------------------------------------------------------
pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
@ -241,7 +241,7 @@ pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
integer :: &
i,k,l,m,n
@ -254,7 +254,7 @@ pure module subroutine kinehardening_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
associate(prm => param(ph))
call kinetics(Mp,ph,me,gdot_pos,gdot_neg,dgdot_dtau_pos,dgdot_dtau_neg)
call kinetics(Mp,ph,en,gdot_pos,gdot_neg,dgdot_dtau_pos,dgdot_dtau_neg)
do i = 1, prm%sum_N_sl
Lp = Lp + (gdot_pos(i)+gdot_neg(i))*prm%P(1:3,1:3,i)
@ -272,13 +272,13 @@ end subroutine kinehardening_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine plastic_kinehardening_dotState(Mp,ph,me)
module subroutine plastic_kinehardening_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: &
sumGamma
@ -289,22 +289,22 @@ module subroutine plastic_kinehardening_dotState(Mp,ph,me)
associate(prm => param(ph), stt => state(ph),&
dot => dotState(ph))
call kinetics(Mp,ph,me,gdot_pos,gdot_neg)
dot%accshear(:,me) = abs(gdot_pos+gdot_neg)
sumGamma = sum(stt%accshear(:,me))
call kinetics(Mp,ph,en,gdot_pos,gdot_neg)
dot%accshear(:,en) = abs(gdot_pos+gdot_neg)
sumGamma = sum(stt%accshear(:,en))
dot%crss(:,me) = matmul(prm%interaction_SlipSlip,dot%accshear(:,me)) &
dot%crss(:,en) = matmul(prm%interaction_SlipSlip,dot%accshear(:,en)) &
* ( prm%h_inf_f &
+ (prm%h_0_f - prm%h_inf_f + prm%h_0_f*prm%h_inf_f*sumGamma/prm%xi_inf_f) &
* exp(-sumGamma*prm%h_0_f/prm%xi_inf_f) &
)
dot%crss_back(:,me) = stt%sense(:,me)*dot%accshear(:,me) * &
dot%crss_back(:,en) = stt%sense(:,en)*dot%accshear(:,en) * &
( prm%h_inf_b + &
(prm%h_0_b - prm%h_inf_b &
+ prm%h_0_b*prm%h_inf_b/(prm%xi_inf_b+stt%chi0(:,me))*(stt%accshear(:,me)-stt%gamma0(:,me))&
) *exp(-(stt%accshear(:,me)-stt%gamma0(:,me)) *prm%h_0_b/(prm%xi_inf_b+stt%chi0(:,me))) &
+ prm%h_0_b*prm%h_inf_b/(prm%xi_inf_b+stt%chi0(:,en))*(stt%accshear(:,en)-stt%gamma0(:,en))&
) *exp(-(stt%accshear(:,en)-stt%gamma0(:,en)) *prm%h_0_b/(prm%xi_inf_b+stt%chi0(:,en))) &
)
end associate
@ -315,13 +315,13 @@ end subroutine plastic_kinehardening_dotState
!--------------------------------------------------------------------------------------------------
!> @brief Calculate (instantaneous) incremental change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine plastic_kinehardening_deltaState(Mp,ph,me)
module subroutine plastic_kinehardening_deltaState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_sl) :: &
gdot_pos,gdot_neg, &
@ -329,22 +329,22 @@ module subroutine plastic_kinehardening_deltaState(Mp,ph,me)
associate(prm => param(ph), stt => state(ph), dlt => deltaState(ph))
call kinetics(Mp,ph,me,gdot_pos,gdot_neg)
sense = merge(state(ph)%sense(:,me), & ! keep existing...
call kinetics(Mp,ph,en,gdot_pos,gdot_neg)
sense = merge(state(ph)%sense(:,en), & ! keep existing...
sign(1.0_pReal,gdot_pos+gdot_neg), & ! ...or have a defined
dEq0(gdot_pos+gdot_neg,1e-10_pReal)) ! current sense of shear direction
!--------------------------------------------------------------------------------------------------
! switch in sense me shear?
where(dNeq(sense,stt%sense(:,me),0.1_pReal))
dlt%sense (:,me) = sense - stt%sense(:,me) ! switch sense
dlt%chi0 (:,me) = abs(stt%crss_back(:,me)) - stt%chi0(:,me) ! remember current backstress magnitude
dlt%gamma0(:,me) = stt%accshear(:,me) - stt%gamma0(:,me) ! remember current accumulated shear
! switch in sense en shear?
where(dNeq(sense,stt%sense(:,en),0.1_pReal))
dlt%sense (:,en) = sense - stt%sense(:,en) ! switch sense
dlt%chi0 (:,en) = abs(stt%crss_back(:,en)) - stt%chi0(:,en) ! remember current backstress magnitude
dlt%gamma0(:,en) = stt%accshear(:,en) - stt%gamma0(:,en) ! remember current accumulated shear
else where
dlt%sense (:,me) = 0.0_pReal
dlt%chi0 (:,me) = 0.0_pReal
dlt%gamma0(:,me) = 0.0_pReal
dlt%sense (:,en) = 0.0_pReal
dlt%chi0 (:,en) = 0.0_pReal
dlt%gamma0(:,en) = 0.0_pReal
end where
end associate
@ -397,14 +397,14 @@ end subroutine plastic_kinehardening_results
! 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(Mp,ph,me, &
pure subroutine kinetics(Mp,ph,en, &
gdot_pos,gdot_neg,dgdot_dtau_pos,dgdot_dtau_neg)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(out), dimension(param(ph)%sum_N_sl) :: &
gdot_pos, &
@ -421,21 +421,21 @@ pure subroutine kinetics(Mp,ph,me, &
associate(prm => param(ph), stt => state(ph))
do i = 1, prm%sum_N_sl
tau_pos(i) = math_tensordot(Mp,prm%nonSchmid_pos(1:3,1:3,i)) - stt%crss_back(i,me)
tau_neg(i) = merge(math_tensordot(Mp,prm%nonSchmid_neg(1:3,1:3,i)) - stt%crss_back(i,me), &
tau_pos(i) = math_tensordot(Mp,prm%nonSchmid_pos(1:3,1:3,i)) - stt%crss_back(i,en)
tau_neg(i) = merge(math_tensordot(Mp,prm%nonSchmid_neg(1:3,1:3,i)) - stt%crss_back(i,en), &
0.0_pReal, prm%nonSchmidActive)
enddo
where(dNeq0(tau_pos))
gdot_pos = prm%dot_gamma_0 * merge(0.5_pReal,1.0_pReal, prm%nonSchmidActive) & ! 1/2 if non-Schmid active
* sign(abs(tau_pos/stt%crss(:,me))**prm%n, tau_pos)
* sign(abs(tau_pos/stt%crss(:,en))**prm%n, tau_pos)
else where
gdot_pos = 0.0_pReal
end where
where(dNeq0(tau_neg))
gdot_neg = prm%dot_gamma_0 * 0.5_pReal & ! only used if non-Schmid active, always 1/2
* sign(abs(tau_neg/stt%crss(:,me))**prm%n, tau_neg)
* sign(abs(tau_neg/stt%crss(:,en))**prm%n, tau_neg)
else where
gdot_neg = 0.0_pReal
end where

158
src/phase_mechanical_plastic_nonlocal.f90
View File

@ -49,7 +49,7 @@ submodule(phase:plastic) nonlocal
!END DEPRECATED
real(pReal), dimension(:,:,:,:,:,:), allocatable :: &
compatibility !< slip system compatibility between me and my neighbors
compatibility !< slip system compatibility between en and my neighbors
type :: tInitialParameters !< container type for internal constitutive parameters
real(pReal) :: &
@ -558,11 +558,11 @@ end function plastic_nonlocal_init
!--------------------------------------------------------------------------------------------------
!> @brief calculates quantities characterizing the microstructure
!--------------------------------------------------------------------------------------------------
module subroutine nonlocal_dependentState(ph, me, ip, el)
module subroutine nonlocal_dependentState(ph, en, ip, el)
integer, intent(in) :: &
ph, &
me, &
en, &
ip, &
el
@ -615,9 +615,9 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
associate(prm => param(ph),dst => microstructure(ph), stt => state(ph))
rho = getRho(ph,me)
rho = getRho(ph,en)
stt%rho_forest(:,me) = matmul(prm%forestProjection_Edge, sum(abs(rho(:,edg)),2)) &
stt%rho_forest(:,en) = matmul(prm%forestProjection_Edge, sum(abs(rho(:,edg)),2)) &
+ matmul(prm%forestProjection_Screw,sum(abs(rho(:,scr)),2))
@ -627,13 +627,13 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
myInteractionMatrix = prm%h_sl_sl &
* spread(( 1.0_pReal - prm%f_F &
+ prm%f_F &
* log(0.35_pReal * prm%b_sl * sqrt(max(stt%rho_forest(:,me),prm%rho_significant))) &
* log(0.35_pReal * prm%b_sl * sqrt(max(stt%rho_forest(:,en),prm%rho_significant))) &
/ log(0.35_pReal * prm%b_sl * 1e6_pReal))** 2.0_pReal,2,prm%sum_N_sl)
else
myInteractionMatrix = prm%h_sl_sl
endif
dst%tau_pass(:,me) = prm%mu * prm%b_sl &
dst%tau_pass(:,en) = prm%mu * prm%b_sl &
* sqrt(matmul(myInteractionMatrix,sum(abs(rho),2)))
!*** calculate the dislocation stress of the neighboring excess dislocation densities
@ -643,10 +643,10 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
! ToDo: MD: this is most likely only correct for F_i = I
!#################################################################################################
rho0 = getRho0(ph,me)
rho0 = getRho0(ph,en)
if (.not. phase_localPlasticity(material_phaseAt(1,el)) .and. prm%shortRangeStressCorrection) then
invFp = math_inv33(phase_mechanical_Fp(ph)%data(1:3,1:3,me))
invFe = math_inv33(phase_mechanical_Fe(ph)%data(1:3,1:3,me))
invFp = math_inv33(phase_mechanical_Fp(ph)%data(1:3,1:3,en))
invFe = math_inv33(phase_mechanical_Fe(ph)%data(1:3,1:3,en))
rho_edg_delta = rho0(:,mob_edg_pos) - rho0(:,mob_edg_neg)
rho_scr_delta = rho0(:,mob_scr_pos) - rho0(:,mob_scr_neg)
@ -654,7 +654,7 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
rhoExcess(1,:) = rho_edg_delta
rhoExcess(2,:) = rho_scr_delta
FVsize = geom(ph)%V_0(me) ** (1.0_pReal/3.0_pReal)
FVsize = geom(ph)%V_0(en) ** (1.0_pReal/3.0_pReal)
!* loop through my neighborhood and get the connection vectors (in lattice frame) and the excess densities
@ -734,7 +734,7 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
where(rhoTotal > 0.0_pReal) rhoExcessGradient_over_rho = rhoExcessGradient / rhoTotal
! ... gives the local stress correction when multiplied with a factor
dst%tau_back(s,me) = - prm%mu * prm%b_sl(s) / (2.0_pReal * PI) &
dst%tau_back(s,en) = - prm%mu * prm%b_sl(s) / (2.0_pReal * PI) &
* ( rhoExcessGradient_over_rho(1) / (1.0_pReal - prm%nu) &
+ rhoExcessGradient_over_rho(2))
enddo
@ -745,9 +745,9 @@ module subroutine nonlocal_dependentState(ph, me, ip, el)
.and. ((debugConstitutive%element == el .and. debugConstitutive%ip == ip)&
.or. .not. debugConstitutive%selective)) then
print'(/,a,i8,1x,i2,1x,i1,/)', '<< CONST >> nonlocal_microstructure at el ip ',el,ip
print'(a,/,12x,12(e10.3,1x))', '<< CONST >> rhoForest', stt%rho_forest(:,me)
print'(a,/,12x,12(f10.5,1x))', '<< CONST >> tauThreshold / MPa', dst%tau_pass(:,me)*1e-6
print'(a,/,12x,12(f10.5,1x),/)', '<< CONST >> tauBack / MPa', dst%tau_back(:,me)*1e-6
print'(a,/,12x,12(e10.3,1x))', '<< CONST >> rhoForest', stt%rho_forest(:,en)
print'(a,/,12x,12(f10.5,1x))', '<< CONST >> tauThreshold / MPa', dst%tau_pass(:,en)*1e-6
print'(a,/,12x,12(f10.5,1x),/)', '<< CONST >> tauBack / MPa', dst%tau_back(:,en)*1e-6
endif
#endif
@ -760,14 +760,14 @@ end subroutine nonlocal_dependentState
!> @brief calculates plastic velocity gradient and its tangent
!--------------------------------------------------------------------------------------------------
module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
Mp,Temperature,ph,me)
Mp,Temperature,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
real(pReal), dimension(3,3,3,3), intent(out) :: &
dLp_dMp
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(in) :: &
Temperature !< temperature
@ -800,7 +800,7 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
ns = prm%sum_N_sl
!*** shortcut to state variables
rho = getRho(ph,me)
rho = getRho(ph,en)
rhoSgl = rho(:,sgl)
do s = 1,ns
@ -815,12 +815,12 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
tauNS(s,4) = math_tensordot(Mp, -prm%nonSchmid_pos(1:3,1:3,s))
endif
enddo
tauNS = tauNS + spread(dst%tau_back(:,me),2,4)
tau = tau + dst%tau_back(:,me)
tauNS = tauNS + spread(dst%tau_back(:,en),2,4)
tau = tau + dst%tau_back(:,en)
! edges
call kinetics(v(:,1), dv_dtau(:,1), dv_dtauNS(:,1), &
tau, tauNS(:,1), dst%tau_pass(:,me),1,Temperature, ph)
tau, tauNS(:,1), dst%tau_pass(:,en),1,Temperature, ph)
v(:,2) = v(:,1)
dv_dtau(:,2) = dv_dtau(:,1)
dv_dtauNS(:,2) = dv_dtauNS(:,1)
@ -829,7 +829,7 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
if (prm%nonSchmidActive) then
do t = 3,4
call kinetics(v(:,t), dv_dtau(:,t), dv_dtauNS(:,t), &
tau, tauNS(:,t), dst%tau_pass(:,me),2,Temperature, ph)
tau, tauNS(:,t), dst%tau_pass(:,en),2,Temperature, ph)
enddo
else
v(:,3:4) = spread(v(:,1),2,2)
@ -837,7 +837,7 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
dv_dtauNS(:,3:4) = spread(dv_dtauNS(:,1),2,2)
endif
stt%v(:,me) = pack(v,.true.)
stt%v(:,en) = pack(v,.true.)
!*** Bauschinger effect
forall (s = 1:ns, t = 5:8, rhoSgl(s,t) * v(s,t-4) < 0.0_pReal) &
@ -866,13 +866,13 @@ end subroutine nonlocal_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief (instantaneous) incremental change of microstructure
!--------------------------------------------------------------------------------------------------
module subroutine plastic_nonlocal_deltaState(Mp,ph,me)
module subroutine plastic_nonlocal_deltaState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< MandelStress
integer, intent(in) :: &
ph, &
me
en
integer :: &
ns, & ! short notation for the total number of active slip systems
@ -898,10 +898,10 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,me)
ns = prm%sum_N_sl
!*** shortcut to state variables
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),me)
forall (s = 1:ns, c = 1:2) dUpperOld(s,c) = plasticState(ph)%state(iD(s,c,ph),me)
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),en)
forall (s = 1:ns, c = 1:2) dUpperOld(s,c) = plasticState(ph)%state(iD(s,c,ph),en)
rho = getRho(ph,me)
rho = getRho(ph,en)
rhoDip = rho(:,dip)
!****************************************************************************
@ -922,7 +922,7 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,me)
!*** calculate limits for stable dipole height
do s = 1,prm%sum_N_sl
tau(s) = math_tensordot(Mp, prm%Schmid(1:3,1:3,s)) +dst%tau_back(s,me)
tau(s) = math_tensordot(Mp, prm%Schmid(1:3,1:3,s)) +dst%tau_back(s,en)
if (abs(tau(s)) < 1.0e-15_pReal) tau(s) = 1.0e-15_pReal
enddo
@ -946,10 +946,10 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,me)
/ (dUpperOld(s,c) - prm%minDipoleHeight(s,c))
forall (t=1:4) deltaRhoDipole2SingleStress(:,t) = -0.5_pReal * deltaRhoDipole2SingleStress(:,(t-1)/2+9)
forall (s = 1:ns, c = 1:2) plasticState(ph)%state(iD(s,c,ph),me) = dUpper(s,c)
forall (s = 1:ns, c = 1:2) plasticState(ph)%state(iD(s,c,ph),en) = dUpper(s,c)
plasticState(ph)%deltaState(:,me) = 0.0_pReal
del%rho(:,me) = reshape(deltaRhoRemobilization + deltaRhoDipole2SingleStress, [10*ns])
plasticState(ph)%deltaState(:,en) = 0.0_pReal
del%rho(:,en) = reshape(deltaRhoRemobilization + deltaRhoDipole2SingleStress, [10*ns])
end associate
@ -960,7 +960,7 @@ end subroutine plastic_nonlocal_deltaState
!> @brief calculates the rate of change of microstructure
!---------------------------------------------------------------------------------------------------
module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
ph,me,ip,el)
ph,en,ip,el)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< MandelStress
@ -969,7 +969,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
timestep !< substepped crystallite time increment
integer, intent(in) :: &
ph, &
me, &
en, &
ip, & !< current integration point
el !< current element number
@ -1017,13 +1017,13 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
tau = 0.0_pReal
gdot = 0.0_pReal
rho = getRho(ph,me)
rho = getRho(ph,en)
rhoSgl = rho(:,sgl)
rhoDip = rho(:,dip)
rho0 = getRho0(ph,me)
rho0 = getRho0(ph,en)
my_rhoSgl0 = rho0(:,sgl)
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),me)
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),en)
gdot = rhoSgl(:,1:4) * v * spread(prm%b_sl,2,4)
#ifdef DEBUG
@ -1038,7 +1038,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
!****************************************************************************
!*** limits for stable dipole height
do s = 1,ns
tau(s) = math_tensordot(Mp, prm%Schmid(1:3,1:3,s)) + dst%tau_back(s,me)
tau(s) = math_tensordot(Mp, prm%Schmid(1:3,1:3,s)) + dst%tau_back(s,en)
if (abs(tau(s)) < 1.0e-15_pReal) tau(s) = 1.0e-15_pReal
enddo
@ -1059,20 +1059,20 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
isBCC: if (lattice_structure(ph) == LATTICE_bcc_ID) then
forall (s = 1:ns, sum(abs(v(s,1:4))) > 0.0_pReal)
rhoDotMultiplication(s,1:2) = sum(abs(gdot(s,3:4))) / prm%b_sl(s) & ! assuming double-cross-slip of screws to be decisive for multiplication
* sqrt(stt%rho_forest(s,me)) / prm%i_sl(s) ! & ! mean free path
* sqrt(stt%rho_forest(s,en)) / prm%i_sl(s) ! & ! mean free path
! * 2.0_pReal * sum(abs(v(s,3:4))) / sum(abs(v(s,1:4))) ! ratio of screw to overall velocity determines edge generation
rhoDotMultiplication(s,3:4) = sum(abs(gdot(s,3:4))) /prm%b_sl(s) & ! assuming double-cross-slip of screws to be decisive for multiplication
* sqrt(stt%rho_forest(s,me)) / prm%i_sl(s) ! & ! mean free path
* sqrt(stt%rho_forest(s,en)) / prm%i_sl(s) ! & ! mean free path
! * 2.0_pReal * sum(abs(v(s,1:2))) / sum(abs(v(s,1:4))) ! ratio of edge to overall velocity determines screw generation
endforall
else isBCC
rhoDotMultiplication(:,1:4) = spread( &
(sum(abs(gdot(:,1:2)),2) * prm%f_ed_mult + sum(abs(gdot(:,3:4)),2)) &
* sqrt(stt%rho_forest(:,me)) / prm%i_sl / prm%b_sl, 2, 4)
* sqrt(stt%rho_forest(:,en)) / prm%i_sl / prm%b_sl, 2, 4)
endif isBCC
forall (s = 1:ns, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),me)
forall (s = 1:ns, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),en)
!****************************************************************************
@ -1115,10 +1115,10 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
if (lattice_structure(ph) == LATTICE_fcc_ID) &
forall (s = 1:ns, prm%colinearSystem(s) > 0) &
rhoDotAthermalAnnihilation(prm%colinearSystem(s),1:2) = - rhoDotAthermalAnnihilation(s,10) &
* 0.25_pReal * sqrt(stt%rho_forest(s,me)) * (dUpper(s,2) + dLower(s,2)) * prm%f_ed
* 0.25_pReal * sqrt(stt%rho_forest(s,en)) * (dUpper(s,2) + dLower(s,2)) * prm%f_ed
!*** thermally activated annihilation me edge dipoles by climb
!*** thermally activated annihilation en edge dipoles by climb
rhoDotThermalAnnihilation = 0.0_pReal
selfDiffusion = prm%D_0 * exp(-prm%Q_cl / (kB * Temperature))
vClimb = prm%V_at * selfDiffusion * prm%mu &
@ -1128,7 +1128,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
- rhoDip(s,1) / timestep - rhoDotAthermalAnnihilation(s,9) &
- rhoDotSingle2DipoleGlide(s,9)) ! make sure that we do not annihilate more dipoles than we have
rhoDot = rhoDotFlux(timestep, ph,me,ip,el) &
rhoDot = rhoDotFlux(timestep, ph,en,ip,el) &
+ rhoDotMultiplication &
+ rhoDotSingle2DipoleGlide &
+ rhoDotAthermalAnnihilation &
@ -1145,8 +1145,8 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
#endif
plasticState(ph)%dotState = IEEE_value(1.0_pReal,IEEE_quiet_NaN)
else
dot%rho(:,me) = pack(rhoDot,.true.)
dot%gamma(:,me) = sum(gdot,2)
dot%rho(:,en) = pack(rhoDot,.true.)
dot%gamma(:,en) = sum(gdot,2)
endif
end associate
@ -1157,13 +1157,13 @@ end subroutine nonlocal_dotState
!---------------------------------------------------------------------------------------------------
!> @brief calculates the rate of change of microstructure
!---------------------------------------------------------------------------------------------------
function rhoDotFlux(timestep,ph,me,ip,el)
function rhoDotFlux(timestep,ph,en,ip,el)
real(pReal), intent(in) :: &
timestep !< substepped crystallite time increment
integer, intent(in) :: &
ph, &
me, &
en, &
ip, & !< current integration point
el !< current element number
@ -1174,11 +1174,11 @@ function rhoDotFlux(timestep,ph,me,ip,el)
n, & !< index of my current neighbor
neighbor_el, & !< element number of my neighbor
neighbor_ip, & !< integration point of my neighbor
neighbor_n, & !< neighbor index pointing to me when looking from my neighbor
neighbor_n, & !< neighbor index pointing to en when looking from my neighbor
opposite_neighbor, & !< index of my opposite neighbor
opposite_ip, & !< ip of my opposite neighbor
opposite_el, & !< element index of my opposite neighbor
opposite_n, & !< neighbor index pointing to me when looking from my opposite neighbor
opposite_n, & !< neighbor index pointing to en when looking from my opposite neighbor
t, & !< type of dislocation
no,& !< neighbor offset shortcut
np,& !< neighbor phase shortcut
@ -1204,12 +1204,12 @@ function rhoDotFlux(timestep,ph,me,ip,el)
neighbor_F, & !< total deformation gradient of my neighbor
my_Fe, & !< my elastic deformation gradient
neighbor_Fe, & !< elastic deformation gradient of my neighbor
Favg !< average total deformation gradient of me and my neighbor
Favg !< average total deformation gradient of en and my neighbor
real(pReal), dimension(3) :: &
normal_neighbor2me, & !< interface normal pointing from my neighbor to me in neighbor's lattice configuration
normal_neighbor2me_defConf, & !< interface normal pointing from my neighbor to me in shared deformed configuration
normal_me2neighbor, & !< interface normal pointing from me to my neighbor in my lattice configuration
normal_me2neighbor_defConf !< interface normal pointing from me to my neighbor in shared deformed configuration
normal_neighbor2me, & !< interface normal pointing from my neighbor to en in neighbor's lattice configuration
normal_neighbor2me_defConf, & !< interface normal pointing from my neighbor to en in shared deformed configuration
normal_me2neighbor, & !< interface normal pointing from en to my neighbor in my lattice configuration
normal_me2neighbor_defConf !< interface normal pointing from en to my neighbor in shared deformed configuration
real(pReal) :: &
area, & !< area of the current interface
transmissivity, & !< overall transmissivity of dislocation flux to neighboring material point
@ -1224,16 +1224,16 @@ function rhoDotFlux(timestep,ph,me,ip,el)
gdot = 0.0_pReal
rho = getRho(ph,me)
rho = getRho(ph,en)
rhoSgl = rho(:,sgl)
rho0 = getRho0(ph,me)
rho0 = getRho0(ph,en)
my_rhoSgl0 = rho0(:,sgl)
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),me) !ToDo: MD: I think we should use state0 here
forall (s = 1:ns, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),en) !ToDo: MD: I think we should use state0 here
gdot = rhoSgl(:,1:4) * v * spread(prm%b_sl,2,4)
forall (s = 1:ns, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),me)
forall (s = 1:ns, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),en)
!****************************************************************************
!*** calculate dislocation fluxes (only for nonlocal plasticity)
@ -1268,8 +1268,8 @@ function rhoDotFlux(timestep,ph,me,ip,el)
m(1:3,:,3) = -prm%slip_transverse
m(1:3,:,4) = prm%slip_transverse
my_F = phase_mechanical_F(ph)%data(1:3,1:3,me)
my_Fe = matmul(my_F, math_inv33(phase_mechanical_Fp(ph)%data(1:3,1:3,me)))
my_F = phase_mechanical_F(ph)%data(1:3,1:3,en)
my_Fe = matmul(my_F, math_inv33(phase_mechanical_Fp(ph)%data(1:3,1:3,en)))
neighbors: do n = 1,nIPneighbors
@ -1316,7 +1316,7 @@ function rhoDotFlux(timestep,ph,me,ip,el)
.or. neighbor_rhoSgl0 < prm%rho_significant) &
neighbor_rhoSgl0 = 0.0_pReal
normal_neighbor2me_defConf = math_det33(Favg) * matmul(math_inv33(transpose(Favg)), &
IPareaNormal(1:3,neighbor_n,neighbor_ip,neighbor_el)) ! normal of the interface in (average) deformed configuration (pointing neighbor => me)
IPareaNormal(1:3,neighbor_n,neighbor_ip,neighbor_el)) ! normal of the interface in (average) deformed configuration (pointing neighbor => en)
normal_neighbor2me = matmul(transpose(neighbor_Fe), normal_neighbor2me_defConf) &
/ math_det33(neighbor_Fe) ! interface normal in the lattice configuration of my neighbor
area = IParea(neighbor_n,neighbor_ip,neighbor_el) * norm2(normal_neighbor2me)
@ -1325,7 +1325,7 @@ function rhoDotFlux(timestep,ph,me,ip,el)
do t = 1,4
c = (t + 1) / 2
topp = t + mod(t,2) - mod(t+1,2)
if (neighbor_v0(s,t) * math_inner(m(1:3,s,t), normal_neighbor2me) > 0.0_pReal & ! flux from my neighbor to me == entering flux for me
if (neighbor_v0(s,t) * math_inner(m(1:3,s,t), normal_neighbor2me) > 0.0_pReal & ! flux from my neighbor to en == entering flux for en
.and. v0(s,t) * neighbor_v0(s,t) >= 0.0_pReal ) then ! ... only if no sign change in flux density
lineLength = neighbor_rhoSgl0(s,t) * neighbor_v0(s,t) &
* math_inner(m(1:3,s,t), normal_neighbor2me) * area ! positive line length that wants to enter through this interface
@ -1344,7 +1344,7 @@ function rhoDotFlux(timestep,ph,me,ip,el)
!* FLUX FROM ME TO MY NEIGHBOR
!* This is not considered, if my opposite neighbor has a different constitutive law than nonlocal (still considered for nonlocal law with local properties).
!* Then, we assume, that the opposite(!) neighbor sends an equal amount of dislocations to me.
!* Then, we assume, that the opposite(!) neighbor sends an equal amount of dislocations to en.
!* So the net flux in the direction of my neighbor is equal to zero:
!* leaving flux to neighbor == entering flux from opposite neighbor
!* In case of reduced transmissivity, part of the leaving flux is stored as dead dislocation density.
@ -1353,7 +1353,7 @@ function rhoDotFlux(timestep,ph,me,ip,el)
if (phase_plasticity(material_phaseAt(1,opposite_el)) == PLASTICITY_NONLOCAL_ID) then
normal_me2neighbor_defConf = math_det33(Favg) &
* matmul(math_inv33(transpose(Favg)),IPareaNormal(1:3,n,ip,el)) ! normal of the interface in (average) deformed configuration (pointing me => neighbor)
* matmul(math_inv33(transpose(Favg)),IPareaNormal(1:3,n,ip,el)) ! normal of the interface in (average) deformed configuration (pointing en => neighbor)
normal_me2neighbor = matmul(transpose(my_Fe), normal_me2neighbor_defConf) &
/ math_det33(my_Fe) ! interface normal in my lattice configuration
area = IParea(n,ip,el) * norm2(normal_me2neighbor)
@ -1361,7 +1361,7 @@ function rhoDotFlux(timestep,ph,me,ip,el)
do s = 1,ns
do t = 1,4
c = (t + 1) / 2
if (v0(s,t) * math_inner(m(1:3,s,t), normal_me2neighbor) > 0.0_pReal ) then ! flux from me to my neighbor == leaving flux for me (might also be a pure flux from my mobile density to dead density if interface not at all transmissive)
if (v0(s,t) * math_inner(m(1:3,s,t), normal_me2neighbor) > 0.0_pReal ) then ! flux from en to my neighbor == leaving flux for en (might also be a pure flux from my mobile density to dead density if interface not at all transmissive)
if (v0(s,t) * neighbor_v0(s,t) >= 0.0_pReal) then ! no sign change in flux density
transmissivity = sum(compatibility(c,:,s,n,ip,el)**2.0_pReal) ! overall transmissivity from this slip system to my neighbor
else ! sign change in flux density means sign change in stress which does not allow for dislocations to arive at the neighbor
@ -1403,13 +1403,13 @@ module subroutine plastic_nonlocal_updateCompatibility(orientation,ph,i,e)
integer :: &
n, & ! neighbor index
me, &
en, &
neighbor_e, & ! element index of my neighbor
neighbor_i, & ! integration point index of my neighbor
neighbor_me, &
neighbor_phase, &
ns, & ! number of active slip systems
s1, & ! slip system index (me)
s1, & ! slip system index (en)
s2 ! slip system index (my neighbor)
real(pReal), dimension(2,param(ph)%sum_N_sl,param(ph)%sum_N_sl,nIPneighbors) :: &
my_compatibility ! my_compatibility for current element and ip
@ -1424,7 +1424,7 @@ module subroutine plastic_nonlocal_updateCompatibility(orientation,ph,i,e)
associate(prm => param(ph))
ns = prm%sum_N_sl
me = material_phaseMemberAt(1,i,e)
en = material_phaseMemberAt(1,i,e)
!*** start out fully compatible
my_compatibility = 0.0_pReal
forall(s1 = 1:ns) my_compatibility(:,s1,s1,:) = 1.0_pReal
@ -1450,7 +1450,7 @@ module subroutine plastic_nonlocal_updateCompatibility(orientation,ph,i,e)
elseif (prm%chi_GB >= 0.0_pReal) then
!* GRAIN BOUNDARY !
!* fixed transmissivity for adjacent ips with different texture (only if explicitly given in material.config)
if (any(dNeq(material_orientation0(1,ph,me)%asQuaternion(), &
if (any(dNeq(material_orientation0(1,ph,en)%asQuaternion(), &
material_orientation0(1,neighbor_phase,neighbor_me)%asQuaternion())) .and. &
(.not. phase_localPlasticity(neighbor_phase))) &
forall(s1 = 1:ns) my_compatibility(:,s1,s1,n) = sqrt(prm%chi_GB)
@ -1767,21 +1767,21 @@ end subroutine kinetics
!> @brief returns copy of current dislocation densities from state
!> @details raw values is rectified
!--------------------------------------------------------------------------------------------------
pure function getRho(ph,me)
pure function getRho(ph,en)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal), dimension(param(ph)%sum_N_sl,10) :: getRho
associate(prm => param(ph))
getRho = reshape(state(ph)%rho(:,me),[prm%sum_N_sl,10])
getRho = reshape(state(ph)%rho(:,en),[prm%sum_N_sl,10])
! ensure positive densities (not for imm, they have a sign)
getRho(:,mob) = max(getRho(:,mob),0.0_pReal)
getRho(:,dip) = max(getRho(:,dip),0.0_pReal)
where(abs(getRho) < max(prm%rho_min/geom(ph)%V_0(me)**(2.0_pReal/3.0_pReal),prm%rho_significant)) &
where(abs(getRho) < max(prm%rho_min/geom(ph)%V_0(en)**(2.0_pReal/3.0_pReal),prm%rho_significant)) &
getRho = 0.0_pReal
end associate
@ -1793,21 +1793,21 @@ end function getRho
!> @brief returns copy of current dislocation densities from state
!> @details raw values is rectified
!--------------------------------------------------------------------------------------------------
pure function getRho0(ph,me)
pure function getRho0(ph,en)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal), dimension(param(ph)%sum_N_sl,10) :: getRho0
associate(prm => param(ph))
getRho0 = reshape(state0(ph)%rho(:,me),[prm%sum_N_sl,10])
getRho0 = reshape(state0(ph)%rho(:,en),[prm%sum_N_sl,10])
! ensure positive densities (not for imm, they have a sign)
getRho0(:,mob) = max(getRho0(:,mob),0.0_pReal)
getRho0(:,dip) = max(getRho0(:,dip),0.0_pReal)
where (abs(getRho0) < max(prm%rho_min/geom(ph)%V_0(me)**(2.0_pReal/3.0_pReal),prm%rho_significant)) &
where (abs(getRho0) < max(prm%rho_min/geom(ph)%V_0(en)**(2.0_pReal/3.0_pReal),prm%rho_significant)) &
getRho0 = 0.0_pReal
end associate

52
src/phase_mechanical_plastic_phenopowerlaw.f90
View File

@ -283,7 +283,7 @@ end function plastic_phenopowerlaw_init
!> @details asummes that deformation by dislocation glide affects twinned and untwinned volume
! equally (Taylor assumption). Twinning happens only in untwinned volume
!--------------------------------------------------------------------------------------------------
pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
@ -294,7 +294,7 @@ pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
integer :: &
i,k,l,m,n
@ -309,7 +309,7 @@ pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
associate(prm => param(ph))
call kinetics_slip(Mp,ph,me,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
call kinetics_slip(Mp,ph,en,gdot_slip_pos,gdot_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg)
slipSystems: do i = 1, prm%sum_N_sl
Lp = Lp + (gdot_slip_pos(i)+gdot_slip_neg(i))*prm%P_sl(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -318,7 +318,7 @@ pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,me)
+ dgdot_dtauslip_neg(i) * prm%P_sl(k,l,i) * prm%nonSchmid_neg(m,n,i)
enddo slipSystems
call kinetics_twin(Mp,ph,me,gdot_twin,dgdot_dtautwin)
call kinetics_twin(Mp,ph,en,gdot_twin,dgdot_dtautwin)
twinSystems: do i = 1, prm%sum_N_tw
Lp = Lp + gdot_twin(i)*prm%P_tw(1:3,1:3,i)
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
@ -334,13 +334,13 @@ end subroutine phenopowerlaw_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine phenopowerlaw_dotState(Mp,ph,me)
module subroutine phenopowerlaw_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: &
c_SlipSlip,c_TwinSlip,c_TwinTwin, &
@ -353,8 +353,8 @@ module subroutine phenopowerlaw_dotState(Mp,ph,me)
associate(prm => param(ph), stt => state(ph), &
dot => dotState(ph))
sumGamma = sum(stt%gamma_slip(:,me))
sumF = sum(stt%gamma_twin(:,me)/prm%gamma_char)
sumGamma = sum(stt%gamma_slip(:,en))
sumF = sum(stt%gamma_twin(:,en)/prm%gamma_char)
!--------------------------------------------------------------------------------------------------
! system-independent (nonlinear) prefactors to M_Xx (X influenced by x) matrices
@ -366,23 +366,23 @@ module subroutine phenopowerlaw_dotState(Mp,ph,me)
! calculate left and right vectors
left_SlipSlip = 1.0_pReal + prm%h_int
xi_slip_sat_offset = prm%f_sat_sl_tw*sqrt(sumF)
right_SlipSlip = abs(1.0_pReal-stt%xi_slip(:,me) / (prm%xi_inf_sl+xi_slip_sat_offset)) **prm%a_sl &
* sign(1.0_pReal,1.0_pReal-stt%xi_slip(:,me) / (prm%xi_inf_sl+xi_slip_sat_offset))
right_SlipSlip = abs(1.0_pReal-stt%xi_slip(:,en) / (prm%xi_inf_sl+xi_slip_sat_offset)) **prm%a_sl &
* sign(1.0_pReal,1.0_pReal-stt%xi_slip(:,en) / (prm%xi_inf_sl+xi_slip_sat_offset))
!--------------------------------------------------------------------------------------------------
! shear rates
call kinetics_slip(Mp,ph,me,gdot_slip_pos,gdot_slip_neg)
dot%gamma_slip(:,me) = abs(gdot_slip_pos+gdot_slip_neg)
call kinetics_twin(Mp,ph,me,dot%gamma_twin(:,me))
call kinetics_slip(Mp,ph,en,gdot_slip_pos,gdot_slip_neg)
dot%gamma_slip(:,en) = abs(gdot_slip_pos+gdot_slip_neg)
call kinetics_twin(Mp,ph,en,dot%gamma_twin(:,en))
!--------------------------------------------------------------------------------------------------
! hardening
dot%xi_slip(:,me) = c_SlipSlip * left_SlipSlip * &
matmul(prm%h_sl_sl,dot%gamma_slip(:,me)*right_SlipSlip) &
+ matmul(prm%h_sl_tw,dot%gamma_twin(:,me))
dot%xi_slip(:,en) = c_SlipSlip * left_SlipSlip * &
matmul(prm%h_sl_sl,dot%gamma_slip(:,en)*right_SlipSlip) &
+ matmul(prm%h_sl_tw,dot%gamma_twin(:,en))
dot%xi_twin(:,me) = c_TwinSlip * matmul(prm%h_tw_sl,dot%gamma_slip(:,me)) &
+ c_TwinTwin * matmul(prm%h_tw_tw,dot%gamma_twin(:,me))
dot%xi_twin(:,en) = c_TwinSlip * matmul(prm%h_tw_sl,dot%gamma_slip(:,en)) &
+ c_TwinTwin * matmul(prm%h_tw_tw,dot%gamma_twin(:,en))
end associate
end subroutine phenopowerlaw_dotState
@ -430,14 +430,14 @@ end subroutine plastic_phenopowerlaw_results
! 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(Mp,ph,me, &
pure subroutine kinetics_slip(Mp,ph,en, &
gdot_slip_pos,gdot_slip_neg,dgdot_dtau_slip_pos,dgdot_dtau_slip_neg)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal), intent(out), dimension(param(ph)%sum_N_sl) :: &
gdot_slip_pos, &
@ -461,14 +461,14 @@ pure subroutine kinetics_slip(Mp,ph,me, &
where(dNeq0(tau_slip_pos))
gdot_slip_pos = prm%dot_gamma_0_sl * merge(0.5_pReal,1.0_pReal, prm%nonSchmidActive) & ! 1/2 if non-Schmid active
* sign(abs(tau_slip_pos/stt%xi_slip(:,me))**prm%n_sl, tau_slip_pos)
* sign(abs(tau_slip_pos/stt%xi_slip(:,en))**prm%n_sl, tau_slip_pos)
else where
gdot_slip_pos = 0.0_pReal
end where
where(dNeq0(tau_slip_neg))
gdot_slip_neg = prm%dot_gamma_0_sl * 0.5_pReal & ! only used if non-Schmid active, always 1/2
* sign(abs(tau_slip_neg/stt%xi_slip(:,me))**prm%n_sl, tau_slip_neg)
* sign(abs(tau_slip_neg/stt%xi_slip(:,en))**prm%n_sl, tau_slip_neg)
else where
gdot_slip_neg = 0.0_pReal
end where
@ -499,14 +499,14 @@ 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(Mp,ph,me,&
pure subroutine kinetics_twin(Mp,ph,en,&
gdot_twin,dgdot_dtau_twin)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
me
en
real(pReal), dimension(param(ph)%sum_N_tw), intent(out) :: &
gdot_twin
@ -524,8 +524,8 @@ pure subroutine kinetics_twin(Mp,ph,me,&
enddo
where(tau_twin > 0.0_pReal)
gdot_twin = (1.0_pReal-sum(stt%gamma_twin(:,me)/prm%gamma_char)) & ! only twin in untwinned volume fraction
* prm%dot_gamma_0_tw*(abs(tau_twin)/stt%xi_twin(:,me))**prm%n_tw
gdot_twin = (1.0_pReal-sum(stt%gamma_twin(:,en)/prm%gamma_char)) & ! only twin in untwinned volume fraction
* prm%dot_gamma_0_tw*(abs(tau_twin)/stt%xi_twin(:,en))**prm%n_tw
else where
gdot_twin = 0.0_pReal
end where

58
src/phase_thermal.f90
View File

@ -26,7 +26,7 @@ submodule(phase) thermal
integer(kind(THERMAL_UNDEFINED_ID)), dimension(:,:), allocatable :: &
thermal_source
type(tDataContainer), dimension(:), allocatable :: current ! ?? not very telling name. Better: "field" ?? MD: current(ho)%T(me) reads quite good
type(tDataContainer), dimension(:), allocatable :: current ! ?? not very telling name. Better: "field" ?? MD: current(ho)%T(en) reads quite good
type(tThermalParameters), dimension(:), allocatable :: param
@ -46,23 +46,23 @@ submodule(phase) thermal
end function externalheat_init
module subroutine externalheat_dotState(ph, me)
module subroutine externalheat_dotState(ph, en)
integer, intent(in) :: &
ph, &
me
en
end subroutine externalheat_dotState
module function dissipation_f_T(ph,me) result(f_T)
module function dissipation_f_T(ph,en) result(f_T)
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: f_T
end function dissipation_f_T
module function externalheat_f_T(ph,me) result(f_T)
module function externalheat_f_T(ph,en) result(f_T)
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: f_T
end function externalheat_f_T
@ -137,9 +137,9 @@ end subroutine thermal_init
!----------------------------------------------------------------------------------------------
!< @brief calculates thermal dissipation rate
!----------------------------------------------------------------------------------------------
module function phase_f_T(ph,me) result(f)
module function phase_f_T(ph,en) result(f)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal) :: f
@ -152,10 +152,10 @@ module function phase_f_T(ph,me) result(f)
select case(thermal_source(so,ph))
case (THERMAL_DISSIPATION_ID)
f = f + dissipation_f_T(ph,me)
f = f + dissipation_f_T(ph,en)
case (THERMAL_EXTERNALHEAT_ID)
f = f + externalheat_f_T(ph,me)
f = f + externalheat_f_T(ph,en)
end select
@ -167,9 +167,9 @@ end function phase_f_T
!--------------------------------------------------------------------------------------------------
!> @brief contains the constitutive equation for calculating the rate of change of microstructure
!--------------------------------------------------------------------------------------------------
function phase_thermal_collectDotState(ph,me) result(broken)
function phase_thermal_collectDotState(ph,en) result(broken)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
logical :: broken
integer :: i
@ -180,9 +180,9 @@ function phase_thermal_collectDotState(ph,me) result(broken)
SourceLoop: do i = 1, thermal_Nsources(ph)
if (thermal_source(i,ph) == THERMAL_EXTERNALHEAT_ID) &
call externalheat_dotState(ph,me)
call externalheat_dotState(ph,en)
broken = broken .or. any(IEEE_is_NaN(thermalState(ph)%p(i)%dotState(:,me)))
broken = broken .or. any(IEEE_is_NaN(thermalState(ph)%p(i)%dotState(:,en)))
enddo SourceLoop
@ -218,14 +218,14 @@ module function phase_K_T(co,ce) result(K)
end function phase_K_T
module function thermal_stress(Delta_t,ph,me) result(converged_) ! ?? why is this called "stress" when it seems closer to "updateState" ??
module function thermal_stress(Delta_t,ph,en) result(converged_) ! ?? why is this called "stress" when it seems closer to "updateState" ??
real(pReal), intent(in) :: Delta_t
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
logical :: converged_
converged_ = .not. integrateThermalState(Delta_t,ph,me)
converged_ = .not. integrateThermalState(Delta_t,ph,en)
end function thermal_stress
@ -233,10 +233,10 @@ end function thermal_stress
!--------------------------------------------------------------------------------------------------
!> @brief integrate state with 1st order explicit Euler method
!--------------------------------------------------------------------------------------------------
function integrateThermalState(Delta_t, ph,me) result(broken)
function integrateThermalState(Delta_t, ph,en) result(broken)
real(pReal), intent(in) :: Delta_t
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
logical :: &
broken
@ -244,13 +244,13 @@ function integrateThermalState(Delta_t, ph,me) result(broken)
so, &
sizeDotState
broken = phase_thermal_collectDotState(ph,me)
broken = phase_thermal_collectDotState(ph,en)
if (broken) return
do so = 1, thermal_Nsources(ph)
sizeDotState = thermalState(ph)%p(so)%sizeDotState
thermalState(ph)%p(so)%state(1:sizeDotState,me) = thermalState(ph)%p(so)%state0(1:sizeDotState,me) &
+ thermalState(ph)%p(so)%dotState(1:sizeDotState,me) * Delta_t
thermalState(ph)%p(so)%state(1:sizeDotState,en) = thermalState(ph)%p(so)%state0(1:sizeDotState,en) &
+ thermalState(ph)%p(so)%dotState(1:sizeDotState,en) * Delta_t
enddo
end function integrateThermalState
@ -273,13 +273,13 @@ end subroutine thermal_forward
!----------------------------------------------------------------------------------------------
!< @brief Get temperature (for use by non-thermal physics)
!----------------------------------------------------------------------------------------------
module function thermal_T(ph,me) result(T)
module function thermal_T(ph,en) result(T)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal) :: T
T = current(ph)%T(me)
T = current(ph)%T(en)
end function thermal_T
@ -287,13 +287,13 @@ end function thermal_T
!----------------------------------------------------------------------------------------------
!< @brief Get rate of temperature (for use by non-thermal physics)
!----------------------------------------------------------------------------------------------
module function thermal_dot_T(ph,me) result(dot_T)
module function thermal_dot_T(ph,en) result(dot_T)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal) :: dot_T
dot_T = current(ph)%dot_T(me)
dot_T = current(ph)%dot_T(en)
end function thermal_dot_T

6
src/phase_thermal_dissipation.f90
View File

@ -69,15 +69,15 @@ end function dissipation_init
!--------------------------------------------------------------------------------------------------
!> @brief Ninstancess dissipation rate
!--------------------------------------------------------------------------------------------------
module function dissipation_f_T(ph,me) result(f_T)
module function dissipation_f_T(ph,en) result(f_T)
integer, intent(in) :: ph, me
integer, intent(in) :: ph, en
real(pReal) :: &
f_T
associate(prm => param(ph))
f_T = prm%kappa*sum(abs(mechanical_S(ph,me)*mechanical_L_p(ph,me)))
f_T = prm%kappa*sum(abs(mechanical_S(ph,en)*mechanical_L_p(ph,en)))
end associate
end function dissipation_f_T

14
src/phase_thermal_externalheat.f90
View File

@ -81,18 +81,18 @@ end function externalheat_init
!> @brief rate of change of state
!> @details state only contains current time to linearly interpolate given heat powers
!--------------------------------------------------------------------------------------------------
module subroutine externalheat_dotState(ph, me)
module subroutine externalheat_dotState(ph, en)
integer, intent(in) :: &
ph, &
me
en
integer :: &
so
so = source_thermal_externalheat_offset(ph)
thermalState(ph)%p(so)%dotState(1,me) = 1.0_pReal ! state is current time
thermalState(ph)%p(so)%dotState(1,en) = 1.0_pReal ! state is current time
end subroutine externalheat_dotState
@ -100,11 +100,11 @@ end subroutine externalheat_dotState
!--------------------------------------------------------------------------------------------------
!> @brief returns local heat generation rate
!--------------------------------------------------------------------------------------------------
module function externalheat_f_T(ph,me) result(f_T)
module function externalheat_f_T(ph,en) result(f_T)
integer, intent(in) :: &
ph, &
me
en
real(pReal) :: &
f_T
@ -117,14 +117,14 @@ module function externalheat_f_T(ph,me) result(f_T)
associate(prm => param(ph))
do interval = 1, prm%nIntervals ! scan through all rate segments
frac_time = (thermalState(ph)%p(so)%state(1,me) - prm%t_n(interval)) &
frac_time = (thermalState(ph)%p(so)%state(1,en) - prm%t_n(interval)) &
/ (prm%t_n(interval+1) - prm%t_n(interval)) ! fractional time within segment
if ( (frac_time < 0.0_pReal .and. interval == 1) &
.or. (frac_time >= 1.0_pReal .and. interval == prm%nIntervals) &
.or. (frac_time >= 0.0_pReal .and. frac_time < 1.0_pReal) ) &
f_T = prm%f_T(interval ) * (1.0_pReal - frac_time) + &
prm%f_T(interval+1) * frac_time ! interpolate heat rate between segment boundaries...
! ...or extrapolate if outside me bounds
! ...or extrapolate if outside of bounds
enddo
end associate