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DAMASK_EICMD
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naming reflect change from Piola-Kirchhoff to Mandel stress 

not using the symmetrized stress anymore to avoid handling of
symmetrized Schmid matrizes. The time saved when calculating the double
contraction is probably anyway lost during the conversion from (3,3) to
(6) of Mstar
This commit is contained in:
Martin Diehl 2018-08-03 14:53:40 +02:00
parent 0a6bde70c5
commit 5cf2973715
2 changed files with 39 additions and 27 deletions
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8
src/constitutive.f90
View File

@ -482,7 +482,8 @@ subroutine constitutive_LpAndItsTangent(Lp, dLp_dTstar3333, dLp_dFi3333, Tstar_v
real(pReal), dimension(9,9) :: &
dLp_dMstar !< derivative of Lp with respect to Mstar (4th-order tensor)
real(pReal), dimension(3,3) :: &
temp_33
temp_33, &
Mstar
integer(pInt) :: &
ho, & !< homogenization
tme !< thermal member position
@ -492,7 +493,8 @@ subroutine constitutive_LpAndItsTangent(Lp, dLp_dTstar3333, dLp_dFi3333, Tstar_v
ho = material_homog(ip,el)
tme = thermalMapping(ho)%p(ip,el)
Mstar_v = math_Mandel33to6(math_mul33x33(math_mul33x33(transpose(Fi),Fi),math_Mandel6to33(Tstar_v)))
Mstar = math_mul33x33(math_mul33x33(transpose(Fi),Fi),math_Mandel6to33(Tstar_v))
Mstar_v = math_Mandel33to6(Mstar)
plasticityType: select case (phase_plasticity(material_phase(ipc,ip,el)))
case (PLASTICITY_NONE_ID) plasticityType
@ -501,7 +503,7 @@ subroutine constitutive_LpAndItsTangent(Lp, dLp_dTstar3333, dLp_dFi3333, Tstar_v
case (PLASTICITY_ISOTROPIC_ID) plasticityType
call plastic_isotropic_LpAndItsTangent (Lp,dLp_dMstar,Mstar_v,ipc,ip,el)
case (PLASTICITY_PHENOPOWERLAW_ID) plasticityType
call plastic_phenopowerlaw_LpAndItsTangent (Lp,dLp_dMstar,Mstar_v,ipc,ip,el)
call plastic_phenopowerlaw_LpAndItsTangent (Lp,dLp_dMstar,Mstar,ipc,ip,el)
case (PLASTICITY_KINEHARDENING_ID) plasticityType
call plastic_kinehardening_LpAndItsTangent (Lp,dLp_dMstar,Mstar_v,ipc,ip,el)
case (PLASTICITY_NONLOCAL_ID) plasticityType

58
src/plastic_phenopowerlaw.f90
View File

@ -320,7 +320,7 @@ subroutine plastic_phenopowerlaw_init
!--------------------------------------------------------------------------------------------------
! 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 ','accshear_slip']) * prm%TotalNslip &
+ size(['tau_twin ','accshear_twin']) * prm%TotalNtwin &
+ size(['sum(gamma)', 'sum(f) '])
@ -357,6 +357,16 @@ subroutine plastic_phenopowerlaw_init
index_myFamily = sum(prm%Nslip(1:f-1_pInt))
mySlipSystems: do j = 1_pInt,prm%Nslip(f)
!prm%Schmid_pos(1:3,1:3,index_myFamily+j) = lattice_Sslip(1:3,1:3,1,index_myFamily+j,p)
!prm%Schmid_neg(1:3,1:3,index_myFamily+j) = lattice_Sslip(1:3,1:3,2,index_myFamily+j,p)
!do k = 1,size(prm%nonSchmidCoeff)
! prm%nonSchmid_pos(1:3,1:3,k,index_myFamily+j) = lattice_Sslip(1:3,1:3,2*k, index_myFamily+j,p)
! prm%nonSchmid_neg(1:3,1:3,k,index_myFamily+j) = lattice_Sslip(1:3,1:3,2*k+1,index_myFamily+j,p)
! !nonSchmid_tensor(1:3,1:3,1) = nonSchmid_tensor(1:3,1:3,1) + prm%nonSchmidCoeff(k)*&
! ! lattice_Sslip(1:3,1:3,2*k,index_myFamily+i,ph)
! !nonSchmid_tensor(1:3,1:3,2) = nonSchmid_tensor(1:3,1:3,2) + prm%nonSchmidCoeff(k)*&
! ! lattice_Sslip(1:3,1:3,2*k+1,index_myFamily+i,ph)
!enddo
otherSlipFamilies: do o = 1_pInt,size(prm%Nslip,1)
index_otherFamily = sum(prm%Nslip(1:o-1_pInt))
otherSlipSystems: do k = 1_pInt,prm%Nslip(o)
@ -467,17 +477,16 @@ end subroutine plastic_phenopowerlaw_init
!--------------------------------------------------------------------------------------------------
!> @brief calculates plastic velocity gradient and its tangent
!--------------------------------------------------------------------------------------------------
subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,el)
subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dMstar99,Mstar,ipc,ip,el)
use prec, only: &
dNeq0
use math, only: &
math_mul33xx33,&
math_Plain3333to99, &
math_Mandel6to33
use lattice, only: &
lattice_Sslip, &
lattice_Sslip_v, &
lattice_Stwin, &
lattice_Stwin_v, &
lattice_NslipSystem, &
lattice_NtwinSystem
use material, only: &
@ -488,15 +497,15 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
implicit none
real(pReal), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
real(pReal), dimension(9,9), intent(out) :: &
dLp_dTstar99 !< derivative of Lp with respect to 2nd Piola Kirchhoff stress
real(pReal), dimension(9,9), intent(out) :: &
dLp_dMstar99 !< derivative of Lp with respect to the Mandel stress
integer(pInt), intent(in) :: &
ipc, & !< component-ID of integration point
ip, & !< integration point
el !< element
real(pReal), dimension(6), intent(in) :: &
Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
real(pReal), dimension(3,3), intent(in) :: &
Mstar !< Mandel stress
integer(pInt) :: &
index_myFamily, &
@ -509,7 +518,7 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
dgdot_dtauslip_pos,dgdot_dtauslip_neg, &
gdot_twin,dgdot_dtautwin,tau_twin
real(pReal), dimension(3,3,3,3) :: &
dLp_dTstar3333 !< derivative of Lp with respect to Tstar as 4th order tensor
dLp_dMstar3333 !< derivative of Lp with respect to Mstar as 4th order tensor
real(pReal), dimension(3,3,2) :: &
nonSchmid_tensor
type(tParameters) :: prm
@ -518,30 +527,31 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
of = phasememberAt(ipc,ip,el)
ph = material_phase(ipc,ip,el)
associate(prm => param(phase_plasticityInstance(ph)), stt => state(phase_plasticityInstance(ph)))
associate(prm => param(phase_plasticityInstance(ph)),&
stt => state(phase_plasticityInstance(ph)))
Lp = 0.0_pReal
dLp_dTstar3333 = 0.0_pReal
dLp_dTstar99 = 0.0_pReal
dLp_dMstar3333 = 0.0_pReal
dLp_dMstar99 = 0.0_pReal
!--------------------------------------------------------------------------------------------------
! Slip part
j = 0_pInt
slipFamilies: do f = 1_pInt,size(prm%Nslip,1)
index_myFamily = sum(lattice_NslipSystem(1:f-1_pInt,ph)) ! at which index starts my family
index_myFamily = sum(lattice_NslipSystem(1:f-1_pInt,ph)) ! at which index starts my family
slipSystems: do i = 1_pInt,prm%Nslip(f)
j = j+1_pInt
! Calculation of Lp
tau_slip_pos = dot_product(Tstar_v,lattice_Sslip_v(1:6,1,index_myFamily+i,ph))
tau_slip_pos = math_mul33xx33(Mstar,lattice_Sslip(1:3,1:3,1,index_myFamily+i,ph))
tau_slip_neg = tau_slip_pos
nonSchmid_tensor(1:3,1:3,1) = lattice_Sslip(1:3,1:3,1,index_myFamily+i,ph)
nonSchmid_tensor(1:3,1:3,2) = nonSchmid_tensor(1:3,1:3,1)
do k = 1,size(prm%nonSchmidCoeff)
tau_slip_pos = tau_slip_pos + prm%nonSchmidCoeff(k)* &
dot_product(Tstar_v,lattice_Sslip_v(1:6,2*k,index_myFamily+i,ph))
math_mul33xx33(Mstar,lattice_Sslip(1:3,1:3,2*k,index_myFamily+i,ph))
tau_slip_neg = tau_slip_neg + prm%nonSchmidCoeff(k)* &
dot_product(Tstar_v,lattice_Sslip_v(1:6,2*k+1,index_myFamily+i,ph))
math_mul33xx33(Mstar,lattice_Sslip(1:3,1:3,2*k+1,index_myFamily+i,ph))
nonSchmid_tensor(1:3,1:3,1) = nonSchmid_tensor(1:3,1:3,1) + prm%nonSchmidCoeff(k)*&
lattice_Sslip(1:3,1:3,2*k,index_myFamily+i,ph)
nonSchmid_tensor(1:3,1:3,2) = nonSchmid_tensor(1:3,1:3,2) + prm%nonSchmidCoeff(k)*&
@ -560,7 +570,7 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
if (dNeq0(tau_slip_pos)) then
dgdot_dtauslip_pos = gdot_slip_pos*prm%n_slip/tau_slip_pos
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
dLp_dTstar3333(k,l,m,n) = dLp_dTstar3333(k,l,m,n) + &
dLp_dMstar3333(k,l,m,n) = dLp_dMstar3333(k,l,m,n) + &
dgdot_dtauslip_pos*lattice_Sslip(k,l,1,index_myFamily+i,ph)* &
nonSchmid_tensor(m,n,1)
endif
@ -568,7 +578,7 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
if (dNeq0(tau_slip_neg)) then
dgdot_dtauslip_neg = gdot_slip_neg*prm%n_slip/tau_slip_neg
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
dLp_dTstar3333(k,l,m,n) = dLp_dTstar3333(k,l,m,n) + &
dLp_dMstar3333(k,l,m,n) = dLp_dMstar3333(k,l,m,n) + &
dgdot_dtauslip_neg*lattice_Sslip(k,l,1,index_myFamily+i,ph)* &
nonSchmid_tensor(m,n,2)
endif
@ -584,7 +594,7 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
j = j+1_pInt
! Calculation of Lp
tau_twin = dot_product(Tstar_v,lattice_Stwin_v(1:6,index_myFamily+i,ph))
tau_twin = math_mul33xx33(Mstar,lattice_Stwin(1:3,1:3,index_myFamily+i,ph))
gdot_twin = (1.0_pReal-stt%sumF(of))*prm%gdot0_twin*&
(abs(tau_twin)/stt%s_twin(j,of))**&
prm%n_twin*max(0.0_pReal,sign(1.0_pReal,tau_twin))
@ -594,14 +604,14 @@ subroutine plastic_phenopowerlaw_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,ipc,ip,
if (dNeq0(gdot_twin)) then
dgdot_dtautwin = gdot_twin*prm%n_twin/tau_twin
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
dLp_dTstar3333(k,l,m,n) = dLp_dTstar3333(k,l,m,n) + &
dLp_dMstar3333(k,l,m,n) = dLp_dMstar3333(k,l,m,n) + &
dgdot_dtautwin*lattice_Stwin(k,l,index_myFamily+i,ph)* &
lattice_Stwin(m,n,index_myFamily+i,ph)
endif
enddo twinSystems
enddo twinFamilies
dLp_dTstar99 = math_Plain3333to99(dLp_dTstar3333)
dLp_dMstar99 = math_Plain3333to99(dLp_dMstar3333)
end associate
end subroutine plastic_phenopowerlaw_LpAndItsTangent
@ -650,9 +660,9 @@ subroutine plastic_phenopowerlaw_dotState(Tstar_v,ipc,ip,el)
of = phasememberAt(ipc,ip,el)
ph = material_phase(ipc,ip,el)
associate( prm => param(phase_plasticityInstance(ph)), &
stt => state(phase_plasticityInstance(ph)), &
dst => dotState(phase_plasticityInstance(ph)))
associate(prm => param(phase_plasticityInstance(ph)), &
stt => state(phase_plasticityInstance(ph)), &
dst => dotState(phase_plasticityInstance(ph)))
dst%whole(:,of) = 0.0_pReal