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DAMASK_EICMD
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not needed

This commit is contained in:
Martin Diehl 2021-07-22 00:11:16 +02:00
parent 3f7043de74
commit 85fd2e3fad
1 changed files with 18 additions and 31 deletions
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49
src/phase_mechanical_plastic_nonlocal.f90
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@ -755,11 +755,7 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
Mp
!< derivative of Lp with respect to Mp
integer :: &
ns, & !< short notation for the total number of active slip systems
i, &
j, &
k, &
l, &
i, j, k, l, &
t, & !< dislocation type
s !< index of my current slip system
real(pReal), dimension(param(ph)%sum_N_sl,8) :: &
@ -775,15 +771,13 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
tau, & !< resolved shear stress including backstress terms
dot_gamma !< shear rate
associate(prm => param(ph),dst=>microstructure(ph),&
stt=>state(ph))
ns = prm%sum_N_sl
associate(prm => param(ph),dst=>microstructure(ph),stt=>state(ph))
!*** shortcut to state variables
rho = getRho(ph,en)
rhoSgl = rho(:,sgl)
do s = 1,ns
do s = 1,prm%sum_N_sl
tau(s) = math_tensordot(Mp, prm%P_sl(1:3,1:3,s))
tauNS(s,1) = tau(s)
tauNS(s,2) = tau(s)
@ -820,14 +814,14 @@ module subroutine nonlocal_LpAndItsTangent(Lp,dLp_dMp, &
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) &
forall (s = 1:prm%sum_N_sl, t = 5:8, rhoSgl(s,t) * v(s,t-4) < 0.0_pReal) &
rhoSgl(s,t-4) = rhoSgl(s,t-4) + abs(rhoSgl(s,t))
dot_gamma = sum(rhoSgl(:,1:4) * v, 2) * prm%b_sl
Lp = 0.0_pReal
dLp_dMp = 0.0_pReal
do s = 1,ns
do s = 1,prm%sum_N_sl
Lp = Lp + dot_gamma(s) * prm%P_sl(1:3,1:3,s)
forall (i=1:3,j=1:3,k=1:3,l=1:3) &
dLp_dMp(i,j,k,l) = dLp_dMp(i,j,k,l) &
@ -855,7 +849,6 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,en)
en
integer :: &
ns, & ! short notation for the total number of active slip systems
c, & ! character of dislocation
t, & ! type of dislocation
s ! index of my current slip system
@ -875,11 +868,10 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,en)
deltaDUpper ! change in maximum stable dipole distance for edges and screws
associate(prm => param(ph),dst => microstructure(ph),del => deltaState(ph))
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),en)
forall (s = 1:ns, c = 1:2) dUpperOld(s,c) = plasticState(ph)%state(iD(s,c,ph),en)
forall (s = 1:prm%sum_N_sl, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),en)
forall (s = 1:prm%sum_N_sl, c = 1:2) dUpperOld(s,c) = plasticState(ph)%state(iD(s,c,ph),en)
rho = getRho(ph,en)
rhoDip = rho(:,dip)
@ -920,16 +912,16 @@ module subroutine plastic_nonlocal_deltaState(Mp,ph,en)
!*** dissociation by stress increase
deltaRhoDipole2SingleStress = 0.0_pReal
forall (c=1:2, s=1:ns, deltaDUpper(s,c) < 0.0_pReal .and. &
forall (c=1:2, s=1:prm%sum_N_sl, deltaDUpper(s,c) < 0.0_pReal .and. &
dNeq0(dUpperOld(s,c) - prm%minDipoleHeight(s,c))) &
deltaRhoDipole2SingleStress(s,8+c) = rhoDip(s,c) * deltaDUpper(s,c) &
/ (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),en) = dUpper(s,c)
forall (s = 1:prm%sum_N_sl, c = 1:2) plasticState(ph)%state(iD(s,c,ph),en) = dUpper(s,c)
plasticState(ph)%deltaState(:,en) = 0.0_pReal
del%rho(:,en) = reshape(deltaRhoRemobilization + deltaRhoDipole2SingleStress, [10*ns])
del%rho(:,en) = reshape(deltaRhoRemobilization + deltaRhoDipole2SingleStress, [10*prm%sum_N_sl])
end associate
@ -940,7 +932,7 @@ end subroutine plastic_nonlocal_deltaState
!> @brief calculates the rate of change of microstructure
!---------------------------------------------------------------------------------------------------
module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
ph,en,ip,el)
ph,en,ip,el)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< MandelStress
@ -954,7 +946,6 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
el !< current element number
integer :: &
ns, & !< short notation for the total number of active slip systems
c, & !< character of dislocation
t, & !< type of dislocation
s !< index of my current slip system
@ -988,11 +979,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
return
endif
associate(prm => param(ph), &
dst => microstructure(ph), &
dot => dotState(ph), &
stt => state(ph))
ns = prm%sum_N_sl
associate(prm => param(ph), dst => microstructure(ph), dot => dotState(ph), stt => state(ph))
tau = 0.0_pReal
dot_gamma = 0.0_pReal
@ -1003,13 +990,13 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
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),en)
forall (s = 1:prm%sum_N_sl, t = 1:4) v(s,t) = plasticState(ph)%state(iV(s,t,ph),en)
dot_gamma = rhoSgl(:,1:4) * v * spread(prm%b_sl,2,4)
! limits for stable dipole height
do s = 1,ns
do s = 1,prm%sum_N_sl
tau(s) = math_tensordot(Mp, prm%P_sl(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
@ -1029,7 +1016,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
! dislocation multiplication
rhoDotMultiplication = 0.0_pReal
isBCC: if (phase_lattice(ph) == 'cI') then
forall (s = 1:ns, sum(abs(v(s,1:4))) > 0.0_pReal)
forall (s = 1:prm%sum_N_sl, sum(abs(v(s,1:4))) > 0.0_pReal)
rhoDotMultiplication(s,1:2) = sum(abs(dot_gamma(s,3:4))) / prm%b_sl(s) & ! assuming double-cross-slip of screws to be decisive for multiplication
* 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
@ -1044,7 +1031,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
* sqrt(stt%rho_forest(:,en)) / prm%i_sl / prm%b_sl, 2, 4) ! eq. 3.26
endif isBCC
forall (s = 1:ns, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),en)
forall (s = 1:prm%sum_N_sl, t = 1:4) v0(s,t) = plasticState(ph)%state0(iV(s,t,ph),en)
!****************************************************************************
@ -1085,7 +1072,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
! annihilated screw dipoles leave edge jogs behind on the colinear system
if (phase_lattice(ph) == 'cF') &
forall (s = 1:ns, prm%colinearSystem(s) > 0) &
forall (s = 1:prm%sum_N_sl, prm%colinearSystem(s) > 0) &
rhoDotAthermalAnnihilation(prm%colinearSystem(s),1:2) = - rhoDotAthermalAnnihilation(s,10) &
* 0.25_pReal * sqrt(stt%rho_forest(s,en)) * (dUpper(s,2) + dLower(s,2)) * prm%f_ed
@ -1095,7 +1082,7 @@ module subroutine nonlocal_dotState(Mp, Temperature,timestep, &
D_SD = prm%D_0 * exp(-prm%Q_cl / (kB * Temperature)) ! eq. 3.53
v_climb = D_SD * prm%mu * prm%V_at &
/ (PI * (1.0_pReal-prm%nu) * (dUpper(:,1) + dLower(:,1)) * kB * Temperature) ! eq. 3.54
forall (s = 1:ns, dUpper(s,1) > dLower(s,1)) &
forall (s = 1:prm%sum_N_sl, dUpper(s,1) > dLower(s,1)) &
rhoDotThermalAnnihilation(s,9) = max(- 4.0_pReal * rhoDip(s,1) * v_climb(s) / (dUpper(s,1) - dLower(s,1)), &
- rhoDip(s,1) / timestep - rhoDotAthermalAnnihilation(s,9) &
- rhoDotSingle2DipoleGlide(s,9)) ! make sure that we do not annihilate more dipoles than we have