adopted from Viteshs branch
This commit is contained in:
parent
4340c558d7
commit
eeb5f45e88
|
@ -53,7 +53,8 @@ module plastic_dislotwin
|
|||
nu, &
|
||||
D0, & !< prefactor for self-diffusion coefficient
|
||||
Qsd, & !< activation energy for dislocation climb
|
||||
D, & !<grain size
|
||||
omega, & !< frequency factor for dislocation climb
|
||||
D, & !< grain size
|
||||
p_sb, & !< p-exponent in shear band velocity
|
||||
q_sb, & !< q-exponent in shear band velocity
|
||||
CEdgeDipMinDistance, & !<
|
||||
|
@ -104,6 +105,7 @@ module plastic_dislotwin
|
|||
integer, dimension(:,:), allocatable :: &
|
||||
fcc_twinNucleationSlipPair ! ToDo: Better name? Is also use for trans
|
||||
real(pReal), dimension(:,:), allocatable :: &
|
||||
n0_sl, & !< slip system normal
|
||||
forestProjection, &
|
||||
C66
|
||||
real(pReal), dimension(:,:,:), allocatable :: &
|
||||
|
@ -251,6 +253,8 @@ subroutine plastic_dislotwin_init
|
|||
prm%forestProjection = lattice_forestProjection (prm%N_sl,config%getString('lattice_structure'),&
|
||||
config%getFloat('c/a',defaultVal=0.0_pReal))
|
||||
|
||||
prm%n0_sl = lattice_slip_normal(prm%N_sl,config%getString('lattice_structure'),&
|
||||
config%getFloat('c/a',defaultVal=0.0_pReal))
|
||||
prm%fccTwinTransNucleation = merge(.true., .false., lattice_structure(p) == LATTICE_FCC_ID) &
|
||||
.and. (prm%N_sl(1) == 12)
|
||||
if(prm%fccTwinTransNucleation) &
|
||||
|
@ -271,7 +275,17 @@ subroutine plastic_dislotwin_init
|
|||
prm%CEdgeDipMinDistance = config%getFloat('cedgedipmindistance')
|
||||
prm%D0 = config%getFloat('d0')
|
||||
prm%Qsd = config%getFloat('qsd')
|
||||
prm%omega = config%getFloat('omega',defaultVal=1000.0_pReal)
|
||||
prm%atomicVolume = config%getFloat('catomicvolume') * prm%b_sl**3.0_pReal
|
||||
prm%SFE_0K = config%getFloat('sfe_0k',defaultVal = 0.0_pReal)
|
||||
prm%dSFE_dT = config%getFloat('dsfe_dt',defaultVal = 0.0_pReal)
|
||||
|
||||
! multiplication factor according to slip system
|
||||
if (lattice_structure(p) == LATTICE_FCC_ID .or. lattice_structure(p) == LATTICE_HEX_ID ) then
|
||||
prm%omega = prm%omega * 11.0_pReal
|
||||
else
|
||||
prm%omega = prm%omega * 8.0_pReal
|
||||
endif
|
||||
|
||||
! expand: family => system
|
||||
prm%rho_mob_0 = math_expand(prm%rho_mob_0, prm%N_sl)
|
||||
|
@ -740,8 +754,11 @@ subroutine plastic_dislotwin_dotState(Mp,T,instance,of)
|
|||
f_unrotated, &
|
||||
VacancyDiffusion, &
|
||||
rho_dip_distance, &
|
||||
v_cl, &
|
||||
tau
|
||||
v_cl, & !< climb velocity
|
||||
Gamma, & !< stacking fault energy
|
||||
tau, &
|
||||
tau_cl, & ! ToDo: MD: good name? It is not a resolved stress but a different projection
|
||||
b_d
|
||||
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
||||
dot_rho_dip_formation, &
|
||||
dot_rho_dip_climb, &
|
||||
|
@ -760,6 +777,8 @@ subroutine plastic_dislotwin_dotState(Mp,T,instance,of)
|
|||
- sum(stt%f_tr(1:prm%sum_N_tr,of))
|
||||
VacancyDiffusion = prm%D0*exp(-prm%Qsd/(kB*T))
|
||||
|
||||
Gamma = prm%SFE_0K + prm%dSFE_dT * T
|
||||
|
||||
call kinetics_slip(Mp,T,instance,of,dot_gamma_sl)
|
||||
dot%gamma_sl(:,of) = abs(dot_gamma_sl)
|
||||
|
||||
|
@ -786,8 +805,16 @@ subroutine plastic_dislotwin_dotState(Mp,T,instance,of)
|
|||
if (dEq0(rho_dip_distance-rho_dip_distance_min(i))) then
|
||||
dot_rho_dip_climb(i) = 0.0_pReal
|
||||
else
|
||||
v_cl = 3.0_pReal*prm%mu*VacancyDiffusion*prm%atomicVolume(i) &
|
||||
/ (2.0_pReal*PI*kB*T*(rho_dip_distance+rho_dip_distance_min(i)))
|
||||
tau_cl = norm2(matmul(Mp,prm%n0_sl(1:3,i))) ! ToDo: MD: correct?
|
||||
|
||||
if (prm%SFE_0K > 0.0_pReal) then ! ToDo: MD: I'm not really sure if this is correct. Maybe Gamma(0K) = 0
|
||||
b_d = 24.0_pReal*PI*(1.0_pReal - prm%nu)/(2.0_pReal + prm%nu)* Gamma/(prm%mu*prm%b_sl(i))
|
||||
else
|
||||
b_d = 1.0_pReal
|
||||
endif
|
||||
|
||||
v_cl = 2.0_pReal*prm%omega*b_d**2.0_pReal*exp(-prm%Qsd/(kB*T)) &
|
||||
* (exp(abs(tau_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,of) &
|
||||
/ (rho_dip_distance-rho_dip_distance_min(i))
|
||||
endif
|
||||
|
|
Loading…
Reference in New Issue