DAMASK_EICMD/src/phase_mechanical_plastic_di...

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!--------------------------------------------------------------------------------------------------
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
!> @author Su Leen Wong, Max-Planck-Institut für Eisenforschung GmbH
!> @author Nan Jia, Max-Planck-Institut für Eisenforschung GmbH
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @brief material subroutine incoprorating dislocation and twinning physics
!> @details to be done
!--------------------------------------------------------------------------------------------------
submodule(phase:plastic) dislotwin
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real(pREAL), parameter :: gamma_char_tr = sqrt(0.125_pREAL) !< Characteristic shear for transformation
type :: tParameters
real(pREAL) :: &
Q_cl = 1.0_pREAL, & !< activation energy for dislocation climb
omega = 1.0_pREAL, & !< frequency factor for dislocation climb
D = 1.0_pREAL, & !< grain size
p_sb = 1.0_pREAL, & !< p-exponent in shear band velocity
q_sb = 1.0_pREAL, & !< q-exponent in shear band velocity
i_tw = 1.0_pREAL, & !< adjustment parameter to calculate MFP for twinning
i_tr = 1.0_pREAL, & !< adjustment parameter to calculate MFP for transformation
L_tw = 1.0_pREAL, & !< length of twin nuclei
L_tr = 1.0_pREAL, & !< length of trans nuclei
x_c = 1.0_pREAL, & !< critical distance for formation of twin/trans nucleus
V_cs = 1.0_pREAL, & !< cross slip volume
tau_sb = 1.0_pREAL, & !< value for shearband resistance
gamma_0_sb = 1.0_pREAL, & !< value for shearband velocity_0
E_sb = 1.0_pREAL, & !< activation energy for shear bands
h = 1.0_pREAL, & !< stack height of hex nucleus
cOverA_hP = 1.0_pREAL, &
V_mol = 1.0_pREAL, &
rho = 1.0_pREAL
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type(tPolynomial) :: &
Gamma_sf, & !< stacking fault energy
Delta_G !< free energy difference between austensite and martensite
real(pREAL), allocatable, dimension(:) :: &
b_sl, & !< magnitude of Burgers vector (m) for each slip system
b_tw, & !< magnitude of Burgers vector (m) for each twin system
b_tr, & !< magnitude of Burgers vector (m) for each transformation system
Q_sl,& !< activation energy for glide (J) for each slip system
v_0, & !< dislocation velocity prefactor (m/s) for each slip system
dot_N_0_tw, & !< twin nucleation rate (1/m³s) for each twin system
t_tw, & !< twin thickness (m) for each twin system
i_sl, & !< Adj. parameter for distance between 2 forest dislocations for each slip system
t_tr, & !< martensite lamellar thickness (m) for each trans system
p, & !< p-exponent in glide velocity
q, & !< q-exponent in glide velocity
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r, & !< exponent in twin nucleation rate
s, & !< exponent in trans nucleation rate
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tau_0, & !< strength due to elements in solid solution
gamma_char_tw, & !< characteristic shear for twins
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B, & !< drag coefficient
d_caron !< distance of spontaneous annhihilation
real(pREAL), allocatable, dimension(:,:) :: &
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h_sl_sl, & !< components of slip-slip interaction matrix
h_sl_tw, & !< components of slip-twin interaction matrix
h_sl_tr, & !< components of slip-trans interaction matrix
h_tw_tw, & !< components of twin-twin interaction matrix
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h_tr_tr, & !< components of trans-trans interaction matrix
n0_sl, & !< slip system normal
forestProjection
real(pREAL), allocatable, dimension(:,:,:) :: &
P_sl, &
P_tw, &
P_tr
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integer :: &
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sum_N_sl, & !< total number of active slip systems
sum_N_tw, & !< total number of active twin systems
sum_N_tr !< total number of active transformation systems
integer, allocatable, dimension(:) :: &
N_tw, &
N_tr
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integer, allocatable, dimension(:,:) :: &
fcc_twinNucleationSlipPair ! ToDo: Better name? Is also used for trans
character(len=:), allocatable :: &
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crystal_tr, &
isotropic_bound
character(len=pSTRLEN), allocatable, dimension(:) :: &
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output
logical :: &
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extendedDislocations, & !< consider split into partials for climb calculation
fccTwinTransNucleation, & !< twinning and transformation models are for fcc
omitDipoles !< flag controlling consideration of dipole formation
character(len=:), allocatable, dimension(:) :: &
systems_sl, &
systems_tw
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end type tParameters !< container type for internal constitutive parameters
type :: tIndexDotState
integer, dimension(2) :: &
rho_mob, &
rho_dip, &
gamma_sl, &
f_tw, &
f_tr
end type tIndexDotState
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type :: tDislotwinState
real(pREAL), dimension(:,:), pointer :: &
rho_mob, &
rho_dip, &
gamma_sl, &
f_tw, &
f_tr
end type tDislotwinState
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type :: tDislotwinDependentState
real(pREAL), dimension(:,:), allocatable :: &
Lambda_sl, & !< mean free path between 2 obstacles seen by a moving dislocation
Lambda_tw, & !< mean free path between 2 obstacles seen by a growing twin
Lambda_tr, & !< mean free path between 2 obstacles seen by a growing martensite
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tau_pass !< threshold stress for slip
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end type tDislotwinDependentState
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!--------------------------------------------------------------------------------------------------
! containers for parameters and state
type(tParameters), allocatable, dimension(:) :: param
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type(tIndexDotState), allocatable, dimension(:) :: indexDotState
type(tDislotwinState), allocatable, dimension(:) :: state
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type(tDislotwinDependentState), allocatable, dimension(:) :: dependentState
contains
!--------------------------------------------------------------------------------------------------
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!> @brief Perform module initialization.
!> @details reads in material parameters, allocates arrays, and does sanity checks
!--------------------------------------------------------------------------------------------------
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module function plastic_dislotwin_init() result(myPlasticity)
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logical, dimension(:), allocatable :: myPlasticity
integer :: &
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ph, i, &
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Nmembers, &
sizeState, sizeDotState, &
startIndex, endIndex
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integer, dimension(:), allocatable :: &
N_sl
real(pREAL) :: a_cF
real(pREAL), allocatable, dimension(:) :: &
f_edge, & !< edge character fraction of total dislocation density
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rho_mob_0, & !< initial unipolar dislocation density per slip system
rho_dip_0 !< initial dipole dislocation density per slip system
character(len=:), allocatable :: &
refs, &
extmsg
type(tDict), pointer :: &
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phases, &
phase, &
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mech, &
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pl
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myPlasticity = plastic_active('dislotwin')
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if (count(myPlasticity) == 0) return
print'(/,1x,a)', '<<<+- phase:mechanical:plastic:dislotwin init -+>>>'
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print'(/,1x,a)', 'A. Ma and F. Roters, Acta Materialia 52(12):36033612, 2004'
print'( 1x,a)', 'https://doi.org/10.1016/j.actamat.2004.04.012'
print'(/,1x,a)', 'F. Roters et al., Computational Materials Science 39:9195, 2007'
print'( 1x,a)', 'https://doi.org/10.1016/j.commatsci.2006.04.014'
print'(/,1x,a)', 'S.L. Wong et al., Acta Materialia 118:140151, 2016'
print'( 1x,a)', 'https://doi.org/10.1016/j.actamat.2016.07.032'
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print'(/,1x,a,1x,i0)', '# phases:',count(myPlasticity); flush(IO_STDOUT)
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phases => config_material%get_dict('phase')
allocate(param(phases%length))
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allocate(indexDotState(phases%length))
allocate(state(phases%length))
allocate(dependentState(phases%length))
extmsg = ''
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do ph = 1, phases%length
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if (.not. myPlasticity(ph)) cycle
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associate(prm => param(ph), &
stt => state(ph), dst => dependentState(ph), &
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idx_dot => indexDotState(ph))
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phase => phases%get_dict(ph)
mech => phase%get_dict('mechanical')
pl => mech%get_dict('plastic')
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print'(/,1x,a,1x,i0,a)', 'phase',ph,': '//phases%key(ph)
refs = config_listReferences(pl,indent=3)
if (len(refs) > 0) print'(/,1x,a)', refs
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#if defined (__GFORTRAN__)
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prm%output = output_as1dStr(pl)
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#else
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prm%output = pl%get_as1dStr('output',defaultVal=emptyStrArray)
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#endif
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prm%isotropic_bound = pl%get_asStr('isotropic_bound',defaultVal='isostrain')
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!--------------------------------------------------------------------------------------------------
! slip related parameters
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N_sl = pl%get_as1dInt('N_sl',defaultVal=emptyIntArray)
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prm%sum_N_sl = sum(abs(N_sl))
slipActive: if (prm%sum_N_sl > 0) then
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prm%systems_sl = crystal_labels_slip(N_sl,phase_lattice(ph))
prm%P_sl = crystal_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph))
prm%n0_sl = crystal_slip_normal(N_sl,phase_lattice(ph),phase_cOverA(ph))
prm%extendedDislocations = pl%get_asBool('extend_dislocations',defaultVal=.false.)
prm%omitDipoles = pl%get_asBool('omit_dipoles', defaultVal=.false.)
prm%Q_cl = pl%get_asReal('Q_cl')
f_edge = math_expand(pl%get_as1dReal('f_edge', requiredSize=size(N_sl), &
defaultVal=[(0.5_pREAL,i=1,size(N_sl))]),N_sl)
rho_mob_0 = math_expand(pl%get_as1dReal('rho_mob_0', requiredSize=size(N_sl)),N_sl)
rho_dip_0 = math_expand(pl%get_as1dReal('rho_dip_0', requiredSize=size(N_sl)),N_sl)
prm%v_0 = math_expand(pl%get_as1dReal('v_0', requiredSize=size(N_sl)),N_sl)
prm%b_sl = math_expand(pl%get_as1dReal('b_sl', requiredSize=size(N_sl)),N_sl)
prm%Q_sl = math_expand(pl%get_as1dReal('Q_sl', requiredSize=size(N_sl)),N_sl)
prm%i_sl = math_expand(pl%get_as1dReal('i_sl', requiredSize=size(N_sl)),N_sl)
prm%p = math_expand(pl%get_as1dReal('p_sl', requiredSize=size(N_sl)),N_sl)
prm%q = math_expand(pl%get_as1dReal('q_sl', requiredSize=size(N_sl)),N_sl)
prm%tau_0 = math_expand(pl%get_as1dReal('tau_0', requiredSize=size(N_sl)),N_sl)
prm%B = math_expand(pl%get_as1dReal('B', requiredSize=size(N_sl), &
defaultVal=[(0.0_pREAL,i=1,size(N_sl))]),N_sl)
prm%d_caron = prm%b_sl * pl%get_asReal('D_a')
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prm%h_sl_sl = crystal_interaction_SlipBySlip(N_sl,pl%get_as1dReal('h_sl-sl'),phase_lattice(ph))
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prm%forestProjection = spread( f_edge,1,prm%sum_N_sl) &
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* crystal_forestProjection_edge (N_sl,phase_lattice(ph),phase_cOverA(ph)) &
+ spread(1.0_pREAL-f_edge,1,prm%sum_N_sl) &
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* crystal_forestProjection_screw(N_sl,phase_lattice(ph),phase_cOverA(ph))
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prm%fccTwinTransNucleation = phase_lattice(ph) == 'cF' .and. N_sl(1) == 12
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if (prm%fccTwinTransNucleation) prm%fcc_twinNucleationSlipPair = crystal_CF_TWINNUCLEATIONSLIPPAIR
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! multiplication factor according to crystal structure (nearest neighbors bcc vs fcc/hex)
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! details: Argon & Moffat, Acta Metallurgica, Vol. 29, pg 293 to 299, 1981
prm%omega = pl%get_asReal('omega', defaultVal=1000.0_pREAL) &
* merge(12.0_pREAL,8.0_pREAL,any(phase_lattice(ph) == ['cF','hP']))
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! sanity checks
if ( prm%Q_cl <= 0.0_pREAL) extmsg = trim(extmsg)//' Q_cl'
if (any(rho_mob_0 < 0.0_pREAL)) extmsg = trim(extmsg)//' rho_mob_0'
if (any(rho_dip_0 < 0.0_pREAL)) extmsg = trim(extmsg)//' rho_dip_0'
if (any(prm%v_0 < 0.0_pREAL)) extmsg = trim(extmsg)//' v_0'
if (any(prm%b_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' b_sl'
if (any(prm%Q_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' Q_sl'
if (any(prm%i_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' i_sl'
if (any(prm%B < 0.0_pREAL)) extmsg = trim(extmsg)//' B'
if (any(prm%d_caron < 0.0_pREAL)) extmsg = trim(extmsg)//' d_caron(D_a,b_sl)'
if (any(prm%p<=0.0_pREAL .or. prm%p>1.0_pREAL)) extmsg = trim(extmsg)//' p_sl'
if (any(prm%q< 1.0_pREAL .or. prm%q>2.0_pREAL)) extmsg = trim(extmsg)//' q_sl'
else slipActive
rho_mob_0 = emptyRealArray
rho_dip_0 = emptyRealArray
allocate(prm%v_0, &
prm%b_sl, &
prm%Q_sl, &
prm%i_sl, &
prm%p, &
prm%q, &
prm%tau_0, &
prm%B, &
source=emptyRealArray)
allocate(prm%forestProjection(0,0), &
prm%h_sl_sl(0,0)) ! PE: What about P_sl and systems_sl?
end if slipActive
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!--------------------------------------------------------------------------------------------------
! twin related parameters
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prm%N_tw = pl%get_as1dInt('N_tw', defaultVal=emptyIntArray)
prm%sum_N_tw = sum(abs(prm%N_tw))
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twinActive: if (prm%sum_N_tw > 0) then
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prm%systems_tw = crystal_labels_twin(prm%N_tw,phase_lattice(ph))
prm%P_tw = crystal_SchmidMatrix_twin(prm%N_tw,phase_lattice(ph),phase_cOverA(ph))
prm%gamma_char_tw = crystal_characteristicShear_Twin(prm%N_tw,phase_lattice(ph),phase_cOverA(ph))
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prm%L_tw = pl%get_asReal('L_tw')
prm%i_tw = pl%get_asReal('i_tw')
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prm%b_tw = math_expand(pl%get_as1dReal('b_tw', requiredSize=size(prm%N_tw)),prm%N_tw)
prm%t_tw = math_expand(pl%get_as1dReal('t_tw', requiredSize=size(prm%N_tw)),prm%N_tw)
prm%r = math_expand(pl%get_as1dReal('p_tw', requiredSize=size(prm%N_tw)),prm%N_tw)
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prm%h_tw_tw = crystal_interaction_TwinByTwin(prm%N_tw,pl%get_as1dReal('h_tw-tw'), &
phase_lattice(ph))
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! sanity checks
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if (.not. prm%fccTwinTransNucleation) extmsg = trim(extmsg)//' TWIP for non-fcc'
if ( prm%L_tw < 0.0_pREAL) extmsg = trim(extmsg)//' L_tw'
if ( prm%i_tw < 0.0_pREAL) extmsg = trim(extmsg)//' i_tw'
if (any(prm%b_tw < 0.0_pREAL)) extmsg = trim(extmsg)//' b_tw'
if (any(prm%t_tw < 0.0_pREAL)) extmsg = trim(extmsg)//' t_tw'
if (any(prm%r < 0.0_pREAL)) extmsg = trim(extmsg)//' p_tw'
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else twinActive
allocate(prm%gamma_char_tw, &
prm%b_tw, &
prm%t_tw, &
prm%r, &
source=emptyRealArray)
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allocate(prm%h_tw_tw(0,0))
end if twinActive
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!--------------------------------------------------------------------------------------------------
! transformation related parameters
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prm%N_tr = pl%get_as1dInt('N_tr', defaultVal=emptyIntArray)
prm%sum_N_tr = sum(abs(prm%N_tr))
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transActive: if (prm%sum_N_tr > 0) then
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prm%P_tr = crystal_SchmidMatrix_trans(prm%N_tr,'hP',prm%cOverA_hP)
prm%Delta_G = polynomial(pl,'Delta_G','T')
prm%i_tr = pl%get_asReal('i_tr')
prm%L_tr = pl%get_asReal('L_tr')
prm%cOverA_hP = pl%get_asReal('c/a_hP')
prm%V_mol = pl%get_asReal('V_mol')
prm%b_tr = math_expand(pl%get_as1dReal('b_tr'),prm%N_tr)
prm%t_tr = math_expand(pl%get_as1dReal('t_tr'),prm%N_tr)
prm%s = math_expand(pl%get_as1dReal('p_tr'),prm%N_tr)
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a_cF = prm%b_tr(1)*sqrt(6.0_pREAL) ! b_tr is Shockley partial
prm%h = 5.0_pREAL * a_cF/sqrt(3.0_pREAL)
prm%rho = 4.0_pREAL/(sqrt(3.0_pREAL)*a_cF**2)/N_A
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prm%h_tr_tr = crystal_interaction_TransByTrans(prm%N_tr,pl%get_as1dReal('h_tr-tr'),&
phase_lattice(ph))
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! sanity checks
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if (.not. prm%fccTwinTransNucleation) extmsg = trim(extmsg)//' TRIP for non-fcc'
if ( prm%L_tr < 0.0_pREAL) extmsg = trim(extmsg)//' L_tr'
if ( prm%V_mol < 0.0_pREAL) extmsg = trim(extmsg)//' V_mol'
if ( prm%i_tr < 0.0_pREAL) extmsg = trim(extmsg)//' i_tr'
if (any(prm%t_tr < 0.0_pREAL)) extmsg = trim(extmsg)//' t_tr'
if (any(prm%s < 0.0_pREAL)) extmsg = trim(extmsg)//' p_tr'
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else transActive
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allocate(prm%s,prm%b_tr,prm%t_tr,source=emptyRealArray)
allocate(prm%h_tr_tr(0,0))
end if transActive
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!--------------------------------------------------------------------------------------------------
! shearband related parameters
prm%gamma_0_sb = pl%get_asReal('gamma_0_sb',defaultVal=0.0_pREAL)
if (prm%gamma_0_sb > 0.0_pREAL) then
prm%tau_sb = pl%get_asReal('tau_sb')
prm%E_sb = pl%get_asReal('Q_sb')
prm%p_sb = pl%get_asReal('p_sb')
prm%q_sb = pl%get_asReal('q_sb')
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! sanity checks
if (prm%tau_sb < 0.0_pREAL) extmsg = trim(extmsg)//' tau_sb'
if (prm%E_sb < 0.0_pREAL) extmsg = trim(extmsg)//' Q_sb'
if (prm%p_sb <= 0.0_pREAL) extmsg = trim(extmsg)//' p_sb'
if (prm%q_sb <= 0.0_pREAL) extmsg = trim(extmsg)//' q_sb'
end if
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!--------------------------------------------------------------------------------------------------
! parameters required for several mechanisms and their interactions
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if (prm%sum_N_sl + prm%sum_N_tw + prm%sum_N_tw > 0) &
prm%D = pl%get_asReal('D')
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if (prm%sum_N_tw + prm%sum_N_tr > 0) then
prm%x_c = pl%get_asReal('x_c')
prm%V_cs = pl%get_asReal('V_cs')
if (prm%x_c < 0.0_pREAL) extmsg = trim(extmsg)//' x_c'
if (prm%V_cs < 0.0_pREAL) extmsg = trim(extmsg)//' V_cs'
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end if
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if (prm%sum_N_tw + prm%sum_N_tr > 0 .or. prm%extendedDislocations) &
prm%Gamma_sf = polynomial(pl,'Gamma_sf','T')
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slipAndTwinActive: if (prm%sum_N_sl * prm%sum_N_tw > 0) then
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prm%h_sl_tw = crystal_interaction_SlipByTwin(N_sl,prm%N_tw,pl%get_as1dReal('h_sl-tw'), &
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phase_lattice(ph))
if (prm%fccTwinTransNucleation .and. size(prm%N_tw) /= 1) extmsg = trim(extmsg)//' N_tw: nucleation'
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end if slipAndTwinActive
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slipAndTransActive: if (prm%sum_N_sl * prm%sum_N_tr > 0) then
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prm%h_sl_tr = crystal_interaction_SlipByTrans(N_sl,prm%N_tr,pl%get_as1dReal('h_sl-tr'), &
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phase_lattice(ph))
if (prm%fccTwinTransNucleation .and. size(prm%N_tr) /= 1) extmsg = trim(extmsg)//' N_tr: nucleation'
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end if slipAndTransActive
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twinAndTransActive: if (prm%sum_N_tw * prm%sum_N_tr > 0) then
if (dNeq(prm%b_tw(1),prm%b_tr(1))) extmsg = trim(extmsg)//' b_tw != b_tr'
end if twinAndTransActive
!--------------------------------------------------------------------------------------------------
! allocate state arrays
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Nmembers = count(material_ID_phase == ph)
sizeDotState = size(['rho_mob ','rho_dip ','gamma_sl']) * prm%sum_N_sl &
+ size(['f_tw']) * prm%sum_N_tw &
+ size(['f_tr']) * prm%sum_N_tr
sizeState = sizeDotState
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call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,0)
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deallocate(plasticState(ph)%dotState) ! ToDo: remove dotState completely
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!--------------------------------------------------------------------------------------------------
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! state aliases and initialization
startIndex = 1
endIndex = prm%sum_N_sl
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idx_dot%rho_mob = [startIndex,endIndex]
stt%rho_mob => plasticState(ph)%state(startIndex:endIndex,:)
stt%rho_mob = spread(rho_mob_0,2,Nmembers)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_rho',defaultVal=1.0_pREAL)
if (any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pREAL)) extmsg = trim(extmsg)//' atol_rho'
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startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_sl
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idx_dot%rho_dip = [startIndex,endIndex]
stt%rho_dip => plasticState(ph)%state(startIndex:endIndex,:)
stt%rho_dip = spread(rho_dip_0,2,Nmembers)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_rho',defaultVal=1.0_pREAL)
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startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_sl
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idx_dot%gamma_sl = [startIndex,endIndex]
stt%gamma_sl => plasticState(ph)%state(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_gamma',defaultVal=1.0e-6_pREAL)
if (any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pREAL)) extmsg = trim(extmsg)//' atol_gamma'
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startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_tw
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idx_dot%f_tw = [startIndex,endIndex]
stt%f_tw => plasticState(ph)%state(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_f_tw',defaultVal=1.0e-6_pREAL)
if (any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pREAL)) extmsg = trim(extmsg)//' atol_f_tw'
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startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_tr
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idx_dot%f_tr = [startIndex,endIndex]
stt%f_tr => plasticState(ph)%state(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_f_tr',defaultVal=1.0e-6_pREAL)
if (any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pREAL)) extmsg = trim(extmsg)//' atol_f_tr'
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allocate(dst%tau_pass (prm%sum_N_sl,Nmembers),source=0.0_pREAL)
allocate(dst%Lambda_sl(prm%sum_N_sl,Nmembers),source=0.0_pREAL)
allocate(dst%Lambda_tw(prm%sum_N_tw,Nmembers),source=0.0_pREAL)
allocate(dst%Lambda_tr(prm%sum_N_tr,Nmembers),source=0.0_pREAL)
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end associate
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!--------------------------------------------------------------------------------------------------
! exit if any parameter is out of range
if (extmsg /= '') call IO_error(211,ext_msg=trim(extmsg))
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end do
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end function plastic_dislotwin_init
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!--------------------------------------------------------------------------------------------------
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!> @brief Return the homogenized elasticity matrix.
!--------------------------------------------------------------------------------------------------
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module function plastic_dislotwin_homogenizedC(ph,en) result(homogenizedC)
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integer, intent(in) :: &
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ph, en
real(pREAL), dimension(6,6) :: &
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homogenizedC, &
C
real(pREAL), dimension(:,:,:), allocatable :: &
C66_tw, &
C66_tr
integer :: i
real(pREAL) :: f_matrix
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C = elastic_C66(ph,en)
associate(prm => param(ph), stt => state(ph))
f_matrix = 1.0_pREAL &
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- sum(stt%f_tw(1:prm%sum_N_tw,en)) &
- sum(stt%f_tr(1:prm%sum_N_tr,en))
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homogenizedC = f_matrix * C
twinActive: if (prm%sum_N_tw > 0) then
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C66_tw = crystal_C66_twin(prm%N_tw,C,phase_lattice(ph),phase_cOverA(ph))
do i = 1, prm%sum_N_tw
homogenizedC = homogenizedC &
+ stt%f_tw(i,en)*C66_tw(1:6,1:6,i)
end do
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end if twinActive
transActive: if (prm%sum_N_tr > 0) then
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C66_tr = crystal_C66_trans(prm%N_tr,C,'hP',prm%cOverA_hP)
do i = 1, prm%sum_N_tr
homogenizedC = homogenizedC &
+ stt%f_tr(i,en)*C66_tr(1:6,1:6,i)
end do
end if transActive
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end associate
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end function plastic_dislotwin_homogenizedC
!--------------------------------------------------------------------------------------------------
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!> @brief Calculate plastic velocity gradient and its tangent.
!--------------------------------------------------------------------------------------------------
module subroutine dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
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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
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integer, intent(in) :: ph,en
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integer :: i,k,l,m,n
real(pREAL) :: &
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f_matrix,StressRatio_p,&
E_kB_T, &
ddot_gamma_dtau, &
tau, &
T
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
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dot_gamma_sl,ddot_gamma_dtau_sl
real(pREAL), dimension(param(ph)%sum_N_tw) :: &
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dot_gamma_tw,ddot_gamma_dtau_tw
real(pREAL), dimension(param(ph)%sum_N_tr) :: &
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dot_gamma_tr,ddot_gamma_dtau_tr
real(pREAL):: dot_gamma_sb
real(pREAL), dimension(3,3) :: eigVectors, P_sb
real(pREAL), dimension(3) :: eigValues
real(pREAL), dimension(3,6), parameter :: &
sb_sComposition = &
reshape(real([&
1, 0, 1, &
1, 0,-1, &
1, 1, 0, &
1,-1, 0, &
0, 1, 1, &
0, 1,-1 &
],pREAL),[ 3,6]), &
sb_mComposition = &
reshape(real([&
1, 0,-1, &
1, 0,+1, &
1,-1, 0, &
1, 1, 0, &
0, 1,-1, &
0, 1, 1 &
],pREAL),[ 3,6])
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T = thermal_T(ph,en)
Lp = 0.0_pREAL
dLp_dMp = 0.0_pREAL
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associate(prm => param(ph), stt => state(ph))
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f_matrix = 1.0_pREAL &
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- sum(stt%f_tw(1:prm%sum_N_tw,en)) &
- sum(stt%f_tr(1:prm%sum_N_tr,en))
call kinetics_sl(Mp,T,ph,en,dot_gamma_sl,ddot_gamma_dtau_sl)
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) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ ddot_gamma_dtau_sl(i) * prm%P_sl(k,l,i) * prm%P_sl(m,n,i)
end do slipContribution
if (prm%sum_N_tw > 0) call kinetics_tw(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) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ ddot_gamma_dtau_tw(i)* prm%P_tw(k,l,i)*prm%P_tw(m,n,i)
end do twinContibution
if (prm%sum_N_tr > 0) call kinetics_tr(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) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ ddot_gamma_dtau_tr(i)* prm%P_tr(k,l,i)*prm%P_tr(m,n,i)
end do transContibution
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Lp = Lp * f_matrix
dLp_dMp = dLp_dMp * f_matrix
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shearBandingContribution: if (dNeq0(prm%gamma_0_sb)) then
E_kB_T = prm%E_sb/(K_B*T)
call math_eigh33(eigValues,eigVectors,Mp) ! is Mp symmetric by design?
do i = 1,6
P_sb = 0.5_pREAL * math_outer(matmul(eigVectors,sb_sComposition(1:3,i)),&
matmul(eigVectors,sb_mComposition(1:3,i)))
tau = math_tensordot(Mp,P_sb)
significantShearBandStress: if (abs(tau) > tol_math_check) then
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StressRatio_p = (abs(tau)/prm%tau_sb)**prm%p_sb
dot_gamma_sb = sign(prm%gamma_0_sb*exp(-E_kB_T*(1-StressRatio_p)**prm%q_sb), tau)
ddot_gamma_dtau = abs(dot_gamma_sb)*E_kB_T*prm%p_sb*prm%q_sb/prm%tau_sb &
* (abs(tau)/prm%tau_sb)**(prm%p_sb-1.0_pREAL) &
* (1.0_pREAL-StressRatio_p)**(prm%q_sb-1.0_pREAL)
Lp = Lp + dot_gamma_sb * P_sb
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ ddot_gamma_dtau * P_sb(k,l) * P_sb(m,n)
end if significantShearBandStress
end do
end if shearBandingContribution
end associate
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end subroutine dislotwin_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
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!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
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module function dislotwin_dotState(Mp,ph,en) result(dotState)
real(pREAL), dimension(3,3), intent(in):: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
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en
real(pREAL), dimension(plasticState(ph)%sizeDotState) :: &
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dotState
integer :: i
real(pREAL) :: &
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f_matrix, &
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d_hat, &
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v_cl, & !< climb velocity
tau, &
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sigma_cl, & !< climb stress
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b_d !< ratio of Burgers vector to stacking fault width
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
dot_rho_dip_formation, &
dot_rho_dip_climb, &
dot_gamma_sl
real(pREAL), dimension(param(ph)%sum_N_tw) :: &
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dot_gamma_tw
real(pREAL), dimension(param(ph)%sum_N_tr) :: &
dot_gamma_tr
real(pREAL) :: &
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mu, nu, &
T
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associate(prm => param(ph), stt => state(ph), dst => dependentState(ph), &
dot_rho_mob => dotState(indexDotState(ph)%rho_mob(1):indexDotState(ph)%rho_mob(2)), &
dot_rho_dip => dotState(indexDotState(ph)%rho_dip(1):indexDotState(ph)%rho_dip(2)), &
abs_dot_gamma_sl => dotState(indexDotState(ph)%gamma_sl(1):indexDotState(ph)%gamma_sl(2)), &
dot_f_tw => dotState(indexDotState(ph)%f_tw(1):indexDotState(ph)%f_tw(2)), &
dot_f_tr => dotState(indexDotState(ph)%f_tr(1):indexDotState(ph)%f_tr(2)))
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mu = elastic_mu(ph,en,prm%isotropic_bound)
nu = elastic_nu(ph,en,prm%isotropic_bound)
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T = thermal_T(ph,en)
f_matrix = 1.0_pREAL &
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- sum(stt%f_tw(1:prm%sum_N_tw,en)) &
- sum(stt%f_tr(1:prm%sum_N_tr,en))
call kinetics_sl(Mp,T,ph,en,dot_gamma_sl)
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abs_dot_gamma_sl = abs(dot_gamma_sl)
slipState: do i = 1, prm%sum_N_sl
tau = math_tensordot(Mp,prm%P_sl(1:3,1:3,i))
significantSlipStress: if (dEq0(tau) .or. prm%omitDipoles) then
dot_rho_dip_formation(i) = 0.0_pREAL
dot_rho_dip_climb(i) = 0.0_pREAL
else significantSlipStress
d_hat = 3.0_pREAL*mu*prm%b_sl(i)/(16.0_pREAL*PI*abs(tau))
d_hat = math_clip(d_hat, right = dst%Lambda_sl(i,en))
d_hat = math_clip(d_hat, left = prm%d_caron(i))
dot_rho_dip_formation(i) = 2.0_pREAL*(d_hat-prm%d_caron(i))/prm%b_sl(i) &
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* stt%rho_mob(i,en)*abs_dot_gamma_sl(i)
if (dEq(d_hat,prm%d_caron(i))) then
dot_rho_dip_climb(i) = 0.0_pREAL
else
! Argon & Moffat, Acta Metallurgica, Vol. 29, pg 293 to 299, 1981
sigma_cl = dot_product(prm%n0_sl(1:3,i),matmul(Mp,prm%n0_sl(1:3,i)))
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if (prm%extendedDislocations) then
b_d = 24.0_pREAL*PI*(1.0_pREAL - nu)/(2.0_pREAL + nu) * prm%Gamma_sf%at(T) / (mu*prm%b_sl(i))
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else
b_d = 1.0_pREAL
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end if
v_cl = 2.0_pREAL*prm%omega*b_d**2*exp(-prm%Q_cl/(K_B*T)) &
* (exp(abs(sigma_cl)*prm%b_sl(i)**3/(K_B*T)) - 1.0_pREAL)
dot_rho_dip_climb(i) = 4.0_pREAL*v_cl*stt%rho_dip(i,en) &
/ (d_hat-prm%d_caron(i))
end if
end if significantSlipStress
end do slipState
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dot_rho_mob = abs_dot_gamma_sl/(prm%b_sl*dst%Lambda_sl(:,en)) &
- dot_rho_dip_formation &
- 2.0_pREAL*prm%d_caron/prm%b_sl * stt%rho_mob(:,en)*abs_dot_gamma_sl
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dot_rho_dip = dot_rho_dip_formation &
- 2.0_pREAL*prm%d_caron/prm%b_sl * stt%rho_dip(:,en)*abs_dot_gamma_sl &
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- dot_rho_dip_climb
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if (prm%sum_N_tw > 0) call kinetics_tw(Mp,T,abs_dot_gamma_sl,ph,en,dot_gamma_tw)
dot_f_tw = f_matrix*dot_gamma_tw/prm%gamma_char_tw
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if (prm%sum_N_tr > 0) call kinetics_tr(Mp,T,abs_dot_gamma_sl,ph,en,dot_gamma_tr)
dot_f_tr = f_matrix*dot_gamma_tr/gamma_char_tr
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end associate
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end function dislotwin_dotState
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate derived quantities from state.
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!--------------------------------------------------------------------------------------------------
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module subroutine dislotwin_dependentState(ph,en)
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integer, intent(in) :: &
ph, &
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en
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real(pREAL) :: &
sumf_tw, sumf_tr
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
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inv_lambda_sl
real(pREAL), dimension(param(ph)%sum_N_tw) :: &
inv_lambda_tw_tw, & !< 1/mean free distance between 2 twin stacks from different systems seen by a growing twin
f_over_t_tw
real(pREAL), dimension(param(ph)%sum_N_tr) :: &
inv_lambda_tr_tr, & !< 1/mean free distance between 2 martensite stacks from different systems seen by a growing martensite
f_over_t_tr
real(pREAL) :: &
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mu
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associate(prm => param(ph), stt => state(ph), dst => dependentState(ph))
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mu = elastic_mu(ph,en,prm%isotropic_bound)
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sumf_tw = sum(stt%f_tw(1:prm%sum_N_tw,en))
sumf_tr = sum(stt%f_tr(1:prm%sum_N_tr,en))
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!* rescaled volume fraction for topology
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
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! ToDo ...Physically correct, but naming could be adjusted
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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)
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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(:,en) = prm%D / (1.0_pREAL+prm%D*inv_lambda_sl)
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inv_lambda_tw_tw = matmul(prm%h_tw_tw,f_over_t_tw)/(1.0_pREAL-sumf_tw)
dst%Lambda_tw(:,en) = prm%i_tw*prm%D/(1.0_pREAL+prm%D*inv_lambda_tw_tw)
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inv_lambda_tr_tr = matmul(prm%h_tr_tr,f_over_t_tr)/(1.0_pREAL-sumf_tr)
dst%Lambda_tr(:,en) = prm%i_tr*prm%D/(1.0_pREAL+prm%D*inv_lambda_tr_tr)
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!* threshold stress for dislocation motion
dst%tau_pass(:,en) = mu*prm%b_sl* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,en)+stt%rho_dip(:,en)))
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end associate
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end subroutine dislotwin_dependentState
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!--------------------------------------------------------------------------------------------------
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!> @brief Write results to HDF5 output file.
!--------------------------------------------------------------------------------------------------
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module subroutine plastic_dislotwin_result(ph,group)
integer, intent(in) :: ph
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character(len=*), intent(in) :: group
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integer :: ou
associate(prm => param(ph), stt => state(ph), dst => dependentState(ph))
do ou = 1,size(prm%output)
select case(trim(prm%output(ou)))
case('rho_mob')
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call result_writeDataset(stt%rho_mob,group,trim(prm%output(ou)), &
'mobile dislocation density','1/m²',prm%systems_sl)
case('rho_dip')
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call result_writeDataset(stt%rho_dip,group,trim(prm%output(ou)), &
'dislocation dipole density','1/m²',prm%systems_sl)
case('gamma_sl')
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call result_writeDataset(stt%gamma_sl,group,trim(prm%output(ou)), &
'plastic shear','1',prm%systems_sl)
case('Lambda_sl')
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call result_writeDataset(dst%Lambda_sl,group,trim(prm%output(ou)), &
'mean free path for slip','m',prm%systems_sl)
case('tau_pass')
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call result_writeDataset(dst%tau_pass,group,trim(prm%output(ou)), &
'passing stress for slip','Pa',prm%systems_sl)
case('f_tw')
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call result_writeDataset(stt%f_tw,group,trim(prm%output(ou)), &
'twinned volume fraction','m³/m³',prm%systems_tw)
case('Lambda_tw')
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call result_writeDataset(dst%Lambda_tw,group,trim(prm%output(ou)), &
'mean free path for twinning','m',prm%systems_tw)
case('f_tr')
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if (prm%sum_N_tr>0) call result_writeDataset(stt%f_tr,group,trim(prm%output(ou)), &
'martensite volume fraction','m³/m³')
end select
end do
end associate
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end subroutine plastic_dislotwin_result
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate shear rates on slip systems, their derivatives with respect to resolved
! stress, and the resolved stress.
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!> @details Derivatives and resolved stress are calculated only optionally.
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! NOTE: Contrary to common convention, here the result (i.e. intent(out)) variables have to be put
! at the end since some of them are optional.
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_sl(Mp,T,ph,en, &
dot_gamma_sl,ddot_gamma_dtau_sl,tau_sl)
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real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pREAL), intent(in) :: &
T !< temperature
integer, intent(in) :: &
ph, &
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en
real(pREAL), dimension(param(ph)%sum_N_sl), intent(out) :: &
dot_gamma_sl
real(pREAL), dimension(param(ph)%sum_N_sl), optional, intent(out) :: &
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ddot_gamma_dtau_sl, &
tau_sl
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real(pREAL), dimension(param(ph)%sum_N_sl) :: &
ddot_gamma_dtau
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
tau, &
stressRatio, &
StressRatio_p, &
Q_kB_T, &
v_wait_inverse, & !< inverse of the effective velocity of a dislocation waiting at obstacles (unsigned)
v_run_inverse, & !< inverse of the velocity of a free moving dislocation (unsigned)
dV_wait_inverse_dTau, &
dV_run_inverse_dTau, &
dV_dTau, &
tau_eff !< effective resolved stress
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integer :: i
associate(prm => param(ph), stt => state(ph), dst => dependentState(ph))
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tau = [(math_tensordot(Mp,prm%P_sl(1:3,1:3,i)),i = 1, prm%sum_N_sl)]
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tau_eff = abs(tau)-dst%tau_pass(:,en)
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significantStress: where(tau_eff > tol_math_check)
stressRatio = tau_eff/prm%tau_0
StressRatio_p = stressRatio** prm%p
Q_kB_T = prm%Q_sl/(K_B*T)
v_wait_inverse = exp(Q_kB_T*(1.0_pREAL-StressRatio_p)** prm%q) &
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/ prm%v_0
v_run_inverse = prm%B/(tau_eff*prm%b_sl)
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dot_gamma_sl = sign(stt%rho_mob(:,en)*prm%b_sl/(v_wait_inverse+v_run_inverse),tau)
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dV_wait_inverse_dTau = -1.0_pREAL * v_wait_inverse * prm%p * prm%q * Q_kB_T &
* (stressRatio**(prm%p-1.0_pREAL)) &
* (1.0_pREAL-StressRatio_p)**(prm%q-1.0_pREAL) &
/ prm%tau_0
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
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
end where significantStress
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end associate
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if (present(ddot_gamma_dtau_sl)) ddot_gamma_dtau_sl = ddot_gamma_dtau
if (present(tau_sl)) tau_sl = tau
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end subroutine kinetics_sl
!--------------------------------------------------------------------------------------------------
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!> @brief Calculate shear rates on twin systems and their derivatives with respect to resolved
! stress.
!> @details Derivatives are calculated only optionally.
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! NOTE: Contrary to common convention, here the result (i.e. intent(out)) variables have to be put
! at the end since some of them are optional.
!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_tw(Mp,T,abs_dot_gamma_sl,ph,en,&
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dot_gamma_tw,ddot_gamma_dtau_tw)
real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pREAL), intent(in) :: &
T !< temperature
integer, intent(in) :: &
ph, &
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en
real(pREAL), dimension(param(ph)%sum_N_sl), intent(in) :: &
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abs_dot_gamma_sl
real(pREAL), dimension(param(ph)%sum_N_tw), intent(out) :: &
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dot_gamma_tw
real(pREAL), dimension(param(ph)%sum_N_tw), optional, intent(out) :: &
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ddot_gamma_dtau_tw
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real(pREAL) :: &
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tau, tau_r, tau_hat, &
dot_N_0, &
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x0, V, &
Gamma_sf, &
mu, nu, &
P_ncs, dP_ncs_dtau, &
P, dP_dtau
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integer, dimension(2) :: &
s
integer :: i
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associate(prm => param(ph), stt => state(ph), dst => dependentState(ph))
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mu = elastic_mu(ph,en,prm%isotropic_bound)
nu = elastic_nu(ph,en,prm%isotropic_bound)
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Gamma_sf = prm%Gamma_sf%at(T)
tau_hat = 3.0_pREAL*prm%b_tw(1)*mu/prm%L_tw &
+ Gamma_sf/(3.0_pREAL*prm%b_tw(1))
x0 = mu*prm%b_sl(1)**2*(2.0_pREAL+nu)/(Gamma_sf*8.0_pREAL*PI*(1.0_pREAL-nu))
tau_r = mu*prm%b_sl(1)/(2.0_pREAL*PI)*(1.0_pREAL/(x0+prm%x_c)+cos(PI/3.0_pREAL)/x0)
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do i = 1, prm%sum_N_tw
tau = math_tensordot(Mp,prm%P_tw(1:3,1:3,i))
if (tau > tol_math_check .and. tau < tau_r) then
P = exp(-(tau_hat/tau)**prm%r(i))
dP_dTau = prm%r(i) * (tau_hat/tau)**prm%r(i)/tau * P
s = prm%fcc_twinNucleationSlipPair(1:2,i)
dot_N_0 = sum(abs_dot_gamma_sl(s(2:1:-1))*(stt%rho_mob(s,en)+stt%rho_dip(s,en)))/(prm%L_tw*3.0_pREAL)
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P_ncs = 1.0_pREAL-exp(-prm%V_cs/(K_B*T)*(tau_r-tau))
dP_ncs_dtau = prm%V_cs / (K_B * T) * (P_ncs - 1.0_pREAL)
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V = PI/4.0_pREAL*dst%Lambda_tw(i,en)**2*prm%t_tw(i)
dot_gamma_tw(i) = V*dot_N_0*P_ncs*P*prm%gamma_char_tw(i)
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if (present(ddot_gamma_dtau_tw)) &
ddot_gamma_dtau_tw(i) = V*dot_N_0*(P*dP_ncs_dtau + P_ncs*dP_dtau)*prm%gamma_char_tw(i)
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else
dot_gamma_tw(i) = 0.0_pREAL
if (present(ddot_gamma_dtau_tw)) ddot_gamma_dtau_tw(i) = 0.0_pREAL
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end if
end do
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end associate
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end subroutine kinetics_tw
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate shear rates on transformation systems and their derivatives with respect to
! resolved stress.
!> @details Derivatives are calculated only optionally.
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! NOTE: Contrary to common convention, here the result (i.e. intent(out)) variables have to be put
! at the end since some of them are optional.
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_tr(Mp,T,abs_dot_gamma_sl,ph,en,&
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dot_gamma_tr,ddot_gamma_dtau_tr)
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real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pREAL), intent(in) :: &
T !< temperature
integer, intent(in) :: &
ph, &
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en
real(pREAL), dimension(param(ph)%sum_N_sl), intent(in) :: &
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abs_dot_gamma_sl
real(pREAL), dimension(param(ph)%sum_N_tr), intent(out) :: &
dot_gamma_tr
real(pREAL), dimension(param(ph)%sum_N_tr), optional, intent(out) :: &
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ddot_gamma_dtau_tr
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real(pREAL) :: &
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tau, tau_r, tau_hat, &
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dot_N_0, &
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x0, V, &
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Gamma_sf, &
mu, nu, &
P_ncs, dP_ncs_dtau, &
P, dP_dtau
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integer, dimension(2) :: &
s
integer :: i
associate(prm => param(ph), stt => state(ph), dst => dependentState(ph))
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mu = elastic_mu(ph,en,prm%isotropic_bound)
nu = elastic_nu(ph,en,prm%isotropic_bound)
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Gamma_sf = prm%Gamma_sf%at(T)
tau_hat = 3.0_pREAL*prm%b_tr(1)*mu/prm%L_tr &
+ (Gamma_sf + (prm%h/prm%V_mol - 2.0_pREAL*prm%rho)*prm%Delta_G%at(T))/(3.0_pREAL*prm%b_tr(1))
x0 = mu*prm%b_sl(1)**2*(2.0_pREAL+nu)/(Gamma_sf*8.0_pREAL*PI*(1.0_pREAL-nu))
tau_r = mu*prm%b_sl(1)/(2.0_pREAL*PI)*(1.0_pREAL/(x0+prm%x_c)+cos(PI/3.0_pREAL)/x0)
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do i = 1, prm%sum_N_tr
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tau = math_tensordot(Mp,prm%P_tr(1:3,1:3,i))
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if (tau > tol_math_check .and. tau < tau_r) then
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P = exp(-(tau_hat/tau)**prm%s(i))
dP_dTau = prm%s(i) * (tau_hat/tau)**prm%s(i)/tau * P
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s = prm%fcc_twinNucleationSlipPair(1:2,i)
dot_N_0 = sum(abs_dot_gamma_sl(s(2:1:-1))*(stt%rho_mob(s,en)+stt%rho_dip(s,en)))/(prm%L_tr*3.0_pREAL)
P_ncs = 1.0_pREAL-exp(-prm%V_cs/(K_B*T)*(tau_r-tau))
dP_ncs_dtau = prm%V_cs / (K_B * T) * (P_ncs - 1.0_pREAL)
V = PI/4.0_pREAL*dst%Lambda_tr(i,en)**2*prm%t_tr(i)
dot_gamma_tr(i) = V*dot_N_0*P_ncs*P*gamma_char_tr
if (present(ddot_gamma_dtau_tr)) &
ddot_gamma_dtau_tr(i) = V*dot_N_0*(P*dP_ncs_dtau + P_ncs*dP_dtau)*gamma_char_tr
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else
dot_gamma_tr(i) = 0.0_pREAL
if (present(ddot_gamma_dtau_tr)) ddot_gamma_dtau_tr(i) = 0.0_pREAL
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end if
end do
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end associate
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end subroutine kinetics_tr
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end submodule dislotwin