DAMASK_EICMD/src/phase_mechanical_plastic_ph...

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!--------------------------------------------------------------------------------------------------
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
!> @brief phenomenological crystal plasticity formulation using a powerlaw fitting
!--------------------------------------------------------------------------------------------------
submodule(phase:plastic) phenopowerlaw
type :: tParameters
real(pREAL), allocatable, dimension(:) :: &
dot_gamma_0_sl, & !< reference shear strain rate for slip
dot_gamma_0_tw, & !< reference shear strain rate for twin
a_sl, &
n_sl, & !< stress exponent for slip
n_tw, & !< stress exponent for twin
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xi_inf_sl, & !< maximum critical shear stress for slip
f_sat_sl_tw, & !< push-up factor for slip saturation due to twinning
c_1, &
c_2, &
c_3, &
c_4, &
h_0_sl_sl, & !< reference hardening slip - slip
h_0_tw_sl, & !< reference hardening twin - slip
h_0_tw_tw, & !< reference hardening twin - twin
gamma_char !< characteristic shear for twins
real(pREAL), allocatable, dimension(:,:) :: &
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h_sl_sl, & !< slip resistance from slip activity
h_sl_tw, & !< slip resistance from twin activity
h_tw_sl, & !< twin resistance from slip activity
h_tw_tw !< twin resistance from twin activity
real(pREAL), allocatable, dimension(:,:,:) :: &
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P_sl, &
P_tw, &
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P_nS_pos, &
P_nS_neg
integer :: &
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sum_N_sl, & !< total number of active slip system
sum_N_tw !< total number of active twin systems
character(len=pSTRLEN), allocatable, dimension(:) :: &
output
character(len=:), allocatable, dimension(:) :: &
systems_sl, &
systems_tw
end type tParameters
type :: tIndexDotState
integer, dimension(2) :: &
xi_sl, &
xi_tw, &
gamma_sl, &
gamma_tw
end type tIndexDotState
type :: tPhenopowerlawState
real(pREAL), pointer, dimension(:,:) :: &
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xi_sl, &
xi_tw, &
gamma_sl, &
gamma_tw
end type tPhenopowerlawState
!--------------------------------------------------------------------------------------------------
! containers for parameters, dot state index, and state
type(tParameters), allocatable, dimension(:) :: param
type(tIndexDotState), allocatable, dimension(:) :: indexDotState
type(tPhenopowerlawState), allocatable, dimension(:) :: state
contains
!--------------------------------------------------------------------------------------------------
!> @brief Perform module initialization.
!> @details reads in material parameters, allocates arrays, and does sanity checks
!--------------------------------------------------------------------------------------------------
module function plastic_phenopowerlaw_init() result(myPlasticity)
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logical, dimension(:), allocatable :: myPlasticity
integer :: &
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ph, i, &
N_fam, &
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Nmembers, &
sizeState, sizeDotState, &
startIndex, endIndex
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integer, dimension(:), allocatable :: &
N_sl, & !< number of slip-systems for a given slip family
N_tw !< number of twin-systems for a given twin family
real(pREAL), dimension(:), allocatable :: &
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xi_0_sl, & !< initial critical shear stress for slip
xi_0_tw, & !< initial critical shear stress for twin
ones
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real(pREAL), dimension(:,:), allocatable :: &
a_nS !< non-Schmid coefficients
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('phenopowerlaw')
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if (count(myPlasticity) == 0) return
print'(/,1x,a)', '<<<+- phase:mechanical:plastic:phenopowerlaw init -+>>>'
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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')
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allocate(param(phases%length))
allocate(indexDotState(phases%length))
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allocate(state(phases%length))
extmsg = ''
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do ph = 1, phases%length
if (.not. myPlasticity(ph)) cycle
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associate(prm => param(ph), stt => state(ph), &
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
#if defined (__GFORTRAN__)
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prm%output = output_as1dStr(pl)
#else
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prm%output = pl%get_as1dStr('output',defaultVal=emptyStrArray)
#endif
N_sl = pl%get_as1dInt('N_sl',defaultVal=emptyIntArray)
N_tw = pl%get_as1dInt('N_tw',defaultVal=emptyIntArray)
prm%sum_N_sl = sum(abs(N_sl))
prm%sum_N_tw = sum(abs(N_tw))
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!--------------------------------------------------------------------------------------------------
! slip related parameters
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slipActive: if (prm%sum_N_sl > 0) then
N_fam = size(N_sl)
ones = [(1.0_pREAL,i=1,N_fam)]
prm%dot_gamma_0_sl = math_expand(pl%get_as1dReal('dot_gamma_0_sl',requiredSize=N_fam,defaultVal= ones), N_sl)
prm%n_sl = math_expand(pl%get_as1dReal('n_sl', requiredSize=N_fam,defaultVal= ones), N_sl)
prm%a_sl = math_expand(pl%get_as1dReal('a_sl', requiredSize=N_fam,defaultVal= ones), N_sl)
prm%h_0_sl_sl = math_expand(pl%get_as1dReal('h_0_sl-sl', requiredSize=N_fam,defaultVal=0.0_pREAL*ones), N_sl)
prm%c_1 = math_expand(pl%get_as1dReal('c_1', requiredSize=N_fam,defaultVal=0.0_pREAL*ones), N_sl)
prm%c_2 = math_expand(pl%get_as1dReal('c_2', requiredSize=N_fam,defaultVal= ones), N_sl)
xi_0_sl = math_expand(pl%get_as1dReal('xi_0_sl', requiredSize=N_fam), N_sl)
prm%xi_inf_sl = math_expand(pl%get_as1dReal('xi_inf_sl', requiredSize=N_fam), N_sl)
prm%f_sat_sl_tw = math_expand(pl%get_as1dReal('f_sat_sl-tw',requiredSize=N_fam,defaultVal=0.0_pREAL*ones), N_sl)
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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%P_sl = crystal_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph))
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if (phase_lattice(ph) == 'cI') then
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allocate(a_nS(3,size(pl%get_as1dReal('a_nonSchmid_110',defaultVal=emptyRealArray))),source=0.0_pREAL)
a_nS(1,:) = pl%get_as1dReal('a_nonSchmid_110',defaultVal=emptyRealArray)
prm%P_nS_pos = crystal_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph),nonSchmidCoefficients=a_nS,sense=+1)
prm%P_nS_neg = crystal_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph),nonSchmidCoefficients=a_nS,sense=-1)
else
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prm%P_nS_pos = +prm%P_sl
prm%P_nS_neg = -prm%P_sl
end if
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prm%systems_sl = crystal_labels_slip(N_sl,phase_lattice(ph))
! sanity checks
if (any(prm%dot_gamma_0_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' dot_gamma_0_sl'
if (any(prm%n_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' n_sl'
if (any(prm%a_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' a_sl'
if (any(xi_0_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' xi_0_sl'
if (any(prm%xi_inf_sl <= 0.0_pREAL)) extmsg = trim(extmsg)//' xi_inf_sl'
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else slipActive
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xi_0_sl = emptyRealArray
allocate(prm%dot_gamma_0_sl, & !< reference shear strain rate for slip
prm%a_sl, &
prm%n_sl, & !< stress exponent for slip
prm%xi_inf_sl, & !< maximum critical shear stress for slip
prm%f_sat_sl_tw, & !< push-up factor for slip saturation due to twinning
prm%c_1, &
prm%c_2, &
prm%h_0_sl_sl, & !< reference hardening slip - slip
source=emptyRealArray)
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allocate(prm%h_sl_sl(0,0))
end if slipActive
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!--------------------------------------------------------------------------------------------------
! twin related parameters
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twinActive: if (prm%sum_N_tw > 0) then
N_fam = size(N_tw)
ones = [(1.0_pREAL,i=1,N_fam)]
prm%dot_gamma_0_tw = math_expand(pl%get_as1dReal('dot_gamma_0_tw', requiredSize=N_fam,defaultVal=ones), N_tw)
prm%n_tw = math_expand(pl%get_as1dReal('n_tw', requiredSize=N_fam,defaultVal= ones), N_tw)
prm%c_3 = math_expand(pl%get_as1dReal('c_3', requiredSize=N_fam,defaultVal=0.0_pREAL*ones), N_tw)
prm%c_4 = math_expand(pl%get_as1dReal('c_4', requiredSize=N_fam,defaultVal=0.0_pREAL*ones), N_tw)
prm%h_0_tw_tw = math_expand(pl%get_as1dReal('h_0_tw-tw', requiredSize=N_fam,defaultVal=0.0_pReal*ones), N_tw)
xi_0_tw = math_expand(pl%get_as1dReal('xi_0_tw', requiredSize=N_fam), N_tw)
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prm%gamma_char = crystal_characteristicShear_twin(N_tw,phase_lattice(ph),phase_cOverA(ph))
prm%h_tw_tw = crystal_interaction_TwinByTwin(N_tw,pl%get_as1dReal('h_tw-tw'),phase_lattice(ph))
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prm%P_tw = crystal_SchmidMatrix_twin(N_tw,phase_lattice(ph),phase_cOverA(ph))
prm%systems_tw = crystal_labels_twin(N_tw,phase_lattice(ph))
! sanity checks
if (any(prm%dot_gamma_0_tw <= 0.0_pREAL)) extmsg = trim(extmsg)//' dot_gamma_0_tw'
if (any(prm%n_tw <= 0.0_pREAL)) extmsg = trim(extmsg)//' n_tw'
if (any(xi_0_tw <= 0.0_pREAL)) extmsg = trim(extmsg)//' xi_0_tw'
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else twinActive
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xi_0_tw = emptyRealArray
allocate(prm%dot_gamma_0_tw, & !< reference shear strain rate for twin
prm%n_tw, & !< stress exponent for twin
prm%c_3, &
prm%c_4, &
prm%gamma_char, & !< characteristic shear for twins
prm%h_0_tw_sl, & !< reference hardening twin - slip
prm%h_0_tw_tw, & !< reference hardening twin - twin
source=emptyRealArray)
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allocate(prm%h_tw_tw(0,0))
end if twinActive
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!--------------------------------------------------------------------------------------------------
! slip-twin related parameters
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slipAndTwinActive: if (prm%sum_N_sl > 0 .and. prm%sum_N_tw > 0) then
prm%h_0_tw_sl = math_expand(pl%get_as1dReal('h_0_tw-sl',requiredSize=N_fam,defaultVal=0.0_pReal*ones), N_tw)
prm%h_sl_tw = crystal_interaction_SlipByTwin(N_sl,N_tw,pl%get_as1dReal('h_sl-tw'),phase_lattice(ph))
prm%h_tw_sl = crystal_interaction_TwinBySlip(N_tw,N_sl,pl%get_as1dReal('h_tw-sl'),phase_lattice(ph))
else slipAndTwinActive
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allocate(prm%h_sl_tw(prm%sum_N_sl,prm%sum_N_tw)) ! at least one dimension is 0
allocate(prm%h_tw_sl(prm%sum_N_tw,prm%sum_N_sl)) ! at least one dimension is 0
prm%h_0_tw_sl = [(0.0_pREAL,i=1,size(N_tw))]
end if slipAndTwinActive
!--------------------------------------------------------------------------------------------------
! allocate state arrays
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Nmembers = count(material_ID_phase == ph)
sizeDotState = size(['xi_sl ','gamma_sl']) * prm%sum_N_sl &
+ size(['xi_tw ','gamma_tw']) * prm%sum_N_tw
sizeState = sizeDotState
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call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,0)
deallocate(plasticState(ph)%dotState) ! ToDo: remove dotState completely
!--------------------------------------------------------------------------------------------------
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! state aliases and initialization
startIndex = 1
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endIndex = prm%sum_N_sl
idx_dot%xi_sl = [startIndex,endIndex]
stt%xi_sl => plasticState(ph)%state(startIndex:endIndex,:)
stt%xi_sl = spread(xi_0_sl, 2, Nmembers)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_xi',defaultVal=1.0_pREAL)
if (any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pREAL)) extmsg = trim(extmsg)//' atol_xi'
startIndex = endIndex + 1
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endIndex = endIndex + prm%sum_N_tw
idx_dot%xi_tw = [startIndex,endIndex]
stt%xi_tw => plasticState(ph)%state(startIndex:endIndex,:)
stt%xi_tw = spread(xi_0_tw, 2, Nmembers)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_xi',defaultVal=1.0_pREAL)
startIndex = endIndex + 1
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endIndex = endIndex + prm%sum_N_sl
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
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endIndex = endIndex + prm%sum_N_tw
idx_dot%gamma_tw = [startIndex,endIndex]
stt%gamma_tw => plasticState(ph)%state(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asReal('atol_gamma',defaultVal=1.0e-6_pREAL)
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_phenopowerlaw_init
!--------------------------------------------------------------------------------------------------
!> @brief Calculate plastic velocity gradient and its tangent.
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!> @details assumes that deformation by dislocation glide affects twinned and untwinned volume
! equally (Taylor assumption). Twinning happens only in untwinned volume
!--------------------------------------------------------------------------------------------------
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pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
real(pREAL), dimension(3,3), intent(out) :: &
Lp !< plastic velocity gradient
real(pREAL), dimension(3,3,3,3), intent(out) :: &
dLp_dMp !< derivative of Lp with respect to the Mandel stress
real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
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en
integer :: &
i,k,l,m,n
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
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Lp = 0.0_pREAL
dLp_dMp = 0.0_pREAL
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associate(prm => param(ph))
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call kinetics_sl(Mp,ph,en,dot_gamma_sl,ddot_gamma_dtau_sl)
slipSystems: 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) &
* merge(prm%P_nS_pos(m,n,i), &
prm%P_nS_neg(m,n,i), dot_gamma_sl(i)>0.0_pREAL)
end do slipSystems
call kinetics_tw(Mp,ph,en,dot_gamma_tw,ddot_gamma_dtau_tw)
twinSystems: 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 twinSystems
end associate
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end subroutine phenopowerlaw_LpAndItsTangent
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!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module function phenopowerlaw_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) :: &
dotState
real(pREAL) :: &
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sumF
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
xi_sl_sat_offset, &
left_SlipSlip
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associate(prm => param(ph), stt => state(ph), &
dot_xi_sl => dotState(indexDotState(ph)%xi_sl(1):indexDotState(ph)%xi_sl(2)), &
dot_xi_tw => dotState(indexDotState(ph)%xi_tw(1):indexDotState(ph)%xi_tw(2)), &
dot_gamma_sl => dotState(indexDotState(ph)%gamma_sl(1):indexDotState(ph)%gamma_sl(2)), &
dot_gamma_tw => dotState(indexDotState(ph)%gamma_tw(1):indexDotState(ph)%gamma_tw(2)))
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call kinetics_sl(Mp,ph,en, dot_gamma_sl)
call kinetics_tw(Mp,ph,en, dot_gamma_tw)
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dot_gamma_sl = abs(dot_gamma_sl)
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sumF = sum(stt%gamma_tw(:,en)/prm%gamma_char)
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xi_sl_sat_offset = prm%f_sat_sl_tw*sqrt(sumF)
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left_SlipSlip = sign(abs(1.0_pREAL - stt%xi_sl(:,en) / (prm%xi_inf_sl+xi_sl_sat_offset))**prm%a_sl, &
1.0_pREAL - stt%xi_sl(:,en) / (prm%xi_inf_sl+xi_sl_sat_offset))
dot_xi_sl = prm%h_0_sl_sl * (1.0_pREAL + prm%c_1 * sumF**prm%c_2) &
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* left_SlipSlip &
* matmul(prm%h_sl_sl,dot_gamma_sl) &
+ matmul(prm%h_sl_tw,dot_gamma_tw)
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dot_xi_tw = prm%h_0_tw_sl * sum(stt%gamma_sl(:,en))**prm%c_3 * matmul(prm%h_tw_sl,dot_gamma_sl) &
+ prm%h_0_tw_tw * sumF **prm%c_4 * matmul(prm%h_tw_tw,dot_gamma_tw)
end associate
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end function phenopowerlaw_dotState
!--------------------------------------------------------------------------------------------------
!> @brief Write results to HDF5 output file.
!--------------------------------------------------------------------------------------------------
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module subroutine plastic_phenopowerlaw_result(ph,group)
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integer, intent(in) :: ph
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character(len=*), intent(in) :: group
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integer :: ou
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associate(prm => param(ph), stt => state(ph))
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do ou = 1,size(prm%output)
select case(trim(prm%output(ou)))
case('xi_sl')
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call result_writeDataset(stt%xi_sl,group,trim(prm%output(ou)), &
'resistance against plastic slip','Pa',prm%systems_sl)
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case('gamma_sl')
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call result_writeDataset(stt%gamma_sl,group,trim(prm%output(ou)), &
'plastic shear','1',prm%systems_sl)
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case('xi_tw')
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call result_writeDataset(stt%xi_tw,group,trim(prm%output(ou)), &
'resistance against twinning','Pa',prm%systems_tw)
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case('gamma_tw')
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call result_writeDataset(stt%gamma_tw,group,trim(prm%output(ou)), &
'twinning shear','1',prm%systems_tw)
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end select
end do
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end associate
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end subroutine plastic_phenopowerlaw_result
!--------------------------------------------------------------------------------------------------
!> @brief Calculate shear rates on slip systems and their derivatives with respect to resolved
! stress.
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!> @details Sign of dot_gamma_sl conveys sense of shear.
! Derivatives are calculated only optionally, hence, contrary to common convention,
! here the result (i.e. intent(out)) variables have to be put at the end.
!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_sl(Mp,ph,en, &
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dot_gamma_sl,ddot_gamma_dtau_sl)
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real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
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integer, intent(in) :: &
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ph, &
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en
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real(pREAL), dimension(param(ph)%sum_N_sl), intent(out) :: &
dot_gamma_sl
real(pREAL), dimension(param(ph)%sum_N_sl), optional, intent(out) :: &
ddot_gamma_dtau_sl
real(pREAL), dimension(param(ph)%sum_N_sl) :: &
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tau_sl_pos, &
tau_sl_neg
integer :: i
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associate(prm => param(ph), stt => state(ph))
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tau_sl_pos = [(math_tensordot(Mp,prm%P_nS_pos(1:3,1:3,i)),i=1,prm%sum_N_sl)]
tau_sl_neg = [(math_tensordot(Mp,prm%P_nS_neg(1:3,1:3,i)),i=1,prm%sum_N_sl)]
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dot_gamma_sl = merge(+1.0_pREAL,-1.0_pREAL, tau_sl_pos>tau_sl_neg) &
* prm%dot_gamma_0_sl &
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* (max(tau_sl_pos,tau_sl_neg)/stt%xi_sl(:,en))**prm%n_sl
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if (present(ddot_gamma_dtau_sl)) then
where(dNeq0(dot_gamma_sl))
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ddot_gamma_dtau_sl = dot_gamma_sl*prm%n_sl/max(tau_sl_pos,tau_sl_neg)
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else where
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ddot_gamma_dtau_sl = 0.0_pREAL
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end where
end if
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end associate
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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.
! Twinning is assumed to take place only in an untwinned volume.
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!> @details Derivatives are calculated and returned if corresponding output variables are present in the argument list.
! 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,ph,en,&
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dot_gamma_tw,ddot_gamma_dtau_tw)
real(pREAL), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
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ph, &
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en
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), intent(out), optional :: &
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ddot_gamma_dtau_tw
real(pREAL), dimension(param(ph)%sum_N_tw) :: &
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tau_tw
integer :: i
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associate(prm => param(ph), stt => state(ph))
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tau_tw = [(math_tensordot(Mp,prm%P_tw(1:3,1:3,i)),i=1,prm%sum_N_tw)]
where(tau_tw > 0.0_pREAL)
dot_gamma_tw = (1.0_pREAL-sum(stt%gamma_tw(:,en)/prm%gamma_char)) & ! only twin in untwinned volume fraction
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* prm%dot_gamma_0_tw*(tau_tw/stt%xi_tw(:,en))**prm%n_tw
else where
dot_gamma_tw = 0.0_pREAL
end where
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if (present(ddot_gamma_dtau_tw)) then
where(dNeq0(dot_gamma_tw))
ddot_gamma_dtau_tw = dot_gamma_tw*prm%n_tw/tau_tw
else where
ddot_gamma_dtau_tw = 0.0_pREAL
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end where
end if
end associate
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end subroutine kinetics_tw
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end submodule phenopowerlaw