DAMASK_EICMD/src/phase_mechanical_plastic_ph...

521 lines
23 KiB
Fortran

!--------------------------------------------------------------------------------------------------
!> @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) :: &
dot_gamma_0_sl = 1.0_pReal, & !< reference shear strain rate for slip
dot_gamma_0_tw = 1.0_pReal, & !< reference shear strain rate for twin
n_sl = 1.0_pReal, & !< stress exponent for slip
n_tw = 1.0_pReal, & !< stress exponent for twin
f_sat_sl_tw = 1.0_pReal, & !< push-up factor for slip saturation due to twinning
c_1 = 1.0_pReal, &
c_2 = 1.0_pReal, &
c_3 = 1.0_pReal, &
c_4 = 1.0_pReal, &
h_0_sl_sl = 1.0_pReal, & !< reference hardening slip - slip
h_0_tw_sl = 1.0_pReal, & !< reference hardening twin - slip
h_0_tw_tw = 1.0_pReal, & !< reference hardening twin - twin
a_sl = 1.0_pReal
real(pReal), allocatable, dimension(:) :: &
xi_inf_sl, & !< maximum critical shear stress for slip
h_int, & !< per family hardening activity (optional)
gamma_char !< characteristic shear for twins
real(pReal), allocatable, dimension(:,:) :: &
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(:,:,:) :: &
P_sl, &
P_tw, &
P_nS_pos, &
P_nS_neg
integer :: &
sum_N_sl, & !< total number of active slip system
sum_N_tw !< total number of active twin systems
logical :: &
nonSchmidActive = .false.
character(len=pStringLen), allocatable, dimension(:) :: &
output
end type tParameters
type :: tPhenopowerlawState
real(pReal), pointer, dimension(:,:) :: &
xi_sl, &
xi_tw, &
gamma_sl, &
gamma_tw
end type tPhenopowerlawState
!--------------------------------------------------------------------------------------------------
! containers for parameters and state
type(tParameters), allocatable, dimension(:) :: param
type(tPhenopowerlawState), allocatable, dimension(:) :: &
dotState, &
state
contains
!--------------------------------------------------------------------------------------------------
!> @brief Perform module initialization.
!> @details reads in material parameters, allocates arrays, and does sanity checks
!--------------------------------------------------------------------------------------------------
module function plastic_phenopowerlaw_init() result(myPlasticity)
logical, dimension(:), allocatable :: myPlasticity
integer :: &
ph, i, &
Nmembers, &
sizeState, sizeDotState, &
startIndex, endIndex
integer, dimension(:), allocatable :: &
N_sl, N_tw
real(pReal), dimension(:), allocatable :: &
xi_0_sl, & !< initial critical shear stress for slip
xi_0_tw, & !< initial critical shear stress for twin
a !< non-Schmid coefficients
character(len=pStringLen) :: &
extmsg = ''
class(tNode), pointer :: &
phases, &
phase, &
mech, &
pl
myPlasticity = plastic_active('phenopowerlaw')
if(count(myPlasticity) == 0) return
print'(/,a)', ' <<<+- phase:mechanical:plastic:phenopowerlaw init -+>>>'
print'(a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
phases => config_material%get('phase')
allocate(param(phases%length))
allocate(state(phases%length))
allocate(dotState(phases%length))
do ph = 1, phases%length
if(.not. myPlasticity(ph)) cycle
associate(prm => param(ph), dot => dotState(ph), stt => state(ph))
phase => phases%get(ph)
mech => phase%get('mechanical')
pl => mech%get('plastic')
!--------------------------------------------------------------------------------------------------
! slip related parameters
N_sl = pl%get_as1dInt('N_sl',defaultVal=emptyIntArray)
prm%sum_N_sl = sum(abs(N_sl))
slipActive: if (prm%sum_N_sl > 0) then
prm%P_sl = lattice_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph))
if (phase_lattice(ph) == 'cI') then
a = pl%get_as1dFloat('a_nonSchmid',defaultVal=emptyRealArray)
if(size(a) > 0) prm%nonSchmidActive = .true.
prm%P_nS_pos = lattice_nonSchmidMatrix(N_sl,a,+1)
prm%P_nS_neg = lattice_nonSchmidMatrix(N_sl,a,-1)
else
prm%P_nS_pos = prm%P_sl
prm%P_nS_neg = prm%P_sl
endif
prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl-sl'), &
phase_lattice(ph))
xi_0_sl = pl%get_as1dFloat('xi_0_sl', requiredSize=size(N_sl))
prm%xi_inf_sl = pl%get_as1dFloat('xi_inf_sl', requiredSize=size(N_sl))
prm%h_int = pl%get_as1dFloat('h_int', requiredSize=size(N_sl), &
defaultVal=[(0.0_pReal,i=1,size(N_sl))])
prm%dot_gamma_0_sl = pl%get_asFloat('dot_gamma_0_sl')
prm%n_sl = pl%get_asFloat('n_sl')
prm%a_sl = pl%get_asFloat('a_sl')
prm%h_0_sl_sl = pl%get_asFloat('h_0_sl-sl')
! expand: family => system
xi_0_sl = math_expand(xi_0_sl, N_sl)
prm%xi_inf_sl = math_expand(prm%xi_inf_sl,N_sl)
prm%h_int = math_expand(prm%h_int, N_sl)
! sanity checks
if ( prm%dot_gamma_0_sl <= 0.0_pReal) extmsg = trim(extmsg)//' dot_gamma_0_sl'
if ( prm%a_sl <= 0.0_pReal) extmsg = trim(extmsg)//' a_sl'
if ( prm%n_sl <= 0.0_pReal) extmsg = trim(extmsg)//' n_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'
else slipActive
xi_0_sl = emptyRealArray
allocate(prm%xi_inf_sl,prm%h_int,source=emptyRealArray)
allocate(prm%h_sl_sl(0,0))
endif slipActive
!--------------------------------------------------------------------------------------------------
! twin related parameters
N_tw = pl%get_as1dInt('N_tw', defaultVal=emptyIntArray)
prm%sum_N_tw = sum(abs(N_tw))
twinActive: if (prm%sum_N_tw > 0) then
prm%P_tw = lattice_SchmidMatrix_twin(N_tw,phase_lattice(ph),phase_cOverA(ph))
prm%h_tw_tw = lattice_interaction_TwinByTwin(N_tw,pl%get_as1dFloat('h_tw-tw'), &
phase_lattice(ph))
prm%gamma_char = lattice_characteristicShear_twin(N_tw,phase_lattice(ph),&
phase_cOverA(ph))
xi_0_tw = pl%get_as1dFloat('xi_0_tw',requiredSize=size(N_tw))
prm%c_1 = pl%get_asFloat('c_1',defaultVal=0.0_pReal)
prm%c_2 = pl%get_asFloat('c_2',defaultVal=1.0_pReal)
prm%c_3 = pl%get_asFloat('c_3',defaultVal=0.0_pReal)
prm%c_4 = pl%get_asFloat('c_4',defaultVal=0.0_pReal)
prm%dot_gamma_0_tw = pl%get_asFloat('dot_gamma_0_tw')
prm%n_tw = pl%get_asFloat('n_tw')
prm%f_sat_sl_tw = pl%get_asFloat('f_sat_sl-tw')
prm%h_0_tw_tw = pl%get_asFloat('h_0_tw-tw')
! expand: family => system
xi_0_tw = math_expand(xi_0_tw,N_tw)
! sanity checks
if (prm%dot_gamma_0_tw <= 0.0_pReal) extmsg = trim(extmsg)//' dot_gamma_0_tw'
if (prm%n_tw <= 0.0_pReal) extmsg = trim(extmsg)//' n_tw'
else twinActive
xi_0_tw = emptyRealArray
allocate(prm%gamma_char,source=emptyRealArray)
allocate(prm%h_tw_tw(0,0))
endif twinActive
!--------------------------------------------------------------------------------------------------
! slip-twin related parameters
slipAndTwinActive: if (prm%sum_N_sl > 0 .and. prm%sum_N_tw > 0) then
prm%h_0_tw_sl = pl%get_asFloat('h_0_tw-sl')
prm%h_sl_tw = lattice_interaction_SlipByTwin(N_sl,N_tw,pl%get_as1dFloat('h_sl-tw'), &
phase_lattice(ph))
prm%h_tw_sl = lattice_interaction_TwinBySlip(N_tw,N_sl,pl%get_as1dFloat('h_tw-sl'), &
phase_lattice(ph))
else slipAndTwinActive
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
endif slipAndTwinActive
!--------------------------------------------------------------------------------------------------
! output pararameters
#if defined (__GFORTRAN__)
prm%output = output_as1dString(pl)
#else
prm%output = pl%get_as1dString('output',defaultVal=emptyStringArray)
#endif
!--------------------------------------------------------------------------------------------------
! allocate state arrays
Nmembers = count(material_phaseID == ph)
sizeDotState = size(['xi_sl ','gamma_sl']) * prm%sum_N_sl &
+ size(['xi_tw ','gamma_tw']) * prm%sum_N_tw
sizeState = sizeDotState
call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,0)
!--------------------------------------------------------------------------------------------------
! state aliases and initialization
startIndex = 1
endIndex = prm%sum_N_sl
stt%xi_sl => plasticState(ph)%state (startIndex:endIndex,:)
stt%xi_sl = spread(xi_0_sl, 2, Nmembers)
dot%xi_sl => plasticState(ph)%dotState(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_xi',defaultVal=1.0_pReal)
if(any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pReal)) extmsg = trim(extmsg)//' atol_xi'
startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_tw
stt%xi_tw => plasticState(ph)%state (startIndex:endIndex,:)
stt%xi_tw = spread(xi_0_tw, 2, Nmembers)
dot%xi_tw => plasticState(ph)%dotState(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_xi',defaultVal=1.0_pReal)
startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_sl
stt%gamma_sl => plasticState(ph)%state (startIndex:endIndex,:)
dot%gamma_sl => plasticState(ph)%dotState(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_gamma',defaultVal=1.0e-6_pReal)
if(any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pReal)) extmsg = trim(extmsg)//' atol_gamma'
startIndex = endIndex + 1
endIndex = endIndex + prm%sum_N_tw
stt%gamma_tw => plasticState(ph)%state (startIndex:endIndex,:)
dot%gamma_tw => plasticState(ph)%dotState(startIndex:endIndex,:)
plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_gamma',defaultVal=1.0e-6_pReal)
end associate
!--------------------------------------------------------------------------------------------------
! exit if any parameter is out of range
if (extmsg /= '') call IO_error(211,ext_msg=trim(extmsg)//'(phenopowerlaw)')
enddo
end function plastic_phenopowerlaw_init
!--------------------------------------------------------------------------------------------------
!> @brief Calculate plastic velocity gradient and its tangent.
!> @details asummes that deformation by dislocation glide affects twinned and untwinned volume
! equally (Taylor assumption). Twinning happens only in untwinned volume
!--------------------------------------------------------------------------------------------------
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, &
en
integer :: &
i,k,l,m,n
real(pReal), dimension(param(ph)%sum_N_sl) :: &
dot_gamma_sl_pos,dot_gamma_sl_neg, &
ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg
real(pReal), dimension(param(ph)%sum_N_tw) :: &
dot_gamma_tw,ddot_gamma_dtautwin
Lp = 0.0_pReal
dLp_dMp = 0.0_pReal
associate(prm => param(ph))
call kinetics_sl(Mp,ph,en,dot_gamma_sl_pos,dot_gamma_sl_neg,ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg)
slipSystems: do i = 1, prm%sum_N_sl
Lp = Lp + (dot_gamma_sl_pos(i)+dot_gamma_sl_neg(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_pos(i) * prm%P_sl(k,l,i) * prm%P_nS_pos(m,n,i) &
+ ddot_gamma_dtau_sl_neg(i) * prm%P_sl(k,l,i) * prm%P_nS_neg(m,n,i)
enddo slipSystems
call kinetics_tw(Mp,ph,en,dot_gamma_tw,ddot_gamma_dtautwin)
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_dtautwin(i)*prm%P_tw(k,l,i)*prm%P_tw(m,n,i)
enddo twinSystems
end associate
end subroutine phenopowerlaw_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief Calculate the rate of change of microstructure.
!--------------------------------------------------------------------------------------------------
module subroutine phenopowerlaw_dotState(Mp,ph,en)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
en
real(pReal) :: &
xi_sl_sat_offset,&
sumF
real(pReal), dimension(param(ph)%sum_N_sl) :: &
dot_gamma_sl_pos,dot_gamma_sl_neg, &
right_SlipSlip
associate(prm => param(ph), stt => state(ph), dot => dotState(ph))
call kinetics_sl(Mp,ph,en,dot_gamma_sl_pos,dot_gamma_sl_neg)
dot%gamma_sl(:,en) = abs(dot_gamma_sl_pos+dot_gamma_sl_neg)
call kinetics_tw(Mp,ph,en,dot%gamma_tw(:,en))
sumF = sum(stt%gamma_tw(:,en)/prm%gamma_char)
xi_sl_sat_offset = prm%f_sat_sl_tw*sqrt(sumF)
right_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(:,en) = prm%h_0_sl_sl * (1.0_pReal + prm%c_1*sumF** prm%c_2) * (1.0_pReal + prm%h_int) &
* matmul(prm%h_sl_sl,dot%gamma_sl(:,en)*right_SlipSlip) &
+ matmul(prm%h_sl_tw,dot%gamma_tw(:,en))
dot%xi_tw(:,en) = prm%h_0_tw_sl * sum(stt%gamma_sl(:,en))**prm%c_3 &
* matmul(prm%h_tw_sl,dot%gamma_sl(:,en)) &
+ prm%h_0_tw_tw * sumF**prm%c_4 * matmul(prm%h_tw_tw,dot%gamma_tw(:,en))
end associate
end subroutine phenopowerlaw_dotState
!--------------------------------------------------------------------------------------------------
!> @brief Write results to HDF5 output file.
!--------------------------------------------------------------------------------------------------
module subroutine plastic_phenopowerlaw_results(ph,group)
integer, intent(in) :: ph
character(len=*), intent(in) :: group
integer :: o
associate(prm => param(ph), stt => state(ph))
outputsLoop: do o = 1,size(prm%output)
select case(trim(prm%output(o)))
case('xi_sl')
if(prm%sum_N_sl>0) call results_writeDataset(stt%xi_sl,group,trim(prm%output(o)), &
'resistance against plastic slip','Pa')
case('gamma_sl')
if(prm%sum_N_sl>0) call results_writeDataset(stt%gamma_sl,group,trim(prm%output(o)), &
'plastic shear','1')
case('xi_tw')
if(prm%sum_N_tw>0) call results_writeDataset(stt%xi_tw,group,trim(prm%output(o)), &
'resistance against twinning','Pa')
case('gamma_tw')
if(prm%sum_N_tw>0) call results_writeDataset(stt%gamma_tw,group,trim(prm%output(o)), &
'twinning shear','1')
end select
enddo outputsLoop
end associate
end subroutine plastic_phenopowerlaw_results
!--------------------------------------------------------------------------------------------------
!> @brief Calculate shear rates on slip systems and their derivatives with respect to resolved
! stress.
!> @details Derivatives are calculated only optionally.
! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
! have the optional arguments at the end.
!--------------------------------------------------------------------------------------------------
pure subroutine kinetics_sl(Mp,ph,en, &
dot_gamma_sl_pos,dot_gamma_sl_neg,ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
en
real(pReal), intent(out), dimension(param(ph)%sum_N_sl) :: &
dot_gamma_sl_pos, &
dot_gamma_sl_neg
real(pReal), intent(out), optional, dimension(param(ph)%sum_N_sl) :: &
ddot_gamma_dtau_sl_pos, &
ddot_gamma_dtau_sl_neg
real(pReal), dimension(param(ph)%sum_N_sl) :: &
tau_sl_pos, &
tau_sl_neg
integer :: i
associate(prm => param(ph), stt => state(ph))
do i = 1, prm%sum_N_sl
tau_sl_pos(i) = math_tensordot(Mp,prm%P_nS_pos(1:3,1:3,i))
tau_sl_neg(i) = merge(math_tensordot(Mp,prm%P_nS_neg(1:3,1:3,i)), &
0.0_pReal, prm%nonSchmidActive)
enddo
where(dNeq0(tau_sl_pos))
dot_gamma_sl_pos = prm%dot_gamma_0_sl * merge(0.5_pReal,1.0_pReal, prm%nonSchmidActive) & ! 1/2 if non-Schmid active
* sign(abs(tau_sl_pos/stt%xi_sl(:,en))**prm%n_sl, tau_sl_pos)
else where
dot_gamma_sl_pos = 0.0_pReal
end where
where(dNeq0(tau_sl_neg))
dot_gamma_sl_neg = prm%dot_gamma_0_sl * 0.5_pReal & ! only used if non-Schmid active, always 1/2
* sign(abs(tau_sl_neg/stt%xi_sl(:,en))**prm%n_sl, tau_sl_neg)
else where
dot_gamma_sl_neg = 0.0_pReal
end where
if (present(ddot_gamma_dtau_sl_pos)) then
where(dNeq0(dot_gamma_sl_pos))
ddot_gamma_dtau_sl_pos = dot_gamma_sl_pos*prm%n_sl/tau_sl_pos
else where
ddot_gamma_dtau_sl_pos = 0.0_pReal
end where
endif
if (present(ddot_gamma_dtau_sl_neg)) then
where(dNeq0(dot_gamma_sl_neg))
ddot_gamma_dtau_sl_neg = dot_gamma_sl_neg*prm%n_sl/tau_sl_neg
else where
ddot_gamma_dtau_sl_neg = 0.0_pReal
end where
endif
end associate
end subroutine kinetics_sl
!--------------------------------------------------------------------------------------------------
!> @brief Calculate shear rates on twin systems and their derivatives with respect to resolved
! stress. Twinning is assumed to take place only in untwinned volume.
!> @details Derivatives are calculated only optionally.
! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
! have the optional arguments at the end.
!--------------------------------------------------------------------------------------------------
pure subroutine kinetics_tw(Mp,ph,en,&
dot_gamma_tw,ddot_gamma_dtau_tw)
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
integer, intent(in) :: &
ph, &
en
real(pReal), dimension(param(ph)%sum_N_tw), intent(out) :: &
dot_gamma_tw
real(pReal), dimension(param(ph)%sum_N_tw), intent(out), optional :: &
ddot_gamma_dtau_tw
real(pReal), dimension(param(ph)%sum_N_tw) :: &
tau_tw
integer :: i
associate(prm => param(ph), stt => state(ph))
do i = 1, prm%sum_N_tw
tau_tw(i) = math_tensordot(Mp,prm%P_tw(1:3,1:3,i))
enddo
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
* prm%dot_gamma_0_tw*(abs(tau_tw)/stt%xi_tw(:,en))**prm%n_tw
else where
dot_gamma_tw = 0.0_pReal
end where
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
end where
endif
end associate
end subroutine kinetics_tw
end submodule phenopowerlaw