733 lines
33 KiB
Fortran
733 lines
33 KiB
Fortran
!--------------------------------------------------------------------------------------------------
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!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
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!> @brief phenomenological crystal plasticity formulation using a powerlaw fitting
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!--------------------------------------------------------------------------------------------------
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submodule(phase:plastic) phenopowerlaw
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use geometry_plastic_nonlocal, only: & !< Achal Copied from nonlocal
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nIPneighbors => geometry_plastic_nonlocal_nIPneighbors, &
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IPneighborhood => geometry_plastic_nonlocal_IPneighborhood, &
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IPvolume => geometry_plastic_nonlocal_IPvolume0, &
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IParea => geometry_plastic_nonlocal_IParea0, &
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IPareaNormal => geometry_plastic_nonlocal_IPareaNormal0, &
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geometry_plastic_nonlocal_disable
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type :: tGeometry
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real(pReal), dimension(:), allocatable :: V_0
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integer, dimension(:,:,:), allocatable :: IPneighborhood
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real(pReal), dimension(:,:), allocatable :: IParea, IPcoordinates
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real(pReal), dimension(:,:,:), allocatable :: IPareaNormal
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end type tGeometry
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type(tGeometry), dimension(:), allocatable :: geom
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type :: tParameters
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real(pReal) :: &
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dot_gamma_0_sl = 1.0_pReal, & !< reference shear strain rate for slip
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dot_gamma_0_tw = 1.0_pReal, & !< reference shear strain rate for twin
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n_sl = 1.0_pReal, & !< stress exponent for slip
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n_tw = 1.0_pReal, & !< stress exponent for twin
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f_sat_sl_tw = 1.0_pReal, & !< push-up factor for slip saturation due to twinning
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c_1 = 1.0_pReal, &
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c_2 = 1.0_pReal, &
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c_3 = 1.0_pReal, &
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c_4 = 1.0_pReal, &
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h_0_sl_sl = 1.0_pReal, & !< reference hardening slip - slip
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h_0_tw_sl = 1.0_pReal, & !< reference hardening twin - slip
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h_0_tw_tw = 1.0_pReal, & !< reference hardening twin - twin
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a_sl = 1.0_pReal
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real(pReal), allocatable, dimension(:) :: &
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xi_inf_sl, & !< maximum critical shear stress for slip
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h_int, & !< per family hardening activity (optional)
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gamma_char !< characteristic shear for twins
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real(pReal), allocatable, dimension(:,:) :: &
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h_sl_sl, & !< slip resistance from slip activity
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h_sl_tw, & !< slip resistance from twin activity
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h_tw_sl, & !< twin resistance from slip activity
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h_tw_tw !< twin resistance from twin activity
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real(pReal), allocatable, dimension(:,:,:) :: &
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P_sl, &
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P_tw, &
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P_nS_pos, &
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P_nS_neg, &
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CorrespondanceMatrix !< Achal
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integer :: &
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sum_N_sl, & !< total number of active slip system
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sum_N_tw !< total number of active twin systems
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logical :: &
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nonSchmidActive = .false.
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character(len=pStringLen), allocatable, dimension(:) :: &
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output
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character(len=:), allocatable, dimension(:) :: &
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systems_sl, &
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systems_tw
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end type tParameters
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type :: tIndexDotState
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integer, dimension(2) :: &
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xi_sl, &
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xi_tw, &
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gamma_sl, &
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gamma_tw, &
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f_twin !< Achal
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end type tIndexDotState
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type :: tPhenopowerlawState
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real(pReal), pointer, dimension(:,:) :: &
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xi_sl, &
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xi_tw, &
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gamma_sl, &
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gamma_tw, &
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f_twin !< Achal
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end type tPhenopowerlawState
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!--------------------------------------------------------------------------------------------------
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! containers for parameters, dot state index, and state
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type(tParameters), allocatable, dimension(:) :: param
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type(tIndexDotState), allocatable, dimension(:) :: indexDotState
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type(tPhenopowerlawState), allocatable, dimension(:) :: state, dotState, deltastate !< Achal. added deltastate
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contains
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!--------------------------------------------------------------------------------------------------
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!> @brief Perform module initialization.
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!> @details reads in material parameters, allocates arrays, and does sanity checks
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!--------------------------------------------------------------------------------------------------
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module function plastic_phenopowerlaw_init() result(myPlasticity)
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logical, dimension(:), allocatable :: myPlasticity
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integer :: &
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ph, i, o, &
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Nmembers, &
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sizeState, sizeDotState, sizeDeltaState, &
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startIndex, endIndex
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integer, dimension(:), allocatable :: &
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N_sl, N_tw
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real(pReal), dimension(:), allocatable :: &
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xi_0_sl, & !< initial critical shear stress for slip
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xi_0_tw, & !< initial critical shear stress for twin
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a !< non-Schmid coefficients
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character(len=pStringLen) :: &
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extmsg = ''
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class(tNode), pointer :: &
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phases, &
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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
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print'(/,1x,a)', '<<<+- phase:mechanical:plastic:phenopowerlaw init -+>>>'
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print'(/,a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
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phases => config_material%get('phase')
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allocate(geom(phases%length)) !< Achal
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allocate(param(phases%length))
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allocate(indexDotState(phases%length))
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allocate(state(phases%length))
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allocate(deltastate(phases%length)) !< Achal
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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), dot => dotState(ph), &
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idx_dot => indexDotState(ph))
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phase => phases%get(ph)
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mech => phase%get('mechanical')
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pl => mech%get('plastic')
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!--------------------------------------------------------------------------------------------------
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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))
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slipActive: if (prm%sum_N_sl > 0) then
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prm%systems_sl = lattice_labels_slip(N_sl,phase_lattice(ph))
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prm%P_sl = lattice_SchmidMatrix_slip(N_sl,phase_lattice(ph),phase_cOverA(ph))
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if (phase_lattice(ph) == 'cI') then
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a = pl%get_as1dFloat('a_nonSchmid',defaultVal=emptyRealArray)
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if(size(a) > 0) prm%nonSchmidActive = .true.
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prm%P_nS_pos = lattice_nonSchmidMatrix(N_sl,a,+1)
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prm%P_nS_neg = lattice_nonSchmidMatrix(N_sl,a,-1)
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else
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prm%P_nS_pos = prm%P_sl
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prm%P_nS_neg = prm%P_sl
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end if
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prm%h_sl_sl = lattice_interaction_SlipBySlip(N_sl,pl%get_as1dFloat('h_sl-sl'),phase_lattice(ph))
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xi_0_sl = pl%get_as1dFloat('xi_0_sl', requiredSize=size(N_sl))
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prm%xi_inf_sl = pl%get_as1dFloat('xi_inf_sl', requiredSize=size(N_sl))
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prm%h_int = pl%get_as1dFloat('h_int', requiredSize=size(N_sl), &
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defaultVal=[(0.0_pReal,i=1,size(N_sl))])
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prm%dot_gamma_0_sl = pl%get_asFloat('dot_gamma_0_sl')
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prm%n_sl = pl%get_asFloat('n_sl')
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prm%a_sl = pl%get_asFloat('a_sl')
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prm%h_0_sl_sl = pl%get_asFloat('h_0_sl-sl')
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! expand: family => system
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xi_0_sl = math_expand(xi_0_sl, N_sl)
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prm%xi_inf_sl = math_expand(prm%xi_inf_sl,N_sl)
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prm%h_int = math_expand(prm%h_int, N_sl)
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! sanity checks
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if ( prm%dot_gamma_0_sl <= 0.0_pReal) extmsg = trim(extmsg)//' dot_gamma_0_sl'
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if ( prm%a_sl <= 0.0_pReal) extmsg = trim(extmsg)//' a_sl'
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if ( prm%n_sl <= 0.0_pReal) extmsg = trim(extmsg)//' n_sl'
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if (any(xi_0_sl <= 0.0_pReal)) extmsg = trim(extmsg)//' xi_0_sl'
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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
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allocate(prm%xi_inf_sl,prm%h_int,source=emptyRealArray)
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allocate(prm%h_sl_sl(0,0))
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end if slipActive
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!--------------------------------------------------------------------------------------------------
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! twin related parameters
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N_tw = pl%get_as1dInt('N_tw', defaultVal=emptyIntArray)
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prm%sum_N_tw = sum(abs(N_tw))
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twinActive: if (prm%sum_N_tw > 0) then
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prm%systems_tw = lattice_labels_twin(N_tw,phase_lattice(ph))
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prm%P_tw = lattice_SchmidMatrix_twin(N_tw,phase_lattice(ph),phase_cOverA(ph))
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prm%h_tw_tw = lattice_interaction_TwinByTwin(N_tw,pl%get_as1dFloat('h_tw-tw'),phase_lattice(ph))
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prm%gamma_char = lattice_characteristicShear_twin(N_tw,phase_lattice(ph),phase_cOverA(ph))
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prm%CorrespondanceMatrix = lattice_CorrespondanceMatrix_twin(N_tw,phase_lattice(ph),phase_cOverA(ph)) !< Achal
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xi_0_tw = pl%get_as1dFloat('xi_0_tw',requiredSize=size(N_tw))
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prm%c_1 = pl%get_asFloat('c_1',defaultVal=0.0_pReal)
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prm%c_2 = pl%get_asFloat('c_2',defaultVal=1.0_pReal)
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prm%c_3 = pl%get_asFloat('c_3',defaultVal=0.0_pReal)
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prm%c_4 = pl%get_asFloat('c_4',defaultVal=0.0_pReal)
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prm%dot_gamma_0_tw = pl%get_asFloat('dot_gamma_0_tw')
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prm%n_tw = pl%get_asFloat('n_tw')
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prm%f_sat_sl_tw = pl%get_asFloat('f_sat_sl-tw')
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prm%h_0_tw_tw = pl%get_asFloat('h_0_tw-tw')
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! expand: family => system
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xi_0_tw = math_expand(xi_0_tw,N_tw)
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! sanity checks
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if (prm%dot_gamma_0_tw <= 0.0_pReal) extmsg = trim(extmsg)//' dot_gamma_0_tw'
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if (prm%n_tw <= 0.0_pReal) extmsg = trim(extmsg)//' n_tw'
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else twinActive
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xi_0_tw = emptyRealArray
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allocate(prm%gamma_char,source=emptyRealArray)
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allocate(prm%h_tw_tw(0,0))
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end if twinActive
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!--------------------------------------------------------------------------------------------------
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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
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prm%h_0_tw_sl = pl%get_asFloat('h_0_tw-sl') ! sanity checks
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prm%h_sl_tw = lattice_interaction_SlipByTwin(N_sl,N_tw,pl%get_as1dFloat('h_sl-tw'), &
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phase_lattice(ph))
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prm%h_tw_sl = lattice_interaction_TwinBySlip(N_tw,N_sl,pl%get_as1dFloat('h_tw-sl'), &
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phase_lattice(ph))
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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
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allocate(prm%h_tw_sl(prm%sum_N_tw,prm%sum_N_sl)) ! at least one dimension is 0
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prm%h_0_tw_sl = 0.0_pReal
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end if slipAndTwinActive
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!--------------------------------------------------------------------------------------------------
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! output pararameters
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#if defined (__GFORTRAN__)
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prm%output = output_as1dString(pl)
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#else
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prm%output = pl%get_as1dString('output',defaultVal=emptyStringArray)
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#endif
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!--------------------------------------------------------------------------------------------------
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! allocate state arrays
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Nmembers = count(material_phaseID == ph)
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sizeDotState = size(['xi_sl ','gamma_sl']) * prm%sum_N_sl &
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+ size(['xi_tw ','gamma_tw']) * prm%sum_N_tw &
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+ size(['xi_tw ','f_twin ']) * prm%sum_N_tw !Achal
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sizeState = sizeDotState
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!write(6,*)"size fn", sizeDotState ! Achal Delete
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sizeDeltaState = size(['xi_sl ','gamma_sl']) * prm%sum_N_sl & !Achal
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+ size(['xi_tw ','gamma_tw']) * prm%sum_N_tw &
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+ size(['xi_tw ','f_twin ']) * prm%sum_N_tw !Achal
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call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,sizeDeltaState)
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!deallocate(plasticState(ph)%dotState) ! ToDo: remove dotState completely !Achal, dot state needed!
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allocate(geom(ph)%V_0(Nmembers)) !Achal
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allocate(geom(ph)%IPneighborhood(3,nIPneighbors,Nmembers)) !Achal
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allocate(geom(ph)%IPareaNormal(3,nIPneighbors,Nmembers))
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allocate(geom(ph)%IParea(nIPneighbors,Nmembers))
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allocate(geom(ph)%IPcoordinates(3,Nmembers))
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call storeGeometry(ph) !Achal
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!--------------------------------------------------------------------------------------------------
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! state aliases and initialization
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startIndex = 1
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endIndex = prm%sum_N_sl
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idx_dot%xi_sl = [startIndex,endIndex]
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stt%xi_sl => plasticState(ph)%state(startIndex:endIndex,:)
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stt%xi_sl = spread(xi_0_sl, 2, Nmembers)
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plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_xi',defaultVal=1.0_pReal)
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if(any(plasticState(ph)%atol(startIndex:endIndex) < 0.0_pReal)) extmsg = trim(extmsg)//' atol_xi'
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startIndex = endIndex + 1
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endIndex = endIndex + prm%sum_N_tw
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idx_dot%xi_tw = [startIndex,endIndex]
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stt%xi_tw => plasticState(ph)%state(startIndex:endIndex,:)
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stt%xi_tw = spread(xi_0_tw, 2, Nmembers)
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plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_xi',defaultVal=1.0_pReal)
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startIndex = endIndex + 1
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endIndex = endIndex + prm%sum_N_sl
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idx_dot%gamma_sl = [startIndex,endIndex]
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stt%gamma_sl => plasticState(ph)%state(startIndex:endIndex,:)
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plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_gamma',defaultVal=1.0e-6_pReal)
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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
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idx_dot%gamma_tw = [startIndex,endIndex]
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stt%gamma_tw => plasticState(ph)%state(startIndex:endIndex,:)
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plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_gamma',defaultVal=1.0e-6_pReal)
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o = plasticState(ph)%offsetDeltaState
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startIndex = endIndex + 1 ! Achal
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endIndex = endIndex + prm%sum_N_tw ! Achal
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idx_dot%f_twin = [startIndex,endIndex] ! Achal
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stt%f_twin => plasticState(ph)%state(startIndex:endIndex,:) ! Achal
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!dot%f_twin => plasticState(ph)%dotState(startIndex:endIndex,:)
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deltastate(ph)%f_twin => plasticState(ph)%state(startIndex-o:endIndex-o,:) ! Achal
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plasticState(ph)%atol(startIndex:endIndex) = pl%get_asFloat('atol_gamma',defaultVal=1.0e-6_pReal)
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write(6,*)"index", startIndex ! Achal Delete
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end associate
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!--------------------------------------------------------------------------------------------------
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! exit if any parameter is out of range
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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
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate plastic velocity gradient and its tangent.
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!> @details asummes that deformation by dislocation glide affects twinned and untwinned volume
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! equally (Taylor assumption). Twinning happens only in untwinned volume
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!--------------------------------------------------------------------------------------------------
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pure module subroutine phenopowerlaw_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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ph, &
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en
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integer :: &
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i,k,l,m,n
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real(pReal), dimension(param(ph)%sum_N_sl) :: &
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dot_gamma_sl_pos,dot_gamma_sl_neg, &
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ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg
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real(pReal), dimension(param(ph)%sum_N_tw) :: &
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dot_gamma_tw,fdot_twin, ddot_gamma_dtau_tw
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Lp = 0.0_pReal
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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_pos,dot_gamma_sl_neg,ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg)
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slipSystems: do i = 1, prm%sum_N_sl
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Lp = Lp + (dot_gamma_sl_pos(i)+dot_gamma_sl_neg(i))*prm%P_sl(1:3,1:3,i)
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forall (k=1:3,l=1:3,m=1:3,n=1:3) &
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dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
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+ ddot_gamma_dtau_sl_pos(i) * prm%P_sl(k,l,i) * prm%P_nS_pos(m,n,i) &
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+ ddot_gamma_dtau_sl_neg(i) * prm%P_sl(k,l,i) * prm%P_nS_neg(m,n,i)
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end do slipSystems
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call kinetics_tw(Mp,ph,en,dot_gamma_tw,fdot_twin, ddot_gamma_dtau_tw) !< Achal, Skip Lp route, delete/comment
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twinSystems: do i = 1, prm%sum_N_tw !< Achal, Skip Lp route, delete/comment
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Lp = Lp + dot_gamma_tw(i)*prm%P_tw(1:3,1:3,i) !< Achal, Skip Lp route, delete/comment
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forall (k=1:3,l=1:3,m=1:3,n=1:3) & !< Achal, Skip Lp route, delete/comment
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dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
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+ ddot_gamma_dtau_tw(i)*prm%P_tw(k,l,i)*prm%P_tw(m,n,i)
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end do twinSystems
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end associate
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end subroutine phenopowerlaw_LpAndItsTangent
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate the rate of change of microstructure.
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!--------------------------------------------------------------------------------------------------
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module function phenopowerlaw_dotState(Mp,ph,en) result(dotState)
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real(pReal), dimension(3,3), intent(in) :: &
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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(plasticState(ph)%sizeDotState) :: &
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dotState
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real(pReal) :: &
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xi_sl_sat_offset,&
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sumF
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real(pReal), dimension(param(ph)%sum_N_sl) :: &
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dot_gamma_sl_pos,dot_gamma_sl_neg, &
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right_SlipSlip
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logical :: twinJump !delete this
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real(pReal), dimension(3,3) :: deltaFp !delete this
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associate(prm => param(ph), stt => state(ph), &
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dot_xi_sl => dotState(indexDotState(ph)%xi_sl(1):indexDotState(ph)%xi_sl(2)), &
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dot_xi_tw => dotState(indexDotState(ph)%xi_tw(1):indexDotState(ph)%xi_tw(2)), &
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dot_gamma_sl => dotState(indexDotState(ph)%gamma_sl(1):indexDotState(ph)%gamma_sl(2)), &
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dot_gamma_tw => dotState(indexDotState(ph)%gamma_tw(1):indexDotState(ph)%gamma_tw(2)), & !Achal)
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fdot_twin => dotState(indexDotState(ph)%f_twin(1):indexDotState(ph)%f_twin(2))) !Achal
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call kinetics_sl(Mp,ph,en,dot_gamma_sl_pos,dot_gamma_sl_neg)
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dot_gamma_sl = abs(dot_gamma_sl_pos+dot_gamma_sl_neg)
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call kinetics_tw(Mp,ph,en,dot_gamma_tw,fdot_twin)
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!if(en==1) call plastic_kinematic_deltaFp(Mp,ph,en,twinJump,deltaFp) ! delete this ! delete this
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!write(6,*)'deltaFp', deltaFp ! delete this
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!write(6,*)'characteristicShearTwin', prm%gamma_char
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!write(6,*)'Schmid_twin',prm%P_sl
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!if(en==1) write(6,*)'maxF',maxval(stt%gamma_tw(:,en)/prm%gamma_char) ! delete Achal
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!if(en==1) write(6,*)'f_twin',fdot_twin
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!if(en==1) write(6,*)'f_twin',f_twin
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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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right_SlipSlip = sign(abs(1.0_pReal-stt%xi_sl(:,en) / (prm%xi_inf_sl+xi_sl_sat_offset))**prm%a_sl, &
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1.0_pReal-stt%xi_sl(:,en) / (prm%xi_inf_sl+xi_sl_sat_offset))
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dot_xi_sl = prm%h_0_sl_sl * (1.0_pReal + prm%c_1*sumF** prm%c_2) * (1.0_pReal + prm%h_int) &
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* matmul(prm%h_sl_sl,dot_gamma_sl*right_SlipSlip) &
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+ 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 &
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* matmul(prm%h_tw_sl,dot_gamma_sl) &
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+ prm%h_0_tw_tw * sumF**prm%c_4 * matmul(prm%h_tw_tw,dot_gamma_tw)
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end associate
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end function phenopowerlaw_dotState
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates instantaneous incremental change of kinematics and associated jump state
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!> Satya, Achal
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!--------------------------------------------------------------------------------------------------
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module subroutine plastic_kinematic_deltaFp(Mp,ph,en,twinJump,deltaFp)
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use math, only: &
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math_I3
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real(pReal), dimension(3,3), intent(in) :: &
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Mp
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integer, intent(in) :: &
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ph, &
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en
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logical , intent(out) :: &
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twinJump
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real(pReal), dimension(3,3), intent(out) :: &
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deltaFp
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integer :: &
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n, & ! neighbor index
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en, &
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neighbor_e, & ! element index of my neighbor
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neighbor_i, & ! integration point index of my neighbor
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neighbor_me, &
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neighbor_phase
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real(pReal) :: &
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random, &
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nRealNeighbors !Achal number of really existing neighbors
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integer :: &
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twin_var
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real(pReal), dimension(param(ph)%sum_N_tw) :: &
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fdot_twin
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real(pReal), dimension(param(ph)%sum_N_tw) :: &
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tau_tw
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integer :: i
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twinJump = .false.
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deltaFp = math_I3
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!* loop through my neighborhood and get the connection vectors (in lattice frame) and the excess densities !Achal
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nRealNeighbors = 0.0_pReal !Achal
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neighbors: do n = 1,nIPneighbors
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neighbor_e = geom(ph)%IPneighborhood(1,n,en)
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neighbor_i = geom(ph)%IPneighborhood(2,n,en)
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neighbor_me = material_phaseEntry(1,(neighbor_e-1)*discretization_nIPs + neighbor_i) !Neighbour offset
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neighbor_phase = material_phaseID(1,(neighbor_e-1)*discretization_nIPs + neighbor_i)
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enddo neighbors
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tau_tw = [(math_tensordot(Mp,param(ph)%P_tw(1:3,1:3,i)),i=1,param(ph)%sum_N_tw)]
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twin_var = maxloc((0.05_pReal*(abs(tau_tw)/state(ph)%xi_tw(:,en))**param(ph)%n_tw)/param(ph)%gamma_char,dim=1) ! This prints values from 1 to 6, fdot0_twin is taken as 0.05
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fdot_twin = (0.05_pReal*(abs(tau_tw)/state(ph)%xi_tw(:,en))**param(ph)%n_tw)/param(ph)%gamma_char ! This is sometimes >1
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!write(6,*) 'twin_var', twin_var !delete this
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!if (en==1) write(6,*)'correspondanceMatrix1', param(ph)%CorrespondanceMatrix(:,:,1) !delete this !delete this
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call RANDOM_NUMBER(random)
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!write(6,*)'random',random !delete this
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Success_Growth: if (random*0.0000000000000000000000001_pReal <= maxval((0.05_pReal*(abs(tau_tw) &
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/state(ph)%xi_tw(:,en))**param(ph)%n_tw)/param(ph)%gamma_char)) then ! Instead of sum take max
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twinJump = .true.
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deltaFp = param(ph)%CorrespondanceMatrix(:,:,twin_var)
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deltastate(ph)%f_twin(:,en) = 0.0_pReal - state(ph)%f_twin(:,en)
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end if Success_Growth
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end subroutine plastic_kinematic_deltaFp
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates (instantaneous) incremental change of microstructure
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!> Satya, Achal
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!--------------------------------------------------------------------------------------------------
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module subroutine plastic_phenopowerlaw_deltaState(ph,en)
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implicit none
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integer, intent(in)::&
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ph, &
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en
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deltastate(ph)%f_twin=1.0_pReal
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end subroutine plastic_phenopowerlaw_deltaState
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!--------------------------------------------------------------------------------------------------
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!> @brief Write results to HDF5 output file.
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!--------------------------------------------------------------------------------------------------
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module subroutine plastic_phenopowerlaw_results(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)
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select case(trim(prm%output(ou)))
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case('xi_sl')
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call results_writeDataset(stt%xi_sl,group,trim(prm%output(ou)), &
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'resistance against plastic slip','Pa',prm%systems_sl)
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case('gamma_sl')
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call results_writeDataset(stt%gamma_sl,group,trim(prm%output(ou)), &
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'plastic shear','1',prm%systems_sl)
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case('xi_tw')
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call results_writeDataset(stt%xi_tw,group,trim(prm%output(ou)), &
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'resistance against twinning','Pa',prm%systems_tw)
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case('gamma_tw')
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call results_writeDataset(stt%gamma_tw,group,trim(prm%output(ou)), &
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'twinning shear','1',prm%systems_tw)
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end select
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end do
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end associate
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end subroutine plastic_phenopowerlaw_results
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate shear rates on slip systems and their derivatives with respect to resolved
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! stress.
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!> @details Derivatives are calculated only optionally.
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! NOTE: Against the common convention, the result (i.e. intent(out)) variables are the last to
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! have the optional arguments at the end.
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!--------------------------------------------------------------------------------------------------
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pure subroutine kinetics_sl(Mp,ph,en, &
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dot_gamma_sl_pos,dot_gamma_sl_neg,ddot_gamma_dtau_sl_pos,ddot_gamma_dtau_sl_neg)
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real(pReal), dimension(3,3), intent(in) :: &
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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), intent(out), dimension(param(ph)%sum_N_sl) :: &
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dot_gamma_sl_pos, &
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dot_gamma_sl_neg
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real(pReal), intent(out), optional, dimension(param(ph)%sum_N_sl) :: &
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ddot_gamma_dtau_sl_pos, &
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ddot_gamma_dtau_sl_neg
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real(pReal), dimension(param(ph)%sum_N_sl) :: &
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tau_sl_pos, &
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tau_sl_neg
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integer :: i
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associate(prm => param(ph), stt => state(ph))
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do i = 1, prm%sum_N_sl
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tau_sl_pos(i) = math_tensordot(Mp,prm%P_nS_pos(1:3,1:3,i))
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tau_sl_neg(i) = merge(math_tensordot(Mp,prm%P_nS_neg(1:3,1:3,i)), &
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0.0_pReal, prm%nonSchmidActive)
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end do
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|
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where(dNeq0(tau_sl_pos))
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dot_gamma_sl_pos = prm%dot_gamma_0_sl * merge(0.5_pReal,1.0_pReal, prm%nonSchmidActive) & ! 1/2 if non-Schmid active
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* sign(abs(tau_sl_pos/stt%xi_sl(:,en))**prm%n_sl, tau_sl_pos)
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else where
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dot_gamma_sl_pos = 0.0_pReal
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end where
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where(dNeq0(tau_sl_neg))
|
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dot_gamma_sl_neg = prm%dot_gamma_0_sl * 0.5_pReal & ! only used if non-Schmid active, always 1/2
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* sign(abs(tau_sl_neg/stt%xi_sl(:,en))**prm%n_sl, tau_sl_neg)
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else where
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dot_gamma_sl_neg = 0.0_pReal
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end where
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|
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if (present(ddot_gamma_dtau_sl_pos)) then
|
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where(dNeq0(dot_gamma_sl_pos))
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ddot_gamma_dtau_sl_pos = dot_gamma_sl_pos*prm%n_sl/tau_sl_pos
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else where
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ddot_gamma_dtau_sl_pos = 0.0_pReal
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end where
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end if
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if (present(ddot_gamma_dtau_sl_neg)) then
|
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where(dNeq0(dot_gamma_sl_neg))
|
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ddot_gamma_dtau_sl_neg = dot_gamma_sl_neg*prm%n_sl/tau_sl_neg
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else where
|
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ddot_gamma_dtau_sl_neg = 0.0_pReal
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end where
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end if
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end associate
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end subroutine kinetics_sl
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|
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!--------------------------------------------------------------------------------------------------
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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 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,&
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dot_gamma_tw, fdot_twin, ddot_gamma_dtau_tw) !< Achal added fdot
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|
|
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real(pReal), dimension(3,3), intent(in) :: &
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|
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_tw), intent(out) :: &
|
|
dot_gamma_tw, fdot_twin
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|
real(pReal), dimension(param(ph)%sum_N_tw), intent(out), optional :: &
|
|
ddot_gamma_dtau_tw
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|
|
real(pReal), dimension(param(ph)%sum_N_tw) :: &
|
|
tau_tw
|
|
integer :: i
|
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|
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associate(prm => param(ph), stt => state(ph))
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|
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tau_tw = [(math_tensordot(Mp,prm%P_tw(1:3,1:3,i)),i=1,prm%sum_N_tw)]
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|
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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*(abs(tau_tw)/stt%xi_tw(:,en))**prm%n_tw
|
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fdot_twin = (0.05_pReal*(abs(tau_tw)/state(ph)%xi_tw(:,en))**param(ph)%n_tw)/param(ph)%gamma_char
|
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else where
|
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dot_gamma_tw = 0.0_pReal
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end where
|
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|
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if (present(ddot_gamma_dtau_tw)) then
|
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where(dNeq0(dot_gamma_tw))
|
|
ddot_gamma_dtau_tw = dot_gamma_tw*prm%n_tw/tau_tw
|
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else where
|
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ddot_gamma_dtau_tw = 0.0_pReal
|
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end where
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end if
|
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end associate
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|
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end subroutine kinetics_tw
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|
|
!--------------------------------------------------------------------------------------------------
|
|
!> Achal: Added from nonlocal
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
subroutine storeGeometry(ph)
|
|
|
|
integer, intent(in) :: ph
|
|
|
|
integer :: ce, co, nCell
|
|
real(pReal), dimension(:), allocatable :: V
|
|
integer, dimension(:,:,:), allocatable :: neighborhood
|
|
real(pReal), dimension(:,:), allocatable :: area, coords
|
|
real(pReal), dimension(:,:,:), allocatable :: areaNormal
|
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|
|
nCell = product(shape(IPvolume))
|
|
|
|
V = reshape(IPvolume,[nCell])
|
|
neighborhood = reshape(IPneighborhood,[3,nIPneighbors,nCell])
|
|
area = reshape(IParea,[nIPneighbors,nCell])
|
|
areaNormal = reshape(IPareaNormal,[3,nIPneighbors,nCell])
|
|
coords = reshape(discretization_IPcoords,[3,nCell])
|
|
|
|
do ce = 1, size(material_homogenizationEntry,1)
|
|
do co = 1, homogenization_maxNconstituents
|
|
if (material_phaseID(co,ce) == ph) then
|
|
geom(ph)%V_0(material_phaseEntry(co,ce)) = V(ce)
|
|
geom(ph)%IPneighborhood(:,:,material_phaseEntry(co,ce)) = neighborhood(:,:,ce)
|
|
geom(ph)%IParea(:,material_phaseEntry(co,ce)) = area(:,ce)
|
|
geom(ph)%IPareaNormal(:,:,material_phaseEntry(co,ce)) = areaNormal(:,:,ce)
|
|
geom(ph)%IPcoordinates(:,material_phaseEntry(co,ce)) = coords(:,ce)
|
|
end if
|
|
end do
|
|
end do
|
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|
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end subroutine
|
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|
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end submodule phenopowerlaw
|