1156 lines
56 KiB
Fortran
1156 lines
56 KiB
Fortran
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!--------------------------------------------------------------------------------------------------
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!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Su Leen Wong, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Nan Jia, Max-Planck-Institut für Eisenforschung GmbH
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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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!> @brief material subroutine incoprorating dislocation and twinning physics
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!> @details to be done
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!--------------------------------------------------------------------------------------------------
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submodule(constitutive) plastic_dislotwin
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real(pReal), parameter :: &
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kB = 1.38e-23_pReal !< Boltzmann constant in J/Kelvin
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enum, bind(c)
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enumerator :: &
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undefined_ID, &
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rho_mob_ID, &
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rho_dip_ID, &
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dot_gamma_sl_ID, &
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gamma_sl_ID, &
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Lambda_sl_ID, &
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resolved_stress_slip_ID, &
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tau_pass_ID, &
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edge_dipole_distance_ID, &
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f_tw_ID, &
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Lambda_tw_ID, &
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resolved_stress_twin_ID, &
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tau_hat_tw_ID, &
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f_tr_ID
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end enum
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type :: tParameters
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real(pReal) :: &
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mu, &
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nu, &
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D0, & !< prefactor for self-diffusion coefficient
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Qsd, & !< activation energy for dislocation climb
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omega, & !< frequency factor for dislocation climb
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D, & !< grain size
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p_sb, & !< p-exponent in shear band velocity
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q_sb, & !< q-exponent in shear band velocity
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CEdgeDipMinDistance, & !<
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i_tw, & !<
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tau_0, & !< strength due to elements in solid solution
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L_tw, & !< Length of twin nuclei in Burgers vectors
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L_tr, & !< Length of trans nuclei in Burgers vectors
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xc_twin, & !< critical distance for formation of twin nucleus
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xc_trans, & !< critical distance for formation of trans nucleus
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V_cs, & !< cross slip volume
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sbResistance, & !< value for shearband resistance (might become an internal state variable at some point)
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sbVelocity, & !< value for shearband velocity_0
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sbQedge, & !< activation energy for shear bands
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SFE_0K, & !< stacking fault energy at zero K
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dSFE_dT, & !< temperature dependance of stacking fault energy
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aTol_rho, & !< absolute tolerance for integration of dislocation density
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aTol_f_tw, & !< absolute tolerance for integration of twin volume fraction
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aTol_f_tr, & !< absolute tolerance for integration of trans volume fraction
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gamma_fcc_hex, & !< Free energy difference between austensite and martensite
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i_tr, & !<
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h !< Stack height of hex nucleus
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real(pReal), dimension(:), allocatable :: &
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rho_mob_0, & !< initial unipolar dislocation density per slip system
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rho_dip_0, & !< initial dipole dislocation density per slip system
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b_sl, & !< absolute length of burgers vector [m] for each slip system
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b_tw, & !< absolute length of burgers vector [m] for each twin system
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b_tr, & !< absolute length of burgers vector [m] for each transformation system
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Delta_F,& !< activation energy for glide [J] for each slip system
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v0, & !< dislocation velocity prefactor [m/s] for each slip system
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dot_N_0_tw, & !< twin nucleation rate [1/m³s] for each twin system
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dot_N_0_tr, & !< trans nucleation rate [1/m³s] for each trans system
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t_tw, & !< twin thickness [m] for each twin system
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CLambdaSlip, & !< Adj. parameter for distance between 2 forest dislocations for each slip system
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atomicVolume, &
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t_tr, & !< martensite lamellar thickness [m] for each trans system and instance
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p, & !< p-exponent in glide velocity
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q, & !< q-exponent in glide velocity
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r, & !< r-exponent in twin nucleation rate
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s, & !< s-exponent in trans nucleation rate
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gamma_char, & !< characteristic shear for twins
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B !< drag coefficient
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real(pReal), dimension(:,:), allocatable :: &
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h_sl_sl, & !<
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h_sl_tw, & !<
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h_tw_tw, & !<
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h_sl_tr, & !<
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h_tr_tr !<
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integer, dimension(:,:), allocatable :: &
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fcc_twinNucleationSlipPair ! ToDo: Better name? Is also use for trans
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real(pReal), dimension(:,:), allocatable :: &
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n0_sl, & !< slip system normal
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forestProjection, &
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C66
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real(pReal), dimension(:,:,:), allocatable :: &
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P_tr, &
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P_sl, &
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P_tw, &
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C66_tw, &
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C66_tr
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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 system
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sum_N_tr !< total number of active transformation system
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integer, dimension(:), allocatable :: &
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N_sl, & !< number of active slip systems for each family
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N_tw, & !< number of active twin systems for each family
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N_tr !< number of active transformation systems for each family
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integer(kind(undefined_ID)), dimension(:), allocatable :: &
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outputID !< ID of each post result output
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logical :: &
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ExtendedDislocations, & !< consider split into partials for climb calculation
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fccTwinTransNucleation, & !< twinning and transformation models are for fcc
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dipoleFormation !< flag indicating consideration of dipole formation
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end type !< container type for internal constitutive parameters
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type :: tDislotwinState
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real(pReal), dimension(:,:), pointer :: &
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rho_mob, &
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rho_dip, &
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gamma_sl, &
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f_tw, &
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f_tr
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end type tDislotwinState
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type :: tDislotwinMicrostructure
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real(pReal), dimension(:,:), allocatable :: &
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Lambda_sl, & !< mean free path between 2 obstacles seen by a moving dislocation
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Lambda_tw, & !< mean free path between 2 obstacles seen by a growing twin
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Lambda_tr, & !< mean free path between 2 obstacles seen by a growing martensite
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tau_pass, &
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tau_hat_tw, &
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tau_hat_tr, &
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V_tw, & !< volume of a new twin
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V_tr, & !< volume of a new martensite disc
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tau_r_tw, & !< stress to bring partials close together (twin)
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tau_r_tr !< stress to bring partials close together (trans)
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end type tDislotwinMicrostructure
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!--------------------------------------------------------------------------------------------------
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! containers for parameters and state
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type(tParameters), allocatable, dimension(:) :: param
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type(tDislotwinState), allocatable, dimension(:) :: &
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dotState, &
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state
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type(tDislotwinMicrostructure), allocatable, dimension(:) :: dependentState
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contains
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!--------------------------------------------------------------------------------------------------
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!> @brief 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 subroutine plastic_dislotwin_init
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integer :: &
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Ninstance, &
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p, i, &
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NipcMyPhase, outputSize, &
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sizeState, sizeDotState, &
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startIndex, endIndex
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integer(kind(undefined_ID)) :: &
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outputID
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character(len=pStringLen) :: &
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extmsg = ''
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character(len=pStringLen), dimension(:), allocatable :: &
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outputs
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write(6,'(/,a)') ' <<<+- constitutive_'//PLASTICITY_DISLOTWIN_label//' init -+>>>'
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write(6,'(/,a)') ' Ma and Roters, Acta Materialia 52(12):3603–3612, 2004'
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write(6,'(a)') ' https://doi.org/10.1016/j.actamat.2004.04.012'
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write(6,'(/,a)') ' Roters et al., Computational Materials Science 39:91–95, 2007'
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write(6,'(a)') ' https://doi.org/10.1016/j.commatsci.2006.04.014'
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write(6,'(/,a)') ' Wong et al., Acta Materialia 118:140–151, 2016'
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write(6,'(a,/)') ' https://doi.org/10.1016/j.actamat.2016.07.032'
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Ninstance = count(phase_plasticity == PLASTICITY_DISLOTWIN_ID)
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if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0) &
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write(6,'(a16,1x,i5,/)') '# instances:',Ninstance
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allocate(param(Ninstance))
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allocate(state(Ninstance))
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allocate(dotState(Ninstance))
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allocate(dependentState(Ninstance))
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do p = 1, size(phase_plasticity)
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if (phase_plasticity(p) /= PLASTICITY_DISLOTWIN_ID) cycle
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associate(prm => param(phase_plasticityInstance(p)), &
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dot => dotState(phase_plasticityInstance(p)), &
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stt => state(phase_plasticityInstance(p)), &
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dst => dependentState(phase_plasticityInstance(p)), &
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config => config_phase(p))
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prm%aTol_rho = config%getFloat('atol_rho', defaultVal=0.0_pReal)
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prm%aTol_f_tw = config%getFloat('atol_twinfrac', defaultVal=0.0_pReal)
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prm%aTol_f_tr = config%getFloat('atol_transfrac', defaultVal=0.0_pReal)
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! This data is read in already in lattice
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prm%mu = lattice_mu(p)
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prm%nu = lattice_nu(p)
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prm%C66 = lattice_C66(1:6,1:6,p)
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!--------------------------------------------------------------------------------------------------
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! slip related parameters
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prm%N_sl = config%getInts('nslip',defaultVal=emptyIntArray)
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prm%sum_N_sl = sum(prm%N_sl)
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slipActive: if (prm%sum_N_sl > 0) then
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prm%P_sl = lattice_SchmidMatrix_slip(prm%N_sl,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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prm%h_sl_sl = lattice_interaction_SlipBySlip(prm%N_sl, &
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config%getFloats('interaction_slipslip'), &
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config%getString('lattice_structure'))
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prm%forestProjection = lattice_forestProjection_edge(prm%N_sl,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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prm%forestProjection = transpose(prm%forestProjection)
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prm%n0_sl = lattice_slip_normal(prm%N_sl,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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prm%fccTwinTransNucleation = merge(.true., .false., lattice_structure(p) == LATTICE_FCC_ID) &
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.and. (prm%N_sl(1) == 12)
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if(prm%fccTwinTransNucleation) &
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prm%fcc_twinNucleationSlipPair = lattice_fcc_twinNucleationSlipPair
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prm%rho_mob_0 = config%getFloats('rhoedge0', requiredSize=size(prm%N_sl))
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prm%rho_dip_0 = config%getFloats('rhoedgedip0',requiredSize=size(prm%N_sl))
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prm%v0 = config%getFloats('v0', requiredSize=size(prm%N_sl))
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prm%b_sl = config%getFloats('slipburgers',requiredSize=size(prm%N_sl))
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prm%Delta_F = config%getFloats('qedge', requiredSize=size(prm%N_sl))
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prm%CLambdaSlip = config%getFloats('clambdaslip',requiredSize=size(prm%N_sl))
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prm%p = config%getFloats('p_slip', requiredSize=size(prm%N_sl))
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prm%q = config%getFloats('q_slip', requiredSize=size(prm%N_sl))
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prm%B = config%getFloats('b', requiredSize=size(prm%N_sl), &
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defaultVal=[(0.0_pReal, i=1,size(prm%N_sl))])
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prm%tau_0 = config%getFloat('solidsolutionstrength')
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prm%CEdgeDipMinDistance = config%getFloat('cedgedipmindistance')
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prm%D0 = config%getFloat('d0')
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prm%Qsd = config%getFloat('qsd')
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prm%atomicVolume = config%getFloat('catomicvolume') * prm%b_sl**3.0_pReal
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prm%ExtendedDislocations = config%keyExists('/extend_dislocations/')
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if (prm%ExtendedDislocations) then
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prm%SFE_0K = config%getFloat('sfe_0k')
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prm%dSFE_dT = config%getFloat('dsfe_dt')
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endif
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! multiplication factor according to crystal structure (nearest neighbors bcc vs fcc/hex)
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!@details: Refer: Argon & Moffat, Acta Metallurgica, Vol. 29, pg 293 to 299, 1981
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prm%omega = config%getFloat('omega', defaultVal = 1000.0_pReal) &
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* merge(12.0_pReal, &
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8.0_pReal, &
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lattice_structure(p) == LATTICE_FCC_ID .or. lattice_structure(p) == LATTICE_HEX_ID)
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! expand: family => system
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prm%rho_mob_0 = math_expand(prm%rho_mob_0, prm%N_sl)
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prm%rho_dip_0 = math_expand(prm%rho_dip_0, prm%N_sl)
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prm%v0 = math_expand(prm%v0, prm%N_sl)
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prm%b_sl = math_expand(prm%b_sl, prm%N_sl)
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prm%Delta_F = math_expand(prm%Delta_F, prm%N_sl)
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prm%CLambdaSlip = math_expand(prm%CLambdaSlip, prm%N_sl)
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prm%p = math_expand(prm%p, prm%N_sl)
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prm%q = math_expand(prm%q, prm%N_sl)
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prm%B = math_expand(prm%B, prm%N_sl)
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prm%atomicVolume = math_expand(prm%atomicVolume,prm%N_sl)
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! sanity checks
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if ( prm%D0 <= 0.0_pReal) extmsg = trim(extmsg)//' D0'
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if ( prm%Qsd <= 0.0_pReal) extmsg = trim(extmsg)//' Qsd'
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if (any(prm%rho_mob_0 < 0.0_pReal)) extmsg = trim(extmsg)//' rho_mob_0'
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if (any(prm%rho_dip_0 < 0.0_pReal)) extmsg = trim(extmsg)//' rho_dip_0'
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if (any(prm%v0 < 0.0_pReal)) extmsg = trim(extmsg)//' v0'
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if (any(prm%b_sl <= 0.0_pReal)) extmsg = trim(extmsg)//' b_sl'
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if (any(prm%Delta_F <= 0.0_pReal)) extmsg = trim(extmsg)//' Delta_F'
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if (any(prm%CLambdaSlip <= 0.0_pReal)) extmsg = trim(extmsg)//' CLambdaSlip'
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if (any(prm%B < 0.0_pReal)) extmsg = trim(extmsg)//' B'
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if (any(prm%p<=0.0_pReal .or. prm%p>1.0_pReal)) extmsg = trim(extmsg)//' p'
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if (any(prm%q< 1.0_pReal .or. prm%q>2.0_pReal)) extmsg = trim(extmsg)//' q'
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else slipActive
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allocate(prm%b_sl(0))
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endif slipActive
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!--------------------------------------------------------------------------------------------------
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! twin related parameters
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prm%N_tw = config%getInts('ntwin', defaultVal=emptyIntArray)
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prm%sum_N_tw = sum(prm%N_tw)
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if (prm%sum_N_tw > 0) then
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prm%P_tw = lattice_SchmidMatrix_twin(prm%N_tw,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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prm%h_tw_tw = lattice_interaction_TwinByTwin(prm%N_tw,&
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config%getFloats('interaction_twintwin'), &
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config%getString('lattice_structure'))
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prm%b_tw = config%getFloats('twinburgers', requiredSize=size(prm%N_tw))
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prm%t_tw = config%getFloats('twinsize', requiredSize=size(prm%N_tw))
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prm%r = config%getFloats('r_twin', requiredSize=size(prm%N_tw))
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prm%xc_twin = config%getFloat('xc_twin')
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prm%L_tw = config%getFloat('l0_twin')
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prm%i_tw = config%getFloat('cmfptwin')
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prm%gamma_char= lattice_characteristicShear_Twin(prm%N_tw,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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prm%C66_tw = lattice_C66_twin(prm%N_tw,prm%C66,config%getString('lattice_structure'),&
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config%getFloat('c/a',defaultVal=0.0_pReal))
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if (.not. prm%fccTwinTransNucleation) then
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prm%dot_N_0_tw = config%getFloats('ndot0_twin')
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prm%dot_N_0_tw = math_expand(prm%dot_N_0_tw,prm%N_tw)
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endif
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|
! expand: family => system
|
|||
|
prm%b_tw = math_expand(prm%b_tw,prm%N_tw)
|
|||
|
prm%t_tw = math_expand(prm%t_tw,prm%N_tw)
|
|||
|
prm%r = math_expand(prm%r,prm%N_tw)
|
|||
|
|
|||
|
else
|
|||
|
allocate(prm%gamma_char(0))
|
|||
|
allocate(prm%t_tw (0))
|
|||
|
allocate(prm%b_tw (0))
|
|||
|
allocate(prm%r (0))
|
|||
|
allocate(prm%h_tw_tw (0,0))
|
|||
|
endif
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
! transformation related parameters
|
|||
|
prm%N_tr = config%getInts('ntrans', defaultVal=emptyIntArray)
|
|||
|
prm%sum_N_tr = sum(prm%N_tr)
|
|||
|
if (prm%sum_N_tr > 0) then
|
|||
|
prm%b_tr = config%getFloats('transburgers')
|
|||
|
prm%b_tr = math_expand(prm%b_tr,prm%N_tr)
|
|||
|
|
|||
|
prm%h = config%getFloat('transstackheight', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|||
|
prm%i_tr = config%getFloat('cmfptrans', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|||
|
prm%gamma_fcc_hex = config%getFloat('deltag')
|
|||
|
prm%xc_trans = config%getFloat('xc_trans', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|||
|
prm%L_tr = config%getFloat('l0_trans')
|
|||
|
|
|||
|
prm%h_tr_tr = lattice_interaction_TransByTrans(prm%N_tr,&
|
|||
|
config%getFloats('interaction_transtrans'), &
|
|||
|
config%getString('lattice_structure'))
|
|||
|
|
|||
|
prm%C66_tr = lattice_C66_trans(prm%N_tr,prm%C66, &
|
|||
|
config%getString('trans_lattice_structure'), &
|
|||
|
0.0_pReal, &
|
|||
|
config%getFloat('a_bcc', defaultVal=0.0_pReal), &
|
|||
|
config%getFloat('a_fcc', defaultVal=0.0_pReal))
|
|||
|
|
|||
|
prm%P_tr = lattice_SchmidMatrix_trans(prm%N_tr, &
|
|||
|
config%getString('trans_lattice_structure'), &
|
|||
|
0.0_pReal, &
|
|||
|
config%getFloat('a_bcc', defaultVal=0.0_pReal), &
|
|||
|
config%getFloat('a_fcc', defaultVal=0.0_pReal))
|
|||
|
|
|||
|
if (lattice_structure(p) /= LATTICE_fcc_ID) then
|
|||
|
prm%dot_N_0_tr = config%getFloats('ndot0_trans')
|
|||
|
prm%dot_N_0_tr = math_expand(prm%dot_N_0_tr,prm%N_tr)
|
|||
|
endif
|
|||
|
prm%t_tr = config%getFloats('lamellarsize')
|
|||
|
prm%t_tr = math_expand(prm%t_tr,prm%N_tr)
|
|||
|
prm%s = config%getFloats('s_trans',defaultVal=[0.0_pReal])
|
|||
|
prm%s = math_expand(prm%s,prm%N_tr)
|
|||
|
else
|
|||
|
allocate(prm%t_tr (0))
|
|||
|
allocate(prm%b_tr (0))
|
|||
|
allocate(prm%s (0))
|
|||
|
allocate(prm%h_tr_tr(0,0))
|
|||
|
endif
|
|||
|
|
|||
|
if (sum(prm%N_tw) > 0 .or. prm%sum_N_tr > 0) then
|
|||
|
prm%SFE_0K = config%getFloat('sfe_0k')
|
|||
|
prm%dSFE_dT = config%getFloat('dsfe_dt')
|
|||
|
prm%V_cs = config%getFloat('vcrossslip')
|
|||
|
endif
|
|||
|
|
|||
|
if (prm%sum_N_sl > 0 .and. prm%sum_N_tw > 0) then
|
|||
|
prm%h_sl_tw = lattice_interaction_SlipByTwin(prm%N_sl,prm%N_tw,&
|
|||
|
config%getFloats('interaction_sliptwin'), &
|
|||
|
config%getString('lattice_structure'))
|
|||
|
if (prm%fccTwinTransNucleation .and. prm%sum_N_tw > 12) write(6,*) 'mist' ! ToDo: implement better test. The model will fail also if N_tw is [6,6]
|
|||
|
endif
|
|||
|
|
|||
|
if (prm%sum_N_sl > 0 .and. prm%sum_N_tr > 0) then
|
|||
|
prm%h_sl_tr = lattice_interaction_SlipByTrans(prm%N_sl,prm%N_tr,&
|
|||
|
config%getFloats('interaction_sliptrans'), &
|
|||
|
config%getString('lattice_structure'))
|
|||
|
if (prm%fccTwinTransNucleation .and. prm%sum_N_tr > 12) write(6,*) 'mist' ! ToDo: implement better test. The model will fail also if N_tr is [6,6]
|
|||
|
endif
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
! shearband related parameters
|
|||
|
prm%sbVelocity = config%getFloat('shearbandvelocity',defaultVal=0.0_pReal)
|
|||
|
if (prm%sbVelocity > 0.0_pReal) then
|
|||
|
prm%sbResistance = config%getFloat('shearbandresistance')
|
|||
|
prm%sbQedge = config%getFloat('qedgepersbsystem')
|
|||
|
prm%p_sb = config%getFloat('p_shearband')
|
|||
|
prm%q_sb = config%getFloat('q_shearband')
|
|||
|
|
|||
|
! sanity checks
|
|||
|
if (prm%sbResistance < 0.0_pReal) extmsg = trim(extmsg)//' shearbandresistance'
|
|||
|
if (prm%sbQedge < 0.0_pReal) extmsg = trim(extmsg)//' qedgepersbsystem'
|
|||
|
if (prm%p_sb <= 0.0_pReal) extmsg = trim(extmsg)//' p_shearband'
|
|||
|
if (prm%q_sb <= 0.0_pReal) extmsg = trim(extmsg)//' q_shearband'
|
|||
|
endif
|
|||
|
|
|||
|
|
|||
|
|
|||
|
prm%D = config%getFloat('grainsize')
|
|||
|
|
|||
|
if (config%keyExists('dipoleformationfactor')) call IO_error(1,ext_msg='use /nodipoleformation/')
|
|||
|
prm%dipoleformation = .not. config%keyExists('/nodipoleformation/')
|
|||
|
|
|||
|
|
|||
|
!if (Ndot0PerTwinFamily(f,p) < 0.0_pReal) &
|
|||
|
! call IO_error(211,el=p,ext_msg='dot_N_0_tw ('//PLASTICITY_DISLOTWIN_label//')')
|
|||
|
|
|||
|
if (any(prm%atomicVolume <= 0.0_pReal)) &
|
|||
|
call IO_error(211,el=p,ext_msg='cAtomicVolume ('//PLASTICITY_DISLOTWIN_label//')')
|
|||
|
if (prm%sum_N_tw > 0) then
|
|||
|
if (prm%aTol_rho <= 0.0_pReal) &
|
|||
|
call IO_error(211,el=p,ext_msg='aTol_rho ('//PLASTICITY_DISLOTWIN_label//')')
|
|||
|
if (prm%aTol_f_tw <= 0.0_pReal) &
|
|||
|
call IO_error(211,el=p,ext_msg='aTol_f_tw ('//PLASTICITY_DISLOTWIN_label//')')
|
|||
|
endif
|
|||
|
if (prm%sum_N_tr > 0) then
|
|||
|
if (prm%aTol_f_tr <= 0.0_pReal) &
|
|||
|
call IO_error(211,el=p,ext_msg='aTol_f_tr ('//PLASTICITY_DISLOTWIN_label//')')
|
|||
|
endif
|
|||
|
|
|||
|
outputs = config%getStrings('(output)', defaultVal=emptyStringArray)
|
|||
|
allocate(prm%outputID(0))
|
|||
|
do i= 1, size(outputs)
|
|||
|
outputID = undefined_ID
|
|||
|
select case(outputs(i))
|
|||
|
case ('rho_mob')
|
|||
|
outputID = merge(rho_mob_ID,undefined_ID,prm%sum_N_sl > 0)
|
|||
|
outputSize = prm%sum_N_sl
|
|||
|
case ('rho_dip')
|
|||
|
outputID = merge(rho_dip_ID,undefined_ID,prm%sum_N_sl > 0)
|
|||
|
outputSize = prm%sum_N_sl
|
|||
|
case ('gamma_sl')
|
|||
|
outputID = merge(gamma_sl_ID,undefined_ID,prm%sum_N_sl > 0)
|
|||
|
outputSize = prm%sum_N_sl
|
|||
|
case ('lambda_sl')
|
|||
|
outputID = merge(Lambda_sl_ID,undefined_ID,prm%sum_N_sl > 0)
|
|||
|
outputSize = prm%sum_N_sl
|
|||
|
case ('tau_pass')
|
|||
|
outputID= merge(tau_pass_ID,undefined_ID,prm%sum_N_sl > 0)
|
|||
|
outputSize = prm%sum_N_sl
|
|||
|
|
|||
|
case ('f_tw')
|
|||
|
outputID = merge(f_tw_ID,undefined_ID,prm%sum_N_tw >0)
|
|||
|
outputSize = prm%sum_N_tw
|
|||
|
case ('lambda_tw')
|
|||
|
outputID = merge(Lambda_tw_ID,undefined_ID,prm%sum_N_tw >0)
|
|||
|
outputSize = prm%sum_N_tw
|
|||
|
case ('tau_hat_tw')
|
|||
|
outputID = merge(tau_hat_tw_ID,undefined_ID,prm%sum_N_tw >0)
|
|||
|
outputSize = prm%sum_N_tw
|
|||
|
|
|||
|
case ('f_tr')
|
|||
|
outputID = f_tr_ID
|
|||
|
outputSize = prm%sum_N_tr
|
|||
|
|
|||
|
end select
|
|||
|
|
|||
|
if (outputID /= undefined_ID) then
|
|||
|
prm%outputID = [prm%outputID, outputID]
|
|||
|
endif
|
|||
|
|
|||
|
enddo
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
! allocate state arrays
|
|||
|
NipcMyPhase = count(material_phaseAt == p) * discretization_nIP
|
|||
|
sizeDotState = size(['rho_mob ','rho_dip ','gamma_sl']) * prm%sum_N_sl &
|
|||
|
+ size(['f_tw']) * prm%sum_N_tw &
|
|||
|
+ size(['f_tr']) * prm%sum_N_tr
|
|||
|
sizeState = sizeDotState
|
|||
|
|
|||
|
call material_allocatePlasticState(p,NipcMyPhase,sizeState,sizeDotState,0)
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
! locally defined state aliases and initialization of state0 and aTolState
|
|||
|
startIndex = 1
|
|||
|
endIndex = prm%sum_N_sl
|
|||
|
stt%rho_mob=>plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
stt%rho_mob= spread(prm%rho_mob_0,2,NipcMyPhase)
|
|||
|
dot%rho_mob=>plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_rho
|
|||
|
|
|||
|
startIndex = endIndex + 1
|
|||
|
endIndex = endIndex + prm%sum_N_sl
|
|||
|
stt%rho_dip=>plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
stt%rho_dip= spread(prm%rho_dip_0,2,NipcMyPhase)
|
|||
|
dot%rho_dip=>plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_rho
|
|||
|
|
|||
|
startIndex = endIndex + 1
|
|||
|
endIndex = endIndex + prm%sum_N_sl
|
|||
|
stt%gamma_sl=>plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
dot%gamma_sl=>plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%aTolState(startIndex:endIndex) = 1.0e6_pReal !ToDo: better make optional parameter
|
|||
|
! global alias
|
|||
|
plasticState(p)%slipRate => plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%accumulatedSlip => plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
|
|||
|
startIndex = endIndex + 1
|
|||
|
endIndex = endIndex + prm%sum_N_tw
|
|||
|
stt%f_tw=>plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
dot%f_tw=>plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_f_tw
|
|||
|
|
|||
|
startIndex = endIndex + 1
|
|||
|
endIndex = endIndex + prm%sum_N_tr
|
|||
|
stt%f_tr=>plasticState(p)%state(startIndex:endIndex,:)
|
|||
|
dot%f_tr=>plasticState(p)%dotState(startIndex:endIndex,:)
|
|||
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_f_tr
|
|||
|
|
|||
|
allocate(dst%Lambda_sl (prm%sum_N_sl,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%tau_pass (prm%sum_N_sl,NipcMyPhase),source=0.0_pReal)
|
|||
|
|
|||
|
allocate(dst%Lambda_tw (prm%sum_N_tw,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%tau_hat_tw (prm%sum_N_tw,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%tau_r_tw (prm%sum_N_tw,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%V_tw (prm%sum_N_tw,NipcMyPhase),source=0.0_pReal)
|
|||
|
|
|||
|
allocate(dst%Lambda_tr (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%tau_hat_tr (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%tau_r_tr (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|||
|
allocate(dst%V_tr (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|||
|
|
|||
|
|
|||
|
plasticState(p)%state0 = plasticState(p)%state ! ToDo: this could be done centrally
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
enddo
|
|||
|
|
|||
|
end subroutine plastic_dislotwin_init
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief returns the homogenized elasticity matrix
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
module function plastic_dislotwin_homogenizedC(ipc,ip,el) result(homogenizedC)
|
|||
|
|
|||
|
real(pReal), dimension(6,6) :: &
|
|||
|
homogenizedC
|
|||
|
integer, intent(in) :: &
|
|||
|
ipc, & !< component-ID of integration point
|
|||
|
ip, & !< integration point
|
|||
|
el !< element
|
|||
|
|
|||
|
integer :: i, &
|
|||
|
of
|
|||
|
real(pReal) :: f_unrotated
|
|||
|
|
|||
|
of = material_phasememberAt(ipc,ip,el)
|
|||
|
associate(prm => param(phase_plasticityInstance(material_phaseAt(ipc,el))),&
|
|||
|
stt => state(phase_plasticityInstance(material_phaseAT(ipc,el))))
|
|||
|
|
|||
|
f_unrotated = 1.0_pReal &
|
|||
|
- sum(stt%f_tw(1:prm%sum_N_tw,of)) &
|
|||
|
- sum(stt%f_tr(1:prm%sum_N_tr,of))
|
|||
|
|
|||
|
homogenizedC = f_unrotated * prm%C66
|
|||
|
do i=1,prm%sum_N_tw
|
|||
|
homogenizedC = homogenizedC &
|
|||
|
+ stt%f_tw(i,of)*prm%C66_tw(1:6,1:6,i)
|
|||
|
enddo
|
|||
|
do i=1,prm%sum_N_tr
|
|||
|
homogenizedC = homogenizedC &
|
|||
|
+ stt%f_tr(i,of)*prm%C66_tr(1:6,1:6,i)
|
|||
|
enddo
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
end function plastic_dislotwin_homogenizedC
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief calculates plastic velocity gradient and its tangent
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
module subroutine plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,T,instance,of)
|
|||
|
|
|||
|
real(pReal), dimension(3,3), intent(out) :: Lp
|
|||
|
real(pReal), dimension(3,3,3,3), intent(out) :: dLp_dMp
|
|||
|
real(pReal), dimension(3,3), intent(in) :: Mp
|
|||
|
integer, intent(in) :: instance,of
|
|||
|
real(pReal), intent(in) :: T
|
|||
|
|
|||
|
integer :: i,k,l,m,n
|
|||
|
real(pReal) :: f_unrotated,StressRatio_p,&
|
|||
|
BoltzmannRatio, &
|
|||
|
ddot_gamma_dtau, &
|
|||
|
tau
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|||
|
dot_gamma_sl,ddot_gamma_dtau_slip
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
|||
|
dot_gamma_twin,ddot_gamma_dtau_twin
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
|||
|
dot_gamma_tr,ddot_gamma_dtau_trans
|
|||
|
real(pReal):: dot_gamma_sb
|
|||
|
real(pReal), dimension(3,3) :: eigVectors, P_sb
|
|||
|
real(pReal), dimension(3) :: eigValues
|
|||
|
logical :: error
|
|||
|
real(pReal), dimension(3,6), parameter :: &
|
|||
|
sb_sComposition = &
|
|||
|
reshape(real([&
|
|||
|
1, 0, 1, &
|
|||
|
1, 0,-1, &
|
|||
|
1, 1, 0, &
|
|||
|
1,-1, 0, &
|
|||
|
0, 1, 1, &
|
|||
|
0, 1,-1 &
|
|||
|
],pReal),[ 3,6]), &
|
|||
|
sb_mComposition = &
|
|||
|
reshape(real([&
|
|||
|
1, 0,-1, &
|
|||
|
1, 0,+1, &
|
|||
|
1,-1, 0, &
|
|||
|
1, 1, 0, &
|
|||
|
0, 1,-1, &
|
|||
|
0, 1, 1 &
|
|||
|
],pReal),[ 3,6])
|
|||
|
|
|||
|
associate(prm => param(instance), stt => state(instance))
|
|||
|
|
|||
|
f_unrotated = 1.0_pReal &
|
|||
|
- sum(stt%f_tw(1:prm%sum_N_tw,of)) &
|
|||
|
- sum(stt%f_tr(1:prm%sum_N_tr,of))
|
|||
|
|
|||
|
Lp = 0.0_pReal
|
|||
|
dLp_dMp = 0.0_pReal
|
|||
|
|
|||
|
call kinetics_slip(Mp,T,instance,of,dot_gamma_sl,ddot_gamma_dtau_slip)
|
|||
|
slipContribution: do i = 1, prm%sum_N_sl
|
|||
|
Lp = Lp + dot_gamma_sl(i)*prm%P_sl(1:3,1:3,i)
|
|||
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
|||
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
|||
|
+ ddot_gamma_dtau_slip(i) * prm%P_sl(k,l,i) * prm%P_sl(m,n,i)
|
|||
|
enddo slipContribution
|
|||
|
|
|||
|
!ToDo: Why do this before shear banding?
|
|||
|
Lp = Lp * f_unrotated
|
|||
|
dLp_dMp = dLp_dMp * f_unrotated
|
|||
|
|
|||
|
shearBandingContribution: if(dNeq0(prm%sbVelocity)) then
|
|||
|
|
|||
|
BoltzmannRatio = prm%sbQedge/(kB*T)
|
|||
|
call math_eigenValuesVectorsSym(Mp,eigValues,eigVectors,error)
|
|||
|
|
|||
|
do i = 1,6
|
|||
|
P_sb = 0.5_pReal * math_outer(matmul(eigVectors,sb_sComposition(1:3,i)),&
|
|||
|
matmul(eigVectors,sb_mComposition(1:3,i)))
|
|||
|
tau = math_mul33xx33(Mp,P_sb)
|
|||
|
|
|||
|
significantShearBandStress: if (abs(tau) > tol_math_check) then
|
|||
|
StressRatio_p = (abs(tau)/prm%sbResistance)**prm%p_sb
|
|||
|
dot_gamma_sb = sign(prm%sbVelocity*exp(-BoltzmannRatio*(1-StressRatio_p)**prm%q_sb), tau)
|
|||
|
ddot_gamma_dtau = abs(dot_gamma_sb)*BoltzmannRatio* prm%p_sb*prm%q_sb/ prm%sbResistance &
|
|||
|
* (abs(tau)/prm%sbResistance)**(prm%p_sb-1.0_pReal) &
|
|||
|
* (1.0_pReal-StressRatio_p)**(prm%q_sb-1.0_pReal)
|
|||
|
|
|||
|
Lp = Lp + dot_gamma_sb * P_sb
|
|||
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
|||
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
|||
|
+ ddot_gamma_dtau * P_sb(k,l) * P_sb(m,n)
|
|||
|
endif significantShearBandStress
|
|||
|
enddo
|
|||
|
|
|||
|
endif shearBandingContribution
|
|||
|
|
|||
|
call kinetics_twin(Mp,T,dot_gamma_sl,instance,of,dot_gamma_twin,ddot_gamma_dtau_twin)
|
|||
|
twinContibution: do i = 1, prm%sum_N_tw
|
|||
|
Lp = Lp + dot_gamma_twin(i)*prm%P_tw(1:3,1:3,i) * f_unrotated
|
|||
|
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_twin(i)* prm%P_tw(k,l,i)*prm%P_tw(m,n,i) * f_unrotated
|
|||
|
enddo twinContibution
|
|||
|
|
|||
|
call kinetics_trans(Mp,T,dot_gamma_sl,instance,of,dot_gamma_tr,ddot_gamma_dtau_trans)
|
|||
|
transContibution: do i = 1, prm%sum_N_tr
|
|||
|
Lp = Lp + dot_gamma_tr(i)*prm%P_tr(1:3,1:3,i) * f_unrotated
|
|||
|
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_trans(i)* prm%P_tr(k,l,i)*prm%P_tr(m,n,i) * f_unrotated
|
|||
|
enddo transContibution
|
|||
|
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
end subroutine plastic_dislotwin_LpAndItsTangent
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief calculates the rate of change of microstructure
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
module subroutine plastic_dislotwin_dotState(Mp,T,instance,of)
|
|||
|
|
|||
|
real(pReal), dimension(3,3), intent(in):: &
|
|||
|
Mp !< Mandel stress
|
|||
|
real(pReal), intent(in) :: &
|
|||
|
T !< temperature at integration point
|
|||
|
integer, intent(in) :: &
|
|||
|
instance, &
|
|||
|
of
|
|||
|
|
|||
|
integer :: i
|
|||
|
real(pReal) :: &
|
|||
|
f_unrotated, &
|
|||
|
VacancyDiffusion, &
|
|||
|
rho_dip_distance, &
|
|||
|
v_cl, & !< climb velocity
|
|||
|
Gamma, & !< stacking fault energy
|
|||
|
tau, &
|
|||
|
sigma_cl, & !< climb stress
|
|||
|
b_d !< ratio of burgers vector to stacking fault width
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|||
|
dot_rho_dip_formation, &
|
|||
|
dot_rho_dip_climb, &
|
|||
|
rho_dip_distance_min, &
|
|||
|
dot_gamma_sl
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
|||
|
dot_gamma_twin
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
|||
|
dot_gamma_tr
|
|||
|
|
|||
|
associate(prm => param(instance), stt => state(instance), &
|
|||
|
dot => dotState(instance), dst => dependentState(instance))
|
|||
|
|
|||
|
f_unrotated = 1.0_pReal &
|
|||
|
- sum(stt%f_tw(1:prm%sum_N_tw,of)) &
|
|||
|
- sum(stt%f_tr(1:prm%sum_N_tr,of))
|
|||
|
VacancyDiffusion = prm%D0*exp(-prm%Qsd/(kB*T))
|
|||
|
|
|||
|
call kinetics_slip(Mp,T,instance,of,dot_gamma_sl)
|
|||
|
dot%gamma_sl(:,of) = abs(dot_gamma_sl)
|
|||
|
|
|||
|
rho_dip_distance_min = prm%CEdgeDipMinDistance*prm%b_sl
|
|||
|
|
|||
|
slipState: do i = 1, prm%sum_N_sl
|
|||
|
tau = math_mul33xx33(Mp,prm%P_sl(1:3,1:3,i))
|
|||
|
|
|||
|
significantSlipStress: if (dEq0(tau)) then
|
|||
|
dot_rho_dip_formation(i) = 0.0_pReal
|
|||
|
dot_rho_dip_climb(i) = 0.0_pReal
|
|||
|
else significantSlipStress
|
|||
|
rho_dip_distance = 3.0_pReal*prm%mu*prm%b_sl(i)/(16.0_pReal*PI*abs(tau))
|
|||
|
rho_dip_distance = math_clip(rho_dip_distance, right = dst%Lambda_sl(i,of))
|
|||
|
rho_dip_distance = math_clip(rho_dip_distance, left = rho_dip_distance_min(i))
|
|||
|
|
|||
|
if (prm%dipoleFormation) then
|
|||
|
dot_rho_dip_formation(i) = 2.0_pReal*(rho_dip_distance-rho_dip_distance_min(i))/prm%b_sl(i) &
|
|||
|
* stt%rho_mob(i,of)*abs(dot_gamma_sl(i))
|
|||
|
else
|
|||
|
dot_rho_dip_formation(i) = 0.0_pReal
|
|||
|
endif
|
|||
|
|
|||
|
if (dEq(rho_dip_distance,rho_dip_distance_min(i))) then
|
|||
|
dot_rho_dip_climb(i) = 0.0_pReal
|
|||
|
else
|
|||
|
!@details: Refer: Argon & Moffat, Acta Metallurgica, Vol. 29, pg 293 to 299, 1981
|
|||
|
sigma_cl = dot_product(prm%n0_sl(1:3,i),matmul(Mp,prm%n0_sl(1:3,i)))
|
|||
|
if (prm%ExtendedDislocations) then
|
|||
|
Gamma = prm%SFE_0K + prm%dSFE_dT * T
|
|||
|
b_d = 24.0_pReal*PI*(1.0_pReal - prm%nu)/(2.0_pReal + prm%nu)* Gamma/(prm%mu*prm%b_sl(i))
|
|||
|
else
|
|||
|
b_d = 1.0_pReal
|
|||
|
endif
|
|||
|
v_cl = 2.0_pReal*prm%omega*b_d**2.0_pReal*exp(-prm%Qsd/(kB*T)) &
|
|||
|
* (exp(abs(sigma_cl)*prm%b_sl(i)**3.0_pReal/(kB*T)) - 1.0_pReal)
|
|||
|
|
|||
|
dot_rho_dip_climb(i) = 4.0_pReal*v_cl*stt%rho_dip(i,of) &
|
|||
|
/ (rho_dip_distance-rho_dip_distance_min(i))
|
|||
|
endif
|
|||
|
endif significantSlipStress
|
|||
|
enddo slipState
|
|||
|
|
|||
|
dot%rho_mob(:,of) = abs(dot_gamma_sl)/(prm%b_sl*dst%Lambda_sl(:,of)) &
|
|||
|
- dot_rho_dip_formation &
|
|||
|
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_mob(:,of)*abs(dot_gamma_sl)
|
|||
|
|
|||
|
dot%rho_dip(:,of) = dot_rho_dip_formation &
|
|||
|
- 2.0_pReal*rho_dip_distance_min/prm%b_sl * stt%rho_dip(:,of)*abs(dot_gamma_sl) &
|
|||
|
- dot_rho_dip_climb
|
|||
|
|
|||
|
call kinetics_twin(Mp,T,dot_gamma_sl,instance,of,dot_gamma_twin)
|
|||
|
dot%f_tw(:,of) = f_unrotated*dot_gamma_twin/prm%gamma_char
|
|||
|
|
|||
|
call kinetics_trans(Mp,T,dot_gamma_sl,instance,of,dot_gamma_tr)
|
|||
|
dot%f_tr(:,of) = f_unrotated*dot_gamma_tr
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
end subroutine plastic_dislotwin_dotState
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief calculates derived quantities from state
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
module subroutine plastic_dislotwin_dependentState(T,instance,of)
|
|||
|
|
|||
|
integer, intent(in) :: &
|
|||
|
instance, &
|
|||
|
of
|
|||
|
real(pReal), intent(in) :: &
|
|||
|
T
|
|||
|
|
|||
|
real(pReal) :: &
|
|||
|
sumf_twin,Gamma,sumf_trans
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|||
|
inv_lambda_sl_sl, & !< 1/mean free distance between 2 forest dislocations seen by a moving dislocation
|
|||
|
inv_lambda_sl_tw, & !< 1/mean free distance between 2 twin stacks from different systems seen by a moving dislocation
|
|||
|
inv_lambda_sl_tr !< 1/mean free distance between 2 martensite lamellar from different systems seen by a moving dislocation
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
|||
|
inv_lambda_tw_tw, & !< 1/mean free distance between 2 twin stacks from different systems seen by a growing twin
|
|||
|
f_over_t_tw
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
|||
|
inv_lambda_tr_tr, & !< 1/mean free distance between 2 martensite stacks from different systems seen by a growing martensite
|
|||
|
f_over_t_tr
|
|||
|
real(pReal), dimension(:), allocatable :: &
|
|||
|
x0
|
|||
|
|
|||
|
|
|||
|
associate(prm => param(instance),&
|
|||
|
stt => state(instance),&
|
|||
|
dst => dependentState(instance))
|
|||
|
|
|||
|
sumf_twin = sum(stt%f_tw(1:prm%sum_N_tw,of))
|
|||
|
sumf_trans = sum(stt%f_tr(1:prm%sum_N_tr,of))
|
|||
|
|
|||
|
Gamma = prm%SFE_0K + prm%dSFE_dT * T
|
|||
|
|
|||
|
!* rescaled volume fraction for topology
|
|||
|
f_over_t_tw = stt%f_tw(1:prm%sum_N_tw,of)/prm%t_tw ! this is per system ...
|
|||
|
f_over_t_tr = sumf_trans/prm%t_tr ! but this not
|
|||
|
! ToDo ...Physically correct, but naming could be adjusted
|
|||
|
|
|||
|
inv_lambda_sl_sl = sqrt(matmul(prm%forestProjection, &
|
|||
|
stt%rho_mob(:,of)+stt%rho_dip(:,of)))/prm%CLambdaSlip
|
|||
|
|
|||
|
if (prm%sum_N_tw > 0 .and. prm%sum_N_sl > 0) &
|
|||
|
inv_lambda_sl_tw = matmul(prm%h_sl_tw,f_over_t_tw)/(1.0_pReal-sumf_twin)
|
|||
|
|
|||
|
inv_lambda_tw_tw = matmul(prm%h_tw_tw,f_over_t_tw)/(1.0_pReal-sumf_twin)
|
|||
|
|
|||
|
if (prm%sum_N_tr > 0 .and. prm%sum_N_sl > 0) &
|
|||
|
inv_lambda_sl_tr = matmul(prm%h_sl_tr,f_over_t_tr)/(1.0_pReal-sumf_trans)
|
|||
|
|
|||
|
inv_lambda_tr_tr = matmul(prm%h_tr_tr,f_over_t_tr)/(1.0_pReal-sumf_trans)
|
|||
|
|
|||
|
if ((prm%sum_N_tw > 0) .or. (prm%sum_N_tr > 0)) then ! ToDo: better logic needed here
|
|||
|
dst%Lambda_sl(:,of) = prm%D &
|
|||
|
/ (1.0_pReal+prm%D*(inv_lambda_sl_sl + inv_lambda_sl_tw + inv_lambda_sl_tr))
|
|||
|
else
|
|||
|
dst%Lambda_sl(:,of) = prm%D &
|
|||
|
/ (1.0_pReal+prm%D*inv_lambda_sl_sl) !!!!!! correct?
|
|||
|
endif
|
|||
|
|
|||
|
dst%Lambda_tw(:,of) = prm%i_tw*prm%D/(1.0_pReal+prm%D*inv_lambda_tw_tw)
|
|||
|
dst%Lambda_tr(:,of) = prm%i_tr*prm%D/(1.0_pReal+prm%D*inv_lambda_tr_tr)
|
|||
|
|
|||
|
!* threshold stress for dislocation motion
|
|||
|
dst%tau_pass(:,of) = prm%mu*prm%b_sl* sqrt(matmul(prm%h_sl_sl,stt%rho_mob(:,of)+stt%rho_dip(:,of)))
|
|||
|
|
|||
|
!* threshold stress for growing twin/martensite
|
|||
|
if(prm%sum_N_tw == prm%sum_N_sl) &
|
|||
|
dst%tau_hat_tw(:,of) = Gamma/(3.0_pReal*prm%b_tw) &
|
|||
|
+ 3.0_pReal*prm%b_tw*prm%mu/(prm%L_tw*prm%b_sl) ! slip burgers here correct?
|
|||
|
if(prm%sum_N_tr == prm%sum_N_sl) &
|
|||
|
dst%tau_hat_tr(:,of) = Gamma/(3.0_pReal*prm%b_tr) &
|
|||
|
+ 3.0_pReal*prm%b_tr*prm%mu/(prm%L_tr*prm%b_sl) & ! slip burgers here correct?
|
|||
|
+ prm%h*prm%gamma_fcc_hex/ (3.0_pReal*prm%b_tr)
|
|||
|
|
|||
|
dst%V_tw(:,of) = (PI/4.0_pReal)*prm%t_tw*dst%Lambda_tw(:,of)**2.0_pReal
|
|||
|
dst%V_tr(:,of) = (PI/4.0_pReal)*prm%t_tr*dst%Lambda_tr(:,of)**2.0_pReal
|
|||
|
|
|||
|
|
|||
|
x0 = prm%mu*prm%b_tw**2.0_pReal/(Gamma*8.0_pReal*PI)*(2.0_pReal+prm%nu)/(1.0_pReal-prm%nu) ! ToDo: In the paper, this is the burgers vector for slip and is the same for twin and trans
|
|||
|
dst%tau_r_tw(:,of) = prm%mu*prm%b_tw/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%xc_twin)+cos(pi/3.0_pReal)/x0)
|
|||
|
|
|||
|
x0 = prm%mu*prm%b_tr**2.0_pReal/(Gamma*8.0_pReal*PI)*(2.0_pReal+prm%nu)/(1.0_pReal-prm%nu) ! ToDo: In the paper, this is the burgers vector for slip
|
|||
|
dst%tau_r_tr(:,of) = prm%mu*prm%b_tr/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%xc_trans)+cos(pi/3.0_pReal)/x0)
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
end subroutine plastic_dislotwin_dependentState
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief writes results to HDF5 output file
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
module subroutine plastic_dislotwin_results(instance,group)
|
|||
|
|
|||
|
integer, intent(in) :: instance
|
|||
|
character(len=*), intent(in) :: group
|
|||
|
integer :: o
|
|||
|
|
|||
|
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
|
|||
|
outputsLoop: do o = 1,size(prm%outputID)
|
|||
|
select case(prm%outputID(o))
|
|||
|
|
|||
|
case (rho_mob_ID)
|
|||
|
call results_writeDataset(group,stt%rho_mob,'rho_mob',&
|
|||
|
'mobile dislocation density','1/m²')
|
|||
|
case (rho_dip_ID)
|
|||
|
call results_writeDataset(group,stt%rho_dip,'rho_dip',&
|
|||
|
'dislocation dipole density''1/m²')
|
|||
|
case (gamma_sl_ID)
|
|||
|
call results_writeDataset(group,stt%gamma_sl,'gamma_sl',&
|
|||
|
'plastic shear','1')
|
|||
|
case (Lambda_sl_ID)
|
|||
|
call results_writeDataset(group,dst%Lambda_sl,'Lambda_sl',&
|
|||
|
'mean free path for slip','m')
|
|||
|
case (tau_pass_ID)
|
|||
|
call results_writeDataset(group,dst%tau_pass,'tau_pass',&
|
|||
|
'passing stress for slip','Pa')
|
|||
|
|
|||
|
case (f_tw_ID)
|
|||
|
call results_writeDataset(group,stt%f_tw,'f_tw',&
|
|||
|
'twinned volume fraction','m³/m³')
|
|||
|
case (Lambda_tw_ID)
|
|||
|
call results_writeDataset(group,dst%Lambda_tw,'Lambda_tw',&
|
|||
|
'mean free path for twinning','m')
|
|||
|
case (tau_hat_tw_ID)
|
|||
|
call results_writeDataset(group,dst%tau_hat_tw,'tau_hat_tw',&
|
|||
|
'threshold stress for twinning','Pa')
|
|||
|
|
|||
|
case (f_tr_ID)
|
|||
|
call results_writeDataset(group,stt%f_tr,'f_tr',&
|
|||
|
'martensite volume fraction','m³/m³')
|
|||
|
|
|||
|
end select
|
|||
|
enddo outputsLoop
|
|||
|
end associate
|
|||
|
|
|||
|
end subroutine plastic_dislotwin_results
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief Shear rates on slip systems, their derivatives with respect to resolved stress and the
|
|||
|
! resolved stresss
|
|||
|
!> @details Derivatives and resolved stress 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_slip(Mp,T,instance,of, &
|
|||
|
dot_gamma_sl,ddot_gamma_dtau_slip,tau_slip)
|
|||
|
|
|||
|
real(pReal), dimension(3,3), intent(in) :: &
|
|||
|
Mp !< Mandel stress
|
|||
|
real(pReal), intent(in) :: &
|
|||
|
T !< temperature
|
|||
|
integer, intent(in) :: &
|
|||
|
instance, &
|
|||
|
of
|
|||
|
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl), intent(out) :: &
|
|||
|
dot_gamma_sl
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl), optional, intent(out) :: &
|
|||
|
ddot_gamma_dtau_slip, &
|
|||
|
tau_slip
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|||
|
ddot_gamma_dtau
|
|||
|
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|||
|
tau, &
|
|||
|
stressRatio, &
|
|||
|
StressRatio_p, &
|
|||
|
BoltzmannRatio, &
|
|||
|
v_wait_inverse, & !< inverse of the effective velocity of a dislocation waiting at obstacles (unsigned)
|
|||
|
v_run_inverse, & !< inverse of the velocity of a free moving dislocation (unsigned)
|
|||
|
dV_wait_inverse_dTau, &
|
|||
|
dV_run_inverse_dTau, &
|
|||
|
dV_dTau, &
|
|||
|
tau_eff !< effective resolved stress
|
|||
|
integer :: i
|
|||
|
|
|||
|
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
|
|||
|
|
|||
|
do i = 1, prm%sum_N_sl
|
|||
|
tau(i) = math_mul33xx33(Mp,prm%P_sl(1:3,1:3,i))
|
|||
|
enddo
|
|||
|
|
|||
|
tau_eff = abs(tau)-dst%tau_pass(:,of)
|
|||
|
|
|||
|
significantStress: where(tau_eff > tol_math_check)
|
|||
|
stressRatio = tau_eff/prm%tau_0
|
|||
|
StressRatio_p = stressRatio** prm%p
|
|||
|
BoltzmannRatio = prm%Delta_F/(kB*T)
|
|||
|
v_wait_inverse = prm%v0**(-1.0_pReal) * exp(BoltzmannRatio*(1.0_pReal-StressRatio_p)** prm%q)
|
|||
|
v_run_inverse = prm%B/(tau_eff*prm%b_sl)
|
|||
|
|
|||
|
dot_gamma_sl = sign(stt%rho_mob(:,of)*prm%b_sl/(v_wait_inverse+v_run_inverse),tau)
|
|||
|
|
|||
|
dV_wait_inverse_dTau = -1.0_pReal * v_wait_inverse * prm%p * prm%q * BoltzmannRatio &
|
|||
|
* (stressRatio**(prm%p-1.0_pReal)) &
|
|||
|
* (1.0_pReal-StressRatio_p)**(prm%q-1.0_pReal) &
|
|||
|
/ prm%tau_0
|
|||
|
dV_run_inverse_dTau = -1.0_pReal * v_run_inverse/tau_eff
|
|||
|
dV_dTau = -1.0_pReal * (dV_wait_inverse_dTau+dV_run_inverse_dTau) &
|
|||
|
/ (v_wait_inverse+v_run_inverse)**2.0_pReal
|
|||
|
ddot_gamma_dtau = dV_dTau*stt%rho_mob(:,of)*prm%b_sl
|
|||
|
else where significantStress
|
|||
|
dot_gamma_sl = 0.0_pReal
|
|||
|
ddot_gamma_dtau = 0.0_pReal
|
|||
|
end where significantStress
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
if(present(ddot_gamma_dtau_slip)) ddot_gamma_dtau_slip = ddot_gamma_dtau
|
|||
|
if(present(tau_slip)) tau_slip = tau
|
|||
|
|
|||
|
end subroutine kinetics_slip
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief calculates shear rates on twin systems
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
pure subroutine kinetics_twin(Mp,T,dot_gamma_sl,instance,of,&
|
|||
|
dot_gamma_twin,ddot_gamma_dtau_twin)
|
|||
|
|
|||
|
real(pReal), dimension(3,3), intent(in) :: &
|
|||
|
Mp !< Mandel stress
|
|||
|
real(pReal), intent(in) :: &
|
|||
|
T !< temperature
|
|||
|
integer, intent(in) :: &
|
|||
|
instance, &
|
|||
|
of
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl), intent(in) :: &
|
|||
|
dot_gamma_sl
|
|||
|
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tw), intent(out) :: &
|
|||
|
dot_gamma_twin
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tw), optional, intent(out) :: &
|
|||
|
ddot_gamma_dtau_twin
|
|||
|
|
|||
|
real, dimension(param(instance)%sum_N_tw) :: &
|
|||
|
tau, &
|
|||
|
Ndot0, &
|
|||
|
stressRatio_r, &
|
|||
|
ddot_gamma_dtau
|
|||
|
|
|||
|
integer :: i,s1,s2
|
|||
|
|
|||
|
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
|
|||
|
|
|||
|
do i = 1, prm%sum_N_tw
|
|||
|
tau(i) = math_mul33xx33(Mp,prm%P_tw(1:3,1:3,i))
|
|||
|
isFCC: if (prm%fccTwinTransNucleation) then
|
|||
|
s1=prm%fcc_twinNucleationSlipPair(1,i)
|
|||
|
s2=prm%fcc_twinNucleationSlipPair(2,i)
|
|||
|
if (tau(i) < dst%tau_r_tw(i,of)) then ! ToDo: correct?
|
|||
|
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,of)+stt%rho_dip(s2,of))+&
|
|||
|
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,of)+stt%rho_dip(s1,of)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
|
|||
|
(prm%L_tw*prm%b_sl(i))*&
|
|||
|
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tw(i,of)-tau(i)))) ! P_ncs
|
|||
|
else
|
|||
|
Ndot0=0.0_pReal
|
|||
|
end if
|
|||
|
else isFCC
|
|||
|
Ndot0=prm%dot_N_0_tw(i)
|
|||
|
endif isFCC
|
|||
|
enddo
|
|||
|
|
|||
|
significantStress: where(tau > tol_math_check)
|
|||
|
StressRatio_r = (dst%tau_hat_tw(:,of)/tau)**prm%r
|
|||
|
dot_gamma_twin = prm%gamma_char * dst%V_tw(:,of) * Ndot0*exp(-StressRatio_r)
|
|||
|
ddot_gamma_dtau = (dot_gamma_twin*prm%r/tau)*StressRatio_r
|
|||
|
else where significantStress
|
|||
|
dot_gamma_twin = 0.0_pReal
|
|||
|
ddot_gamma_dtau = 0.0_pReal
|
|||
|
end where significantStress
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
if(present(ddot_gamma_dtau_twin)) ddot_gamma_dtau_twin = ddot_gamma_dtau
|
|||
|
|
|||
|
end subroutine kinetics_twin
|
|||
|
|
|||
|
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
!> @brief calculates shear rates on twin systems
|
|||
|
!--------------------------------------------------------------------------------------------------
|
|||
|
pure subroutine kinetics_trans(Mp,T,dot_gamma_sl,instance,of,&
|
|||
|
dot_gamma_tr,ddot_gamma_dtau_trans)
|
|||
|
|
|||
|
real(pReal), dimension(3,3), intent(in) :: &
|
|||
|
Mp !< Mandel stress
|
|||
|
real(pReal), intent(in) :: &
|
|||
|
T !< temperature
|
|||
|
integer, intent(in) :: &
|
|||
|
instance, &
|
|||
|
of
|
|||
|
real(pReal), dimension(param(instance)%sum_N_sl), intent(in) :: &
|
|||
|
dot_gamma_sl
|
|||
|
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tr), intent(out) :: &
|
|||
|
dot_gamma_tr
|
|||
|
real(pReal), dimension(param(instance)%sum_N_tr), optional, intent(out) :: &
|
|||
|
ddot_gamma_dtau_trans
|
|||
|
|
|||
|
real, dimension(param(instance)%sum_N_tr) :: &
|
|||
|
tau, &
|
|||
|
Ndot0, &
|
|||
|
stressRatio_s, &
|
|||
|
ddot_gamma_dtau
|
|||
|
|
|||
|
integer :: i,s1,s2
|
|||
|
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
|
|||
|
|
|||
|
do i = 1, prm%sum_N_tr
|
|||
|
tau(i) = math_mul33xx33(Mp,prm%P_tr(1:3,1:3,i))
|
|||
|
isFCC: if (prm%fccTwinTransNucleation) then
|
|||
|
s1=prm%fcc_twinNucleationSlipPair(1,i)
|
|||
|
s2=prm%fcc_twinNucleationSlipPair(2,i)
|
|||
|
if (tau(i) < dst%tau_r_tr(i,of)) then ! ToDo: correct?
|
|||
|
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rho_mob(s2,of)+stt%rho_dip(s2,of))+&
|
|||
|
abs(dot_gamma_sl(s2))*(stt%rho_mob(s1,of)+stt%rho_dip(s1,of)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
|
|||
|
(prm%L_tr*prm%b_sl(i))*&
|
|||
|
(1.0_pReal-exp(-prm%V_cs/(kB*T)*(dst%tau_r_tr(i,of)-tau(i)))) ! P_ncs
|
|||
|
else
|
|||
|
Ndot0=0.0_pReal
|
|||
|
end if
|
|||
|
else isFCC
|
|||
|
Ndot0=prm%dot_N_0_tr(i)
|
|||
|
endif isFCC
|
|||
|
enddo
|
|||
|
|
|||
|
significantStress: where(tau > tol_math_check)
|
|||
|
StressRatio_s = (dst%tau_hat_tr(:,of)/tau)**prm%s
|
|||
|
dot_gamma_tr = dst%V_tr(:,of) * Ndot0*exp(-StressRatio_s)
|
|||
|
ddot_gamma_dtau = (dot_gamma_tr*prm%s/tau)*StressRatio_s
|
|||
|
else where significantStress
|
|||
|
dot_gamma_tr = 0.0_pReal
|
|||
|
ddot_gamma_dtau = 0.0_pReal
|
|||
|
end where significantStress
|
|||
|
|
|||
|
end associate
|
|||
|
|
|||
|
if(present(ddot_gamma_dtau_trans)) ddot_gamma_dtau_trans = ddot_gamma_dtau
|
|||
|
|
|||
|
end subroutine kinetics_trans
|
|||
|
|
|||
|
end submodule plastic_dislotwin
|