2018-07-06 22:27:37 +05:30
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!--------------------------------------------------------------------------------------------------
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2018-09-06 03:11:35 +05:30
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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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2013-10-08 21:57:26 +05:30
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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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2014-12-08 21:25:30 +05:30
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module plastic_dislotwin
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2013-11-27 13:34:05 +05:30
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use prec, only: &
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2019-03-19 02:47:11 +05:30
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pReal
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2019-01-27 16:07:50 +05:30
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2013-10-08 21:57:26 +05:30
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implicit none
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private
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2019-03-19 02:47:11 +05:30
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integer, dimension(:,:), allocatable, target, public :: &
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2019-01-27 16:07:50 +05:30
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plastic_dislotwin_sizePostResult !< size of each post result output
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2019-03-19 02:47:11 +05:30
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character(len=64), dimension(:,:), allocatable, target, public :: &
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2019-01-27 16:07:50 +05:30
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plastic_dislotwin_output !< name of each post result output
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2019-03-19 02:47:11 +05:30
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real(pReal), parameter, private :: &
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2019-01-27 16:07:50 +05:30
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kB = 1.38e-23_pReal !< Boltzmann constant in J/Kelvin
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2018-08-31 19:38:01 +05:30
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2019-01-27 16:07:50 +05:30
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enum, bind(c)
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enumerator :: &
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2018-10-18 01:17:50 +05:30
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undefined_ID, &
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2019-03-19 02:38:41 +05:30
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rho_mob_ID, &
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rho_dip_ID, &
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gamma_dot_sl_ID, &
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gamma_sl_ID, &
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2019-03-20 14:16:49 +05:30
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Lambda_sl_ID, &
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2018-10-18 01:17:50 +05:30
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resolved_stress_slip_ID, &
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threshold_stress_slip_ID, &
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edge_dipole_distance_ID, &
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2019-03-19 02:38:41 +05:30
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f_tw_ID, &
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2019-03-20 14:16:49 +05:30
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Lambda_tw_ID, &
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2018-10-18 01:17:50 +05:30
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resolved_stress_twin_ID, &
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threshold_stress_twin_ID, &
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2019-03-20 14:16:49 +05:30
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f_tr_ID
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2013-12-12 05:12:33 +05:30
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end enum
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2019-01-27 16:07:50 +05:30
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2018-10-18 01:17:50 +05:30
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type, private :: tParameters
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2018-05-02 23:00:27 +05:30
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real(pReal) :: &
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2018-09-05 19:15:44 +05:30
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mu, &
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nu, &
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2018-07-20 07:32:49 +05:30
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D0, & !< prefactor for self-diffusion coefficient
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Qsd, & !< activation energy for dislocation climb
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2018-10-18 01:17:50 +05:30
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GrainSize, & !<grain size
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pShearBand, & !< p-exponent in shear band velocity
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qShearBand, & !< q-exponent in shear band velocity
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CEdgeDipMinDistance, & !<
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Cmfptwin, & !<
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SolidSolutionStrength, & !<strength due to elements in solid solution
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L0_twin, & !< Length of twin nuclei in Burgers vectors
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L0_trans, & !< 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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VcrossSlip, & !< 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, & !< value for shearband systems Qedge
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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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2019-03-19 10:55:21 +05:30
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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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2018-10-18 01:17:50 +05:30
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deltaG, & !< Free energy difference between austensite and martensite
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Cmfptrans, & !<
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transStackHeight !< Stack height of hex nucleus
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:), allocatable :: &
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2019-03-19 03:14:54 +05:30
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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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2019-03-20 14:16:49 +05:30
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b_tr, & !< absolute length of burgers vector [m] for each transformation system
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2018-10-18 01:17:50 +05:30
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Qedge,& !< 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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tau_peierls,& !< Peierls stress [Pa] for each slip system
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Ndot0_twin, & !< twin nucleation rate [1/m³s] for each twin system
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Ndot0_trans, & !< trans nucleation rate [1/m³s] for each trans system
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twinsize, & !< 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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2019-01-29 10:44:58 +05:30
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atomicVolume, &
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lamellarsize, & !< martensite lamellar thickness [m] for each trans system and instance
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2018-10-18 01:17:50 +05:30
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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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shear_twin, & !< characteristic shear for twins
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B !< drag coefficient
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:,:), allocatable :: &
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2019-03-19 02:38:41 +05:30
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h_sl_sl, & !<
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h_sl_tw, & !<
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2019-03-19 02:54:45 +05:30
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h_tw_tw, & !<
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2019-01-27 16:07:50 +05:30
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interaction_SlipTrans, & !<
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interaction_TransTrans !<
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2019-03-19 02:47:11 +05:30
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integer, dimension(:,:), allocatable :: &
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2018-12-10 13:04:24 +05:30
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fcc_twinNucleationSlipPair ! ToDo: Better name? Is also use for trans
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:,:), allocatable :: &
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2018-12-22 12:19:52 +05:30
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forestProjection, &
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2018-09-05 19:15:44 +05:30
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C66
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:,:,:), allocatable :: &
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2018-08-31 15:07:14 +05:30
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Schmid_trans, &
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Schmid_slip, &
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2018-09-05 19:15:44 +05:30
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Schmid_twin, &
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C66_twin, &
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C66_trans
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2019-03-19 02:47:11 +05:30
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integer :: &
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2019-03-20 14:16:49 +05:30
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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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2019-03-19 02:47:11 +05:30
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integer, dimension(:), allocatable :: &
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2019-03-19 02:54:45 +05:30
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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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2019-03-19 11:18:12 +05:30
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N_tr !< number of active transformation systems for each family
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2019-03-19 02:47:11 +05:30
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integer(kind(undefined_ID)), dimension(:), allocatable :: &
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2019-01-27 16:07:50 +05:30
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outputID !< ID of each post result output
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logical :: &
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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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2015-11-06 22:30:00 +05:30
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type, private :: tDislotwinState
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:,:), pointer :: &
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2015-11-09 14:21:05 +05:30
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rhoEdge, &
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rhoEdgeDip, &
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2015-11-06 22:30:00 +05:30
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accshear_slip, &
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2015-11-10 18:31:03 +05:30
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twinFraction, &
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2019-01-28 04:06:34 +05:30
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strainTransFraction
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2018-09-05 14:37:00 +05:30
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end type tDislotwinState
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type, private :: tDislotwinMicrostructure
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2019-03-19 02:47:11 +05:30
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real(pReal), dimension(:,:), allocatable :: &
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2019-03-19 11:18:12 +05:30
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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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2019-03-19 10:51:40 +05:30
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tau_pass, &
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2018-09-05 14:37:00 +05:30
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threshold_stress_twin, &
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threshold_stress_trans, &
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twinVolume, &
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martensiteVolume, &
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2019-01-29 11:11:27 +05:30
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tau_r_twin, & !< stress to bring partials close together (twin)
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tau_r_trans !< stress to bring partials close together (trans)
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2018-09-05 14:37:00 +05:30
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end type tDislotwinMicrostructure
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2018-07-17 16:02:57 +05:30
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2019-01-27 16:07:50 +05:30
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!--------------------------------------------------------------------------------------------------
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! containers for parameters and state
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type(tParameters), allocatable, dimension(:), private :: param
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2019-03-19 02:47:11 +05:30
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type(tDislotwinState), allocatable, dimension(:), private :: &
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2019-01-27 16:07:50 +05:30
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dotState, &
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state
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type(tDislotwinMicrostructure), allocatable, dimension(:), private :: microstructure
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2013-10-08 21:57:26 +05:30
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public :: &
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2014-12-08 21:25:30 +05:30
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plastic_dislotwin_init, &
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plastic_dislotwin_homogenizedC, &
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2019-01-27 13:05:07 +05:30
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plastic_dislotwin_dependentState, &
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2014-12-08 21:25:30 +05:30
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plastic_dislotwin_LpAndItsTangent, &
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plastic_dislotwin_dotState, &
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2019-03-10 01:13:31 +05:30
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plastic_dislotwin_postResults, &
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plastic_dislotwin_results
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2019-01-27 16:07:50 +05:30
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private :: &
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kinetics_slip, &
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kinetics_twin, &
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kinetics_trans
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2013-10-08 21:57:26 +05:30
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contains
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2011-04-13 17:21:46 +05:30
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2013-03-28 13:10:30 +05:30
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2013-10-08 21:57:26 +05:30
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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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2018-12-11 06:17:13 +05:30
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subroutine plastic_dislotwin_init
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2016-05-27 15:16:34 +05:30
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use prec, only: &
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2018-10-18 01:48:33 +05:30
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pStringLen, &
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2016-10-29 13:09:08 +05:30
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dEq0, &
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dNeq0, &
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2016-05-27 15:16:34 +05:30
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dNeq
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2013-10-08 21:57:26 +05:30
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use debug, only: &
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debug_level,&
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2013-10-14 16:24:45 +05:30
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debug_constitutive,&
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debug_levelBasic
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2013-10-08 21:57:26 +05:30
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use math, only: &
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2018-05-17 23:02:41 +05:30
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math_expand,&
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2018-09-05 20:16:38 +05:30
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PI
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2013-12-19 14:19:47 +05:30
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use IO, only: &
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2019-03-09 05:37:26 +05:30
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IO_error
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2013-12-19 14:19:47 +05:30
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use material, only: &
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phase_plasticity, &
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phase_plasticityInstance, &
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phase_Noutput, &
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2018-11-21 00:16:55 +05:30
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material_allocatePlasticState, &
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2013-12-19 14:19:47 +05:30
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PLASTICITY_DISLOTWIN_label, &
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PLASTICITY_DISLOTWIN_ID, &
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2014-06-11 17:41:14 +05:30
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material_phase, &
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2018-06-10 21:31:52 +05:30
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plasticState
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2018-06-14 10:09:49 +05:30
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use config, only: &
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2018-06-27 21:08:52 +05:30
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config_phase
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2013-10-08 21:57:26 +05:30
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use lattice
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2014-06-11 17:41:14 +05:30
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2013-10-08 21:57:26 +05:30
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implicit none
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2019-03-19 02:47:11 +05:30
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integer :: &
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2019-01-27 16:07:50 +05:30
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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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2019-03-19 02:47:11 +05:30
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integer, dimension(0), parameter :: emptyIntArray = [integer::]
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real(pReal), dimension(0), parameter :: emptyRealArray = [real(pReal)::]
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character(len=65536), dimension(0), parameter :: emptyStringArray = [character(len=65536)::]
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2018-06-27 21:08:52 +05:30
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2018-10-18 01:48:33 +05:30
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integer(kind(undefined_ID)) :: &
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2019-01-27 16:07:50 +05:30
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outputID
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2018-10-18 01:48:33 +05:30
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character(len=pStringLen) :: &
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extmsg = ''
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character(len=65536), dimension(:), allocatable :: &
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2019-01-27 16:07:50 +05:30
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outputs
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2018-10-18 01:48:33 +05:30
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2016-07-25 23:42:00 +05:30
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write(6,'(/,a)') ' <<<+- constitutive_'//PLASTICITY_DISLOTWIN_label//' init -+>>>'
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2019-03-09 15:32:12 +05:30
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write(6,'(/,a)') ' Ma and Roters, Acta Materialia 52(12):3603–3612, 2004'
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2018-07-17 00:44:33 +05:30
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write(6,'(a)') ' https://doi.org/10.1016/j.actamat.2004.04.012'
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2019-03-09 15:32:12 +05:30
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write(6,'(/,a)') ' Roters et al., Computational Materials Science 39:91–95, 2007'
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2018-07-17 00:44:33 +05:30
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write(6,'(a)') ' https://doi.org/10.1016/j.commatsci.2006.04.014'
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2019-03-09 15:32:12 +05:30
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write(6,'(/,a)') ' Wong et al., Acta Materialia 118:140–151, 2016'
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2018-08-31 18:03:42 +05:30
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write(6,'(a,/)') ' https://doi.org/10.1016/j.actamat.2016.07.032'
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2019-03-09 05:37:26 +05:30
|
|
|
|
Ninstance = count(phase_plasticity == PLASTICITY_DISLOTWIN_ID)
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0) &
|
2018-10-18 01:48:33 +05:30
|
|
|
|
write(6,'(a16,1x,i5,/)') '# instances:',Ninstance
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
allocate(plastic_dislotwin_sizePostResult(maxval(phase_Noutput),Ninstance),source=0)
|
2018-10-18 01:48:33 +05:30
|
|
|
|
allocate(plastic_dislotwin_output(maxval(phase_Noutput),Ninstance))
|
2014-12-08 21:25:30 +05:30
|
|
|
|
plastic_dislotwin_output = ''
|
2018-09-06 03:11:35 +05:30
|
|
|
|
|
2018-10-18 01:48:33 +05:30
|
|
|
|
allocate(param(Ninstance))
|
|
|
|
|
allocate(state(Ninstance))
|
|
|
|
|
allocate(dotState(Ninstance))
|
|
|
|
|
allocate(microstructure(Ninstance))
|
2018-05-29 21:59:38 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
do p = 1, size(phase_plasticity)
|
2018-06-27 21:08:52 +05:30
|
|
|
|
if (phase_plasticity(p) /= PLASTICITY_DISLOTWIN_ID) cycle
|
2018-09-05 19:45:57 +05:30
|
|
|
|
associate(prm => param(phase_plasticityInstance(p)), &
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot => dotState(phase_plasticityInstance(p)), &
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt => state(phase_plasticityInstance(p)), &
|
2019-01-28 02:38:36 +05:30
|
|
|
|
dst => microstructure(phase_plasticityInstance(p)), &
|
2018-12-22 04:49:51 +05:30
|
|
|
|
config => config_phase(p))
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
2019-03-19 10:55:21 +05:30
|
|
|
|
prm%aTol_rho = config%getFloat('atol_rho', defaultVal=0.0_pReal)
|
|
|
|
|
prm%aTol_f_tw = config%getFloat('atol_twinfrac', defaultVal=0.0_pReal)
|
|
|
|
|
prm%aTol_f_tr = config%getFloat('atol_transfrac', defaultVal=0.0_pReal)
|
2019-01-29 11:11:27 +05:30
|
|
|
|
|
2018-09-05 19:45:57 +05:30
|
|
|
|
! This data is read in already in lattice
|
|
|
|
|
prm%mu = lattice_mu(p)
|
|
|
|
|
prm%nu = lattice_nu(p)
|
|
|
|
|
prm%C66 = lattice_C66(1:6,1:6,p)
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
2018-10-18 02:43:47 +05:30
|
|
|
|
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
! slip related parameters
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%N_sl = config%getInts('nslip',defaultVal=emptyIntArray)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
prm%sum_N_sl = sum(prm%N_sl)
|
|
|
|
|
slipActive: if (prm%sum_N_sl > 0) then
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%Schmid_slip = lattice_SchmidMatrix_slip(prm%N_sl,config%getString('lattice_structure'),&
|
2018-12-22 04:49:51 +05:30
|
|
|
|
config%getFloat('c/a',defaultVal=0.0_pReal))
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%h_sl_sl = lattice_interaction_SlipBySlip(prm%N_sl, &
|
2019-03-19 02:38:41 +05:30
|
|
|
|
config%getFloats('interaction_slipslip'), &
|
|
|
|
|
config%getString('lattice_structure'))
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%forestProjection = lattice_forestProjection (prm%N_sl,config%getString('lattice_structure'),&
|
2019-01-27 16:07:50 +05:30
|
|
|
|
config%getFloat('c/a',defaultVal=0.0_pReal))
|
|
|
|
|
|
|
|
|
|
prm%fccTwinTransNucleation = merge(.true., .false., lattice_structure(p) == LATTICE_FCC_ID) &
|
2019-03-19 02:54:45 +05:30
|
|
|
|
.and. (prm%N_sl(1) == 12)
|
2019-01-27 16:07:50 +05:30
|
|
|
|
if(prm%fccTwinTransNucleation) &
|
|
|
|
|
prm%fcc_twinNucleationSlipPair = lattice_fcc_twinNucleationSlipPair
|
2018-10-18 02:43:47 +05:30
|
|
|
|
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%rho_mob_0 = config%getFloats('rhoedge0', requiredSize=size(prm%N_sl))
|
|
|
|
|
prm%rho_dip_0 = config%getFloats('rhoedgedip0',requiredSize=size(prm%N_sl))
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%v0 = config%getFloats('v0', requiredSize=size(prm%N_sl))
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%b_sl = config%getFloats('slipburgers',requiredSize=size(prm%N_sl))
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%Qedge = config%getFloats('qedge', requiredSize=size(prm%N_sl)) !ToDo: rename (ask Karo)
|
|
|
|
|
prm%CLambdaSlip = config%getFloats('clambdaslip',requiredSize=size(prm%N_sl))
|
|
|
|
|
prm%p = config%getFloats('p_slip', requiredSize=size(prm%N_sl))
|
|
|
|
|
prm%q = config%getFloats('q_slip', requiredSize=size(prm%N_sl))
|
|
|
|
|
prm%B = config%getFloats('b', requiredSize=size(prm%N_sl), &
|
|
|
|
|
defaultVal=[(0.0_pReal, i=1,size(prm%N_sl))])
|
|
|
|
|
prm%tau_peierls = config%getFloats('tau_peierls',requiredSize=size(prm%N_sl), &
|
|
|
|
|
defaultVal=[(0.0_pReal, i=1,size(prm%N_sl))]) ! Deprecated
|
2018-06-27 21:08:52 +05:30
|
|
|
|
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%CEdgeDipMinDistance = config%getFloat('cedgedipmindistance')
|
2019-01-29 11:11:27 +05:30
|
|
|
|
prm%D0 = config%getFloat('d0')
|
|
|
|
|
prm%Qsd = config%getFloat('qsd')
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%atomicVolume = config%getFloat('catomicvolume') * prm%b_sl**3.0_pReal
|
2018-06-27 21:08:52 +05:30
|
|
|
|
|
2018-10-18 03:26:57 +05:30
|
|
|
|
! expand: family => system
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%rho_mob_0 = math_expand(prm%rho_mob_0, prm%N_sl)
|
|
|
|
|
prm%rho_dip_0 = math_expand(prm%rho_dip_0, prm%N_sl)
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%v0 = math_expand(prm%v0, prm%N_sl)
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%b_sl = math_expand(prm%b_sl,prm%N_sl)
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%Qedge = math_expand(prm%Qedge, prm%N_sl)
|
|
|
|
|
prm%CLambdaSlip = math_expand(prm%CLambdaSlip, prm%N_sl)
|
|
|
|
|
prm%p = math_expand(prm%p, prm%N_sl)
|
|
|
|
|
prm%q = math_expand(prm%q, prm%N_sl)
|
|
|
|
|
prm%B = math_expand(prm%B, prm%N_sl)
|
|
|
|
|
prm%tau_peierls = math_expand(prm%tau_peierls, prm%N_sl)
|
|
|
|
|
prm%atomicVolume = math_expand(prm%atomicVolume,prm%N_sl)
|
2018-10-12 20:54:46 +05:30
|
|
|
|
|
2018-10-18 03:26:57 +05:30
|
|
|
|
! sanity checks
|
2019-01-29 11:11:27 +05:30
|
|
|
|
if ( prm%D0 <= 0.0_pReal) extmsg = trim(extmsg)//' D0'
|
|
|
|
|
if ( prm%Qsd <= 0.0_pReal) extmsg = trim(extmsg)//' Qsd'
|
2019-03-19 03:14:54 +05:30
|
|
|
|
if (any(prm%rho_mob_0 < 0.0_pReal)) extmsg = trim(extmsg)//' rho_mob_0'
|
|
|
|
|
if (any(prm%rho_dip_0 < 0.0_pReal)) extmsg = trim(extmsg)//' rho_dip_0'
|
2019-01-29 11:11:27 +05:30
|
|
|
|
if (any(prm%v0 < 0.0_pReal)) extmsg = trim(extmsg)//' v0'
|
2019-03-19 03:14:54 +05:30
|
|
|
|
if (any(prm%b_sl <= 0.0_pReal)) extmsg = trim(extmsg)//' b_sl'
|
2019-01-29 11:11:27 +05:30
|
|
|
|
if (any(prm%Qedge <= 0.0_pReal)) extmsg = trim(extmsg)//' Qedge'
|
|
|
|
|
if (any(prm%CLambdaSlip <= 0.0_pReal)) extmsg = trim(extmsg)//' CLambdaSlip'
|
|
|
|
|
if (any(prm%B < 0.0_pReal)) extmsg = trim(extmsg)//' B'
|
|
|
|
|
if (any(prm%tau_peierls < 0.0_pReal)) extmsg = trim(extmsg)//' tau_peierls'
|
|
|
|
|
if (any(prm%p<=0.0_pReal .or. prm%p>1.0_pReal)) extmsg = trim(extmsg)//' p'
|
|
|
|
|
if (any(prm%q< 1.0_pReal .or. prm%q>2.0_pReal)) extmsg = trim(extmsg)//' q'
|
2018-10-12 20:54:46 +05:30
|
|
|
|
|
|
|
|
|
else slipActive
|
2019-03-19 03:14:54 +05:30
|
|
|
|
allocate(prm%b_sl(0))
|
2018-10-12 20:54:46 +05:30
|
|
|
|
endif slipActive
|
2018-06-27 21:08:52 +05:30
|
|
|
|
|
2018-10-18 02:43:47 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
! twin related parameters
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%N_tw = config%getInts('ntwin', defaultVal=emptyIntArray)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
prm%sum_N_tw = sum(prm%N_tw)
|
|
|
|
|
if (prm%sum_N_tw > 0) then
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%Schmid_twin = lattice_SchmidMatrix_twin(prm%N_tw,config%getString('lattice_structure'),&
|
|
|
|
|
config%getFloat('c/a',defaultVal=0.0_pReal))
|
|
|
|
|
prm%h_tw_tw = lattice_interaction_TwinByTwin(prm%N_tw,&
|
|
|
|
|
config%getFloats('interaction_twintwin'), &
|
|
|
|
|
config%getString('lattice_structure'))
|
2018-10-18 02:43:47 +05:30
|
|
|
|
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%b_tw = config%getFloats('twinburgers', requiredSize=size(prm%N_tw))
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%twinsize = config%getFloats('twinsize', requiredSize=size(prm%N_tw))
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%r = config%getFloats('r_twin', requiredSize=size(prm%N_tw))
|
2018-10-18 03:26:57 +05:30
|
|
|
|
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%xc_twin = config%getFloat('xc_twin')
|
|
|
|
|
prm%L0_twin = config%getFloat('l0_twin')
|
|
|
|
|
prm%Cmfptwin = config%getFloat('cmfptwin', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
2018-10-18 03:26:57 +05:30
|
|
|
|
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%shear_twin = lattice_characteristicShear_Twin(prm%N_tw,config%getString('lattice_structure'),&
|
2019-03-19 03:14:54 +05:30
|
|
|
|
config%getFloat('c/a',defaultVal=0.0_pReal))
|
2018-12-10 02:50:18 +05:30
|
|
|
|
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%C66_twin = lattice_C66_twin(prm%N_tw,prm%C66,config%getString('lattice_structure'),&
|
2019-03-19 03:14:54 +05:30
|
|
|
|
config%getFloat('c/a',defaultVal=0.0_pReal))
|
2018-06-27 21:08:52 +05:30
|
|
|
|
|
2018-12-10 13:04:24 +05:30
|
|
|
|
if (.not. prm%fccTwinTransNucleation) then
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%Ndot0_twin = config%getFloats('ndot0_twin')
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%Ndot0_twin = math_expand(prm%Ndot0_twin,prm%N_tw)
|
2018-06-25 23:37:35 +05:30
|
|
|
|
endif
|
2018-07-05 16:15:50 +05:30
|
|
|
|
|
2018-10-18 03:26:57 +05:30
|
|
|
|
! expand: family => system
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%b_tw = math_expand(prm%b_tw,prm%N_tw)
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%twinsize = math_expand(prm%twinsize,prm%N_tw)
|
|
|
|
|
prm%r = math_expand(prm%r,prm%N_tw)
|
2018-06-25 23:37:35 +05:30
|
|
|
|
|
2018-10-04 18:21:32 +05:30
|
|
|
|
else
|
|
|
|
|
allocate(prm%twinsize(0))
|
2019-03-19 03:14:54 +05:30
|
|
|
|
allocate(prm%b_tw(0))
|
2018-10-04 18:21:32 +05:30
|
|
|
|
allocate(prm%r(0))
|
2018-07-05 16:15:50 +05:30
|
|
|
|
endif
|
2018-10-04 18:21:32 +05:30
|
|
|
|
|
2018-10-19 01:50:26 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
! transformation related parameters
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%N_tr = config%getInts('ntrans', defaultVal=emptyIntArray)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
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)
|
2018-06-25 23:37:35 +05:30
|
|
|
|
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%transStackHeight = config%getFloat('transstackheight', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|
|
|
|
prm%Cmfptrans = config%getFloat('cmfptrans', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|
|
|
|
prm%deltaG = config%getFloat('deltag')
|
|
|
|
|
prm%xc_trans = config%getFloat('xc_trans', defaultVal=0.0_pReal) ! ToDo: How to handle that???
|
|
|
|
|
prm%L0_trans = config%getFloat('l0_trans')
|
2018-07-05 16:15:50 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%interaction_TransTrans = lattice_interaction_TransByTrans(prm%N_tr,&
|
2019-03-12 03:11:59 +05:30
|
|
|
|
config%getFloats('interaction_transtrans'), &
|
|
|
|
|
config%getString('lattice_structure'))
|
2018-12-22 04:49:51 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%C66_trans = lattice_C66_trans(prm%N_tr,prm%C66, &
|
2018-12-22 04:49:51 +05:30
|
|
|
|
config%getString('trans_lattice_structure'), &
|
|
|
|
|
0.0_pReal, &
|
|
|
|
|
config%getFloat('a_bcc', defaultVal=0.0_pReal), &
|
|
|
|
|
config%getFloat('a_fcc', defaultVal=0.0_pReal))
|
2018-12-22 12:19:52 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%Schmid_trans = lattice_SchmidMatrix_trans(prm%N_tr, &
|
2018-12-22 12:19:52 +05:30
|
|
|
|
config%getString('trans_lattice_structure'), &
|
|
|
|
|
0.0_pReal, &
|
|
|
|
|
config%getFloat('a_bcc', defaultVal=0.0_pReal), &
|
|
|
|
|
config%getFloat('a_fcc', defaultVal=0.0_pReal))
|
2018-12-22 04:49:51 +05:30
|
|
|
|
|
2018-07-05 16:15:50 +05:30
|
|
|
|
if (lattice_structure(p) /= LATTICE_fcc_ID) then
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%Ndot0_trans = config%getFloats('ndot0_trans')
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%Ndot0_trans = math_expand(prm%Ndot0_trans,prm%N_tr)
|
2018-07-05 16:15:50 +05:30
|
|
|
|
endif
|
2019-01-28 04:06:34 +05:30
|
|
|
|
prm%lamellarsize = config%getFloats('lamellarsize')
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%lamellarsize = math_expand(prm%lamellarsize,prm%N_tr)
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%s = config%getFloats('s_trans',defaultVal=[0.0_pReal])
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%s = math_expand(prm%s,prm%N_tr)
|
2018-10-04 18:21:32 +05:30
|
|
|
|
else
|
2019-01-28 04:06:34 +05:30
|
|
|
|
allocate(prm%lamellarsize(0))
|
2019-03-20 14:16:49 +05:30
|
|
|
|
allocate(prm%b_tr(0))
|
2018-07-05 16:15:50 +05:30
|
|
|
|
endif
|
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (sum(prm%N_tw) > 0 .or. prm%sum_N_tr > 0) then
|
2018-12-22 04:49:51 +05:30
|
|
|
|
prm%SFE_0K = config%getFloat('sfe_0k')
|
|
|
|
|
prm%dSFE_dT = config%getFloat('dsfe_dt')
|
|
|
|
|
prm%VcrossSlip = config%getFloat('vcrossslip')
|
2018-07-05 16:15:50 +05:30
|
|
|
|
endif
|
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_sl > 0 .and. prm%sum_N_tw > 0) then
|
2019-03-19 02:54:45 +05:30
|
|
|
|
prm%h_sl_tw = lattice_interaction_SlipByTwin(prm%N_sl,prm%N_tw,&
|
2019-03-19 02:38:41 +05:30
|
|
|
|
config%getFloats('interaction_sliptwin'), &
|
|
|
|
|
config%getString('lattice_structure'))
|
2019-03-20 14:16:49 +05:30
|
|
|
|
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]
|
2018-08-31 19:38:01 +05:30
|
|
|
|
endif
|
2018-07-05 16:15:50 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_sl > 0 .and. prm%sum_N_tr > 0) then
|
2019-03-19 11:18:12 +05:30
|
|
|
|
prm%interaction_SlipTrans = lattice_interaction_SlipByTrans(prm%N_sl,prm%N_tr,&
|
2019-03-12 03:11:59 +05:30
|
|
|
|
config%getFloats('interaction_sliptrans'), &
|
|
|
|
|
config%getString('lattice_structure'))
|
2019-03-20 14:16:49 +05:30
|
|
|
|
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]
|
2019-01-29 11:11:27 +05:30
|
|
|
|
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%pShearBand = config%getFloat('p_shearband')
|
|
|
|
|
prm%qShearBand = 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%pShearBand <= 0.0_pReal) extmsg = trim(extmsg)//' p_shearband'
|
|
|
|
|
if (prm%qShearBand <= 0.0_pReal) extmsg = trim(extmsg)//' q_shearband'
|
|
|
|
|
endif
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
2018-10-04 18:24:00 +05:30
|
|
|
|
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
2019-01-29 11:11:27 +05:30
|
|
|
|
prm%GrainSize = config%getFloat('grainsize')
|
2018-12-22 12:19:52 +05:30
|
|
|
|
prm%SolidSolutionStrength = config%getFloat('solidsolutionstrength') ! Deprecated
|
2019-01-29 11:11:27 +05:30
|
|
|
|
|
2018-12-22 04:49:51 +05:30
|
|
|
|
if (config%keyExists('dipoleformationfactor')) call IO_error(1,ext_msg='use /nodipoleformation/')
|
|
|
|
|
prm%dipoleformation = .not. config%keyExists('/nodipoleformation/')
|
2019-01-29 11:11:27 +05:30
|
|
|
|
|
2018-10-19 01:04:26 +05:30
|
|
|
|
|
|
|
|
|
!if (Ndot0PerTwinFamily(f,p) < 0.0_pReal) &
|
2019-03-19 02:47:11 +05:30
|
|
|
|
! call IO_error(211,el=p,ext_msg='ndot0_twin ('//PLASTICITY_DISLOTWIN_label//')')
|
2018-10-19 01:04:26 +05:30
|
|
|
|
|
2019-01-29 10:44:58 +05:30
|
|
|
|
if (any(prm%atomicVolume <= 0.0_pReal)) &
|
2019-03-19 02:47:11 +05:30
|
|
|
|
call IO_error(211,el=p,ext_msg='cAtomicVolume ('//PLASTICITY_DISLOTWIN_label//')')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_tw > 0) then
|
2019-03-19 10:55:21 +05:30
|
|
|
|
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//')')
|
2018-10-19 01:04:26 +05:30
|
|
|
|
endif
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_tr > 0) then
|
2019-03-19 10:55:21 +05:30
|
|
|
|
if (prm%aTol_f_tr <= 0.0_pReal) &
|
|
|
|
|
call IO_error(211,el=p,ext_msg='aTol_f_tr ('//PLASTICITY_DISLOTWIN_label//')')
|
2018-10-19 01:04:26 +05:30
|
|
|
|
endif
|
2018-07-20 21:22:15 +05:30
|
|
|
|
|
2018-12-22 04:49:51 +05:30
|
|
|
|
outputs = config%getStrings('(output)', defaultVal=emptyStringArray)
|
2018-09-05 19:15:44 +05:30
|
|
|
|
allocate(prm%outputID(0))
|
2019-03-19 02:47:11 +05:30
|
|
|
|
do i= 1, size(outputs)
|
2018-09-05 19:15:44 +05:30
|
|
|
|
outputID = undefined_ID
|
|
|
|
|
select case(outputs(i))
|
|
|
|
|
case ('edge_density')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(rho_mob_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('dipole_density')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(rho_dip_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('shear_rate_slip','shearrate_slip')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(gamma_dot_sl_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('accumulated_shear_slip')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(gamma_sl_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('mfp_slip')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(Lambda_sl_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('resolved_stress_slip')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(resolved_stress_slip_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('threshold_stress_slip')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID= merge(threshold_stress_slip_ID,undefined_ID,prm%sum_N_sl > 0)
|
|
|
|
|
outputSize = prm%sum_N_sl
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
|
|
|
|
case ('twin_fraction')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(f_tw_ID,undefined_ID,prm%sum_N_tw >0)
|
|
|
|
|
outputSize = prm%sum_N_tw
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('mfp_twin')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(Lambda_tw_ID,undefined_ID,prm%sum_N_tw >0)
|
|
|
|
|
outputSize = prm%sum_N_tw
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('resolved_stress_twin')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(resolved_stress_twin_ID,undefined_ID,prm%sum_N_tw >0)
|
|
|
|
|
outputSize = prm%sum_N_tw
|
2018-09-05 19:15:44 +05:30
|
|
|
|
case ('threshold_stress_twin')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = merge(threshold_stress_twin_ID,undefined_ID,prm%sum_N_tw >0)
|
|
|
|
|
outputSize = prm%sum_N_tw
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
|
|
|
|
case ('strain_trans_fraction')
|
2019-03-20 14:16:49 +05:30
|
|
|
|
outputID = f_tr_ID
|
|
|
|
|
outputSize = prm%sum_N_tr
|
2018-09-05 19:15:44 +05:30
|
|
|
|
|
|
|
|
|
end select
|
|
|
|
|
|
|
|
|
|
if (outputID /= undefined_ID) then
|
2018-09-05 19:45:57 +05:30
|
|
|
|
plastic_dislotwin_output(i,phase_plasticityInstance(p)) = outputs(i)
|
|
|
|
|
plastic_dislotwin_sizePostResult(i,phase_plasticityInstance(p)) = outputSize
|
|
|
|
|
prm%outputID = [prm%outputID, outputID]
|
2018-09-05 19:15:44 +05:30
|
|
|
|
endif
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2018-09-05 19:15:44 +05:30
|
|
|
|
enddo
|
2018-06-25 23:37:35 +05:30
|
|
|
|
|
2014-07-02 17:57:39 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
! allocate state arrays
|
2019-01-27 16:07:50 +05:30
|
|
|
|
NipcMyPhase = count(material_phase == p)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
sizeDotState = size(['rho ','rhoDip ','accshearslip']) * prm%sum_N_sl &
|
|
|
|
|
+ size(['twinFraction']) * prm%sum_N_tw &
|
|
|
|
|
+ size(['strainTransFraction']) * prm%sum_N_tr
|
2019-01-27 16:07:50 +05:30
|
|
|
|
sizeState = sizeDotState
|
2018-11-21 00:16:55 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
call material_allocatePlasticState(p,NipcMyPhase,sizeState,sizeDotState,0, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
prm%sum_N_sl,prm%sum_N_tw,prm%sum_N_tr)
|
2018-09-05 19:45:57 +05:30
|
|
|
|
plasticState(p)%sizePostResults = sum(plastic_dislotwin_sizePostResult(:,phase_plasticityInstance(p)))
|
2018-09-05 20:16:38 +05:30
|
|
|
|
|
2018-12-10 13:04:24 +05:30
|
|
|
|
|
2019-01-27 16:07:50 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
! locally defined state aliases and initialization of state0 and aTolState
|
2019-03-19 02:47:11 +05:30
|
|
|
|
startIndex = 1
|
2019-03-20 14:16:49 +05:30
|
|
|
|
endIndex = prm%sum_N_sl
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt%rhoEdge=>plasticState(p)%state(startIndex:endIndex,:)
|
2019-03-19 03:14:54 +05:30
|
|
|
|
stt%rhoEdge= spread(prm%rho_mob_0,2,NipcMyPhase)
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%rhoEdge=>plasticState(p)%dotState(startIndex:endIndex,:)
|
2019-03-19 10:55:21 +05:30
|
|
|
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_rho
|
2018-08-31 15:12:54 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
startIndex = endIndex + 1
|
2019-03-20 14:16:49 +05:30
|
|
|
|
endIndex = endIndex + prm%sum_N_sl
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt%rhoEdgeDip=>plasticState(p)%state(startIndex:endIndex,:)
|
2019-03-19 03:14:54 +05:30
|
|
|
|
stt%rhoEdgeDip= spread(prm%rho_dip_0,2,NipcMyPhase)
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%rhoEdgeDip=>plasticState(p)%dotState(startIndex:endIndex,:)
|
2019-03-19 10:55:21 +05:30
|
|
|
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_rho
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
startIndex = endIndex + 1
|
2019-03-20 14:16:49 +05:30
|
|
|
|
endIndex = endIndex + prm%sum_N_sl
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt%accshear_slip=>plasticState(p)%state(startIndex:endIndex,:)
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%accshear_slip=>plasticState(p)%dotState(startIndex:endIndex,:)
|
2019-01-27 16:07:50 +05:30
|
|
|
|
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,:)
|
2018-08-31 15:12:54 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
startIndex = endIndex + 1
|
2019-03-20 14:16:49 +05:30
|
|
|
|
endIndex = endIndex + prm%sum_N_tw
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt%twinFraction=>plasticState(p)%state(startIndex:endIndex,:)
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%twinFraction=>plasticState(p)%dotState(startIndex:endIndex,:)
|
2019-03-19 10:55:21 +05:30
|
|
|
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_f_tw
|
2018-08-31 15:12:54 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
startIndex = endIndex + 1
|
2019-03-20 14:16:49 +05:30
|
|
|
|
endIndex = endIndex + prm%sum_N_tr
|
2018-09-05 19:45:57 +05:30
|
|
|
|
stt%strainTransFraction=>plasticState(p)%state(startIndex:endIndex,:)
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%strainTransFraction=>plasticState(p)%dotState(startIndex:endIndex,:)
|
2019-03-19 10:55:21 +05:30
|
|
|
|
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTol_f_tr
|
2018-09-05 20:16:38 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
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)
|
2018-08-31 15:12:54 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
allocate(dst%Lambda_tw (prm%sum_N_tw, NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%threshold_stress_twin (prm%sum_N_tw, NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%tau_r_twin (prm%sum_N_tw, NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%twinVolume (prm%sum_N_tw, NipcMyPhase),source=0.0_pReal)
|
2018-08-31 15:12:54 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
allocate(dst%Lambda_tr (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%threshold_stress_trans(prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%tau_r_trans (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
|
|
|
|
allocate(dst%martensiteVolume (prm%sum_N_tr,NipcMyPhase),source=0.0_pReal)
|
2018-09-13 10:18:06 +05:30
|
|
|
|
|
2019-01-28 04:06:34 +05:30
|
|
|
|
|
2019-01-27 16:07:50 +05:30
|
|
|
|
plasticState(p)%state0 = plasticState(p)%state ! ToDo: this could be done centrally
|
|
|
|
|
|
2018-09-05 19:15:44 +05:30
|
|
|
|
end associate
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2018-09-05 19:15:44 +05:30
|
|
|
|
enddo
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2018-08-03 11:00:09 +05:30
|
|
|
|
end subroutine plastic_dislotwin_init
|
2014-07-22 13:13:03 +05:30
|
|
|
|
|
2019-01-27 16:07:50 +05:30
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief returns the homogenized elasticity matrix
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2019-01-27 16:45:11 +05:30
|
|
|
|
function plastic_dislotwin_homogenizedC(ipc,ip,el) result(homogenizedC)
|
2013-10-08 21:57:26 +05:30
|
|
|
|
use material, only: &
|
2018-09-05 19:15:44 +05:30
|
|
|
|
material_phase, &
|
2014-07-02 17:57:39 +05:30
|
|
|
|
phase_plasticityInstance, &
|
2018-09-05 19:15:44 +05:30
|
|
|
|
phasememberAt
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2018-09-05 19:15:44 +05:30
|
|
|
|
implicit none
|
|
|
|
|
real(pReal), dimension(6,6) :: &
|
2019-01-27 16:45:11 +05:30
|
|
|
|
homogenizedC
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2018-09-05 19:15:44 +05:30
|
|
|
|
ipc, & !< component-ID of integration point
|
|
|
|
|
ip, & !< integration point
|
|
|
|
|
el !< element
|
2018-07-17 16:02:57 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i, &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
of
|
2018-09-15 11:54:12 +05:30
|
|
|
|
real(pReal) :: f_unrotated
|
2014-07-02 17:57:39 +05:30
|
|
|
|
|
2016-01-15 05:49:44 +05:30
|
|
|
|
of = phasememberAt(ipc,ip,el)
|
2018-09-05 19:15:44 +05:30
|
|
|
|
associate(prm => param(phase_plasticityInstance(material_phase(ipc,ip,el))),&
|
|
|
|
|
stt => state(phase_plasticityInstance(material_phase(ipc,ip,el))))
|
2014-09-10 17:42:17 +05:30
|
|
|
|
|
2018-09-15 11:54:12 +05:30
|
|
|
|
f_unrotated = 1.0_pReal &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
- sum(stt%twinFraction(1:prm%sum_N_tw,of)) &
|
|
|
|
|
- sum(stt%strainTransFraction(1:prm%sum_N_tr,of))
|
2014-09-10 17:42:17 +05:30
|
|
|
|
|
2019-01-27 16:45:11 +05:30
|
|
|
|
homogenizedC = f_unrotated * prm%C66
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do i=1,prm%sum_N_tw
|
2019-01-27 16:45:11 +05:30
|
|
|
|
homogenizedC = homogenizedC &
|
|
|
|
|
+ stt%twinFraction(i,of)*prm%C66_twin(1:6,1:6,i)
|
2013-10-08 21:57:26 +05:30
|
|
|
|
enddo
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do i=1,prm%sum_N_tr
|
2019-01-27 16:45:11 +05:30
|
|
|
|
homogenizedC = homogenizedC &
|
2019-01-28 02:36:08 +05:30
|
|
|
|
+ stt%strainTransFraction(i,of)*prm%C66_trans(1:6,1:6,i)
|
2014-09-10 17:42:17 +05:30
|
|
|
|
enddo
|
2019-01-27 16:45:11 +05:30
|
|
|
|
|
2018-07-17 01:07:26 +05:30
|
|
|
|
end associate
|
2019-01-27 16:45:11 +05:30
|
|
|
|
|
|
|
|
|
end function plastic_dislotwin_homogenizedC
|
2018-09-06 03:11:35 +05:30
|
|
|
|
|
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief calculates plastic velocity gradient and its tangent
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2018-10-02 01:44:54 +05:30
|
|
|
|
subroutine plastic_dislotwin_LpAndItsTangent(Lp,dLp_dMp,Mp,Temperature,instance,of)
|
2013-10-08 21:57:26 +05:30
|
|
|
|
use prec, only: &
|
2016-05-29 14:15:03 +05:30
|
|
|
|
tol_math_check, &
|
2016-10-29 13:09:08 +05:30
|
|
|
|
dNeq0
|
2013-10-08 21:57:26 +05:30
|
|
|
|
use math, only: &
|
2016-02-26 20:06:24 +05:30
|
|
|
|
math_eigenValuesVectorsSym, &
|
2019-03-09 21:28:59 +05:30
|
|
|
|
math_outer, &
|
2013-10-08 21:57:26 +05:30
|
|
|
|
math_symmetric33, &
|
2018-08-31 15:07:14 +05:30
|
|
|
|
math_mul33xx33, &
|
2016-01-09 17:42:31 +05:30
|
|
|
|
math_mul33x3
|
2013-10-14 16:24:45 +05:30
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
implicit none
|
2018-10-02 01:44:54 +05:30
|
|
|
|
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
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: instance,of
|
2018-10-02 01:44:54 +05:30
|
|
|
|
real(pReal), intent(in) :: Temperature
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i,k,l,m,n
|
2018-09-15 11:54:12 +05:30
|
|
|
|
real(pReal) :: f_unrotated,StressRatio_p,&
|
2019-01-27 13:05:07 +05:30
|
|
|
|
BoltzmannRatio, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dgamma_dtau, &
|
2018-08-31 20:06:19 +05:30
|
|
|
|
tau
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|
|
|
|
dot_gamma_sl,dgamma_dtau_slip
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
|
|
|
|
dot_gamma_twin,dgamma_dtau_twin
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
|
|
|
|
dot_gamma_trans,dgamma_dtau_trans
|
|
|
|
|
real(pReal):: dot_gamma_sb
|
2018-09-05 14:37:00 +05:30
|
|
|
|
real(pReal), dimension(3,3) :: eigVectors, Schmid_shearBand
|
2019-01-28 00:14:53 +05:30
|
|
|
|
real(pReal), dimension(3) :: eigValues
|
2016-01-31 22:19:56 +05:30
|
|
|
|
logical :: error
|
2013-10-08 21:57:26 +05:30
|
|
|
|
real(pReal), dimension(3,6), parameter :: &
|
2013-10-14 16:24:45 +05:30
|
|
|
|
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])
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
2019-03-19 10:51:40 +05:30
|
|
|
|
associate(prm => param(instance), stt => state(instance))
|
2018-06-27 21:08:52 +05:30
|
|
|
|
|
2018-09-15 11:54:12 +05:30
|
|
|
|
f_unrotated = 1.0_pReal &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
- sum(stt%twinFraction(1:prm%sum_N_tw,of)) &
|
|
|
|
|
- sum(stt%strainTransFraction(1:prm%sum_N_tr,of))
|
2014-06-11 17:41:14 +05:30
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
Lp = 0.0_pReal
|
2018-09-17 11:53:23 +05:30
|
|
|
|
dLp_dMp = 0.0_pReal
|
2018-08-31 15:07:14 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_slip(Mp,temperature,instance,of,dot_gamma_sl,dgamma_dtau_slip)
|
|
|
|
|
slipContribution: do i = 1, prm%sum_N_sl
|
|
|
|
|
Lp = Lp + dot_gamma_sl(i)*prm%Schmid_slip(1:3,1:3,i)
|
2019-03-19 02:47:11 +05:30
|
|
|
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
2018-09-17 11:53:23 +05:30
|
|
|
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
+ dgamma_dtau_slip(i) * prm%Schmid_slip(k,l,i) * prm%Schmid_slip(m,n,i)
|
2018-09-01 14:15:34 +05:30
|
|
|
|
enddo slipContribution
|
|
|
|
|
|
|
|
|
|
!ToDo: Why do this before shear banding?
|
2018-09-17 11:53:23 +05:30
|
|
|
|
Lp = Lp * f_unrotated
|
|
|
|
|
dLp_dMp = dLp_dMp * f_unrotated
|
2014-11-05 23:22:49 +05:30
|
|
|
|
|
2018-09-05 14:37:00 +05:30
|
|
|
|
shearBandingContribution: if(dNeq0(prm%sbVelocity)) then
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
|
|
|
|
BoltzmannRatio = prm%sbQedge/(kB*Temperature)
|
2018-09-17 11:53:23 +05:30
|
|
|
|
call math_eigenValuesVectorsSym(Mp,eigValues,eigVectors,error)
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
do i = 1,6
|
2019-03-09 21:28:59 +05:30
|
|
|
|
Schmid_shearBand = 0.5_pReal * math_outer(math_mul33x3(eigVectors,sb_sComposition(1:3,i)),&
|
|
|
|
|
math_mul33x3(eigVectors,sb_mComposition(1:3,i)))
|
2018-09-26 12:52:12 +05:30
|
|
|
|
tau = math_mul33xx33(Mp,Schmid_shearBand)
|
2013-10-14 16:24:45 +05:30
|
|
|
|
|
2018-09-05 14:37:00 +05:30
|
|
|
|
significantShearBandStress: if (abs(tau) > tol_math_check) then
|
2019-01-28 00:14:53 +05:30
|
|
|
|
StressRatio_p = (abs(tau)/prm%sbResistance)**prm%pShearBand
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_sb = sign(prm%sbVelocity*exp(-BoltzmannRatio*(1-StressRatio_p)**prm%qShearBand), tau)
|
|
|
|
|
dgamma_dtau = abs(dot_gamma_sb)*BoltzmannRatio* prm%pShearBand*prm%qShearBand/ prm%sbResistance &
|
2018-09-15 11:54:12 +05:30
|
|
|
|
* (abs(tau)/prm%sbResistance)**(prm%pShearBand-1.0_pReal) &
|
|
|
|
|
* (1.0_pReal-StressRatio_p)**(prm%qShearBand-1.0_pReal)
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
Lp = Lp + dot_gamma_sb * Schmid_shearBand
|
2019-03-19 02:47:11 +05:30
|
|
|
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
2018-09-17 11:53:23 +05:30
|
|
|
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
+ dgamma_dtau * Schmid_shearBand(k,l) * Schmid_shearBand(m,n)
|
2018-09-05 14:37:00 +05:30
|
|
|
|
endif significantShearBandStress
|
2013-10-14 16:24:45 +05:30
|
|
|
|
enddo
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
2018-09-05 14:37:00 +05:30
|
|
|
|
endif shearBandingContribution
|
2012-05-16 20:13:26 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_twin(Mp,temperature,dot_gamma_sl,instance,of,dot_gamma_twin,dgamma_dtau_twin)
|
|
|
|
|
twinContibution: do i = 1, prm%sum_N_tw
|
|
|
|
|
Lp = Lp + dot_gamma_twin(i)*prm%Schmid_twin(1:3,1:3,i) * f_unrotated
|
2019-03-19 02:47:11 +05:30
|
|
|
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
2018-09-17 11:53:23 +05:30
|
|
|
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
+ dgamma_dtau_twin(i)* prm%Schmid_twin(k,l,i)*prm%Schmid_twin(m,n,i) * f_unrotated
|
2018-09-01 14:15:34 +05:30
|
|
|
|
enddo twinContibution
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_twin(Mp,temperature,dot_gamma_sl,instance,of,dot_gamma_trans,dgamma_dtau_trans)
|
|
|
|
|
transContibution: do i = 1, prm%sum_N_tr
|
|
|
|
|
Lp = Lp + dot_gamma_trans(i)*prm%Schmid_trans(1:3,1:3,i) * f_unrotated
|
2019-03-19 02:47:11 +05:30
|
|
|
|
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
2019-01-28 00:14:53 +05:30
|
|
|
|
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
+ dgamma_dtau_trans(i)* prm%Schmid_trans(k,l,i)*prm%Schmid_trans(m,n,i) * f_unrotated
|
2019-01-28 00:14:53 +05:30
|
|
|
|
enddo transContibution
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
|
|
|
|
|
2018-07-17 01:07:26 +05:30
|
|
|
|
end associate
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2014-12-08 21:25:30 +05:30
|
|
|
|
end subroutine plastic_dislotwin_LpAndItsTangent
|
2011-04-13 17:21:46 +05:30
|
|
|
|
|
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief calculates the rate of change of microstructure
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2018-10-02 01:44:54 +05:30
|
|
|
|
subroutine plastic_dislotwin_dotState(Mp,Temperature,instance,of)
|
2013-11-27 21:50:27 +05:30
|
|
|
|
use prec, only: &
|
2016-05-29 14:15:03 +05:30
|
|
|
|
tol_math_check, &
|
2016-10-29 13:09:08 +05:30
|
|
|
|
dEq0
|
2013-11-27 21:50:27 +05:30
|
|
|
|
use math, only: &
|
2019-01-29 11:11:27 +05:30
|
|
|
|
math_clip, &
|
2018-08-31 15:07:14 +05:30
|
|
|
|
math_mul33xx33, &
|
2019-01-29 11:11:27 +05:30
|
|
|
|
PI
|
2013-11-27 21:50:27 +05:30
|
|
|
|
use material, only: &
|
2018-12-11 06:05:36 +05:30
|
|
|
|
plasticState
|
2011-04-13 17:21:46 +05:30
|
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
|
implicit none
|
2018-09-17 11:53:23 +05:30
|
|
|
|
real(pReal), dimension(3,3), intent(in):: &
|
|
|
|
|
Mp !< Mandel stress
|
2018-10-02 01:44:54 +05:30
|
|
|
|
real(pReal), intent(in) :: &
|
2013-10-08 21:57:26 +05:30
|
|
|
|
temperature !< temperature at integration point
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2018-10-02 01:44:54 +05:30
|
|
|
|
instance, &
|
|
|
|
|
of
|
2014-07-02 17:57:39 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i
|
2019-01-27 13:05:07 +05:30
|
|
|
|
real(pReal) :: f_unrotated,&
|
2019-01-29 11:22:55 +05:30
|
|
|
|
VacancyDiffusion,&
|
2019-01-28 00:14:53 +05:30
|
|
|
|
EdgeDipDistance, ClimbVelocity,DotRhoEdgeDipClimb,DotRhoEdgeDipAnnihilation, &
|
2019-01-29 11:22:55 +05:30
|
|
|
|
DotRhoDipFormation,DotRhoEdgeEdgeAnnihilation, &
|
2018-08-31 20:06:19 +05:30
|
|
|
|
tau
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
2019-01-29 11:22:55 +05:30
|
|
|
|
EdgeDipMinDistance, &
|
|
|
|
|
DotRhoMultiplication, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_sl
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
|
|
|
|
dot_gamma_twin
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
|
|
|
|
dot_gamma_trans
|
2015-12-12 00:06:58 +05:30
|
|
|
|
|
2018-10-02 01:44:54 +05:30
|
|
|
|
associate(prm => param(instance), stt => state(instance), &
|
2019-01-28 02:38:36 +05:30
|
|
|
|
dot => dotstate(instance), dst => microstructure(instance))
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
2018-09-15 11:54:12 +05:30
|
|
|
|
f_unrotated = 1.0_pReal &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
- sum(stt%twinFraction(1:prm%sum_N_tw,of)) &
|
|
|
|
|
- sum(stt%strainTransFraction(1:prm%sum_N_tr,of))
|
2019-01-29 11:22:55 +05:30
|
|
|
|
VacancyDiffusion = prm%D0*exp(-prm%Qsd/(kB*Temperature))
|
2018-09-15 11:54:12 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_slip(Mp,temperature,instance,of,dot_gamma_sl)
|
|
|
|
|
dot%accshear_slip(:,of) = abs(dot_gamma_sl)
|
2019-01-29 11:22:55 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
DotRhoMultiplication = abs(dot_gamma_sl)/(prm%b_sl*dst%Lambda_sl(:,of))
|
2019-03-19 03:14:54 +05:30
|
|
|
|
EdgeDipMinDistance = prm%CEdgeDipMinDistance*prm%b_sl
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
slipState: do i = 1, prm%sum_N_sl
|
2018-10-11 20:58:00 +05:30
|
|
|
|
tau = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,i))
|
2018-08-31 18:03:42 +05:30
|
|
|
|
|
2019-01-29 11:52:56 +05:30
|
|
|
|
significantSlipStress: if (dEq0(tau)) then
|
2018-08-31 18:03:42 +05:30
|
|
|
|
DotRhoDipFormation = 0.0_pReal
|
2019-01-29 11:52:56 +05:30
|
|
|
|
DotRhoEdgeDipClimb = 0.0_pReal
|
|
|
|
|
else significantSlipStress
|
2019-03-19 03:14:54 +05:30
|
|
|
|
EdgeDipDistance = 3.0_pReal*prm%mu*prm%b_sl(i)/(16.0_pReal*PI*abs(tau))
|
2019-03-19 11:18:12 +05:30
|
|
|
|
EdgeDipDistance = math_clip(EdgeDipDistance, right = dst%Lambda_sl(i,of))
|
2019-01-29 11:52:56 +05:30
|
|
|
|
EdgeDipDistance = math_clip(EdgeDipDistance, left = EdgeDipMinDistance(i))
|
|
|
|
|
|
2018-10-18 01:11:21 +05:30
|
|
|
|
if (prm%dipoleFormation) then
|
2019-03-19 03:14:54 +05:30
|
|
|
|
DotRhoDipFormation = 2.0_pReal*(EdgeDipDistance-EdgeDipMinDistance(i))/prm%b_sl(i) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
* stt%rhoEdge(i,of)*abs(dot_gamma_sl(i))
|
2018-10-18 01:11:21 +05:30
|
|
|
|
else
|
|
|
|
|
DotRhoDipFormation = 0.0_pReal
|
|
|
|
|
endif
|
2019-01-29 11:52:56 +05:30
|
|
|
|
|
|
|
|
|
if (dEq0(EdgeDipDistance-EdgeDipMinDistance(i))) then
|
|
|
|
|
DotRhoEdgeDipClimb = 0.0_pReal
|
|
|
|
|
else
|
|
|
|
|
ClimbVelocity = 3.0_pReal*prm%mu*VacancyDiffusion*prm%atomicVolume(i) &
|
|
|
|
|
/ (2.0_pReal*PI*kB*Temperature*(EdgeDipDistance+EdgeDipMinDistance(i)))
|
|
|
|
|
DotRhoEdgeDipClimb = 4.0_pReal*ClimbVelocity*stt%rhoEdgeDip(i,of) &
|
|
|
|
|
/ (EdgeDipDistance-EdgeDipMinDistance(i))
|
|
|
|
|
endif
|
|
|
|
|
endif significantSlipStress
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2018-08-31 18:03:42 +05:30
|
|
|
|
!* Spontaneous annihilation of 2 single edge dislocations
|
2019-03-19 03:14:54 +05:30
|
|
|
|
DotRhoEdgeEdgeAnnihilation = 2.0_pReal*EdgeDipMinDistance(i)/prm%b_sl(i) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
* stt%rhoEdge(i,of)*abs(dot_gamma_sl(i))
|
2018-08-31 18:03:42 +05:30
|
|
|
|
!* Spontaneous annihilation of a single edge dislocation with a dipole constituent
|
2019-03-19 03:14:54 +05:30
|
|
|
|
DotRhoEdgeDipAnnihilation = 2.0_pReal*EdgeDipMinDistance(i)/prm%b_sl(i) &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
* stt%rhoEdgeDip(i,of)*abs(dot_gamma_sl(i))
|
2019-01-29 11:52:56 +05:30
|
|
|
|
|
2019-01-29 11:22:55 +05:30
|
|
|
|
dot%rhoEdge(i,of) = DotRhoMultiplication(i)-DotRhoDipFormation-DotRhoEdgeEdgeAnnihilation
|
2018-09-14 15:26:36 +05:30
|
|
|
|
dot%rhoEdgeDip(i,of) = DotRhoDipFormation-DotRhoEdgeDipAnnihilation-DotRhoEdgeDipClimb
|
2018-10-11 20:58:00 +05:30
|
|
|
|
enddo slipState
|
2013-10-08 21:57:26 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_twin(Mp,temperature,dot_gamma_sl,instance,of,dot_gamma_twin)
|
|
|
|
|
dot%twinFraction(:,of) = f_unrotated*dot_gamma_twin/prm%shear_twin
|
2018-09-01 14:15:34 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_trans(Mp,temperature,dot_gamma_sl,instance,of,dot_gamma_trans)
|
|
|
|
|
dot%twinFraction(:,of) = f_unrotated*dot_gamma_trans
|
2018-08-31 19:38:01 +05:30
|
|
|
|
|
|
|
|
|
end associate
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2014-12-08 21:25:30 +05:30
|
|
|
|
end subroutine plastic_dislotwin_dotState
|
2011-04-13 17:21:46 +05:30
|
|
|
|
|
2018-09-12 16:55:18 +05:30
|
|
|
|
|
2019-01-27 13:05:07 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief calculates derived quantities from state
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
subroutine plastic_dislotwin_dependentState(temperature,instance,of)
|
|
|
|
|
use math, only: &
|
|
|
|
|
PI
|
|
|
|
|
|
|
|
|
|
implicit none
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2019-01-29 10:44:58 +05:30
|
|
|
|
instance, &
|
2019-01-27 13:05:07 +05:30
|
|
|
|
of
|
|
|
|
|
real(pReal), intent(in) :: &
|
2019-01-29 10:44:58 +05:30
|
|
|
|
temperature
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: &
|
2019-01-27 13:05:07 +05:30
|
|
|
|
i
|
|
|
|
|
real(pReal) :: &
|
|
|
|
|
sumf_twin,SFE,sumf_trans
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_sl_sl_inv, & !* 1/mean free distance between 2 forest dislocations seen by a moving dislocation
|
|
|
|
|
lambda_sl_tw_inv, & !* 1/mean free distance between 2 twin stacks from different systems seen by a moving dislocation
|
|
|
|
|
lambda_sl_tr_inv !* 1/mean free distance between 2 martensite lamellar from different systems seen by a moving dislocation
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tw) :: &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_tw_tw_inv !* 1/mean free distance between 2 twin stacks from different systems seen by a growing twin
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tr) :: &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_tr_tr_inv !* 1/mean free distance between 2 martensite stacks from different systems seen by a growing martensite (1/lambda_trans)
|
|
|
|
|
|
2019-01-27 13:05:07 +05:30
|
|
|
|
real(pReal), dimension(:), allocatable :: &
|
|
|
|
|
x0, &
|
|
|
|
|
fOverStacksize, &
|
|
|
|
|
ftransOverLamellarSize
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
associate(prm => param(instance),&
|
|
|
|
|
stt => state(instance),&
|
2019-01-28 02:38:36 +05:30
|
|
|
|
dst => microstructure(instance))
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
sumf_twin = sum(stt%twinFraction(1:prm%sum_N_tw,of))
|
|
|
|
|
sumf_trans = sum(stt%strainTransFraction(1:prm%sum_N_tr,of))
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-01-29 11:11:27 +05:30
|
|
|
|
SFE = prm%SFE_0K + prm%dSFE_dT * Temperature
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
|
|
|
|
!* rescaled volume fraction for topology
|
2019-03-20 14:16:49 +05:30
|
|
|
|
fOverStacksize = stt%twinFraction(1:prm%sum_N_tw,of)/prm%twinsize !ToDo: this is per system
|
2019-01-28 04:06:34 +05:30
|
|
|
|
ftransOverLamellarSize = sumf_trans/prm%lamellarsize !ToDo: But this not ...
|
2019-01-27 13:05:07 +05:30
|
|
|
|
!Todo: Physically ok, but naming could be adjusted
|
|
|
|
|
|
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
forall (i = 1:prm%sum_N_sl) &
|
2019-03-19 19:26:36 +05:30
|
|
|
|
lambda_sl_sl_inv(i) = &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
sqrt(dot_product((stt%rhoEdge(1:prm%sum_N_sl,of)+stt%rhoEdgeDip(1:prm%sum_N_sl,of)),&
|
|
|
|
|
prm%forestProjection(1:prm%sum_N_sl,i)))/prm%CLambdaSlip(i) ! change order and use matmul
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_tw > 0 .and. prm%sum_N_sl > 0) &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_sl_tw_inv = &
|
|
|
|
|
matmul(transpose(prm%h_sl_tw),fOverStacksize)/(1.0_pReal-sumf_twin) ! ToDo: Change order/no transpose
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
!ToDo: needed? if (prm%sum_N_tw > 0) &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_tw_tw_inv = matmul(prm%h_tw_tw,fOverStacksize)/(1.0_pReal-sumf_twin)
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if (prm%sum_N_tr > 0 .and. prm%sum_N_sl > 0) &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_sl_tr_inv = & ! ToDo: does not work if N_tr is not 12
|
|
|
|
|
matmul(transpose(prm%interaction_SlipTrans),ftransOverLamellarSize)/(1.0_pReal-sumf_trans) ! ToDo: remove transpose
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
!ToDo: needed? if (prm%sum_N_tr > 0) &
|
2019-03-19 11:18:12 +05:30
|
|
|
|
lambda_tr_tr_inv = matmul(prm%interaction_TransTrans,ftransOverLamellarSize)/(1.0_pReal-sumf_trans)
|
|
|
|
|
|
|
|
|
|
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if ((prm%sum_N_tw > 0) .or. (prm%sum_N_tr > 0)) then ! ToDo: Change order
|
2019-03-19 11:18:12 +05:30
|
|
|
|
dst%Lambda_sl(:,of) = &
|
2019-01-27 13:05:07 +05:30
|
|
|
|
prm%GrainSize/(1.0_pReal+prm%GrainSize*&
|
2019-03-19 11:18:12 +05:30
|
|
|
|
(lambda_sl_sl_inv + lambda_sl_tw_inv + lambda_sl_tr_inv))
|
2019-01-27 13:05:07 +05:30
|
|
|
|
else
|
2019-03-19 11:18:12 +05:30
|
|
|
|
dst%Lambda_sl(:,of) = prm%GrainSize &
|
|
|
|
|
/ (1.0_pReal+prm%GrainSize*lambda_sl_sl_inv) !!!!!! correct?
|
2019-01-27 13:05:07 +05:30
|
|
|
|
endif
|
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
|
|
|
|
|
|
|
|
|
|
dst%Lambda_tw(:,of) = prm%Cmfptwin *prm%GrainSize/(1.0_pReal+prm%GrainSize*lambda_tw_tw_inv)
|
|
|
|
|
dst%Lambda_tr(:,of) = prm%Cmfptrans*prm%GrainSize/(1.0_pReal+prm%GrainSize*lambda_tr_tr_inv)
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
|
|
|
|
!* threshold stress for dislocation motion
|
2019-03-20 14:16:49 +05:30
|
|
|
|
forall (i = 1:prm%sum_N_sl) dst%tau_pass(i,of) = &
|
2019-03-19 03:14:54 +05:30
|
|
|
|
prm%mu*prm%b_sl(i)*&
|
2019-03-20 14:16:49 +05:30
|
|
|
|
sqrt(dot_product(stt%rhoEdge(1:prm%sum_N_sl,of)+stt%rhoEdgeDip(1:prm%sum_N_sl,of),&
|
2019-03-19 02:38:41 +05:30
|
|
|
|
prm%h_sl_sl(:,i)))
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
|
|
|
|
!* threshold stress for growing twin/martensite
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if(prm%sum_N_tw == prm%sum_N_sl) &
|
2019-03-19 10:51:40 +05:30
|
|
|
|
dst%threshold_stress_twin(:,of) = &
|
|
|
|
|
(SFE/(3.0_pReal*prm%b_tw)+ 3.0_pReal*prm%b_tw*prm%mu/(prm%L0_twin*prm%b_sl)) ! slip burgers here correct?
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if(prm%sum_N_tr == prm%sum_N_sl) &
|
2019-03-19 10:51:40 +05:30
|
|
|
|
dst%threshold_stress_trans(:,of) = &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
(SFE/(3.0_pReal*prm%b_tr) + 3.0_pReal*prm%b_tr*prm%mu/&
|
|
|
|
|
(prm%L0_trans*prm%b_sl) + prm%transStackHeight*prm%deltaG/ (3.0_pReal*prm%b_tr) )
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
|
|
|
|
|
2019-03-19 11:18:12 +05:30
|
|
|
|
dst%twinVolume(:,of) = (PI/4.0_pReal)*prm%twinsize*dst%Lambda_tw(:,of)**2.0_pReal
|
|
|
|
|
dst%martensiteVolume(:,of) = (PI/4.0_pReal)*prm%lamellarsize*dst%Lambda_tr(:,of)**2.0_pReal
|
2019-01-28 04:06:34 +05:30
|
|
|
|
|
|
|
|
|
|
2019-03-19 03:14:54 +05:30
|
|
|
|
x0 = prm%mu*prm%b_tw**2.0_pReal/(SFE*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_twin(:,of) = prm%mu*prm%b_tw/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%xc_twin)+cos(pi/3.0_pReal)/x0)
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
x0 = prm%mu*prm%b_tr**2.0_pReal/(SFE*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_trans(:,of) = prm%mu*prm%b_tr/(2.0_pReal*PI)*(1.0_pReal/(x0+prm%xc_trans)+cos(pi/3.0_pReal)/x0)
|
2019-01-27 13:05:07 +05:30
|
|
|
|
|
2019-01-28 00:14:53 +05:30
|
|
|
|
end associate
|
|
|
|
|
|
2019-01-27 13:05:07 +05:30
|
|
|
|
end subroutine plastic_dislotwin_dependentState
|
|
|
|
|
|
|
|
|
|
|
2019-01-27 12:47:08 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief return array of constitutive results
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
function plastic_dislotwin_postResults(Mp,Temperature,instance,of) result(postResults)
|
|
|
|
|
use prec, only: &
|
|
|
|
|
tol_math_check, &
|
|
|
|
|
dEq0
|
|
|
|
|
use math, only: &
|
|
|
|
|
PI, &
|
2019-01-27 16:07:50 +05:30
|
|
|
|
math_mul33xx33
|
2019-01-27 12:47:08 +05:30
|
|
|
|
|
|
|
|
|
implicit none
|
|
|
|
|
real(pReal), dimension(3,3),intent(in) :: &
|
|
|
|
|
Mp !< 2nd Piola Kirchhoff stress tensor in Mandel notation
|
|
|
|
|
real(pReal), intent(in) :: &
|
|
|
|
|
temperature !< temperature at integration point
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2019-01-27 12:47:08 +05:30
|
|
|
|
instance, &
|
|
|
|
|
of
|
|
|
|
|
|
|
|
|
|
real(pReal), dimension(sum(plastic_dislotwin_sizePostResult(:,instance))) :: &
|
|
|
|
|
postResults
|
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: &
|
2019-01-28 00:14:53 +05:30
|
|
|
|
o,c,j
|
2019-01-27 12:47:08 +05:30
|
|
|
|
|
2019-01-28 02:38:36 +05:30
|
|
|
|
associate(prm => param(instance), stt => state(instance), dst => microstructure(instance))
|
2019-01-27 12:47:08 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
c = 0
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
do o = 1,size(prm%outputID)
|
2019-01-27 12:47:08 +05:30
|
|
|
|
select case(prm%outputID(o))
|
|
|
|
|
|
2019-03-19 02:38:41 +05:30
|
|
|
|
case (rho_mob_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_sl) = stt%rhoEdge(1:prm%sum_N_sl,of)
|
|
|
|
|
c = c + prm%sum_N_sl
|
2019-03-19 02:38:41 +05:30
|
|
|
|
case (rho_dip_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_sl) = stt%rhoEdgeDip(1:prm%sum_N_sl,of)
|
|
|
|
|
c = c + prm%sum_N_sl
|
2019-03-19 02:38:41 +05:30
|
|
|
|
case (gamma_dot_sl_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
call kinetics_slip(Mp,temperature,instance,of,postResults(c+1:c+prm%sum_N_sl))
|
|
|
|
|
c = c + prm%sum_N_sl
|
2019-03-19 02:38:41 +05:30
|
|
|
|
case (gamma_sl_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_sl) = stt%accshear_slip(1:prm%sum_N_sl,of)
|
|
|
|
|
c = c + prm%sum_N_sl
|
|
|
|
|
case (Lambda_sl_ID)
|
|
|
|
|
postResults(c+1:c+prm%sum_N_sl) = dst%Lambda_sl(1:prm%sum_N_sl,of)
|
|
|
|
|
c = c + prm%sum_N_sl
|
2019-01-27 12:47:08 +05:30
|
|
|
|
case (resolved_stress_slip_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do j = 1, prm%sum_N_sl
|
2019-01-27 12:47:08 +05:30
|
|
|
|
postResults(c+j) = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,j))
|
|
|
|
|
enddo
|
2019-03-20 14:16:49 +05:30
|
|
|
|
c = c + prm%sum_N_sl
|
2019-01-27 12:47:08 +05:30
|
|
|
|
case (threshold_stress_slip_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_sl) = dst%tau_pass(1:prm%sum_N_sl,of)
|
|
|
|
|
c = c + prm%sum_N_sl
|
2019-01-28 02:42:27 +05:30
|
|
|
|
|
2019-03-19 02:38:41 +05:30
|
|
|
|
case (f_tw_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_tw) = stt%twinFraction(1:prm%sum_N_tw,of)
|
|
|
|
|
c = c + prm%sum_N_tw
|
|
|
|
|
case (Lambda_tw_ID)
|
|
|
|
|
postResults(c+1:c+prm%sum_N_tw) = dst%Lambda_tw(1:prm%sum_N_tw,of)
|
|
|
|
|
c = c + prm%sum_N_tw
|
2019-01-27 12:47:08 +05:30
|
|
|
|
case (resolved_stress_twin_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do j = 1, prm%sum_N_tw
|
2019-01-27 12:47:08 +05:30
|
|
|
|
postResults(c+j) = math_mul33xx33(Mp,prm%Schmid_twin(1:3,1:3,j))
|
|
|
|
|
enddo
|
2019-03-20 14:16:49 +05:30
|
|
|
|
c = c + prm%sum_N_tw
|
2019-01-27 12:47:08 +05:30
|
|
|
|
case (threshold_stress_twin_ID)
|
2019-03-20 14:16:49 +05:30
|
|
|
|
postResults(c+1:c+prm%sum_N_tw) = dst%threshold_stress_twin(1:prm%sum_N_tw,of)
|
|
|
|
|
c = c + prm%sum_N_tw
|
2019-01-27 19:44:50 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
case (f_tr_ID)
|
|
|
|
|
postResults(c+1:c+prm%sum_N_tr) = stt%strainTransFraction(1:prm%sum_N_tr,of)
|
|
|
|
|
c = c + prm%sum_N_tr
|
2019-01-27 12:47:08 +05:30
|
|
|
|
end select
|
|
|
|
|
enddo
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-01-27 12:47:08 +05:30
|
|
|
|
end associate
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-01-27 12:47:08 +05:30
|
|
|
|
end function plastic_dislotwin_postResults
|
|
|
|
|
|
|
|
|
|
|
2019-03-10 01:13:31 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
!> @brief writes results to HDF5 output file
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
|
subroutine plastic_dislotwin_results(instance,group)
|
|
|
|
|
#if defined(PETSc) || defined(DAMASKHDF5)
|
|
|
|
|
use results
|
|
|
|
|
|
|
|
|
|
implicit none
|
|
|
|
|
integer, intent(in) :: instance
|
|
|
|
|
character(len=*) :: group
|
|
|
|
|
integer :: o
|
|
|
|
|
|
|
|
|
|
associate(prm => param(instance), stt => state(instance))
|
2019-03-19 02:47:11 +05:30
|
|
|
|
outputsLoop: do o = 1,size(prm%outputID)
|
2019-03-10 01:13:31 +05:30
|
|
|
|
select case(prm%outputID(o))
|
|
|
|
|
end select
|
|
|
|
|
enddo outputsLoop
|
|
|
|
|
end associate
|
|
|
|
|
#else
|
|
|
|
|
integer, intent(in) :: instance
|
|
|
|
|
character(len=*) :: group
|
|
|
|
|
#endif
|
|
|
|
|
|
|
|
|
|
end subroutine plastic_dislotwin_results
|
|
|
|
|
|
|
|
|
|
|
2018-09-12 16:55:18 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2019-01-27 21:29:44 +05:30
|
|
|
|
!> @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
|
2018-09-12 16:55:18 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2019-01-27 21:29:44 +05:30
|
|
|
|
pure subroutine kinetics_slip(Mp,Temperature,instance,of, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_sl,dgamma_dtau_slip,tau_slip)
|
2018-09-12 16:55:18 +05:30
|
|
|
|
use prec, only: &
|
|
|
|
|
tol_math_check, &
|
|
|
|
|
dNeq0
|
|
|
|
|
use math, only: &
|
|
|
|
|
math_mul33xx33
|
|
|
|
|
|
|
|
|
|
implicit none
|
2019-01-27 21:29:44 +05:30
|
|
|
|
real(pReal), dimension(3,3), intent(in) :: &
|
|
|
|
|
Mp !< Mandel stress
|
|
|
|
|
real(pReal), intent(in) :: &
|
|
|
|
|
temperature !< temperature
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2019-01-27 21:29:44 +05:30
|
|
|
|
instance, &
|
2018-09-12 16:55:18 +05:30
|
|
|
|
of
|
2019-01-27 21:29:44 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl), intent(out) :: &
|
|
|
|
|
dot_gamma_sl
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl), optional, intent(out) :: &
|
|
|
|
|
dgamma_dtau_slip, &
|
2019-01-27 21:29:44 +05:30
|
|
|
|
tau_slip
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
|
|
|
|
dgamma_dtau
|
2018-09-12 16:55:18 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl) :: &
|
2018-09-13 01:37:59 +05:30
|
|
|
|
tau, &
|
2018-09-12 16:55:18 +05:30
|
|
|
|
stressRatio, &
|
|
|
|
|
StressRatio_p, &
|
2018-10-02 19:26:18 +05:30
|
|
|
|
BoltzmannRatio, &
|
2019-01-27 21:29:44 +05:30
|
|
|
|
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)
|
2018-10-02 20:14:13 +05:30
|
|
|
|
dV_wait_inverse_dTau, &
|
|
|
|
|
dV_run_inverse_dTau, &
|
|
|
|
|
dV_dTau, &
|
2019-01-27 21:29:44 +05:30
|
|
|
|
tau_eff !< effective resolved stress
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i
|
2019-01-27 21:29:44 +05:30
|
|
|
|
|
|
|
|
|
associate(prm => param(instance), stt => state(instance), dst => microstructure(instance))
|
2018-09-12 16:55:18 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do i = 1, prm%sum_N_sl
|
2018-09-17 11:53:23 +05:30
|
|
|
|
tau(i) = math_mul33xx33(Mp,prm%Schmid_slip(1:3,1:3,i))
|
2018-09-12 16:55:18 +05:30
|
|
|
|
enddo
|
2018-10-02 19:26:18 +05:30
|
|
|
|
|
2019-03-19 10:51:40 +05:30
|
|
|
|
tau_eff = abs(tau)-dst%tau_pass(:,of)
|
2018-10-04 19:42:14 +05:30
|
|
|
|
|
2018-10-02 19:26:18 +05:30
|
|
|
|
significantStress: where(tau_eff > tol_math_check)
|
|
|
|
|
stressRatio = tau_eff/(prm%SolidSolutionStrength+prm%tau_peierls)
|
|
|
|
|
StressRatio_p = stressRatio** prm%p
|
|
|
|
|
BoltzmannRatio = prm%Qedge/(kB*Temperature)
|
|
|
|
|
v_wait_inverse = prm%v0**(-1.0_pReal) * exp(BoltzmannRatio*(1.0_pReal-StressRatio_p)** prm%q)
|
2019-03-19 03:14:54 +05:30
|
|
|
|
v_run_inverse = prm%B/(tau_eff*prm%b_sl)
|
2018-10-02 19:26:18 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_sl = sign(stt%rhoEdge(:,of)*prm%b_sl/(v_wait_inverse+v_run_inverse),tau)
|
2018-09-12 16:55:18 +05:30
|
|
|
|
|
2018-10-02 20:14:13 +05:30
|
|
|
|
dV_wait_inverse_dTau = 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%SolidSolutionStrength+prm%tau_peierls)
|
|
|
|
|
dV_run_inverse_dTau = v_run_inverse/tau_eff
|
|
|
|
|
dV_dTau = (dV_wait_inverse_dTau+dV_run_inverse_dTau) &
|
|
|
|
|
/ (v_wait_inverse+v_run_inverse)**2.0_pReal
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dgamma_dtau = dV_dTau*stt%rhoEdge(:,of)*prm%b_sl
|
2018-09-13 01:37:59 +05:30
|
|
|
|
else where significantStress
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_sl = 0.0_pReal
|
|
|
|
|
dgamma_dtau = 0.0_pReal
|
2018-09-13 01:37:59 +05:30
|
|
|
|
end where significantStress
|
|
|
|
|
|
2019-01-28 00:14:53 +05:30
|
|
|
|
end associate
|
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if(present(dgamma_dtau_slip)) dgamma_dtau_slip = dgamma_dtau
|
2019-01-27 21:29:44 +05:30
|
|
|
|
if(present(tau_slip)) tau_slip = tau
|
|
|
|
|
|
2018-10-02 19:26:18 +05:30
|
|
|
|
end subroutine kinetics_slip
|
2018-10-02 01:44:54 +05:30
|
|
|
|
|
|
|
|
|
|
2018-09-13 01:37:59 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2018-10-02 19:26:18 +05:30
|
|
|
|
!> @brief calculates shear rates on twin systems
|
2018-09-13 01:37:59 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2019-03-20 14:16:49 +05:30
|
|
|
|
pure subroutine kinetics_twin(Mp,temperature,dot_gamma_sl,instance,of,&
|
|
|
|
|
dot_gamma_twin,dgamma_dtau_twin)
|
2018-09-13 01:37:59 +05:30
|
|
|
|
use prec, only: &
|
|
|
|
|
tol_math_check, &
|
|
|
|
|
dNeq0
|
|
|
|
|
use math, only: &
|
|
|
|
|
math_mul33xx33
|
|
|
|
|
|
|
|
|
|
implicit none
|
2019-01-28 00:14:53 +05:30
|
|
|
|
real(pReal), dimension(3,3), intent(in) :: &
|
|
|
|
|
Mp !< Mandel stress
|
|
|
|
|
real(pReal), intent(in) :: &
|
|
|
|
|
temperature !< temperature
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer, intent(in) :: &
|
2019-01-28 00:14:53 +05:30
|
|
|
|
instance, &
|
2018-09-13 01:37:59 +05:30
|
|
|
|
of
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_sl), intent(in) :: &
|
|
|
|
|
dot_gamma_sl
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tw), intent(out) :: &
|
|
|
|
|
dot_gamma_twin
|
|
|
|
|
real(pReal), dimension(param(instance)%sum_N_tw), optional, intent(out) :: &
|
|
|
|
|
dgamma_dtau_twin
|
2018-09-12 16:55:18 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
real, dimension(param(instance)%sum_N_tw) :: &
|
2018-09-13 01:37:59 +05:30
|
|
|
|
tau, &
|
2019-01-28 00:14:53 +05:30
|
|
|
|
Ndot0, &
|
2018-09-13 01:37:59 +05:30
|
|
|
|
stressRatio_r, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dgamma_dtau
|
2018-09-13 01:37:59 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i,s1,s2
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
|
|
|
|
associate(prm => param(instance), stt => state(instance), dst => microstructure(instance))
|
2018-09-13 01:37:59 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do i = 1, prm%sum_N_tw
|
2018-09-17 11:53:23 +05:30
|
|
|
|
tau(i) = math_mul33xx33(Mp,prm%Schmid_twin(1:3,1:3,i))
|
2018-12-10 13:04:24 +05:30
|
|
|
|
isFCC: if (prm%fccTwinTransNucleation) then
|
2018-09-13 01:37:59 +05:30
|
|
|
|
s1=prm%fcc_twinNucleationSlipPair(1,i)
|
|
|
|
|
s2=prm%fcc_twinNucleationSlipPair(2,i)
|
2019-01-28 00:14:53 +05:30
|
|
|
|
if (tau(i) < dst%tau_r_twin(i,of)) then
|
2019-03-20 14:16:49 +05:30
|
|
|
|
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+&
|
|
|
|
|
abs(dot_gamma_sl(s2))*(stt%rhoEdge(s1,of)+stt%rhoEdgeDip(s1,of)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
|
2019-03-19 03:14:54 +05:30
|
|
|
|
(prm%L0_twin*prm%b_sl(i))*&
|
2018-09-13 01:37:59 +05:30
|
|
|
|
(1.0_pReal-exp(-prm%VcrossSlip/(kB*Temperature)*&
|
2019-01-28 00:14:53 +05:30
|
|
|
|
(dst%tau_r_twin(i,of)-tau)))
|
2018-09-13 01:37:59 +05:30
|
|
|
|
else
|
2019-01-28 00:14:53 +05:30
|
|
|
|
Ndot0=0.0_pReal
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2018-09-13 01:37:59 +05:30
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end if
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else isFCC
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2019-01-28 00:14:53 +05:30
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Ndot0=prm%Ndot0_twin(i)
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2018-09-13 01:37:59 +05:30
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endif isFCC
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enddo
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significantStress: where(tau > tol_math_check)
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2019-01-28 00:14:53 +05:30
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StressRatio_r = (dst%threshold_stress_twin(:,of)/tau)**prm%r
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2019-03-20 14:16:49 +05:30
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dot_gamma_twin = prm%shear_twin * dst%twinVolume(:,of) * Ndot0*exp(-StressRatio_r)
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dgamma_dtau = (dot_gamma_twin*prm%r/tau)*StressRatio_r
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2018-09-13 01:37:59 +05:30
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else where significantStress
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2019-03-20 14:16:49 +05:30
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dot_gamma_twin = 0.0_pReal
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dgamma_dtau = 0.0_pReal
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2018-09-13 01:37:59 +05:30
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end where significantStress
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2019-01-28 00:14:53 +05:30
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end associate
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2018-09-13 01:37:59 +05:30
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2019-03-20 14:16:49 +05:30
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if(present(dgamma_dtau_twin)) dgamma_dtau_twin = dgamma_dtau
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2018-09-12 16:55:18 +05:30
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2018-10-02 19:26:18 +05:30
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end subroutine kinetics_twin
|
2018-09-13 01:37:59 +05:30
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2019-01-28 00:14:53 +05:30
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2018-09-15 14:13:05 +05:30
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!--------------------------------------------------------------------------------------------------
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2019-01-28 00:14:53 +05:30
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!> @brief calculates shear rates on twin systems
|
2018-09-15 14:13:05 +05:30
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!--------------------------------------------------------------------------------------------------
|
2019-03-20 14:16:49 +05:30
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pure subroutine kinetics_trans(Mp,temperature,dot_gamma_sl,instance,of,&
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dot_gamma_trans,dgamma_dtau_trans)
|
2018-09-15 14:13:05 +05:30
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use prec, only: &
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tol_math_check, &
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dNeq0
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use math, only: &
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math_mul33xx33
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implicit none
|
2019-01-28 00:14:53 +05:30
|
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
|
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real(pReal), intent(in) :: &
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|
temperature !< temperature
|
2019-03-19 02:47:11 +05:30
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|
integer, intent(in) :: &
|
2019-01-28 00:14:53 +05:30
|
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|
instance, &
|
2018-09-15 14:13:05 +05:30
|
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|
of
|
2019-03-20 14:16:49 +05:30
|
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|
real(pReal), dimension(param(instance)%sum_N_sl), intent(in) :: &
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|
dot_gamma_sl
|
2019-01-28 00:14:53 +05:30
|
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|
2019-03-20 14:16:49 +05:30
|
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real(pReal), dimension(param(instance)%sum_N_tr), intent(out) :: &
|
|
|
|
|
dot_gamma_trans
|
|
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|
|
real(pReal), dimension(param(instance)%sum_N_tr), optional, intent(out) :: &
|
|
|
|
|
dgamma_dtau_trans
|
2018-09-15 14:13:05 +05:30
|
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|
2019-03-20 14:16:49 +05:30
|
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|
|
real, dimension(param(instance)%sum_N_tr) :: &
|
2018-09-15 14:13:05 +05:30
|
|
|
|
tau, &
|
2019-01-28 00:14:53 +05:30
|
|
|
|
Ndot0, &
|
|
|
|
|
stressRatio_s, &
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dgamma_dtau
|
2018-09-15 14:13:05 +05:30
|
|
|
|
|
2019-03-19 02:47:11 +05:30
|
|
|
|
integer :: i,s1,s2
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
|
|
|
|
associate(prm => param(instance), stt => state(instance), dst => microstructure(instance))
|
2018-09-15 14:13:05 +05:30
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
do i = 1, prm%sum_N_tr
|
2018-09-17 11:53:23 +05:30
|
|
|
|
tau(i) = math_mul33xx33(Mp,prm%Schmid_trans(1:3,1:3,i))
|
2018-12-10 13:04:24 +05:30
|
|
|
|
isFCC: if (prm%fccTwinTransNucleation) then
|
2018-09-15 14:13:05 +05:30
|
|
|
|
s1=prm%fcc_twinNucleationSlipPair(1,i)
|
|
|
|
|
s2=prm%fcc_twinNucleationSlipPair(2,i)
|
2019-01-28 00:14:53 +05:30
|
|
|
|
if (tau(i) < dst%tau_r_trans(i,of)) then
|
2019-03-20 14:16:49 +05:30
|
|
|
|
Ndot0=(abs(dot_gamma_sl(s1))*(stt%rhoEdge(s2,of)+stt%rhoEdgeDip(s2,of))+&
|
|
|
|
|
abs(dot_gamma_sl(s2))*(stt%rhoEdge(s1,of)+stt%rhoEdgeDip(s1,of)))/& ! ToDo: MD: it would be more consistent to use shearrates from state
|
2019-03-19 03:14:54 +05:30
|
|
|
|
(prm%L0_trans*prm%b_sl(i))*&
|
2018-09-15 14:13:05 +05:30
|
|
|
|
(1.0_pReal-exp(-prm%VcrossSlip/(kB*Temperature)*&
|
2019-01-28 00:14:53 +05:30
|
|
|
|
(dst%tau_r_trans(i,of)-tau)))
|
2018-09-15 14:13:05 +05:30
|
|
|
|
else
|
2019-01-28 00:14:53 +05:30
|
|
|
|
Ndot0=0.0_pReal
|
2018-09-15 14:13:05 +05:30
|
|
|
|
end if
|
|
|
|
|
else isFCC
|
2019-01-28 00:14:53 +05:30
|
|
|
|
Ndot0=prm%Ndot0_trans(i)
|
2018-09-15 14:13:05 +05:30
|
|
|
|
endif isFCC
|
|
|
|
|
enddo
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
|
|
|
|
significantStress: where(tau > tol_math_check)
|
|
|
|
|
StressRatio_s = (dst%threshold_stress_trans(:,of)/tau)**prm%s
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_trans = dst%martensiteVolume(:,of) * Ndot0*exp(-StressRatio_s)
|
|
|
|
|
dgamma_dtau = (dot_gamma_trans*prm%r/tau)*StressRatio_s
|
2019-01-28 00:14:53 +05:30
|
|
|
|
else where significantStress
|
2019-03-20 14:16:49 +05:30
|
|
|
|
dot_gamma_trans = 0.0_pReal
|
|
|
|
|
dgamma_dtau = 0.0_pReal
|
2019-01-28 00:14:53 +05:30
|
|
|
|
end where significantStress
|
|
|
|
|
|
|
|
|
|
end associate
|
|
|
|
|
|
2019-03-20 14:16:49 +05:30
|
|
|
|
if(present(dgamma_dtau_trans)) dgamma_dtau_trans = dgamma_dtau
|
2019-01-28 00:14:53 +05:30
|
|
|
|
|
2018-10-02 19:26:18 +05:30
|
|
|
|
end subroutine kinetics_trans
|
2018-09-15 11:54:12 +05:30
|
|
|
|
|
2016-02-26 20:06:24 +05:30
|
|
|
|
end module plastic_dislotwin
|