3297 lines
181 KiB
Fortran
3297 lines
181 KiB
Fortran
! Copyright 2011 Max-Planck-Institut für Eisenforschung GmbH
|
|
!
|
|
! This file is part of DAMASK,
|
|
! the Düsseldorf Advanced MAterial Simulation Kit.
|
|
!
|
|
! DAMASK is free software: you can redistribute it and/or modify
|
|
! it under the terms of the GNU General Public License as published by
|
|
! the Free Software Foundation, either version 3 of the License, or
|
|
! (at your option) any later version.
|
|
!
|
|
! DAMASK is distributed in the hope that it will be useful,
|
|
! but WITHOUT ANY WARRANTY; without even the implied warranty of
|
|
! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
|
|
! GNU General Public License for more details.
|
|
!
|
|
! You should have received a copy of the GNU General Public License
|
|
! along with DAMASK. If not, see <http://www.gnu.org/licenses/>.
|
|
!
|
|
!##############################################################
|
|
!* $Id$
|
|
!************************************
|
|
!* Module: CONSTITUTIVE_NONLOCAL *
|
|
!************************************
|
|
!* contains: *
|
|
!* - constitutive equations *
|
|
!* - parameters definition *
|
|
!************************************
|
|
|
|
|
|
MODULE constitutive_nonlocal
|
|
|
|
!* Include other modules
|
|
use prec, only: pReal,pInt
|
|
|
|
implicit none
|
|
private
|
|
|
|
|
|
!* Definition of parameters
|
|
|
|
character (len=*), parameter, public :: &
|
|
constitutive_nonlocal_label = 'nonlocal'
|
|
|
|
character(len=22), dimension(10), parameter, private :: &
|
|
constitutive_nonlocal_listBasicStates = (/'rhoSglEdgePosMobile ', &
|
|
'rhoSglEdgeNegMobile ', &
|
|
'rhoSglScrewPosMobile ', &
|
|
'rhoSglScrewNegMobile ', &
|
|
'rhoSglEdgePosImmobile ', &
|
|
'rhoSglEdgeNegImmobile ', &
|
|
'rhoSglScrewPosImmobile', &
|
|
'rhoSglScrewNegImmobile', &
|
|
'rhoDipEdge ', &
|
|
'rhoDipScrew ' /)! list of "basic" microstructural state variables that are independent from other state variables
|
|
|
|
character(len=16), dimension(3), parameter, private :: &
|
|
constitutive_nonlocal_listDependentStates = (/'rhoForest ', &
|
|
'tauThreshold ', &
|
|
'tauBack ' /) ! list of microstructural state variables that depend on other state variables
|
|
|
|
character(len=20), dimension(6), parameter, private :: &
|
|
constitutive_nonlocal_listOtherStates = (/'velocityEdgePos ', &
|
|
'velocityEdgeNeg ', &
|
|
'velocityScrewPos ', &
|
|
'velocityScrewNeg ', &
|
|
'maxDipoleHeightEdge ', &
|
|
'maxDipoleHeightScrew' /) ! list of other dependent state variables that are not updated by microstructure
|
|
|
|
real(pReal), parameter, private :: &
|
|
kB = 1.38e-23_pReal ! Physical parameter, Boltzmann constant in J/Kelvin
|
|
|
|
|
|
!* Definition of global variables
|
|
|
|
integer(pInt), dimension(:), allocatable, public :: &
|
|
constitutive_nonlocal_sizeDotState, & ! number of dotStates = number of basic state variables
|
|
constitutive_nonlocal_sizeDependentState, & ! number of dependent state variables
|
|
constitutive_nonlocal_sizeState, & ! total number of state variables
|
|
constitutive_nonlocal_sizePostResults ! cumulative size of post results
|
|
|
|
integer(pInt), dimension(:,:), allocatable, target, public :: &
|
|
constitutive_nonlocal_sizePostResult ! size of each post result output
|
|
|
|
character(len=64), dimension(:,:), allocatable, target, public :: &
|
|
constitutive_nonlocal_output ! name of each post result output
|
|
|
|
integer(pInt), dimension(:), allocatable, private :: &
|
|
constitutive_nonlocal_Noutput ! number of outputs per instance of this plasticity
|
|
|
|
character(len=32), dimension(:), allocatable, private :: &
|
|
constitutive_nonlocal_structureName ! name of the lattice structure
|
|
|
|
integer(pInt), dimension(:), allocatable, public :: &
|
|
constitutive_nonlocal_structure ! number representing the kind of lattice structure
|
|
|
|
integer(pInt), dimension(:), allocatable, private :: &
|
|
constitutive_nonlocal_totalNslip ! total number of active slip systems for each instance
|
|
|
|
integer(pInt), dimension(:,:), allocatable, private :: &
|
|
constitutive_nonlocal_Nslip, & ! number of active slip systems for each family and instance
|
|
constitutive_nonlocal_slipFamily, & ! lookup table relating active slip system to slip family for each instance
|
|
constitutive_nonlocal_slipSystemLattice, & ! lookup table relating active slip system index to lattice slip system index for each instance
|
|
constitutive_nonlocal_colinearSystem ! colinear system to the active slip system (only valid for fcc!)
|
|
|
|
real(pReal), dimension(:), allocatable, private :: &
|
|
constitutive_nonlocal_CoverA, & ! c/a ratio for hex type lattice
|
|
constitutive_nonlocal_C11, & ! C11 element in elasticity matrix
|
|
constitutive_nonlocal_C12, & ! C12 element in elasticity matrix
|
|
constitutive_nonlocal_C13, & ! C13 element in elasticity matrix
|
|
constitutive_nonlocal_C33, & ! C33 element in elasticity matrix
|
|
constitutive_nonlocal_C44, & ! C44 element in elasticity matrix
|
|
constitutive_nonlocal_Gmod, & ! shear modulus
|
|
constitutive_nonlocal_nu, & ! poisson's ratio
|
|
constitutive_nonlocal_atomicVolume, & ! atomic volume
|
|
constitutive_nonlocal_Dsd0, & ! prefactor for self-diffusion coefficient
|
|
constitutive_nonlocal_Qsd, & ! activation enthalpy for diffusion
|
|
constitutive_nonlocal_aTolRho, & ! absolute tolerance for dislocation density in state integration
|
|
constitutive_nonlocal_R, & ! cutoff radius for dislocation stress
|
|
constitutive_nonlocal_doublekinkwidth, & ! width of a doubkle kink in multiples of the burgers vector length b
|
|
constitutive_nonlocal_solidSolutionEnergy, & ! activation energy for solid solution in J
|
|
constitutive_nonlocal_solidSolutionSize, & ! solid solution obstacle size in multiples of the burgers vector length
|
|
constitutive_nonlocal_solidSolutionConcentration, & ! concentration of solid solution in atomic parts
|
|
constitutive_nonlocal_p, & ! parameter for kinetic law (Kocks,Argon,Ashby)
|
|
constitutive_nonlocal_q, & ! parameter for kinetic law (Kocks,Argon,Ashby)
|
|
constitutive_nonlocal_viscosity, & ! viscosity for dislocation glide in Pa s
|
|
constitutive_nonlocal_fattack, & ! attack frequency in Hz
|
|
constitutive_nonlocal_rhoSglScatter, & ! standard deviation of scatter in initial dislocation density
|
|
constitutive_nonlocal_surfaceTransmissivity, & ! transmissivity at free surface
|
|
constitutive_nonlocal_grainboundaryTransmissivity, & ! transmissivity at grain boundary (identified by different texture)
|
|
constitutive_nonlocal_CFLfactor ! safety factor for CFL flux condition
|
|
|
|
real(pReal), dimension(:,:), allocatable, private :: &
|
|
constitutive_nonlocal_rhoSglEdgePos0, & ! initial edge_pos dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_rhoSglEdgeNeg0, & ! initial edge_neg dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_rhoSglScrewPos0, & ! initial screw_pos dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_rhoSglScrewNeg0, & ! initial screw_neg dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_rhoDipEdge0, & ! initial edge dipole dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_rhoDipScrew0, & ! initial screw dipole dislocation density per slip system for each family and instance
|
|
constitutive_nonlocal_lambda0PerSlipFamily, & ! mean free path prefactor for each family and instance
|
|
constitutive_nonlocal_lambda0, & ! mean free path prefactor for each slip system and instance
|
|
constitutive_nonlocal_burgersPerSlipFamily, & ! absolute length of burgers vector [m] for each family and instance
|
|
constitutive_nonlocal_burgers, & ! absolute length of burgers vector [m] for each slip system and instance
|
|
constitutive_nonlocal_interactionSlipSlip ! coefficients for slip-slip interaction for each interaction type and instance
|
|
|
|
real(pReal), dimension(:,:,:), allocatable, private :: &
|
|
constitutive_nonlocal_Cslip_66, & ! elasticity matrix in Mandel notation for each instance
|
|
constitutive_nonlocal_minimumDipoleHeightPerSlipFamily, & ! minimum stable edge/screw dipole height for each family and instance
|
|
constitutive_nonlocal_minimumDipoleHeight, & ! minimum stable edge/screw dipole height for each slip system and instance
|
|
constitutive_nonlocal_peierlsStressPerSlipFamily, & ! Peierls stress (edge and screw)
|
|
constitutive_nonlocal_peierlsStress, & ! Peierls stress (edge and screw)
|
|
constitutive_nonlocal_forestProjectionEdge, & ! matrix of forest projections of edge dislocations for each instance
|
|
constitutive_nonlocal_forestProjectionScrew, & ! matrix of forest projections of screw dislocations for each instance
|
|
constitutive_nonlocal_interactionMatrixSlipSlip ! interaction matrix of the different slip systems for each instance
|
|
|
|
real(pReal), dimension(:,:,:,:), allocatable, private :: &
|
|
constitutive_nonlocal_lattice2slip, & ! orthogonal transformation matrix from lattice coordinate system to slip coordinate system (passive rotation !!!)
|
|
constitutive_nonlocal_accumulatedShear, & ! accumulated shear per slip system up to the start of the FE increment
|
|
constitutive_nonlocal_rhoDotEdgeJogs
|
|
|
|
real(pReal), dimension(:,:,:,:,:), allocatable, private :: &
|
|
constitutive_nonlocal_Cslip_3333, & ! elasticity matrix for each instance
|
|
constitutive_nonlocal_rhoDotFlux, & ! dislocation convection term
|
|
constitutive_nonlocal_rhoDotMultiplication, &
|
|
constitutive_nonlocal_rhoDotSingle2DipoleGlide, &
|
|
constitutive_nonlocal_rhoDotAthermalAnnihilation, &
|
|
constitutive_nonlocal_rhoDotThermalAnnihilation
|
|
|
|
real(pReal), dimension(:,:,:,:,:,:), allocatable, private :: &
|
|
constitutive_nonlocal_compatibility ! slip system compatibility between me and my neighbors
|
|
|
|
logical, dimension(:), allocatable, private :: &
|
|
constitutive_nonlocal_shortRangeStressCorrection ! flag indicating the use of the short range stress correction by a excess density gradient term
|
|
|
|
public :: &
|
|
constitutive_nonlocal_init, &
|
|
constitutive_nonlocal_stateInit, &
|
|
constitutive_nonlocal_aTolState, &
|
|
constitutive_nonlocal_homogenizedC, &
|
|
constitutive_nonlocal_microstructure, &
|
|
constitutive_nonlocal_LpAndItsTangent, &
|
|
constitutive_nonlocal_dotState, &
|
|
constitutive_nonlocal_deltaState, &
|
|
constitutive_nonlocal_dotTemperature, &
|
|
constitutive_nonlocal_updateCompatibility, &
|
|
constitutive_nonlocal_postResults
|
|
|
|
private :: &
|
|
constitutive_nonlocal_kinetics
|
|
|
|
|
|
CONTAINS
|
|
|
|
!**************************************
|
|
!* Module initialization *
|
|
!**************************************
|
|
subroutine constitutive_nonlocal_init(myFile)
|
|
|
|
use, intrinsic :: iso_fortran_env ! to get compiler_version and compiler_options (at least for gfortran 4.6 at the moment)
|
|
use prec, only: pInt, pReal
|
|
use math, only: math_Mandel3333to66, &
|
|
math_Voigt66to3333, &
|
|
math_mul3x3, &
|
|
math_transpose33
|
|
use IO, only: IO_lc, &
|
|
IO_getTag, &
|
|
IO_isBlank, &
|
|
IO_stringPos, &
|
|
IO_stringValue, &
|
|
IO_floatValue, &
|
|
IO_intValue, &
|
|
IO_error
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips, &
|
|
FE_maxNipNeighbors
|
|
use material, only: homogenization_maxNgrains, &
|
|
phase_plasticity, &
|
|
phase_plasticityInstance, &
|
|
phase_Noutput
|
|
use lattice, only: lattice_maxNslipFamily, &
|
|
lattice_maxNslip, &
|
|
lattice_maxNinteraction, &
|
|
lattice_NslipSystem, &
|
|
lattice_initializeStructure, &
|
|
lattice_sd, &
|
|
lattice_sn, &
|
|
lattice_st, &
|
|
lattice_interactionSlipSlip
|
|
|
|
!*** output variables
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: myFile
|
|
|
|
!*** local variables
|
|
integer(pInt), parameter :: maxNchunks = 21_pInt
|
|
integer(pInt), &
|
|
dimension(1_pInt+2_pInt*maxNchunks) :: positions
|
|
integer(pInt) section, &
|
|
maxNinstance, &
|
|
maxTotalNslip, &
|
|
myStructure, &
|
|
f, & ! index of my slip family
|
|
i, & ! index of my instance of this plasticity
|
|
j, &
|
|
k, &
|
|
l, &
|
|
ns, & ! short notation for total number of active slip systems for the current instance
|
|
o, & ! index of my output
|
|
s, & ! index of my slip system
|
|
s1, & ! index of my slip system
|
|
s2, & ! index of my slip system
|
|
it, & ! index of my interaction type
|
|
mySize
|
|
character(len=64) tag
|
|
character(len=1024) line
|
|
|
|
|
|
!$OMP CRITICAL (write2out)
|
|
write(6,*)
|
|
write(6,*) '<<<+- constitutive_',trim(constitutive_nonlocal_label),' init -+>>>'
|
|
write(6,*) '$Id$'
|
|
#include "compilation_info.f90"
|
|
!$OMP END CRITICAL (write2out)
|
|
|
|
maxNinstance = int(count(phase_plasticity == constitutive_nonlocal_label),pInt)
|
|
if (maxNinstance == 0) return ! we don't have to do anything if there's no instance for this constitutive law
|
|
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt) then
|
|
!$OMP CRITICAL (write2out)
|
|
write(6,'(a16,1x,i5)') '# instances:',maxNinstance
|
|
!$OMP END CRITICAL (write2out)
|
|
endif
|
|
|
|
|
|
!*** space allocation for global variables
|
|
|
|
allocate(constitutive_nonlocal_sizeDotState(maxNinstance))
|
|
allocate(constitutive_nonlocal_sizeDependentState(maxNinstance))
|
|
allocate(constitutive_nonlocal_sizeState(maxNinstance))
|
|
allocate(constitutive_nonlocal_sizePostResults(maxNinstance))
|
|
allocate(constitutive_nonlocal_sizePostResult(maxval(phase_Noutput), maxNinstance))
|
|
allocate(constitutive_nonlocal_output(maxval(phase_Noutput), maxNinstance))
|
|
allocate(constitutive_nonlocal_Noutput(maxNinstance))
|
|
constitutive_nonlocal_sizeDotState = 0_pInt
|
|
constitutive_nonlocal_sizeDependentState = 0_pInt
|
|
constitutive_nonlocal_sizeState = 0_pInt
|
|
constitutive_nonlocal_sizePostResults = 0_pInt
|
|
constitutive_nonlocal_sizePostResult = 0_pInt
|
|
constitutive_nonlocal_output = ''
|
|
constitutive_nonlocal_Noutput = 0_pInt
|
|
|
|
allocate(constitutive_nonlocal_structureName(maxNinstance))
|
|
allocate(constitutive_nonlocal_structure(maxNinstance))
|
|
allocate(constitutive_nonlocal_Nslip(lattice_maxNslipFamily, maxNinstance))
|
|
allocate(constitutive_nonlocal_slipFamily(lattice_maxNslip, maxNinstance))
|
|
allocate(constitutive_nonlocal_slipSystemLattice(lattice_maxNslip, maxNinstance))
|
|
allocate(constitutive_nonlocal_totalNslip(maxNinstance))
|
|
constitutive_nonlocal_structureName = ''
|
|
constitutive_nonlocal_structure = 0_pInt
|
|
constitutive_nonlocal_Nslip = 0_pInt
|
|
constitutive_nonlocal_slipFamily = 0_pInt
|
|
constitutive_nonlocal_slipSystemLattice = 0_pInt
|
|
constitutive_nonlocal_totalNslip = 0_pInt
|
|
|
|
allocate(constitutive_nonlocal_CoverA(maxNinstance))
|
|
allocate(constitutive_nonlocal_C11(maxNinstance))
|
|
allocate(constitutive_nonlocal_C12(maxNinstance))
|
|
allocate(constitutive_nonlocal_C13(maxNinstance))
|
|
allocate(constitutive_nonlocal_C33(maxNinstance))
|
|
allocate(constitutive_nonlocal_C44(maxNinstance))
|
|
allocate(constitutive_nonlocal_Gmod(maxNinstance))
|
|
allocate(constitutive_nonlocal_nu(maxNinstance))
|
|
allocate(constitutive_nonlocal_atomicVolume(maxNinstance))
|
|
allocate(constitutive_nonlocal_Dsd0(maxNinstance))
|
|
allocate(constitutive_nonlocal_Qsd(maxNinstance))
|
|
allocate(constitutive_nonlocal_aTolRho(maxNinstance))
|
|
allocate(constitutive_nonlocal_Cslip_66(6,6,maxNinstance))
|
|
allocate(constitutive_nonlocal_Cslip_3333(3,3,3,3,maxNinstance))
|
|
allocate(constitutive_nonlocal_R(maxNinstance))
|
|
allocate(constitutive_nonlocal_doublekinkwidth(maxNinstance))
|
|
allocate(constitutive_nonlocal_solidSolutionEnergy(maxNinstance))
|
|
allocate(constitutive_nonlocal_solidSolutionSize(maxNinstance))
|
|
allocate(constitutive_nonlocal_solidSolutionConcentration(maxNinstance))
|
|
allocate(constitutive_nonlocal_p(maxNinstance))
|
|
allocate(constitutive_nonlocal_q(maxNinstance))
|
|
allocate(constitutive_nonlocal_viscosity(maxNinstance))
|
|
allocate(constitutive_nonlocal_fattack(maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoSglScatter(maxNinstance))
|
|
allocate(constitutive_nonlocal_surfaceTransmissivity(maxNinstance))
|
|
allocate(constitutive_nonlocal_grainboundaryTransmissivity(maxNinstance))
|
|
allocate(constitutive_nonlocal_shortRangeStressCorrection(maxNinstance))
|
|
allocate(constitutive_nonlocal_CFLfactor(maxNinstance))
|
|
constitutive_nonlocal_CoverA = 0.0_pReal
|
|
constitutive_nonlocal_C11 = 0.0_pReal
|
|
constitutive_nonlocal_C12 = 0.0_pReal
|
|
constitutive_nonlocal_C13 = 0.0_pReal
|
|
constitutive_nonlocal_C33 = 0.0_pReal
|
|
constitutive_nonlocal_C44 = 0.0_pReal
|
|
constitutive_nonlocal_Gmod = 0.0_pReal
|
|
constitutive_nonlocal_atomicVolume = 0.0_pReal
|
|
constitutive_nonlocal_Dsd0 = -1.0_pReal
|
|
constitutive_nonlocal_Qsd = 0.0_pReal
|
|
constitutive_nonlocal_aTolRho = 0.0_pReal
|
|
constitutive_nonlocal_nu = 0.0_pReal
|
|
constitutive_nonlocal_Cslip_66 = 0.0_pReal
|
|
constitutive_nonlocal_Cslip_3333 = 0.0_pReal
|
|
constitutive_nonlocal_R = -1.0_pReal
|
|
constitutive_nonlocal_doublekinkwidth = 0.0_pReal
|
|
constitutive_nonlocal_solidSolutionEnergy = 0.0_pReal
|
|
constitutive_nonlocal_solidSolutionSize = 0.0_pReal
|
|
constitutive_nonlocal_solidSolutionConcentration = 0.0_pReal
|
|
constitutive_nonlocal_p = 1.0_pReal
|
|
constitutive_nonlocal_q = 1.0_pReal
|
|
constitutive_nonlocal_viscosity = 0.0_pReal
|
|
constitutive_nonlocal_fattack = 0.0_pReal
|
|
constitutive_nonlocal_rhoSglScatter = 0.0_pReal
|
|
constitutive_nonlocal_surfaceTransmissivity = 1.0_pReal
|
|
constitutive_nonlocal_grainboundaryTransmissivity = -1.0_pReal
|
|
constitutive_nonlocal_CFLfactor = 2.0_pReal
|
|
constitutive_nonlocal_shortRangeStressCorrection = .true.
|
|
|
|
allocate(constitutive_nonlocal_rhoSglEdgePos0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoSglEdgeNeg0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoSglScrewPos0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoSglScrewNeg0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoDipEdge0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_rhoDipScrew0(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_burgersPerSlipFamily(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_Lambda0PerSlipFamily(lattice_maxNslipFamily,maxNinstance))
|
|
allocate(constitutive_nonlocal_interactionSlipSlip(lattice_maxNinteraction,maxNinstance))
|
|
constitutive_nonlocal_rhoSglEdgePos0 = -1.0_pReal
|
|
constitutive_nonlocal_rhoSglEdgeNeg0 = -1.0_pReal
|
|
constitutive_nonlocal_rhoSglScrewPos0 = -1.0_pReal
|
|
constitutive_nonlocal_rhoSglScrewNeg0 = -1.0_pReal
|
|
constitutive_nonlocal_rhoDipEdge0 = -1.0_pReal
|
|
constitutive_nonlocal_rhoDipScrew0 = -1.0_pReal
|
|
constitutive_nonlocal_burgersPerSlipFamily = 0.0_pReal
|
|
constitutive_nonlocal_lambda0PerSlipFamily = 0.0_pReal
|
|
constitutive_nonlocal_interactionSlipSlip = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(lattice_maxNslipFamily,2,maxNinstance))
|
|
allocate(constitutive_nonlocal_peierlsStressPerSlipFamily(lattice_maxNslipFamily,2,maxNinstance))
|
|
constitutive_nonlocal_minimumDipoleHeightPerSlipFamily = -1.0_pReal
|
|
constitutive_nonlocal_peierlsStressPerSlipFamily = 0.0_pReal
|
|
|
|
!*** readout data from material.config file
|
|
|
|
rewind(myFile)
|
|
line = ''
|
|
section = 0_pInt
|
|
|
|
do while (IO_lc(IO_getTag(line,'<','>')) /= 'phase') ! wind forward to <phase>
|
|
read(myFile,'(a1024)',END=100) line
|
|
enddo
|
|
|
|
do ! read thru sections of phase part
|
|
read(myFile,'(a1024)',END=100) line
|
|
if (IO_isBlank(line)) cycle ! skip empty lines
|
|
if (IO_getTag(line,'<','>') /= '') exit ! stop at next part
|
|
if (IO_getTag(line,'[',']') /= '') then ! next section
|
|
section = section + 1_pInt ! advance section counter
|
|
cycle
|
|
endif
|
|
if (section > 0_pInt .and. phase_plasticity(section) == constitutive_nonlocal_label) then ! one of my sections
|
|
i = phase_plasticityInstance(section) ! which instance of my plasticity is present phase
|
|
positions = IO_stringPos(line,maxNchunks)
|
|
tag = IO_lc(IO_stringValue(line,positions,1_pInt)) ! extract key
|
|
select case(tag)
|
|
case('plasticity','elasticity','/nonlocal/')
|
|
cycle
|
|
case ('(output)')
|
|
constitutive_nonlocal_Noutput(i) = constitutive_nonlocal_Noutput(i) + 1_pInt
|
|
constitutive_nonlocal_output(constitutive_nonlocal_Noutput(i),i) = IO_lc(IO_stringValue(line,positions,2_pInt))
|
|
case ('lattice_structure')
|
|
constitutive_nonlocal_structureName(i) = IO_lc(IO_stringValue(line,positions,2_pInt))
|
|
case ('c/a_ratio','covera_ratio')
|
|
constitutive_nonlocal_CoverA(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('c11')
|
|
constitutive_nonlocal_C11(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('c12')
|
|
constitutive_nonlocal_C12(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('c13')
|
|
constitutive_nonlocal_C13(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('c33')
|
|
constitutive_nonlocal_C33(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('c44')
|
|
constitutive_nonlocal_C44(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('nslip')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_Nslip(f,i) = IO_intValue(line,positions,1_pInt+f)
|
|
case ('rhosgledgepos0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoSglEdgePos0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('rhosgledgeneg0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoSglEdgeNeg0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('rhosglscrewpos0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoSglScrewPos0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('rhosglscrewneg0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoSglScrewNeg0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('rhodipedge0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoDipEdge0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('rhodipscrew0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_rhoDipScrew0(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('lambda0')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_lambda0PerSlipFamily(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case ('burgers')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_burgersPerSlipFamily(f,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case('cutoffradius','r')
|
|
constitutive_nonlocal_R(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('minimumdipoleheightedge','ddipminedge')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(f,1_pInt,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case('minimumdipoleheightscrew','ddipminscrew')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(f,2_pInt,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case('atomicvolume')
|
|
constitutive_nonlocal_atomicVolume(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('selfdiffusionprefactor','dsd0')
|
|
constitutive_nonlocal_Dsd0(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('selfdiffusionenergy','qsd')
|
|
constitutive_nonlocal_Qsd(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('atol_rho')
|
|
constitutive_nonlocal_aTolRho(i) = IO_floatValue(line,positions,2_pInt)
|
|
case ('interaction_slipslip')
|
|
forall (it = 1_pInt:lattice_maxNinteraction) &
|
|
constitutive_nonlocal_interactionSlipSlip(it,i) = IO_floatValue(line,positions,1_pInt+it)
|
|
case('peierlsstressedge')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_peierlsStressPerSlipFamily(f,1_pInt,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case('peierlsstressscrew')
|
|
forall (f = 1_pInt:lattice_maxNslipFamily) &
|
|
constitutive_nonlocal_peierlsStressPerSlipFamily(f,2_pInt,i) = IO_floatValue(line,positions,1_pInt+f)
|
|
case('doublekinkwidth')
|
|
constitutive_nonlocal_doublekinkwidth(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('solidsolutionenergy')
|
|
constitutive_nonlocal_solidSolutionEnergy(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('solidsolutionsize')
|
|
constitutive_nonlocal_solidSolutionSize(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('solidsolutionconcentration')
|
|
constitutive_nonlocal_solidSolutionConcentration(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('p')
|
|
constitutive_nonlocal_p(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('q')
|
|
constitutive_nonlocal_q(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('viscosity','glideviscosity')
|
|
constitutive_nonlocal_viscosity(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('attackfrequency','fattack')
|
|
constitutive_nonlocal_fattack(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('rhosglscatter')
|
|
constitutive_nonlocal_rhoSglScatter(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('surfacetransmissivity')
|
|
constitutive_nonlocal_surfaceTransmissivity(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('grainboundarytransmissivity')
|
|
constitutive_nonlocal_grainboundaryTransmissivity(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('cflfactor')
|
|
constitutive_nonlocal_CFLfactor(i) = IO_floatValue(line,positions,2_pInt)
|
|
case('shortrangestresscorrection')
|
|
constitutive_nonlocal_shortRangeStressCorrection(i) = IO_floatValue(line,positions,2_pInt) > 0.0_pReal
|
|
case default
|
|
call IO_error(210_pInt,ext_msg=tag//' ('//constitutive_nonlocal_label//')')
|
|
end select
|
|
endif
|
|
enddo
|
|
|
|
|
|
100 do i = 1_pInt,maxNinstance
|
|
|
|
constitutive_nonlocal_structure(i) = &
|
|
lattice_initializeStructure(constitutive_nonlocal_structureName(i), constitutive_nonlocal_CoverA(i)) ! our lattice structure is defined in the material.config file by the structureName (and the c/a ratio)
|
|
myStructure = constitutive_nonlocal_structure(i)
|
|
|
|
|
|
!*** sanity checks
|
|
|
|
if (myStructure < 1_pInt) call IO_error(205_pInt,e=i)
|
|
if (sum(constitutive_nonlocal_Nslip(:,i)) <= 0_pInt) call IO_error(211_pInt,ext_msg='Nslip (' &
|
|
//constitutive_nonlocal_label//')')
|
|
do o = 1_pInt,maxval(phase_Noutput)
|
|
if(len(constitutive_nonlocal_output(o,i)) > 64_pInt) call IO_error(666_pInt)
|
|
enddo
|
|
do f = 1_pInt,lattice_maxNslipFamily
|
|
if (constitutive_nonlocal_Nslip(f,i) > 0_pInt) then
|
|
if (constitutive_nonlocal_rhoSglEdgePos0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoSglEdgePos0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoSglEdgeNeg0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoSglEdgeNeg0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoSglScrewPos0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoSglScrewPos0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoSglScrewNeg0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoSglScrewNeg0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoDipEdge0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoDipEdge0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoDipScrew0(f,i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoDipScrew0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_burgersPerSlipFamily(f,i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='Burgers (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_lambda0PerSlipFamily(f,i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='lambda0 (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(f,1,i) < 0.0_pReal) &
|
|
call IO_error(211_pInt,ext_msg='minimumDipoleHeightEdge (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(f,2,i) < 0.0_pReal) &
|
|
call IO_error(211_pInt,ext_msg='minimumDipoleHeightScrew (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_peierlsStressPerSlipFamily(f,1,i) <= 0.0_pReal) &
|
|
call IO_error(211_pInt,ext_msg='peierlsStressEdge (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_peierlsStressPerSlipFamily(f,2,i) <= 0.0_pReal) &
|
|
call IO_error(211_pInt,ext_msg='peierlsStressScrew (' &
|
|
//constitutive_nonlocal_label//')')
|
|
endif
|
|
enddo
|
|
if (any(constitutive_nonlocal_interactionSlipSlip(1:maxval(lattice_interactionSlipSlip(:,:,myStructure)),i) < 0.0_pReal)) &
|
|
call IO_error(211_pInt,ext_msg='interaction_SlipSlip (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_R(i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='r (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_atomicVolume(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='atomicVolume (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_Dsd0(i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='selfDiffusionPrefactor (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_Qsd(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='selfDiffusionEnergy (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_aTolRho(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='aTol_rho (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_doublekinkwidth(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='doublekinkwidth (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_solidSolutionEnergy(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='solidSolutionEnergy (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_solidSolutionSize(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='solidSolutionSize (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_solidSolutionConcentration(i) <= 0.0_pReal) &
|
|
call IO_error(211_pInt,ext_msg='solidSolutionConcentration (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_p(i) <= 0.0_pReal .or. constitutive_nonlocal_p(i) > 1.0_pReal) call IO_error(211_pInt,ext_msg='p (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_q(i) < 1.0_pReal .or. constitutive_nonlocal_q(i) > 2.0_pReal) call IO_error(211_pInt,ext_msg='q (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_viscosity(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='viscosity (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_fattack(i) <= 0.0_pReal) call IO_error(211_pInt,ext_msg='attackFrequency (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_rhoSglScatter(i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='rhoSglScatter (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_surfaceTransmissivity(i) < 0.0_pReal &
|
|
.or. constitutive_nonlocal_surfaceTransmissivity(i) > 1.0_pReal) call IO_error(211_pInt,ext_msg='surfaceTransmissivity (' &
|
|
//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_grainboundaryTransmissivity(i) > 1.0_pReal) call IO_error(211_pInt,&
|
|
ext_msg='grainboundaryTransmissivity ('//constitutive_nonlocal_label//')')
|
|
if (constitutive_nonlocal_CFLfactor(i) < 0.0_pReal) call IO_error(211_pInt,ext_msg='CFLfactor (' &
|
|
//constitutive_nonlocal_label//')')
|
|
|
|
|
|
!*** determine total number of active slip systems
|
|
|
|
constitutive_nonlocal_Nslip(1:lattice_maxNslipFamily,i) = min( lattice_NslipSystem(1:lattice_maxNslipFamily, myStructure), &
|
|
constitutive_nonlocal_Nslip(1:lattice_maxNslipFamily,i) ) ! we can't use more slip systems per family than specified in lattice
|
|
constitutive_nonlocal_totalNslip(i) = sum(constitutive_nonlocal_Nslip(1:lattice_maxNslipFamily,i))
|
|
|
|
enddo
|
|
|
|
|
|
!*** allocation of variables whose size depends on the total number of active slip systems
|
|
|
|
maxTotalNslip = maxval(constitutive_nonlocal_totalNslip)
|
|
|
|
allocate(constitutive_nonlocal_burgers(maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_burgers = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_lambda0(maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_lambda0 = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_minimumDipoleHeight(maxTotalNslip,2,maxNinstance))
|
|
constitutive_nonlocal_minimumDipoleHeight = -1.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_forestProjectionEdge(maxTotalNslip, maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_forestProjectionEdge = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_forestProjectionScrew(maxTotalNslip, maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_forestProjectionScrew = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_interactionMatrixSlipSlip(maxTotalNslip, maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_interactionMatrixSlipSlip = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_lattice2slip(1:3, 1:3, maxTotalNslip, maxNinstance))
|
|
constitutive_nonlocal_lattice2slip = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_accumulatedShear(maxTotalNslip, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
constitutive_nonlocal_accumulatedShear = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_rhoDotFlux(maxTotalNslip, 8, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
allocate(constitutive_nonlocal_rhoDotMultiplication(maxTotalNslip, 2, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
allocate(constitutive_nonlocal_rhoDotSingle2DipoleGlide(maxTotalNslip, 2, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
allocate(constitutive_nonlocal_rhoDotAthermalAnnihilation(maxTotalNslip, 2, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
allocate(constitutive_nonlocal_rhoDotThermalAnnihilation(maxTotalNslip, 2, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
allocate(constitutive_nonlocal_rhoDotEdgeJogs(maxTotalNslip, homogenization_maxNgrains, mesh_maxNips, mesh_NcpElems))
|
|
constitutive_nonlocal_rhoDotFlux = 0.0_pReal
|
|
constitutive_nonlocal_rhoDotMultiplication = 0.0_pReal
|
|
constitutive_nonlocal_rhoDotSingle2DipoleGlide = 0.0_pReal
|
|
constitutive_nonlocal_rhoDotAthermalAnnihilation = 0.0_pReal
|
|
constitutive_nonlocal_rhoDotThermalAnnihilation = 0.0_pReal
|
|
constitutive_nonlocal_rhoDotEdgeJogs = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_compatibility(2,maxTotalNslip, maxTotalNslip, FE_maxNipNeighbors, mesh_maxNips, mesh_NcpElems))
|
|
constitutive_nonlocal_compatibility = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_peierlsStress(maxTotalNslip,2,maxNinstance))
|
|
constitutive_nonlocal_peierlsStress = 0.0_pReal
|
|
|
|
allocate(constitutive_nonlocal_colinearSystem(maxTotalNslip,maxNinstance))
|
|
constitutive_nonlocal_colinearSystem = 0_pInt
|
|
|
|
do i = 1,maxNinstance
|
|
|
|
myStructure = constitutive_nonlocal_structure(i) ! lattice structure of this instance
|
|
|
|
|
|
!*** Inverse lookup of my slip system family and the slip system in lattice
|
|
|
|
l = 0_pInt
|
|
do f = 1_pInt,lattice_maxNslipFamily
|
|
do s = 1_pInt,constitutive_nonlocal_Nslip(f,i)
|
|
l = l + 1_pInt
|
|
constitutive_nonlocal_slipFamily(l,i) = f
|
|
constitutive_nonlocal_slipSystemLattice(l,i) = sum(lattice_NslipSystem(1:f-1_pInt, myStructure)) + s
|
|
enddo; enddo
|
|
|
|
|
|
!*** determine size of state array
|
|
|
|
ns = constitutive_nonlocal_totalNslip(i)
|
|
constitutive_nonlocal_sizeDotState(i) = int(size(constitutive_nonlocal_listBasicStates),pInt) * ns
|
|
constitutive_nonlocal_sizeDependentState(i) = int(size(constitutive_nonlocal_listDependentStates),pInt) * ns
|
|
constitutive_nonlocal_sizeState(i) = constitutive_nonlocal_sizeDotState(i) &
|
|
+ constitutive_nonlocal_sizeDependentState(i) &
|
|
+ int(size(constitutive_nonlocal_listOtherStates),pInt) * ns
|
|
|
|
|
|
!*** determine size of postResults array
|
|
|
|
do o = 1_pInt,constitutive_nonlocal_Noutput(i)
|
|
select case(constitutive_nonlocal_output(o,i))
|
|
case( 'rho', &
|
|
'delta', &
|
|
'rho_edge', &
|
|
'rho_screw', &
|
|
'rho_sgl', &
|
|
'delta_sgl', &
|
|
'rho_sgl_edge', &
|
|
'rho_sgl_edge_pos', &
|
|
'rho_sgl_edge_neg', &
|
|
'rho_sgl_screw', &
|
|
'rho_sgl_screw_pos', &
|
|
'rho_sgl_screw_neg', &
|
|
'rho_sgl_mobile', &
|
|
'rho_sgl_edge_mobile', &
|
|
'rho_sgl_edge_pos_mobile', &
|
|
'rho_sgl_edge_neg_mobile', &
|
|
'rho_sgl_screw_mobile', &
|
|
'rho_sgl_screw_pos_mobile', &
|
|
'rho_sgl_screw_neg_mobile', &
|
|
'rho_sgl_immobile', &
|
|
'rho_sgl_edge_immobile', &
|
|
'rho_sgl_edge_pos_immobile', &
|
|
'rho_sgl_edge_neg_immobile', &
|
|
'rho_sgl_screw_immobile', &
|
|
'rho_sgl_screw_pos_immobile', &
|
|
'rho_sgl_screw_neg_immobile', &
|
|
'rho_dip', &
|
|
'delta_dip', &
|
|
'rho_dip_edge', &
|
|
'rho_dip_screw', &
|
|
'excess_rho', &
|
|
'excess_rho_edge', &
|
|
'excess_rho_screw', &
|
|
'rho_forest', &
|
|
'shearrate', &
|
|
'resolvedstress', &
|
|
'resolvedstress_external', &
|
|
'resolvedstress_back', &
|
|
'resistance', &
|
|
'rho_dot', &
|
|
'rho_dot_sgl', &
|
|
'rho_dot_dip', &
|
|
'rho_dot_gen', &
|
|
'rho_dot_gen_edge', &
|
|
'rho_dot_gen_screw', &
|
|
'rho_dot_sgl2dip', &
|
|
'rho_dot_ann_ath', &
|
|
'rho_dot_ann_the', &
|
|
'rho_dot_flux', &
|
|
'rho_dot_flux_edge', &
|
|
'rho_dot_flux_screw', &
|
|
'velocity_edge_pos', &
|
|
'velocity_edge_neg', &
|
|
'velocity_screw_pos', &
|
|
'velocity_screw_neg', &
|
|
'fluxdensity_edge_pos_x', &
|
|
'fluxdensity_edge_pos_y', &
|
|
'fluxdensity_edge_pos_z', &
|
|
'fluxdensity_edge_neg_x', &
|
|
'fluxdensity_edge_neg_y', &
|
|
'fluxdensity_edge_neg_z', &
|
|
'fluxdensity_screw_pos_x', &
|
|
'fluxdensity_screw_pos_y', &
|
|
'fluxdensity_screw_pos_z', &
|
|
'fluxdensity_screw_neg_x', &
|
|
'fluxdensity_screw_neg_y', &
|
|
'fluxdensity_screw_neg_z', &
|
|
'maximumdipoleheight_edge', &
|
|
'maximumdipoleheight_screw', &
|
|
'accumulatedshear' )
|
|
mySize = constitutive_nonlocal_totalNslip(i)
|
|
case('dislocationstress')
|
|
mySize = 6_pInt
|
|
case default
|
|
call IO_error(212_pInt,ext_msg=constitutive_nonlocal_output(o,i)//' ('//constitutive_nonlocal_label//')')
|
|
end select
|
|
|
|
if (mySize > 0_pInt) then ! any meaningful output found
|
|
constitutive_nonlocal_sizePostResult(o,i) = mySize
|
|
constitutive_nonlocal_sizePostResults(i) = constitutive_nonlocal_sizePostResults(i) + mySize
|
|
endif
|
|
enddo
|
|
|
|
|
|
!*** elasticity matrix and shear modulus according to material.config
|
|
|
|
select case (myStructure)
|
|
case(1_pInt:2_pInt) ! cubic(s)
|
|
forall(k=1_pInt:3_pInt)
|
|
forall(j=1_pInt:3_pInt) constitutive_nonlocal_Cslip_66(k,j,i) = constitutive_nonlocal_C12(i)
|
|
constitutive_nonlocal_Cslip_66(k,k,i) = constitutive_nonlocal_C11(i)
|
|
constitutive_nonlocal_Cslip_66(k+3_pInt,k+3_pInt,i) = constitutive_nonlocal_C44(i)
|
|
end forall
|
|
case(3_pInt:) ! all hex
|
|
constitutive_nonlocal_Cslip_66(1,1,i) = constitutive_nonlocal_C11(i)
|
|
constitutive_nonlocal_Cslip_66(2,2,i) = constitutive_nonlocal_C11(i)
|
|
constitutive_nonlocal_Cslip_66(3,3,i) = constitutive_nonlocal_C33(i)
|
|
constitutive_nonlocal_Cslip_66(1,2,i) = constitutive_nonlocal_C12(i)
|
|
constitutive_nonlocal_Cslip_66(2,1,i) = constitutive_nonlocal_C12(i)
|
|
constitutive_nonlocal_Cslip_66(1,3,i) = constitutive_nonlocal_C13(i)
|
|
constitutive_nonlocal_Cslip_66(3,1,i) = constitutive_nonlocal_C13(i)
|
|
constitutive_nonlocal_Cslip_66(2,3,i) = constitutive_nonlocal_C13(i)
|
|
constitutive_nonlocal_Cslip_66(3,2,i) = constitutive_nonlocal_C13(i)
|
|
constitutive_nonlocal_Cslip_66(4,4,i) = constitutive_nonlocal_C44(i)
|
|
constitutive_nonlocal_Cslip_66(5,5,i) = constitutive_nonlocal_C44(i)
|
|
constitutive_nonlocal_Cslip_66(6,6,i) = 0.5_pReal*(constitutive_nonlocal_C11(i)- constitutive_nonlocal_C12(i))
|
|
end select
|
|
constitutive_nonlocal_Cslip_66(1:6,1:6,i) = math_Mandel3333to66(math_Voigt66to3333(constitutive_nonlocal_Cslip_66(1:6,1:6,i)))
|
|
constitutive_nonlocal_Cslip_3333(1:3,1:3,1:3,1:3,i) = math_Voigt66to3333(constitutive_nonlocal_Cslip_66(1:6,1:6,i))
|
|
|
|
constitutive_nonlocal_Gmod(i) = 0.2_pReal * ( constitutive_nonlocal_C11(i) - constitutive_nonlocal_C12(i) &
|
|
+ 3.0_pReal*constitutive_nonlocal_C44(i) ) ! (C11iso-C12iso)/2 with C11iso=(3*C11+2*C12+4*C44)/5 and C12iso=(C11+4*C12-2*C44)/5
|
|
constitutive_nonlocal_nu(i) = ( constitutive_nonlocal_C11(i) + 4.0_pReal*constitutive_nonlocal_C12(i) &
|
|
- 2.0_pReal*constitutive_nonlocal_C44(i) ) &
|
|
/ ( 4.0_pReal*constitutive_nonlocal_C11(i) + 6.0_pReal*constitutive_nonlocal_C12(i) &
|
|
+ 2.0_pReal*constitutive_nonlocal_C44(i) ) ! C12iso/(C11iso+C12iso) with C11iso=(3*C11+2*C12+4*C44)/5 and C12iso=(C11+4*C12-2*C44)/5
|
|
|
|
do s1 = 1_pInt,ns
|
|
f = constitutive_nonlocal_slipFamily(s1,i)
|
|
|
|
!*** burgers vector, mean free path prefactor and minimum dipole distance for each slip system
|
|
|
|
constitutive_nonlocal_burgers(s1,i) = constitutive_nonlocal_burgersPerSlipFamily(f,i)
|
|
constitutive_nonlocal_lambda0(s1,i) = constitutive_nonlocal_lambda0PerSlipFamily(f,i)
|
|
constitutive_nonlocal_minimumDipoleHeight(s1,1:2,i) = constitutive_nonlocal_minimumDipoleHeightPerSlipFamily(f,1:2,i)
|
|
constitutive_nonlocal_peierlsStress(s1,1:2,i) = constitutive_nonlocal_peierlsStressPerSlipFamily(f,1:2,i)
|
|
|
|
do s2 = 1_pInt,ns
|
|
|
|
!*** calculation of forest projections for edge and screw dislocations. s2 acts as forest for s1
|
|
|
|
constitutive_nonlocal_forestProjectionEdge(s1,s2,i) &
|
|
= abs(math_mul3x3(lattice_sn(1:3,constitutive_nonlocal_slipSystemLattice(s1,i),myStructure), &
|
|
lattice_st(1:3,constitutive_nonlocal_slipSystemLattice(s2,i),myStructure))) ! forest projection of edge dislocations is the projection of (t = b x n) onto the slip normal of the respective slip plane
|
|
|
|
constitutive_nonlocal_forestProjectionScrew(s1,s2,i) &
|
|
= abs(math_mul3x3(lattice_sn(1:3,constitutive_nonlocal_slipSystemLattice(s1,i),myStructure), &
|
|
lattice_sd(1:3,constitutive_nonlocal_slipSystemLattice(s2,i),myStructure))) ! forest projection of screw dislocations is the projection of b onto the slip normal of the respective splip plane
|
|
|
|
!*** calculation of interaction matrices
|
|
|
|
constitutive_nonlocal_interactionMatrixSlipSlip(s1,s2,i) &
|
|
= constitutive_nonlocal_interactionSlipSlip(lattice_interactionSlipSlip(constitutive_nonlocal_slipSystemLattice(s1,i), &
|
|
constitutive_nonlocal_slipSystemLattice(s2,i), &
|
|
myStructure), i)
|
|
|
|
!*** colinear slip system (only makes sense for fcc like it is defined here)
|
|
|
|
if (lattice_interactionSlipSlip(constitutive_nonlocal_slipSystemLattice(s1,i), &
|
|
constitutive_nonlocal_slipSystemLattice(s2,i), &
|
|
myStructure) == 3_pInt) then
|
|
constitutive_nonlocal_colinearSystem(s1,i) = s2
|
|
endif
|
|
|
|
enddo
|
|
|
|
!*** rotation matrix from lattice configuration to slip system
|
|
|
|
constitutive_nonlocal_lattice2slip(1:3,1:3,s1,i) &
|
|
= math_transpose33( reshape([ lattice_sd(1:3, constitutive_nonlocal_slipSystemLattice(s1,i), myStructure), &
|
|
-lattice_st(1:3, constitutive_nonlocal_slipSystemLattice(s1,i), myStructure), &
|
|
lattice_sn(1:3, constitutive_nonlocal_slipSystemLattice(s1,i), myStructure)], [3,3]))
|
|
enddo
|
|
|
|
enddo
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* initial microstructural state (just the "basic" states) *
|
|
!*********************************************************************
|
|
function constitutive_nonlocal_stateInit(myInstance)
|
|
|
|
use prec, only: pReal, &
|
|
pInt
|
|
use lattice, only: lattice_maxNslipFamily
|
|
use math, only: math_sampleGaussVar
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: myInstance ! number specifying the current instance of the plasticity
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(constitutive_nonlocal_sizeState(myInstance)) :: &
|
|
constitutive_nonlocal_stateInit
|
|
|
|
!*** local variables
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(myInstance)) :: &
|
|
rhoSglEdgePos, & ! positive edge dislocation density
|
|
rhoSglEdgeNeg, & ! negative edge dislocation density
|
|
rhoSglScrewPos, & ! positive screw dislocation density
|
|
rhoSglScrewNeg, & ! negative screw dislocation density
|
|
rhoSglEdgePosUsed, & ! used positive edge dislocation density
|
|
rhoSglEdgeNegUsed, & ! used negative edge dislocation density
|
|
rhoSglScrewPosUsed, & ! used positive screw dislocation density
|
|
rhoSglScrewNegUsed, & ! used negative screw dislocation density
|
|
rhoDipEdge, & ! edge dipole dislocation density
|
|
rhoDipScrew ! screw dipole dislocation density
|
|
integer(pInt) ns, & ! short notation for total number of active slip systems
|
|
f, & ! index of lattice family
|
|
from, &
|
|
upto, &
|
|
s, & ! index of slip system
|
|
i
|
|
real(pReal), dimension(2) :: noise
|
|
|
|
constitutive_nonlocal_stateInit = 0.0_pReal
|
|
ns = constitutive_nonlocal_totalNslip(myInstance)
|
|
|
|
!*** set the basic state variables
|
|
|
|
do f = 1_pInt,lattice_maxNslipFamily
|
|
from = 1_pInt + sum(constitutive_nonlocal_Nslip(1:f-1_pInt,myInstance))
|
|
upto = sum(constitutive_nonlocal_Nslip(1:f,myInstance))
|
|
do s = from,upto
|
|
do i = 1_pInt,2_pInt
|
|
noise(i) = math_sampleGaussVar(0.0_pReal, constitutive_nonlocal_rhoSglScatter(myInstance))
|
|
enddo
|
|
rhoSglEdgePos(s) = constitutive_nonlocal_rhoSglEdgePos0(f, myInstance) + noise(1)
|
|
rhoSglEdgeNeg(s) = constitutive_nonlocal_rhoSglEdgeNeg0(f, myInstance) + noise(1)
|
|
rhoSglScrewPos(s) = constitutive_nonlocal_rhoSglScrewPos0(f, myInstance) + noise(2)
|
|
rhoSglScrewNeg(s) = constitutive_nonlocal_rhoSglScrewNeg0(f, myInstance) + noise(2)
|
|
enddo
|
|
rhoSglEdgePosUsed(from:upto) = 0.0_pReal
|
|
rhoSglEdgeNegUsed(from:upto) = 0.0_pReal
|
|
rhoSglScrewPosUsed(from:upto) = 0.0_pReal
|
|
rhoSglScrewNegUsed(from:upto) = 0.0_pReal
|
|
rhoDipEdge(from:upto) = constitutive_nonlocal_rhoDipEdge0(f, myInstance)
|
|
rhoDipScrew(from:upto) = constitutive_nonlocal_rhoDipScrew0(f, myInstance)
|
|
enddo
|
|
|
|
|
|
!*** put everything together and in right order
|
|
|
|
constitutive_nonlocal_stateInit( 1: ns) = rhoSglEdgePos
|
|
constitutive_nonlocal_stateInit( ns+1: 2*ns) = rhoSglEdgeNeg
|
|
constitutive_nonlocal_stateInit( 2*ns+1: 3*ns) = rhoSglScrewPos
|
|
constitutive_nonlocal_stateInit( 3*ns+1: 4*ns) = rhoSglScrewNeg
|
|
constitutive_nonlocal_stateInit( 4*ns+1: 5*ns) = rhoSglEdgePosUsed
|
|
constitutive_nonlocal_stateInit( 5*ns+1: 6*ns) = rhoSglEdgeNegUsed
|
|
constitutive_nonlocal_stateInit( 6*ns+1: 7*ns) = rhoSglScrewPosUsed
|
|
constitutive_nonlocal_stateInit( 7*ns+1: 8*ns) = rhoSglScrewNegUsed
|
|
constitutive_nonlocal_stateInit( 8*ns+1: 9*ns) = rhoDipEdge
|
|
constitutive_nonlocal_stateInit( 9*ns+1:10*ns) = rhoDipScrew
|
|
|
|
endfunction
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* absolute state tolerance *
|
|
!*********************************************************************
|
|
pure function constitutive_nonlocal_aTolState(myInstance)
|
|
|
|
use prec, only: pReal, &
|
|
pInt
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: myInstance ! number specifying the current instance of the plasticity
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(constitutive_nonlocal_sizeState(myInstance)) :: &
|
|
constitutive_nonlocal_aTolState ! absolute state tolerance for the current instance of this plasticity
|
|
|
|
!*** local variables
|
|
|
|
constitutive_nonlocal_aTolState = constitutive_nonlocal_aTolRho(myInstance)
|
|
|
|
endfunction
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* calculates homogenized elacticity matrix *
|
|
!*********************************************************************
|
|
pure function constitutive_nonlocal_homogenizedC(state,g,ip,el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_plasticityInstance
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain ID
|
|
ip, & ! current integration point
|
|
el ! current element
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: state ! microstructural state
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(6,6) :: constitutive_nonlocal_homogenizedC ! homogenized elasticity matrix
|
|
|
|
!*** local variables
|
|
integer(pInt) myInstance ! current instance of this plasticity
|
|
|
|
myInstance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
|
|
constitutive_nonlocal_homogenizedC = constitutive_nonlocal_Cslip_66(1:6,1:6,myInstance)
|
|
|
|
endfunction
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* calculates quantities characterizing the microstructure *
|
|
!*********************************************************************
|
|
subroutine constitutive_nonlocal_microstructure(state, Temperature, Fe, Fp, g, ip, el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use IO, only: IO_error
|
|
use math, only: math_Mandel33to6, &
|
|
math_mul33x33, &
|
|
math_mul33x3, &
|
|
math_mul3x3, &
|
|
math_norm3, &
|
|
math_inv33, &
|
|
math_invert33, &
|
|
math_transpose33, &
|
|
pi
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic, &
|
|
debug_levelSelective, &
|
|
debug_g, &
|
|
debug_i, &
|
|
debug_e
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips, &
|
|
mesh_element, &
|
|
FE_NipNeighbors, &
|
|
FE_maxNipNeighbors, &
|
|
mesh_ipNeighborhood, &
|
|
mesh_ipCenterOfGravity, &
|
|
mesh_ipVolume, &
|
|
mesh_ipAreaNormal
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_localPlasticity, &
|
|
phase_plasticityInstance
|
|
use lattice, only: lattice_sd, &
|
|
lattice_st
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain ID
|
|
ip, & ! current integration point
|
|
el ! current element
|
|
real(pReal), intent(in) :: Temperature ! temperature
|
|
real(pReal), dimension(3,3), intent(in) :: &
|
|
Fe, & ! elastic deformation gradient
|
|
Fp ! elastic deformation gradient
|
|
|
|
!*** input/output variables
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(inout) :: &
|
|
state ! microstructural state
|
|
|
|
!*** output variables
|
|
|
|
!*** local variables
|
|
integer(pInt) neighboring_el, & ! element number of neighboring material point
|
|
neighboring_ip, & ! integration point of neighboring material point
|
|
instance, & ! my instance of this plasticity
|
|
neighboring_instance, & ! instance of this plasticity of neighboring material point
|
|
latticeStruct, & ! my lattice structure
|
|
neighboring_latticeStruct, & ! lattice structure of neighboring material point
|
|
phase, &
|
|
neighboring_phase, &
|
|
ns, & ! total number of active slip systems at my material point
|
|
neighboring_ns, & ! total number of active slip systems at neighboring material point
|
|
c, & ! index of dilsocation character (edge, screw)
|
|
s, & ! slip system index
|
|
t, & ! index of dilsocation type (e+, e-, s+, s-, used e+, used e-, used s+, used s-)
|
|
dir, &
|
|
n
|
|
integer(pInt), dimension(2) :: neighbor
|
|
real(pReal) nu, & ! poisson's ratio
|
|
mu, &
|
|
b, &
|
|
detFe, &
|
|
detFp, &
|
|
FVsize, &
|
|
temp
|
|
real(pReal), dimension(2) :: rhoExcessGradient, &
|
|
rhoExcessGradient_over_rho, &
|
|
rhoTotal
|
|
real(pReal), dimension(3) :: ipCoords, &
|
|
neighboring_ipCoords, &
|
|
rhoExcessDifferences
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
rhoForest, & ! forest dislocation density
|
|
tauBack, & ! back stress from pileup on same slip system
|
|
tauThreshold ! threshold shear stress
|
|
real(pReal), dimension(3,3) :: invFe, & ! inverse of elastic deformation gradient
|
|
invFp, & ! inverse of plastic deformation gradient
|
|
connections, &
|
|
invConnections
|
|
real(pReal), dimension(3,FE_maxNipNeighbors) :: &
|
|
connection_latticeConf
|
|
real(pReal), dimension(2,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
rhoExcess
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
rhoDip ! dipole dislocation density (edge, screw)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),8) :: &
|
|
rhoSgl ! single dislocation density (edge+, edge-, screw+, screw-, used edge+, used edge-, used screw+, used screw-)
|
|
real(pReal), dimension(2,maxval(constitutive_nonlocal_totalNslip),FE_maxNipNeighbors) :: &
|
|
neighboring_rhoExcess ! excess density at neighboring material point
|
|
real(pReal), dimension(3,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
m ! direction of dislocation motion
|
|
logical inversionError
|
|
|
|
|
|
phase = material_phase(g,ip,el)
|
|
instance = phase_plasticityInstance(phase)
|
|
latticeStruct = constitutive_nonlocal_structure(instance)
|
|
ns = constitutive_nonlocal_totalNslip(instance)
|
|
|
|
|
|
|
|
!*** get basic states
|
|
|
|
forall (s = 1_pInt:ns, t = 1_pInt:4_pInt) &
|
|
rhoSgl(s,t) = max(state(g,ip,el)%p((t-1_pInt)*ns+s), 0.0_pReal) ! ensure positive single mobile densities
|
|
forall (t = 5_pInt:8_pInt) &
|
|
rhoSgl(1:ns,t) = state(g,ip,el)%p((t-1_pInt)*ns+1_pInt:t*ns)
|
|
forall (s = 1_pInt:ns, c = 1_pInt:2_pInt) &
|
|
rhoDip(s,c) = max(state(g,ip,el)%p((7_pInt+c)*ns+s), 0.0_pReal) ! ensure positive dipole densities
|
|
|
|
|
|
|
|
!*** calculate the forest dislocation density
|
|
!*** (= projection of screw and edge dislocations)
|
|
|
|
forall (s = 1_pInt:ns) &
|
|
rhoForest(s) = dot_product((sum(abs(rhoSgl(1:ns,[1,2,5,6])),2) + rhoDip(1:ns,1)), &
|
|
constitutive_nonlocal_forestProjectionEdge(s,1:ns,instance)) &
|
|
+ dot_product((sum(abs(rhoSgl(1:ns,[3,4,7,8])),2) + rhoDip(1:ns,2)), &
|
|
constitutive_nonlocal_forestProjectionScrew(s,1:ns,instance))
|
|
|
|
|
|
|
|
!*** calculate the threshold shear stress for dislocation slip
|
|
|
|
forall (s = 1_pInt:ns) &
|
|
tauThreshold(s) = constitutive_nonlocal_Gmod(instance) * constitutive_nonlocal_burgers(s,instance) &
|
|
* sqrt(dot_product((sum(abs(rhoSgl),2) + sum(abs(rhoDip),2)), &
|
|
constitutive_nonlocal_interactionMatrixSlipSlip(s,1:ns,instance)))
|
|
|
|
|
|
|
|
!*** calculate the dislocation stress of the neighboring excess dislocation densities
|
|
!*** zero for material points of local plasticity
|
|
|
|
tauBack = 0.0_pReal
|
|
|
|
if (.not. phase_localPlasticity(phase) .and. constitutive_nonlocal_shortRangeStressCorrection(instance)) then
|
|
call math_invert33(Fe, invFe, detFe, inversionError)
|
|
call math_invert33(Fp, invFp, detFp, inversionError)
|
|
ipCoords = mesh_ipCenterOfGravity(1:3,ip,el)
|
|
rhoExcess(1,1:ns) = rhoSgl(1:ns,1) - rhoSgl(1:ns,2)
|
|
rhoExcess(2,1:ns) = rhoSgl(1:ns,3) - rhoSgl(1:ns,4)
|
|
FVsize = mesh_ipVolume(ip,el) ** (1.0_pReal/3.0_pReal)
|
|
nu = constitutive_nonlocal_nu(instance)
|
|
mu = constitutive_nonlocal_Gmod(instance)
|
|
|
|
!* loop through my neighborhood and get the connection vectors (in lattice frame) and the excess densities
|
|
|
|
do n = 1_pInt,FE_NipNeighbors(mesh_element(2,el))
|
|
neighboring_el = mesh_ipNeighborhood(1,n,ip,el)
|
|
neighboring_ip = mesh_ipNeighborhood(2,n,ip,el)
|
|
if (neighboring_el > 0 .and. neighboring_ip > 0) then
|
|
neighboring_phase = material_phase(g,neighboring_ip,neighboring_el)
|
|
neighboring_instance = phase_plasticityInstance(neighboring_phase)
|
|
neighboring_latticeStruct = constitutive_nonlocal_structure(neighboring_instance)
|
|
neighboring_ns = constitutive_nonlocal_totalNslip(neighboring_instance)
|
|
neighboring_ipCoords = mesh_ipCenterOfGravity(1:3,neighboring_ip,neighboring_el)
|
|
if (.not. phase_localPlasticity(neighboring_phase) &
|
|
.and. neighboring_latticeStruct == latticeStruct &
|
|
.and. neighboring_instance == instance) then
|
|
if (neighboring_ns == ns) then
|
|
if (neighboring_el /= el .or. neighboring_ip /= ip) then
|
|
connection_latticeConf(1:3,n) = math_mul33x3(invFe, neighboring_ipCoords - ipCoords)
|
|
forall (s = 1_pInt:ns, c = 1_pInt:2_pInt) &
|
|
neighboring_rhoExcess(c,s,n) = state(g,neighboring_ip,neighboring_el)%p((2_pInt*c-2_pInt)*ns+s) & ! positive mobiles
|
|
- state(g,neighboring_ip,neighboring_el)%p((2_pInt*c-1_pInt)*ns+s) ! negative mobiles
|
|
else
|
|
! thats myself! probably using periodic images -> assume constant excess density
|
|
connection_latticeConf(1:3,n) = math_mul33x3(math_transpose33(invFp), mesh_ipAreaNormal(1:3,n,ip,el)) ! direction of area normal
|
|
neighboring_rhoExcess(1:2,1:ns,n) = rhoExcess
|
|
endif
|
|
else
|
|
! different number of active slip systems
|
|
call IO_error(-1_pInt,ext_msg='different number of active slip systems in neighboring IPs of same crystal structure')
|
|
endif
|
|
else
|
|
! local neighbor or different lattice structure or different constitution instance -> use central values instead
|
|
connection_latticeConf(1:3,n) = 0.0_pReal
|
|
neighboring_rhoExcess(1:2,1:ns,n) = rhoExcess
|
|
endif
|
|
else
|
|
! free surface -> use central values instead
|
|
connection_latticeConf(1:3,n) = 0.0_pReal
|
|
neighboring_rhoExcess(1:2,1:ns,n) = rhoExcess
|
|
endif
|
|
enddo
|
|
|
|
|
|
!* loop through the slip systems and calculate the dislocation gradient by
|
|
!* 1. interpolation of the excess density in the neighorhood
|
|
!* 2. interpolation of the dead dislocation density in the central volume
|
|
|
|
m(1:3,1:ns,1) = lattice_sd(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,instance), latticeStruct)
|
|
m(1:3,1:ns,2) = -lattice_st(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,instance), latticeStruct)
|
|
|
|
do s = 1_pInt,ns
|
|
|
|
!* gradient from interpolation of neighboring excess density
|
|
|
|
do c = 1_pInt,2_pInt
|
|
do dir = 1_pInt,3_pInt
|
|
neighbor(1) = 2_pInt * dir - 1_pInt
|
|
neighbor(2) = 2_pInt * dir
|
|
connections(dir,1:3) = connection_latticeConf(1:3,neighbor(1)) - connection_latticeConf(1:3,neighbor(2))
|
|
rhoExcessDifferences(dir) = neighboring_rhoExcess(c,s,neighbor(1)) - neighboring_rhoExcess(c,s,neighbor(2))
|
|
enddo
|
|
call math_invert33(connections,invConnections,temp,inversionError)
|
|
if (inversionError) then
|
|
call IO_error(-1_pInt,ext_msg='back stress calculation: inversion error')
|
|
endif
|
|
rhoExcessGradient(c) = math_mul3x3(math_mul33x3(invConnections, rhoExcessDifferences), m(1:3,s,c))
|
|
enddo
|
|
|
|
!* plus gradient from deads
|
|
|
|
do t = 1_pInt,4_pInt
|
|
c = (t - 1_pInt) / 2_pInt + 1_pInt
|
|
rhoExcessGradient(c) = rhoExcessGradient(c) + rhoSgl(s,t+4_pInt) / FVsize
|
|
enddo
|
|
|
|
!* normalized with the total density
|
|
|
|
rhoExcessGradient_over_rho = 0.0_pReal
|
|
rhoTotal(1_pInt) = sum(abs(rhoSgl(s,[1_pInt,2_pInt,5_pInt,6_pInt]))) + rhoDip(s,1_pInt)
|
|
rhoTotal(2_pInt) = sum(abs(rhoSgl(s,[3_pInt,4_pInt,7_pInt,8_pInt]))) + rhoDip(s,2_pInt)
|
|
forall (c = 1_pInt:2_pInt, rhoTotal(c) > 0.0_pReal) &
|
|
rhoExcessGradient_over_rho(c) = rhoExcessGradient(c) / rhoTotal(c)
|
|
|
|
!* gives the local stress correction when multiplied with a factor
|
|
|
|
b = constitutive_nonlocal_burgers(s,instance)
|
|
tauBack(s) = - mu * b / (2.0_pReal * pi) * (rhoExcessGradient_over_rho(1) / (1.0_pReal - nu) + rhoExcessGradient_over_rho(2))
|
|
|
|
enddo
|
|
endif
|
|
|
|
|
|
!*** set dependent states
|
|
|
|
state(g,ip,el)%p(10_pInt*ns+1:11_pInt*ns) = rhoForest
|
|
state(g,ip,el)%p(11_pInt*ns+1:12_pInt*ns) = tauThreshold
|
|
state(g,ip,el)%p(12_pInt*ns+1:13_pInt*ns) = tauBack
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt)) then
|
|
write(6,*)
|
|
write(6,'(a,i8,1x,i2,1x,i1)') '<< CONST >> nonlocal_microstructure at el ip g',el,ip,g
|
|
write(6,*)
|
|
write(6,'(a,/,12x,12(e10.3,1x))') '<< CONST >> rhoForest', rhoForest
|
|
write(6,'(a,/,12x,12(f10.5,1x))') '<< CONST >> tauThreshold / MPa', tauThreshold/1e6
|
|
write(6,'(a,/,12x,12(f10.5,1x))') '<< CONST >> tauBack / MPa', tauBack/1e6
|
|
endif
|
|
#endif
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* calculates kinetics *
|
|
!*********************************************************************
|
|
subroutine constitutive_nonlocal_kinetics(v, tau, c, Temperature, state, g, ip, el, dv_dtau)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic, &
|
|
debug_levelSelective, &
|
|
debug_g, &
|
|
debug_i, &
|
|
debug_e
|
|
use material, only: material_phase, &
|
|
phase_plasticityInstance
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain number
|
|
ip, & ! current integration point
|
|
el, & ! current element number
|
|
c ! dislocation character (1:edge, 2:screw)
|
|
real(pReal), intent(in) :: Temperature ! temperature
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))), &
|
|
intent(in) :: tau ! resolved external shear stress (for bcc this already contains non Schmid effects)
|
|
type(p_vec), intent(in) :: state ! microstructural state
|
|
|
|
!*** input/output variables
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))), &
|
|
intent(out) :: v ! velocity
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))), &
|
|
intent(out), optional :: dv_dtau ! velocity derivative with respect to resolved shear stress
|
|
|
|
!*** local variables
|
|
integer(pInt) instance, & ! current instance of this plasticity
|
|
ns, & ! short notation for the total number of active slip systems
|
|
s ! index of my current slip system
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
tauThreshold, & ! threshold shear stress
|
|
tauEff ! effective shear stress
|
|
real(pReal) tauRel_P, &
|
|
tauRel_S, &
|
|
tPeierls, & ! waiting time in front of a peierls barriers
|
|
tSolidSolution, & ! waiting time in front of a solid solution obstacle
|
|
vViscous, & ! viscous glide velocity
|
|
dtPeierls_dtau, & ! derivative with respect to resolved shear stress
|
|
dtSolidSolution_dtau, & ! derivative with respect to resolved shear stress
|
|
p, & ! shortcut to Kocks,Argon,Ashby parameter p
|
|
q, & ! shortcut to Kocks,Argon,Ashby parameter q
|
|
meanfreepath_S, & ! mean free travel distance for dislocations between two solid solution obstacles
|
|
meanfreepath_P, & ! mean free travel distance for dislocations between two Peierls barriers
|
|
jumpWidth_P, & ! depth of activated area
|
|
jumpWidth_S, & ! depth of activated area
|
|
activationLength_P, & ! length of activated dislocation line
|
|
activationLength_S, & ! length of activated dislocation line
|
|
activationVolume_P, & ! volume that needs to be activated to overcome barrier
|
|
activationVolume_S, & ! volume that needs to be activated to overcome barrier
|
|
activationEnergy_P, & ! energy that is needed to overcome barrier
|
|
activationEnergy_S, & ! energy that is needed to overcome barrier
|
|
criticalStress_P, & ! maximum obstacle strength
|
|
criticalStress_S, & ! maximum obstacle strength
|
|
mobility ! dislocation mobility
|
|
|
|
|
|
instance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
ns = constitutive_nonlocal_totalNslip(instance)
|
|
|
|
tauThreshold = state%p(11_pInt*ns+1:12_pInt*ns)
|
|
tauEff = abs(tau) - tauThreshold
|
|
|
|
p = constitutive_nonlocal_p(instance)
|
|
q = constitutive_nonlocal_q(instance)
|
|
|
|
v = 0.0_pReal
|
|
if (present(dv_dtau)) dv_dtau = 0.0_pReal
|
|
|
|
|
|
if (Temperature > 0.0_pReal) then
|
|
do s = 1_pInt,ns
|
|
if (tauEff(s) > 0.0_pReal) then
|
|
|
|
!* Peierls contribution
|
|
!* The derivative only gives absolute values; the correct sign is taken care of in the formula for the derivative of the velocity
|
|
|
|
meanfreepath_P = constitutive_nonlocal_burgers(s,instance)
|
|
jumpWidth_P = constitutive_nonlocal_burgers(s,instance)
|
|
activationLength_P = constitutive_nonlocal_doublekinkwidth(instance) * constitutive_nonlocal_burgers(s,instance)
|
|
activationVolume_P = activationLength_P * jumpWidth_P * constitutive_nonlocal_burgers(s,instance)
|
|
criticalStress_P = constitutive_nonlocal_peierlsStress(s,c,instance)
|
|
activationEnergy_P = criticalStress_P * activationVolume_P
|
|
tauRel_P = tauEff(s) / criticalStress_P
|
|
tPeierls = 1.0_pReal / constitutive_nonlocal_fattack(instance) &
|
|
* exp(activationEnergy_P / (kB * Temperature) * (1.0_pReal - tauRel_P**p)**q)
|
|
if (present(dv_dtau)) then
|
|
dtPeierls_dtau = tPeierls * p * q * activationVolume_P / (kB * Temperature) &
|
|
* (1.0_pReal - tauRel_P**p)**(q-1.0_pReal) * tauRel_P**(p-1.0_pReal)
|
|
endif
|
|
|
|
|
|
!* Contribution from solid solution strengthening
|
|
!* The derivative only gives absolute values; the correct sign is taken care of in the formula for the derivative of the velocity
|
|
|
|
meanfreepath_S = constitutive_nonlocal_burgers(s,instance) / sqrt(constitutive_nonlocal_solidSolutionConcentration(instance))
|
|
jumpWidth_S = constitutive_nonlocal_solidSolutionSize(instance) * constitutive_nonlocal_burgers(s,instance)
|
|
activationLength_S = constitutive_nonlocal_burgers(s,instance) &
|
|
/ sqrt(constitutive_nonlocal_solidSolutionConcentration(instance))
|
|
activationVolume_S = activationLength_S * jumpWidth_S * constitutive_nonlocal_burgers(s,instance)
|
|
activationEnergy_S = constitutive_nonlocal_solidSolutionEnergy(instance)
|
|
criticalStress_S = activationEnergy_S / activationVolume_S
|
|
tauRel_S = tauEff(s) / criticalStress_S
|
|
tSolidSolution = 1.0_pReal / constitutive_nonlocal_fattack(instance) &
|
|
* exp(activationEnergy_S / (kB * Temperature) * (1.0_pReal - tauRel_S**p)**q)
|
|
if (present(dv_dtau)) then
|
|
dtSolidSolution_dtau = tSolidSolution * p * q * activationVolume_S / (kB * Temperature) &
|
|
* (1.0_pReal - tauRel_S**p)**(q-1.0_pReal) * tauRel_S**(p-1.0_pReal)
|
|
endif
|
|
|
|
|
|
!* viscous glide velocity
|
|
|
|
mobility = constitutive_nonlocal_burgers(s,instance) / constitutive_nonlocal_viscosity(instance)
|
|
vViscous = mobility * tauEff(s)
|
|
|
|
|
|
!* Mean velocity results from waiting time at peierls barriers and solid solution obstacles with respective meanfreepath of
|
|
!* free flight at glide velocity in between. Backward jumps at low stresses are considered only at peierls barriers,
|
|
!* since those have the smallest activation volume, thus are decisive.
|
|
|
|
v(s) = 1.0_pReal / (tPeierls / meanfreepath_P + tSolidSolution / meanfreepath_S + 1.0_pReal / vViscous) &
|
|
* (1.0_pReal - exp(-tauEff(s) * activationVolume_P / (kB * Temperature)))
|
|
v(s) = sign(v(s),tau(s))
|
|
if (present(dv_dtau)) then
|
|
dv_dtau(s) = 1.0_pReal / (tPeierls / meanfreepath_P + tSolidSolution / meanfreepath_S + 1.0_pReal / vViscous) &
|
|
* (abs(v(s)) * (dtPeierls_dtau + dtSolidSolution_dtau + 1.0_pReal / (mobility * tauEff(s)*tauEff(s))) &
|
|
+ activationVolume_P / (kB * Temperature) * exp(-tauEff(s) * activationVolume_P / (kB * Temperature)))
|
|
endif
|
|
|
|
endif
|
|
enddo
|
|
endif
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt)) then
|
|
write(6,*)
|
|
write(6,'(a,i8,1x,i2,1x,i1)') '<< CONST >> nonlocal_kinetics at el ip g',el,ip,g
|
|
write(6,*)
|
|
write(6,'(a,/,12x,12(f12.5,1x))') '<< CONST >> tau / MPa', tau / 1e6_pReal
|
|
write(6,'(a,/,12x,12(f12.5,1x))') '<< CONST >> tauEff / MPa', tauEff / 1e6_pReal
|
|
write(6,'(a,/,12x,12(f12.5,1x))') '<< CONST >> v / 1e-3m/s', v * 1e3
|
|
endif
|
|
#endif
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* calculates plastic velocity gradient and its tangent *
|
|
!*********************************************************************
|
|
subroutine constitutive_nonlocal_LpAndItsTangent(Lp, dLp_dTstar99, Tstar_v, Temperature, state, g, ip, el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use math, only: math_Plain3333to99, &
|
|
math_mul6x6
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic, &
|
|
debug_levelSelective, &
|
|
debug_g, &
|
|
debug_i, &
|
|
debug_e
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_plasticityInstance
|
|
use lattice, only: lattice_Sslip, &
|
|
lattice_Sslip_v
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain number
|
|
ip, & ! current integration point
|
|
el ! current element number
|
|
real(pReal), intent(in) :: Temperature ! temperature
|
|
real(pReal), dimension(6), intent(in) :: Tstar_v ! 2nd Piola-Kirchhoff stress in Mandel notation
|
|
|
|
!*** input/output variables
|
|
type(p_vec), intent(inout) :: state ! microstructural state
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(3,3), intent(out) :: Lp ! plastic velocity gradient
|
|
real(pReal), dimension(9,9), intent(out) :: dLp_dTstar99 ! derivative of Lp with respect to Tstar (9x9 matrix)
|
|
|
|
!*** local variables
|
|
integer(pInt) myInstance, & ! current instance of this plasticity
|
|
myStructure, & ! current lattice structure
|
|
ns, & ! short notation for the total number of active slip systems
|
|
c, &
|
|
i, &
|
|
j, &
|
|
k, &
|
|
l, &
|
|
t, & ! dislocation type
|
|
s, & ! index of my current slip system
|
|
sLattice ! index of my current slip system according to lattice order
|
|
real(pReal), dimension(3,3,3,3) :: dLp_dTstar3333 ! derivative of Lp with respect to Tstar (3x3x3x3 matrix)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),4) :: &
|
|
rhoSgl, & ! single dislocation densities (including used)
|
|
v, & ! velocity
|
|
dv_dtau ! velocity derivative with respect to the shear stress
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
tau, & ! resolved shear stress including non Schmid and backstress terms
|
|
gdotTotal, & ! shear rate
|
|
dgdotTotal_dtau, & ! derivative of the shear rate with respect to the shear stress
|
|
tauBack ! back stress from dislocation gradients on same slip system
|
|
|
|
|
|
!*** initialize local variables
|
|
|
|
Lp = 0.0_pReal
|
|
dLp_dTstar3333 = 0.0_pReal
|
|
|
|
myInstance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
myStructure = constitutive_nonlocal_structure(myInstance)
|
|
ns = constitutive_nonlocal_totalNslip(myInstance)
|
|
|
|
|
|
!*** shortcut to state variables
|
|
|
|
forall (s = 1_pInt:ns, t = 1_pInt:4_pInt) &
|
|
rhoSgl(s,t) = max(state%p((t-1_pInt)*ns+s), 0.0_pReal)
|
|
tauBack = state%p(12_pInt*ns+1:13_pInt*ns)
|
|
|
|
|
|
!*** get effective resolved shear stress
|
|
|
|
do s = 1_pInt,ns
|
|
tau(s) = math_mul6x6(Tstar_v, lattice_Sslip_v(:,constitutive_nonlocal_slipSystemLattice(s,myInstance),myStructure)) &
|
|
+ tauBack(s)
|
|
enddo
|
|
|
|
|
|
!*** get dislocation velocity and its tangent and store the velocity in the state array
|
|
|
|
if (myStructure == 1_pInt) then ! for fcc all velcities are equal
|
|
call constitutive_nonlocal_kinetics(v(1:ns,1), tau, 1_pInt, Temperature, state, g, ip, el, dv_dtau(1:ns,1))
|
|
do t = 1_pInt,4_pInt
|
|
v(1:ns,t) = v(1:ns,1)
|
|
dv_dtau(1:ns,t) = dv_dtau(1:ns,1)
|
|
state%p((12_pInt+t)*ns+1:(13_pInt+t)*ns) = v(1:ns,1)
|
|
enddo
|
|
else ! for all other lattice structures the velcities may vary with character and sign
|
|
do t = 1_pInt,4_pInt
|
|
c = (t-1_pInt)/2_pInt+1_pInt
|
|
call constitutive_nonlocal_kinetics(v(1:ns,t), tau, c, Temperature, state, g, ip, el, dv_dtau(1:ns,t))
|
|
state%p((12+t)*ns+1:(13+t)*ns) = v(1:ns,t)
|
|
enddo
|
|
endif
|
|
|
|
|
|
!*** Bauschinger effect
|
|
|
|
forall (s = 1_pInt:ns, t = 5_pInt:8_pInt, state%p((t-1)*ns+s) * v(s,t-4_pInt) < 0.0_pReal) &
|
|
rhoSgl(s,t-4_pInt) = rhoSgl(s,t-4_pInt) + abs(state%p((t-1_pInt)*ns+s))
|
|
|
|
|
|
!*** Calculation of gdot and its tangent
|
|
|
|
gdotTotal = sum(rhoSgl * v, 2) * constitutive_nonlocal_burgers(1:ns,myInstance)
|
|
dgdotTotal_dtau = sum(rhoSgl * dv_dtau, 2) * constitutive_nonlocal_burgers(1:ns,myInstance)
|
|
|
|
|
|
!*** Calculation of Lp and its tangent
|
|
|
|
do s = 1_pInt,ns
|
|
sLattice = constitutive_nonlocal_slipSystemLattice(s,myInstance)
|
|
Lp = Lp + gdotTotal(s) * lattice_Sslip(1:3,1:3,sLattice,myStructure)
|
|
forall (i=1_pInt:3_pInt,j=1_pInt:3_pInt,k=1_pInt:3_pInt,l=1_pInt:3_pInt) &
|
|
dLp_dTstar3333(i,j,k,l) = dLp_dTstar3333(i,j,k,l) + dgdotTotal_dtau(s) * lattice_Sslip(i,j, sLattice,myStructure) &
|
|
* lattice_Sslip(k,l, sLattice,myStructure)
|
|
enddo
|
|
dLp_dTstar99 = math_Plain3333to99(dLp_dTstar3333)
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt )) then
|
|
write(6,*)
|
|
write(6,'(a,i8,1x,i2,1x,i1)') '<< CONST >> nonlocal_LpandItsTangent at el ip g ',el,ip,g
|
|
write(6,*)
|
|
write(6,'(a,/,12x,12(f12.5,1x))') '<< CONST >> gdot total / 1e-3',gdotTotal*1e3_pReal
|
|
write(6,'(a,/,3(12x,3(f12.7,1x),/))') '<< CONST >> Lp',Lp
|
|
endif
|
|
#endif
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* incremental change of microstructure *
|
|
!*********************************************************************
|
|
subroutine constitutive_nonlocal_deltaState(deltaState, state, Tstar_v, Temperature, g,ip,el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic, &
|
|
debug_levelSelective, &
|
|
debug_g, &
|
|
debug_i, &
|
|
debug_e
|
|
use math, only: pi, &
|
|
math_mul6x6
|
|
use lattice, only: lattice_Sslip_v
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_plasticityInstance
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain number
|
|
ip, & ! current integration point
|
|
el ! current element number
|
|
real(pReal), intent(in) :: Temperature ! temperature
|
|
real(pReal), dimension(6), intent(in) :: Tstar_v ! current 2nd Piola-Kirchhoff stress in Mandel notation
|
|
|
|
!*** input/output variables
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(inout) :: &
|
|
state ! current microstructural state
|
|
|
|
!*** output variables
|
|
type(p_vec), intent(out) :: deltaState ! change of state variables / microstructure
|
|
|
|
!*** local variables
|
|
integer(pInt) myInstance, & ! current instance of this plasticity
|
|
myStructure, & ! current lattice structure
|
|
ns, & ! short notation for the total number of active slip systems
|
|
c, & ! character of dislocation
|
|
n, & ! index of my current neighbor
|
|
t, & ! type of dislocation
|
|
s, & ! index of my current slip system
|
|
sLattice ! index of my current slip system according to lattice order
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),10) :: &
|
|
deltaRho, & ! density increment
|
|
deltaRhoRemobilization, & ! density increment by remobilization
|
|
deltaRhoDipole2SingleStress ! density increment by dipole dissociation (by stress change)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),8) :: &
|
|
rhoSgl ! current single dislocation densities (positive/negative screw and edge without dipoles)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),4) :: &
|
|
v ! dislocation glide velocity
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
tau, & ! current resolved shear stress
|
|
tauBack ! current back stress from pileups on same slip system
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
rhoDip, & ! current dipole dislocation densities (screw and edge dipoles)
|
|
dLower, & ! minimum stable dipole distance for edges and screws
|
|
dUpper, & ! current maximum stable dipole distance for edges and screws
|
|
dUpperOld, & ! old maximum stable dipole distance for edges and screws
|
|
deltaDUpper ! change in maximum stable dipole distance for edges and screws
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt)) then
|
|
write(6,*)
|
|
write(6,'(a,i8,1x,i2,1x,i1)') '<< CONST >> nonlocal_deltaState at el ip g ',el,ip,g
|
|
write(6,*)
|
|
endif
|
|
#endif
|
|
|
|
myInstance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
myStructure = constitutive_nonlocal_structure(myInstance)
|
|
ns = constitutive_nonlocal_totalNslip(myInstance)
|
|
|
|
|
|
!*** shortcut to state variables
|
|
|
|
forall (s = 1_pInt:ns, t = 1_pInt:4_pInt) &
|
|
rhoSgl(s,t) = max(state(g,ip,el)%p((t-1_pInt)*ns+s), 0.0_pReal)
|
|
forall (s = 1_pInt:ns, t = 5_pInt:8_pInt) &
|
|
rhoSgl(s,t) = state(g,ip,el)%p((t-1_pInt)*ns+s)
|
|
forall (s = 1_pInt:ns, c = 1_pInt:2_pInt) &
|
|
rhoDip(s,c) = max(state(g,ip,el)%p((7_pInt+c)*ns+s), 0.0_pReal)
|
|
tauBack = state(g,ip,el)%p(12_pInt*ns+1:13_pInt*ns)
|
|
forall (t = 1_pInt:4_pInt) &
|
|
v(1_pInt:ns,t) = state(g,ip,el)%p((12_pInt+t)*ns+1_pInt:(13_pInt+t)*ns)
|
|
forall (c = 1_pInt:2_pInt) &
|
|
dUpperOld(1_pInt:ns,c) = state(g,ip,el)%p((16_pInt+c)*ns+1_pInt:(17_pInt+c)*ns)
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** dislocation remobilization (bauschinger effect)
|
|
|
|
deltaRhoRemobilization = 0.0_pReal
|
|
do t = 1_pInt,4_pInt
|
|
do s = 1_pInt,ns
|
|
if (rhoSgl(s,t+4_pInt) * v(s,t) < 0.0_pReal) then
|
|
deltaRhoRemobilization(s,t) = abs(rhoSgl(s,t+4_pInt))
|
|
rhoSgl(s,t) = rhoSgl(s,t) + abs(rhoSgl(s,t+4_pInt))
|
|
deltaRhoRemobilization(s,t+4_pInt) = - rhoSgl(s,t+4_pInt)
|
|
rhoSgl(s,t+4_pInt) = 0.0_pReal
|
|
endif
|
|
enddo
|
|
enddo
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** calculate dipole formation and dissociation by stress change
|
|
|
|
!*** calculate limits for stable dipole height
|
|
|
|
do s = 1_pInt,ns
|
|
sLattice = constitutive_nonlocal_slipSystemLattice(s,myInstance)
|
|
tau(s) = math_mul6x6(Tstar_v, lattice_Sslip_v(1:6,sLattice,myStructure)) + tauBack(s)
|
|
if (abs(tau(s)) < 1.0e-15_pReal) tau(s) = 1.0e-15_pReal
|
|
enddo
|
|
dLower = constitutive_nonlocal_minimumDipoleHeight(1:ns,1:2,myInstance)
|
|
dUpper(1:ns,1) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (8.0_pReal * pi * (1.0_pReal - constitutive_nonlocal_nu(myInstance)) * abs(tau))
|
|
dUpper(1:ns,2) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (4.0_pReal * pi * abs(tau))
|
|
forall (c = 1_pInt:2_pInt) &
|
|
dUpper(1:ns,c) = min(1.0_pReal / sqrt(sum(abs(rhoSgl),c) + sum(rhoDip,c)), dUpper(1:ns,c))
|
|
dUpper = max(dUpper,dLower)
|
|
deltaDUpper = dUpper - dUpperOld
|
|
|
|
|
|
!*** dissociation by stress increase
|
|
|
|
deltaRhoDipole2SingleStress = 0.0_pReal
|
|
forall (c=1_pInt:2_pInt, s=1_pInt:ns, deltaDUpper(s,c) < 0.0_pReal) &
|
|
deltaRhoDipole2SingleStress(s,8_pInt+c) = rhoDip(s,c) * deltaDUpper(s,c) / (dUpperOld(s,c) - dLower(s,c))
|
|
|
|
forall (t=1_pInt:4_pInt) &
|
|
deltaRhoDipole2SingleStress(1_pInt:ns,t) = -0.5_pReal * deltaRhoDipole2SingleStress(1_pInt:ns,(t-1_pInt)/2_pInt+9_pInt)
|
|
|
|
|
|
|
|
!*** store new maximum dipole height in state
|
|
|
|
forall (c = 1_pInt:2_pInt) &
|
|
state(g,ip,el)%p((16_pInt+c)*ns+1_pInt:(17_pInt+c)*ns) = dUpper(1_pInt:ns,c)
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** assign the changes in the dislocation densities to deltaState
|
|
|
|
deltaRho = 0.0_pReal
|
|
deltaRho = deltaRhoRemobilization &
|
|
+ deltaRhoDipole2SingleStress
|
|
|
|
deltaState%p = reshape(deltaRho,(/10_pInt*ns/))
|
|
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt )) then
|
|
write(6,'(a,/,8(12x,12(e12.5,1x),/))') '<< CONST >> dislocation remobilization', deltaRhoRemobilization(1:ns,1:8)
|
|
write(6,'(a,/,10(12x,12(e12.5,1x),/))') '<< CONST >> dipole dissociation by stress increase', deltaRhoDipole2SingleStress
|
|
write(6,*)
|
|
endif
|
|
#endif
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* rate of change of microstructure *
|
|
!*********************************************************************
|
|
function constitutive_nonlocal_dotState(Tstar_v, Fe, Fp, Temperature, state, timestep, orientation, g,ip,el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec, &
|
|
DAMASK_NaN
|
|
use numerics, only: numerics_integrationMode
|
|
use IO, only: IO_error
|
|
use debug, only: debug_level, &
|
|
debug_constitutive, &
|
|
debug_levelBasic, &
|
|
debug_levelSelective, &
|
|
debug_g, &
|
|
debug_i, &
|
|
debug_e
|
|
use math, only: math_norm3, &
|
|
math_mul6x6, &
|
|
math_mul3x3, &
|
|
math_mul33x3, &
|
|
math_mul33x33, &
|
|
math_inv33, &
|
|
math_det33, &
|
|
math_transpose33, &
|
|
pi
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips, &
|
|
mesh_element, &
|
|
FE_NipNeighbors, &
|
|
mesh_ipNeighborhood, &
|
|
mesh_ipVolume, &
|
|
mesh_ipArea, &
|
|
mesh_ipAreaNormal
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_plasticityInstance, &
|
|
phase_localPlasticity, &
|
|
phase_plasticity
|
|
use lattice, only: lattice_Sslip_v, &
|
|
lattice_sd, &
|
|
lattice_st
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain number
|
|
ip, & ! current integration point
|
|
el ! current element number
|
|
real(pReal), intent(in) :: Temperature, & ! temperature
|
|
timestep ! substepped crystallite time increment
|
|
real(pReal), dimension(6), intent(in) :: Tstar_v ! current 2nd Piola-Kirchhoff stress in Mandel notation
|
|
real(pReal), dimension(3,3,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
Fe, & ! elastic deformation gradient
|
|
Fp ! plastic deformation gradient
|
|
real(pReal), dimension(4,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
orientation ! crystal lattice orientation
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
state ! current microstructural state
|
|
!*** input/output variables
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(constitutive_nonlocal_sizeDotState(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
constitutive_nonlocal_dotState ! evolution of state variables / microstructure
|
|
|
|
!*** local variables
|
|
integer(pInt) myInstance, & ! current instance of this plasticity
|
|
myStructure, & ! current lattice structure
|
|
ns, & ! short notation for the total number of active slip systems
|
|
c, & ! character of dislocation
|
|
n, & ! index of my current neighbor
|
|
neighboring_el, & ! element number of my neighbor
|
|
neighboring_ip, & ! integration point of my neighbor
|
|
neighboring_n, & ! neighbor index pointing to me when looking from my neighbor
|
|
opposite_n, & ! index of my opposite neighbor
|
|
opposite_ip, & ! ip of my opposite neighbor
|
|
opposite_el, & ! element index of my opposite neighbor
|
|
t, & ! type of dislocation
|
|
topp, & ! type of dislocation with opposite sign to t
|
|
s, & ! index of my current slip system
|
|
sLattice, & ! index of my current slip system according to lattice order
|
|
deads
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),10) :: &
|
|
rhoDot, & ! density evolution
|
|
rhoDotMultiplication, & ! density evolution by multiplication
|
|
rhoDotFlux, & ! density evolution by flux
|
|
rhoDotSingle2DipoleGlide, & ! density evolution by dipole formation (by glide)
|
|
rhoDotAthermalAnnihilation, & ! density evolution by athermal annihilation
|
|
rhoDotThermalAnnihilation ! density evolution by thermal annihilation
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),8) :: &
|
|
neighboring_rhoSgl, & ! current single dislocation densities (positive/negative screw and edge without dipoles)
|
|
rhoSgl ! current single dislocation densities (positive/negative screw and edge without dipoles)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),4) :: &
|
|
v, & ! dislocation glide velocity
|
|
neighboring_v, & ! dislocation glide velocity
|
|
gdot ! shear rates
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
rhoForest, & ! forest dislocation density
|
|
tauThreshold, & ! threshold shear stress
|
|
tau, & ! current resolved shear stress
|
|
tauBack, & ! current back stress from pileups on same slip system
|
|
vClimb ! climb velocity of edge dipoles
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
rhoDip, & ! current dipole dislocation densities (screw and edge dipoles)
|
|
dLower, & ! minimum stable dipole distance for edges and screws
|
|
dUpper ! current maximum stable dipole distance for edges and screws
|
|
real(pReal), dimension(3,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),4) :: &
|
|
m ! direction of dislocation motion
|
|
real(pReal), dimension(3,3) :: my_F, & ! my total deformation gradient
|
|
neighboring_F, & ! total deformation gradient of my neighbor
|
|
my_Fe, & ! my elastic deformation gradient
|
|
neighboring_Fe, & ! elastic deformation gradient of my neighbor
|
|
Favg ! average total deformation gradient of me and my neighbor
|
|
real(pReal), dimension(3) :: normal_neighbor2me, & ! interface normal pointing from my neighbor to me in neighbor's lattice configuration
|
|
normal_neighbor2me_defConf, & ! interface normal pointing from my neighbor to me in shared deformed configuration
|
|
normal_me2neighbor, & ! interface normal pointing from me to my neighbor in my lattice configuration
|
|
normal_me2neighbor_defConf ! interface normal pointing from me to my neighbor in shared deformed configuration
|
|
real(pReal) area, & ! area of the current interface
|
|
transmissivity, & ! overall transmissivity of dislocation flux to neighboring material point
|
|
lineLength, & ! dislocation line length leaving the current interface
|
|
D ! self diffusion
|
|
logical considerEnteringFlux, &
|
|
considerLeavingFlux
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt)) then
|
|
write(6,*)
|
|
write(6,'(a,i8,1x,i2,1x,i1)') '<< CONST >> nonlocal_dotState at el ip g ',el,ip,g
|
|
write(6,*)
|
|
endif
|
|
#endif
|
|
|
|
|
|
myInstance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
myStructure = constitutive_nonlocal_structure(myInstance)
|
|
ns = constitutive_nonlocal_totalNslip(myInstance)
|
|
|
|
tau = 0.0_pReal
|
|
gdot = 0.0_pReal
|
|
|
|
|
|
!*** shortcut to state variables
|
|
|
|
forall (s = 1_pInt:ns, t = 1_pInt:4_pInt) &
|
|
rhoSgl(s,t) = max(state(g,ip,el)%p((t-1_pInt)*ns+s), 0.0_pReal)
|
|
forall (s = 1_pInt:ns, t = 5_pInt:8_pInt) &
|
|
rhoSgl(s,t) = state(g,ip,el)%p((t-1_pInt)*ns+s)
|
|
forall (s = 1_pInt:ns, c = 1_pInt:2_pInt) &
|
|
rhoDip(s,c) = max(state(g,ip,el)%p((7_pInt+c)*ns+s), 0.0_pReal)
|
|
rhoForest = state(g,ip,el)%p(10_pInt*ns+1:11_pInt*ns)
|
|
tauThreshold = state(g,ip,el)%p(11_pInt*ns+1_pInt:12_pInt*ns)
|
|
tauBack = state(g,ip,el)%p(12_pInt*ns+1:13_pInt*ns)
|
|
forall (t = 1_pInt:4_pInt) &
|
|
v(1_pInt:ns,t) = state(g,ip,el)%p((12_pInt+t)*ns+1_pInt:(13_pInt+t)*ns)
|
|
|
|
|
|
!*** sanity check for timestep
|
|
|
|
if (timestep <= 0.0_pReal) then ! if illegal timestep...
|
|
constitutive_nonlocal_dotState = 0.0_pReal ! ...return without doing anything (-> zero dotState)
|
|
return
|
|
endif
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** Calculate shear rate
|
|
|
|
forall (t = 1_pInt:4_pInt) &
|
|
gdot(1_pInt:ns,t) = rhoSgl(1_pInt:ns,t) * constitutive_nonlocal_burgers(1:ns,myInstance) * v(1:ns,t)
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt )) then
|
|
write(6,'(a,/,10(12x,12(e12.5,1x),/))') '<< CONST >> rho / 1/m^2', rhoSgl, rhoDip
|
|
write(6,'(a,/,4(12x,12(e12.5,1x),/))') '<< CONST >> gdot / 1/s',gdot
|
|
endif
|
|
#endif
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** calculate limits for stable dipole height
|
|
|
|
do s = 1_pInt,ns ! loop over slip systems
|
|
sLattice = constitutive_nonlocal_slipSystemLattice(s,myInstance)
|
|
tau(s) = math_mul6x6(Tstar_v, lattice_Sslip_v(1:6,sLattice,myStructure)) + tauBack(s)
|
|
if (abs(tau(s)) < 1.0e-15_pReal) tau(s) = 1.0e-15_pReal
|
|
enddo
|
|
|
|
dLower = constitutive_nonlocal_minimumDipoleHeight(1:ns,1:2,myInstance)
|
|
dUpper(1:ns,1) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (8.0_pReal * pi * (1.0_pReal - constitutive_nonlocal_nu(myInstance)) * abs(tau))
|
|
dUpper(1:ns,2) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (4.0_pReal * pi * abs(tau))
|
|
forall (c = 1_pInt:2_pInt) &
|
|
dUpper(1:ns,c) = min(1.0_pReal / sqrt(sum(abs(rhoSgl),c) + sum(rhoDip,c)), dUpper(1:ns,c))
|
|
dUpper = max(dUpper,dLower)
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** calculate dislocation multiplication
|
|
|
|
rhoDotMultiplication = 0.0_pReal
|
|
where (rhoSgl(1:ns,3:4) > 0.0_pReal) &
|
|
rhoDotMultiplication(1:ns,1:2) = spread(0.5_pReal * sum(abs(gdot(1:ns,3:4)),2) * sqrt(rhoForest) &
|
|
/ constitutive_nonlocal_lambda0(1:ns,myInstance) &
|
|
/ constitutive_nonlocal_burgers(1:ns,myInstance), 2, 2)
|
|
rhoDotMultiplication(1:ns,3:4) = rhoDotMultiplication(1:ns,1:2)
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** calculate dislocation fluxes (only for nonlocal plasticity)
|
|
|
|
rhoDotFlux = 0.0_pReal
|
|
|
|
if (.not. phase_localPlasticity(material_phase(g,ip,el))) then ! only for nonlocal plasticity
|
|
|
|
|
|
!*** check CFL (Courant-Friedrichs-Lewy) condition for flux
|
|
|
|
if (any( abs(gdot) > 0.0_pReal & ! any active slip system ...
|
|
.and. constitutive_nonlocal_CFLfactor(myInstance) * abs(v) * timestep &
|
|
> mesh_ipVolume(ip,el) / maxval(mesh_ipArea(:,ip,el)))) then ! ...with velocity above critical value (we use the reference volume and area for simplicity here)
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt) then
|
|
write(6,'(a,i5,a,i2)') '<< CONST >> CFL condition not fullfilled at el ',el,' ip ',ip
|
|
write(6,'(a,e10.3,a,e10.3)') '<< CONST >> velocity is at ',maxval(abs(v)),' at a timestep of ',timestep
|
|
write(6,'(a)') '<< CONST >> enforcing cutback !!!'
|
|
endif
|
|
#endif
|
|
constitutive_nonlocal_dotState = DAMASK_NaN ! -> return NaN and, hence, enforce cutback
|
|
return
|
|
endif
|
|
|
|
|
|
!*** be aware of the definition of lattice_st = lattice_sd x lattice_sn !!!
|
|
!*** opposite sign to our p vector in the (s,p,n) triplet !!!
|
|
|
|
m(1:3,1:ns,1) = lattice_sd(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,myInstance), myStructure)
|
|
m(1:3,1:ns,2) = -lattice_sd(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,myInstance), myStructure)
|
|
m(1:3,1:ns,3) = -lattice_st(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,myInstance), myStructure)
|
|
m(1:3,1:ns,4) = lattice_st(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,myInstance), myStructure)
|
|
|
|
my_Fe = Fe(1:3,1:3,g,ip,el)
|
|
my_F = math_mul33x33(my_Fe, Fp(1:3,1:3,g,ip,el))
|
|
|
|
do n = 1_pInt,FE_NipNeighbors(mesh_element(2,el)) ! loop through my neighbors
|
|
neighboring_el = mesh_ipNeighborhood(1,n,ip,el)
|
|
neighboring_ip = mesh_ipNeighborhood(2,n,ip,el)
|
|
if (neighboring_el > 0_pInt .and. neighboring_ip > 0_pInt) then ! if neighbor exists ...
|
|
do neighboring_n = 1_pInt,FE_NipNeighbors(mesh_element(2,neighboring_el)) ! find neighboring index that points from my neighbor to myself
|
|
if ( el == mesh_ipNeighborhood(1,neighboring_n,neighboring_ip,neighboring_el) &
|
|
.and. ip == mesh_ipNeighborhood(2,neighboring_n,neighboring_ip,neighboring_el)) then ! possible candidate
|
|
if (math_mul3x3(mesh_ipAreaNormal(1:3,n,ip,el),&
|
|
mesh_ipAreaNormal(1:3,neighboring_n,neighboring_ip,neighboring_el)) < 0.0_pReal) then ! area normals have opposite orientation (we have to check that because of special case for single element with two ips and periodicity. In this case the neighbor is identical in two different directions.)
|
|
exit
|
|
endif
|
|
endif
|
|
enddo
|
|
endif
|
|
|
|
opposite_n = n + mod(n,2_pInt) - mod(n+1_pInt,2_pInt)
|
|
opposite_el = mesh_ipNeighborhood(1,opposite_n,ip,el)
|
|
opposite_ip = mesh_ipNeighborhood(2,opposite_n,ip,el)
|
|
|
|
if (neighboring_el > 0_pInt .and. neighboring_ip > 0_pInt) then ! if neighbor exists, average deformation gradient
|
|
neighboring_Fe = Fe(1:3,1:3,g,neighboring_ip,neighboring_el)
|
|
neighboring_F = math_mul33x33(neighboring_Fe, Fp(1:3,1:3,g,neighboring_ip,neighboring_el))
|
|
Favg = 0.5_pReal * (my_F + neighboring_F)
|
|
else ! if no neighbor, take my value as average
|
|
Favg = my_F
|
|
endif
|
|
|
|
|
|
!* FLUX FROM MY NEIGHBOR TO ME
|
|
!* This is only considered, if I have a neighbor of nonlocal plasticity (also nonlocal constitutive law with local properties) that is at least a little bit compatible.
|
|
!* If it's not at all compatible, no flux is arriving, because everything is dammed in front of my neighbor's interface.
|
|
!* The entering flux from my neighbor will be distributed on my slip systems according to the compatibility
|
|
|
|
considerEnteringFlux = .false.
|
|
neighboring_v = 0.0_pReal ! needed for check of sign change in flux density below
|
|
neighboring_rhoSgl = 0.0_pReal
|
|
if (neighboring_el > 0_pInt .or. neighboring_ip > 0_pInt) then
|
|
if (phase_plasticity(material_phase(1,neighboring_ip,neighboring_el)) == constitutive_nonlocal_label &
|
|
.and. any(constitutive_nonlocal_compatibility(:,:,:,n,ip,el) > 0.0_pReal)) &
|
|
considerEnteringFlux = .true.
|
|
endif
|
|
|
|
if (considerEnteringFlux) then
|
|
forall (t = 1_pInt:4_pInt) &
|
|
neighboring_v(1_pInt:ns,t) = state(g,neighboring_ip,neighboring_el)%p((12_pInt+t)*ns+1_pInt:(13_pInt+t)*ns)
|
|
forall (t = 1_pInt:4_pInt) &
|
|
neighboring_rhoSgl(1_pInt:ns,t) = max(state(g,neighboring_ip,neighboring_el)%p((t-1_pInt)*ns+1_pInt:t*ns), 0.0_pReal)
|
|
forall (t = 5_pInt:8_pInt) &
|
|
neighboring_rhoSgl(1_pInt:ns,t) = state(g,neighboring_ip,neighboring_el)%p((t-1_pInt)*ns+1_pInt:t*ns)
|
|
normal_neighbor2me_defConf = math_det33(Favg) &
|
|
* math_mul33x3(math_inv33(transpose(Favg)), mesh_ipAreaNormal(1:3,neighboring_n,neighboring_ip,neighboring_el)) ! calculate the normal of the interface in (average) deformed configuration (now pointing from my neighbor to me!!!)
|
|
normal_neighbor2me = math_mul33x3(transpose(neighboring_Fe), normal_neighbor2me_defConf) / math_det33(neighboring_Fe) ! interface normal in the lattice configuration of my neighbor
|
|
area = mesh_ipArea(neighboring_n,neighboring_ip,neighboring_el) * math_norm3(normal_neighbor2me)
|
|
normal_neighbor2me = normal_neighbor2me / math_norm3(normal_neighbor2me) ! normalize the surface normal to unit length
|
|
do s = 1_pInt,ns
|
|
do t = 1_pInt,4_pInt
|
|
c = (t + 1_pInt) / 2
|
|
topp = t + mod(t,2_pInt) - mod(t+1_pInt,2_pInt)
|
|
if (neighboring_v(s,t) * math_mul3x3(m(1:3,s,t), normal_neighbor2me) > 0.0_pReal & ! flux from my neighbor to me == entering flux for me
|
|
.and. v(s,t) * neighboring_v(s,t) >= 0.0_pReal ) then ! ... only if no sign change in flux density
|
|
do deads = 0_pInt,4_pInt,4_pInt
|
|
lineLength = abs(neighboring_rhoSgl(s,t+deads)) * neighboring_v(s,t) &
|
|
* math_mul3x3(m(1:3,s,t), normal_neighbor2me) * area ! positive line length that wants to enter through this interface
|
|
where (constitutive_nonlocal_compatibility(c,1_pInt:ns,s,n,ip,el) > 0.0_pReal) & ! positive compatibility...
|
|
rhoDotFlux(1_pInt:ns,t) = rhoDotFlux(1_pInt:ns,t) + lineLength / mesh_ipVolume(ip,el) & ! ... transferring to equally signed mobile dislocation type
|
|
* constitutive_nonlocal_compatibility(c,1_pInt:ns,s,n,ip,el) ** 2.0_pReal
|
|
where (constitutive_nonlocal_compatibility(c,1_pInt:ns,s,n,ip,el) < 0.0_pReal) & ! ..negative compatibility...
|
|
rhoDotFlux(1_pInt:ns,topp) = rhoDotFlux(1_pInt:ns,topp) + lineLength / mesh_ipVolume(ip,el) & ! ... transferring to opposite signed mobile dislocation type
|
|
* constitutive_nonlocal_compatibility(c,1_pInt:ns,s,n,ip,el) ** 2.0_pReal
|
|
enddo
|
|
endif
|
|
enddo
|
|
enddo
|
|
endif
|
|
|
|
|
|
!* FLUX FROM ME TO MY NEIGHBOR
|
|
!* This is not considered, if my opposite neighbor has a different constitutive law than nonlocal (still considered for nonlocal law with lcal properties).
|
|
!* Then, we assume, that the opposite(!) neighbor sends an equal amount of dislocations to me.
|
|
!* So the net flux in the direction of my neighbor is equal to zero:
|
|
!* leaving flux to neighbor == entering flux from opposite neighbor
|
|
!* In case of reduced transmissivity, part of the leaving flux is stored as dead dislocation density.
|
|
!* That means for an interface of zero transmissivity the leaving flux is fully converted to dead dislocations.
|
|
|
|
considerLeavingFlux = .true.
|
|
if (opposite_el > 0_pInt .and. opposite_ip > 0_pInt) then
|
|
if (phase_plasticity(material_phase(1,opposite_ip,opposite_el)) /= constitutive_nonlocal_label) &
|
|
considerLeavingFlux = .false.
|
|
endif
|
|
|
|
if (considerLeavingFlux) then
|
|
normal_me2neighbor_defConf = math_det33(Favg) * math_mul33x3(math_inv33(math_transpose33(Favg)), &
|
|
mesh_ipAreaNormal(1:3,n,ip,el)) ! calculate the normal of the interface in (average) deformed configuration (pointing from me to my neighbor!!!)
|
|
normal_me2neighbor = math_mul33x3(math_transpose33(my_Fe), normal_me2neighbor_defConf) / math_det33(my_Fe) ! interface normal in my lattice configuration
|
|
area = mesh_ipArea(n,ip,el) * math_norm3(normal_me2neighbor)
|
|
normal_me2neighbor = normal_me2neighbor / math_norm3(normal_me2neighbor) ! normalize the surface normal to unit length
|
|
do s = 1_pInt,ns
|
|
do t = 1_pInt,4_pInt
|
|
c = (t + 1_pInt) / 2_pInt
|
|
if (v(s,t) * math_mul3x3(m(1:3,s,t), normal_me2neighbor) > 0.0_pReal ) then ! flux from me to my neighbor == leaving flux for me (might also be a pure flux from my mobile density to dead density if interface not at all transmissive)
|
|
if (v(s,t) * neighboring_v(s,t) >= 0.0_pReal) then ! no sign change in flux density
|
|
transmissivity = sum(constitutive_nonlocal_compatibility(c,1_pInt:ns,s,n,ip,el)**2.0_pReal) ! overall transmissivity from this slip system to my neighbor
|
|
else ! sign change in flux density means sign change in stress which does not allow for dislocations to arive at the neighbor
|
|
transmissivity = 0.0_pReal
|
|
endif
|
|
lineLength = rhoSgl(s,t) * v(s,t) * math_mul3x3(m(1:3,s,t), normal_me2neighbor) * area ! positive line length of mobiles that wants to leave through this interface
|
|
rhoDotFlux(s,t) = rhoDotFlux(s,t) - lineLength / mesh_ipVolume(ip,el) ! subtract dislocation flux from current type
|
|
rhoDotFlux(s,t+4_pInt) = rhoDotFlux(s,t+4_pInt) + lineLength / mesh_ipVolume(ip,el) * (1.0_pReal - transmissivity) &
|
|
* sign(1.0_pReal, v(s,t)) ! dislocation flux that is not able to leave through interface (because of low transmissivity) will remain as immobile single density at the material point
|
|
lineLength = rhoSgl(s,t+4_pInt) * v(s,t) * math_mul3x3(m(1:3,s,t), normal_me2neighbor) * area ! positive line length of deads that wants to leave through this interface
|
|
rhoDotFlux(s,t+4_pInt) = rhoDotFlux(s,t+4_pInt) - lineLength / mesh_ipVolume(ip,el) * transmissivity ! dead dislocations leaving through this interface
|
|
endif
|
|
enddo
|
|
enddo
|
|
endif
|
|
|
|
enddo ! neighbor loop
|
|
endif
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** calculate dipole formation and annihilation
|
|
|
|
!*** formation by glide
|
|
|
|
do c = 1_pInt,2_pInt
|
|
|
|
rhoDotSingle2DipoleGlide(1:ns,2*c-1) = -2.0_pReal * dUpper(1:ns,c) / constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
* (rhoSgl(1:ns,2*c-1) * abs(gdot(1:ns,2*c)) & ! negative mobile --> positive mobile
|
|
+ rhoSgl(1:ns,2*c) * abs(gdot(1:ns,2*c-1)) & ! positive mobile --> negative mobile
|
|
+ abs(rhoSgl(1:ns,2*c+4)) * abs(gdot(1:ns,2*c-1))) ! positive mobile --> negative immobile
|
|
|
|
rhoDotSingle2DipoleGlide(1:ns,2*c) = -2.0_pReal * dUpper(1:ns,c) / constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
* (rhoSgl(1:ns,2*c-1) * abs(gdot(1:ns,2*c)) & ! negative mobile --> positive mobile
|
|
+ rhoSgl(1:ns,2*c) * abs(gdot(1:ns,2*c-1)) & ! positive mobile --> negative mobile
|
|
+ abs(rhoSgl(1:ns,2*c+3)) * abs(gdot(1:ns,2*c))) ! negative mobile --> positive immobile
|
|
|
|
rhoDotSingle2DipoleGlide(1:ns,2*c+3) = -2.0_pReal * dUpper(1:ns,c) / constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
* rhoSgl(1:ns,2*c+3) * abs(gdot(1:ns,2*c)) ! negative mobile --> positive immobile
|
|
|
|
rhoDotSingle2DipoleGlide(1:ns,2*c+4) = -2.0_pReal * dUpper(1:ns,c) / constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
* rhoSgl(1:ns,2*c+4) * abs(gdot(1:ns,2*c-1)) ! positive mobile --> negative immobile
|
|
|
|
rhoDotSingle2DipoleGlide(1:ns,c+8) = - rhoDotSingle2DipoleGlide(1:ns,2*c-1) - rhoDotSingle2DipoleGlide(1:ns,2*c) &
|
|
+ abs(rhoDotSingle2DipoleGlide(1:ns,2*c+3)) + abs(rhoDotSingle2DipoleGlide(1:ns,2*c+4))
|
|
enddo
|
|
|
|
|
|
!*** athermal annihilation
|
|
|
|
rhoDotAthermalAnnihilation = 0.0_pReal
|
|
|
|
forall (c=1_pInt:2_pInt) &
|
|
rhoDotAthermalAnnihilation(1:ns,c+8_pInt) = -2.0_pReal * dLower(1:ns,c) / constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
* ( 2.0_pReal * (rhoSgl(1:ns,2*c-1) * abs(gdot(1:ns,2*c)) + rhoSgl(1:ns,2*c) * abs(gdot(1:ns,2*c-1))) & ! was single hitting single
|
|
+ 2.0_pReal * (abs(rhoSgl(1:ns,2*c+3)) * abs(gdot(1:ns,2*c)) + abs(rhoSgl(1:ns,2*c+4)) * abs(gdot(1:ns,2*c-1))) & ! was single hitting immobile single or was immobile single hit by single
|
|
+ rhoDip(1:ns,c) * (abs(gdot(1:ns,2*c-1)) + abs(gdot(1:ns,2*c)))) ! single knocks dipole constituent
|
|
|
|
|
|
!*** thermally activated annihilation of dipoles
|
|
|
|
rhoDotThermalAnnihilation = 0.0_pReal
|
|
|
|
! edge annihilation by thermally activate climb
|
|
D = constitutive_nonlocal_Dsd0(myInstance) * exp(-constitutive_nonlocal_Qsd(myInstance) / (kB * Temperature))
|
|
vClimb = constitutive_nonlocal_atomicVolume(myInstance) * D / ( kB * Temperature ) &
|
|
* constitutive_nonlocal_Gmod(myInstance) / ( 2.0_pReal * pi * (1.0_pReal-constitutive_nonlocal_nu(myInstance)) ) &
|
|
* 2.0_pReal / ( dUpper(1:ns,1) + dLower(1:ns,1) )
|
|
rhoDotThermalAnnihilation(1:ns,9) = - 4.0_pReal * rhoDip(1:ns,1) * vClimb / (dUpper(1:ns,1) - dLower(1:ns,1))
|
|
|
|
! annihilation of screw dipoles: we assume that all screws annihilate instantaneously by cross-slipping on the colinear system
|
|
! (so right now this is actually an athermal process, could be enriched by a thermally activated probability for cross-slip)
|
|
! annihilated screw dipoles leave edge jogs behind on the colinear system
|
|
if (myStructure == 1_pInt) then ! only fcc
|
|
rhoDotThermalAnnihilation(1:ns,10) = -rhoDip(1:ns,2) / timestep
|
|
forall (s = 1:ns, constitutive_nonlocal_colinearSystem(s,myInstance) > 0_pInt) &
|
|
rhoDotThermalAnnihilation(constitutive_nonlocal_colinearSystem(s,myInstance),1:2) = -rhoDotThermalAnnihilation(s,10) &
|
|
* 0.25_pReal * sqrt(rhoForest(s)) * (dUpper(s,2) + dLower(s,2))
|
|
endif
|
|
|
|
|
|
|
|
!****************************************************************************
|
|
!*** assign the rates of dislocation densities to my dotState
|
|
!*** if evolution rates lead to negative densities, a cutback is enforced
|
|
|
|
rhoDot = 0.0_pReal
|
|
rhoDot = rhoDotFlux &
|
|
+ rhoDotMultiplication &
|
|
+ rhoDotSingle2DipoleGlide &
|
|
+ rhoDotAthermalAnnihilation &
|
|
+ rhoDotThermalAnnihilation
|
|
|
|
if (numerics_integrationMode == 1_pInt) then ! save rates for output if in central integration mode
|
|
constitutive_nonlocal_rhoDotFlux(1:ns,1:8,g,ip,el) = rhoDotFlux(1:ns,1:8)
|
|
constitutive_nonlocal_rhoDotMultiplication(1:ns,1:2,g,ip,el) = rhoDotMultiplication(1:ns,[1,3])
|
|
constitutive_nonlocal_rhoDotSingle2DipoleGlide(1:ns,1:2,g,ip,el) = rhoDotSingle2DipoleGlide(1:ns,9:10)
|
|
constitutive_nonlocal_rhoDotAthermalAnnihilation(1:ns,1:2,g,ip,el) = rhoDotAthermalAnnihilation(1:ns,9:10)
|
|
constitutive_nonlocal_rhoDotThermalAnnihilation(1:ns,1:2,g,ip,el) = rhoDotThermalAnnihilation(1:ns,9:10)
|
|
constitutive_nonlocal_rhoDotEdgeJogs(1:ns,g,ip,el) = &
|
|
2.0_pReal * rhoDotThermalAnnihilation(constitutive_nonlocal_colinearSystem(1:ns,myInstance),1)
|
|
endif
|
|
|
|
|
|
if ( any(rhoSgl(1:ns,1:4) + rhoDot(1:ns,1:4) * timestep < - constitutive_nonlocal_aTolRho(myInstance)) &
|
|
.or. any(rhoDip(1:ns,1:2) + rhoDot(1:ns,9:10) * timestep < - constitutive_nonlocal_aTolRho(myInstance))) then
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt) then
|
|
write(6,'(a,i5,a,i2)') '<< CONST >> evolution rate leads to negative density at el ',el,' ip ',ip
|
|
write(6,'(a)') '<< CONST >> enforcing cutback !!!'
|
|
endif
|
|
#endif
|
|
constitutive_nonlocal_dotState = DAMASK_NaN
|
|
return
|
|
else
|
|
constitutive_nonlocal_dotState(1:10_pInt*ns) = reshape(rhoDot,(/10_pInt*ns/))
|
|
endif
|
|
|
|
|
|
|
|
#ifndef _OPENMP
|
|
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt &
|
|
.and. ((debug_e == el .and. debug_i == ip .and. debug_g == g)&
|
|
.or. .not. iand(debug_level(debug_constitutive),debug_levelSelective) /= 0_pInt )) then
|
|
write(6,'(a,/,4(12x,12(e12.5,1x),/))') '<< CONST >> dislocation multiplication', rhoDotMultiplication(1:ns,1:4) * timestep
|
|
write(6,'(a,/,8(12x,12(e12.5,1x),/))') '<< CONST >> dislocation flux', rhoDotFlux(1:ns,1:8) * timestep
|
|
write(6,'(a,/,10(12x,12(e12.5,1x),/))') '<< CONST >> dipole formation by glide', rhoDotSingle2DipoleGlide * timestep
|
|
write(6,'(a,/,2(12x,12(e12.5,1x),/))') '<< CONST >> athermal dipole annihilation', &
|
|
rhoDotAthermalAnnihilation(1:ns,9:10) * timestep
|
|
write(6,'(a,/,10(12x,12(e12.5,1x),/))') '<< CONST >> thermally activated dipole annihilation', &
|
|
rhoDotThermalAnnihilation * timestep
|
|
write(6,'(a,/,10(12x,12(e12.5,1x),/))') '<< CONST >> total density change', rhoDot * timestep
|
|
write(6,'(a,/,10(12x,12(f12.7,1x),/))') '<< CONST >> relative density change', &
|
|
rhoDot(1:ns,1:8) * timestep / (abs(rhoSgl)+1.0e-10), &
|
|
rhoDot(1:ns,9:10) * timestep / (rhoDip+1.0e-10)
|
|
write(6,*)
|
|
endif
|
|
#endif
|
|
|
|
endfunction
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* COMPATIBILITY UPDATE *
|
|
!* Compatibility is defined as normalized product of signed cosine *
|
|
!* of the angle between the slip plane normals and signed cosine of *
|
|
!* the angle between the slip directions. Only the largest values *
|
|
!* that sum up to a total of 1 are considered, all others are set to *
|
|
!* zero. *
|
|
!*********************************************************************
|
|
subroutine constitutive_nonlocal_updateCompatibility(orientation,i,e)
|
|
|
|
use prec, only: pReal, &
|
|
pInt
|
|
use math, only: math_QuaternionDisorientation, &
|
|
math_mul3x3, &
|
|
math_qRot
|
|
use material, only: material_phase, &
|
|
material_texture, &
|
|
phase_localPlasticity, &
|
|
phase_plasticityInstance, &
|
|
homogenization_maxNgrains
|
|
use mesh, only: mesh_element, &
|
|
mesh_ipNeighborhood, &
|
|
FE_NipNeighbors, &
|
|
mesh_maxNips, &
|
|
mesh_NcpElems
|
|
use lattice, only: lattice_sn, &
|
|
lattice_sd
|
|
|
|
implicit none
|
|
|
|
!* input variables
|
|
integer(pInt), intent(in) :: i, & ! ip index
|
|
e ! element index
|
|
real(pReal), dimension(4,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
orientation ! crystal orientation in quaternions
|
|
|
|
!* output variables
|
|
|
|
!* local variables
|
|
integer(pInt) Nneighbors, & ! number of neighbors
|
|
n, & ! neighbor index
|
|
neighboring_e, & ! element index of my neighbor
|
|
neighboring_i, & ! integration point index of my neighbor
|
|
my_phase, &
|
|
neighboring_phase, &
|
|
my_texture, &
|
|
neighboring_texture, &
|
|
my_structure, & ! lattice structure
|
|
my_instance, & ! instance of plasticity
|
|
ns, & ! number of active slip systems
|
|
s1, & ! slip system index (me)
|
|
s2 ! slip system index (my neighbor)
|
|
real(pReal), dimension(4) :: absoluteMisorientation ! absolute misorientation (without symmetry) between me and my neighbor
|
|
real(pReal), dimension(2,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(1,i,e))),&
|
|
constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(1,i,e))),&
|
|
FE_NipNeighbors(mesh_element(2,e))) :: &
|
|
compatibility ! compatibility for current element and ip
|
|
real(pReal), dimension(3,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(1,i,e)))) :: &
|
|
slipNormal, &
|
|
slipDirection
|
|
real(pReal) compatibilitySum, &
|
|
thresholdValue, &
|
|
nThresholdValues
|
|
logical, dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(1,i,e)))) :: &
|
|
belowThreshold
|
|
|
|
|
|
Nneighbors = FE_NipNeighbors(mesh_element(2,e))
|
|
my_phase = material_phase(1,i,e)
|
|
my_texture = material_texture(1,i,e)
|
|
my_instance = phase_plasticityInstance(my_phase)
|
|
my_structure = constitutive_nonlocal_structure(my_instance)
|
|
ns = constitutive_nonlocal_totalNslip(my_instance)
|
|
slipNormal(1:3,1:ns) = lattice_sn(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,my_instance), my_structure)
|
|
slipDirection(1:3,1:ns) = lattice_sd(1:3, constitutive_nonlocal_slipSystemLattice(1:ns,my_instance), my_structure)
|
|
|
|
|
|
!*** start out fully compatible
|
|
|
|
compatibility = 0.0_pReal
|
|
forall(s1 = 1_pInt:ns) &
|
|
compatibility(1:2,s1,s1,1:Nneighbors) = 1.0_pReal
|
|
|
|
|
|
!*** Loop thrugh neighbors and check whether there is any compatibility.
|
|
|
|
do n = 1_pInt,Nneighbors
|
|
neighboring_e = mesh_ipNeighborhood(1,n,i,e)
|
|
neighboring_i = mesh_ipNeighborhood(2,n,i,e)
|
|
|
|
|
|
!* FREE SURFACE
|
|
!* Set surface transmissivity to the value specified in the material.config
|
|
|
|
if (neighboring_e <= 0_pInt .or. neighboring_i <= 0_pInt) then
|
|
forall(s1 = 1_pInt:ns) &
|
|
compatibility(1:2,s1,s1,n) = sqrt(constitutive_nonlocal_surfaceTransmissivity(my_instance))
|
|
cycle
|
|
endif
|
|
|
|
|
|
!* PHASE BOUNDARY
|
|
!* If we encounter a different nonlocal "cpfem" phase at the neighbor,
|
|
!* we consider this to be a real "physical" phase boundary, so completely incompatible.
|
|
!* If the neighboring "cpfem" phase has a local plasticity,
|
|
!* we do not consider this to be a phase boundary, so completely compatible.
|
|
|
|
neighboring_phase = material_phase(1,neighboring_i,neighboring_e)
|
|
if (neighboring_phase /= my_phase) then
|
|
if (.not. phase_localPlasticity(neighboring_phase)) then
|
|
forall(s1 = 1_pInt:ns) &
|
|
compatibility(1:2,s1,s1,n) = 0.0_pReal ! = sqrt(0.0)
|
|
endif
|
|
cycle
|
|
endif
|
|
|
|
|
|
!* GRAIN BOUNDARY !
|
|
!* fixed transmissivity for adjacent ips with different texture (only if explicitly given in material.config)
|
|
|
|
if (constitutive_nonlocal_grainboundaryTransmissivity(my_instance) >= 0.0_pReal) then
|
|
neighboring_texture = material_texture(1,neighboring_i,neighboring_e)
|
|
if (neighboring_texture /= my_texture) then
|
|
if (.not. phase_localPlasticity(neighboring_phase)) then
|
|
forall(s1 = 1_pInt:ns) &
|
|
compatibility(1:2,s1,s1,n) = sqrt(constitutive_nonlocal_grainboundaryTransmissivity(my_instance))
|
|
endif
|
|
cycle
|
|
endif
|
|
|
|
!* GRAIN BOUNDARY ?
|
|
!* Compatibility defined by relative orientation of slip systems:
|
|
!* The compatibility value is defined as the product of the slip normal projection and the slip direction projection.
|
|
!* Its sign is always positive for screws, for edges it has the same sign as the slip normal projection.
|
|
!* Since the sum for each slip system can easily exceed one (which would result in a transmissivity larger than one),
|
|
!* only values above or equal to a certain threshold value are considered. This threshold value is chosen, such that
|
|
!* the number of compatible slip systems is minimized with the sum of the original compatibility values exceeding one.
|
|
!* Finally the smallest compatibility value is decreased until the sum is exactly equal to one.
|
|
!* All values below the threshold are set to zero.
|
|
else
|
|
absoluteMisorientation = math_QuaternionDisorientation(orientation(1:4,1,i,e), &
|
|
orientation(1:4,1,neighboring_i,neighboring_e), &
|
|
0_pInt) ! no symmetry
|
|
do s1 = 1_pInt,ns ! my slip systems
|
|
do s2 = 1_pInt,ns ! my neighbor's slip systems
|
|
compatibility(1,s2,s1,n) = math_mul3x3(slipNormal(1:3,s1), math_qRot(absoluteMisorientation, slipNormal(1:3,s2))) &
|
|
* abs(math_mul3x3(slipDirection(1:3,s1), math_qRot(absoluteMisorientation, slipDirection(1:3,s2))))
|
|
compatibility(2,s2,s1,n) = abs(math_mul3x3(slipNormal(1:3,s1), math_qRot(absoluteMisorientation, slipNormal(1:3,s2)))) &
|
|
* abs(math_mul3x3(slipDirection(1:3,s1), math_qRot(absoluteMisorientation, slipDirection(1:3,s2))))
|
|
enddo
|
|
|
|
compatibilitySum = 0.0_pReal
|
|
belowThreshold = .true.
|
|
do while (compatibilitySum < 1.0_pReal .and. any(belowThreshold(1:ns)))
|
|
thresholdValue = maxval(compatibility(2,1:ns,s1,n), belowThreshold(1:ns)) ! screws always positive
|
|
nThresholdValues = real(count(compatibility(2,1:ns,s1,n) == thresholdValue),pReal)
|
|
where (compatibility(2,1:ns,s1,n) >= thresholdValue) &
|
|
belowThreshold(1:ns) = .false.
|
|
if (compatibilitySum + thresholdValue * nThresholdValues > 1.0_pReal) &
|
|
where (abs(compatibility(1:2,1:ns,s1,n)) == thresholdValue) &
|
|
compatibility(1:2,1:ns,s1,n) = sign((1.0_pReal - compatibilitySum) / nThresholdValues, compatibility(1:2,1:ns,s1,n))
|
|
compatibilitySum = compatibilitySum + nThresholdValues * thresholdValue
|
|
enddo
|
|
where (belowThreshold(1:ns)) compatibility(1,1:ns,s1,n) = 0.0_pReal
|
|
where (belowThreshold(1:ns)) compatibility(2,1:ns,s1,n) = 0.0_pReal
|
|
enddo ! my slip systems cycle
|
|
endif
|
|
|
|
enddo ! neighbor cycle
|
|
|
|
constitutive_nonlocal_compatibility(1:2,1:ns,1:ns,1:Nneighbors,i,e) = compatibility
|
|
|
|
endsubroutine
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* rate of change of temperature *
|
|
!*********************************************************************
|
|
pure function constitutive_nonlocal_dotTemperature(Tstar_v,Temperature,state,g,ip,el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips
|
|
use material, only: homogenization_maxNgrains
|
|
implicit none
|
|
|
|
!* input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain ID
|
|
ip, & ! current integration point
|
|
el ! current element
|
|
real(pReal), intent(in) :: Temperature ! temperature
|
|
real(pReal), dimension(6), intent(in) :: Tstar_v ! 2nd Piola-Kirchhoff stress in Mandel notation
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
state ! microstructural state
|
|
|
|
!* output variables
|
|
real(pReal) constitutive_nonlocal_dotTemperature ! evolution of Temperature
|
|
|
|
!* local variables
|
|
|
|
constitutive_nonlocal_dotTemperature = 0.0_pReal
|
|
|
|
endfunction
|
|
|
|
|
|
|
|
|
|
!*********************************************************************
|
|
!* calculates quantities characterizing the microstructure *
|
|
!*********************************************************************
|
|
function constitutive_nonlocal_dislocationstress(state, Fe, g, ip, el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use math, only: math_mul33x33, &
|
|
math_mul33x3, &
|
|
math_invert33, &
|
|
math_transpose33, &
|
|
pi
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips, &
|
|
mesh_element, &
|
|
mesh_node0, &
|
|
FE_Nips, &
|
|
mesh_ipCenterOfGravity, &
|
|
mesh_ipVolume, &
|
|
mesh_periodicSurface
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_localPlasticity, &
|
|
phase_plasticityInstance
|
|
|
|
implicit none
|
|
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain ID
|
|
ip, & ! current integration point
|
|
el ! current element
|
|
real(pReal), dimension(3,3,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
Fe ! elastic deformation gradient
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
state ! microstructural state
|
|
|
|
!*** input/output variables
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(3,3) :: constitutive_nonlocal_dislocationstress
|
|
|
|
!*** local variables
|
|
integer(pInt) neighboring_el, & ! element number of neighboring material point
|
|
neighboring_ip, & ! integration point of neighboring material point
|
|
instance, & ! my instance of this plasticity
|
|
neighboring_instance, & ! instance of this plasticity of neighboring material point
|
|
latticeStruct, & ! my lattice structure
|
|
neighboring_latticeStruct, & ! lattice structure of neighboring material point
|
|
phase, &
|
|
neighboring_phase, &
|
|
ns, & ! total number of active slip systems at my material point
|
|
neighboring_ns, & ! total number of active slip systems at neighboring material point
|
|
c, & ! index of dilsocation character (edge, screw)
|
|
s, & ! slip system index
|
|
t, & ! index of dilsocation type (e+, e-, s+, s-, used e+, used e-, used s+, used s-)
|
|
dir, &
|
|
deltaX, deltaY, deltaZ, &
|
|
side, &
|
|
j
|
|
integer(pInt), dimension(2,3) :: periodicImages
|
|
real(pReal) nu, & ! poisson's ratio
|
|
x, y, z, & ! coordinates of connection vector in neighboring lattice frame
|
|
xsquare, ysquare, zsquare, & ! squares of respective coordinates
|
|
distance, & ! length of connection vector
|
|
segmentLength, & ! segment length of dislocations
|
|
lambda, &
|
|
R, Rsquare, Rcube, &
|
|
denominator, &
|
|
flipSign, &
|
|
neighboring_ipVolumeSideLength, &
|
|
detFe
|
|
real(pReal), dimension(3) :: connection, & ! connection vector between me and my neighbor in the deformed configuration
|
|
connection_neighboringLattice, & ! connection vector between me and my neighbor in the lattice configuration of my neighbor
|
|
connection_neighboringSlip, & ! connection vector between me and my neighbor in the slip system frame of my neighbor
|
|
maxCoord, minCoord, &
|
|
meshSize, &
|
|
ipCoords, &
|
|
neighboring_ipCoords
|
|
real(pReal), dimension(3,3) :: sigma, & ! dislocation stress for one slip system in neighboring material point's slip system frame
|
|
Tdislo_neighboringLattice, & ! dislocation stress as 2nd Piola-Kirchhoff stress at neighboring material point
|
|
invFe, & ! inverse of my elastic deformation gradient
|
|
neighboring_invFe, &
|
|
neighboringLattice2myLattice ! mapping from neighboring MPs lattice configuration to my lattice configuration
|
|
real(pReal), dimension(2,2,maxval(constitutive_nonlocal_totalNslip)) :: &
|
|
neighboring_rhoExcess ! excess density at neighboring material point (edge/screw,mobile/dead,slipsystem)
|
|
real(pReal), dimension(2,maxval(constitutive_nonlocal_totalNslip)) :: &
|
|
rhoExcessDead
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),8) :: &
|
|
rhoSgl ! single dislocation density (edge+, edge-, screw+, screw-, used edge+, used edge-, used screw+, used screw-)
|
|
logical inversionError
|
|
|
|
phase = material_phase(g,ip,el)
|
|
instance = phase_plasticityInstance(phase)
|
|
latticeStruct = constitutive_nonlocal_structure(instance)
|
|
ns = constitutive_nonlocal_totalNslip(instance)
|
|
|
|
|
|
|
|
!*** get basic states
|
|
|
|
forall (s = 1_pInt:ns, t = 1_pInt:4_pInt) &
|
|
rhoSgl(s,t) = max(state(g,ip,el)%p((t-1_pInt)*ns+s), 0.0_pReal) ! ensure positive single mobile densities
|
|
forall (t = 5_pInt:8_pInt) &
|
|
rhoSgl(1:ns,t) = state(g,ip,el)%p((t-1_pInt)*ns+1_pInt:t*ns)
|
|
|
|
|
|
|
|
!*** calculate the dislocation stress of the neighboring excess dislocation densities
|
|
!*** zero for material points of local plasticity
|
|
|
|
constitutive_nonlocal_dislocationstress = 0.0_pReal
|
|
|
|
if (.not. phase_localPlasticity(phase)) then
|
|
call math_invert33(Fe(1:3,1:3,g,ip,el), invFe, detFe, inversionError)
|
|
! if (inversionError) then
|
|
! return
|
|
! endif
|
|
|
|
!* in case of periodic surfaces we have to find out how many periodic images in each direction we need
|
|
|
|
do dir = 1_pInt,3_pInt
|
|
maxCoord(dir) = maxval(mesh_node0(dir,:))
|
|
minCoord(dir) = minval(mesh_node0(dir,:))
|
|
enddo
|
|
meshSize = maxCoord - minCoord
|
|
ipCoords = mesh_ipCenterOfGravity(1:3,ip,el)
|
|
periodicImages = 0_pInt
|
|
do dir = 1_pInt,3_pInt
|
|
if (mesh_periodicSurface(dir)) then
|
|
periodicImages(1,dir) = floor((ipCoords(dir) - constitutive_nonlocal_R(instance) - minCoord(dir)) / meshSize(dir), pInt)
|
|
periodicImages(2,dir) = ceiling((ipCoords(dir) + constitutive_nonlocal_R(instance) - maxCoord(dir)) / meshSize(dir), pInt)
|
|
endif
|
|
enddo
|
|
|
|
|
|
!* loop through all material points (also through their periodic images if present),
|
|
!* but only consider nonlocal neighbors within a certain cutoff radius R
|
|
|
|
do neighboring_el = 1_pInt,mesh_NcpElems
|
|
ipLoop: do neighboring_ip = 1_pInt,FE_Nips(mesh_element(2,neighboring_el))
|
|
neighboring_phase = material_phase(g,neighboring_ip,neighboring_el)
|
|
if (phase_localPlasticity(neighboring_phase)) then
|
|
cycle
|
|
endif
|
|
neighboring_instance = phase_plasticityInstance(neighboring_phase)
|
|
neighboring_latticeStruct = constitutive_nonlocal_structure(neighboring_instance)
|
|
neighboring_ns = constitutive_nonlocal_totalNslip(neighboring_instance)
|
|
call math_invert33(Fe(1:3,1:3,1,neighboring_ip,neighboring_el), neighboring_invFe, detFe, inversionError)
|
|
! if (inversionError) then
|
|
! return
|
|
! endif
|
|
neighboring_ipVolumeSideLength = mesh_ipVolume(neighboring_ip,neighboring_el) ** (1.0_pReal/3.0_pReal) ! reference volume used here
|
|
forall (s = 1_pInt:neighboring_ns, c = 1_pInt:2_pInt) &
|
|
neighboring_rhoExcess(c,1,s) = state(g,neighboring_ip,neighboring_el)%p((2_pInt*c-2_pInt)*neighboring_ns+s) & ! positive mobiles
|
|
- state(g,neighboring_ip,neighboring_el)%p((2_pInt*c-1_pInt)*neighboring_ns+s) ! negative mobiles
|
|
forall (s = 1_pInt:neighboring_ns, c = 1_pInt:2_pInt) &
|
|
neighboring_rhoExcess(c,2,s) = abs(state(g,neighboring_ip,neighboring_el)%p((2_pInt*c+2_pInt)*neighboring_ns+s)) & ! positive deads
|
|
- abs(state(g,neighboring_ip,neighboring_el)%p((2_pInt*c+3_pInt)*neighboring_ns+s)) ! negative deads
|
|
nu = constitutive_nonlocal_nu(neighboring_instance)
|
|
Tdislo_neighboringLattice = 0.0_pReal
|
|
do deltaX = periodicImages(1,1),periodicImages(2,1)
|
|
do deltaY = periodicImages(1,2),periodicImages(2,2)
|
|
do deltaZ = periodicImages(1,3),periodicImages(2,3)
|
|
|
|
|
|
!* regular case
|
|
|
|
if (neighboring_el /= el .or. neighboring_ip /= ip &
|
|
.or. deltaX /= 0_pInt .or. deltaY /= 0_pInt .or. deltaZ /= 0_pInt) then
|
|
|
|
neighboring_ipCoords = mesh_ipCenterOfGravity(1:3,neighboring_ip,neighboring_el) &
|
|
+ (/real(deltaX,pReal), real(deltaY,pReal), real(deltaZ,pReal)/) * meshSize
|
|
connection = neighboring_ipCoords - ipCoords
|
|
distance = sqrt(sum(connection * connection))
|
|
if (distance > constitutive_nonlocal_R(instance)) then
|
|
cycle
|
|
endif
|
|
|
|
|
|
!* the segment length is the minimum of the third root of the control volume and the ip distance
|
|
!* this ensures, that the central MP never sits on a neighboring dislocation segment
|
|
|
|
connection_neighboringLattice = math_mul33x3(neighboring_invFe, connection)
|
|
segmentLength = min(neighboring_ipVolumeSideLength, distance)
|
|
|
|
|
|
!* loop through all slip systems of the neighboring material point
|
|
!* and add up the stress contributions from egde and screw excess on these slip systems (if significant)
|
|
|
|
do s = 1_pInt,neighboring_ns
|
|
if (all(abs(neighboring_rhoExcess(:,:,s)) < constitutive_nonlocal_aTolRho(instance))) then
|
|
cycle ! not significant
|
|
endif
|
|
|
|
|
|
!* map the connection vector from the lattice into the slip system frame
|
|
|
|
connection_neighboringSlip = math_mul33x3(constitutive_nonlocal_lattice2slip(1:3,1:3,s,neighboring_instance), &
|
|
connection_neighboringLattice)
|
|
|
|
|
|
!* edge contribution to stress
|
|
sigma = 0.0_pReal
|
|
|
|
x = connection_neighboringSlip(1)
|
|
y = connection_neighboringSlip(2)
|
|
z = connection_neighboringSlip(3)
|
|
xsquare = x * x
|
|
ysquare = y * y
|
|
zsquare = z * z
|
|
|
|
do j = 1_pInt,2_pInt
|
|
if (abs(neighboring_rhoExcess(1,j,s)) < constitutive_nonlocal_aTolRho(instance)) then
|
|
cycle
|
|
elseif (j > 1_pInt) then
|
|
x = connection_neighboringSlip(1) + sign(0.5_pReal * segmentLength, &
|
|
state(g,neighboring_ip,neighboring_el)%p(4*neighboring_ns+s) &
|
|
- state(g,neighboring_ip,neighboring_el)%p(5*neighboring_ns+s))
|
|
xsquare = x * x
|
|
endif
|
|
|
|
flipSign = sign(1.0_pReal, -y)
|
|
do side = 1_pInt,-1_pInt,-2_pInt
|
|
lambda = real(side,pReal) * 0.5_pReal * segmentLength - y
|
|
R = sqrt(xsquare + zsquare + lambda * lambda)
|
|
Rsquare = R * R
|
|
Rcube = Rsquare * R
|
|
denominator = R * (R + flipSign * lambda)
|
|
if (denominator == 0.0_pReal) then
|
|
exit ipLoop
|
|
endif
|
|
|
|
sigma(1,1) = sigma(1,1) - real(side,pReal) * flipSign * z / denominator &
|
|
* (1.0_pReal + xsquare / Rsquare + xsquare / denominator) &
|
|
* neighboring_rhoExcess(1,j,s)
|
|
sigma(2,2) = sigma(2,2) - real(side,pReal) * (flipSign * 2.0_pReal * nu * z / denominator + z * lambda / Rcube)&
|
|
* neighboring_rhoExcess(1,j,s)
|
|
sigma(3,3) = sigma(3,3) + real(side,pReal) * flipSign * z / denominator &
|
|
* (1.0_pReal - zsquare / Rsquare - zsquare / denominator) &
|
|
* neighboring_rhoExcess(1,j,s)
|
|
sigma(1,2) = sigma(1,2) + real(side,pReal) * x * z / Rcube * neighboring_rhoExcess(1,j,s)
|
|
sigma(1,3) = sigma(1,3) + real(side,pReal) * flipSign * x / denominator &
|
|
* (1.0_pReal - zsquare / Rsquare - zsquare / denominator) &
|
|
* neighboring_rhoExcess(1,j,s)
|
|
sigma(2,3) = sigma(2,3) - real(side,pReal) * (nu / R - zsquare / Rcube) * neighboring_rhoExcess(1,j,s)
|
|
enddo
|
|
enddo
|
|
|
|
!* screw contribution to stress
|
|
|
|
x = connection_neighboringSlip(1) ! have to restore this value, because position might have been adapted for edge deads before
|
|
do j = 1_pInt,2_pInt
|
|
if (abs(neighboring_rhoExcess(2,j,s)) < constitutive_nonlocal_aTolRho(instance)) then
|
|
cycle
|
|
elseif (j > 1_pInt) then
|
|
y = connection_neighboringSlip(2) + sign(0.5_pReal * segmentLength, &
|
|
state(g,neighboring_ip,neighboring_el)%p(6_pInt*neighboring_ns+s) &
|
|
- state(g,neighboring_ip,neighboring_el)%p(7_pInt*neighboring_ns+s))
|
|
ysquare = y * y
|
|
endif
|
|
|
|
flipSign = sign(1.0_pReal, x)
|
|
do side = 1_pInt,-1_pInt,-2_pInt
|
|
lambda = x + real(side,pReal) * 0.5_pReal * segmentLength
|
|
R = sqrt(ysquare + zsquare + lambda * lambda)
|
|
Rsquare = R * R
|
|
Rcube = Rsquare * R
|
|
denominator = R * (R + flipSign * lambda)
|
|
if (denominator == 0.0_pReal) then
|
|
exit ipLoop
|
|
endif
|
|
|
|
sigma(1,2) = sigma(1,2) - real(side,pReal) * flipSign * z * (1.0_pReal - nu) / denominator &
|
|
* neighboring_rhoExcess(2,j,s)
|
|
sigma(1,3) = sigma(1,3) + real(side,pReal) * flipSign * y * (1.0_pReal - nu) / denominator &
|
|
* neighboring_rhoExcess(2,j,s)
|
|
enddo
|
|
enddo
|
|
|
|
if (all(abs(sigma) < 1.0e-10_pReal)) then ! SIGMA IS NOT A REAL STRESS, THATS WHY WE NEED A REALLY SMALL VALUE HERE
|
|
cycle
|
|
endif
|
|
|
|
!* copy symmetric parts
|
|
|
|
sigma(2,1) = sigma(1,2)
|
|
sigma(3,1) = sigma(1,3)
|
|
sigma(3,2) = sigma(2,3)
|
|
|
|
|
|
!* scale stresses and map them into the neighboring material point's lattice configuration
|
|
|
|
sigma = sigma * constitutive_nonlocal_Gmod(neighboring_instance) &
|
|
* constitutive_nonlocal_burgers(s,neighboring_instance) &
|
|
/ (4.0_pReal * pi * (1.0_pReal - nu)) &
|
|
* mesh_ipVolume(neighboring_ip,neighboring_el) / segmentLength ! reference volume is used here (according to the segment length calculation)
|
|
Tdislo_neighboringLattice = Tdislo_neighboringLattice &
|
|
+ math_mul33x33(math_transpose33(constitutive_nonlocal_lattice2slip(1:3,1:3,s,neighboring_instance)), &
|
|
math_mul33x33(sigma, constitutive_nonlocal_lattice2slip(1:3,1:3,s,neighboring_instance)))
|
|
|
|
enddo ! slip system loop
|
|
|
|
|
|
!* special case of central ip volume
|
|
!* only consider dead dislocations
|
|
!* we assume that they all sit at a distance equal to half the third root of V
|
|
!* in direction of the according slip direction
|
|
|
|
else
|
|
|
|
forall (s = 1_pInt:ns, c = 1_pInt:2_pInt) &
|
|
rhoExcessDead(c,s) = state(g,ip,el)%p((2_pInt*c+2_pInt)*ns+s) & ! positive deads (here we use symmetry: if this has negative sign it is treated as negative density at positive position instead of positive density at negative position)
|
|
+ state(g,ip,el)%p((2_pInt*c+3_pInt)*ns+s) ! negative deads (here we use symmetry: if this has negative sign it is treated as positive density at positive position instead of negative density at negative position)
|
|
|
|
do s = 1_pInt,ns
|
|
if (all(abs(rhoExcessDead(:,s)) < constitutive_nonlocal_aTolRho(instance))) then
|
|
cycle ! not significant
|
|
endif
|
|
sigma = 0.0_pReal ! all components except for sigma13 are zero
|
|
sigma(1,3) = - (rhoExcessDead(1,s) + rhoExcessDead(2,s) * (1.0_pReal - nu)) * neighboring_ipVolumeSideLength &
|
|
* constitutive_nonlocal_Gmod(instance) * constitutive_nonlocal_burgers(s,instance) &
|
|
/ (sqrt(2.0_pReal) * pi * (1.0_pReal - nu))
|
|
sigma(3,1) = sigma(1,3)
|
|
|
|
Tdislo_neighboringLattice = Tdislo_neighboringLattice &
|
|
+ math_mul33x33(math_transpose33(constitutive_nonlocal_lattice2slip(1:3,1:3,s,instance)), &
|
|
math_mul33x33(sigma, constitutive_nonlocal_lattice2slip(1:3,1:3,s,instance)))
|
|
|
|
enddo ! slip system loop
|
|
|
|
endif
|
|
|
|
enddo ! deltaZ loop
|
|
enddo ! deltaY loop
|
|
enddo ! deltaX loop
|
|
|
|
|
|
!* map the stress from the neighboring MP's lattice configuration into the deformed configuration
|
|
!* and back into my lattice configuration
|
|
|
|
neighboringLattice2myLattice = math_mul33x33(invFe, Fe(1:3,1:3,1,neighboring_ip,neighboring_el))
|
|
constitutive_nonlocal_dislocationstress = constitutive_nonlocal_dislocationstress &
|
|
+ math_mul33x33(neighboringLattice2myLattice, &
|
|
math_mul33x33(Tdislo_neighboringLattice, &
|
|
math_transpose33(neighboringLattice2myLattice)))
|
|
|
|
enddo ipLoop
|
|
enddo ! element loop
|
|
|
|
endif
|
|
|
|
endfunction
|
|
|
|
|
|
!*********************************************************************
|
|
!* return array of constitutive results *
|
|
!*********************************************************************
|
|
function constitutive_nonlocal_postResults(Tstar_v, Fe, Temperature, dt, state, dotState, g,ip,el)
|
|
|
|
use prec, only: pReal, &
|
|
pInt, &
|
|
p_vec
|
|
use math, only: math_mul6x6, &
|
|
math_mul33x3, &
|
|
math_mul33x33, &
|
|
pi
|
|
use mesh, only: mesh_NcpElems, &
|
|
mesh_maxNips
|
|
use material, only: homogenization_maxNgrains, &
|
|
material_phase, &
|
|
phase_plasticityInstance, &
|
|
phase_Noutput
|
|
use lattice, only: lattice_Sslip_v, &
|
|
lattice_sd, &
|
|
lattice_st
|
|
|
|
implicit none
|
|
|
|
!*** input variables
|
|
integer(pInt), intent(in) :: g, & ! current grain number
|
|
ip, & ! current integration point
|
|
el ! current element number
|
|
real(pReal), intent(in) :: Temperature, & ! temperature
|
|
dt ! time increment
|
|
real(pReal), dimension(6), intent(in) :: Tstar_v ! current 2nd Piola-Kirchhoff stress in Mandel notation
|
|
real(pReal), dimension(3,3,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
Fe ! elastic deformation gradient
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
state ! current microstructural state
|
|
type(p_vec), intent(in) :: dotState ! evolution rate of microstructural state
|
|
|
|
!*** output variables
|
|
real(pReal), dimension(constitutive_nonlocal_sizePostResults(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
constitutive_nonlocal_postResults
|
|
|
|
!*** local variables
|
|
integer(pInt) myInstance, & ! current instance of this plasticity
|
|
myStructure, & ! current lattice structure
|
|
ns, & ! short notation for the total number of active slip systems
|
|
c, & ! character of dislocation
|
|
cs, & ! constitutive result index
|
|
o, & ! index of current output
|
|
t, & ! type of dislocation
|
|
s, & ! index of my current slip system
|
|
sLattice ! index of my current slip system according to lattice order
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),8) :: &
|
|
rhoSgl, & ! current single dislocation densities (positive/negative screw and edge without dipoles)
|
|
rhoDotSgl ! evolution rate of single dislocation densities (positive/negative screw and edge without dipoles)
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),4) :: &
|
|
gdot, & ! shear rates
|
|
v ! velocities
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el)))) :: &
|
|
rhoForest, & ! forest dislocation density
|
|
tauThreshold, & ! threshold shear stress
|
|
tau, & ! current resolved shear stress
|
|
tauBack, & ! back stress from pileups on same slip system
|
|
vClimb ! climb velocity of edge dipoles
|
|
real(pReal), dimension(constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
rhoDip, & ! current dipole dislocation densities (screw and edge dipoles)
|
|
rhoDotDip, & ! evolution rate of dipole dislocation densities (screw and edge dipoles)
|
|
dLower, & ! minimum stable dipole distance for edges and screws
|
|
dUpper ! current maximum stable dipole distance for edges and screws
|
|
real(pReal), dimension(3,constitutive_nonlocal_totalNslip(phase_plasticityInstance(material_phase(g,ip,el))),2) :: &
|
|
m, & ! direction of dislocation motion for edge and screw (unit vector)
|
|
m_currentconf ! direction of dislocation motion for edge and screw (unit vector) in current configuration
|
|
real(pReal) D ! self diffusion
|
|
real(pReal), dimension(3,3) :: sigma
|
|
|
|
myInstance = phase_plasticityInstance(material_phase(g,ip,el))
|
|
myStructure = constitutive_nonlocal_structure(myInstance)
|
|
ns = constitutive_nonlocal_totalNslip(myInstance)
|
|
|
|
cs = 0_pInt
|
|
constitutive_nonlocal_postResults = 0.0_pReal
|
|
|
|
|
|
!* short hand notations for state variables
|
|
|
|
forall (t = 1_pInt:8_pInt) rhoSgl(1:ns,t) = state(g,ip,el)%p((t-1_pInt)*ns+1_pInt:t*ns)
|
|
forall (c = 1_pInt:2_pInt) rhoDip(1:ns,c) = state(g,ip,el)%p((7_pInt+c)*ns+1_pInt:(8_pInt+c)*ns)
|
|
rhoForest = state(g,ip,el)%p(10_pInt*ns+1:11_pInt*ns)
|
|
tauThreshold = state(g,ip,el)%p(11_pInt*ns+1:12_pInt*ns)
|
|
tauBack = state(g,ip,el)%p(12_pInt*ns+1:13_pInt*ns)
|
|
forall (t = 1_pInt:8_pInt) rhoDotSgl(1:ns,t) = dotState%p((t-1_pInt)*ns+1_pInt:t*ns)
|
|
forall (c = 1_pInt:2_pInt) rhoDotDip(1:ns,c) = dotState%p((7_pInt+c)*ns+1_pInt:(8_pInt+c)*ns)
|
|
forall (t = 1_pInt:4_pInt) v(1:ns,t) = state(g,ip,el)%p((12_pInt+t)*ns+1_pInt:(13_pInt+t)*ns)
|
|
|
|
|
|
!* Calculate shear rate
|
|
|
|
do t = 1_pInt,4_pInt
|
|
do s = 1_pInt,ns
|
|
if (rhoSgl(s,t+4_pInt) * v(s,t) < 0.0_pReal) then
|
|
rhoSgl(s,t) = rhoSgl(s,t) + abs(rhoSgl(s,t+4_pInt)) ! remobilization of immobile singles for changing sign of v (bauschinger effect)
|
|
rhoSgl(s,t+4_pInt) = 0.0_pReal ! remobilization of immobile singles for changing sign of v (bauschinger effect)
|
|
endif
|
|
enddo
|
|
enddo
|
|
|
|
forall (t = 1_pInt:4_pInt) &
|
|
gdot(1:ns,t) = rhoSgl(1:ns,t) * constitutive_nonlocal_burgers(1:ns,myInstance) * v(1:ns,t)
|
|
|
|
|
|
!* calculate limits for stable dipole height
|
|
|
|
do s = 1_pInt,ns
|
|
sLattice = constitutive_nonlocal_slipSystemLattice(s,myInstance)
|
|
tau(s) = math_mul6x6(Tstar_v, lattice_Sslip_v(1:6,sLattice,myStructure)) + tauBack(s)
|
|
enddo
|
|
|
|
dLower = constitutive_nonlocal_minimumDipoleHeight(1:ns,1:2,myInstance)
|
|
dUpper(1:ns,1) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (8.0_pReal * pi * (1.0_pReal - constitutive_nonlocal_nu(myInstance)) * abs(tau))
|
|
dUpper(1:ns,2) = constitutive_nonlocal_Gmod(myInstance) * constitutive_nonlocal_burgers(1:ns,myInstance) &
|
|
/ (4.0_pReal * pi * abs(tau))
|
|
forall (c = 1_pInt:2_pInt) &
|
|
dUpper(1:ns,c) = min(1.0_pReal / sqrt(sum(abs(rhoSgl),c) + sum(rhoDip,c)), dUpper(1:ns,c))
|
|
dUpper = max(dUpper,dLower)
|
|
|
|
|
|
!*** dislocation motion
|
|
|
|
m(1:3,1:ns,1) = lattice_sd(1:3,constitutive_nonlocal_slipSystemLattice(1:ns,myInstance),myStructure)
|
|
m(1:3,1:ns,2) = -lattice_st(1:3,constitutive_nonlocal_slipSystemLattice(1:ns,myInstance),myStructure)
|
|
forall (c = 1_pInt:2_pInt, s = 1_pInt:ns) &
|
|
m_currentconf(1:3,s,c) = math_mul33x3(Fe, m(1:3,s,c))
|
|
|
|
|
|
do o = 1_pInt,phase_Noutput(material_phase(g,ip,el))
|
|
select case(constitutive_nonlocal_output(o,myInstance))
|
|
|
|
case ('rho')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl),2) + sum(rhoDip,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl(1:ns,1:4)),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoSgl(1:ns,5:8),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dip')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoDip,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl(1:ns,(/1,2,5,6/))),2) + rhoDip(1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl(1:ns,(/1,2,5,6/))),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoSgl(1:ns,1:2),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoSgl(1:ns,5:6),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_pos')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,1) + abs(rhoSgl(1:ns,5))
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_pos_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_pos_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,5)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_neg')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,2) + abs(rhoSgl(1:ns,6))
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_neg_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_edge_neg_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,6)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dip_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoDip(1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('rho_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl(1:ns,(/3,4,7,8/))),2) + rhoDip(1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(abs(rhoSgl(1:ns,(/3,4,7,8/))),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoSgl(1:ns,3:4),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoSgl(1:ns,7:8),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_pos')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,3) + abs(rhoSgl(1:ns,7))
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_pos_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,3)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_pos_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,7)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_neg')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,4) + abs(rhoSgl(1:ns,8))
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_neg_mobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,4)
|
|
cs = cs + ns
|
|
|
|
case ('rho_sgl_screw_neg_immobile')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,8)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dip_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoDip(1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('excess_rho')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = (rhoSgl(1:ns,1) + abs(rhoSgl(1:ns,5))) &
|
|
- (rhoSgl(1:ns,2) + abs(rhoSgl(1:ns,6))) &
|
|
+ (rhoSgl(1:ns,3) + abs(rhoSgl(1:ns,7))) &
|
|
- (rhoSgl(1:ns,4) + abs(rhoSgl(1:ns,8)))
|
|
cs = cs + ns
|
|
|
|
case ('excess_rho_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = (rhoSgl(1:ns,1) + abs(rhoSgl(1:ns,5))) &
|
|
- (rhoSgl(1:ns,2) + abs(rhoSgl(1:ns,6)))
|
|
cs = cs + ns
|
|
|
|
case ('excess_rho_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = (rhoSgl(1:ns,3) + abs(rhoSgl(1:ns,7))) &
|
|
- (rhoSgl(1:ns,4) + abs(rhoSgl(1:ns,8)))
|
|
cs = cs + ns
|
|
|
|
case ('rho_forest')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoForest
|
|
cs = cs + ns
|
|
|
|
case ('delta')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = 1.0_pReal / sqrt(sum(abs(rhoSgl),2) + sum(rhoDip,2))
|
|
cs = cs + ns
|
|
|
|
case ('delta_sgl')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = 1.0_pReal / sqrt(sum(abs(rhoSgl),2))
|
|
cs = cs + ns
|
|
|
|
case ('delta_dip')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = 1.0_pReal / sqrt(sum(rhoDip,2))
|
|
cs = cs + ns
|
|
|
|
case ('shearrate')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(gdot,2)
|
|
cs = cs + ns
|
|
|
|
case ('resolvedstress')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = tau
|
|
cs = cs + ns
|
|
|
|
case ('resolvedstress_back')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = tauBack
|
|
cs = cs + ns
|
|
|
|
case ('resolvedstress_external')
|
|
do s = 1_pInt,ns
|
|
sLattice = constitutive_nonlocal_slipSystemLattice(s,myInstance)
|
|
constitutive_nonlocal_postResults(cs+s) = math_mul6x6(Tstar_v, lattice_Sslip_v(1:6,sLattice,myStructure))
|
|
enddo
|
|
cs = cs + ns
|
|
|
|
case ('resistance')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = tauThreshold
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoDotSgl,2) + sum(rhoDotDip,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_sgl')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoDotSgl,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_dip')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(rhoDotDip,2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_gen')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotMultiplication(1:ns,1,g,ip,el) &
|
|
+ constitutive_nonlocal_rhoDotMultiplication(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_gen_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotMultiplication(1:ns,1,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_gen_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotMultiplication(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_sgl2dip')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotSingle2DipoleGlide(1:ns,1,g,ip,el) &
|
|
+ constitutive_nonlocal_rhoDotSingle2DipoleGlide(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_ann_ath')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotAthermalAnnihilation(1:ns,1,g,ip,el) &
|
|
+ constitutive_nonlocal_rhoDotAthermalAnnihilation(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_ann_the')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotThermalAnnihilation(1:ns,1,g,ip,el) &
|
|
+ constitutive_nonlocal_rhoDotThermalAnnihilation(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_ann_the_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotThermalAnnihilation(1:ns,1,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_ann_the_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotThermalAnnihilation(1:ns,2,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_edgejogs')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_rhoDotEdgeJogs(1:ns,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_flux')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(constitutive_nonlocal_rhoDotFlux(1:ns,1:4,g,ip,el),2) &
|
|
+ sum(abs(constitutive_nonlocal_rhoDotFlux(1:ns,5:8,g,ip,el)),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_flux_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(constitutive_nonlocal_rhoDotFlux(1:ns,1:2,g,ip,el),2) &
|
|
+ sum(abs(constitutive_nonlocal_rhoDotFlux(1:ns,5:6,g,ip,el)),2)
|
|
cs = cs + ns
|
|
|
|
case ('rho_dot_flux_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = sum(constitutive_nonlocal_rhoDotFlux(1:ns,3:4,g,ip,el),2) &
|
|
+ sum(abs(constitutive_nonlocal_rhoDotFlux(1:ns,7:8,g,ip,el)),2)
|
|
cs = cs + ns
|
|
|
|
case ('velocity_edge_pos')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = v(1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('velocity_edge_neg')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = v(1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('velocity_screw_pos')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = v(1:ns,3)
|
|
cs = cs + ns
|
|
|
|
case ('velocity_screw_neg')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = v(1:ns,4)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_pos_x')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,1) * v(1:ns,1) * m_currentconf(1,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_pos_y')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,1) * v(1:ns,1) * m_currentconf(2,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_pos_z')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,1) * v(1:ns,1) * m_currentconf(3,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_neg_x')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,2) * v(1:ns,2) * m_currentconf(1,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_neg_y')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,2) * v(1:ns,2) * m_currentconf(2,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_edge_neg_z')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,2) * v(1:ns,2) * m_currentconf(3,1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_pos_x')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,3) * v(1:ns,3) * m_currentconf(1,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_pos_y')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,3) * v(1:ns,3) * m_currentconf(2,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_pos_z')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = rhoSgl(1:ns,3) * v(1:ns,3) * m_currentconf(3,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_neg_x')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,4) * v(1:ns,4) * m_currentconf(1,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_neg_y')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,4) * v(1:ns,4) * m_currentconf(2,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('fluxdensity_screw_neg_z')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = - rhoSgl(1:ns,4) * v(1:ns,4) * m_currentconf(3,1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case ('maximumdipoleheight_edge')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = dUpper(1:ns,1)
|
|
cs = cs + ns
|
|
|
|
case ('maximumdipoleheight_screw')
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = dUpper(1:ns,2)
|
|
cs = cs + ns
|
|
|
|
case('dislocationstress')
|
|
sigma = constitutive_nonlocal_dislocationstress(state, Fe, g, ip, el)
|
|
constitutive_nonlocal_postResults(cs+1_pInt) = sigma(1,1)
|
|
constitutive_nonlocal_postResults(cs+2_pInt) = sigma(2,2)
|
|
constitutive_nonlocal_postResults(cs+3_pInt) = sigma(3,3)
|
|
constitutive_nonlocal_postResults(cs+4_pInt) = sigma(1,2)
|
|
constitutive_nonlocal_postResults(cs+5_pInt) = sigma(2,3)
|
|
constitutive_nonlocal_postResults(cs+6_pInt) = sigma(3,1)
|
|
cs = cs + 6_pInt
|
|
|
|
case('accumulatedshear')
|
|
constitutive_nonlocal_accumulatedShear(1:ns,g,ip,el) = constitutive_nonlocal_accumulatedShear(1:ns,g,ip,el) + sum(gdot,2)*dt
|
|
constitutive_nonlocal_postResults(cs+1_pInt:cs+ns) = constitutive_nonlocal_accumulatedShear(1:ns,g,ip,el)
|
|
cs = cs + ns
|
|
|
|
end select
|
|
enddo
|
|
|
|
endfunction
|
|
|
|
END MODULE
|