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!--------------------------------------------------------------------------------------------------
!> @author Christoph Kords, Max-Planck-Institut für Eisenforschung GmbH
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @brief material subroutine for plasticity including dislocation flux
!--------------------------------------------------------------------------------------------------
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module plastic_nonlocal
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use prec
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use IO
use math
use debug
use material
use lattice
use rotations
use config
use lattice
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use discretization
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use geometry_plastic_nonlocal , only : &
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nIPneighbors = > geometry_plastic_nonlocal_nIPneighbors , &
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IPneighborhood = > geometry_plastic_nonlocal_IPneighborhood , &
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IPvolume = > geometry_plastic_nonlocal_IPvolume0 , &
IParea = > geometry_plastic_nonlocal_IParea0 , &
IPareaNormal = > geometry_plastic_nonlocal_IPareaNormal0
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implicit none
private
real ( pReal ) , parameter , private :: &
KB = 1.38e-23_pReal !< Physical parameter, Boltzmann constant in J/Kelvin
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integer , dimension ( : , : ) , allocatable , target , public :: &
plastic_nonlocal_sizePostResult !< size of each post result output
character ( len = 64 ) , dimension ( : , : ) , allocatable , target , public :: &
plastic_nonlocal_output !< name of each post result output
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! storage order of dislocation types
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integer , dimension ( 8 ) , parameter :: &
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sgl = [ 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 ] !< signed (single)
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integer , dimension ( 5 ) , parameter :: &
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edg = [ 1 , 2 , 5 , 6 , 9 ] , & !< edge
scr = [ 3 , 4 , 7 , 8 , 10 ] !< screw
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integer , dimension ( 4 ) , parameter :: &
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mob = [ 1 , 2 , 3 , 4 ] , & !< mobile
imm = [ 5 , 6 , 7 , 8 ] !< immobile (blocked)
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integer , dimension ( 2 ) , parameter :: &
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dip = [ 9 , 10 ] , & !< dipole
imm_edg = imm ( 1 : 2 ) , & !< immobile edge
imm_scr = imm ( 3 : 4 ) !< immobile screw
integer , parameter :: &
mob_edg_pos = 1 , & !< mobile edge positive
mob_edg_neg = 2 , & !< mobile edge negative
mob_scr_pos = 3 , & !< mobile screw positive
mob_scr_neg = 4 !< mobile screw positive
! BEGIN DEPRECATES
integer , dimension ( : , : , : ) , allocatable , private :: &
iRhoU , & !< state indices for unblocked density
iRhoB , & !< state indices for blocked density
iRhoD , & !< state indices for dipole density
iV , & !< state indices for dislcation velocities
iD !< state indices for stable dipole height
integer , dimension ( : ) , allocatable , private , protected :: &
totalNslip !< total number of active slip systems for each instance
!END DEPRECATED
real ( pReal ) , dimension ( : , : , : , : , : , : ) , allocatable , private :: &
compatibility !< slip system compatibility between me and my neighbors
enum , bind ( c )
enumerator :: &
undefined_ID , &
rho_sgl_mob_edg_pos_ID , &
rho_sgl_mob_edg_neg_ID , &
rho_sgl_mob_scr_pos_ID , &
rho_sgl_mob_scr_neg_ID , &
rho_sgl_imm_edg_pos_ID , &
rho_sgl_imm_edg_neg_ID , &
rho_sgl_imm_scr_pos_ID , &
rho_sgl_imm_scr_neg_ID , &
rho_dip_edg_ID , &
rho_dip_scr_ID , &
rho_forest_ID , &
resolvedstress_back_ID , &
resistance_ID , &
rho_dot_sgl_ID , &
rho_dot_sgl_mobile_ID , &
rho_dot_dip_ID , &
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v_edg_pos_ID , &
v_edg_neg_ID , &
v_scr_pos_ID , &
v_scr_neg_ID , &
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accumulatedshear_ID
end enum
type , private :: tParameters !< container type for internal constitutive parameters
real ( pReal ) :: &
atomicVolume , & !< atomic volume
Dsd0 , & !< prefactor for self-diffusion coefficient
selfDiffusionEnergy , & !< activation enthalpy for diffusion
aTolRho , & !< absolute tolerance for dislocation density in state integration
aTolShear , & !< absolute tolerance for accumulated shear in state integration
significantRho , & !< density considered significant
significantN , & !< number of dislocations considered significant
doublekinkwidth , & !< width of a doubkle kink in multiples of the burgers vector length b
solidSolutionEnergy , & !< activation energy for solid solution in J
solidSolutionSize , & !< solid solution obstacle size in multiples of the burgers vector length
solidSolutionConcentration , & !< concentration of solid solution in atomic parts
p , & !< parameter for kinetic law (Kocks,Argon,Ashby)
q , & !< parameter for kinetic law (Kocks,Argon,Ashby)
viscosity , & !< viscosity for dislocation glide in Pa s
fattack , & !< attack frequency in Hz
rhoSglScatter , & !< standard deviation of scatter in initial dislocation density
surfaceTransmissivity , & !< transmissivity at free surface
grainboundaryTransmissivity , & !< transmissivity at grain boundary (identified by different texture)
CFLfactor , & !< safety factor for CFL flux condition
fEdgeMultiplication , & !< factor that determines how much edge dislocations contribute to multiplication (0...1)
rhoSglRandom , &
rhoSglRandomBinning , &
linetensionEffect , &
edgeJogFactor , &
mu , &
nu
real ( pReal ) , dimension ( : ) , allocatable :: &
minDipoleHeight_edge , & !< minimum stable edge dipole height
minDipoleHeight_screw , & !< minimum stable screw dipole height
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peierlsstress_edge , &
peierlsstress_screw , &
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rhoSglEdgePos0 , & !< initial edge_pos dislocation density
rhoSglEdgeNeg0 , & !< initial edge_neg dislocation density
rhoSglScrewPos0 , & !< initial screw_pos dislocation density
rhoSglScrewNeg0 , & !< initial screw_neg dislocation density
rhoDipEdge0 , & !< initial edge dipole dislocation density
rhoDipScrew0 , & !< initial screw dipole dislocation density
lambda0 , & !< mean free path prefactor for each
burgers !< absolute length of burgers vector [m]
real ( pReal ) , dimension ( : , : ) , allocatable :: &
slip_normal , &
slip_direction , &
slip_transverse , &
minDipoleHeight , & ! edge and screw
peierlsstress , & ! edge and screw
interactionSlipSlip , & !< coefficients for slip-slip interaction
forestProjection_Edge , & !< matrix of forest projections of edge dislocations
forestProjection_Screw !< matrix of forest projections of screw dislocations
real ( pReal ) , dimension ( : ) , allocatable , private :: &
nonSchmidCoeff
real ( pReal ) , dimension ( : , : , : ) , allocatable , private :: &
Schmid , & !< Schmid contribution
nonSchmid_pos , &
nonSchmid_neg !< combined projection of Schmid and non-Schmid contributions to the resolved shear stress (only for screws)
integer :: &
totalNslip
integer , dimension ( : ) , allocatable , public :: &
Nslip , &
colinearSystem !< colinear system to the active slip system (only valid for fcc!)
logical , private :: &
shortRangeStressCorrection , & !< flag indicating the use of the short range stress correction by a excess density gradient term
probabilisticMultiplication
integer ( kind ( undefined_ID ) ) , dimension ( : ) , allocatable :: &
outputID !< ID of each post result output
end type tParameters
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type , private :: tNonlocalMicrostructure
real ( pReal ) , allocatable , dimension ( : , : ) :: &
tau_Threshold , &
tau_Back
end type tNonlocalMicrostructure
type , private :: tNonlocalState
real ( pReal ) , pointer , dimension ( : , : ) :: &
rho , & ! < all dislocations
rhoSgl , &
rhoSglMobile , & ! iRhoU
rho_sgl_mob_edg_pos , &
rho_sgl_mob_edg_neg , &
rho_sgl_mob_scr_pos , &
rho_sgl_mob_scr_neg , &
rhoSglImmobile , & ! iRhoB
rho_sgl_imm_edg_pos , &
rho_sgl_imm_edg_neg , &
rho_sgl_imm_scr_pos , &
rho_sgl_imm_scr_neg , &
rhoDip , & ! iRhoD
rho_dip_edg , &
rho_dip_scr , &
rho_forest , &
accumulatedshear , &
v
end type tNonlocalState
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type ( tNonlocalState ) , allocatable , dimension ( : ) , private :: &
deltaState , &
dotState , &
state
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type ( tParameters ) , dimension ( : ) , allocatable , private :: param !< containers of constitutive parameters (len Ninstance)
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type ( tNonlocalMicrostructure ) , dimension ( : ) , allocatable , private :: microstructure
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integer ( kind ( undefined_ID ) ) , dimension ( : , : ) , allocatable , private :: &
plastic_nonlocal_outputID !< ID of each post result output
public :: &
plastic_nonlocal_init , &
plastic_nonlocal_dependentState , &
plastic_nonlocal_LpAndItsTangent , &
plastic_nonlocal_dotState , &
plastic_nonlocal_deltaState , &
plastic_nonlocal_updateCompatibility , &
plastic_nonlocal_postResults , &
plastic_nonlocal_results
private :: &
plastic_nonlocal_kinetics
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contains
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!--------------------------------------------------------------------------------------------------
!> @brief module initialization
!> @details reads in material parameters, allocates arrays, and does sanity checks
!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_init
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character ( len = 65536 ) , dimension ( 0 ) , parameter :: emptyStringArray = [ character ( len = 65536 ) :: ]
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integer , dimension ( 0 ) , parameter :: emptyIntArray = [ integer :: ]
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real ( pReal ) , dimension ( 0 ) , parameter :: emptyRealArray = [ real ( pReal ) :: ]
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integer :: &
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sizeState , sizeDotState , sizeDependentState , sizeDeltaState , &
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maxNinstances , &
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p , i , &
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l , &
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s1 , s2 , &
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s , &
t , &
c
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integer ( kind ( undefined_ID ) ) :: &
outputID
character ( len = 512 ) :: &
extmsg = '' , &
structure
character ( len = 65536 ) , dimension ( : ) , allocatable :: outputs
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integer :: NofMyPhase
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write ( 6 , '(/,a)' ) ' <<<+- constitutive_' / / PLASTICITY_NONLOCAL_label / / ' init -+>>>'
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write ( 6 , '(/,a)' ) ' Reuber et al., Acta Materialia 71:333–
write ( 6 , '(a)' ) ' https://doi.org/10.1016/j.actamat.2014.03.012'
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write ( 6 , '(/,a)' ) ' Kords, Dissertation RWTH Aachen, 2014'
write ( 6 , '(a)' ) ' http://publications.rwth-aachen.de/record/229993'
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maxNinstances = count ( phase_plasticity == PLASTICITY_NONLOCAL_ID )
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelBasic ) / = 0 ) &
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write ( 6 , '(a16,1x,i5,/)' ) '# instances:' , maxNinstances
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allocate ( param ( maxNinstances ) )
allocate ( state ( maxNinstances ) )
allocate ( dotState ( maxNinstances ) )
allocate ( deltaState ( maxNinstances ) )
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allocate ( microstructure ( maxNinstances ) )
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allocate ( plastic_nonlocal_sizePostResult ( maxval ( phase_Noutput ) , maxNinstances ) , source = 0 )
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allocate ( plastic_nonlocal_output ( maxval ( phase_Noutput ) , maxNinstances ) )
plastic_nonlocal_output = ''
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allocate ( plastic_nonlocal_outputID ( maxval ( phase_Noutput ) , maxNinstances ) , source = undefined_ID )
allocate ( totalNslip ( maxNinstances ) , source = 0 )
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do p = 1 , size ( config_phase )
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if ( phase_plasticity ( p ) / = PLASTICITY_NONLOCAL_ID ) cycle
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associate ( prm = > param ( phase_plasticityInstance ( p ) ) , &
dot = > dotState ( phase_plasticityInstance ( p ) ) , &
stt = > state ( phase_plasticityInstance ( p ) ) , &
del = > deltaState ( phase_plasticityInstance ( p ) ) , &
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dst = > microstructure ( phase_plasticityInstance ( p ) ) , &
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config = > config_phase ( p ) )
prm % aTolRho = config % getFloat ( 'atol_rho' , defaultVal = 0.0_pReal )
prm % aTolShear = config % getFloat ( 'atol_shear' , defaultVal = 0.0_pReal )
structure = config % getString ( 'lattice_structure' )
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! This data is read in already in lattice
prm % mu = lattice_mu ( p )
prm % nu = lattice_nu ( p )
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prm % Nslip = config % getInts ( 'nslip' , defaultVal = emptyIntArray )
prm % totalNslip = sum ( prm % Nslip )
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slipActive : if ( prm % totalNslip > 0 ) then
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prm % Schmid = lattice_SchmidMatrix_slip ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
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if ( trim ( config % getString ( 'lattice_structure' ) ) == 'bcc' ) then
prm % nonSchmidCoeff = config % getFloats ( 'nonschmid_coefficients' , &
defaultVal = emptyRealArray )
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prm % nonSchmid_pos = lattice_nonSchmidMatrix ( prm % Nslip , prm % nonSchmidCoeff , + 1 )
prm % nonSchmid_neg = lattice_nonSchmidMatrix ( prm % Nslip , prm % nonSchmidCoeff , - 1 )
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else
prm % nonSchmid_pos = prm % Schmid
prm % nonSchmid_neg = prm % Schmid
endif
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prm % interactionSlipSlip = lattice_interaction_SlipBySlip ( prm % Nslip , &
config % getFloats ( 'interaction_slipslip' ) , &
config % getString ( 'lattice_structure' ) )
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prm % forestProjection_edge = lattice_forestProjection_edge ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
prm % forestProjection_screw = lattice_forestProjection_screw ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
prm % slip_direction = lattice_slip_direction ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
prm % slip_transverse = lattice_slip_transverse ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
prm % slip_normal = lattice_slip_normal ( prm % Nslip , config % getString ( 'lattice_structure' ) , &
config % getFloat ( 'c/a' , defaultVal = 0.0_pReal ) )
! collinear systems (only for octahedral slip systems in fcc)
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allocate ( prm % colinearSystem ( prm % totalNslip ) , source = - 1 )
do s1 = 1 , prm % totalNslip
do s2 = 1 , prm % totalNslip
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if ( all ( dEq0 ( math_cross ( prm % slip_direction ( 1 : 3 , s1 ) , prm % slip_direction ( 1 : 3 , s2 ) ) ) ) . and . &
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any ( dNeq0 ( math_cross ( prm % slip_normal ( 1 : 3 , s1 ) , prm % slip_normal ( 1 : 3 , s2 ) ) ) ) ) &
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prm % colinearSystem ( s1 ) = s2
enddo
enddo
prm % rhoSglEdgePos0 = config % getFloats ( 'rhosgledgepos0' , requiredSize = size ( prm % Nslip ) )
prm % rhoSglEdgeNeg0 = config % getFloats ( 'rhosgledgeneg0' , requiredSize = size ( prm % Nslip ) )
prm % rhoSglScrewPos0 = config % getFloats ( 'rhosglscrewpos0' , requiredSize = size ( prm % Nslip ) )
prm % rhoSglScrewNeg0 = config % getFloats ( 'rhosglscrewneg0' , requiredSize = size ( prm % Nslip ) )
prm % rhoDipEdge0 = config % getFloats ( 'rhodipedge0' , requiredSize = size ( prm % Nslip ) )
prm % rhoDipScrew0 = config % getFloats ( 'rhodipscrew0' , requiredSize = size ( prm % Nslip ) )
prm % lambda0 = config % getFloats ( 'lambda0' , requiredSize = size ( prm % Nslip ) )
prm % burgers = config % getFloats ( 'burgers' , requiredSize = size ( prm % Nslip ) )
prm % lambda0 = math_expand ( prm % lambda0 , prm % Nslip )
prm % burgers = math_expand ( prm % burgers , prm % Nslip )
prm % minDipoleHeight_edge = config % getFloats ( 'minimumdipoleheightedge' , requiredSize = size ( prm % Nslip ) )
prm % minDipoleHeight_screw = config % getFloats ( 'minimumdipoleheightscrew' , requiredSize = size ( prm % Nslip ) )
prm % minDipoleHeight_edge = math_expand ( prm % minDipoleHeight_edge , prm % Nslip )
prm % minDipoleHeight_screw = math_expand ( prm % minDipoleHeight_screw , prm % Nslip )
allocate ( prm % minDipoleHeight ( prm % totalNslip , 2 ) )
prm % minDipoleHeight ( : , 1 ) = prm % minDipoleHeight_edge
prm % minDipoleHeight ( : , 2 ) = prm % minDipoleHeight_screw
prm % peierlsstress_edge = config % getFloats ( 'peierlsstressedge' , requiredSize = size ( prm % Nslip ) )
prm % peierlsstress_screw = config % getFloats ( 'peierlsstressscrew' , requiredSize = size ( prm % Nslip ) )
prm % peierlsstress_edge = math_expand ( prm % peierlsstress_edge , prm % Nslip )
prm % peierlsstress_screw = math_expand ( prm % peierlsstress_screw , prm % Nslip )
allocate ( prm % peierlsstress ( prm % totalNslip , 2 ) )
prm % peierlsstress ( : , 1 ) = prm % peierlsstress_edge
prm % peierlsstress ( : , 2 ) = prm % peierlsstress_screw
prm % significantRho = config % getFloat ( 'significantrho' )
prm % significantN = config % getFloat ( 'significantn' , 0.0_pReal )
prm % CFLfactor = config % getFloat ( 'cflfactor' , defaultVal = 2.0_pReal )
prm % atomicVolume = config % getFloat ( 'atomicvolume' )
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prm % Dsd0 = config % getFloat ( 'selfdiffusionprefactor' ) !,'dsd0'
prm % selfDiffusionEnergy = config % getFloat ( 'selfdiffusionenergy' ) !,'qsd'
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prm % linetensionEffect = config % getFloat ( 'linetension' )
prm % edgeJogFactor = config % getFloat ( 'edgejog' ) !,'edgejogs'
prm % doublekinkwidth = config % getFloat ( 'doublekinkwidth' )
prm % solidSolutionEnergy = config % getFloat ( 'solidsolutionenergy' )
prm % solidSolutionSize = config % getFloat ( 'solidsolutionsize' )
prm % solidSolutionConcentration = config % getFloat ( 'solidsolutionconcentration' )
prm % p = config % getFloat ( 'p' )
prm % q = config % getFloat ( 'q' )
prm % viscosity = config % getFloat ( 'viscosity' )
prm % fattack = config % getFloat ( 'attackfrequency' )
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! ToDo: discuss logic
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prm % rhoSglScatter = config % getFloat ( 'rhosglscatter' )
prm % rhoSglRandom = config % getFloat ( 'rhosglrandom' , 0.0_pReal )
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if ( config % keyExists ( '/rhosglrandom/' ) ) &
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prm % rhoSglRandomBinning = config % getFloat ( 'rhosglrandombinning' , 0.0_pReal ) !ToDo: useful default?
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! if (rhoSglRandom(instance) < 0.0_pReal) &
! if (rhoSglRandomBinning(instance) <= 0.0_pReal) &
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prm % surfaceTransmissivity = config % getFloat ( 'surfacetransmissivity' , defaultVal = 1.0_pReal )
prm % grainboundaryTransmissivity = config % getFloat ( 'grainboundarytransmissivity' , defaultVal = - 1.0_pReal )
prm % fEdgeMultiplication = config % getFloat ( 'edgemultiplication' )
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prm % shortRangeStressCorrection = config % keyExists ( '/shortrangestresscorrection/' )
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!--------------------------------------------------------------------------------------------------
! sanity checks
if ( any ( prm % burgers < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' burgers'
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if ( any ( prm % lambda0 < = 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' lambda0'
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if ( any ( prm % rhoSglEdgePos0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoSglEdgePos0'
if ( any ( prm % rhoSglEdgeNeg0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoSglEdgeNeg0'
if ( any ( prm % rhoSglScrewPos0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoSglScrewPos0'
if ( any ( prm % rhoSglScrewNeg0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoSglScrewNeg0'
if ( any ( prm % rhoDipEdge0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoDipEdge0'
if ( any ( prm % rhoDipScrew0 < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' rhoDipScrew0'
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if ( any ( prm % peierlsstress < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' peierlsstress'
if ( any ( prm % minDipoleHeight < 0.0_pReal ) ) extmsg = trim ( extmsg ) / / ' minDipoleHeight'
if ( prm % viscosity < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' viscosity'
if ( prm % selfDiffusionEnergy < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' selfDiffusionEnergy'
if ( prm % fattack < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' fattack'
if ( prm % doublekinkwidth < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' doublekinkwidth'
if ( prm % Dsd0 < 0.0_pReal ) extmsg = trim ( extmsg ) / / ' Dsd0'
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if ( prm % atomicVolume < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' atomicVolume' ! ToDo: in disloUCLA/dislotwin, the atomic volume is given as a factor
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if ( prm % significantN < 0.0_pReal ) extmsg = trim ( extmsg ) / / ' significantN'
if ( prm % significantrho < 0.0_pReal ) extmsg = trim ( extmsg ) / / ' significantrho'
if ( prm % atolshear < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' atolshear'
if ( prm % atolrho < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' atolrho'
if ( prm % CFLfactor < 0.0_pReal ) extmsg = trim ( extmsg ) / / ' CFLfactor'
if ( prm % p < = 0.0_pReal . or . prm % p > 1.0_pReal ) extmsg = trim ( extmsg ) / / ' p'
if ( prm % q < 1.0_pReal . or . prm % q > 2.0_pReal ) extmsg = trim ( extmsg ) / / ' q'
if ( prm % linetensionEffect < 0.0_pReal . or . prm % linetensionEffect > 1.0_pReal ) &
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extmsg = trim ( extmsg ) / / ' linetensionEffect'
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if ( prm % edgeJogFactor < 0.0_pReal . or . prm % edgeJogFactor > 1.0_pReal ) &
extmsg = trim ( extmsg ) / / ' edgeJogFactor'
if ( prm % solidSolutionEnergy < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' solidSolutionEnergy'
if ( prm % solidSolutionSize < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' solidSolutionSize'
if ( prm % solidSolutionConcentration < = 0.0_pReal ) extmsg = trim ( extmsg ) / / ' solidSolutionConcentration'
if ( prm % grainboundaryTransmissivity > 1.0_pReal ) extmsg = trim ( extmsg ) / / ' grainboundaryTransmissivity'
if ( prm % surfaceTransmissivity < 0.0_pReal . or . prm % surfaceTransmissivity > 1.0_pReal ) &
extmsg = trim ( extmsg ) / / ' surfaceTransmissivity'
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if ( prm % fEdgeMultiplication < 0.0_pReal . or . prm % fEdgeMultiplication > 1.0_pReal ) &
extmsg = trim ( extmsg ) / / ' fEdgeMultiplication'
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endif slipActive
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outputs = config % getStrings ( '(output)' , defaultVal = emptyStringArray )
allocate ( prm % outputID ( 0 ) )
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do i = 1 , size ( outputs )
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outputID = undefined_ID
select case ( trim ( outputs ( i ) ) )
case ( 'rho_sgl_edge_pos_mobile' )
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outputID = merge ( rho_sgl_mob_edg_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_edge_neg_mobile' )
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outputID = merge ( rho_sgl_mob_edg_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_screw_pos_mobile' )
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outputID = merge ( rho_sgl_mob_scr_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_screw_neg_mobile' )
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outputID = merge ( rho_sgl_mob_scr_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_edge_pos_immobile' )
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outputID = merge ( rho_sgl_imm_edg_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_edge_neg_immobile' )
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outputID = merge ( rho_sgl_imm_edg_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_screw_pos_immobile' )
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outputID = merge ( rho_sgl_imm_scr_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_sgl_screw_neg_immobile' )
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outputID = merge ( rho_sgl_imm_scr_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_dip_edge' )
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outputID = merge ( rho_dip_edg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_dip_screw' )
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outputID = merge ( rho_dip_scr_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_forest' )
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outputID = merge ( rho_forest_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'resolvedstress_back' )
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outputID = merge ( resolvedstress_back_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'resistance' )
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outputID = merge ( resistance_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_dot_sgl' )
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outputID = merge ( rho_dot_sgl_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_dot_sgl_mobile' )
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outputID = merge ( rho_dot_sgl_mobile_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'rho_dot_dip' )
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outputID = merge ( rho_dot_dip_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'velocity_edge_pos' )
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outputID = merge ( v_edg_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'velocity_edge_neg' )
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outputID = merge ( v_edg_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'velocity_screw_pos' )
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outputID = merge ( v_scr_pos_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'velocity_screw_neg' )
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outputID = merge ( v_scr_neg_ID , undefined_ID , prm % totalNslip > 0 )
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case ( 'accumulatedshear' , 'accumulated_shear' )
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outputID = merge ( accumulatedshear_ID , undefined_ID , prm % totalNslip > 0 )
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end select
if ( outputID / = undefined_ID ) then
plastic_nonlocal_output ( i , phase_plasticityInstance ( p ) ) = outputs ( i )
plastic_nonlocal_sizePostResult ( i , phase_plasticityInstance ( p ) ) = prm % totalNslip
prm % outputID = [ prm % outputID , outputID ]
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endif
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enddo
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!--------------------------------------------------------------------------------------------------
! allocate state arrays
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NofMyPhase = count ( material_phaseAt == p ) * discretization_nIP
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sizeDotState = size ( [ 'rhoSglEdgePosMobile ' , 'rhoSglEdgeNegMobile ' , &
'rhoSglScrewPosMobile ' , 'rhoSglScrewNegMobile ' , &
'rhoSglEdgePosImmobile ' , 'rhoSglEdgeNegImmobile ' , &
'rhoSglScrewPosImmobile' , 'rhoSglScrewNegImmobile' , &
'rhoDipEdge ' , 'rhoDipScrew ' , &
'accumulatedshear ' ] ) * prm % totalNslip !< "basic" microstructural state variables that are independent from other state variables
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sizeDependentState = size ( [ 'rhoForest ' ] ) * prm % totalNslip !< microstructural state variables that depend on other state variables
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sizeState = sizeDotState + sizeDependentState &
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+ size ( [ 'velocityEdgePos ' , 'velocityEdgeNeg ' , &
'velocityScrewPos ' , 'velocityScrewNeg ' , &
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'maxDipoleHeightEdge ' , 'maxDipoleHeightScrew' ] ) * prm % totalNslip !< other dependent state variables that are not updated by microstructure
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sizeDeltaState = sizeDotState
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call material_allocatePlasticState ( p , NofMyPhase , sizeState , sizeDotState , sizeDeltaState , &
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prm % totalNslip , 0 , 0 )
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plasticState ( p ) % nonlocal = . true .
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plasticState ( p ) % offsetDeltaState = 0 ! ToDo: state structure does not follow convention
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plasticState ( p ) % sizePostResults = sum ( plastic_nonlocal_sizePostResult ( : , phase_plasticityInstance ( p ) ) )
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totalNslip ( phase_plasticityInstance ( p ) ) = prm % totalNslip
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stt % rho = > plasticState ( p ) % state ( 0 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
dot % rho = > plasticState ( p ) % dotState ( 0 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
del % rho = > plasticState ( p ) % deltaState ( 0 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
plasticState ( p ) % aTolState ( 1 : 10 * prm % totalNslip ) = prm % aTolRho
stt % rhoSgl = > plasticState ( p ) % state ( 0 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
dot % rhoSgl = > plasticState ( p ) % dotState ( 0 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
del % rhoSgl = > plasticState ( p ) % deltaState ( 0 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
stt % rhoSglMobile = > plasticState ( p ) % state ( 0 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
dot % rhoSglMobile = > plasticState ( p ) % dotState ( 0 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
del % rhoSglMobile = > plasticState ( p ) % deltaState ( 0 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
stt % rho_sgl_mob_edg_pos = > plasticState ( p ) % state ( 0 * prm % totalNslip + 1 : 1 * prm % totalNslip , : )
dot % rho_sgl_mob_edg_pos = > plasticState ( p ) % dotState ( 0 * prm % totalNslip + 1 : 1 * prm % totalNslip , : )
del % rho_sgl_mob_edg_pos = > plasticState ( p ) % deltaState ( 0 * prm % totalNslip + 1 : 1 * prm % totalNslip , : )
stt % rho_sgl_mob_edg_neg = > plasticState ( p ) % state ( 1 * prm % totalNslip + 1 : 2 * prm % totalNslip , : )
dot % rho_sgl_mob_edg_neg = > plasticState ( p ) % dotState ( 1 * prm % totalNslip + 1 : 2 * prm % totalNslip , : )
del % rho_sgl_mob_edg_neg = > plasticState ( p ) % deltaState ( 1 * prm % totalNslip + 1 : 2 * prm % totalNslip , : )
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stt % rho_sgl_mob_scr_pos = > plasticState ( p ) % state ( 2 * prm % totalNslip + 1 : 3 * prm % totalNslip , : )
dot % rho_sgl_mob_scr_pos = > plasticState ( p ) % dotState ( 2 * prm % totalNslip + 1 : 3 * prm % totalNslip , : )
del % rho_sgl_mob_scr_pos = > plasticState ( p ) % deltaState ( 2 * prm % totalNslip + 1 : 3 * prm % totalNslip , : )
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stt % rho_sgl_mob_scr_neg = > plasticState ( p ) % state ( 3 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
dot % rho_sgl_mob_scr_neg = > plasticState ( p ) % dotState ( 3 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
del % rho_sgl_mob_scr_neg = > plasticState ( p ) % deltaState ( 3 * prm % totalNslip + 1 : 4 * prm % totalNslip , : )
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stt % rhoSglImmobile = > plasticState ( p ) % state ( 4 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
dot % rhoSglImmobile = > plasticState ( p ) % dotState ( 4 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
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del % rhoSglImmobile = > plasticState ( p ) % deltaState ( 4 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
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stt % rho_sgl_imm_edg_pos = > plasticState ( p ) % state ( 4 * prm % totalNslip + 1 : 5 * prm % totalNslip , : )
dot % rho_sgl_imm_edg_pos = > plasticState ( p ) % dotState ( 4 * prm % totalNslip + 1 : 5 * prm % totalNslip , : )
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del % rho_sgl_imm_edg_pos = > plasticState ( p ) % deltaState ( 4 * prm % totalNslip + 1 : 5 * prm % totalNslip , : )
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stt % rho_sgl_imm_edg_neg = > plasticState ( p ) % state ( 5 * prm % totalNslip + 1 : 6 * prm % totalNslip , : )
dot % rho_sgl_imm_edg_neg = > plasticState ( p ) % dotState ( 5 * prm % totalNslip + 1 : 6 * prm % totalNslip , : )
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del % rho_sgl_imm_edg_neg = > plasticState ( p ) % deltaState ( 5 * prm % totalNslip + 1 : 6 * prm % totalNslip , : )
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stt % rho_sgl_imm_scr_pos = > plasticState ( p ) % state ( 6 * prm % totalNslip + 1 : 7 * prm % totalNslip , : )
dot % rho_sgl_imm_scr_pos = > plasticState ( p ) % dotState ( 6 * prm % totalNslip + 1 : 7 * prm % totalNslip , : )
del % rho_sgl_imm_scr_pos = > plasticState ( p ) % deltaState ( 6 * prm % totalNslip + 1 : 7 * prm % totalNslip , : )
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stt % rho_sgl_imm_scr_neg = > plasticState ( p ) % state ( 7 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
dot % rho_sgl_imm_scr_neg = > plasticState ( p ) % dotState ( 7 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
del % rho_sgl_imm_scr_neg = > plasticState ( p ) % deltaState ( 7 * prm % totalNslip + 1 : 8 * prm % totalNslip , : )
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stt % rhoDip = > plasticState ( p ) % state ( 8 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
dot % rhoDip = > plasticState ( p ) % dotState ( 8 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
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del % rhoDip = > plasticState ( p ) % deltaState ( 8 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
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stt % rho_dip_edg = > plasticState ( p ) % state ( 8 * prm % totalNslip + 1 : 9 * prm % totalNslip , : )
dot % rho_dip_edg = > plasticState ( p ) % dotState ( 8 * prm % totalNslip + 1 : 9 * prm % totalNslip , : )
del % rho_dip_edg = > plasticState ( p ) % deltaState ( 8 * prm % totalNslip + 1 : 9 * prm % totalNslip , : )
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stt % rho_dip_scr = > plasticState ( p ) % state ( 9 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
dot % rho_dip_scr = > plasticState ( p ) % dotState ( 9 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
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del % rho_dip_scr = > plasticState ( p ) % deltaState ( 9 * prm % totalNslip + 1 : 10 * prm % totalNslip , : )
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stt % accumulatedshear = > plasticState ( p ) % state ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip , 1 : NofMyPhase )
dot % accumulatedshear = > plasticState ( p ) % dotState ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip , 1 : NofMyPhase )
del % accumulatedshear = > plasticState ( p ) % deltaState ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip , 1 : NofMyPhase )
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plasticState ( p ) % aTolState ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip ) = prm % aTolShear
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plasticState ( p ) % slipRate = > plasticState ( p ) % dotState ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip , 1 : NofMyPhase )
plasticState ( p ) % accumulatedSlip = > plasticState ( p ) % state ( 10 * prm % totalNslip + 1 : 11 * prm % totalNslip , 1 : NofMyPhase )
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stt % rho_forest = > plasticState ( p ) % state ( 11 * prm % totalNslip + 1 : 12 * prm % totalNslip , 1 : NofMyPhase )
stt % v = > plasticState ( p ) % state ( 12 * prm % totalNslip + 1 : 16 * prm % totalNslip , 1 : NofMyPhase )
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allocate ( dst % tau_Threshold ( prm % totalNslip , NofMyPhase ) , source = 0.0_pReal )
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allocate ( dst % tau_Back ( prm % totalNslip , NofMyPhase ) , source = 0.0_pReal )
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end associate
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if ( NofMyPhase > 0 ) call stateInit ( p , NofMyPhase )
plasticState ( p ) % state0 = plasticState ( p ) % state
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enddo
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allocate ( compatibility ( 2 , maxval ( totalNslip ) , maxval ( totalNslip ) , nIPneighbors , &
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discretization_nIP , discretization_nElem ) , source = 0.0_pReal )
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! BEGIN DEPRECATED----------------------------------------------------------------------------------
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allocate ( iRhoU ( maxval ( totalNslip ) , 4 , maxNinstances ) , source = 0 )
allocate ( iRhoB ( maxval ( totalNslip ) , 4 , maxNinstances ) , source = 0 )
allocate ( iRhoD ( maxval ( totalNslip ) , 2 , maxNinstances ) , source = 0 )
allocate ( iV ( maxval ( totalNslip ) , 4 , maxNinstances ) , source = 0 )
allocate ( iD ( maxval ( totalNslip ) , 2 , maxNinstances ) , source = 0 )
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initializeInstances : do p = 1 , size ( phase_plasticity )
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NofMyPhase = count ( material_phaseAt == p ) * discretization_nIP
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myPhase2 : if ( phase_plasticity ( p ) == PLASTICITY_NONLOCAL_ID ) then
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!*** determine indices to state array
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l = 0
do t = 1 , 4
do s = 1 , param ( phase_plasticityInstance ( p ) ) % totalNslip
l = l + 1
iRhoU ( s , t , phase_plasticityInstance ( p ) ) = l
enddo
enddo
do t = 1 , 4
do s = 1 , param ( phase_plasticityInstance ( p ) ) % totalNslip
l = l + 1
iRhoB ( s , t , phase_plasticityInstance ( p ) ) = l
enddo
enddo
do c = 1 , 2
do s = 1 , param ( phase_plasticityInstance ( p ) ) % totalNslip
l = l + 1
iRhoD ( s , c , phase_plasticityInstance ( p ) ) = l
enddo
enddo
l = l + param ( phase_plasticityInstance ( p ) ) % totalNslip ! shear(rates)
l = l + param ( phase_plasticityInstance ( p ) ) % totalNslip ! rho_forest
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do t = 1 , 4
do s = 1 , param ( phase_plasticityInstance ( p ) ) % totalNslip
l = l + 1
iV ( s , t , phase_plasticityInstance ( p ) ) = l
enddo
enddo
do c = 1 , 2
do s = 1 , param ( phase_plasticityInstance ( p ) ) % totalNslip
l = l + 1
iD ( s , c , phase_plasticityInstance ( p ) ) = l
enddo
enddo
if ( iD ( param ( phase_plasticityInstance ( p ) ) % totalNslip , 2 , phase_plasticityInstance ( p ) ) / = plasticState ( p ) % sizeState ) &
call IO_error ( 0 , ext_msg = 'state indices not properly set (' / / PLASTICITY_NONLOCAL_label / / ')' )
endif myPhase2
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enddo initializeInstances
! END DEPRECATED------------------------------------------------------------------------------------
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contains
!--------------------------------------------------------------------------------------------------
!> @brief populates the initial dislocation density
!--------------------------------------------------------------------------------------------------
subroutine stateInit ( phase , NofMyPhase )
integer , intent ( in ) :: &
phase , &
NofMyPhase
integer :: &
e , &
i , &
f , &
from , &
upto , &
s , &
instance , &
phasemember
real ( pReal ) , dimension ( 2 ) :: &
noise , &
rnd
real ( pReal ) :: &
meanDensity , &
totalVolume , &
densityBinning , &
minimumIpVolume
real ( pReal ) , dimension ( NofMyPhase ) :: &
volume
instance = phase_plasticityInstance ( phase )
associate ( prm = > param ( instance ) , stt = > state ( instance ) )
! randomly distribute dislocation segments on random slip system and of random type in the volume
if ( prm % rhoSglRandom > 0.0_pReal ) then
! get the total volume of the instance
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do e = 1 , discretization_nElem
do i = 1 , discretization_nIP
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if ( material_phaseAt ( 1 , e ) == phase ) volume ( material_phasememberAt ( 1 , i , e ) ) = IPvolume ( i , e )
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enddo
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enddo
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totalVolume = sum ( volume )
minimumIPVolume = minval ( volume )
densityBinning = prm % rhoSglRandomBinning / minimumIpVolume ** ( 2.0_pReal / 3.0_pReal )
! subsequently fill random ips with dislocation segments until we reach the desired overall density
meanDensity = 0.0_pReal
do while ( meanDensity < prm % rhoSglRandom )
call random_number ( rnd )
phasemember = nint ( rnd ( 1 ) * real ( NofMyPhase , pReal ) + 0.5_pReal )
s = nint ( rnd ( 2 ) * real ( prm % totalNslip , pReal ) * 4.0_pReal + 0.5_pReal )
meanDensity = meanDensity + densityBinning * volume ( phasemember ) / totalVolume
stt % rhoSglMobile ( s , phasemember ) = densityBinning
enddo
! homogeneous distribution of density with some noise
else
do e = 1 , NofMyPhase
do f = 1 , size ( prm % Nslip , 1 )
from = 1 + sum ( prm % Nslip ( 1 : f - 1 ) )
upto = sum ( prm % Nslip ( 1 : f ) )
do s = from , upto
noise = [ math_sampleGaussVar ( 0.0_pReal , prm % rhoSglScatter ) , &
math_sampleGaussVar ( 0.0_pReal , prm % rhoSglScatter ) ]
stt % rho_sgl_mob_edg_pos ( s , e ) = prm % rhoSglEdgePos0 ( f ) + noise ( 1 )
stt % rho_sgl_mob_edg_neg ( s , e ) = prm % rhoSglEdgeNeg0 ( f ) + noise ( 1 )
stt % rho_sgl_mob_scr_pos ( s , e ) = prm % rhoSglScrewPos0 ( f ) + noise ( 2 )
stt % rho_sgl_mob_scr_neg ( s , e ) = prm % rhoSglScrewNeg0 ( f ) + noise ( 2 )
enddo
stt % rho_dip_edg ( from : upto , e ) = prm % rhoDipEdge0 ( f )
stt % rho_dip_scr ( from : upto , e ) = prm % rhoDipScrew0 ( f )
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enddo
enddo
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endif
end associate
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end subroutine stateInit
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end subroutine plastic_nonlocal_init
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!--------------------------------------------------------------------------------------------------
!> @brief calculates quantities characterizing the microstructure
!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_dependentState ( Fe , Fp , ip , el )
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integer , intent ( in ) :: &
ip , &
el
real ( pReal ) , dimension ( 3 , 3 ) , intent ( in ) :: &
Fe , &
Fp
integer :: &
ph , & !< phase
of , & !< offset
no , & !< neighbor offset
ns , &
neighbor_el , & ! element number of neighboring material point
neighbor_ip , & ! integration point of neighboring material point
instance , & ! my instance of this plasticity
neighbor_instance , & ! instance of this plasticity of neighboring material point
c , & ! index of dilsocation character (edge, screw)
s , & ! slip system index
dir , &
n
real ( pReal ) :: &
FVsize , &
correction , &
nRealNeighbors ! number of really existing neighbors
integer , dimension ( 2 ) :: &
neighbors
real ( pReal ) , dimension ( 2 ) :: &
rhoExcessGradient , &
rhoExcessGradient_over_rho , &
rhoTotal
real ( pReal ) , dimension ( 3 ) :: &
rhoExcessDifferences , &
normal_latticeConf
real ( pReal ) , dimension ( 3 , 3 ) :: &
invFe , & !< inverse of elastic deformation gradient
invFp , & !< inverse of plastic deformation gradient
connections , &
invConnections
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real ( pReal ) , dimension ( 3 , nIPneighbors ) :: &
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connection_latticeConf
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real ( pReal ) , dimension ( 2 , totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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rhoExcess
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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rho_edg_delta , &
rho_scr_delta
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 10 ) :: &
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rho , &
rho_neighbor
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , &
totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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myInteractionMatrix ! corrected slip interaction matrix
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , nIPneighbors ) :: &
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rho_edg_delta_neighbor , &
rho_scr_delta_neighbor
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real ( pReal ) , dimension ( 2 , maxval ( totalNslip ) , nIPneighbors ) :: &
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neighbor_rhoExcess , & ! excess density at neighboring material point
neighbor_rhoTotal ! total density at neighboring material point
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real ( pReal ) , dimension ( 3 , totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 2 ) :: &
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m ! direction of dislocation motion
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ph = material_phaseAt ( 1 , el )
of = material_phasememberAt ( 1 , ip , el )
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instance = phase_plasticityInstance ( ph )
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associate ( prm = > param ( instance ) , dst = > microstructure ( instance ) , stt = > state ( instance ) )
ns = prm % totalNslip
rho = getRho ( instance , of , ip , el )
stt % rho_forest ( : , of ) = matmul ( prm % forestProjection_Edge , sum ( abs ( rho ( : , edg ) ) , 2 ) ) &
+ matmul ( prm % forestProjection_Screw , sum ( abs ( rho ( : , scr ) ) , 2 ) )
! coefficients are corrected for the line tension effect
! (see Kubin,Devincre,Hoc; 2008; Modeling dislocation storage rates and mean free paths in face-centered cubic crystals)
if ( lattice_structure ( ph ) == LATTICE_bcc_ID . or . lattice_structure ( ph ) == LATTICE_fcc_ID ) then ! only fcc and bcc
do s = 1 , ns
correction = ( 1.0_pReal - prm % linetensionEffect &
+ prm % linetensionEffect &
* log ( 0.35_pReal * prm % burgers ( s ) * sqrt ( max ( stt % rho_forest ( s , of ) , prm % significantRho ) ) ) &
/ log ( 0.35_pReal * prm % burgers ( s ) * 1e6_pReal ) ) ** 2.0_pReal
myInteractionMatrix ( 1 : ns , s ) = correction * prm % interactionSlipSlip ( 1 : ns , s )
enddo
else
myInteractionMatrix = prm % interactionSlipSlip
endif
forall ( s = 1 : ns ) &
dst % tau_threshold ( s , of ) = prm % mu * prm % burgers ( s ) &
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* sqrt ( dot_product ( sum ( abs ( rho ) , 2 ) , myInteractionMatrix ( 1 : ns , s ) ) )
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!*** calculate the dislocation stress of the neighboring excess dislocation densities
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!*** zero for material points of local plasticity
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!#################################################################################################
! ToDo: MD: this is most likely only correct for F_i = I
!#################################################################################################
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if ( . not . phase_localPlasticity ( ph ) . and . prm % shortRangeStressCorrection ) then
invFe = math_inv33 ( Fe )
invFp = math_inv33 ( Fp )
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rho_edg_delta = rho ( : , mob_edg_pos ) - rho ( : , mob_edg_neg )
rho_scr_delta = rho ( : , mob_scr_pos ) - rho ( : , mob_scr_neg )
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rhoExcess ( 1 , 1 : ns ) = rho_edg_delta
rhoExcess ( 2 , 1 : ns ) = rho_scr_delta
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FVsize = IPvolume ( ip , el ) ** ( 1.0_pReal / 3.0_pReal )
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!* loop through my neighborhood and get the connection vectors (in lattice frame) and the excess densities
nRealNeighbors = 0.0_pReal
neighbor_rhoTotal = 0.0_pReal
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do n = 1 , nIPneighbors
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neighbor_el = IPneighborhood ( 1 , n , ip , el )
neighbor_ip = IPneighborhood ( 2 , n , ip , el )
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no = material_phasememberAt ( 1 , neighbor_ip , neighbor_el )
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if ( neighbor_el > 0 . and . neighbor_ip > 0 ) then
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neighbor_instance = phase_plasticityInstance ( material_phaseAt ( 1 , neighbor_el ) )
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if ( neighbor_instance == instance ) then
nRealNeighbors = nRealNeighbors + 1.0_pReal
rho_neighbor = getRho ( instance , no , neighbor_ip , neighbor_el )
rho_edg_delta_neighbor ( : , n ) = rho_neighbor ( : , mob_edg_pos ) - rho_neighbor ( : , mob_edg_neg )
rho_scr_delta_neighbor ( : , n ) = rho_neighbor ( : , mob_scr_pos ) - rho_neighbor ( : , mob_scr_neg )
neighbor_rhoTotal ( 1 , : , n ) = sum ( abs ( rho_neighbor ( : , edg ) ) , 2 )
neighbor_rhoTotal ( 2 , : , n ) = sum ( abs ( rho_neighbor ( : , scr ) ) , 2 )
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connection_latticeConf ( 1 : 3 , n ) = matmul ( invFe , discretization_IPcoords ( 1 : 3 , neighbor_el + neighbor_ip - 1 ) &
- discretization_IPcoords ( 1 : 3 , el + neighbor_ip - 1 ) )
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normal_latticeConf = matmul ( transpose ( invFp ) , IPareaNormal ( 1 : 3 , n , ip , el ) )
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if ( math_inner ( normal_latticeConf , connection_latticeConf ( 1 : 3 , n ) ) < 0.0_pReal ) & ! neighboring connection points in opposite direction to face normal: must be periodic image
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connection_latticeConf ( 1 : 3 , n ) = normal_latticeConf * IPvolume ( ip , el ) / IParea ( n , ip , el ) ! instead take the surface normal scaled with the diameter of the cell
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else
! local neighbor or different lattice structure or different constitution instance -> use central values instead
connection_latticeConf ( 1 : 3 , n ) = 0.0_pReal
rho_edg_delta_neighbor ( : , n ) = rho_edg_delta
rho_scr_delta_neighbor ( : , n ) = rho_scr_delta
endif
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else
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! free surface -> use central values instead
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connection_latticeConf ( 1 : 3 , n ) = 0.0_pReal
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rho_edg_delta_neighbor ( : , n ) = rho_edg_delta
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rho_scr_delta_neighbor ( : , n ) = rho_scr_delta
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endif
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enddo
neighbor_rhoExcess ( 1 , : , : ) = rho_edg_delta_neighbor
neighbor_rhoExcess ( 2 , : , : ) = rho_scr_delta_neighbor
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!* 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 ) = prm % slip_direction
m ( 1 : 3 , 1 : ns , 2 ) = - prm % slip_transverse
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do s = 1 , ns
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! gradient from interpolation of neighboring excess density ...
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do c = 1 , 2
do dir = 1 , 3
neighbors ( 1 ) = 2 * dir - 1
neighbors ( 2 ) = 2 * dir
connections ( dir , 1 : 3 ) = connection_latticeConf ( 1 : 3 , neighbors ( 1 ) ) &
- connection_latticeConf ( 1 : 3 , neighbors ( 2 ) )
rhoExcessDifferences ( dir ) = neighbor_rhoExcess ( c , s , neighbors ( 1 ) ) &
- neighbor_rhoExcess ( c , s , neighbors ( 2 ) )
enddo
invConnections = math_inv33 ( connections )
if ( all ( dEq0 ( invConnections ) ) ) call IO_error ( - 1 , ext_msg = 'back stress calculation: inversion error' )
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rhoExcessGradient ( c ) = math_inner ( m ( 1 : 3 , s , c ) , matmul ( invConnections , rhoExcessDifferences ) )
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enddo
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! ... plus gradient from deads ...
rhoExcessGradient ( 1 ) = rhoExcessGradient ( 1 ) + sum ( rho ( s , imm_edg ) ) / FVsize
rhoExcessGradient ( 2 ) = rhoExcessGradient ( 2 ) + sum ( rho ( s , imm_scr ) ) / FVsize
! ... normalized with the total density ...
rhoTotal ( 1 ) = ( sum ( abs ( rho ( s , edg ) ) ) + sum ( neighbor_rhoTotal ( 1 , s , : ) ) ) / ( 1.0_pReal + nRealNeighbors )
rhoTotal ( 2 ) = ( sum ( abs ( rho ( s , scr ) ) ) + sum ( neighbor_rhoTotal ( 2 , s , : ) ) ) / ( 1.0_pReal + nRealNeighbors )
rhoExcessGradient_over_rho = 0.0_pReal
where ( rhoTotal > 0.0_pReal ) &
rhoExcessGradient_over_rho = rhoExcessGradient / rhoTotal
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! ... gives the local stress correction when multiplied with a factor
dst % tau_back ( s , of ) = - prm % mu * prm % burgers ( s ) / ( 2.0_pReal * pi ) &
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* ( rhoExcessGradient_over_rho ( 1 ) / ( 1.0_pReal - prm % nu ) &
+ rhoExcessGradient_over_rho ( 2 ) )
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enddo
endif
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#ifdef DEBUG
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelExtensive ) / = 0 &
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. and . ( ( debug_e == el . and . debug_i == ip ) &
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. or . . not . iand ( debug_level ( debug_constitutive ) , debug_levelSelective ) / = 0 ) ) then
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write ( 6 , '(/,a,i8,1x,i2,1x,i1,/)' ) '<< CONST >> nonlocal_microstructure at el ip ' , el , ip
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write ( 6 , '(a,/,12x,12(e10.3,1x))' ) '<< CONST >> rhoForest' , stt % rho_forest ( : , of )
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write ( 6 , '(a,/,12x,12(f10.5,1x))' ) '<< CONST >> tauThreshold / MPa' , dst % tau_threshold ( : , of ) * 1e-6
write ( 6 , '(a,/,12x,12(f10.5,1x),/)' ) '<< CONST >> tauBack / MPa' , dst % tau_back ( : , of ) * 1e-6
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endif
#endif
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end associate
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end subroutine plastic_nonlocal_dependentState
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!--------------------------------------------------------------------------------------------------
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!> @brief calculates kinetics
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!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_kinetics ( v , dv_dtau , dv_dtauNS , tau , tauNS , &
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tauThreshold , c , Temperature , instance , of )
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integer , intent ( in ) :: &
c , & !< dislocation character (1:edge, 2:screw)
instance , of
real ( pReal ) , intent ( in ) :: &
Temperature !< temperature
real ( pReal ) , dimension ( param ( instance ) % totalNslip ) , intent ( in ) :: &
tau , & !< resolved external shear stress (without non Schmid effects)
tauNS , & !< resolved external shear stress (including non Schmid effects)
tauThreshold !< threshold shear stress
real ( pReal ) , dimension ( param ( instance ) % totalNslip ) , intent ( out ) :: &
v , & !< velocity
dv_dtau , & !< velocity derivative with respect to resolved shear stress (without non Schmid contributions)
dv_dtauNS !< velocity derivative with respect to resolved shear stress (including non Schmid contributions)
integer :: &
ns , & !< short notation for the total number of active slip systems
s !< index of my current slip system
real ( pReal ) :: &
tauRel_P , &
tauRel_S , &
tauEff , & !< effective shear stress
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
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
associate ( prm = > param ( instance ) )
ns = prm % totalNslip
v = 0.0_pReal
dv_dtau = 0.0_pReal
dv_dtauNS = 0.0_pReal
if ( Temperature > 0.0_pReal ) then
do s = 1 , ns
if ( abs ( tau ( s ) ) > tauThreshold ( s ) ) then
!* Peierls contribution
!* Effective stress includes non Schmid constributions
!* The derivative only gives absolute values; the correct sign is taken care of in the formula for the derivative of the velocity
tauEff = max ( 0.0_pReal , abs ( tauNS ( s ) ) - tauThreshold ( s ) ) ! ensure that the effective stress is positive
meanfreepath_P = prm % burgers ( s )
jumpWidth_P = prm % burgers ( s )
activationLength_P = prm % doublekinkwidth * prm % burgers ( s )
activationVolume_P = activationLength_P * jumpWidth_P * prm % burgers ( s )
criticalStress_P = prm % peierlsStress ( s , c )
activationEnergy_P = criticalStress_P * activationVolume_P
tauRel_P = min ( 1.0_pReal , tauEff / criticalStress_P ) ! ensure that the activation probability cannot become greater than one
tPeierls = 1.0_pReal / prm % fattack &
* exp ( activationEnergy_P / ( KB * Temperature ) &
* ( 1.0_pReal - tauRel_P ** prm % p ) ** prm % q )
if ( tauEff < criticalStress_P ) then
dtPeierls_dtau = tPeierls * prm % p * prm % q * activationVolume_P / ( KB * Temperature ) &
* ( 1.0_pReal - tauRel_P ** prm % p ) ** ( prm % q - 1.0_pReal ) &
* tauRel_P ** ( prm % p - 1.0_pReal )
else
dtPeierls_dtau = 0.0_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
tauEff = abs ( tau ( s ) ) - tauThreshold ( s )
meanfreepath_S = prm % burgers ( s ) / sqrt ( prm % solidSolutionConcentration )
jumpWidth_S = prm % solidSolutionSize * prm % burgers ( s )
activationLength_S = prm % burgers ( s ) / sqrt ( prm % solidSolutionConcentration )
activationVolume_S = activationLength_S * jumpWidth_S * prm % burgers ( s )
activationEnergy_S = prm % solidSolutionEnergy
criticalStress_S = activationEnergy_S / activationVolume_S
tauRel_S = min ( 1.0_pReal , tauEff / criticalStress_S ) ! ensure that the activation probability cannot become greater than one
tSolidSolution = 1.0_pReal / prm % fattack &
* exp ( activationEnergy_S / ( KB * Temperature ) &
* ( 1.0_pReal - tauRel_S ** prm % p ) ** prm % q )
if ( tauEff < criticalStress_S ) then
dtSolidSolution_dtau = tSolidSolution * prm % p * prm % q &
* activationVolume_S / ( KB * Temperature ) &
* ( 1.0_pReal - tauRel_S ** prm % p ) ** ( prm % q - 1.0_pReal ) &
* tauRel_S ** ( prm % p - 1.0_pReal )
else
dtSolidSolution_dtau = 0.0_pReal
endif
!* viscous glide velocity
tauEff = abs ( tau ( s ) ) - tauThreshold ( s )
mobility = prm % burgers ( s ) / prm % viscosity
vViscous = mobility * tauEff
!* Mean velocity results from waiting time at peierls barriers and solid solution obstacles with respective meanfreepath of
!* free flight at glide velocity in between.
!* adopt sign from resolved stress
v ( s ) = sign ( 1.0_pReal , tau ( s ) ) &
/ ( tPeierls / meanfreepath_P + tSolidSolution / meanfreepath_S + 1.0_pReal / vViscous )
dv_dtau ( s ) = v ( s ) * v ( s ) * ( dtSolidSolution_dtau / meanfreepath_S &
+ mobility / ( vViscous * vViscous ) )
dv_dtauNS ( s ) = v ( s ) * v ( s ) * dtPeierls_dtau / meanfreepath_P
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endif
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enddo
endif
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openmp parallelization working again (at least for j2 and nonlocal constitutive model).
In order to keep it like that, please follow these simple rules:
DON'T use implicit array subscripts:
example: real, dimension(3,3) :: A,B
A(:,2) = B(:,1) <--- DON'T USE
A(1:3,2) = B(1:3,1) <--- BETTER USE
In many cases the use of explicit array subscripts is inevitable for parallelization. Additionally, it is an easy means to prevent memory leaks.
Enclose all write statements with the following:
!$OMP CRITICAL (write2out)
<your write statement>
!$OMP END CRITICAL (write2out)
Whenever you change something in the code and are not sure if it affects parallelization and leads to nonconforming behavior, please ask me and/or Franz to check this.
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#ifdef DEBUGTODO
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write ( 6 , '(a,/,12x,12(f12.5,1x))' ) '<< CONST >> tauThreshold / MPa' , tauThreshold * 1e-6_pReal
write ( 6 , '(a,/,12x,12(f12.5,1x))' ) '<< CONST >> tau / MPa' , tau * 1e-6_pReal
write ( 6 , '(a,/,12x,12(f12.5,1x))' ) '<< CONST >> tauNS / MPa' , tauNS * 1e-6_pReal
write ( 6 , '(a,/,12x,12(f12.5,1x))' ) '<< CONST >> v / mm/s' , v * 1e3
write ( 6 , '(a,/,12x,12(e12.5,1x))' ) '<< CONST >> dv_dtau' , dv_dtau
write ( 6 , '(a,/,12x,12(e12.5,1x))' ) '<< CONST >> dv_dtauNS' , dv_dtauNS
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#endif
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end associate
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end subroutine plastic_nonlocal_kinetics
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!--------------------------------------------------------------------------------------------------
!> @brief calculates plastic velocity gradient and its tangent
!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_LpAndItsTangent ( Lp , dLp_dMp , &
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Mp , Temperature , volume , ip , el )
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integer , intent ( in ) :: &
ip , & !< current integration point
el !< current element number
real ( pReal ) , intent ( in ) :: &
Temperature , & !< temperature
volume !< volume of the materialpoint
real ( pReal ) , dimension ( 3 , 3 ) , intent ( in ) :: &
Mp
real ( pReal ) , dimension ( 3 , 3 ) , intent ( out ) :: &
Lp !< plastic velocity gradient
real ( pReal ) , dimension ( 3 , 3 , 3 , 3 ) , intent ( out ) :: &
dLp_dMp !< derivative of Lp with respect to Tstar (9x9 matrix)
integer :: &
instance , & !< current instance of this plasticity
ns , & !< short notation for the total number of active slip systems
i , &
j , &
k , &
l , &
ph , & !phase number
of , & !offset
t , & !< dislocation type
s !< index of my current slip system
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 8 ) :: &
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rhoSgl !< single dislocation densities (including blocked)
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 10 ) :: &
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rho
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 4 ) :: &
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v , & !< velocity
tauNS , & !< resolved shear stress including non Schmid and backstress terms
dv_dtau , & !< velocity derivative with respect to the shear stress
dv_dtauNS !< velocity derivative with respect to the shear stress
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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tau , & !< resolved shear stress including backstress terms
gdotTotal !< shear rate
!*** shortcut for mapping
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ph = material_phaseAt ( 1 , el )
of = material_phasememberAt ( 1 , ip , el )
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instance = phase_plasticityInstance ( ph )
associate ( prm = > param ( instance ) , dst = > microstructure ( instance ) )
ns = prm % totalNslip
!*** shortcut to state variables
rho = getRho ( instance , of , ip , el )
rhoSgl = rho ( : , sgl )
!*** get resolved shear stress
!*** for screws possible non-schmid contributions are also taken into account
do s = 1 , ns
tau ( s ) = math_mul33xx33 ( Mp , prm % Schmid ( 1 : 3 , 1 : 3 , s ) )
tauNS ( s , 1 ) = tau ( s )
tauNS ( s , 2 ) = tau ( s )
if ( tau ( s ) > 0.0_pReal ) then
tauNS ( s , 3 ) = math_mul33xx33 ( Mp , + prm % nonSchmid_pos ( 1 : 3 , 1 : 3 , s ) )
tauNS ( s , 4 ) = math_mul33xx33 ( Mp , - prm % nonSchmid_neg ( 1 : 3 , 1 : 3 , s ) )
else
tauNS ( s , 3 ) = math_mul33xx33 ( Mp , + prm % nonSchmid_neg ( 1 : 3 , 1 : 3 , s ) )
tauNS ( s , 4 ) = math_mul33xx33 ( Mp , - prm % nonSchmid_pos ( 1 : 3 , 1 : 3 , s ) )
endif
enddo
forall ( t = 1 : 4 ) &
tauNS ( 1 : ns , t ) = tauNS ( 1 : ns , t ) + dst % tau_back ( : , of )
tau = tau + dst % tau_back ( : , of )
!*** get dislocation velocity and its tangent and store the velocity in the state array
! edges
call plastic_nonlocal_kinetics ( v ( 1 : ns , 1 ) , dv_dtau ( 1 : ns , 1 ) , dv_dtauNS ( 1 : ns , 1 ) , &
tau ( 1 : ns ) , tauNS ( 1 : ns , 1 ) , dst % tau_Threshold ( 1 : ns , of ) , &
1 , Temperature , instance , of )
v ( 1 : ns , 2 ) = v ( 1 : ns , 1 )
dv_dtau ( 1 : ns , 2 ) = dv_dtau ( 1 : ns , 1 )
dv_dtauNS ( 1 : ns , 2 ) = dv_dtauNS ( 1 : ns , 1 )
!screws
if ( size ( prm % nonSchmidCoeff ) == 0 ) then
forall ( t = 3 : 4 )
v ( 1 : ns , t ) = v ( 1 : ns , 1 )
dv_dtau ( 1 : ns , t ) = dv_dtau ( 1 : ns , 1 )
dv_dtauNS ( 1 : ns , t ) = dv_dtauNS ( 1 : ns , 1 )
endforall
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else
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do t = 3 , 4
call plastic_nonlocal_kinetics ( v ( 1 : ns , t ) , dv_dtau ( 1 : ns , t ) , dv_dtauNS ( 1 : ns , t ) , &
tau ( 1 : ns ) , tauNS ( 1 : ns , t ) , dst % tau_Threshold ( 1 : ns , of ) , &
2 , Temperature , instance , of )
enddo
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endif
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!*** store velocity in state
forall ( t = 1 : 4 ) &
plasticState ( ph ) % state ( iV ( 1 : ns , t , instance ) , of ) = v ( 1 : ns , t )
!*** Bauschinger effect
forall ( s = 1 : ns , t = 5 : 8 , rhoSgl ( s , t ) * v ( s , t - 4 ) < 0.0_pReal ) &
rhoSgl ( s , t - 4 ) = rhoSgl ( s , t - 4 ) + abs ( rhoSgl ( s , t ) )
gdotTotal = sum ( rhoSgl ( 1 : ns , 1 : 4 ) * v , 2 ) * prm % burgers ( 1 : ns )
Lp = 0.0_pReal
dLp_dMp = 0.0_pReal
do s = 1 , ns
Lp = Lp + gdotTotal ( s ) * prm % Schmid ( 1 : 3 , 1 : 3 , s )
forall ( i = 1 : 3 , j = 1 : 3 , k = 1 : 3 , l = 1 : 3 ) &
dLp_dMp ( i , j , k , l ) = dLp_dMp ( i , j , k , l ) &
+ prm % Schmid ( i , j , s ) * prm % Schmid ( k , l , s ) &
* sum ( rhoSgl ( s , 1 : 4 ) * dv_dtau ( s , 1 : 4 ) ) * prm % burgers ( s ) &
+ prm % Schmid ( i , j , s ) &
* ( prm % nonSchmid_pos ( k , l , s ) * rhoSgl ( s , 3 ) * dv_dtauNS ( s , 3 ) &
- prm % nonSchmid_neg ( k , l , s ) * rhoSgl ( s , 4 ) * dv_dtauNS ( s , 4 ) ) * prm % burgers ( s )
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enddo
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end associate
end subroutine plastic_nonlocal_LpAndItsTangent
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!--------------------------------------------------------------------------------------------------
!> @brief (instantaneous) incremental change of microstructure
!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_deltaState ( Mp , ip , el )
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integer , intent ( in ) :: &
ip , &
el
real ( pReal ) , dimension ( 3 , 3 ) , intent ( in ) :: &
Mp !< MandelStress
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integer :: &
ph , & !< phase
of , & !< offset
instance , & ! current instance of this plasticity
ns , & ! short notation for the total number of active slip systems
c , & ! character of dislocation
t , & ! type of dislocation
s ! index of my current slip system
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 10 ) :: &
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deltaRhoRemobilization , & ! density increment by remobilization
deltaRhoDipole2SingleStress ! density increment by dipole dissociation (by stress change)
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 10 ) :: &
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rho ! current dislocation densities
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 4 ) :: &
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v ! dislocation glide velocity
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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tau ! current resolved shear stress
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 2 ) :: &
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rhoDip , & ! current dipole dislocation densities (screw and edge dipoles)
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
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ph = material_phaseAt ( 1 , el )
of = material_phasememberAt ( 1 , ip , el )
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instance = phase_plasticityInstance ( ph )
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associate ( prm = > param ( instance ) , dst = > microstructure ( instance ) , del = > deltaState ( instance ) )
ns = totalNslip ( instance )
!*** shortcut to state variables
forall ( s = 1 : ns , t = 1 : 4 ) &
v ( s , t ) = plasticState ( ph ) % state ( iV ( s , t , instance ) , of )
forall ( s = 1 : ns , c = 1 : 2 ) &
dUpperOld ( s , c ) = plasticState ( ph ) % state ( iD ( s , c , instance ) , of )
rho = getRho ( instance , of , ip , el )
rhoDip = rho ( : , dip )
!****************************************************************************
!*** dislocation remobilization (bauschinger effect)
where ( rho ( : , imm ) * v < 0.0_pReal )
deltaRhoRemobilization ( : , mob ) = abs ( rho ( : , imm ) )
deltaRhoRemobilization ( : , imm ) = - rho ( : , imm )
rho ( : , mob ) = rho ( : , mob ) + abs ( rho ( : , imm ) )
rho ( : , imm ) = 0.0_pReal
elsewhere
deltaRhoRemobilization ( : , mob ) = 0.0_pReal
deltaRhoRemobilization ( : , imm ) = 0.0_pReal
endwhere
deltaRhoRemobilization ( : , dip ) = 0.0_pReal
!****************************************************************************
!*** calculate dipole formation and dissociation by stress change
!*** calculate limits for stable dipole height
do s = 1 , prm % totalNslip
tau ( s ) = math_mul33xx33 ( Mp , prm % Schmid ( 1 : 3 , 1 : 3 , s ) ) + dst % tau_back ( s , of )
if ( abs ( tau ( s ) ) < 1.0e-15_pReal ) tau ( s ) = 1.0e-15_pReal
enddo
dUpper ( 1 : ns , 1 ) = prm % mu * prm % burgers / ( 8.0_pReal * PI * ( 1.0_pReal - prm % nu ) * abs ( tau ) )
dUpper ( 1 : ns , 2 ) = prm % mu * prm % burgers / ( 4.0_pReal * PI * abs ( tau ) )
where ( dNeq0 ( sqrt ( sum ( abs ( rho ( : , edg ) ) , 2 ) ) ) ) &
dUpper ( 1 : ns , 1 ) = min ( 1.0_pReal / sqrt ( sum ( abs ( rho ( : , edg ) ) , 2 ) ) , dUpper ( 1 : ns , 1 ) )
where ( dNeq0 ( sqrt ( sum ( abs ( rho ( : , scr ) ) , 2 ) ) ) ) &
dUpper ( 1 : ns , 2 ) = min ( 1.0_pReal / sqrt ( sum ( abs ( rho ( : , scr ) ) , 2 ) ) , dUpper ( 1 : ns , 2 ) )
dUpper = max ( dUpper , prm % minDipoleHeight )
deltaDUpper = dUpper - dUpperOld
!*** dissociation by stress increase
deltaRhoDipole2SingleStress = 0.0_pReal
forall ( c = 1 : 2 , s = 1 : ns , deltaDUpper ( s , c ) < 0.0_pReal . and . &
dNeq0 ( dUpperOld ( s , c ) - prm % minDipoleHeight ( s , c ) ) ) &
deltaRhoDipole2SingleStress ( s , 8 + c ) = rhoDip ( s , c ) * deltaDUpper ( s , c ) &
/ ( dUpperOld ( s , c ) - prm % minDipoleHeight ( s , c ) )
forall ( t = 1 : 4 ) &
deltaRhoDipole2SingleStress ( 1 : ns , t ) = - 0.5_pReal &
* deltaRhoDipole2SingleStress ( 1 : ns , ( t - 1 ) / 2 + 9 )
forall ( s = 1 : ns , c = 1 : 2 ) &
plasticState ( ph ) % state ( iD ( s , c , instance ) , of ) = dUpper ( s , c )
plasticState ( ph ) % deltaState ( : , of ) = 0.0_pReal
del % rho ( : , of ) = reshape ( deltaRhoRemobilization + deltaRhoDipole2SingleStress , [ 10 * ns ] )
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#ifdef DEBUG
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelExtensive ) / = 0 &
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. and . ( ( debug_e == el . and . debug_i == ip ) &
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. or . . not . iand ( debug_level ( debug_constitutive ) , debug_levelSelective ) / = 0 ) ) then
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write ( 6 , '(a,/,8(12x,12(e12.5,1x),/))' ) '<< CONST >> dislocation remobilization' , deltaRhoRemobilization ( 1 : ns , 1 : 8 )
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write ( 6 , '(a,/,10(12x,12(e12.5,1x),/),/)' ) '<< CONST >> dipole dissociation by stress increase' , deltaRhoDipole2SingleStress
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endif
#endif
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end associate
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end subroutine plastic_nonlocal_deltaState
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!---------------------------------------------------------------------------------------------------
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!> @brief calculates the rate of change of microstructure
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!---------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_dotState ( Mp , Fe , Fp , Temperature , &
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timestep , ip , el )
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integer , intent ( in ) :: &
ip , & !< current integration point
el !< current element number
real ( pReal ) , intent ( in ) :: &
Temperature , & !< temperature
timestep !< substepped crystallite time increment
real ( pReal ) , dimension ( 3 , 3 ) , intent ( in ) :: &
Mp !< MandelStress
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real ( pReal ) , dimension ( 3 , 3 , homogenization_maxNgrains , discretization_nIP , discretization_nElem ) , intent ( in ) :: &
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Fe , & !< elastic deformation gradient
Fp !< plastic deformation gradient
integer :: &
ph , &
instance , & !< current instance of this plasticity
neighbor_instance , & !< instance of my neighbor's plasticity
ns , & !< short notation for the total number of active slip systems
c , & !< character of dislocation
n , & !< index of my current neighbor
neighbor_el , & !< element number of my neighbor
neighbor_ip , & !< integration point of my neighbor
neighbor_n , & !< neighbor index pointing to me when looking from my neighbor
opposite_neighbor , & !< index of my opposite neighbor
opposite_ip , & !< ip of my opposite neighbor
opposite_el , & !< element index of my opposite neighbor
opposite_n , & !< neighbor index pointing to me when looking from my opposite neighbor
t , & !< type of dislocation
o , & !< offset shortcut
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no , & !< neighbor offset shortcut
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p , & !< phase shortcut
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np , & !< neighbor phase shortcut
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topp , & !< type of dislocation with opposite sign to t
s !< index of my current slip system
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 10 ) :: &
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rho , &
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
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 8 ) :: &
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rhoSgl , & !< current single dislocation densities (positive/negative screw and edge without dipoles)
neighbor_rhoSgl , & !< current single dislocation densities of neighboring ip (positive/negative screw and edge without dipoles)
my_rhoSgl !< single dislocation densities of central ip (positive/negative screw and edge without dipoles)
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 4 ) :: &
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v , & !< current dislocation glide velocity
my_v , & !< dislocation glide velocity of central ip
neighbor_v , & !< dislocation glide velocity of enighboring ip
gdot !< shear rates
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) ) :: &
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tau , & !< current resolved shear stress
vClimb !< climb velocity of edge dipoles
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real ( pReal ) , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 2 ) :: &
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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
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real ( pReal ) , dimension ( 3 , totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , el ) ) ) , 4 ) :: &
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m !< direction of dislocation motion
real ( pReal ) , dimension ( 3 , 3 ) :: &
my_F , & !< my total deformation gradient
neighbor_F , & !< total deformation gradient of my neighbor
my_Fe , & !< my elastic deformation gradient
neighbor_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
selfDiffusion !< self diffusion
logical :: &
considerEnteringFlux , &
considerLeavingFlux
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p = material_phaseAt ( 1 , el )
o = material_phasememberAt ( 1 , ip , el )
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if ( timestep < = 0.0_pReal ) then
plasticState ( p ) % dotState = 0.0_pReal
return
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endif
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ph = material_phaseAt ( 1 , el )
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instance = phase_plasticityInstance ( ph )
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associate ( prm = > param ( instance ) , &
dst = > microstructure ( instance ) , &
dot = > dotState ( instance ) , &
stt = > state ( instance ) )
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ns = totalNslip ( instance )
tau = 0.0_pReal
gdot = 0.0_pReal
rho = getRho ( instance , o , ip , el )
rhoSgl = rho ( : , sgl )
rhoDip = rho ( : , dip )
forall ( s = 1 : ns , t = 1 : 4 )
v ( s , t ) = plasticState ( p ) % state ( iV ( s , t , instance ) , o )
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endforall
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!****************************************************************************
!*** Calculate shear rate
forall ( t = 1 : 4 ) &
gdot ( 1 : ns , t ) = rhoSgl ( 1 : ns , t ) * prm % burgers ( 1 : ns ) * v ( 1 : ns , t )
#ifdef DEBUG
if ( iand ( debug_level ( debug_constitutive ) , debug_levelBasic ) / = 0 &
. and . ( ( debug_e == el . and . debug_i == ip ) &
. or . . not . iand ( debug_level ( debug_constitutive ) , debug_levelSelective ) / = 0 ) ) 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 , ns ! loop over slip systems
tau ( s ) = math_mul33xx33 ( Mp , prm % Schmid ( 1 : 3 , 1 : 3 , s ) ) + dst % tau_back ( s , o )
if ( abs ( tau ( s ) ) < 1.0e-15_pReal ) tau ( s ) = 1.0e-15_pReal
enddo
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dLower = prm % minDipoleHeight
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dUpper ( 1 : ns , 1 ) = prm % mu * prm % burgers / ( 8.0_pReal * PI * ( 1.0_pReal - prm % nu ) * abs ( tau ) )
dUpper ( 1 : ns , 2 ) = prm % mu * prm % burgers / ( 4.0_pReal * PI * abs ( tau ) )
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where ( dNeq0 ( sqrt ( sum ( abs ( rho ( : , edg ) ) , 2 ) ) ) ) &
dUpper ( 1 : ns , 1 ) = min ( 1.0_pReal / sqrt ( sum ( abs ( rho ( : , edg ) ) , 2 ) ) , dUpper ( 1 : ns , 1 ) )
where ( dNeq0 ( sqrt ( sum ( abs ( rho ( : , scr ) ) , 2 ) ) ) ) &
dUpper ( 1 : ns , 2 ) = min ( 1.0_pReal / sqrt ( sum ( abs ( rho ( : , scr ) ) , 2 ) ) , dUpper ( 1 : ns , 2 ) )
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dUpper = max ( dUpper , dLower )
!****************************************************************************
!*** calculate dislocation multiplication
rhoDotMultiplication = 0.0_pReal
isBCC : if ( lattice_structure ( ph ) == LATTICE_bcc_ID ) then
forall ( s = 1 : ns , sum ( abs ( v ( s , 1 : 4 ) ) ) > 0.0_pReal )
rhoDotMultiplication ( s , 1 : 2 ) = sum ( abs ( gdot ( s , 3 : 4 ) ) ) / prm % burgers ( s ) & ! assuming double-cross-slip of screws to be decisive for multiplication
* sqrt ( stt % rho_forest ( s , o ) ) / prm % lambda0 ( s ) ! & ! mean free path
! * 2.0_pReal * sum(abs(v(s,3:4))) / sum(abs(v(s,1:4))) ! ratio of screw to overall velocity determines edge generation
rhoDotMultiplication ( s , 3 : 4 ) = sum ( abs ( gdot ( s , 3 : 4 ) ) ) / prm % burgers ( s ) & ! assuming double-cross-slip of screws to be decisive for multiplication
* sqrt ( stt % rho_forest ( s , o ) ) / prm % lambda0 ( s ) ! & ! mean free path
! * 2.0_pReal * sum(abs(v(s,1:2))) / sum(abs(v(s,1:4))) ! ratio of edge to overall velocity determines screw generation
endforall
else isBCC
rhoDotMultiplication ( 1 : ns , 1 : 4 ) = spread ( &
( sum ( abs ( gdot ( 1 : ns , 1 : 2 ) ) , 2 ) * prm % fEdgeMultiplication + sum ( abs ( gdot ( 1 : ns , 3 : 4 ) ) , 2 ) ) &
* sqrt ( stt % rho_forest ( : , o ) ) / prm % lambda0 / prm % burgers ( 1 : ns ) , 2 , 4 )
endif isBCC
!****************************************************************************
!*** calculate dislocation fluxes (only for nonlocal plasticity)
rhoDotFlux = 0.0_pReal
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if ( . not . phase_localPlasticity ( material_phaseAt ( 1 , el ) ) ) then
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!*** check CFL (Courant-Friedrichs-Lewy) condition for flux
if ( any ( abs ( gdot ) > 0.0_pReal & ! any active slip system ...
. and . prm % CFLfactor * abs ( v ) * timestep &
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> IPvolume ( ip , el ) / maxval ( IParea ( : , ip , el ) ) ) ) then ! ...with velocity above critical value (we use the reference volume and area for simplicity here)
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#ifdef DEBUG
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelExtensive ) / = 0 ) then
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write ( 6 , '(a,i5,a,i2)' ) '<< CONST >> CFL condition not fullfilled at el ' , el , ' ip ' , ip
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write ( 6 , '(a,e10.3,a,e10.3)' ) '<< CONST >> velocity is at ' , &
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maxval ( abs ( v ) , abs ( gdot ) > 0.0_pReal &
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. and . prm % CFLfactor * abs ( v ) * timestep &
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> IPvolume ( ip , el ) / maxval ( IParea ( : , ip , el ) ) ) , &
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' at a timestep of ' , timestep
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write ( 6 , '(a)' ) '<< CONST >> enforcing cutback !!!'
endif
#endif
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plasticState ( p ) % dotState = IEEE_value ( 1.0_pReal , IEEE_quiet_NaN ) ! -> return NaN and, hence, enforce cutback
return
endif
constitutive_nonlocal:
- read in activation energy for dislocation glide from material.config
- changed naming of dDipMin/Max to dLower/dUpper
- added new outputs: rho_dot, rho_dot_dip, rho_dot_gen, rho_dot_sgl2dip, rho_dot_dip2sgl, rho_dot_ann_ath, rho_dot_ann_the, rho_dot_flux, d_upper_edge, d_upper_screw, d_upper_dot_edge, d_upper_dot_screw
- poisson's ratio is now calculated from elastic constants
- microstrucutre has state as first argument, since this is our output variable
- periodic boundary conditions are taken into account for fluxes and internal stresses. for the moment, flag has to be set in constitutive_nonlocal.
- corrected calculation for dipole formation by glide
- added terms for dipole formation/annihilation by stress decrease/increase
constitutive:
- passing of arguments is adapted for constitutive_nonlocal model
crystallite:
- in stiffness calculation: call to collect_dotState used wrong arguments
- crystallite_postResults uses own Tstar_v and temperature, no need for passing them from materialpoint_postResults
homogenization:
- crystallite_postResults uses own Tstar_v and temperature, no need for passing them from materialpoint_postResults
IO:
- changed error message 229
material.config:
- changed example for nonlocal constitution according to constitutive_nonlocal
all:
- added some flush statements
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2011-01-11 20:25:36 +05:30
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!*** be aware of the definition of slip_transverse = slip_direction x slip_normal !!!
!*** opposite sign to our p vector in the (s,p,n) triplet !!!
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m ( 1 : 3 , 1 : ns , 1 ) = prm % slip_direction
m ( 1 : 3 , 1 : ns , 2 ) = - prm % slip_direction
m ( 1 : 3 , 1 : ns , 3 ) = - prm % slip_transverse
m ( 1 : 3 , 1 : ns , 4 ) = prm % slip_transverse
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my_Fe = Fe ( 1 : 3 , 1 : 3 , 1 , ip , el )
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my_F = matmul ( my_Fe , Fp ( 1 : 3 , 1 : 3 , 1 , ip , el ) )
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neighbors : do n = 1 , nIPneighbors
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neighbor_el = IPneighborhood ( 1 , n , ip , el )
neighbor_ip = IPneighborhood ( 2 , n , ip , el )
neighbor_n = IPneighborhood ( 3 , n , ip , el )
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np = material_phaseAt ( 1 , neighbor_el )
no = material_phasememberAt ( 1 , neighbor_ip , neighbor_el )
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opposite_neighbor = n + mod ( n , 2 ) - mod ( n + 1 , 2 )
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opposite_el = IPneighborhood ( 1 , opposite_neighbor , ip , el )
opposite_ip = IPneighborhood ( 2 , opposite_neighbor , ip , el )
opposite_n = IPneighborhood ( 3 , opposite_neighbor , ip , el )
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if ( neighbor_n > 0 ) then ! if neighbor exists, average deformation gradient
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neighbor_instance = phase_plasticityInstance ( material_phaseAt ( 1 , neighbor_el ) )
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neighbor_Fe = Fe ( 1 : 3 , 1 : 3 , 1 , neighbor_ip , neighbor_el )
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neighbor_F = matmul ( neighbor_Fe , Fp ( 1 : 3 , 1 : 3 , 1 , neighbor_ip , neighbor_el ) )
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Favg = 0.5_pReal * ( my_F + neighbor_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
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!* compatibility
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considerEnteringFlux = . false .
neighbor_v = 0.0_pReal ! needed for check of sign change in flux density below
neighbor_rhoSgl = 0.0_pReal
if ( neighbor_n > 0 ) then
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if ( phase_plasticity ( material_phaseAt ( 1 , neighbor_el ) ) == PLASTICITY_NONLOCAL_ID &
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. and . any ( compatibility ( : , : , : , n , ip , el ) > 0.0_pReal ) ) &
considerEnteringFlux = . true .
endif
enteringFlux : if ( considerEnteringFlux ) then
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forall ( s = 1 : ns , t = 1 : 4 )
neighbor_v ( s , t ) = plasticState ( np ) % state ( iV ( s , t , neighbor_instance ) , no )
neighbor_rhoSgl ( s , t ) = max ( plasticState ( np ) % state ( iRhoU ( s , t , neighbor_instance ) , no ) , &
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0.0_pReal )
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endforall
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where ( neighbor_rhoSgl * IPvolume ( neighbor_ip , neighbor_el ) ** 0.667_pReal < prm % significantN &
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. or . neighbor_rhoSgl < prm % significantRho ) &
neighbor_rhoSgl = 0.0_pReal
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normal_neighbor2me_defConf = math_det33 ( Favg ) * matmul ( math_inv33 ( transpose ( Favg ) ) , &
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IPareaNormal ( 1 : 3 , neighbor_n , neighbor_ip , neighbor_el ) ) ! calculate the normal of the interface in (average) deformed configuration (now pointing from my neighbor to me!!!)
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normal_neighbor2me = matmul ( transpose ( neighbor_Fe ) , normal_neighbor2me_defConf ) &
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/ math_det33 ( neighbor_Fe ) ! interface normal in the lattice configuration of my neighbor
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area = IParea ( neighbor_n , neighbor_ip , neighbor_el ) * norm2 ( normal_neighbor2me )
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normal_neighbor2me = normal_neighbor2me / norm2 ( normal_neighbor2me ) ! normalize the surface normal to unit length
do s = 1 , ns
do t = 1 , 4
c = ( t + 1 ) / 2
topp = t + mod ( t , 2 ) - mod ( t + 1 , 2 )
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if ( neighbor_v ( s , t ) * math_inner ( m ( 1 : 3 , s , t ) , normal_neighbor2me ) > 0.0_pReal & ! flux from my neighbor to me == entering flux for me
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. and . v ( s , t ) * neighbor_v ( s , t ) > = 0.0_pReal ) then ! ... only if no sign change in flux density
lineLength = neighbor_rhoSgl ( s , t ) * neighbor_v ( s , t ) &
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* math_inner ( m ( 1 : 3 , s , t ) , normal_neighbor2me ) * area ! positive line length that wants to enter through this interface
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where ( compatibility ( c , 1 : ns , s , n , ip , el ) > 0.0_pReal ) & ! positive compatibility...
rhoDotFlux ( 1 : ns , t ) = rhoDotFlux ( 1 : ns , t ) &
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+ lineLength / IPvolume ( ip , el ) & ! ... transferring to equally signed mobile dislocation type
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* compatibility ( c , 1 : ns , s , n , ip , el ) ** 2.0_pReal
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where ( compatibility ( c , 1 : ns , s , n , ip , el ) < 0.0_pReal ) & ! ..negative compatibility...
rhoDotFlux ( 1 : ns , topp ) = rhoDotFlux ( 1 : ns , topp ) &
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+ lineLength / IPvolume ( ip , el ) & ! ... transferring to opposite signed mobile dislocation type
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* compatibility ( c , 1 : ns , s , n , ip , el ) ** 2.0_pReal
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endif
enddo
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enddo
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endif enteringFlux
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!* 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 local 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.
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considerLeavingFlux = . true .
if ( opposite_n > 0 ) then
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if ( phase_plasticity ( material_phaseAt ( 1 , opposite_el ) ) / = PLASTICITY_NONLOCAL_ID ) &
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considerLeavingFlux = . false .
endif
leavingFlux : if ( considerLeavingFlux ) then
my_rhoSgl = rhoSgl
my_v = v
normal_me2neighbor_defConf = math_det33 ( Favg ) &
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* matmul ( math_inv33 ( transpose ( Favg ) ) , &
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IPareaNormal ( 1 : 3 , n , ip , el ) ) ! calculate the normal of the interface in (average) deformed configuration (pointing from me to my neighbor!!!)
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normal_me2neighbor = matmul ( transpose ( my_Fe ) , normal_me2neighbor_defConf ) &
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/ math_det33 ( my_Fe ) ! interface normal in my lattice configuration
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area = IParea ( n , ip , el ) * norm2 ( normal_me2neighbor )
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normal_me2neighbor = normal_me2neighbor / norm2 ( normal_me2neighbor ) ! normalize the surface normal to unit length
do s = 1 , ns
do t = 1 , 4
c = ( t + 1 ) / 2
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if ( my_v ( s , t ) * math_inner ( 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)
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if ( my_v ( s , t ) * neighbor_v ( s , t ) > = 0.0_pReal ) then ! no sign change in flux density
transmissivity = sum ( compatibility ( c , 1 : 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 = my_rhoSgl ( s , t ) * my_v ( s , t ) &
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* math_inner ( m ( 1 : 3 , s , t ) , normal_me2neighbor ) * area ! positive line length of mobiles that wants to leave through this interface
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rhoDotFlux ( s , t ) = rhoDotFlux ( s , t ) - lineLength / IPvolume ( ip , el ) ! subtract dislocation flux from current type
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rhoDotFlux ( s , t + 4 ) = rhoDotFlux ( s , t + 4 ) &
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+ lineLength / IPvolume ( ip , el ) * ( 1.0_pReal - transmissivity ) &
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* sign ( 1.0_pReal , my_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
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endif
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enddo
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enddo
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endif leavingFlux
enddo neighbors
endif
!****************************************************************************
!*** calculate dipole formation and annihilation
!*** formation by glide
do c = 1 , 2
rhoDotSingle2DipoleGlide ( 1 : ns , 2 * c - 1 ) = - 2.0_pReal * dUpper ( 1 : ns , c ) / prm % burgers ( 1 : ns ) &
* ( 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 ) / prm % burgers ( 1 : ns ) &
* ( 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 ) / prm % burgers ( 1 : ns ) &
* 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 ) / prm % burgers ( 1 : ns ) &
* 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 : 2 ) &
rhoDotAthermalAnnihilation ( 1 : ns , c + 8 ) = - 2.0_pReal * dLower ( 1 : ns , c ) / prm % burgers ( 1 : ns ) &
* ( 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
! annihilated screw dipoles leave edge jogs behind on the colinear system
if ( lattice_structure ( ph ) == LATTICE_fcc_ID ) &
forall ( s = 1 : ns , prm % colinearSystem ( s ) > 0 ) &
rhoDotAthermalAnnihilation ( prm % colinearSystem ( s ) , 1 : 2 ) = - rhoDotAthermalAnnihilation ( s , 10 ) &
* 0.25_pReal * sqrt ( stt % rho_forest ( s , o ) ) * ( dUpper ( s , 2 ) + dLower ( s , 2 ) ) * prm % edgeJogFactor
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!*** thermally activated annihilation of edge dipoles by climb
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rhoDotThermalAnnihilation = 0.0_pReal
selfDiffusion = prm % Dsd0 * exp ( - prm % selfDiffusionEnergy / ( KB * Temperature ) )
vClimb = prm % atomicVolume * selfDiffusion / ( KB * Temperature ) &
* prm % mu / ( 2.0_pReal * PI * ( 1.0_pReal - prm % nu ) ) &
* 2.0_pReal / ( dUpper ( 1 : ns , 1 ) + dLower ( 1 : ns , 1 ) )
forall ( s = 1 : ns , dUpper ( s , 1 ) > dLower ( s , 1 ) ) &
rhoDotThermalAnnihilation ( s , 9 ) = max ( - 4.0_pReal * rhoDip ( s , 1 ) * vClimb ( s ) / ( dUpper ( s , 1 ) - dLower ( s , 1 ) ) , &
- rhoDip ( s , 1 ) / timestep - rhoDotAthermalAnnihilation ( s , 9 ) &
- rhoDotSingle2DipoleGlide ( s , 9 ) ) ! make sure that we do not annihilate more dipoles than we have
rhoDot = 0.0_pReal
rhoDot = rhoDotFlux &
+ rhoDotMultiplication &
+ rhoDotSingle2DipoleGlide &
+ rhoDotAthermalAnnihilation &
+ rhoDotThermalAnnihilation
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#ifdef DEBUG
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelExtensive ) / = 0 &
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. and . ( ( debug_e == el . and . debug_i == ip ) &
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. or . . not . iand ( debug_level ( debug_constitutive ) , debug_levelSelective ) / = 0 ) ) then
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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
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write ( 6 , '(a,/,10(12x,12(e12.5,1x),/))' ) '<< CONST >> athermal dipole annihilation' , &
rhoDotAthermalAnnihilation * timestep
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write ( 6 , '(a,/,2(12x,12(e12.5,1x),/))' ) '<< CONST >> thermally activated dipole annihilation' , &
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rhoDotThermalAnnihilation ( 1 : ns , 9 : 10 ) * timestep
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write ( 6 , '(a,/,10(12x,12(e12.5,1x),/))' ) '<< CONST >> total density change' , &
rhoDot * timestep
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write ( 6 , '(a,/,10(12x,12(f12.5,1x),/))' ) '<< CONST >> relative density change' , &
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rhoDot ( 1 : ns , 1 : 8 ) * timestep / ( abs ( stt % rho ( : , sgl ) ) + 1.0e-10 ) , &
rhoDot ( 1 : ns , 9 : 10 ) * timestep / ( stt % rho ( : , dip ) + 1.0e-10 )
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write ( 6 , * )
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endif
#endif
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if ( any ( rho ( : , mob ) + rhoDot ( 1 : ns , 1 : 4 ) * timestep < - prm % aTolRho ) &
. or . any ( rho ( : , dip ) + rhoDot ( 1 : ns , 9 : 10 ) * timestep < - prm % aTolRho ) ) then
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#ifdef DEBUG
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelExtensive ) / = 0 ) 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
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#endif
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plasticState ( p ) % dotState = IEEE_value ( 1.0_pReal , IEEE_quiet_NaN )
else
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dot % rho ( : , o ) = pack ( rhoDot , . true . )
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forall ( s = 1 : ns ) &
dot % accumulatedshear ( s , o ) = sum ( gdot ( s , 1 : 4 ) )
endif
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end associate
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end subroutine plastic_nonlocal_dotState
!--------------------------------------------------------------------------------------------------
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!> @brief Compatibility update
!> @detail Compatibility is defined as normalized product of signed cosine of the angle between the slip
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! 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.
!--------------------------------------------------------------------------------------------------
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subroutine plastic_nonlocal_updateCompatibility ( orientation , i , e )
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integer , intent ( in ) :: &
i , &
e
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type ( rotation ) , dimension ( 1 , discretization_nIP , discretization_nElem ) , intent ( in ) :: &
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orientation ! crystal orientation in quaternions
integer :: &
Nneighbors , & ! number of neighbors
n , & ! neighbor index
neighbor_e , & ! element index of my neighbor
neighbor_i , & ! integration point index of my neighbor
ph , &
neighbor_phase , &
textureID , &
neighbor_textureID , &
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
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real ( pReal ) , dimension ( 2 , totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , e ) ) ) , &
totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , e ) ) ) , &
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nIPneighbors ) :: &
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my_compatibility ! my_compatibility for current element and ip
real ( pReal ) :: &
my_compatibilitySum , &
thresholdValue , &
nThresholdValues
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logical , dimension ( totalNslip ( phase_plasticityInstance ( material_phaseAt ( 1 , e ) ) ) ) :: &
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belowThreshold
type ( rotation ) :: rot
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Nneighbors = nIPneighbors
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ph = material_phaseAt ( 1 , e )
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textureID = material_texture ( 1 , i , e )
instance = phase_plasticityInstance ( ph )
ns = totalNslip ( instance )
associate ( prm = > param ( instance ) )
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!*** start out fully compatible
my_compatibility = 0.0_pReal
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forall ( s1 = 1 : ns ) my_compatibility ( 1 : 2 , s1 , s1 , 1 : Nneighbors ) = 1.0_pReal
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!*** Loop thrugh neighbors and check whether there is any compatibility.
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neighbors : do n = 1 , Nneighbors
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neighbor_e = IPneighborhood ( 1 , n , i , e )
neighbor_i = IPneighborhood ( 2 , n , i , e )
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!* FREE SURFACE
!* Set surface transmissivity to the value specified in the material.config
if ( neighbor_e < = 0 . or . neighbor_i < = 0 ) then
forall ( s1 = 1 : ns ) my_compatibility ( 1 : 2 , s1 , s1 , n ) = sqrt ( prm % surfaceTransmissivity )
cycle
endif
!* PHASE BOUNDARY
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!* If we encounter a different nonlocal phase at the neighbor,
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!* we consider this to be a real "physical" phase boundary, so completely incompatible.
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!* If one of the two phases has a local plasticity law,
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!* we do not consider this to be a phase boundary, so completely compatible.
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neighbor_phase = material_phaseAt ( 1 , neighbor_e )
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if ( neighbor_phase / = ph ) then
if ( . not . phase_localPlasticity ( neighbor_phase ) . and . . not . phase_localPlasticity ( ph ) ) &
forall ( s1 = 1 : ns ) my_compatibility ( 1 : 2 , s1 , s1 , n ) = 0.0_pReal
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cycle
endif
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!* GRAIN BOUNDARY !
!* fixed transmissivity for adjacent ips with different texture (only if explicitly given in material.config)
if ( prm % grainboundaryTransmissivity > = 0.0_pReal ) then
neighbor_textureID = material_texture ( 1 , neighbor_i , neighbor_e )
if ( neighbor_textureID / = textureID ) then
if ( . not . phase_localPlasticity ( neighbor_phase ) ) then
forall ( s1 = 1 : ns ) &
my_compatibility ( 1 : 2 , s1 , s1 , n ) = sqrt ( prm % grainboundaryTransmissivity )
endif
cycle
endif
!* GRAIN BOUNDARY ?
!* Compatibility defined by relative orientation of slip systems:
!* The my_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
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!* 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.
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!* All values below the threshold are set to zero.
else
rot = orientation ( 1 , i , e ) % misorientation ( orientation ( 1 , neighbor_i , neighbor_e ) )
absoluteMisorientation = rot % asQuaternion ( )
mySlipSystems : do s1 = 1 , ns
neighborSlipSystems : do s2 = 1 , ns
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my_compatibility ( 1 , s2 , s1 , n ) = math_inner ( prm % slip_normal ( 1 : 3 , s1 ) , &
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math_qRot ( absoluteMisorientation , prm % slip_normal ( 1 : 3 , s2 ) ) ) &
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* abs ( math_inner ( prm % slip_direction ( 1 : 3 , s1 ) , &
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math_qRot ( absoluteMisorientation , prm % slip_direction ( 1 : 3 , s2 ) ) ) )
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my_compatibility ( 2 , s2 , s1 , n ) = abs ( math_inner ( prm % slip_normal ( 1 : 3 , s1 ) , &
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math_qRot ( absoluteMisorientation , prm % slip_normal ( 1 : 3 , s2 ) ) ) ) &
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* abs ( math_inner ( prm % slip_direction ( 1 : 3 , s1 ) , &
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math_qRot ( absoluteMisorientation , prm % slip_direction ( 1 : 3 , s2 ) ) ) )
enddo neighborSlipSystems
my_compatibilitySum = 0.0_pReal
belowThreshold = . true .
do while ( my_compatibilitySum < 1.0_pReal . and . any ( belowThreshold ( 1 : ns ) ) )
thresholdValue = maxval ( my_compatibility ( 2 , 1 : ns , s1 , n ) , belowThreshold ( 1 : ns ) ) ! screws always positive
nThresholdValues = real ( count ( my_compatibility ( 2 , 1 : ns , s1 , n ) > = thresholdValue ) , pReal )
where ( my_compatibility ( 2 , 1 : ns , s1 , n ) > = thresholdValue ) &
belowThreshold ( 1 : ns ) = . false .
if ( my_compatibilitySum + thresholdValue * nThresholdValues > 1.0_pReal ) &
where ( abs ( my_compatibility ( 1 : 2 , 1 : ns , s1 , n ) ) > = thresholdValue ) & ! MD: rather check below threshold?
my_compatibility ( 1 : 2 , 1 : ns , s1 , n ) = sign ( ( 1.0_pReal - my_compatibilitySum ) &
/ nThresholdValues , my_compatibility ( 1 : 2 , 1 : ns , s1 , n ) )
my_compatibilitySum = my_compatibilitySum + nThresholdValues * thresholdValue
enddo
where ( belowThreshold ( 1 : ns ) ) my_compatibility ( 1 , 1 : ns , s1 , n ) = 0.0_pReal
where ( belowThreshold ( 1 : ns ) ) my_compatibility ( 2 , 1 : ns , s1 , n ) = 0.0_pReal
enddo mySlipSystems
endif
enddo neighbors
compatibility ( 1 : 2 , 1 : ns , 1 : ns , 1 : Nneighbors , i , e ) = my_compatibility
end associate
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end subroutine plastic_nonlocal_updateCompatibility
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!--------------------------------------------------------------------------------------------------
!> @brief return array of constitutive results
!--------------------------------------------------------------------------------------------------
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function plastic_nonlocal_postResults ( ph , instance , of ) result ( postResults )
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integer , intent ( in ) :: &
ph , &
instance , &
of
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real ( pReal ) , dimension ( sum ( plastic_nonlocal_sizePostResult ( : , instance ) ) ) :: &
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postResults
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integer :: &
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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
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s !< index of my current slip system
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real ( pReal ) , dimension ( param ( instance ) % totalNslip , 8 ) :: &
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rhoSgl , &
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rhoDotSgl !< evolution rate of single dislocation densities (positive/negative screw and edge without dipoles)
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real ( pReal ) , dimension ( param ( instance ) % totalNslip , 4 ) :: &
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v !< velocities
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real ( pReal ) , dimension ( param ( instance ) % totalNslip , 2 ) :: &
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rhoDotDip !< evolution rate of dipole dislocation densities (screw and edge dipoles)
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ns = param ( instance ) % totalNslip
openmp parallelization working again (at least for j2 and nonlocal constitutive model).
In order to keep it like that, please follow these simple rules:
DON'T use implicit array subscripts:
example: real, dimension(3,3) :: A,B
A(:,2) = B(:,1) <--- DON'T USE
A(1:3,2) = B(1:3,1) <--- BETTER USE
In many cases the use of explicit array subscripts is inevitable for parallelization. Additionally, it is an easy means to prevent memory leaks.
Enclose all write statements with the following:
!$OMP CRITICAL (write2out)
<your write statement>
!$OMP END CRITICAL (write2out)
Whenever you change something in the code and are not sure if it affects parallelization and leads to nonconforming behavior, please ask me and/or Franz to check this.
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cs = 0
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associate ( prm = > param ( instance ) , dst = > microstructure ( instance ) , stt = > state ( instance ) , dot = > dotState ( instance ) )
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forall ( s = 1 : ns , t = 1 : 4 )
rhoSgl ( s , t + 4 ) = plasticState ( ph ) % State ( iRhoB ( s , t , instance ) , of )
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v ( s , t ) = plasticState ( ph ) % State ( iV ( s , t , instance ) , of )
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rhoDotSgl ( s , t + 4 ) = plasticState ( ph ) % dotState ( iRhoB ( s , t , instance ) , of )
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endforall
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forall ( s = 1 : ns , c = 1 : 2 )
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rhoDotDip ( s , c ) = plasticState ( ph ) % dotState ( iRhoD ( s , c , instance ) , of )
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endforall
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outputsLoop : do o = 1 , size ( param ( instance ) % outputID )
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select case ( param ( instance ) % outputID ( o ) )
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case ( rho_sgl_mob_edg_pos_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_mob_edg_pos ( : , of )
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cs = cs + ns
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case ( rho_sgl_imm_edg_pos_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_imm_edg_pos ( : , of )
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cs = cs + ns
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case ( rho_sgl_mob_edg_neg_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_mob_edg_neg ( : , of )
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cs = cs + ns
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case ( rho_sgl_imm_edg_neg_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_imm_edg_neg ( : , of )
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cs = cs + ns
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case ( rho_dip_edg_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_dip_edg ( : , of )
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cs = cs + ns
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case ( rho_sgl_mob_scr_pos_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_mob_scr_pos ( : , of )
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cs = cs + ns
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case ( rho_sgl_imm_scr_pos_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_imm_scr_pos ( : , of )
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cs = cs + ns
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case ( rho_sgl_mob_scr_neg_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_mob_scr_neg ( : , of )
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cs = cs + ns
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case ( rho_sgl_imm_scr_neg_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_sgl_imm_scr_neg ( : , of )
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cs = cs + ns
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case ( rho_dip_scr_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_dip_scr ( : , of )
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cs = cs + ns
case ( rho_forest_ID )
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postResults ( cs + 1 : cs + ns ) = stt % rho_forest ( : , of )
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cs = cs + ns
case ( resolvedstress_back_ID )
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postResults ( cs + 1 : cs + ns ) = dst % tau_back ( : , of )
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cs = cs + ns
case ( resistance_ID )
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postResults ( cs + 1 : cs + ns ) = dst % tau_Threshold ( : , of )
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cs = cs + ns
case ( rho_dot_sgl_ID )
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postResults ( cs + 1 : cs + ns ) = sum ( rhoDotSgl ( 1 : ns , 1 : 4 ) , 2 ) &
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+ sum ( rhoDotSgl ( 1 : ns , 5 : 8 ) * sign ( 1.0_pReal , rhoSgl ( 1 : ns , 5 : 8 ) ) , 2 )
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cs = cs + ns
case ( rho_dot_sgl_mobile_ID )
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postResults ( cs + 1 : cs + ns ) = sum ( rhoDotSgl ( 1 : ns , 1 : 4 ) , 2 )
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cs = cs + ns
case ( rho_dot_dip_ID )
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postResults ( cs + 1 : cs + ns ) = sum ( rhoDotDip , 2 )
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cs = cs + ns
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case ( v_edg_pos_ID )
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postResults ( cs + 1 : cs + ns ) = v ( 1 : ns , 1 )
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cs = cs + ns
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case ( v_edg_neg_ID )
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postResults ( cs + 1 : cs + ns ) = v ( 1 : ns , 2 )
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cs = cs + ns
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case ( v_scr_pos_ID )
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postResults ( cs + 1 : cs + ns ) = v ( 1 : ns , 3 )
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cs = cs + ns
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case ( v_scr_neg_ID )
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postResults ( cs + 1 : cs + ns ) = v ( 1 : ns , 4 )
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cs = cs + ns
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case ( accumulatedshear_ID )
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postResults ( cs + 1 : cs + ns ) = stt % accumulatedshear ( : , of )
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cs = cs + ns
end select
enddo outputsLoop
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end associate
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end function plastic_nonlocal_postResults
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!--------------------------------------------------------------------------------------------------
!> @brief returns copy of current dislocation densities from state
!> @details raw values is rectified
!--------------------------------------------------------------------------------------------------
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function getRho ( instance , of , ip , el )
integer , intent ( in ) :: instance , of , ip , el
real ( pReal ) , dimension ( param ( instance ) % totalNslip , 10 ) :: getRho
associate ( prm = > param ( instance ) )
getRho = reshape ( state ( instance ) % rho ( : , of ) , [ prm % totalNslip , 10 ] )
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! ensure positive densities (not for imm, they have a sign)
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getRho ( : , mob ) = max ( getRho ( : , mob ) , 0.0_pReal )
getRho ( : , dip ) = max ( getRho ( : , dip ) , 0.0_pReal )
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where ( abs ( getRho ) < max ( prm % significantN / IPvolume ( ip , el ) ** ( 2.0_pReal / 3.0_pReal ) , prm % significantRho ) ) &
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getRho = 0.0_pReal
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end associate
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end function getRho
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!--------------------------------------------------------------------------------------------------
!> @brief writes results to HDF5 output file
!--------------------------------------------------------------------------------------------------
subroutine plastic_nonlocal_results ( instance , group )
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#if defined(PETSc) || defined(DAMASK_HDF5)
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use results , only : &
results_writeDataset
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integer , intent ( in ) :: instance
character ( len = * ) :: group
integer :: o
associate ( prm = > param ( instance ) , stt = > state ( instance ) )
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outputsLoop : do o = 1 , size ( prm % outputID )
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select case ( prm % outputID ( o ) )
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case ( rho_sgl_mob_edg_pos_ID )
call results_writeDataset ( group , stt % rho_sgl_mob_edg_pos , 'rho_sgl_mob_edg_pos' , &
'positive mobile edge density' , '1/m²' )
case ( rho_sgl_imm_edg_pos_ID )
call results_writeDataset ( group , stt % rho_sgl_imm_edg_pos , 'rho_sgl_imm_edg_pos' , &
'positive immobile edge density' , '1/m²' )
case ( rho_sgl_mob_edg_neg_ID )
call results_writeDataset ( group , stt % rho_sgl_mob_edg_neg , 'rho_sgl_mob_edg_neg' , &
'negative mobile edge density' , '1/m²' )
case ( rho_sgl_imm_edg_neg_ID )
call results_writeDataset ( group , stt % rho_sgl_imm_edg_neg , 'rho_sgl_imm_edg_neg' , &
'negative immobile edge density' , '1/m²' )
case ( rho_dip_edg_ID )
call results_writeDataset ( group , stt % rho_dip_edg , 'rho_dip_edg' , &
'edge dipole density' , '1/m²' )
case ( rho_sgl_mob_scr_pos_ID )
call results_writeDataset ( group , stt % rho_sgl_mob_scr_pos , 'rho_sgl_mob_scr_pos' , &
'positive mobile screw density' , '1/m²' )
case ( rho_sgl_imm_scr_pos_ID )
call results_writeDataset ( group , stt % rho_sgl_imm_scr_pos , 'rho_sgl_imm_scr_pos' , &
'positive immobile screw density' , '1/m²' )
case ( rho_sgl_mob_scr_neg_ID )
call results_writeDataset ( group , stt % rho_sgl_mob_scr_neg , 'rho_sgl_mob_scr_neg' , &
'negative mobile screw density' , '1/m²' )
case ( rho_sgl_imm_scr_neg_ID )
call results_writeDataset ( group , stt % rho_sgl_imm_scr_neg , 'rho_sgl_imm_scr_neg' , &
'negative immobile screw density' , '1/m²' )
case ( rho_dip_scr_ID )
call results_writeDataset ( group , stt % rho_dip_scr , 'rho_dip_scr' , &
'screw dipole density' , '1/m²' )
case ( rho_forest_ID )
call results_writeDataset ( group , stt % rho_forest , 'rho_forest' , &
'forest density' , '1/m²' )
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end select
enddo outputsLoop
end associate
#else
integer , intent ( in ) :: instance
character ( len = * ) :: group
#endif
end subroutine plastic_nonlocal_results
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end module plastic_nonlocal
