DAMASK_EICMD/src/plastic_disloUCLA.f90

792 lines
36 KiB
Fortran
Raw Normal View History

!--------------------------------------------------------------------------------------------------
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @author David Cereceda, Lawrence Livermore National Laboratory
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
!> @brief material subroutine incoprorating dislocation and twinning physics
!> @details to be done
!--------------------------------------------------------------------------------------------------
2015-01-21 20:44:00 +05:30
module plastic_disloUCLA
use prec, only: &
pReal, &
pInt
implicit none
private
integer(pInt), dimension(:,:), allocatable, target, public :: &
2016-01-16 12:36:34 +05:30
plastic_disloUCLA_sizePostResult !< size of each post result output
character(len=64), dimension(:,:), allocatable, target, public :: &
2016-01-16 12:36:34 +05:30
plastic_disloUCLA_output !< name of each post result output
real(pReal), parameter, private :: &
2016-04-25 02:06:35 +05:30
kB = 1.38e-23_pReal !< Boltzmann constant in J/Kelvin
2018-12-05 03:00:07 +05:30
enum, bind(c)
enumerator :: undefined_ID, &
2018-11-28 10:29:03 +05:30
rho_ID, &
rhoDip_ID, &
shearrate_ID, &
accumulatedshear_ID, &
mfp_ID, &
resolvedstress_ID, &
thresholdstress_ID, &
dipoledistance_ID, &
stressexponent_ID
end enum
2018-11-28 00:30:45 +05:30
type, private :: tParameters
real(pReal) :: &
2018-11-29 13:14:31 +05:30
aTolRho, &
2018-11-29 15:01:02 +05:30
grainSize, &
2018-12-09 18:59:19 +05:30
SolidSolutionStrength, & !< Strength due to elements in solid solution
2018-12-03 15:55:29 +05:30
mu, &
2018-12-05 02:03:32 +05:30
D0, & !< prefactor for self-diffusion coefficient
Qsd !< activation energy for dislocation climb
2018-11-28 00:30:45 +05:30
real(pReal), allocatable, dimension(:) :: &
2018-11-28 10:29:03 +05:30
rho0, & !< initial edge dislocation density per slip system for each family and instance
rhoDip0, & !< initial edge dipole density per slip system for each family and instance
burgers, & !< absolute length of burgers vector [m] for each slip system and instance
2018-12-09 18:59:19 +05:30
nonSchmidCoeff, &
minDipDistance, &
CLambda, & !< Adj. parameter for distance between 2 forest dislocations for each slip system and instance
atomicVolume, &
!* mobility law parameters
2018-11-28 10:29:03 +05:30
H0kp, & !< activation energy for glide [J] for each slip system and instance
v0, & !< dislocation velocity prefactor [m/s] for each family and instance
p, & !< p-exponent in glide velocity
2018-12-05 03:00:07 +05:30
q, & !< q-exponent in glide velocity
2018-12-09 18:59:19 +05:30
B, & !< friction coeff. B (kMC)
2018-12-05 03:00:07 +05:30
kink_height, & !< height of the kink pair
kink_width, & !< width of the kink pair
2018-12-09 18:59:19 +05:30
omega, & !< attempt frequency for kink pair nucleation
tau_Peierls
2018-11-28 00:30:45 +05:30
real(pReal), allocatable, dimension(:,:) :: &
2018-12-09 18:59:19 +05:30
interaction_SlipSlip, & !< slip resistance from slip activity
forestProjectionEdge
2018-11-28 00:30:45 +05:30
real(pReal), allocatable, dimension(:,:,:) :: &
Schmid_slip, &
Schmid_twin, &
nonSchmid_pos, &
nonSchmid_neg
integer(pInt) :: &
totalNslip !< total number of active slip system
integer(pInt), allocatable, dimension(:) :: &
Nslip !< number of active slip systems for each family
integer(kind(undefined_ID)), allocatable, dimension(:) :: &
outputID !< ID of each post result output
2018-12-04 04:36:46 +05:30
logical :: &
dipoleformation
2018-11-28 00:30:45 +05:30
end type !< container type for internal constitutive parameters
type(tParameters), dimension(:), allocatable, private :: param !< containers of constitutive parameters (len Ninstance)
2018-12-05 03:00:07 +05:30
type, private :: tDisloUCLAState
2018-12-09 18:59:19 +05:30
real(pReal), pointer, dimension(:,:) :: &
rhoEdge, &
rhoEdgeDip, &
accshear_slip, &
whole
2018-12-05 03:00:07 +05:30
end type
2018-12-05 03:00:07 +05:30
type, private :: tDisloUCLAdependentState
real(pReal), allocatable, dimension(:,:) :: &
mfp, &
threshold_stress
2018-12-05 03:00:07 +05:30
end type tDisloUCLAdependentState
type(tDisloUCLAState ), allocatable, dimension(:), private :: &
state, &
dotState
2018-12-05 03:00:07 +05:30
type(tDisloUCLAdependentState), allocatable, dimension(:), private :: &
dependentState
public :: &
2015-01-21 20:44:00 +05:30
plastic_disloUCLA_init, &
plastic_disloUCLA_dependentState, &
2015-01-21 20:44:00 +05:30
plastic_disloUCLA_LpAndItsTangent, &
plastic_disloUCLA_dotState, &
plastic_disloUCLA_postResults
private :: &
2018-11-29 13:51:58 +05:30
kinetics
contains
!--------------------------------------------------------------------------------------------------
!> @brief module initialization
!> @details reads in material parameters, allocates arrays, and does sanity checks
!--------------------------------------------------------------------------------------------------
2018-12-05 02:03:32 +05:30
subroutine plastic_disloUCLA_init()
#if defined(__GFORTRAN__) || __INTEL_COMPILER >= 1800
use, intrinsic :: iso_fortran_env, only: &
compiler_version, &
compiler_options
#endif
use debug, only: &
debug_level,&
debug_constitutive,&
debug_levelBasic
use math, only: &
math_mul3x3, &
math_expand
use IO, only: &
IO_error, &
2018-11-30 13:06:56 +05:30
IO_timeStamp
use material, only: &
phase_plasticity, &
phase_plasticityInstance, &
phase_Noutput, &
2015-01-15 16:26:15 +05:30
PLASTICITY_DISLOUCLA_label, &
PLASTICITY_DISLOUCLA_ID, &
material_phase, &
2018-11-27 23:58:00 +05:30
plasticState, &
2018-12-05 02:03:32 +05:30
material_allocatePlasticState
use config, only: &
2018-11-28 00:30:45 +05:30
MATERIAL_partPhase, &
config_phase
use lattice
2018-12-05 03:00:07 +05:30
implicit none
2018-12-09 22:06:01 +05:30
integer(pInt) :: Ninstance,&
2018-12-05 03:00:07 +05:30
f,j,k,o, i, &
outputSize, &
offset_slip, index_myFamily, index_otherFamily, &
2018-12-05 03:00:07 +05:30
startIndex, endIndex, p, &
sizeState, sizeDotState, &
2018-12-09 22:06:01 +05:30
NipcMyPhase
character(len=65536) :: &
2018-12-03 15:55:29 +05:30
structure = ''
2018-11-28 10:29:03 +05:30
character(len=65536), dimension(:), allocatable :: outputs
integer(kind(undefined_ID)) :: outputID
2018-11-28 00:30:45 +05:30
integer(pInt), dimension(0), parameter :: emptyIntArray = [integer(pInt)::]
real(pReal), dimension(0), parameter :: emptyRealArray = [real(pReal)::]
character(len=65536), dimension(0), parameter :: emptyStringArray = [character(len=65536)::]
2018-12-05 03:00:07 +05:30
write(6,'(/,a)') ' <<<+- constitutive_'//PLASTICITY_DISLOUCLA_label//' init -+>>>'
write(6,'(/,a)') ' Cereceda et al., International Journal of Plasticity 78, 2016, 242-256'
2018-04-09 18:34:37 +05:30
write(6,'(/,a)') ' http://dx.doi.org/10.1016/j.ijplas.2015.09.002'
write(6,'(a15,a)') ' Current time: ',IO_timeStamp()
#include "compilation_info.f90"
2018-12-05 03:00:07 +05:30
2018-12-09 22:06:01 +05:30
Ninstance = int(count(phase_plasticity == PLASTICITY_DISLOUCLA_ID),pInt)
if (Ninstance == 0_pInt) return
2018-12-05 03:00:07 +05:30
if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0_pInt) &
2018-12-09 22:06:01 +05:30
write(6,'(a16,1x,i5,/)') '# instances:',Ninstance
2018-12-09 22:06:01 +05:30
allocate(plastic_disloUCLA_sizePostResult(maxval(phase_Noutput),Ninstance),source=0_pInt)
allocate(plastic_disloUCLA_output(maxval(phase_Noutput),Ninstance))
2015-01-21 20:44:00 +05:30
plastic_disloUCLA_output = ''
2018-12-03 15:55:29 +05:30
2018-12-09 22:06:01 +05:30
allocate(param(Ninstance))
allocate(state(Ninstance))
allocate(dotState(Ninstance))
allocate(dependentState(Ninstance))
2018-11-28 00:30:45 +05:30
2018-12-05 03:00:07 +05:30
do p = 1_pInt, size(phase_plasticityInstance)
2018-11-28 00:30:45 +05:30
if (phase_plasticity(p) /= PLASTICITY_DISLOUCLA_ID) cycle
associate(prm => param(phase_plasticityInstance(p)), &
dot => dotState(phase_plasticityInstance(p)), &
2018-12-04 04:36:46 +05:30
stt => state(phase_plasticityInstance(p)), &
2018-12-05 03:00:07 +05:30
dst => dependentState(phase_plasticityInstance(p)))
2018-11-28 00:30:45 +05:30
structure = config_phase(p)%getString('lattice_structure')
2018-11-30 12:55:23 +05:30
prm%mu = lattice_mu(p)
2018-11-28 00:30:45 +05:30
prm%aTolRho = config_phase(p)%getFloat('atol_rho')
2018-11-28 00:30:45 +05:30
!--------------------------------------------------------------------------------------------------
! slip related parameters
prm%Nslip = config_phase(p)%getInts('nslip',defaultVal=emptyIntArray)
prm%totalNslip = sum(prm%Nslip)
slipActive: if (prm%totalNslip > 0_pInt) then
prm%Schmid_slip = lattice_SchmidMatrix_slip(prm%Nslip,structure(1:3),&
config_phase(p)%getFloat('c/a',defaultVal=0.0_pReal))
if(structure=='bcc') then
prm%nonSchmidCoeff = config_phase(p)%getFloats('nonschmid_coefficients',&
defaultVal = emptyRealArray)
prm%nonSchmid_pos = lattice_nonSchmidMatrix(prm%Nslip,prm%nonSchmidCoeff,+1_pInt)
prm%nonSchmid_neg = lattice_nonSchmidMatrix(prm%Nslip,prm%nonSchmidCoeff,-1_pInt)
else
prm%nonSchmid_pos = prm%Schmid_slip
prm%nonSchmid_neg = prm%Schmid_slip
endif
prm%interaction_SlipSlip = lattice_interaction_SlipSlip(prm%Nslip, &
config_phase(p)%getFloats('interaction_slipslip'), &
structure(1:3))
2018-12-09 20:28:51 +05:30
prm%rho0 = config_phase(p)%getFloats('rhoedge0', requiredShape=shape(prm%Nslip))
prm%rhoDip0 = config_phase(p)%getFloats('rhoedgedip0', requiredShape=shape(prm%Nslip))
prm%burgers = config_phase(p)%getFloats('slipburgers', requiredShape=shape(prm%Nslip))
prm%H0kp = config_phase(p)%getFloats('qedge', requiredShape=shape(prm%Nslip))
prm%v0 = config_phase(p)%getFloats('v0', requiredShape=shape(prm%Nslip))
prm%clambda = config_phase(p)%getFloats('clambdaslip', requiredShape=shape(prm%Nslip))
prm%tau_Peierls = config_phase(p)%getFloats('tau_peierls', requiredShape=shape(prm%Nslip))
prm%p = config_phase(p)%getFloats('p_slip', requiredShape=shape(prm%Nslip), &
defaultVal=[(1.0_pReal,i=1_pInt,size(prm%Nslip))])
prm%q = config_phase(p)%getFloats('q_slip', requiredShape=shape(prm%Nslip), &
defaultVal=[(1.0_pReal,i=1_pInt,size(prm%Nslip))])
prm%kink_height = config_phase(p)%getFloats('kink_height', requiredShape=shape(prm%Nslip))
prm%kink_width = config_phase(p)%getFloats('kink_width', requiredShape=shape(prm%Nslip))
prm%omega = config_phase(p)%getFloats('omega', requiredShape=shape(prm%Nslip))
prm%B = config_phase(p)%getFloats('friction_coeff', requiredShape=shape(prm%Nslip))
2018-11-29 15:01:02 +05:30
prm%SolidSolutionStrength = config_phase(p)%getFloat('solidsolutionstrength')
2018-12-09 20:28:51 +05:30
prm%grainSize = config_phase(p)%getFloat('grainsize')
prm%D0 = config_phase(p)%getFloat('d0')
prm%Qsd = config_phase(p)%getFloat('qsd')
prm%atomicVolume = config_phase(p)%getFloat('catomicvolume') * prm%burgers**3.0_pReal
prm%minDipDistance = config_phase(p)%getFloat('cedgedipmindistance') * prm%burgers
prm%dipoleformation = config_phase(p)%getFloat('dipoleformationfactor') > 0.0_pReal !should be on by default
2018-11-29 15:01:02 +05:30
! expand: family => system
2018-12-09 22:05:48 +05:30
prm%rho0 = math_expand(prm%rho0, prm%Nslip)
prm%rhoDip0 = math_expand(prm%rhoDip0, prm%Nslip)
prm%q = math_expand(prm%q, prm%Nslip)
prm%p = math_expand(prm%p, prm%Nslip)
prm%H0kp = math_expand(prm%H0kp, prm%Nslip)
prm%burgers = math_expand(prm%burgers, prm%Nslip)
prm%kink_height = math_expand(prm%kink_height, prm%Nslip)
prm%kink_width = math_expand(prm%kink_width, prm%Nslip)
prm%omega = math_expand(prm%omega, prm%Nslip)
prm%tau_Peierls = math_expand(prm%tau_Peierls, prm%Nslip)
prm%v0 = math_expand(prm%v0, prm%Nslip)
prm%B = math_expand(prm%B, prm%Nslip)
prm%clambda = math_expand(prm%clambda, prm%Nslip)
prm%atomicVolume = math_expand(prm%atomicVolume, prm%Nslip)
prm%minDipDistance = math_expand(prm%minDipDistance, prm%Nslip)
2018-12-03 15:55:29 +05:30
!if (plastic_disloUCLA_CAtomicVolume(instance) <= 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='cAtomicVolume ('//PLASTICITY_DISLOUCLA_label//')')
2018-12-05 00:05:29 +05:30
! if (prm%D0 <= 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='D0 ('//PLASTICITY_DISLOUCLA_label//')')
! if (plastic_disloUCLA_Qsd(instance) <= 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='Qsd ('//PLASTICITY_DISLOUCLA_label//')')
! if (plastic_disloUCLA_aTolRho(instance) <= 0.0_pReal) &
2018-12-05 03:00:07 +05:30
! call IO_error(211_pInt,el=instance,ext_msg='aTolRho ('//PLASTICITY_DISLOUCLA_label//')')
!if (plastic_disloUCLA_rhoEdge0(f,instance) < 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='rhoEdge0 ('//PLASTICITY_DISLOUCLA_label//')')
!if (plastic_disloUCLA_rhoEdgeDip0(f,instance) < 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='rhoEdgeDip0 ('//PLASTICITY_DISLOUCLA_label//')')
!if (plastic_disloUCLA_burgersPerSlipFamily(f,instance) <= 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='slipBurgers ('//PLASTICITY_DISLOUCLA_label//')')
!if (plastic_disloUCLA_v0PerSlipFamily(f,instance) <= 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='v0 ('//PLASTICITY_DISLOUCLA_label//')')
!if (plastic_disloUCLA_tau_peierlsPerSlipFamily(f,instance) < 0.0_pReal) &
! call IO_error(211_pInt,el=instance,ext_msg='tau_peierls ('//PLASTICITY_DISLOUCLA_label//')')
else slipActive
allocate(prm%rho0(0))
allocate(prm%rhoDip0(0))
2018-11-28 00:30:45 +05:30
endif slipActive
2018-11-28 10:29:03 +05:30
#if defined(__GFORTRAN__)
2018-12-05 03:00:07 +05:30
outputs = ['GfortranBug86277']
outputs = config_phase(p)%getStrings('(output)',defaultVal=outputs)
if (outputs(1) == 'GfortranBug86277') outputs = emptyStringArray
2018-11-28 10:29:03 +05:30
#else
2018-12-05 03:00:07 +05:30
outputs = config_phase(p)%getStrings('(output)',defaultVal=emptyStringArray)
2018-11-28 10:29:03 +05:30
#endif
allocate(prm%outputID(0))
2018-12-05 03:00:07 +05:30
2018-11-28 10:29:03 +05:30
do i = 1_pInt, size(outputs)
outputID = undefined_ID
outputSize = prm%totalNslip
select case(trim(outputs(i)))
2018-12-05 03:00:07 +05:30
case ('edge_density')
outputID = merge(rho_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('dipole_density')
outputID = merge(rhoDip_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('shear_rate','shearrate','shear_rate_slip','shearrate_slip')
outputID = merge(shearrate_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('accumulated_shear','accumulatedshear','accumulated_shear_slip')
outputID = merge(accumulatedshear_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('mfp','mfp_slip')
outputID = merge(mfp_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('resolved_stress','resolved_stress_slip')
outputID = merge(resolvedstress_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('threshold_stress','threshold_stress_slip')
outputID = merge(thresholdstress_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('edge_dipole_distance')
outputID = merge(dipoleDistance_ID,undefined_ID,prm%totalNslip>0_pInt)
case ('stress_exponent')
outputID = merge(stressexponent_ID,undefined_ID,prm%totalNslip>0_pInt)
2018-11-28 10:29:03 +05:30
end select
2018-11-28 21:15:45 +05:30
2018-12-05 03:00:07 +05:30
if (outputID /= undefined_ID) then
2018-11-28 21:15:45 +05:30
plastic_disloUCLA_output(i,phase_plasticityInstance(p)) = outputs(i)
2018-12-05 03:00:07 +05:30
plastic_disloUCLA_sizePostResult(i,phase_plasticityInstance(p)) = outputSize
2018-11-28 21:15:45 +05:30
prm%outputID = [prm%outputID, outputID]
endif
2018-12-05 03:00:07 +05:30
enddo
2018-12-09 22:06:01 +05:30
NipcMyPhase=count(material_phase==p)
!--------------------------------------------------------------------------------------------------
! allocate state arrays
2016-01-16 12:36:34 +05:30
2018-12-05 03:00:07 +05:30
sizeDotState = int(size(['rhoEdge ','rhoEdgeDip ','accshearslip']),pInt) * prm%totalNslip
sizeState = sizeDotState
2016-01-16 12:36:34 +05:30
2018-12-09 22:06:01 +05:30
call material_allocatePlasticState(p,NipcMyPhase,sizeState,sizeDotState,0_pInt, &
2018-12-04 04:36:46 +05:30
prm%totalNslip,0_pInt,0_pInt)
2018-11-27 23:58:00 +05:30
2018-12-05 03:00:07 +05:30
plasticState(p)%sizePostResults = sum(plastic_disloUCLA_sizePostResult(:,phase_plasticityInstance(p)))
2018-12-09 19:19:08 +05:30
allocate(prm%forestProjectionEdge(prm%totalNslip,prm%totalNslip),source = 0.0_pReal)
i = 0_pInt
mySlipFamilies: do f = 1_pInt,size(prm%Nslip,1)
index_myFamily = sum(prm%Nslip(1:f-1_pInt))
slipSystemsLoop: do j = 1_pInt,prm%Nslip(f)
i = i + 1_pInt
do o = 1_pInt, size(prm%Nslip,1)
index_otherFamily = sum(prm%Nslip(1:o-1_pInt))
do k = 1_pInt,prm%Nslip(o) ! loop over (active) systems in other family (slip)
prm%forestProjectionEdge(index_myFamily+j,index_otherFamily+k) = &
abs(math_mul3x3(lattice_sn(:,sum(lattice_NslipSystem(1:f-1,p))+j,p), &
lattice_st(:,sum(lattice_NslipSystem(1:o-1,p))+k,p)))
enddo; enddo
enddo slipSystemsLoop
enddo mySlipFamilies
2018-12-05 03:00:07 +05:30
offset_slip = 2_pInt*plasticState(p)%nSlip
plasticState(p)%slipRate => &
2018-12-09 22:06:01 +05:30
plasticState(p)%dotState(offset_slip+1:offset_slip+plasticState(p)%nSlip,1:NipcMyPhase)
2018-12-05 03:00:07 +05:30
plasticState(p)%accumulatedSlip => &
2018-12-09 22:06:01 +05:30
plasticState(p)%state (offset_slip+1:offset_slip+plasticState(p)%nSlip,1:NipcMyPhase)
2018-12-05 03:00:07 +05:30
startIndex=1_pInt
endIndex=prm%totalNslip
stt%rhoEdge=>plasticState(p)%state(startIndex:endIndex,:)
2018-12-09 22:06:01 +05:30
stt%rhoEdge= spread(prm%rho0,2,NipcMyPhase)
2018-12-05 03:00:07 +05:30
dot%rhoEdge=>plasticState(p)%dotState(startIndex:endIndex,:)
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolRho
2016-04-25 02:06:35 +05:30
2018-12-05 03:00:07 +05:30
startIndex=endIndex+1_pInt
endIndex=endIndex+prm%totalNslip
stt%rhoEdgeDip=>plasticState(p)%state(startIndex:endIndex,:)
2018-12-09 22:06:01 +05:30
stt%rhoEdgeDip= spread(prm%rhoDip0,2,NipcMyPhase)
2018-12-05 03:00:07 +05:30
dot%rhoEdgeDip=>plasticState(p)%dotState(startIndex:endIndex,:)
plasticState(p)%aTolState(startIndex:endIndex) = prm%aTolRho
2016-04-25 02:06:35 +05:30
2018-12-05 03:00:07 +05:30
startIndex=endIndex+1_pInt
endIndex=endIndex+prm%totalNslip
stt%accshear_slip=>plasticState(p)%state(startIndex:endIndex,:)
dot%accshear_slip=>plasticState(p)%dotState(startIndex:endIndex,:)
plasticState(p)%aTolState(startIndex:endIndex) = 1e6_pReal
2016-04-25 02:06:35 +05:30
2018-12-05 03:00:07 +05:30
dot%whole => plasticState(p)%dotState
2018-11-30 14:34:41 +05:30
2018-12-09 22:06:01 +05:30
allocate(dst%mfp(prm%totalNslip,NipcMyPhase),source=0.0_pReal)
allocate(dst%threshold_stress(prm%totalNslip,NipcMyPhase),source=0.0_pReal)
2018-12-05 03:00:07 +05:30
plasticState(p)%state0 = plasticState(p)%state ! ToDo: this could be done centrally
end associate
2018-12-04 04:36:46 +05:30
enddo
2015-01-21 20:44:00 +05:30
end subroutine plastic_disloUCLA_init
!--------------------------------------------------------------------------------------------------
!> @brief calculates derived quantities from state
!--------------------------------------------------------------------------------------------------
2018-12-05 03:00:07 +05:30
subroutine plastic_disloUCLA_dependentState(instance,of)
implicit none
integer(pInt), intent(in) :: instance, of
integer(pInt) :: &
2018-12-05 03:00:07 +05:30
i
real(pReal), dimension(param(instance)%totalNslip) :: &
2018-12-05 01:35:34 +05:30
invLambdaSlip ! 1/mean free distance between 2 forest dislocations seen by a moving dislocation
2018-12-05 03:00:07 +05:30
associate(prm => param(instance), stt => state(instance),dst => dependentState(instance))
forall (i = 1_pInt:prm%totalNslip)
invLambdaSlip(i) = sqrt(dot_product(stt%rhoEdge(:,of)+stt%rhoEdgeDip(:,of), &
2018-12-09 19:19:08 +05:30
prm%forestProjectionEdge(:,i))) &
2018-12-05 03:00:07 +05:30
/ prm%Clambda(i)
dst%threshold_stress(i,of) = prm%mu*prm%burgers(i) &
2018-12-05 01:35:34 +05:30
* sqrt(dot_product(stt%rhoEdge(:,of)+stt%rhoEdgeDip(:,of), &
2018-12-05 03:00:07 +05:30
prm%interaction_SlipSlip(i,:)))
end forall
dst%mfp(:,of) = prm%grainSize/(1.0_pReal+prm%grainSize*invLambdaSlip)
end associate
2018-11-29 13:14:31 +05:30
end subroutine plastic_disloUCLA_dependentState
!--------------------------------------------------------------------------------------------------
!> @brief calculates plastic velocity gradient and its tangent
!--------------------------------------------------------------------------------------------------
2018-12-09 22:05:48 +05:30
pure subroutine plastic_disloUCLA_LpAndItsTangent(Lp,dLp_dMp,Mp,Temperature,instance,of)
2018-12-05 03:00:07 +05:30
implicit none
2018-12-05 02:03:32 +05:30
integer(pInt), intent(in) :: instance, of
real(pReal), intent(in) :: Temperature
2018-11-28 11:14:32 +05:30
real(pReal), dimension(3,3), intent(in) :: Mp
real(pReal), dimension(3,3), intent(out) :: Lp
2018-11-28 11:14:32 +05:30
real(pReal), dimension(3,3,3,3), intent(out) :: dLp_dMp
2018-12-05 02:03:32 +05:30
integer(pInt) :: i,k,l,m,n
2018-11-28 00:19:04 +05:30
2018-12-05 02:03:32 +05:30
real(pReal), dimension(param(instance)%totalNslip) :: &
2018-11-27 23:31:55 +05:30
gdot_slip_pos,gdot_slip_neg,tau_slip_pos,tau_slip_neg,dgdot_dtauslip_pos,dgdot_dtauslip_neg
2018-12-05 03:00:07 +05:30
2018-12-09 19:30:37 +05:30
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
2018-12-05 03:00:07 +05:30
Lp = 0.0_pReal
2018-11-28 11:14:32 +05:30
dLp_dMp = 0.0_pReal
2018-12-05 03:00:07 +05:30
2018-12-09 19:19:08 +05:30
call kinetics(prm,stt,dst,Mp,Temperature,of, &
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg)
slipSystems: do i = 1_pInt, prm%totalNslip
Lp = Lp + (gdot_slip_pos(i)+gdot_slip_neg(i))*prm%Schmid_slip(1:3,1:3,i)
forall (k=1_pInt:3_pInt,l=1_pInt:3_pInt,m=1_pInt:3_pInt,n=1_pInt:3_pInt) &
dLp_dMp(k,l,m,n) = dLp_dMp(k,l,m,n) &
+ dgdot_dtauslip_pos(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_pos(m,n,i) &
+ dgdot_dtauslip_neg(i) * prm%Schmid_slip(k,l,i) * prm%nonSchmid_neg(m,n,i)
enddo slipSystems
2018-12-05 02:03:32 +05:30
end associate
Lp = 0.5_pReal * Lp
dLp_dMp = 0.5_pReal * dLp_dMp
2015-01-21 20:44:00 +05:30
end subroutine plastic_disloUCLA_LpAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief calculates the rate of change of microstructure
!--------------------------------------------------------------------------------------------------
2018-11-30 14:34:41 +05:30
subroutine plastic_disloUCLA_dotState(Mp,Temperature,instance,of)
use prec, only: &
2016-05-29 14:15:03 +05:30
tol_math_check, &
dEq0
use math, only: &
2018-12-05 01:20:02 +05:30
PI, &
math_clip
implicit none
2018-11-28 11:14:32 +05:30
real(pReal), dimension(3,3), intent(in):: &
Mp !< 2nd Piola Kirchhoff stress tensor in Mandel notation
real(pReal), intent(in) :: &
temperature !< temperature at integration point
integer(pInt), intent(in) :: &
2018-12-05 01:20:02 +05:30
instance, of
real(pReal) :: &
2018-12-05 01:20:02 +05:30
VacancyDiffusion
2018-12-09 22:05:48 +05:30
real(pReal), dimension(param(instance)%totalNslip) :: &
2018-11-27 23:11:33 +05:30
gdot_slip_pos, gdot_slip_neg,&
tau_slip_pos,&
2018-11-27 23:23:01 +05:30
tau_slip_neg, &
2018-12-05 01:20:02 +05:30
dgdot_dtauslip_neg,dgdot_dtauslip_pos,DotRhoDipFormation, ClimbVelocity, EdgeDipDistance, &
DotRhoEdgeDipClimb
2016-04-25 02:06:35 +05:30
2018-12-05 03:00:07 +05:30
associate(prm => param(instance), stt => state(instance),dot => dotState(instance), dst => dependentState(instance))
2018-12-05 00:05:29 +05:30
2018-12-09 19:19:08 +05:30
call kinetics(prm,stt,dst,Mp,Temperature,of, &
2018-11-27 23:23:01 +05:30
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg)
2018-12-05 03:00:07 +05:30
2018-12-05 00:05:29 +05:30
dot%whole(:,of) = 0.0_pReal
dot%accshear_slip(:,of) = (gdot_slip_pos+gdot_slip_neg)*0.5_pReal
2018-12-05 02:03:32 +05:30
VacancyDiffusion = prm%D0*exp(-prm%Qsd/(kB*Temperature))
2018-12-05 01:20:02 +05:30
2018-12-05 02:03:32 +05:30
where(dEq0(tau_slip_pos))
2018-12-05 03:00:07 +05:30
EdgeDipDistance = dst%mfp(:,of) !ToDo MD@FR: correct? was not handled properly before
2018-12-05 01:20:02 +05:30
DotRhoDipFormation = 0.0_pReal
DotRhoEdgeDipClimb = 0.0_pReal
else where
EdgeDipDistance = math_clip((3.0_pReal*prm%mu*prm%burgers)/(16.0_pReal*PI*abs(tau_slip_pos)), &
prm%minDipDistance, & ! lower limit
2018-12-05 03:00:07 +05:30
dst%mfp(:,of)) ! upper limit
2018-12-05 01:20:02 +05:30
DotRhoDipFormation = merge(((2.0_pReal*EdgeDipDistance)/prm%burgers)* stt%rhoEdge(:,of)*abs(dot%accshear_slip(:,of)), &
0.0_pReal, &
prm%dipoleformation)
2018-12-09 19:19:08 +05:30
ClimbVelocity = (3.0_pReal*prm%mu*VacancyDiffusion*prm%atomicVolume/(2.0_pReal*pi*kB*Temperature)) &
2018-12-05 01:20:02 +05:30
* (1.0_pReal/(EdgeDipDistance+prm%minDipDistance))
DotRhoEdgeDipClimb = (4.0_pReal*ClimbVelocity*stt%rhoEdgeDip(:,of))/(EdgeDipDistance-prm%minDipDistance)
end where
2018-11-28 00:19:04 +05:30
2018-12-05 03:00:07 +05:30
dot%rhoEdge(:,of) = abs(dot%accshear_slip(:,of))/(prm%burgers*dst%mfp(:,of)) & ! multiplication
2018-12-05 01:35:34 +05:30
- DotRhoDipFormation &
2018-12-09 19:19:08 +05:30
- (2.0_pReal*prm%minDipDistance)/prm%burgers*stt%rhoEdge(:,of)*abs(dot%accshear_slip(:,of)) !* Spontaneous annihilation of 2 single edge dislocations
2018-12-05 01:35:34 +05:30
dot%rhoEdgeDip(:,of) = DotRhoDipFormation &
2018-12-09 19:19:08 +05:30
- (2.0_pReal*prm%minDipDistance)/prm%burgers* stt%rhoEdgeDip(:,of)*abs(dot%accshear_slip(:,of)) & !* Spontaneous annihilation of a single edge dislocation with a dipole constituent
2018-12-05 01:35:34 +05:30
- DotRhoEdgeDipClimb
2018-11-28 00:19:04 +05:30
end associate
2018-12-05 03:00:07 +05:30
2015-01-21 20:44:00 +05:30
end subroutine plastic_disloUCLA_dotState
2018-12-05 03:00:07 +05:30
!--------------------------------------------------------------------------------------------------
!> @brief return array of constitutive results
!--------------------------------------------------------------------------------------------------
2018-11-30 14:34:41 +05:30
function plastic_disloUCLA_postResults(Mp,Temperature,instance,of) result(postResults)
use prec, only: &
2017-11-21 04:13:06 +05:30
dEq, dNeq0
use math, only: &
2018-11-28 11:14:32 +05:30
pi, &
2018-12-03 15:18:37 +05:30
math_mul33xx33
implicit none
2018-12-03 15:18:37 +05:30
real(pReal), dimension(3,3), intent(in) :: &
Mp !< Mandel stress
real(pReal), intent(in) :: &
Temperature !< Mandel stress
integer(pInt), intent(in) :: &
instance, &
of
2018-12-03 15:18:37 +05:30
real(pReal), dimension(sum(plastic_disloUCLA_sizePostResult(:,instance))) :: &
postResults
integer(pInt) :: &
2018-12-03 15:18:37 +05:30
o,c,i
real(pReal), dimension(param(instance)%totalNslip) :: &
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos, &
gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg
2018-11-30 14:34:41 +05:30
2018-12-09 19:19:08 +05:30
associate(prm => param(instance), stt => state(instance), dst => dependentState(instance))
2018-11-30 14:34:41 +05:30
postResults = 0.0_pReal
2018-12-03 15:18:37 +05:30
c = 0_pInt
outputsLoop: do o = 1_pInt,size(prm%outputID)
select case(prm%outputID(o))
case (rho_ID)
postResults(c+1_pInt:c+prm%totalNslip) = stt%rhoEdge(1_pInt:prm%totalNslip,of)
case (rhoDip_ID)
postResults(c+1_pInt:c+prm%totalNslip) = stt%rhoEdgeDip(1_pInt:prm%totalNslip,of)
case (shearrate_ID,stressexponent_ID)
2018-12-09 19:19:08 +05:30
call kinetics(prm,stt,dst,Mp,Temperature,of, &
2018-12-03 15:18:37 +05:30
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg)
if (prm%outputID(o) == shearrate_ID) then
postResults(c+1:c+prm%totalNslip) = (gdot_slip_pos + gdot_slip_neg)*0.5_pReal
elseif(prm%outputID(o) == stressexponent_ID) then
where (dNeq0(gdot_slip_pos+gdot_slip_neg))
postResults(c+1_pInt:c + prm%totalNslip) = (tau_slip_pos+tau_slip_neg) * 0.5_pReal &
/ (gdot_slip_pos+gdot_slip_neg) &
* (dgdot_dtauslip_pos+dgdot_dtauslip_neg)
else where
postResults(c+1_pInt:c + prm%totalNslip) = 0.0_pReal
end where
endif
case (accumulatedshear_ID)
postResults(c+1_pInt:c+prm%totalNslip) = stt%accshear_slip(1_pInt:prm%totalNslip, of)
case (mfp_ID)
2018-12-05 03:00:07 +05:30
postResults(c+1_pInt:c+prm%totalNslip) = dst%mfp(1_pInt:prm%totalNslip, of)
2018-12-03 15:18:37 +05:30
case (resolvedstress_ID)
do i = 1_pInt, prm%totalNslip
postResults(c+i) =math_mul33xx33(Mp,prm%nonSchmid_pos(1:3,1:3,i))
enddo
case (thresholdstress_ID)
2018-12-05 03:00:07 +05:30
postResults(c+1_pInt:c+prm%totalNslip) = dst%threshold_stress(1_pInt:prm%totalNslip,of)
2018-12-03 15:18:37 +05:30
case (dipoleDistance_ID)
do i = 1_pInt, prm%totalNslip
if (dNeq0(abs(math_mul33xx33(Mp,prm%nonSchmid_pos(1:3,1:3,i))))) then
postResults(c+i) = (3.0_pReal*prm%mu*prm%burgers(i)) &
/ (16.0_pReal*pi*abs(math_mul33xx33(Mp,prm%nonSchmid_pos(1:3,1:3,i))))
else
postResults(c+i) = huge(1.0_pReal)
endif
2018-12-09 18:59:19 +05:30
postResults(c+i)=min(postResults(c+i),dst%mfp(i,of))
2018-12-03 15:18:37 +05:30
enddo
end select
c = c + prm%totalNslip
enddo outputsLoop
end associate
end function plastic_disloUCLA_postResults
!--------------------------------------------------------------------------------------------------
!> @brief return array of constitutive results
!--------------------------------------------------------------------------------------------------
2018-12-09 22:05:48 +05:30
pure subroutine kinetics(prm,stt,dst,Mp,Temperature,of, &
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg)
use prec, only: &
tol_math_check, &
dEq, dNeq0
use math, only: &
2018-11-28 11:14:32 +05:30
pi, &
math_mul33xx33
implicit none
2018-12-09 19:30:37 +05:30
type(tParameters), intent(in) :: &
prm
type(tDisloUCLAState), intent(in) :: &
stt
type(tDisloUCLAdependentState), intent(in) :: &
dst
2018-11-28 11:14:32 +05:30
real(pReal), dimension(3,3), intent(in) :: &
Mp !< 2nd Piola Kirchhoff stress tensor in Mandel notation
real(pReal), intent(in) :: &
temperature !< temperature at integration point
integer(pInt), intent(in) :: &
2018-12-09 19:30:37 +05:30
of
integer(pInt) :: &
2018-12-05 02:03:32 +05:30
j
2018-12-09 19:30:37 +05:30
real(pReal), intent(out), dimension(prm%totalNslip) :: &
gdot_slip_pos,dgdot_dtauslip_pos,tau_slip_pos,gdot_slip_neg,dgdot_dtauslip_neg,tau_slip_neg
2018-12-09 19:55:54 +05:30
real(pReal), dimension(prm%totalNslip) :: &
StressRatio, BoltzmannRatio, &
StressRatio_p,StressRatio_pminus1, &
2018-12-09 21:05:28 +05:30
DotGamma0, dvel_slip, vel_slip
2018-12-05 02:03:32 +05:30
do j = 1_pInt, prm%totalNslip
2018-12-09 19:19:08 +05:30
tau_slip_pos(j) = math_mul33xx33(Mp,prm%nonSchmid_pos(1:3,1:3,j))
tau_slip_neg(j) = math_mul33xx33(Mp,prm%nonSchmid_neg(1:3,1:3,j))
enddo
2018-12-05 03:00:07 +05:30
2018-12-09 19:55:54 +05:30
BoltzmannRatio = prm%H0kp/(kB*Temperature)
DotGamma0 = stt%rhoEdge(:,of)*prm%burgers*prm%v0
2018-12-09 22:05:48 +05:30
significantPositiveTau: where(abs(tau_slip_pos)-dst%threshold_stress(:,of) > tol_math_check)
StressRatio = (abs(tau_slip_pos)-dst%threshold_stress(:,of)) &
/ (prm%solidSolutionStrength+prm%tau_Peierls)
StressRatio_p = StressRatio** prm%p
StressRatio_pminus1 = StressRatio**(prm%p-1.0_pReal)
vel_slip = 2.0_pReal*prm%burgers * prm%kink_height * prm%omega &
* ( dst%mfp(:,of) - prm%kink_width ) &
* (tau_slip_pos &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) ) &
2018-12-05 02:03:32 +05:30
/ ( &
2018-12-09 22:05:48 +05:30
2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_pos &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
)
2018-12-05 03:00:07 +05:30
2018-12-09 22:05:48 +05:30
gdot_slip_pos = DotGamma0 * sign(vel_slip,tau_slip_pos)
2018-12-05 02:03:32 +05:30
2018-12-09 22:05:48 +05:30
dvel_slip = 2.0_pReal*prm%burgers * prm%kink_height * prm%omega &
* ( dst%mfp(:,of) - prm%kink_width ) &
2018-12-05 02:03:32 +05:30
* ( &
2018-12-09 22:05:48 +05:30
(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
+ tau_slip_pos &
* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q))&
*BoltzmannRatio*prm%p&
*prm%q/&
(prm%solidSolutionStrength+prm%tau_Peierls)*&
StressRatio_pminus1*(1-StressRatio_p)**(prm%q-1.0_pReal) ) &
2018-12-05 02:03:32 +05:30
) &
2018-12-09 22:05:48 +05:30
* (2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_pos &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
) &
2018-12-09 22:05:48 +05:30
- (tau_slip_pos &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) ) &
* (2.0_pReal*(prm%burgers**2.0_pReal) &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q))&
*BoltzmannRatio*prm%p&
*prm%q/&
(prm%solidSolutionStrength+prm%tau_Peierls)*&
StressRatio_pminus1*(1-StressRatio_p)**(prm%q-1.0_pReal) )&
2018-12-05 02:03:32 +05:30
) &
) &
/ ( &
( &
2018-12-09 22:05:48 +05:30
2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_pos &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
)**2.0_pReal &
)
2018-12-09 22:05:48 +05:30
dgdot_dtauslip_pos = DotGamma0 * dvel_slip
else where significantPositiveTau
gdot_slip_pos = 0.0_pReal
dgdot_dtauslip_pos = 0.0_pReal
end where significantPositiveTau
significantNegativeTau: where(abs(tau_slip_neg)-dst%threshold_stress(:,of) > tol_math_check)
StressRatio = (abs(tau_slip_neg)-dst%threshold_stress(:,of)) &
/ (prm%solidSolutionStrength+prm%tau_Peierls)
StressRatio_p = StressRatio** prm%p
StressRatio_pminus1 = StressRatio**(prm%p-1.0_pReal)
vel_slip = 2.0_pReal*prm%burgers * prm%kink_height * prm%omega &
* ( dst%mfp(:,of) - prm%kink_width ) &
* (tau_slip_neg &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) ) &
2018-12-05 02:03:32 +05:30
/ ( &
2018-12-09 22:05:48 +05:30
2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_neg &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
)
2018-12-05 03:00:07 +05:30
2018-12-09 22:05:48 +05:30
gdot_slip_neg = DotGamma0 * sign(vel_slip,tau_slip_neg)
2018-12-05 03:00:07 +05:30
2018-12-09 22:05:48 +05:30
dvel_slip = 2.0_pReal*prm%burgers * prm%kink_height * prm%omega &
* ( dst%mfp(:,of) - prm%kink_width ) &
2018-12-05 02:03:32 +05:30
* ( &
2018-12-09 22:05:48 +05:30
(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
+ tau_slip_neg &
* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q))&
*BoltzmannRatio*prm%p&
*prm%q/&
(prm%solidSolutionStrength+prm%tau_Peierls)*&
StressRatio_pminus1*(1-StressRatio_p)**(prm%q-1.0_pReal) ) &
2018-12-05 02:03:32 +05:30
) &
2018-12-09 22:05:48 +05:30
* (2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_neg &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
) &
2018-12-09 22:05:48 +05:30
- (tau_slip_neg &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) ) &
* (2.0_pReal*(prm%burgers**2.0_pReal) &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* (abs(exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q))&
*BoltzmannRatio*prm%p&
*prm%q/&
(prm%solidSolutionStrength+prm%tau_Peierls)*&
StressRatio_pminus1*(1-StressRatio_p)**(prm%q-1.0_pReal) )&
2018-12-05 02:03:32 +05:30
) &
) &
/ ( &
( &
2018-12-09 22:05:48 +05:30
2.0_pReal*(prm%burgers**2.0_pReal)*tau_slip_neg &
+ prm%omega * prm%B &
*(( dst%mfp(:,of) - prm%kink_width )**2.0_pReal) &
* exp(-BoltzmannRatio*(1-StressRatio_p) ** prm%q) &
2018-12-05 02:03:32 +05:30
)**2.0_pReal &
)
2018-12-09 22:05:48 +05:30
dgdot_dtauslip_neg = DotGamma0 * dvel_slip
else where significantNegativeTau
gdot_slip_neg = 0.0_pReal
dgdot_dtauslip_neg = 0.0_pReal
end where significantNegativeTau
2018-12-05 02:03:32 +05:30
end subroutine kinetics
2015-01-21 20:44:00 +05:30
end module plastic_disloUCLA