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! Copyright 2011 Max-Planck-Institut für Eisenforschung GmbH
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!
! This file is part of DAMASK,
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! the Düsseldorf Advanced MAterial Simulation Kit.
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!
! DAMASK is free software: you can redistribute it and/or modify
! it under the terms of the GNU General Public License as published by
! the Free Software Foundation, either version 3 of the License, or
! (at your option) any later version.
!
! DAMASK is distributed in the hope that it will be useful,
! but WITHOUT ANY WARRANTY; without even the implied warranty of
! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
! GNU General Public License for more details.
!
! You should have received a copy of the GNU General Public License
! along with DAMASK. If not, see <http://www.gnu.org/licenses/>.
!
!##############################################################
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!* $Id$
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!*****************************************************
!* Module: CONSTITUTIVE_PHENOPOWERLAW *
!*****************************************************
!* contains: *
!* - constitutive equations *
!* - parameters definition *
!*****************************************************
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![Alu]
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!plasticity phenopowerlaw
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!(output) resistance_slip
!(output) shearrate_slip
!(output) resolvedstress_slip
!(output) totalshear
!(output) resistance_twin
!(output) shearrate_twin
!(output) resolvedstress_twin
!(output) totalvolfrac
!lattice_structure hex
!covera_ratio 1.587
!Nslip 3 3 6 12 # per family
!Ntwin 6 6 6 6 # per family
!
!c11 162.2e9
!c12 91.8e9
!c13 68.8e9
!c33 180.5e9
!c44 46.7e9
!
!gdot0_slip 0.001
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!n_slip 50
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!tau0_slip 65e6 22e6 52e6 50e6 # per family
!tausat_slip 80e6 180e6 140e6 140e6 # per family
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!a_slip 1
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!gdot0_twin 0.001
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!n_twin 50
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!tau0_twin 52e6 52e6 52e6 52e6 # per family
!s_pr 50e6 # push-up stress for slip saturation due to twinning
!twin_b 2
!twin_C 25
!twin_d 0.1
!twin_e 0.1
!h0_slipslip 10e6
!h0_sliptwin 0
!h0_twinslip 625e6
!h0_twintwin 400e6
!interaction_slipslip 5.5 5.5 1.0 52.0 5.5 5.5 1.0 52.0 27.5 0.2 72.8 1.0 72.8 72.8 27.5 1.1 1.4 5.5 7.7 7.7
!interaction_sliptwin 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
!interaction_twinslip 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
!interaction_twintwin 1 1 1 1 1 1 1 1 10 10 10 10 10 10 10 10 10 10 10 10
!relevantResistance 1
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module constitutive_phenopowerlaw
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use prec , only : pReal , pInt
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implicit none
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private
character ( len = * ) , parameter , public :: &
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constitutive_phenopowerlaw_label = 'phenopowerlaw'
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integer ( pInt ) , dimension ( : ) , allocatable , public :: &
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constitutive_phenopowerlaw_sizeDotState , &
constitutive_phenopowerlaw_sizeState , &
constitutive_phenopowerlaw_sizePostResults , & ! cumulative size of post results
constitutive_phenopowerlaw_structure
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integer ( pInt ) , dimension ( : ) , allocatable , private :: &
constitutive_phenopowerlaw_Noutput , & ! number of outputs per instance of this constitution
constitutive_phenopowerlaw_totalNslip , & ! no. of slip system used in simulation
constitutive_phenopowerlaw_totalNtwin ! no. of twin system used in simulation
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integer ( pInt ) , dimension ( : , : ) , allocatable , target , public :: &
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constitutive_phenopowerlaw_sizePostResult ! size of each post result output
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integer ( pInt ) , dimension ( : , : ) , allocatable , private :: &
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constitutive_phenopowerlaw_Nslip , & ! active number of slip systems per family
constitutive_phenopowerlaw_Ntwin ! active number of twin systems per family
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character ( len = 64 ) , dimension ( : , : ) , allocatable , target , public :: &
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constitutive_phenopowerlaw_output ! name of each post result output
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character ( len = 32 ) , dimension ( : ) , allocatable , private :: &
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constitutive_phenopowerlaw_structureName
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real ( pReal ) , dimension ( : ) , allocatable , private :: &
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constitutive_phenopowerlaw_CoverA , &
constitutive_phenopowerlaw_C11 , &
constitutive_phenopowerlaw_C12 , &
constitutive_phenopowerlaw_C13 , &
constitutive_phenopowerlaw_C33 , &
constitutive_phenopowerlaw_C44 , &
constitutive_phenopowerlaw_gdot0_slip , &
constitutive_phenopowerlaw_n_slip , &
constitutive_phenopowerlaw_n_twin , &
constitutive_phenopowerlaw_gdot0_twin
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real ( pReal ) , dimension ( : , : ) , allocatable , private :: &
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constitutive_phenopowerlaw_tau0_slip , &
constitutive_phenopowerlaw_tausat_slip , &
constitutive_phenopowerlaw_tau0_twin
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real ( pReal ) , dimension ( : ) , allocatable , private :: &
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constitutive_phenopowerlaw_spr , &
constitutive_phenopowerlaw_twinB , &
constitutive_phenopowerlaw_twinC , &
constitutive_phenopowerlaw_twinD , &
constitutive_phenopowerlaw_twinE , &
constitutive_phenopowerlaw_h0_slipslip , &
constitutive_phenopowerlaw_h0_sliptwin , &
constitutive_phenopowerlaw_h0_twinslip , &
constitutive_phenopowerlaw_h0_twintwin , &
constitutive_phenopowerlaw_a_slip , &
constitutive_phenopowerlaw_aTolResistance
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real ( pReal ) , dimension ( : , : ) , allocatable , private :: &
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constitutive_phenopowerlaw_interaction_slipslip , &
constitutive_phenopowerlaw_interaction_sliptwin , &
constitutive_phenopowerlaw_interaction_twinslip , &
constitutive_phenopowerlaw_interaction_twintwin
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real ( pReal ) , dimension ( : , : , : ) , allocatable , private :: &
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constitutive_phenopowerlaw_hardeningMatrix_slipslip , &
constitutive_phenopowerlaw_hardeningMatrix_sliptwin , &
constitutive_phenopowerlaw_hardeningMatrix_twinslip , &
constitutive_phenopowerlaw_hardeningMatrix_twintwin , &
constitutive_phenopowerlaw_Cslip_66
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public :: &
constitutive_phenopowerlaw_init , &
constitutive_phenopowerlaw_homogenizedC , &
constitutive_phenopowerlaw_aTolState , &
constitutive_phenopowerlaw_dotState , &
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constitutive_phenopowerlaw_deltaState , &
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constitutive_phenopowerlaw_dotTemperature , &
constitutive_phenopowerlaw_microstructure , &
constitutive_phenopowerlaw_LpAndItsTangent , &
constitutive_phenopowerlaw_postResults , &
constitutive_phenopowerlaw_stateInit
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contains
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subroutine constitutive_phenopowerlaw_init ( myFile )
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!**************************************
!* Module initialization *
!**************************************
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use , intrinsic :: iso_fortran_env ! to get compiler_version and compiler_options (at least for gfortran 4.6 at the moment)
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use math , only : math_Mandel3333to66 , &
math_Voigt66to3333
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use IO
use material
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use debug , only : debug_level , &
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debug_constitutive , &
debug_levelBasic
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use lattice , only : lattice_initializeStructure , lattice_symmetryType , &
lattice_maxNslipFamily , lattice_maxNtwinFamily , &
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lattice_maxNinteraction , lattice_NslipSystem , lattice_NtwinSystem , &
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lattice_interactionSlipSlip , &
lattice_interactionSlipTwin , &
lattice_interactionTwinSlip , &
lattice_interactionTwinTwin
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implicit none
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integer ( pInt ) , intent ( in ) :: myFile
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integer ( pInt ) , parameter :: maxNchunks = lattice_maxNinteraction + 1_pInt
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integer ( pInt ) , dimension ( 1 + 2 * maxNchunks ) :: positions
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integer ( pInt ) section , maxNinstance , i , j , k , f , o , &
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mySize , myStructure , index_myFamily , index_otherFamily
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character ( len = 64 ) :: tag
character ( len = 1024 ) :: line
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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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!$OMP CRITICAL (write2out)
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write ( 6 , * )
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write ( 6 , * ) '<<<+- constitutive_' , trim ( constitutive_phenopowerlaw_label ) , ' init -+>>>'
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write ( 6 , * ) '$Id$'
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#include "compilation_info.f90"
openmp parallelization working again (at least for j2 and nonlocal constitutive model).
In order to keep it like that, please follow these simple rules:
DON'T use implicit array subscripts:
example: real, dimension(3,3) :: A,B
A(:,2) = B(:,1) <--- DON'T USE
A(1:3,2) = B(1:3,1) <--- BETTER USE
In many cases the use of explicit array subscripts is inevitable for parallelization. Additionally, it is an easy means to prevent memory leaks.
Enclose all write statements with the following:
!$OMP CRITICAL (write2out)
<your write statement>
!$OMP END CRITICAL (write2out)
Whenever you change something in the code and are not sure if it affects parallelization and leads to nonconforming behavior, please ask me and/or Franz to check this.
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!$OMP END CRITICAL (write2out)
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maxNinstance = int ( count ( phase_plasticity == constitutive_phenopowerlaw_label ) , pInt )
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if ( maxNinstance == 0 ) return
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelBasic ) / = 0_pInt ) then
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!$OMP CRITICAL (write2out)
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write ( 6 , '(a16,1x,i5)' ) '# instances:' , maxNinstance
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write ( 6 , * )
!$OMP END CRITICAL (write2out)
endif
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allocate ( constitutive_phenopowerlaw_sizeDotState ( maxNinstance ) )
constitutive_phenopowerlaw_sizeDotState = 0_pInt
allocate ( constitutive_phenopowerlaw_sizeState ( maxNinstance ) )
constitutive_phenopowerlaw_sizeState = 0_pInt
allocate ( constitutive_phenopowerlaw_sizePostResults ( maxNinstance ) )
constitutive_phenopowerlaw_sizePostResults = 0_pInt
allocate ( constitutive_phenopowerlaw_sizePostResult ( maxval ( phase_Noutput ) , maxNinstance ) )
constitutive_phenopowerlaw_sizePostResult = 0_pInt
allocate ( constitutive_phenopowerlaw_output ( maxval ( phase_Noutput ) , maxNinstance ) )
constitutive_phenopowerlaw_output = ''
allocate ( constitutive_phenopowerlaw_Noutput ( maxNinstance ) )
constitutive_phenopowerlaw_Noutput = 0_pInt
allocate ( constitutive_phenopowerlaw_structureName ( maxNinstance ) )
constitutive_phenopowerlaw_structureName = ''
allocate ( constitutive_phenopowerlaw_structure ( maxNinstance ) )
constitutive_phenopowerlaw_structure = 0_pInt
allocate ( constitutive_phenopowerlaw_Nslip ( lattice_maxNslipFamily , maxNinstance ) )
constitutive_phenopowerlaw_Nslip = 0_pInt
allocate ( constitutive_phenopowerlaw_Ntwin ( lattice_maxNtwinFamily , maxNinstance ) )
constitutive_phenopowerlaw_Ntwin = 0_pInt
allocate ( constitutive_phenopowerlaw_totalNslip ( maxNinstance ) )
constitutive_phenopowerlaw_totalNslip = 0_pInt
allocate ( constitutive_phenopowerlaw_totalNtwin ( maxNinstance ) )
constitutive_phenopowerlaw_totalNtwin = 0_pInt
allocate ( constitutive_phenopowerlaw_CoverA ( maxNinstance ) )
constitutive_phenopowerlaw_CoverA = 0.0_pReal
allocate ( constitutive_phenopowerlaw_C11 ( maxNinstance ) )
constitutive_phenopowerlaw_C11 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_C12 ( maxNinstance ) )
constitutive_phenopowerlaw_C12 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_C13 ( maxNinstance ) )
constitutive_phenopowerlaw_C13 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_C33 ( maxNinstance ) )
constitutive_phenopowerlaw_C33 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_C44 ( maxNinstance ) )
constitutive_phenopowerlaw_C44 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_Cslip_66 ( 6 , 6 , maxNinstance ) )
constitutive_phenopowerlaw_Cslip_66 = 0.0_pReal
allocate ( constitutive_phenopowerlaw_gdot0_slip ( maxNinstance ) )
constitutive_phenopowerlaw_gdot0_slip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_n_slip ( maxNinstance ) )
constitutive_phenopowerlaw_n_slip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_tau0_slip ( lattice_maxNslipFamily , maxNinstance ) )
constitutive_phenopowerlaw_tau0_slip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_tausat_slip ( lattice_maxNslipFamily , maxNinstance ) )
constitutive_phenopowerlaw_tausat_slip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_gdot0_twin ( maxNinstance ) )
constitutive_phenopowerlaw_gdot0_twin = 0.0_pReal
allocate ( constitutive_phenopowerlaw_n_twin ( maxNinstance ) )
constitutive_phenopowerlaw_n_twin = 0.0_pReal
allocate ( constitutive_phenopowerlaw_tau0_twin ( lattice_maxNtwinFamily , maxNinstance ) )
constitutive_phenopowerlaw_tau0_twin = 0.0_pReal
allocate ( constitutive_phenopowerlaw_spr ( maxNinstance ) )
constitutive_phenopowerlaw_spr = 0.0_pReal
allocate ( constitutive_phenopowerlaw_twinB ( maxNinstance ) )
constitutive_phenopowerlaw_twinB = 0.0_pReal
allocate ( constitutive_phenopowerlaw_twinC ( maxNinstance ) )
constitutive_phenopowerlaw_twinC = 0.0_pReal
allocate ( constitutive_phenopowerlaw_twinD ( maxNinstance ) )
constitutive_phenopowerlaw_twinD = 0.0_pReal
allocate ( constitutive_phenopowerlaw_twinE ( maxNinstance ) )
constitutive_phenopowerlaw_twinE = 0.0_pReal
allocate ( constitutive_phenopowerlaw_h0_slipslip ( maxNinstance ) )
constitutive_phenopowerlaw_h0_slipslip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_h0_sliptwin ( maxNinstance ) )
constitutive_phenopowerlaw_h0_sliptwin = 0.0_pReal
allocate ( constitutive_phenopowerlaw_h0_twinslip ( maxNinstance ) )
constitutive_phenopowerlaw_h0_twinslip = 0.0_pReal
allocate ( constitutive_phenopowerlaw_h0_twintwin ( maxNinstance ) )
constitutive_phenopowerlaw_h0_twintwin = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_interaction_slipslip ( lattice_maxNinteraction , maxNinstance ) )
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constitutive_phenopowerlaw_interaction_slipslip = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_interaction_sliptwin ( lattice_maxNinteraction , maxNinstance ) )
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constitutive_phenopowerlaw_interaction_sliptwin = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_interaction_twinslip ( lattice_maxNinteraction , maxNinstance ) )
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constitutive_phenopowerlaw_interaction_twinslip = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_interaction_twintwin ( lattice_maxNinteraction , maxNinstance ) )
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constitutive_phenopowerlaw_interaction_twintwin = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_a_slip ( maxNinstance ) )
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constitutive_phenopowerlaw_a_slip = 0.0_pReal
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allocate ( constitutive_phenopowerlaw_aTolResistance ( maxNinstance ) )
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constitutive_phenopowerlaw_aTolResistance = 0.0_pReal
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rewind ( myFile )
section = 0_pInt
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do while ( IO_lc ( IO_getTag ( line , '<' , '>' ) ) / = 'phase' ) ! wind forward to <phase>
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read ( myFile , '(a1024)' , END = 100 ) line
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enddo
do ! read thru sections of phase part
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read ( myFile , '(a1024)' , END = 100 ) line
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if ( IO_isBlank ( line ) ) cycle ! skip empty lines
if ( IO_getTag ( line , '<' , '>' ) / = '' ) exit ! stop at next part
if ( IO_getTag ( line , '[' , ']' ) / = '' ) then ! next section
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section = section + 1_pInt ! advance section counter
cycle ! skip to next line
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endif
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if ( section > 0_pInt . and . phase_plasticity ( section ) == constitutive_phenopowerlaw_label ) then ! one of my sections
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i = phase_plasticityInstance ( section ) ! which instance of my plasticity is present phase
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positions = IO_stringPos ( line , maxNchunks )
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tag = IO_lc ( IO_stringValue ( line , positions , 1_pInt ) ) ! extract key
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select case ( tag )
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case ( 'plasticity' , 'elasticity' )
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cycle
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case ( '(output)' )
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constitutive_phenopowerlaw_Noutput ( i ) = constitutive_phenopowerlaw_Noutput ( i ) + 1_pInt
constitutive_phenopowerlaw_output ( constitutive_phenopowerlaw_Noutput ( i ) , i ) = IO_lc ( IO_stringValue ( line , positions , 2_pInt ) )
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case ( 'lattice_structure' )
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constitutive_phenopowerlaw_structureName ( i ) = IO_lc ( IO_stringValue ( line , positions , 2_pInt ) )
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case ( 'covera_ratio' )
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constitutive_phenopowerlaw_CoverA ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'c11' )
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constitutive_phenopowerlaw_C11 ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'c12' )
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constitutive_phenopowerlaw_C12 ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'c13' )
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constitutive_phenopowerlaw_C13 ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'c33' )
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constitutive_phenopowerlaw_C33 ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'c44' )
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constitutive_phenopowerlaw_C44 ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'nslip' )
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forall ( j = 1_pInt : lattice_maxNslipFamily ) &
constitutive_phenopowerlaw_Nslip ( j , i ) = IO_intValue ( line , positions , 1_pInt + j )
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case ( 'gdot0_slip' )
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constitutive_phenopowerlaw_gdot0_slip ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'n_slip' )
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constitutive_phenopowerlaw_n_slip ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tau0_slip' )
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forall ( j = 1_pInt : lattice_maxNslipFamily ) &
constitutive_phenopowerlaw_tau0_slip ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 'tausat_slip' )
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forall ( j = 1_pInt : lattice_maxNslipFamily ) &
constitutive_phenopowerlaw_tausat_slip ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 'a_slip' , 'w0_slip' )
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constitutive_phenopowerlaw_a_slip ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'ntwin' )
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forall ( j = 1_pInt : lattice_maxNtwinFamily ) &
constitutive_phenopowerlaw_Ntwin ( j , i ) = IO_intValue ( line , positions , 1_pInt + j )
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case ( 'gdot0_twin' )
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constitutive_phenopowerlaw_gdot0_twin ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'n_twin' )
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constitutive_phenopowerlaw_n_twin ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tau0_twin' )
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forall ( j = 1_pInt : lattice_maxNtwinFamily ) &
constitutive_phenopowerlaw_tau0_twin ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 's_pr' )
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constitutive_phenopowerlaw_spr ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'twin_b' )
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constitutive_phenopowerlaw_twinB ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'twin_c' )
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constitutive_phenopowerlaw_twinC ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'twin_d' )
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constitutive_phenopowerlaw_twinD ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'twin_e' )
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constitutive_phenopowerlaw_twinE ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'h0_slipslip' )
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constitutive_phenopowerlaw_h0_slipslip ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'h0_sliptwin' )
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constitutive_phenopowerlaw_h0_sliptwin ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'h0_twinslip' )
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constitutive_phenopowerlaw_h0_twinslip ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'h0_twintwin' )
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constitutive_phenopowerlaw_h0_twintwin ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'atol_resistance' )
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constitutive_phenopowerlaw_aTolResistance ( i ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'interaction_slipslip' )
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forall ( j = 1_pInt : lattice_maxNinteraction ) &
constitutive_phenopowerlaw_interaction_slipslip ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 'interaction_sliptwin' )
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forall ( j = 1_pInt : lattice_maxNinteraction ) &
constitutive_phenopowerlaw_interaction_sliptwin ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 'interaction_twinslip' )
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forall ( j = 1_pInt : lattice_maxNinteraction ) &
constitutive_phenopowerlaw_interaction_twinslip ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case ( 'interaction_twintwin' )
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forall ( j = 1_pInt : lattice_maxNinteraction ) &
constitutive_phenopowerlaw_interaction_twintwin ( j , i ) = IO_floatValue ( line , positions , 1_pInt + j )
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case default
call IO_error ( 220_pInt , ext_msg = tag )
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end select
endif
enddo
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100 do i = 1_pInt , maxNinstance
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constitutive_phenopowerlaw_structure ( i ) = lattice_initializeStructure ( constitutive_phenopowerlaw_structureName ( i ) , & ! get structure
constitutive_phenopowerlaw_CoverA ( i ) )
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constitutive_phenopowerlaw_Nslip ( 1 : lattice_maxNslipFamily , i ) = &
min ( lattice_NslipSystem ( 1 : lattice_maxNslipFamily , constitutive_phenopowerlaw_structure ( i ) ) , & ! limit active slip systems per family to min of available and requested
constitutive_phenopowerlaw_Nslip ( 1 : lattice_maxNslipFamily , i ) )
constitutive_phenopowerlaw_Ntwin ( 1 : lattice_maxNtwinFamily , i ) = &
min ( lattice_NtwinSystem ( 1 : lattice_maxNtwinFamily , constitutive_phenopowerlaw_structure ( i ) ) , & ! limit active twin systems per family to min of available and requested
constitutive_phenopowerlaw_Ntwin ( : , i ) )
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constitutive_phenopowerlaw_totalNslip ( i ) = sum ( constitutive_phenopowerlaw_Nslip ( : , i ) ) ! how many slip systems altogether
constitutive_phenopowerlaw_totalNtwin ( i ) = sum ( constitutive_phenopowerlaw_Ntwin ( : , i ) ) ! how many twin systems altogether
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if ( constitutive_phenopowerlaw_structure ( i ) < 1 ) call IO_error ( 205_pInt , e = i )
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if ( any ( constitutive_phenopowerlaw_tau0_slip ( : , i ) < 0.0_pReal . and . &
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constitutive_phenopowerlaw_Nslip ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'tau0_slip' )
if ( constitutive_phenopowerlaw_gdot0_slip ( i ) < = 0.0_pReal ) call IO_error ( 221_pInt , e = i , ext_msg = 'gdot0_slip' )
if ( constitutive_phenopowerlaw_n_slip ( i ) < = 0.0_pReal ) call IO_error ( 221_pInt , e = i , ext_msg = 'n_slip' )
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if ( any ( constitutive_phenopowerlaw_tausat_slip ( : , i ) < = 0.0_pReal . and . &
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constitutive_phenopowerlaw_Nslip ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'tausat_slip' )
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if ( any ( constitutive_phenopowerlaw_a_slip ( i ) == 0.0_pReal . and . &
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constitutive_phenopowerlaw_Nslip ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'a_slip' )
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if ( any ( constitutive_phenopowerlaw_tau0_twin ( : , i ) < 0.0_pReal . and . &
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constitutive_phenopowerlaw_Ntwin ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'tau0_twin' )
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if ( constitutive_phenopowerlaw_gdot0_twin ( i ) < = 0.0_pReal . and . &
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any ( constitutive_phenopowerlaw_Ntwin ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'gdot0_twin' )
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if ( constitutive_phenopowerlaw_n_twin ( i ) < = 0.0_pReal . and . &
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any ( constitutive_phenopowerlaw_Ntwin ( : , i ) > 0 ) ) call IO_error ( 221_pInt , e = i , ext_msg = 'n_twin' )
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if ( constitutive_phenopowerlaw_aTolResistance ( i ) < = 0.0_pReal ) &
constitutive_phenopowerlaw_aTolResistance ( i ) = 1.0_pReal ! default absolute tolerance 1 Pa
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enddo
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allocate ( constitutive_phenopowerlaw_hardeningMatrix_slipslip ( maxval ( constitutive_phenopowerlaw_totalNslip ) , & ! slip resistance from slip activity
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maxval ( constitutive_phenopowerlaw_totalNslip ) , &
maxNinstance ) )
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allocate ( constitutive_phenopowerlaw_hardeningMatrix_sliptwin ( maxval ( constitutive_phenopowerlaw_totalNtwin ) , & ! slip resistance from twin activity
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maxval ( constitutive_phenopowerlaw_totalNslip ) , &
maxNinstance ) )
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allocate ( constitutive_phenopowerlaw_hardeningMatrix_twinslip ( maxval ( constitutive_phenopowerlaw_totalNslip ) , & ! twin resistance from slip activity
maxval ( constitutive_phenopowerlaw_totalNtwin ) , &
maxNinstance ) )
allocate ( constitutive_phenopowerlaw_hardeningMatrix_twintwin ( maxval ( constitutive_phenopowerlaw_totalNtwin ) , & ! twin resistance from twin activity
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maxval ( constitutive_phenopowerlaw_totalNtwin ) , &
maxNinstance ) )
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constitutive_phenopowerlaw_hardeningMatrix_slipslip = 0.0_pReal
constitutive_phenopowerlaw_hardeningMatrix_sliptwin = 0.0_pReal
constitutive_phenopowerlaw_hardeningMatrix_twinslip = 0.0_pReal
constitutive_phenopowerlaw_hardeningMatrix_twintwin = 0.0_pReal
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do i = 1_pInt , maxNinstance
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do j = 1_pInt , constitutive_phenopowerlaw_Noutput ( i )
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select case ( constitutive_phenopowerlaw_output ( j , i ) )
case ( 'resistance_slip' , &
'shearrate_slip' , &
'resolvedstress_slip' &
)
mySize = constitutive_phenopowerlaw_totalNslip ( i )
case ( 'resistance_twin' , &
'shearrate_twin' , &
'resolvedstress_twin' &
)
mySize = constitutive_phenopowerlaw_totalNtwin ( i )
case ( 'totalshear' , &
'totalvolfrac' &
)
mySize = 1_pInt
case default
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call IO_error ( 222_pInt , ext_msg = constitutive_phenopowerlaw_output ( j , i ) )
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end select
if ( mySize > 0_pInt ) then ! any meaningful output found
constitutive_phenopowerlaw_sizePostResult ( j , i ) = mySize
constitutive_phenopowerlaw_sizePostResults ( i ) = &
constitutive_phenopowerlaw_sizePostResults ( i ) + mySize
endif
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enddo
constitutive_phenopowerlaw_sizeDotState ( i ) = constitutive_phenopowerlaw_totalNslip ( i ) + &
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constitutive_phenopowerlaw_totalNtwin ( i ) + 2_pInt ! s_slip, s_twin, sum(gamma), sum(f)
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constitutive_phenopowerlaw_sizeState ( i ) = constitutive_phenopowerlaw_totalNslip ( i ) + &
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constitutive_phenopowerlaw_totalNtwin ( i ) + 2_pInt ! s_slip, s_twin, sum(gamma), sum(f)
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myStructure = constitutive_phenopowerlaw_structure ( i )
select case ( lattice_symmetryType ( myStructure ) ) ! assign elasticity tensor
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case ( 1_pInt ) ! cubic(s)
forall ( k = 1_pInt : 3_pInt )
forall ( j = 1_pInt : 3_pInt ) &
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constitutive_phenopowerlaw_Cslip_66 ( k , j , i ) = constitutive_phenopowerlaw_C12 ( i )
constitutive_phenopowerlaw_Cslip_66 ( k , k , i ) = constitutive_phenopowerlaw_C11 ( i )
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constitutive_phenopowerlaw_Cslip_66 ( k + 3_pInt , k + 3_pInt , i ) = constitutive_phenopowerlaw_C44 ( i )
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end forall
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case ( 2_pInt ) ! hex
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constitutive_phenopowerlaw_Cslip_66 ( 1 , 1 , i ) = constitutive_phenopowerlaw_C11 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 2 , 2 , i ) = constitutive_phenopowerlaw_C11 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 3 , 3 , i ) = constitutive_phenopowerlaw_C33 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 1 , 2 , i ) = constitutive_phenopowerlaw_C12 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 2 , 1 , i ) = constitutive_phenopowerlaw_C12 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 1 , 3 , i ) = constitutive_phenopowerlaw_C13 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 3 , 1 , i ) = constitutive_phenopowerlaw_C13 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 2 , 3 , i ) = constitutive_phenopowerlaw_C13 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 3 , 2 , i ) = constitutive_phenopowerlaw_C13 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 4 , 4 , i ) = constitutive_phenopowerlaw_C44 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 5 , 5 , i ) = constitutive_phenopowerlaw_C44 ( i )
constitutive_phenopowerlaw_Cslip_66 ( 6 , 6 , i ) = 0.5_pReal * ( constitutive_phenopowerlaw_C11 ( i ) - &
constitutive_phenopowerlaw_C12 ( i ) )
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end select
constitutive_phenopowerlaw_Cslip_66 ( : , : , i ) = &
math_Mandel3333to66 ( math_Voigt66to3333 ( constitutive_phenopowerlaw_Cslip_66 ( : , : , i ) ) )
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do f = 1_pInt , lattice_maxNslipFamily ! >>> interaction slip -- X
index_myFamily = sum ( constitutive_phenopowerlaw_Nslip ( 1 : f - 1_pInt , i ) )
do j = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , i ) ! loop over (active) systems in my family (slip)
do o = 1_pInt , lattice_maxNslipFamily
index_otherFamily = sum ( constitutive_phenopowerlaw_Nslip ( 1 : o - 1_pInt , i ) )
do k = 1_pInt , constitutive_phenopowerlaw_Nslip ( o , i ) ! loop over (active) systems in other family (slip)
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constitutive_phenopowerlaw_hardeningMatrix_slipslip ( index_otherFamily + k , index_myFamily + j , i ) = &
constitutive_phenopowerlaw_interaction_slipslip ( lattice_interactionSlipSlip ( &
sum ( lattice_NslipSystem ( 1 : o - 1 , myStructure ) ) + k , &
sum ( lattice_NslipSystem ( 1 : f - 1 , myStructure ) ) + j , &
myStructure ) , i )
enddo ; enddo
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do o = 1_pInt , lattice_maxNtwinFamily
index_otherFamily = sum ( constitutive_phenopowerlaw_Ntwin ( 1 : o - 1_pInt , i ) )
do k = 1_pInt , constitutive_phenopowerlaw_Ntwin ( o , i ) ! loop over (active) systems in other family (twin)
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constitutive_phenopowerlaw_hardeningMatrix_sliptwin ( index_otherFamily + k , index_myFamily + j , i ) = &
constitutive_phenopowerlaw_interaction_sliptwin ( lattice_interactionSlipTwin ( &
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sum ( lattice_NtwinSystem ( 1 : o - 1_pInt , myStructure ) ) + k , &
sum ( lattice_NslipSystem ( 1 : f - 1_pInt , myStructure ) ) + j , &
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myStructure ) , i )
enddo ; enddo
enddo ; enddo
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do f = 1_pInt , lattice_maxNtwinFamily ! >>> interaction twin -- X
index_myFamily = sum ( constitutive_phenopowerlaw_Ntwin ( 1 : f - 1_pInt , i ) )
do j = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , i ) ! loop over (active) systems in my family (twin)
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do o = 1_pInt , lattice_maxNslipFamily
index_otherFamily = sum ( constitutive_phenopowerlaw_Nslip ( 1 : o - 1_pInt , i ) )
do k = 1_pInt , constitutive_phenopowerlaw_Nslip ( o , i ) ! loop over (active) systems in other family (slip)
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constitutive_phenopowerlaw_hardeningMatrix_twinslip ( index_otherFamily + k , index_myFamily + j , i ) = &
constitutive_phenopowerlaw_interaction_twinslip ( lattice_interactionTwinSlip ( &
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sum ( lattice_NslipSystem ( 1 : o - 1_pInt , myStructure ) ) + k , &
sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , myStructure ) ) + j , &
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myStructure ) , i )
enddo ; enddo
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do o = 1_pInt , lattice_maxNtwinFamily
index_otherFamily = sum ( constitutive_phenopowerlaw_Ntwin ( 1 : o - 1_pInt , i ) )
do k = 1_pInt , constitutive_phenopowerlaw_Ntwin ( o , i ) ! loop over (active) systems in other family (twin)
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constitutive_phenopowerlaw_hardeningMatrix_twintwin ( index_otherFamily + k , index_myFamily + j , i ) = &
constitutive_phenopowerlaw_interaction_twintwin ( lattice_interactionTwinTwin ( &
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sum ( lattice_NtwinSystem ( 1 : o - 1_pInt , myStructure ) ) + k , &
sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , myStructure ) ) + j , &
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myStructure ) , i )
enddo ; enddo
enddo ; enddo
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! report to out file...
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enddo
return
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end subroutine constitutive_phenopowerlaw_init
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function constitutive_phenopowerlaw_stateInit ( myInstance )
!*********************************************************************
!* initial microstructural state *
!*********************************************************************
use lattice , only : lattice_maxNslipFamily , lattice_maxNtwinFamily
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implicit none
integer ( pInt ) , intent ( in ) :: myInstance
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integer ( pInt ) :: i
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_sizeDotState ( myInstance ) ) :: constitutive_phenopowerlaw_stateInit
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constitutive_phenopowerlaw_stateInit = 0.0_pReal
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do i = 1_pInt , lattice_maxNslipFamily
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constitutive_phenopowerlaw_stateInit ( 1 + &
sum ( constitutive_phenopowerlaw_Nslip ( 1 : i - 1 , myInstance ) ) : &
sum ( constitutive_phenopowerlaw_Nslip ( 1 : i , myInstance ) ) ) = &
constitutive_phenopowerlaw_tau0_slip ( i , myInstance )
enddo
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do i = 1_pInt , lattice_maxNtwinFamily
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constitutive_phenopowerlaw_stateInit ( 1 + sum ( constitutive_phenopowerlaw_Nslip ( : , myInstance ) ) + &
sum ( constitutive_phenopowerlaw_Ntwin ( 1 : i - 1 , myInstance ) ) : &
sum ( constitutive_phenopowerlaw_Nslip ( : , myInstance ) ) + &
sum ( constitutive_phenopowerlaw_Ntwin ( 1 : i , myInstance ) ) ) = &
constitutive_phenopowerlaw_tau0_twin ( i , myInstance )
enddo
return
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end function constitutive_phenopowerlaw_stateInit
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!*********************************************************************
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!* absolute state tolerance *
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!*********************************************************************
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pure function constitutive_phenopowerlaw_aTolState ( myInstance )
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implicit none
!*** input variables
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integer ( pInt ) , intent ( in ) :: myInstance ! number specifying the current instance of the plasticity
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!*** output variables
real ( pReal ) , dimension ( constitutive_phenopowerlaw_sizeState ( myInstance ) ) :: &
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constitutive_phenopowerlaw_aTolState ! relevant state values for the current instance of this plasticity
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!*** local variables
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constitutive_phenopowerlaw_aTolState = constitutive_phenopowerlaw_aTolResistance ( myInstance )
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end function constitutive_phenopowerlaw_aTolState
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function constitutive_phenopowerlaw_homogenizedC ( state , ipc , ip , el )
!*********************************************************************
!* homogenized elacticity matrix *
!* INPUT: *
!* - state : state variables *
!* - ipc : component-ID of current integration point *
!* - ip : current integration point *
!* - el : current element *
!*********************************************************************
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use prec , only : p_vec
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use mesh , only : mesh_NcpElems , mesh_maxNips
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use material , only : homogenization_maxNgrains , material_phase , phase_plasticityInstance
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implicit none
integer ( pInt ) , intent ( in ) :: ipc , ip , el
integer ( pInt ) matID
real ( pReal ) , dimension ( 6 , 6 ) :: constitutive_phenopowerlaw_homogenizedC
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) :: state
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matID = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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constitutive_phenopowerlaw_homogenizedC = constitutive_phenopowerlaw_Cslip_66 ( : , : , matID )
return
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end function constitutive_phenopowerlaw_homogenizedC
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subroutine constitutive_phenopowerlaw_microstructure ( Temperature , state , ipc , ip , el )
!*********************************************************************
!* calculate derived quantities from state (not used here) *
!* INPUT: *
!* - Tp : temperature *
!* - ipc : component-ID of current integration point *
!* - ip : current integration point *
!* - el : current element *
!*********************************************************************
use prec , only : pReal , pInt , p_vec
use mesh , only : mesh_NcpElems , mesh_maxNips
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use material , only : homogenization_maxNgrains , material_phase , phase_plasticityInstance
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implicit none
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integer ( pInt ) ipc , ip , el , matID
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real ( pReal ) Temperature
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) :: state
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matID = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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end subroutine constitutive_phenopowerlaw_microstructure
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subroutine constitutive_phenopowerlaw_LpAndItsTangent ( Lp , dLp_dTstar , Tstar_v , Temperature , state , ipc , ip , el )
!*********************************************************************
!* plastic velocity gradient and its tangent *
!* INPUT: *
!* - Tstar_v : 2nd Piola Kirchhoff stress tensor (Mandel) *
!* - ipc : component-ID at current integration point *
!* - ip : current integration point *
!* - el : current element *
!* OUTPUT: *
!* - Lp : plastic velocity gradient *
!* - dLp_dTstar : derivative of Lp (4th-rank tensor) *
!*********************************************************************
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use prec , only : p_vec
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use math , only : math_Plain3333to99
use lattice , only : lattice_Sslip , lattice_Sslip_v , lattice_Stwin , lattice_Stwin_v , lattice_maxNslipFamily , lattice_maxNtwinFamily , &
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lattice_NslipSystem , lattice_NtwinSystem
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use mesh , only : mesh_NcpElems , mesh_maxNips
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use material , only : homogenization_maxNgrains , material_phase , phase_plasticityInstance
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implicit none
integer ( pInt ) ipc , ip , el
integer ( pInt ) matID , nSlip , nTwin , f , i , j , k , l , m , n , structID , index_Gamma , index_F , index_myFamily
real ( pReal ) Temperature
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) :: state
real ( pReal ) , dimension ( 6 ) :: Tstar_v
real ( pReal ) , dimension ( 3 , 3 ) :: Lp
real ( pReal ) , dimension ( 3 , 3 , 3 , 3 ) :: dLp_dTstar3333
real ( pReal ) , dimension ( 9 , 9 ) :: dLp_dTstar
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_totalNslip ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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gdot_slip , dgdot_dtauslip , tau_slip
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_totalNtwin ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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gdot_twin , dgdot_dtautwin , tau_twin
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matID = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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structID = constitutive_phenopowerlaw_structure ( matID )
nSlip = constitutive_phenopowerlaw_totalNslip ( matID )
nTwin = constitutive_phenopowerlaw_totalNtwin ( matID )
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index_Gamma = nSlip + nTwin + 1_pInt
index_F = nSlip + nTwin + 2_pInt
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Lp = 0.0_pReal
dLp_dTstar3333 = 0.0_pReal
dLp_dTstar = 0.0_pReal
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j = 0_pInt
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do f = 1_pInt , lattice_maxNslipFamily ! loop over all slip families
index_myFamily = sum ( lattice_NslipSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , matID ) ! process each (active) slip system in family
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j = j + 1_pInt
!* Calculation of Lp
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.
2011-03-17 16:16:17 +05:30
tau_slip ( j ) = dot_product ( Tstar_v , lattice_Sslip_v ( 1 : 6 , index_myFamily + i , structID ) )
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gdot_slip ( j ) = constitutive_phenopowerlaw_gdot0_slip ( matID ) * ( abs ( tau_slip ( j ) ) / state ( ipc , ip , el ) % p ( j ) ) ** &
constitutive_phenopowerlaw_n_slip ( matID ) * sign ( 1.0_pReal , tau_slip ( j ) )
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Lp = Lp + ( 1.0_pReal - state ( ipc , ip , el ) % p ( index_F ) ) * & ! 1-F
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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gdot_slip ( j ) * lattice_Sslip ( 1 : 3 , 1 : 3 , index_myFamily + i , structID )
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!* Calculation of the tangent of Lp
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if ( gdot_slip ( j ) / = 0.0_pReal ) then
dgdot_dtauslip ( j ) = gdot_slip ( j ) * constitutive_phenopowerlaw_n_slip ( matID ) / tau_slip ( j )
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forall ( k = 1_pInt : 3_pInt , l = 1_pInt : 3_pInt , m = 1_pInt : 3_pInt , n = 1_pInt : 3_pInt ) &
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dLp_dTstar3333 ( k , l , m , n ) = dLp_dTstar3333 ( k , l , m , n ) + &
dgdot_dtauslip ( j ) * lattice_Sslip ( k , l , index_myFamily + i , structID ) * &
lattice_Sslip ( m , n , index_myFamily + i , structID )
endif
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enddo
enddo
j = 0_pInt
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do f = 1_pInt , lattice_maxNtwinFamily ! loop over all twin families
index_myFamily = sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , matID ) ! process each (active) twin system in family
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j = j + 1_pInt
!* Calculation of Lp
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.
2011-03-17 16:16:17 +05:30
tau_twin ( j ) = dot_product ( Tstar_v , lattice_Stwin_v ( 1 : 6 , index_myFamily + i , structID ) )
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gdot_twin ( j ) = ( 1.0_pReal - state ( ipc , ip , el ) % p ( index_F ) ) * & ! 1-F
constitutive_phenopowerlaw_gdot0_twin ( matID ) * &
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( abs ( tau_twin ( j ) ) / state ( ipc , ip , el ) % p ( nSlip + j ) ) ** &
constitutive_phenopowerlaw_n_twin ( matID ) * max ( 0.0_pReal , sign ( 1.0_pReal , tau_twin ( j ) ) )
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.
2011-03-17 16:16:17 +05:30
Lp = Lp + gdot_twin ( j ) * lattice_Stwin ( 1 : 3 , 1 : 3 , index_myFamily + i , structID )
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!* Calculation of the tangent of Lp
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if ( gdot_twin ( j ) / = 0.0_pReal ) then
dgdot_dtautwin ( j ) = gdot_twin ( j ) * constitutive_phenopowerlaw_n_twin ( matID ) / tau_twin ( j )
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forall ( k = 1_pInt : 3_pInt , l = 1_pInt : 3_pInt , m = 1_pInt : 3_pInt , n = 1_pInt : 3_pInt ) &
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dLp_dTstar3333 ( k , l , m , n ) = dLp_dTstar3333 ( k , l , m , n ) + &
dgdot_dtautwin ( j ) * lattice_Stwin ( k , l , index_myFamily + i , structID ) * &
lattice_Stwin ( m , n , index_myFamily + i , structID )
endif
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enddo
enddo
dLp_dTstar = math_Plain3333to99 ( dLp_dTstar3333 )
return
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end subroutine constitutive_phenopowerlaw_LpAndItsTangent
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function constitutive_phenopowerlaw_dotState ( Tstar_v , Temperature , state , ipc , ip , el )
!*********************************************************************
!* rate of change of microstructure *
!* INPUT: *
!* - Tstar_v : 2nd Piola Kirchhoff stress tensor (Mandel) *
!* - ipc : component-ID at current integration point *
!* - ip : current integration point *
!* - el : current element *
!* OUTPUT: *
!* - constitutive_dotState : evolution of state variable *
!*********************************************************************
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use prec , only : p_vec
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use lattice , only : lattice_Sslip_v , lattice_Stwin_v , lattice_maxNslipFamily , lattice_maxNtwinFamily , &
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lattice_NslipSystem , lattice_NtwinSystem , lattice_shearTwin
use mesh , only : mesh_NcpElems , mesh_maxNips
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use material , only : homogenization_maxNgrains , material_phase , phase_plasticityInstance
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2009-07-22 21:37:19 +05:30
implicit none
integer ( pInt ) ipc , ip , el
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integer ( pInt ) matID , nSlip , nTwin , f , i , j , structID , index_Gamma , index_F , index_myFamily
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real ( pReal ) Temperature , c_slipslip , c_sliptwin , c_twinslip , c_twintwin , ssat_offset
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type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) :: state
real ( pReal ) , dimension ( 6 ) :: Tstar_v
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_totalNslip ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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gdot_slip , tau_slip , h_slipslip , h_sliptwin
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_totalNtwin ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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gdot_twin , tau_twin , h_twinslip , h_twintwin
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_sizeDotState ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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constitutive_phenopowerlaw_dotState
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matID = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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structID = constitutive_phenopowerlaw_structure ( matID )
nSlip = constitutive_phenopowerlaw_totalNslip ( matID )
nTwin = constitutive_phenopowerlaw_totalNtwin ( matID )
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index_Gamma = nSlip + nTwin + 1_pInt
index_F = nSlip + nTwin + 2_pInt
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constitutive_phenopowerlaw_dotState = 0.0_pReal
!-- system-independent (nonlinear) prefactors to M_xx matrices
c_slipslip = constitutive_phenopowerlaw_h0_slipslip ( matID ) * &
( 1.0_pReal + &
constitutive_phenopowerlaw_twinC ( matID ) * state ( ipc , ip , el ) % p ( index_F ) ** constitutive_phenopowerlaw_twinB ( matID ) )
c_sliptwin = 0.0_pReal
c_twinslip = constitutive_phenopowerlaw_h0_twinslip ( matID ) * &
state ( ipc , ip , el ) % p ( index_Gamma ) ** constitutive_phenopowerlaw_twinE ( matID )
c_twintwin = constitutive_phenopowerlaw_h0_twintwin ( matID ) * &
state ( ipc , ip , el ) % p ( index_F ) ** constitutive_phenopowerlaw_twinD ( matID )
!-- add system-dependent part and calculate dot gammas
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ssat_offset = constitutive_phenopowerlaw_spr ( matID ) * sqrt ( state ( ipc , ip , el ) % p ( index_F ) )
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j = 0_pInt
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do f = 1_pInt , lattice_maxNslipFamily ! loop over all slip families
index_myFamily = sum ( lattice_NslipSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , matID ) ! process each (active) slip system in family
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j = j + 1_pInt
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h_slipslip ( j ) = c_slipslip * ( 1.0_pReal - state ( ipc , ip , el ) % p ( j ) / & ! system-dependent prefactor for slip--slip interaction
( constitutive_phenopowerlaw_tausat_slip ( f , matID ) + ssat_offset ) ) ** &
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constitutive_phenopowerlaw_a_slip ( matID )
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h_sliptwin ( j ) = c_sliptwin ! no system-dependent part
!* Calculation of dot gamma
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.
2011-03-17 16:16:17 +05:30
tau_slip ( j ) = dot_product ( Tstar_v , lattice_Sslip_v ( 1 : 6 , index_myFamily + i , structID ) )
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gdot_slip ( j ) = constitutive_phenopowerlaw_gdot0_slip ( matID ) * ( abs ( tau_slip ( j ) ) / state ( ipc , ip , el ) % p ( j ) ) ** &
constitutive_phenopowerlaw_n_slip ( matID ) * sign ( 1.0_pReal , tau_slip ( j ) )
enddo
enddo
j = 0_pInt
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do f = 1_pInt , lattice_maxNtwinFamily ! loop over all twin families
index_myFamily = sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , matID ) ! process each (active) twin system in family
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j = j + 1_pInt
h_twinslip ( j ) = c_twinslip ! no system-dependent parts
h_twintwin ( j ) = c_twintwin
!* Calculation of dot vol frac
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.
2011-03-17 16:16:17 +05:30
tau_twin ( j ) = dot_product ( Tstar_v , lattice_Stwin_v ( 1 : 6 , index_myFamily + i , structID ) )
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gdot_twin ( j ) = ( 1.0_pReal - state ( ipc , ip , el ) % p ( index_F ) ) * & ! 1-F
constitutive_phenopowerlaw_gdot0_twin ( matID ) * &
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( abs ( tau_twin ( j ) ) / state ( ipc , ip , el ) % p ( nSlip + j ) ) ** &
constitutive_phenopowerlaw_n_twin ( matID ) * max ( 0.0_pReal , sign ( 1.0_pReal , tau_twin ( j ) ) )
enddo
enddo
!-- calculate the overall hardening based on above
j = 0_pInt
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do f = 1_pInt , lattice_maxNslipFamily ! loop over all slip families
do i = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , matID ) ! process each (active) slip system in family
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j = j + 1_pInt
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.
2011-03-17 16:16:17 +05:30
constitutive_phenopowerlaw_dotState ( j ) = & ! evolution of slip resistance j
h_slipslip ( j ) * dot_product ( constitutive_phenopowerlaw_hardeningMatrix_slipslip ( 1 : nSlip , j , matID ) , abs ( gdot_slip ) ) + & ! dot gamma_slip
h_sliptwin ( j ) * dot_product ( constitutive_phenopowerlaw_hardeningMatrix_sliptwin ( 1 : nTwin , j , matID ) , gdot_twin ) ! dot gamma_twin
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constitutive_phenopowerlaw_dotState ( index_Gamma ) = constitutive_phenopowerlaw_dotState ( index_Gamma ) + &
abs ( gdot_slip ( j ) )
enddo
enddo
j = 0_pInt
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do f = 1_pInt , lattice_maxNtwinFamily ! loop over all twin families
index_myFamily = sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , matID ) ! process each (active) twin system in family
2009-07-22 21:37:19 +05:30
j = j + 1_pInt
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.
2011-03-17 16:16:17 +05:30
constitutive_phenopowerlaw_dotState ( j + nSlip ) = & ! evolution of twin resistance j
h_twinslip ( j ) * dot_product ( constitutive_phenopowerlaw_hardeningMatrix_twinslip ( 1 : nSlip , j , matID ) , abs ( gdot_slip ) ) + & ! dot gamma_slip
h_twintwin ( j ) * dot_product ( constitutive_phenopowerlaw_hardeningMatrix_twintwin ( 1 : nTwin , j , matID ) , gdot_twin ) ! dot gamma_twin
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constitutive_phenopowerlaw_dotState ( index_F ) = constitutive_phenopowerlaw_dotState ( index_F ) + &
gdot_twin ( j ) / lattice_shearTwin ( index_myFamily + i , structID )
enddo
enddo
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end function constitutive_phenopowerlaw_dotState
2009-07-22 21:37:19 +05:30
2012-05-16 20:13:26 +05:30
!*********************************************************************
!* (instantaneous) incremental change of microstructure *
!*********************************************************************
function constitutive_phenopowerlaw_deltaState ( Tstar_v , Temperature , state , g , ip , el )
use prec , only : pReal , &
pInt , &
p_vec
use mesh , only : mesh_NcpElems , &
mesh_maxNips
use material , only : homogenization_maxNgrains , &
material_phase , &
phase_plasticityInstance
implicit none
!*** input variables
integer ( pInt ) , intent ( in ) :: g , & ! current grain number
ip , & ! current integration point
el ! current element number
real ( pReal ) , intent ( in ) :: Temperature ! temperature
real ( pReal ) , dimension ( 6 ) , intent ( in ) :: Tstar_v ! current 2nd Piola-Kirchhoff stress in Mandel notation
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) , intent ( in ) :: &
state ! current microstructural state
!*** output variables
real ( pReal ) , dimension ( constitutive_phenopowerlaw_sizeDotState ( phase_plasticityInstance ( material_phase ( g , ip , el ) ) ) ) :: &
constitutive_phenopowerlaw_deltaState ! change of state variables / microstructure
!*** local variables
constitutive_phenopowerlaw_deltaState = 0.0_pReal
endfunction
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!****************************************************************
!* calculates the rate of change of temperature *
!****************************************************************
pure function constitutive_phenopowerlaw_dotTemperature ( Tstar_v , Temperature , state , ipc , ip , el )
!*** variables and functions from other modules ***!
use prec , only : pReal , pInt , p_vec
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use mesh , only : mesh_NcpElems , mesh_maxNips
use material , only : homogenization_maxNgrains
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implicit none
!*** input variables ***!
real ( pReal ) , dimension ( 6 ) , intent ( in ) :: Tstar_v ! 2nd Piola Kirchhoff stress tensor in Mandel notation
real ( pReal ) , intent ( in ) :: Temperature
integer ( pInt ) , intent ( in ) :: ipc , & ! grain number
ip , & ! integration point number
el ! element number
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) , intent ( in ) :: state ! state of the current microstructure
!*** output variables ***!
real ( pReal ) constitutive_phenopowerlaw_dotTemperature ! rate of change of temparature
! calculate dotTemperature
constitutive_phenopowerlaw_dotTemperature = 0.0_pReal
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end function constitutive_phenopowerlaw_dotTemperature
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pure function constitutive_phenopowerlaw_postResults ( Tstar_v , Temperature , dt , state , ipc , ip , el )
!*********************************************************************
!* return array of constitutive results *
!* INPUT: *
!* - Tstar_v : 2nd Piola Kirchhoff stress tensor (Mandel) *
!* - dt : current time increment *
!* - ipc : component-ID at current integration point *
!* - ip : current integration point *
!* - el : current element *
!*********************************************************************
use prec , only : pReal , pInt , p_vec
use lattice , only : lattice_Sslip_v , lattice_Stwin_v , lattice_maxNslipFamily , lattice_maxNtwinFamily , &
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lattice_NslipSystem , lattice_NtwinSystem
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use mesh , only : mesh_NcpElems , mesh_maxNips
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use material , only : homogenization_maxNgrains , material_phase , phase_plasticityInstance , phase_Noutput
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implicit none
integer ( pInt ) , intent ( in ) :: ipc , ip , el
real ( pReal ) , intent ( in ) :: dt , Temperature
real ( pReal ) , dimension ( 6 ) , intent ( in ) :: Tstar_v
type ( p_vec ) , dimension ( homogenization_maxNgrains , mesh_maxNips , mesh_NcpElems ) , intent ( in ) :: state
integer ( pInt ) matID , o , f , i , c , nSlip , nTwin , j , structID , index_Gamma , index_F , index_myFamily
real ( pReal ) tau
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real ( pReal ) , dimension ( constitutive_phenopowerlaw_sizePostResults ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
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constitutive_phenopowerlaw_postResults
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matID = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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structID = constitutive_phenopowerlaw_structure ( matID )
nSlip = constitutive_phenopowerlaw_totalNslip ( matID )
nTwin = constitutive_phenopowerlaw_totalNtwin ( matID )
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index_Gamma = nSlip + nTwin + 1_pInt
index_F = nSlip + nTwin + 2_pInt
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constitutive_phenopowerlaw_postResults = 0.0_pReal
c = 0_pInt
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do o = 1_pInt , phase_Noutput ( material_phase ( ipc , ip , el ) )
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select case ( constitutive_phenopowerlaw_output ( o , matID ) )
case ( 'resistance_slip' )
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constitutive_phenopowerlaw_postResults ( c + 1_pInt : c + nSlip ) = state ( ipc , ip , el ) % p ( 1 : nSlip )
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c = c + nSlip
case ( 'shearrate_slip' )
j = 0_pInt
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do f = 1_pInt , lattice_maxNslipFamily ! loop over all slip families
index_myFamily = sum ( lattice_NslipSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , matID ) ! process each (active) slip system in family
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j = j + 1_pInt
tau = dot_product ( Tstar_v , lattice_Sslip_v ( : , index_myFamily + i , structID ) )
constitutive_phenopowerlaw_postResults ( c + j ) = constitutive_phenopowerlaw_gdot0_slip ( matID ) * &
( abs ( tau ) / state ( ipc , ip , el ) % p ( j ) ) ** &
constitutive_phenopowerlaw_n_slip ( matID ) * sign ( 1.0_pReal , tau )
enddo ; enddo
c = c + nSlip
case ( 'resolvedstress_slip' )
j = 0_pInt
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do f = 1_pInt , lattice_maxNslipFamily ! loop over all slip families
index_myFamily = sum ( lattice_NslipSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Nslip ( f , matID ) ! process each (active) slip system in family
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j = j + 1_pInt
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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constitutive_phenopowerlaw_postResults ( c + j ) = dot_product ( Tstar_v , lattice_Sslip_v ( 1 : 6 , index_myFamily + i , structID ) )
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enddo ; enddo
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c = c + nSlip
case ( 'totalshear' )
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constitutive_phenopowerlaw_postResults ( c + 1_pInt ) = state ( ipc , ip , el ) % p ( index_Gamma )
c = c + 1_pInt
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case ( 'resistance_twin' )
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constitutive_phenopowerlaw_postResults ( c + 1_pInt : c + nTwin ) = state ( ipc , ip , el ) % p ( 1_pInt + nSlip : nTwin + nSlip )
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c = c + nTwin
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case ( 'shearrate_twin' )
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j = 0_pInt
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do f = 1_pInt , lattice_maxNtwinFamily ! loop over all twin families
index_myFamily = sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , matID ) ! process each (active) twin system in family
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j = j + 1_pInt
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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tau = dot_product ( Tstar_v , lattice_Stwin_v ( 1 : 6 , index_myFamily + i , structID ) )
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constitutive_phenopowerlaw_postResults ( c + j ) = ( 1.0_pReal - state ( ipc , ip , el ) % p ( index_F ) ) * & ! 1-F
constitutive_phenopowerlaw_gdot0_twin ( matID ) * &
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( abs ( tau ) / state ( ipc , ip , el ) % p ( j + nSlip ) ) ** &
constitutive_phenopowerlaw_n_twin ( matID ) * max ( 0.0_pReal , sign ( 1.0_pReal , tau ) )
enddo ; enddo
c = c + nTwin
case ( 'resolvedstress_twin' )
j = 0_pInt
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do f = 1_pInt , lattice_maxNtwinFamily ! loop over all twin families
index_myFamily = sum ( lattice_NtwinSystem ( 1 : f - 1_pInt , structID ) ) ! at which index starts my family
do i = 1_pInt , constitutive_phenopowerlaw_Ntwin ( f , matID ) ! process each (active) twin system in family
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j = j + 1_pInt
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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constitutive_phenopowerlaw_postResults ( c + j ) = dot_product ( Tstar_v , lattice_Stwin_v ( 1 : 6 , index_myFamily + i , structID ) )
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enddo ; enddo
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c = c + nTwin
case ( 'totalvolfrac' )
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constitutive_phenopowerlaw_postResults ( c + 1_pInt ) = state ( ipc , ip , el ) % p ( index_F )
c = c + 1_pInt
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end select
enddo
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end function constitutive_phenopowerlaw_postResults
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end module constitutive_phenopowerlaw
