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!--------------------------------------------------------------------------------------------------
! $Id$
!--------------------------------------------------------------------------------------------------
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @brief material subroutine for isotropic (J2) plasticity
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!> @details Isotropic (J2) Plasticity which resembles the phenopowerlaw plasticity without
!! resolving the stress on the slip systems. Will give the response of phenopowerlaw for an
!! untextured polycrystal
!--------------------------------------------------------------------------------------------------
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module constitutive_j2
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use prec , only : &
pReal , &
pInt
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implicit none
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private
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integer ( pInt ) , dimension ( : ) , allocatable , public , protected :: &
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constitutive_j2_sizeDotState , & !< number of dotStates
constitutive_j2_sizeState , & !< total number of microstructural variables
constitutive_j2_sizePostResults !< cumulative size of post results
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integer ( pInt ) , dimension ( : , : ) , allocatable , target , public :: &
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constitutive_j2_sizePostResult !< size of each post result output
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character ( len = 64 ) , dimension ( : , : ) , allocatable , target , public :: &
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constitutive_j2_output !< name of each post result output
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integer ( pInt ) , dimension ( : ) , allocatable , private :: &
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constitutive_j2_Noutput !< number of outputs per instance
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real ( pReal ) , dimension ( : ) , allocatable , private :: &
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constitutive_j2_fTaylor , & !< Taylor factor
constitutive_j2_tau0 , & !< initial plastic stress
constitutive_j2_gdot0 , & !< reference velocity
constitutive_j2_n , & !< Visco-plastic parameter
!--------------------------------------------------------------------------------------------------
! h0 as function of h0 = A + B log (gammadot)
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constitutive_j2_h0 , &
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constitutive_j2_h0_slopeLnRate , &
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constitutive_j2_tausat , & !< final plastic stress
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constitutive_j2_a , &
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constitutive_j2_aTolResistance , &
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!--------------------------------------------------------------------------------------------------
! tausat += (asinh((gammadot / SinhFitA)**(1 / SinhFitD)))**(1 / SinhFitC) / (SinhFitB * (gammadot / gammadot0)**(1/n))
constitutive_j2_tausat_SinhFitA , & !< fitting parameter for normalized strain rate vs. stress function
constitutive_j2_tausat_SinhFitB , & !< fitting parameter for normalized strain rate vs. stress function
constitutive_j2_tausat_SinhFitC , & !< fitting parameter for normalized strain rate vs. stress function
constitutive_j2_tausat_SinhFitD !< fitting parameter for normalized strain rate vs. stress function
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enum , bind ( c )
enumerator :: undefined_ID , &
flowstress_ID , &
strainrate_ID
end enum
integer ( kind ( undefined_ID ) ) , dimension ( : , : ) , allocatable , private :: &
constitutive_j2_outputID !< ID of each post result output
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public :: &
constitutive_j2_init , &
constitutive_j2_stateInit , &
constitutive_j2_aTolState , &
constitutive_j2_LpAndItsTangent , &
constitutive_j2_dotState , &
constitutive_j2_postResults
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contains
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!--------------------------------------------------------------------------------------------------
!> @brief module initialization
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!> @details reads in material parameters, allocates arrays, and does sanity checks
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!--------------------------------------------------------------------------------------------------
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subroutine constitutive_j2_init ( fileUnit )
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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 debug , only : &
debug_level , &
debug_constitutive , &
debug_levelBasic
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use math , only : &
math_Mandel3333to66 , &
math_Voigt66to3333
use IO , only : &
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IO_read , &
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IO_lc , &
IO_getTag , &
IO_isBlank , &
IO_stringPos , &
IO_stringValue , &
IO_floatValue , &
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IO_error , &
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IO_timeStamp , &
IO_EOF
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use material , only : &
homogenization_maxNgrains , &
phase_plasticity , &
phase_plasticityInstance , &
phase_Noutput , &
PLASTICITY_J2_label , &
PLASTICITY_J2_ID , &
MATERIAL_partPhase
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use lattice
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implicit none
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integer ( pInt ) , intent ( in ) :: fileUnit
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integer ( pInt ) , parameter :: MAXNCHUNKS = 7_pInt
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integer ( pInt ) , dimension ( 1_pInt + 2_pInt * MAXNCHUNKS ) :: positions
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integer ( pInt ) :: phase , maxNinstance , instance , o , mySize
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character ( len = 65536 ) :: &
tag = '' , &
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line = ''
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write ( 6 , '(/,a)' ) ' <<<+- constitutive_' / / PLASTICITY_J2_label / / ' init -+>>>'
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write ( 6 , '(a)' ) ' $Id$'
write ( 6 , '(a15,a)' ) ' Current time: ' , IO_timeStamp ( )
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#include "compilation_info.f90"
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maxNinstance = int ( count ( phase_plasticity == PLASTICITY_J2_ID ) , pInt )
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if ( maxNinstance == 0_pInt ) return
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if ( iand ( debug_level ( debug_constitutive ) , debug_levelBasic ) / = 0_pInt ) &
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write ( 6 , '(a16,1x,i5,/)' ) '# instances:' , maxNinstance
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allocate ( constitutive_j2_sizeDotState ( maxNinstance ) , source = 1_pInt )
allocate ( constitutive_j2_sizeState ( maxNinstance ) , source = 1_pInt )
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allocate ( constitutive_j2_sizePostResults ( maxNinstance ) , source = 0_pInt )
allocate ( constitutive_j2_sizePostResult ( maxval ( phase_Noutput ) , maxNinstance ) , source = 0_pInt )
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allocate ( constitutive_j2_output ( maxval ( phase_Noutput ) , maxNinstance ) )
constitutive_j2_output = ''
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allocate ( constitutive_j2_outputID ( maxval ( phase_Noutput ) , maxNinstance ) , source = undefined_ID )
allocate ( constitutive_j2_Noutput ( maxNinstance ) , source = 0_pInt )
allocate ( constitutive_j2_fTaylor ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tau0 ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_gdot0 ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_n ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_h0 ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_h0_slopeLnRate ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tausat ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_a ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_aTolResistance ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tausat_SinhFitA ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tausat_SinhFitB ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tausat_SinhFitC ( maxNinstance ) , source = 0.0_pReal )
allocate ( constitutive_j2_tausat_SinhFitD ( maxNinstance ) , source = 0.0_pReal )
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rewind ( fileUnit )
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phase = 0_pInt
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do while ( trim ( line ) / = IO_EOF . and . IO_lc ( IO_getTag ( line , '<' , '>' ) ) / = material_partPhase ) ! wind forward to <phase>
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line = IO_read ( fileUnit )
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enddo
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parsingFile : do while ( trim ( line ) / = IO_EOF ) ! read through sections of phase part
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line = IO_read ( fileUnit )
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if ( IO_isBlank ( line ) ) cycle ! skip empty lines
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if ( IO_getTag ( line , '<' , '>' ) / = '' ) then ! stop at next part
line = IO_read ( fileUnit , . true . ) ! reset IO_read
exit
endif
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if ( IO_getTag ( line , '[' , ']' ) / = '' ) then ! next section
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phase = phase + 1_pInt ! advance section counter
if ( phase_plasticity ( phase ) == PLASTICITY_J2_ID ) then
instance = phase_plasticityInstance ( phase )
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endif
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cycle ! skip to next line
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endif
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if ( phase > 0_pInt ) then ; if ( phase_plasticity ( phase ) == PLASTICITY_J2_ID ) then ! one of my sections. Do not short-circuit here (.and. between if-statements), it's not safe in Fortran
instance = phase_plasticityInstance ( phase ) ! which instance of my plasticity is present phase
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positions = IO_stringPos ( line , MAXNCHUNKS )
tag = IO_lc ( IO_stringValue ( line , positions , 1_pInt ) ) ! extract key
select case ( tag )
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case ( 'plasticity' , 'elasticity' , 'lattice_structure' , &
'covera_ratio' , 'c/a_ratio' , 'c/a' , &
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'c11' , 'c12' , 'c13' , 'c22' , 'c23' , 'c33' , 'c44' , 'c55' , 'c66' )
case ( '(output)' )
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constitutive_j2_Noutput ( instance ) = constitutive_j2_Noutput ( instance ) + 1_pInt
constitutive_j2_output ( constitutive_j2_Noutput ( instance ) , instance ) = &
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IO_lc ( IO_stringValue ( line , positions , 2_pInt ) )
select case ( IO_lc ( IO_stringValue ( line , positions , 2_pInt ) ) )
case ( 'flowstress' )
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constitutive_j2_outputID ( constitutive_j2_Noutput ( instance ) , instance ) = flowstress_ID
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case ( 'strainrate' )
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constitutive_j2_outputID ( constitutive_j2_Noutput ( instance ) , instance ) = strainrate_ID
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case default
call IO_error ( 105_pInt , ext_msg = IO_stringValue ( line , positions , 2_pInt ) / / ' (' / / PLASTICITY_J2_label / / ')' )
end select
case ( 'tau0' )
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constitutive_j2_tau0 ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_tau0 ( instance ) < 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'gdot0' )
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constitutive_j2_gdot0 ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_gdot0 ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'n' )
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constitutive_j2_n ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_n ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'h0' )
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constitutive_j2_h0 ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'h0_slope' , 'slopelnrate' )
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constitutive_j2_h0_slopeLnRate ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tausat' )
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constitutive_j2_tausat ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_tausat ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'tausat_sinhfita' )
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constitutive_j2_tausat_SinhFitA ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tausat_sinhfitb' )
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constitutive_j2_tausat_SinhFitB ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tausat_sinhfitc' )
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constitutive_j2_tausat_SinhFitC ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'tausat_sinhfitd' )
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constitutive_j2_tausat_SinhFitD ( instance ) = IO_floatValue ( line , positions , 2_pInt )
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case ( 'a' , 'w0' )
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constitutive_j2_a ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_a ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'taylorfactor' )
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constitutive_j2_fTaylor ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_fTaylor ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case ( 'atol_resistance' )
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constitutive_j2_aTolResistance ( instance ) = IO_floatValue ( line , positions , 2_pInt )
if ( constitutive_j2_aTolResistance ( instance ) < = 0.0_pReal ) &
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call IO_error ( 211_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
case default
call IO_error ( 210_pInt , ext_msg = trim ( tag ) / / ' (' / / PLASTICITY_J2_label / / ')' )
end select
endif ; endif
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enddo parsingFile
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instancesLoop : do instance = 1_pInt , maxNinstance
outputsLoop : do o = 1_pInt , constitutive_j2_Noutput ( instance )
select case ( constitutive_j2_outputID ( o , instance ) )
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case ( flowstress_ID , strainrate_ID )
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mySize = 1_pInt
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case default
end select
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if ( mySize > 0_pInt ) then ! any meaningful output found
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constitutive_j2_sizePostResult ( o , instance ) = mySize
constitutive_j2_sizePostResults ( instance ) = &
constitutive_j2_sizePostResults ( instance ) + mySize
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endif
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enddo outputsLoop
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enddo instancesLoop
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end subroutine constitutive_j2_init
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!--------------------------------------------------------------------------------------------------
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!> @brief sets the initial microstructural state for a given instance of this plasticity
!> @details initial microstructural state is set to the value specified by tau0
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!--------------------------------------------------------------------------------------------------
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pure function constitutive_j2_stateInit ( instance )
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implicit none
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real ( pReal ) , dimension ( 1 ) :: constitutive_j2_stateInit
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integer ( pInt ) , intent ( in ) :: instance !< number specifying the instance of the plasticity
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constitutive_j2_stateInit = constitutive_j2_tau0 ( instance )
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end function constitutive_j2_stateInit
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!--------------------------------------------------------------------------------------------------
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!> @brief sets the relevant state values for a given instance of this plasticity
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!--------------------------------------------------------------------------------------------------
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pure function constitutive_j2_aTolState ( instance )
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implicit none
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real ( pReal ) , dimension ( 1 ) :: constitutive_j2_aTolState
integer ( pInt ) , intent ( in ) :: instance !< number specifying the instance of the plasticity
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constitutive_j2_aTolState = constitutive_j2_aTolResistance ( instance )
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end function constitutive_j2_aTolState
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!--------------------------------------------------------------------------------------------------
!> @brief calculates plastic velocity gradient and its tangent
!--------------------------------------------------------------------------------------------------
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pure subroutine constitutive_j2_LpAndItsTangent ( Lp , dLp_dTstar99 , Tstar_v , state , ipc , ip , el )
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use prec , only : &
p_vec
use math , only : &
math_mul6x6 , &
math_Mandel6to33 , &
math_Plain3333to99 , &
math_deviatoric33 , &
math_mul33xx33
use mesh , only : &
mesh_NcpElems , &
mesh_maxNips
use material , only : &
homogenization_maxNgrains , &
material_phase , &
phase_plasticityInstance
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implicit none
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real ( pReal ) , dimension ( 3 , 3 ) , intent ( out ) :: &
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Lp !< plastic velocity gradient
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real ( pReal ) , dimension ( 9 , 9 ) , intent ( out ) :: &
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dLp_dTstar99 !< derivative of Lp with respect to 2nd Piola Kirchhoff stress
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real ( pReal ) , dimension ( 6 ) , intent ( in ) :: &
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Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
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integer ( pInt ) , intent ( in ) :: &
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ipc , & !< component-ID of integration point
ip , & !< integration point
el !< element
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type ( p_vec ) , intent ( in ) :: &
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state !< microstructure state
real ( pReal ) , dimension ( 3 , 3 ) :: &
Tstar_dev_33 !< deviatoric part of the 2nd Piola Kirchhoff stress tensor as 2nd order tensor
real ( pReal ) , dimension ( 3 , 3 , 3 , 3 ) :: &
dLp_dTstar_3333 !< derivative of Lp with respect to Tstar as 4th order tensor
real ( pReal ) :: &
gamma_dot , & !< strainrate
norm_Tstar_dev , & !< euclidean norm of Tstar_dev
squarenorm_Tstar_dev !< square of the euclidean norm of Tstar_dev
integer ( pInt ) :: &
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instance , &
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k , l , m , n
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instance = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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Tstar_dev_33 = math_deviatoric33 ( math_Mandel6to33 ( Tstar_v ) ) ! deviatoric part of 2nd Piola-Kirchhoff stress
squarenorm_Tstar_dev = math_mul33xx33 ( Tstar_dev_33 , Tstar_dev_33 )
norm_Tstar_dev = sqrt ( squarenorm_Tstar_dev )
if ( norm_Tstar_dev < = 0.0_pReal ) then ! Tstar == 0 --> both Lp and dLp_dTstar are zero
Lp = 0.0_pReal
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dLp_dTstar99 = 0.0_pReal
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else
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gamma_dot = constitutive_j2_gdot0 ( instance ) &
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* ( sqrt ( 1.5_pReal ) * norm_Tstar_dev / constitutive_j2_fTaylor ( instance ) / state % p ( 1 ) ) &
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** constitutive_j2_n ( instance )
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Lp = Tstar_dev_33 / norm_Tstar_dev * gamma_dot / constitutive_j2_fTaylor ( instance )
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!--------------------------------------------------------------------------------------------------
! Calculation of the tangent of Lp
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_dTstar_3333 ( k , l , m , n ) = ( constitutive_j2_n ( instance ) - 1.0_pReal ) * &
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Tstar_dev_33 ( k , l ) * Tstar_dev_33 ( m , n ) / squarenorm_Tstar_dev
forall ( k = 1_pInt : 3_pInt , l = 1_pInt : 3_pInt ) &
dLp_dTstar_3333 ( k , l , k , l ) = dLp_dTstar_3333 ( k , l , k , l ) + 1.0_pReal
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forall ( k = 1_pInt : 3_pInt , m = 1_pInt : 3_pInt ) &
dLp_dTstar_3333 ( k , k , m , m ) = dLp_dTstar_3333 ( k , k , m , m ) - 1.0_pReal / 3.0_pReal
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dLp_dTstar99 = math_Plain3333to99 ( gamma_dot / constitutive_j2_fTaylor ( instance ) * &
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dLp_dTstar_3333 / norm_Tstar_dev )
end if
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end subroutine constitutive_j2_LpAndItsTangent
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!--------------------------------------------------------------------------------------------------
!> @brief calculates the rate of change of microstructure
!--------------------------------------------------------------------------------------------------
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pure function constitutive_j2_dotState ( Tstar_v , state , ipc , ip , el )
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use prec , only : &
p_vec
use math , only : &
math_mul6x6
use mesh , only : &
mesh_NcpElems , &
mesh_maxNips
use material , only : &
homogenization_maxNgrains , &
material_phase , &
phase_plasticityInstance
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implicit none
real ( pReal ) , dimension ( 1 ) :: &
constitutive_j2_dotState
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real ( pReal ) , dimension ( 6 ) , intent ( in ) :: &
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Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
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integer ( pInt ) , intent ( in ) :: &
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ipc , & !< component-ID of integration point
ip , & !< integration point
el !< element
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type ( p_vec ) , intent ( in ) :: &
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state !< microstructure state
real ( pReal ) , dimension ( 6 ) :: &
Tstar_dev_v !< deviatoric part of the 2nd Piola Kirchhoff stress tensor in Mandel notation
real ( pReal ) :: &
gamma_dot , & !< strainrate
hardening , & !< hardening coefficient
saturation , & !< saturation resistance
norm_Tstar_dev !< euclidean norm of Tstar_dev
integer ( pInt ) :: &
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instance
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instance = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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!--------------------------------------------------------------------------------------------------
! norm of deviatoric part of 2nd Piola-Kirchhoff stress
Tstar_dev_v ( 1 : 3 ) = Tstar_v ( 1 : 3 ) - sum ( Tstar_v ( 1 : 3 ) ) / 3.0_pReal
Tstar_dev_v ( 4 : 6 ) = Tstar_v ( 4 : 6 )
norm_Tstar_dev = sqrt ( math_mul6x6 ( Tstar_dev_v , Tstar_dev_v ) )
!--------------------------------------------------------------------------------------------------
! strain rate
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gamma_dot = constitutive_j2_gdot0 ( instance ) * ( sqrt ( 1.5_pReal ) * norm_Tstar_dev &
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/ & !-----------------------------------------------------------------------------------
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( constitutive_j2_fTaylor ( instance ) * state % p ( 1 ) ) ) ** constitutive_j2_n ( instance )
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!--------------------------------------------------------------------------------------------------
! hardening coefficient
if ( abs ( gamma_dot ) > 1e-12_pReal ) then
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if ( constitutive_j2_tausat_SinhFitA ( instance ) == 0.0_pReal ) then
saturation = constitutive_j2_tausat ( instance )
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else
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saturation = ( constitutive_j2_tausat ( instance ) &
+ ( log ( ( gamma_dot / constitutive_j2_tausat_SinhFitA ( instance ) &
) ** ( 1.0_pReal / constitutive_j2_tausat_SinhFitD ( instance ) ) &
+ sqrt ( ( gamma_dot / constitutive_j2_tausat_SinhFitA ( instance ) &
) ** ( 2.0_pReal / constitutive_j2_tausat_SinhFitD ( instance ) ) &
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+ 1.0_pReal ) &
) & ! asinh(K) = ln(K + sqrt(K^2 +1))
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) ** ( 1.0_pReal / constitutive_j2_tausat_SinhFitC ( instance ) ) &
/ ( constitutive_j2_tausat_SinhFitB ( instance ) &
* ( gamma_dot / constitutive_j2_gdot0 ( instance ) ) ** ( 1.0_pReal / constitutive_j2_n ( instance ) ) &
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) &
)
endif
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hardening = ( constitutive_j2_h0 ( instance ) + constitutive_j2_h0_slopeLnRate ( instance ) * log ( gamma_dot ) ) &
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* abs ( 1.0_pReal - state % p ( 1 ) / saturation ) ** constitutive_j2_a ( instance ) &
* sign ( 1.0_pReal , 1.0_pReal - state % p ( 1 ) / saturation )
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else
hardening = 0.0_pReal
endif
constitutive_j2_dotState = hardening * gamma_dot
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end function constitutive_j2_dotState
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!--------------------------------------------------------------------------------------------------
!> @brief return array of constitutive results
!--------------------------------------------------------------------------------------------------
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pure function constitutive_j2_postResults ( Tstar_v , state , ipc , ip , el )
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use prec , only : &
p_vec
use math , only : &
math_mul6x6
use mesh , only : &
mesh_NcpElems , &
mesh_maxNips
use material , only : &
homogenization_maxNgrains , &
material_phase , &
phase_plasticityInstance , &
phase_Noutput
implicit none
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real ( pReal ) , dimension ( 6 ) , intent ( in ) :: &
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Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
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integer ( pInt ) , intent ( in ) :: &
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ipc , & !< component-ID of integration point
ip , & !< integration point
el !< element
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type ( p_vec ) , intent ( in ) :: &
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state !< microstructure state
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real ( pReal ) , dimension ( constitutive_j2_sizePostResults ( phase_plasticityInstance ( material_phase ( ipc , ip , el ) ) ) ) :: &
constitutive_j2_postResults
real ( pReal ) , dimension ( 6 ) :: &
Tstar_dev_v ! deviatoric part of the 2nd Piola Kirchhoff stress tensor in Mandel notation
real ( pReal ) :: &
norm_Tstar_dev ! euclidean norm of Tstar_dev
integer ( pInt ) :: &
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instance , &
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o , &
c
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instance = phase_plasticityInstance ( material_phase ( ipc , ip , el ) )
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!--------------------------------------------------------------------------------------------------
! calculate deviatoric part of 2nd Piola-Kirchhoff stress and its norm
Tstar_dev_v ( 1 : 3 ) = Tstar_v ( 1 : 3 ) - sum ( Tstar_v ( 1 : 3 ) ) / 3.0_pReal
Tstar_dev_v ( 4 : 6 ) = Tstar_v ( 4 : 6 )
norm_Tstar_dev = sqrt ( math_mul6x6 ( Tstar_dev_v , Tstar_dev_v ) )
c = 0_pInt
constitutive_j2_postResults = 0.0_pReal
outputsLoop : do o = 1_pInt , phase_Noutput ( material_phase ( ipc , ip , el ) )
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select case ( constitutive_j2_outputID ( o , instance ) )
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case ( flowstress_ID )
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constitutive_j2_postResults ( c + 1_pInt ) = state % p ( 1 )
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c = c + 1_pInt
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case ( strainrate_ID )
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constitutive_j2_postResults ( c + 1_pInt ) = &
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constitutive_j2_gdot0 ( instance ) * ( sqrt ( 1.5_pReal ) * norm_Tstar_dev &
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/ & !----------------------------------------------------------------------------------
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( constitutive_j2_fTaylor ( instance ) * state % p ( 1 ) ) ) ** constitutive_j2_n ( instance )
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c = c + 1_pInt
end select
enddo outputsLoop
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end function constitutive_j2_postResults
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end module constitutive_j2