2013-03-22 23:05:05 +05:30
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! Copyright 2011-13 Max-Planck-Institut für Eisenforschung GmbH
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2011-04-04 19:39:54 +05:30
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!
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! This file is part of DAMASK,
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2011-04-07 12:50:28 +05:30
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! the Düsseldorf Advanced MAterial Simulation Kit.
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2011-04-04 19:39:54 +05:30
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!
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! DAMASK is free software: you can redistribute it and/or modify
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! it under the terms of the GNU General Public License as published by
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! the Free Software Foundation, either version 3 of the License, or
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! (at your option) any later version.
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!
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! DAMASK is distributed in the hope that it will be useful,
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! but WITHOUT ANY WARRANTY; without even the implied warranty of
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! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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! GNU General Public License for more details.
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!
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! You should have received a copy of the GNU General Public License
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! along with DAMASK. If not, see <http://www.gnu.org/licenses/>.
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!
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2013-06-29 00:28:10 +05:30
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!--------------------------------------------------------------------------------------------------
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! $Id$
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!--------------------------------------------------------------------------------------------------
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!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
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2013-07-01 11:40:42 +05:30
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!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
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!> @brief material subroutine for isotropic (J2) plasticity
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!> @details Isotropic (J2) Plasticity which resembles the phenopowerlaw plasticity without
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!! resolving the stress on the slip systems. Will give the response of phenopowerlaw for an
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!! untextured polycrystal
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!--------------------------------------------------------------------------------------------------
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module constitutive_j2
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use prec, only: &
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pReal,&
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pInt
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use lattice, only: &
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LATTICE_undefined_ID
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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
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constitutive_j2_sizeState, & !< total number of microstructural variables
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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(kind(LATTICE_undefined_ID)), dimension(:), allocatable, public :: &
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constitutive_j2_structureID !< ID of the lattice structure
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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
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constitutive_j2_tau0, & !< initial plastic stress
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constitutive_j2_gdot0, & !< reference velocity
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constitutive_j2_n, & !< Visco-plastic parameter
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!--------------------------------------------------------------------------------------------------
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! 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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!--------------------------------------------------------------------------------------------------
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! tausat += (asinh((gammadot / SinhFitA)**(1 / SinhFitD)))**(1 / SinhFitC) / (SinhFitB * (gammadot / gammadot0)**(1/n))
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constitutive_j2_tausat_SinhFitA, & !< fitting parameter for normalized strain rate vs. stress function
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constitutive_j2_tausat_SinhFitB, & !< fitting parameter for normalized strain rate vs. stress function
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constitutive_j2_tausat_SinhFitC, & !< fitting parameter for normalized strain rate vs. stress function
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constitutive_j2_tausat_SinhFitD !< fitting parameter for normalized strain rate vs. stress function
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real(pReal), dimension(:,:,:), allocatable, private :: &
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constitutive_j2_Cslip_66
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enum, bind(c)
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enumerator :: undefined_ID, &
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flowstress_ID, &
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strainrate_ID
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end enum
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integer(kind(undefined_ID)), dimension(:,:), allocatable, private :: &
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constitutive_j2_outputID !< ID of each post result output
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public :: &
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constitutive_j2_init, &
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constitutive_j2_stateInit, &
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constitutive_j2_aTolState, &
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constitutive_j2_homogenizedC, &
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constitutive_j2_LpAndItsTangent, &
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constitutive_j2_dotState, &
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constitutive_j2_postResults
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contains
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!--------------------------------------------------------------------------------------------------
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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: &
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debug_level, &
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debug_constitutive, &
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debug_levelBasic
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use math, only: &
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math_Mandel3333to66, &
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math_Voigt66to3333
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use IO, only: &
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IO_read, &
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IO_lc, &
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IO_getTag, &
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IO_isBlank, &
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IO_stringPos, &
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IO_stringValue, &
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IO_floatValue, &
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IO_error, &
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IO_timeStamp, &
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IO_EOF
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use material, only: &
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homogenization_maxNgrains, &
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phase_plasticity, &
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phase_plasticityInstance, &
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phase_Noutput, &
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PLASTICITY_J2_label, &
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PLASTICITY_J2_ID, &
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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) :: section = 0_pInt, maxNinstance, i,o, mySize
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character(len=32) :: &
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structure = ''
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character(len=65536) :: &
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tag = '', &
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line = ''
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2009-07-22 21:37:19 +05:30
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2013-11-27 13:34:05 +05:30
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write(6,'(/,a)') ' <<<+- constitutive_'//PLASTICITY_J2_label//' init -+>>>'
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write(6,'(a)') ' $Id$'
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write(6,'(a15,a)') ' Current time: ',IO_timeStamp()
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2012-02-01 00:48:55 +05:30
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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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2012-02-21 21:30:00 +05:30
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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)
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allocate(constitutive_j2_sizeState(maxNinstance), source=1_pInt)
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allocate(constitutive_j2_sizePostResults(maxNinstance), source=0_pInt)
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allocate(constitutive_j2_sizePostResult(maxval(phase_Noutput), maxNinstance),source=0_pInt)
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allocate(constitutive_j2_output(maxval(phase_Noutput), maxNinstance))
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constitutive_j2_output = ''
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allocate(constitutive_j2_outputID(maxval(phase_Noutput),maxNinstance), source=undefined_ID)
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allocate(constitutive_j2_Noutput(maxNinstance), source=0_pInt)
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allocate(constitutive_j2_structureID(maxNinstance), source=LATTICE_undefined_ID)
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allocate(constitutive_j2_Cslip_66(6,6,maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_fTaylor(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tau0(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_gdot0(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_n(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_h0(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_h0_slopeLnRate(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tausat(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_a(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_aTolResistance(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tausat_SinhFitA(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tausat_SinhFitB(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tausat_SinhFitC(maxNinstance), source=0.0_pReal)
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allocate(constitutive_j2_tausat_SinhFitD(maxNinstance), source=0.0_pReal)
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rewind(fileUnit)
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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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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
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line = IO_read(fileUnit, .true.) ! reset IO_read
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exit
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endif
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if (IO_getTag(line,'[',']') /= '') then ! next section
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section = section + 1_pInt ! advance section counter
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cycle ! skip to next line
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endif
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if (section > 0_pInt ) then ! do not short-circuit here (.and. with next if-statement). It's not safe in Fortran
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if (phase_plasticity(section) == PLASTICITY_J2_ID) 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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case ('(output)')
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constitutive_j2_Noutput(i) = constitutive_j2_Noutput(i) + 1_pInt
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constitutive_j2_output(constitutive_j2_Noutput(i),i) = &
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IO_lc(IO_stringValue(line,positions,2_pInt))
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select case(IO_lc(IO_stringValue(line,positions,2_pInt)))
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case ('flowstress')
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constitutive_j2_outputID(constitutive_j2_Noutput(i),i) = flowstress_ID
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case ('strainrate')
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constitutive_j2_outputID(constitutive_j2_Noutput(i),i) = strainrate_ID
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case default
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call IO_error(105_pInt,ext_msg=IO_stringValue(line,positions,2_pInt)//' ('//PLASTICITY_J2_label//')')
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end select
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case ('lattice_structure')
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structure = IO_lc(IO_stringValue(line,positions,2_pInt))
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select case(structure(1:3))
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case(LATTICE_iso_label)
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constitutive_j2_structureID(i) = LATTICE_iso_ID
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case(LATTICE_fcc_label)
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constitutive_j2_structureID(i) = LATTICE_fcc_ID
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case(LATTICE_bcc_label)
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constitutive_j2_structureID(i) = LATTICE_bcc_ID
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case(LATTICE_hex_label)
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constitutive_j2_structureID(i) = LATTICE_hex_ID
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case(LATTICE_ort_label)
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constitutive_j2_structureID(i) = LATTICE_ort_ID
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end select
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case ('c11')
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constitutive_j2_Cslip_66(1,1,i) = IO_floatValue(line,positions,2_pInt)
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case ('c12')
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constitutive_j2_Cslip_66(1,2,i) = IO_floatValue(line,positions,2_pInt)
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case ('c13')
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constitutive_j2_Cslip_66(1,3,i) = IO_floatValue(line,positions,2_pInt)
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case ('c22')
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constitutive_j2_Cslip_66(2,2,i) = IO_floatValue(line,positions,2_pInt)
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case ('c23')
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constitutive_j2_Cslip_66(2,3,i) = IO_floatValue(line,positions,2_pInt)
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case ('c33')
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constitutive_j2_Cslip_66(3,3,i) = IO_floatValue(line,positions,2_pInt)
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case ('c44')
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constitutive_j2_Cslip_66(4,4,i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('c55')
|
|
|
|
constitutive_j2_Cslip_66(5,5,i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('c66')
|
|
|
|
constitutive_j2_Cslip_66(6,6,i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('tau0')
|
|
|
|
constitutive_j2_tau0(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_tau0(i) < 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('gdot0')
|
|
|
|
constitutive_j2_gdot0(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_gdot0(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('n')
|
|
|
|
constitutive_j2_n(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_n(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('h0')
|
|
|
|
constitutive_j2_h0(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('h0_slope','slopelnrate')
|
|
|
|
constitutive_j2_h0_slopeLnRate(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('tausat')
|
|
|
|
constitutive_j2_tausat(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_tausat(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('tausat_sinhfita')
|
|
|
|
constitutive_j2_tausat_SinhFitA(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('tausat_sinhfitb')
|
|
|
|
constitutive_j2_tausat_SinhFitB(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('tausat_sinhfitc')
|
|
|
|
constitutive_j2_tausat_SinhFitC(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('tausat_sinhfitd')
|
|
|
|
constitutive_j2_tausat_SinhFitD(i) = IO_floatValue(line,positions,2_pInt)
|
|
|
|
case ('a', 'w0')
|
|
|
|
constitutive_j2_a(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_a(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('taylorfactor')
|
|
|
|
constitutive_j2_fTaylor(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_fTaylor(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case ('atol_resistance')
|
|
|
|
constitutive_j2_aTolResistance(i) = IO_floatValue(line,positions,2_pInt)
|
2013-12-20 14:06:15 +05:30
|
|
|
if (constitutive_j2_aTolResistance(i) <= 0.0_pReal) &
|
|
|
|
call IO_error(211_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
case default
|
2013-11-27 13:34:05 +05:30
|
|
|
call IO_error(210_pInt,ext_msg=trim(tag)//' ('//PLASTICITY_J2_label//')')
|
2013-06-12 01:46:40 +05:30
|
|
|
end select
|
|
|
|
endif
|
2009-03-06 15:43:08 +05:30
|
|
|
endif
|
|
|
|
enddo
|
|
|
|
|
2013-07-01 11:40:42 +05:30
|
|
|
instancesLoop: do i = 1_pInt,maxNinstance
|
|
|
|
outputsLoop: do o = 1_pInt,constitutive_j2_Noutput(i)
|
2013-12-12 03:33:09 +05:30
|
|
|
select case(constitutive_j2_outputID(o,i))
|
|
|
|
case(flowstress_ID,strainrate_ID)
|
2012-02-13 23:11:27 +05:30
|
|
|
mySize = 1_pInt
|
2010-10-26 18:46:37 +05:30
|
|
|
case default
|
|
|
|
end select
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
if (mySize > 0_pInt) then ! any meaningful output found
|
2012-08-29 21:46:10 +05:30
|
|
|
constitutive_j2_sizePostResult(o,i) = mySize
|
2010-10-26 18:46:37 +05:30
|
|
|
constitutive_j2_sizePostResults(i) = &
|
|
|
|
constitutive_j2_sizePostResults(i) + mySize
|
|
|
|
endif
|
2013-07-01 11:40:42 +05:30
|
|
|
enddo outputsLoop
|
2009-03-06 15:43:08 +05:30
|
|
|
|
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_j2_Cslip_66(1:6,1:6,i) = &
|
2013-12-20 14:06:15 +05:30
|
|
|
lattice_symmetrizeC66(constitutive_j2_structureID(i),constitutive_j2_Cslip_66(1:6,1:6,i))
|
|
|
|
constitutive_j2_Cslip_66(1:6,1:6,i) = & ! Literature data is Voigt, DAMASK uses Mandel
|
|
|
|
math_Mandel3333to66(math_Voigt66to3333(constitutive_j2_Cslip_66(1:6,1:6,i)))
|
2013-07-01 11:40:42 +05:30
|
|
|
enddo instancesLoop
|
2009-03-06 15:43:08 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end subroutine constitutive_j2_init
|
2009-03-06 15:43:08 +05:30
|
|
|
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-07-01 11:40:42 +05:30
|
|
|
!> @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
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-08 21:57:26 +05:30
|
|
|
pure function constitutive_j2_stateInit(matID)
|
2009-06-23 16:09:29 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
implicit none
|
2013-06-29 00:28:10 +05:30
|
|
|
real(pReal), dimension(1) :: constitutive_j2_stateInit
|
2013-10-08 21:57:26 +05:30
|
|
|
integer(pInt), intent(in) :: matID !< number specifying the instance of the plasticity
|
2013-06-29 00:28:10 +05:30
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
constitutive_j2_stateInit = constitutive_j2_tau0(matID)
|
2009-06-23 16:09:29 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end function constitutive_j2_stateInit
|
2009-03-06 15:43:08 +05:30
|
|
|
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-07-01 11:40:42 +05:30
|
|
|
!> @brief sets the relevant state values for a given instance of this plasticity
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-08 21:57:26 +05:30
|
|
|
pure function constitutive_j2_aTolState(matID)
|
2009-09-18 21:07:14 +05:30
|
|
|
|
2013-07-12 12:27:15 +05:30
|
|
|
implicit none
|
2013-10-08 21:57:26 +05:30
|
|
|
integer(pInt), intent(in) :: matID !< number specifying the instance of the plasticity
|
2009-09-18 21:07:14 +05:30
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
real(pReal), dimension(constitutive_j2_sizeState(matID)) :: &
|
2013-06-29 00:28:10 +05:30
|
|
|
constitutive_j2_aTolState
|
2009-09-18 21:07:14 +05:30
|
|
|
|
2013-10-08 21:57:26 +05:30
|
|
|
constitutive_j2_aTolState = constitutive_j2_aTolResistance(matID)
|
2009-09-18 21:07:14 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end function constitutive_j2_aTolState
|
2009-09-18 21:07:14 +05:30
|
|
|
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-07-01 11:40:42 +05:30
|
|
|
!> @brief returns the homogenized elasticity matrix
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-16 18:34:59 +05:30
|
|
|
pure function constitutive_j2_homogenizedC(ipc,ip,el)
|
2013-06-29 00:28:10 +05:30
|
|
|
use mesh, only: &
|
2013-07-01 11:40:42 +05:30
|
|
|
mesh_NcpElems, &
|
|
|
|
mesh_maxNips
|
2013-06-29 00:28:10 +05:30
|
|
|
use material, only: &
|
|
|
|
homogenization_maxNgrains,&
|
|
|
|
material_phase, &
|
|
|
|
phase_plasticityInstance
|
2012-03-09 01:55:28 +05:30
|
|
|
|
2009-03-06 15:43:08 +05:30
|
|
|
implicit none
|
2013-07-01 11:40:42 +05:30
|
|
|
real(pReal), dimension(6,6) :: &
|
|
|
|
constitutive_j2_homogenizedC
|
2013-06-29 00:28:10 +05:30
|
|
|
integer(pInt), intent(in) :: &
|
|
|
|
ipc, & !< component-ID of integration point
|
|
|
|
ip, & !< integration point
|
|
|
|
el !< element
|
2013-10-14 16:24:45 +05:30
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
constitutive_j2_homogenizedC = constitutive_j2_Cslip_66(1:6,1:6,&
|
|
|
|
phase_plasticityInstance(material_phase(ipc,ip,el)))
|
2009-03-06 15:43:08 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end function constitutive_j2_homogenizedC
|
2009-03-06 15:43:08 +05:30
|
|
|
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
!> @brief calculates plastic velocity gradient and its tangent
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-16 18:34:59 +05:30
|
|
|
pure subroutine constitutive_j2_LpAndItsTangent(Lp,dLp_dTstar99,Tstar_v,state,ipc,ip,el)
|
2013-06-29 00:28:10 +05:30
|
|
|
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
|
2009-06-23 16:09:29 +05:30
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
implicit none
|
2013-07-01 11:40:42 +05:30
|
|
|
real(pReal), dimension(3,3), intent(out) :: &
|
|
|
|
Lp !< plastic velocity gradient
|
|
|
|
real(pReal), dimension(9,9), intent(out) :: &
|
2013-07-12 12:27:15 +05:30
|
|
|
dLp_dTstar99 !< derivative of Lp with respect to 2nd Piola Kirchhoff stress
|
2013-07-01 11:40:42 +05:30
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
real(pReal), dimension(6), intent(in) :: &
|
|
|
|
Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
|
|
|
|
integer(pInt), intent(in) :: &
|
|
|
|
ipc, & !< component-ID of integration point
|
|
|
|
ip, & !< integration point
|
|
|
|
el !< element
|
|
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
|
|
|
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) :: &
|
|
|
|
matID, &
|
|
|
|
k, l, m, n
|
2009-06-23 16:09:29 +05:30
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
matID = phase_plasticityInstance(material_phase(ipc,ip,el))
|
|
|
|
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
|
2013-07-12 12:27:15 +05:30
|
|
|
dLp_dTstar99 = 0.0_pReal
|
2013-06-29 00:28:10 +05:30
|
|
|
else
|
2014-01-16 14:48:26 +05:30
|
|
|
gamma_dot = constitutive_j2_gdot0(matID) &
|
|
|
|
* (sqrt(1.5_pReal) * norm_Tstar_dev &
|
|
|
|
/ constitutive_j2_fTaylor(matID) / state(ipc,ip,el)%p(1)) **constitutive_j2_n(matID)
|
2013-06-29 00:28:10 +05:30
|
|
|
|
|
|
|
Lp = Tstar_dev_33/norm_Tstar_dev * gamma_dot/constitutive_j2_fTaylor(matID)
|
|
|
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
! 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) &
|
|
|
|
dLp_dTstar_3333(k,l,m,n) = (constitutive_j2_n(matID)-1.0_pReal) * &
|
|
|
|
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
|
2014-01-16 14:48:26 +05:30
|
|
|
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
|
2013-07-12 12:27:15 +05:30
|
|
|
dLp_dTstar99 = math_Plain3333to99(gamma_dot / constitutive_j2_fTaylor(matID) * &
|
2013-06-29 00:28:10 +05:30
|
|
|
dLp_dTstar_3333 / norm_Tstar_dev)
|
|
|
|
end if
|
2009-06-23 16:09:29 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end subroutine constitutive_j2_LpAndItsTangent
|
2009-03-06 15:43:08 +05:30
|
|
|
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
!> @brief calculates the rate of change of microstructure
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-16 18:34:59 +05:30
|
|
|
pure function constitutive_j2_dotState(Tstar_v,state,ipc,ip,el)
|
2013-06-29 00:28:10 +05:30
|
|
|
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
|
2012-05-16 20:13:26 +05:30
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
implicit none
|
|
|
|
real(pReal), dimension(1) :: &
|
|
|
|
constitutive_j2_dotState
|
|
|
|
real(pReal), dimension(6), intent(in):: &
|
|
|
|
Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
|
|
|
|
integer(pInt), intent(in) :: &
|
|
|
|
ipc, & !< component-ID of integration point
|
|
|
|
ip, & !< integration point
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el !< element
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type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
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state !< microstructure state
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real(pReal), dimension(6) :: &
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Tstar_dev_v !< deviatoric part of the 2nd Piola Kirchhoff stress tensor in Mandel notation
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real(pReal) :: &
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gamma_dot, & !< strainrate
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hardening, & !< hardening coefficient
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saturation, & !< saturation resistance
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norm_Tstar_dev !< euclidean norm of Tstar_dev
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integer(pInt) :: &
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matID
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2012-05-16 20:13:26 +05:30
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2013-06-29 00:28:10 +05:30
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matID = phase_plasticityInstance(material_phase(ipc,ip,el))
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!--------------------------------------------------------------------------------------------------
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! norm of deviatoric part of 2nd Piola-Kirchhoff stress
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Tstar_dev_v(1:3) = Tstar_v(1:3) - sum(Tstar_v(1:3))/3.0_pReal
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Tstar_dev_v(4:6) = Tstar_v(4:6)
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norm_Tstar_dev = sqrt(math_mul6x6(Tstar_dev_v,Tstar_dev_v))
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!--------------------------------------------------------------------------------------------------
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! strain rate
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gamma_dot = constitutive_j2_gdot0(matID) * ( sqrt(1.5_pReal) * norm_Tstar_dev &
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/ &!-----------------------------------------------------------------------------------
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(constitutive_j2_fTaylor(matID) * state(ipc,ip,el)%p(1)) ) ** constitutive_j2_n(matID)
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!--------------------------------------------------------------------------------------------------
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! hardening coefficient
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if (abs(gamma_dot) > 1e-12_pReal) then
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if (constitutive_j2_tausat_SinhFitA(matID) == 0.0_pReal) then
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saturation = constitutive_j2_tausat(matID)
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else
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saturation = ( constitutive_j2_tausat(matID) &
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+ ( log( ( gamma_dot / constitutive_j2_tausat_SinhFitA(matID)&
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)**(1.0_pReal / constitutive_j2_tausat_SinhFitD(matID))&
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+ sqrt( ( gamma_dot / constitutive_j2_tausat_SinhFitA(matID) &
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)**(2.0_pReal / constitutive_j2_tausat_SinhFitD(matID)) &
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+ 1.0_pReal ) &
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) & ! asinh(K) = ln(K + sqrt(K^2 +1))
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)**(1.0_pReal / constitutive_j2_tausat_SinhFitC(matID)) &
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/ ( constitutive_j2_tausat_SinhFitB(matID) &
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* (gamma_dot / constitutive_j2_gdot0(matID))**(1.0_pReal / constitutive_j2_n(matID)) &
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) &
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)
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endif
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hardening = ( constitutive_j2_h0(matID) + constitutive_j2_h0_slopeLnRate(matID) * log(gamma_dot) ) &
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* abs( 1.0_pReal - state(ipc,ip,el)%p(1)/saturation )**constitutive_j2_a(matID) &
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* sign(1.0_pReal, 1.0_pReal - state(ipc,ip,el)%p(1)/saturation)
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else
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hardening = 0.0_pReal
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endif
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constitutive_j2_dotState = hardening * gamma_dot
|
2012-05-16 20:13:26 +05:30
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2013-06-29 00:28:10 +05:30
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end function constitutive_j2_dotState
|
2012-05-16 20:13:26 +05:30
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|
2013-06-29 00:28:10 +05:30
|
|
|
!--------------------------------------------------------------------------------------------------
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!> @brief return array of constitutive results
|
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|
|
!--------------------------------------------------------------------------------------------------
|
2013-10-16 18:34:59 +05:30
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pure function constitutive_j2_postResults(Tstar_v,state,ipc,ip,el)
|
2013-06-29 00:28:10 +05:30
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use prec, only: &
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p_vec
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use math, only: &
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math_mul6x6
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use mesh, only: &
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mesh_NcpElems, &
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mesh_maxNips
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use material, only: &
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homogenization_maxNgrains, &
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material_phase, &
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phase_plasticityInstance, &
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phase_Noutput
|
|
|
|
|
|
|
|
implicit none
|
|
|
|
real(pReal), dimension(6), intent(in) :: &
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|
|
Tstar_v !< 2nd Piola Kirchhoff stress tensor in Mandel notation
|
|
|
|
integer(pInt), intent(in) :: &
|
|
|
|
ipc, & !< component-ID of integration point
|
|
|
|
ip, & !< integration point
|
|
|
|
el !< element
|
|
|
|
type(p_vec), dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems), intent(in) :: &
|
2013-07-01 11:40:42 +05:30
|
|
|
state !< microstructure state
|
|
|
|
|
2013-06-29 00:28:10 +05:30
|
|
|
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) :: &
|
|
|
|
matID, &
|
|
|
|
o, &
|
|
|
|
c
|
|
|
|
|
|
|
|
matID = phase_plasticityInstance(material_phase(ipc,ip,el))
|
|
|
|
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
|
|
|
! 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))
|
2013-12-12 03:33:09 +05:30
|
|
|
select case(constitutive_j2_outputID(o,matID))
|
|
|
|
case (flowstress_ID)
|
2013-06-29 00:28:10 +05:30
|
|
|
constitutive_j2_postResults(c+1_pInt) = state(ipc,ip,el)%p(1)
|
|
|
|
c = c + 1_pInt
|
2013-12-12 03:33:09 +05:30
|
|
|
case (strainrate_ID)
|
2013-06-29 00:28:10 +05:30
|
|
|
constitutive_j2_postResults(c+1_pInt) = &
|
|
|
|
constitutive_j2_gdot0(matID) * ( sqrt(1.5_pReal) * norm_Tstar_dev &
|
|
|
|
/ &!----------------------------------------------------------------------------------
|
|
|
|
(constitutive_j2_fTaylor(matID) * state(ipc,ip,el)%p(1)) ) ** constitutive_j2_n(matID)
|
|
|
|
c = c + 1_pInt
|
|
|
|
end select
|
|
|
|
enddo outputsLoop
|
2009-03-06 15:43:08 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end function constitutive_j2_postResults
|
2009-03-06 15:43:08 +05:30
|
|
|
|
2012-03-09 01:55:28 +05:30
|
|
|
end module constitutive_j2
|