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DAMASK_EICMD/code/crystallite.f90

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updated copyright header
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! Copyright 2011-13 Max-Planck-Institut für Eisenforschung GmbH
added copyright text to all f90 (free) format files
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!
! This file is part of DAMASK,
changed enconding of all source files to UTF-8 without BOM (signature) Codepage 65001
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! the Düsseldorf Advanced MAterial Simulation Kit.
added copyright text to all f90 (free) format files
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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/>.
!
doxygen comments
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!--------------------------------------------------------------------------------------------------
! $Id$
!--------------------------------------------------------------------------------------------------
!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
!> @author Christoph Kords, Max-Planck-Institut für Eisenforschung GmbH
!> @brief crystallite state integration functions and reporting of results
!--------------------------------------------------------------------------------------------------
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 17:48:49 +05:30
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
module crystallite
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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use prec, only: &
pReal, &
pInt
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
implicit none
doxygen comments
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private
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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character(len=64), dimension(:,:), allocatable, private :: &
doxygen comments
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crystallite_output !< name of each post result output
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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integer(pInt), public, protected :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystallite_maxSizePostResults !< description not available
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
integer(pInt), dimension(:), allocatable, public, protected :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystallite_sizePostResults !< description not available
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
integer(pInt), dimension(:,:), allocatable, private :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystallite_sizePostResult !< description not available
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
integer(pInt), dimension(:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_symmetryID !< crystallographic symmetry 1=cubic 2=hexagonal, needed in all orientation calcs
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
real(pReal), dimension(:,:), allocatable, public :: &
crystallite_temperature !< temperature (same on all components on one IP)
real(pReal), dimension(:,:,:), allocatable, public, protected :: &
crystallite_heat !< heat source
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:), allocatable, public :: &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_dt !< requested time increment of each grain
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_subdt, & !< substepped time increment of each grain
crystallite_subFrac, & !< already calculated fraction of increment
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_subStep !< size of next integration step
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:,:), allocatable, public :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_Tstar_v, & !< current 2nd Piola-Kirchhoff stress vector (end of converged time step)
crystallite_Tstar0_v, & !< 2nd Piola-Kirchhoff stress vector at start of FE inc
crystallite_partionedTstar0_v !< 2nd Piola-Kirchhoff stress vector at start of homog inc
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_subTstar0_v, & !< 2nd Piola-Kirchhoff stress vector at start of crystallite inc
crystallite_orientation, & !< orientation as quaternion
crystallite_orientation0, & !< initial orientation as quaternion
crystallite_rotation !< grain rotation away from initial orientation as axis-angle (in degrees) in crystal reference frame
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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real(pReal), dimension(:,:,:,:,:), allocatable, public :: &
doxygen comments
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crystallite_Fp, & !< current plastic def grad (end of converged time step)
crystallite_Fp0, & !< plastic def grad at start of FE inc
crystallite_partionedFp0,& !< plastic def grad at start of homog inc
crystallite_F0, & !< def grad at start of FE inc
crystallite_partionedF, & !< def grad to be reached at end of homog inc
crystallite_partionedF0, & !< def grad at start of homog inc
crystallite_Lp, & !< current plastic velocitiy grad (end of converged time step)
crystallite_Lp0, & !< plastic velocitiy grad at start of FE inc
crystallite_partionedLp0,& !< plastic velocity grad at start of homog inc
crystallite_P !< 1st Piola-Kirchhoff stress per grain
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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real(pReal), dimension(:,:,:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_Fe, & !< current "elastic" def grad (end of converged time step)
crystallite_subFe0,& !< "elastic" def grad at start of crystallite inc
crystallite_invFp, & !< inverse of current plastic def grad (end of converged time step)
crystallite_subFp0,& !< plastic def grad at start of crystallite inc
crystallite_subF, & !< def grad to be reached at end of crystallite inc
crystallite_subF0, & !< def grad at start of crystallite inc
crystallite_subLp0,& !< plastic velocity grad at start of crystallite inc
crystallite_disorientation !< disorientation between two neighboring ips (only calculated for single grain IPs)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:,:,:,:,:), allocatable, public :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_dPdF, & !< current individual dPdF per grain (end of converged time step)
crystallite_dPdF0, & !< individual dPdF per grain at start of FE inc
crystallite_partioneddPdF0 !< individual dPdF per grain at start of homog inc
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(:,:,:,:,:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_fallbackdPdF !< dPdF fallback for non-converged grains (elastic prediction)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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logical, dimension(:,:,:), allocatable, public :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_requested !< flag to request crystallite calculation
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
logical, dimension(:,:,:), allocatable, public, protected :: &
reorganized calculation modes for CPFEM, now having better readable and cleaner structure
2013-03-01 17:18:29 +05:30
crystallite_converged, & !< convergence flag
crystallite_localPlasticity !< indicates this grain to have purely local constitutive law
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
logical, dimension(:,:,:), allocatable, private :: &
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_todo !< flag to indicate need for further computation
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
logical, dimension(:,:), allocatable, private :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystallite_clearToWindForward, & !< description not available
crystallite_clearToCutback, & !< description not available
crystallite_syncSubFrac, & !< description not available
crystallite_syncSubFracCompleted, & !< description not available
crystallite_neighborEnforcedCutback !< description not available
doxygen comments
2013-02-22 04:38:36 +05:30
public :: &
crystallite_init, &
crystallite_stressAndItsTangent, &
crystallite_orientations, &
crystallite_postResults
private :: &
crystallite_integrateStateFPI, &
crystallite_integrateStateEuler, &
crystallite_integrateStateAdaptiveEuler, &
crystallite_integrateStateRK4, &
crystallite_integrateStateRKCK45, &
crystallite_integrateStress, &
crystallite_stateJump
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
contains
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
!> @brief allocates and initialize per grain variables
!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
subroutine crystallite_init(temperature)
doxygen comments
2013-02-22 04:38:36 +05:30
use, intrinsic :: iso_fortran_env ! to get compiler_version and compiler_options (at least for gfortran 4.6 at the moment)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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use debug, only: &
debug_info, &
debug_reset, &
debug_level, &
debug_crystallite, &
debug_levelBasic
further improvements on implementing the plain mode
2013-04-16 22:37:27 +05:30
use numerics, only: &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
usePingPong
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
use math, only: &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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math_I3, &
math_EulerToR, &
math_inv33, &
math_transpose33, &
math_mul33xx33, &
math_mul33x33
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems, &
mesh_maxNips, &
mesh_maxNipNeighbors
use IO, only: &
added possibility for multi-level inclusion of files in *.config and loadcase files. include subfiles by stating {path/to/include}
2013-06-27 00:49:00 +05:30
IO_read, &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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IO_timeStamp, &
IO_open_jobFile_stat, &
IO_open_file, &
IO_lc, &
IO_getTag, &
IO_isBlank, &
IO_stringPos, &
IO_stringValue, &
IO_write_jobFile, &
IO_error
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
use material
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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use lattice, only: &
lattice_symmetryType
use constitutive, only: &
constitutive_microstructure
use constitutive_phenopowerlaw, only: &
change latticeName to latticeID
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constitutive_phenopowerlaw_structureID
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
use constitutive_dislotwin, only: &
change latticeName to latticeID
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constitutive_dislotwin_structureID
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 13:34:05 +05:30
use constitutive_titanmod, only: &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
constitutive_titanmod_structureID
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
use constitutive_nonlocal, only: &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
constitutive_nonlocal_structureID
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
implicit none
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
real(pReal), intent(in) :: temperature
integer(pInt), parameter :: &
MYUNIT = 200_pInt, &
MAXNCHUNKS = 2_pInt
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
integer(pInt), dimension(1+2*MAXNCHUNKS) :: positions
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
integer(pInt) :: &
g, & !< grain number
i, & !< integration point number
e, & !< element number
gMax, & !< maximum number of grains
iMax, & !< maximum number of integration points
eMax, & !< maximum number of elements
nMax, & !< maximum number of ip neighbors
myNgrains, & !< number of grains in current IP
section, &
j, &
p, &
output, &
mySize, &
myPhase, &
myMat
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
character(len=65536) :: &
tag, &
line
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
write(6,'(/,a)') ' <<<+- crystallite init -+>>>'
write(6,'(a)') ' $Id$'
write(6,'(a15,a)') ' Current time: ',IO_timeStamp()
made code standard conform to Fortran 2008 (ignoring warning concerning comments beyond character 132). Basically, changing "x" format specifier to "Nx" ("1x") plus removing $ format specifier added compiler switches for gfortran and ifort to check for standard conformity old gnu compilers <4.4 are not longer supported because they don't provide the c binding for fftw
2012-02-01 00:48:55 +05:30
#include "compilation_info.f90"
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
line = ''
section = 0_pInt
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
gMax = homogenization_maxNgrains
iMax = mesh_maxNips
eMax = mesh_NcpElems
nMax = mesh_maxNipNeighbors
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
allocate(crystallite_temperature(iMax,eMax)); crystallite_temperature = temperature
allocate(crystallite_heat(gMax,iMax,eMax)); crystallite_heat = 0.0_pReal
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
allocate(crystallite_Tstar0_v(6,gMax,iMax,eMax)); crystallite_Tstar0_v = 0.0_pReal
allocate(crystallite_partionedTstar0_v(6,gMax,iMax,eMax)); crystallite_partionedTstar0_v = 0.0_pReal
allocate(crystallite_subTstar0_v(6,gMax,iMax,eMax)); crystallite_subTstar0_v = 0.0_pReal
allocate(crystallite_Tstar_v(6,gMax,iMax,eMax)); crystallite_Tstar_v = 0.0_pReal
allocate(crystallite_P(3,3,gMax,iMax,eMax)); crystallite_P = 0.0_pReal
allocate(crystallite_F0(3,3,gMax,iMax,eMax)); crystallite_F0 = 0.0_pReal
allocate(crystallite_partionedF0(3,3,gMax,iMax,eMax)); crystallite_partionedF0 = 0.0_pReal
allocate(crystallite_partionedF(3,3,gMax,iMax,eMax)); crystallite_partionedF = 0.0_pReal
allocate(crystallite_subF0(3,3,gMax,iMax,eMax)); crystallite_subF0 = 0.0_pReal
allocate(crystallite_subF(3,3,gMax,iMax,eMax)); crystallite_subF = 0.0_pReal
allocate(crystallite_Fp0(3,3,gMax,iMax,eMax)); crystallite_Fp0 = 0.0_pReal
allocate(crystallite_partionedFp0(3,3,gMax,iMax,eMax)); crystallite_partionedFp0 = 0.0_pReal
allocate(crystallite_subFp0(3,3,gMax,iMax,eMax)); crystallite_subFp0 = 0.0_pReal
allocate(crystallite_Fp(3,3,gMax,iMax,eMax)); crystallite_Fp = 0.0_pReal
allocate(crystallite_invFp(3,3,gMax,iMax,eMax)); crystallite_invFp = 0.0_pReal
allocate(crystallite_Fe(3,3,gMax,iMax,eMax)); crystallite_Fe = 0.0_pReal
allocate(crystallite_subFe0(3,3,gMax,iMax,eMax)); crystallite_subFe0 = 0.0_pReal
allocate(crystallite_Lp0(3,3,gMax,iMax,eMax)); crystallite_Lp0 = 0.0_pReal
allocate(crystallite_partionedLp0(3,3,gMax,iMax,eMax)); crystallite_partionedLp0 = 0.0_pReal
allocate(crystallite_subLp0(3,3,gMax,iMax,eMax)); crystallite_subLp0 = 0.0_pReal
allocate(crystallite_Lp(3,3,gMax,iMax,eMax)); crystallite_Lp = 0.0_pReal
allocate(crystallite_dPdF(3,3,3,3,gMax,iMax,eMax)); crystallite_dPdF = 0.0_pReal
allocate(crystallite_dPdF0(3,3,3,3,gMax,iMax,eMax)); crystallite_dPdF0 = 0.0_pReal
allocate(crystallite_partioneddPdF0(3,3,3,3,gMax,iMax,eMax)); crystallite_partioneddPdF0 = 0.0_pReal
allocate(crystallite_fallbackdPdF(3,3,3,3,gMax,iMax,eMax)); crystallite_fallbackdPdF = 0.0_pReal
allocate(crystallite_dt(gMax,iMax,eMax)); crystallite_dt = 0.0_pReal
allocate(crystallite_subdt(gMax,iMax,eMax)); crystallite_subdt = 0.0_pReal
allocate(crystallite_subFrac(gMax,iMax,eMax)); crystallite_subFrac = 0.0_pReal
allocate(crystallite_subStep(gMax,iMax,eMax)); crystallite_subStep = 0.0_pReal
allocate(crystallite_orientation(4,gMax,iMax,eMax)); crystallite_orientation = 0.0_pReal
allocate(crystallite_orientation0(4,gMax,iMax,eMax)); crystallite_orientation0 = 0.0_pReal
allocate(crystallite_rotation(4,gMax,iMax,eMax)); crystallite_rotation = 0.0_pReal
allocate(crystallite_disorientation(4,nMax,gMax,iMax,eMax)); crystallite_disorientation = 0.0_pReal
allocate(crystallite_symmetryID(gMax,iMax,eMax)); crystallite_symmetryID = 0_pInt
allocate(crystallite_localPlasticity(gMax,iMax,eMax)); crystallite_localPlasticity = .true.
allocate(crystallite_requested(gMax,iMax,eMax)); crystallite_requested = .false.
allocate(crystallite_todo(gMax,iMax,eMax)); crystallite_todo = .false.
allocate(crystallite_converged(gMax,iMax,eMax)); crystallite_converged = .true.
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
allocate(crystallite_clearToWindForward(iMax,eMax)); crystallite_clearToWindForward = .true.
allocate(crystallite_syncSubFrac(iMax,eMax)); crystallite_syncSubFrac = .false.
allocate(crystallite_syncSubFracCompleted(iMax,eMax)); crystallite_syncSubFracCompleted = .false.
allocate(crystallite_clearToCutback(iMax,eMax)); crystallite_clearToCutback = .true.
allocate(crystallite_neighborEnforcedCutback(iMax,eMax)); crystallite_neighborEnforcedCutback = .false.
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
allocate(crystallite_output(maxval(crystallite_Noutput), &
material_Ncrystallite)) ; crystallite_output = ''
allocate(crystallite_sizePostResults(material_Ncrystallite)) ; crystallite_sizePostResults = 0_pInt
allocate(crystallite_sizePostResult(maxval(crystallite_Noutput), &
material_Ncrystallite)) ; crystallite_sizePostResult = 0_pInt
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
if (.not. IO_open_jobFile_stat(myUnit,material_localFileExt)) & ! no local material configuration present...
call IO_open_file(myUnit,material_configFile) ! ...open material.config file
removed long lines
2013-08-09 01:03:21 +05:30
do while (trim(line) /= '#EOF#' .and. IO_lc(IO_getTag(line,'<','>')) /= material_partCrystallite) ! wind forward to <crystallite>
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
line = IO_read(myUnit)
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
enddo
removed long lines
2013-08-09 01:03:21 +05:30
do while (trim(line) /= '#EOF#') ! read thru sections of phase part
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
line = IO_read(myUnit)
doxygen comments
2013-02-22 04:38:36 +05:30
if (IO_isBlank(line)) cycle ! skip empty lines
if (IO_getTag(line,'<','>') /= '') exit ! stop at next part
if (IO_getTag(line,'[',']') /= '') then ! next section
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
section = section + 1_pInt
doxygen comments
2013-02-22 04:38:36 +05:30
output = 0_pInt ! reset output counter
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
endif
if (section > 0_pInt) then
positions = IO_stringPos(line,maxNchunks)
doxygen comments
2013-02-22 04:38:36 +05:30
tag = IO_lc(IO_stringValue(line,positions,1_pInt)) ! extract key
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
select case(tag)
case ('(output)')
output = output + 1_pInt
crystallite_output(output,section) = IO_lc(IO_stringValue(line,positions,2_pInt))
end select
endif
enddo
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
close(myUnit)
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
do i = 1_pInt,material_Ncrystallite
do j = 1_pInt,crystallite_Noutput(i)
select case(crystallite_output(j,i))
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
case('phase','texture','volume','grainrotationx','grainrotationy','grainrotationz','heat')
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
mySize = 1_pInt
doxygen comments
2013-02-22 04:38:36 +05:30
case('orientation','grainrotation') ! orientation as quaternion, or deviation from initial grain orientation in axis-angle form (angle in degrees)
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
mySize = 4_pInt
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
case('eulerangles')
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
mySize = 3_pInt
case('defgrad','f','fe','fp','lp','e','ee','p','firstpiola','1stpiola','s','tstar','secondpiola','2ndpiola')
mySize = 9_pInt
case('elasmatrix')
mySize = 36_pInt
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
case('neighboringip','neighboringelement')
mySize = mesh_maxNipNeighbors
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
case default
mySize = 0_pInt
end select
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
outputFound: if (mySize > 0_pInt) then
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
crystallite_sizePostResult(j,i) = mySize
crystallite_sizePostResults(i) = crystallite_sizePostResults(i) + mySize
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
endif outputFound
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
enddo
enddo
crystallite_maxSizePostResults = 0_pInt
do j = 1_pInt,material_Nmicrostructure
if (microstructure_active(j)) &
crystallite_maxSizePostResults = max(crystallite_maxSizePostResults,&
crystallite_sizePostResults(microstructure_crystallite(j)))
enddo
Tstar_v is now restored at different stages of cutbacking; we need this because preguess of state relies on consistent Tstar_v
2009-06-16 14:33:30 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!--------------------------------------------------------------------------------------------------
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
! write description file for crystallite output
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
call IO_write_jobFile(myUnit,'outputCrystallite')
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
do p = 1_pInt,material_Ncrystallite
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
write(myUnit,'(/,a,/)') '['//trim(crystallite_name(p))//']'
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
do e = 1_pInt,crystallite_Noutput(p)
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
write(myUnit,'(a,i4)') trim(crystallite_output(e,p))//char(9),crystallite_sizePostResult(e,p)
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
enddo
enddo
small bufix, didn't compile
2013-10-17 02:14:04 +05:30
close(myUnit)
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!--------------------------------------------------------------------------------------------------
! initialize
do e = FEsolving_execElem(1),FEsolving_execElem(2) ! iterate over all cp elements
myNgrains = homogenization_Ngrains(mesh_element(3,e)) ! look up homogenization-->grainCount
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1_pInt:myNgrains)
crystallite_Fp0(1:3,1:3,g,i,e) = math_EulerToR(material_EulerAngles(1:3,g,i,e)) ! plastic def gradient reflects init orientation
crystallite_F0(1:3,1:3,g,i,e) = math_I3
crystallite_localPlasticity(g,i,e) = phase_localPlasticity(material_phase(g,i,e))
crystallite_Fe(1:3,1:3,g,i,e) = math_transpose33(crystallite_Fp0(1:3,1:3,g,i,e))
crystallite_Fp(1:3,1:3,g,i,e) = crystallite_Fp0(1:3,1:3,g,i,e)
crystallite_requested(g,i,e) = .true.
endforall
enddo
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
if(any(.not. crystallite_localPlasticity) .and. .not. usePingPong) call IO_error(601_pInt) ! exit if nonlocal but no ping-pong
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_partionedFp0 = crystallite_Fp0
crystallite_partionedF0 = crystallite_F0
crystallite_partionedF = crystallite_F0
!--------------------------------------------------------------------------------------------------
! Initialize crystallite_symmetryID
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
do g = 1_pInt,myNgrains
myPhase = material_phase(g,i,e)
myMat = phase_plasticityInstance(myPhase)
select case (phase_plasticity(myPhase))
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 13:34:05 +05:30
case (PLASTICITY_PHENOPOWERLAW_ID)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_symmetryID(g,i,e) = &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
lattice_symmetryType(constitutive_phenopowerlaw_structureID(myMat))
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 13:34:05 +05:30
case (PLASTICITY_TITANMOD_ID)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_symmetryID(g,i,e) = &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
lattice_symmetryType(constitutive_titanmod_structureID(myMat))
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 13:34:05 +05:30
case (PLASTICITY_DISLOTWIN_ID)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_symmetryID(g,i,e) = &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
lattice_symmetryType(constitutive_dislotwin_structureID(myMat))
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 13:34:05 +05:30
case (PLASTICITY_NONLOCAL_ID)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_symmetryID(g,i,e) = &
change latticeName to latticeID
2013-11-27 21:50:27 +05:30
lattice_symmetryType(constitutive_nonlocal_structureID(myMat))
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
case default
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystallite_symmetryID(g,i,e) = 0_pInt !< @ToDo: does this happen for j2 material?
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
end select
enddo
enddo
enddo
call crystallite_orientations()
crystallite_orientation0 = crystallite_orientation ! store initial orientations for calculation of grain rotations
homogenization_RGC.f90 >> just switching-off one of the debugging statement. crystallite.f90 >> optimizing the perturbation algorithm for local tangent.
2009-12-22 17:58:02 +05:30
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
do g = 1_pInt,myNgrains
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
call constitutive_microstructure(temperature, &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_Fe(1:3,1:3,g,i,e), crystallite_Fp(1:3,1:3,g,i,e),g,i,e) ! update dependent state variables to be consistent with basic states
enddo
enddo
enddo
!$OMP END PARALLEL DO
New output can be requested from crystallite: (output) grainrotation it gives the deviation from the initial grain orientation in axis-angle representation with the angle in degrees.
2010-04-12 16:44:36 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
call crystallite_stressAndItsTangent(.true.,.false.) ! request elastic answers
crystallite_fallbackdPdF = crystallite_dPdF ! use initial elastic stiffness as fallback
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!--------------------------------------------------------------------------------------------------
! debug output
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
write(6,'(a35,1x,7(i8,1x))') 'crystallite_temperature: ', shape(crystallite_temperature)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
write(6,'(a35,1x,7(i8,1x))') 'crystallite_heat: ', shape(crystallite_heat)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Fe: ', shape(crystallite_Fe)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Fp: ', shape(crystallite_Fp)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Lp: ', shape(crystallite_Lp)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_F0: ', shape(crystallite_F0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Fp0: ', shape(crystallite_Fp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Lp0: ', shape(crystallite_Lp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partionedF: ', shape(crystallite_partionedF)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partionedF0: ', shape(crystallite_partionedF0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partionedFp0: ', shape(crystallite_partionedFp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partionedLp0: ', shape(crystallite_partionedLp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subF: ', shape(crystallite_subF)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_symmetryID: ', shape(crystallite_symmetryID)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subF0: ', shape(crystallite_subF0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subFe0: ', shape(crystallite_subFe0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subFp0: ', shape(crystallite_subFp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subLp0: ', shape(crystallite_subLp0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_P: ', shape(crystallite_P)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Tstar_v: ', shape(crystallite_Tstar_v)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_Tstar0_v: ', shape(crystallite_Tstar0_v)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partionedTstar0_v: ', shape(crystallite_partionedTstar0_v)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subTstar0_v: ', shape(crystallite_subTstar0_v)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_dPdF: ', shape(crystallite_dPdF)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_dPdF0: ', shape(crystallite_dPdF0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_partioneddPdF0: ', shape(crystallite_partioneddPdF0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_fallbackdPdF: ', shape(crystallite_fallbackdPdF)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_orientation: ', shape(crystallite_orientation)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_orientation0: ', shape(crystallite_orientation0)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_rotation: ', shape(crystallite_rotation)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_disorientation: ', shape(crystallite_disorientation)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_dt: ', shape(crystallite_dt)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subdt: ', shape(crystallite_subdt)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subFrac: ', shape(crystallite_subFrac)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_subStep: ', shape(crystallite_subStep)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_localPlasticity: ', shape(crystallite_localPlasticity)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_requested: ', shape(crystallite_requested)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_todo: ', shape(crystallite_todo)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_converged: ', shape(crystallite_converged)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_sizePostResults: ', shape(crystallite_sizePostResults)
write(6,'(a35,1x,7(i8,1x))') 'crystallite_sizePostResult: ', shape(crystallite_sizePostResult)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
write(6,'(/,a35,1x,i10)') 'Number of nonlocal grains: ',count(.not. crystallite_localPlasticity)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
flush(6)
endif
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4 new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing) updated preprocessing for documentation to handle precision correctly
2012-08-31 01:56:28 +05:30
call debug_info
call debug_reset
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end subroutine crystallite_init
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
!> @brief calculate stress (P) and tangent (dPdF) for crystallites
!--------------------------------------------------------------------------------------------------
simplified analytic jacobian calculation. removed Lpfrac, time_sensitive. introduced rate_sensitivity flag when calling crystallite_stressAndItsTangent that is currently set to .false. and is to be set according to which dPdF the FE solver is asking for
2012-03-14 19:26:50 +05:30
subroutine crystallite_stressAndItsTangent(updateJaco,rate_sensitivity)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
use numerics, only: &
subStepMinCryst, &
subStepSizeCryst, &
stepIncreaseCryst, &
pert_Fg, &
pert_method, &
nCryst, &
numerics_integrator, &
numerics_integrationMode, &
numerics_timeSyncing, &
relevantStrain, &
analyticJaco
use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_CrystalliteLoopDistribution
use IO, only: &
IO_warning
use math, only: &
math_inv33, &
math_identity2nd, &
math_transpose33, &
math_mul33x33, &
math_mul66x6, &
math_Mandel6to33, &
math_Mandel33to6, &
math_I3, &
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
math_mul3333xx3333, &
math_mul33xx33
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems, &
mesh_maxNips, &
mesh_ipNeighborhood, &
FE_NipNeighbors, &
FE_geomtype, &
FE_cellType
use material, only: &
homogenization_Ngrains, &
homogenization_maxNgrains
use constitutive, only: &
constitutive_sizeState, &
constitutive_sizeDotState, &
constitutive_state, &
constitutive_state_backup, &
constitutive_subState0, &
constitutive_partionedState0, &
constitutive_dotState, &
constitutive_dotState_backup, &
constitutive_TandItsTangent
implicit none
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
logical, intent(in) :: &
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
updateJaco, & !< whether to update the Jacobian (stiffness) or not
rate_sensitivity !< rate sensitiv calculation
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
real(pReal) :: &
myPert, & ! perturbation with correct sign
formerSubStep, &
subFracIntermediate
real(pReal), dimension(3,3) :: &
invFp, & ! inverse of the plastic deformation gradient
Fe_guess, & ! guess for elastic deformation gradient
Tstar ! 2nd Piola-Kirchhoff stress tensor
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(3,3,3,3,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
dPdF_perturbation1, &
dPdF_perturbation2
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(3,3,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
F_backup, &
Fp_backup, &
InvFp_backup, &
Fe_backup, &
Lp_backup, &
P_backup
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
real(pReal), dimension(6,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
Tstar_v_backup
integer(pInt) :: &
NiterationCrystallite, & ! number of iterations in crystallite loop
e, & ! element index
i, & ! integration point index
g, & ! grain index
k, &
l, &
n, startIP, endIP, &
neighboring_e, &
neighboring_i, &
o, &
p, &
perturbation , & ! loop counter for forward,backward perturbation mode
myNgrains
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
logical, dimension(homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
convergenceFlag_backup
! local variables used for calculating analytic Jacobian
real(pReal), dimension(3,3):: Fpinv_rate, &
FDot_inv, &
junk
real(pReal), dimension(3,3,3,3) :: dSdFe, &
dFedF, &
dFedFdot, &
dSdF, &
dSdFdot, &
dFp_invdFdot, &
junk2
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
real(pReal) :: counter
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
if(iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP CRITICAL (write2out)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
write(6,'(/,a,i8,1x,i2,1x,i3)') '<< CRYST >> crystallite start at el ip g ', debug_e, debug_i, debug_g
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
write(6,'(a,/,3(12x,3(f14.9,1x)/))') '<< CRYST >> F0 ', &
math_transpose33(crystallite_partionedF0(1:3,1:3,debug_g,debug_i,debug_e))
write(6,'(a,/,3(12x,3(f14.9,1x)/))') '<< CRYST >> Fp0', &
math_transpose33(crystallite_partionedFp0(1:3,1:3,debug_g,debug_i,debug_e))
write(6,'(a,/,3(12x,3(f14.9,1x)/))') '<< CRYST >> Lp0', &
math_transpose33(crystallite_partionedLp0(1:3,1:3,debug_g,debug_i,debug_e))
!$OMP END CRITICAL (write2out)
endif
!--------------------------------------------------------------------------------------------------
! initialize to starting condition
crystallite_subStep = 0.0_pReal
elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), &
g = 1_pInt:myNgrains, crystallite_requested(g,i,e))
constitutive_subState0(g,i,e)%p = constitutive_partionedState0(g,i,e)%p ! ...microstructure
crystallite_subFp0(1:3,1:3,g,i,e) = crystallite_partionedFp0(1:3,1:3,g,i,e) ! ...plastic def grad
crystallite_subLp0(1:3,1:3,g,i,e) = crystallite_partionedLp0(1:3,1:3,g,i,e) ! ...plastic velocity grad
crystallite_dPdF0(1:3,1:3,1:3,1:3,g,i,e) = crystallite_partioneddPdF0(1:3,1:3,1:3,1:3,g,i,e) ! ...stiffness
crystallite_subF0(1:3,1:3,g,i,e) = crystallite_partionedF0(1:3,1:3,g,i,e) ! ...def grad
crystallite_subTstar0_v(1:6,g,i,e) = crystallite_partionedTstar0_v(1:6,g,i,e) !...2nd PK stress
crystallite_subFe0(1:3,1:3,g,i,e) = math_mul33x33(crystallite_subF0(1:3,1:3,g,i,e), &
math_inv33(crystallite_subFp0(1:3,1:3,g,i,e))) ! only needed later on for stiffness calculation
crystallite_subFrac(g,i,e) = 0.0_pReal
crystallite_subStep(g,i,e) = 1.0_pReal/subStepSizeCryst
crystallite_todo(g,i,e) = .true.
crystallite_converged(g,i,e) = .false. ! pretend failed step of twice the required size
endforall
enddo elementLooping1
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
if (FEsolving_execELem(1) == FEsolving_execElem(2) .and. &
FEsolving_execIP(1,FEsolving_execELem(1))==FEsolving_execIP(2,FEsolving_execELem(1))) then
startIP = FEsolving_execIP(1,FEsolving_execELem(1))
endIP = startIP
else
startIP = 1_pInt
endIP = mesh_maxNips
endif
homogenization_RGC.f90 >> just switching-off one of the debugging statement. crystallite.f90 >> optimizing the perturbation algorithm for local tangent.
2009-12-22 17:58:02 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
NiterationCrystallite = 0_pInt
numerics_integrationMode = 1_pInt
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
cutbackLooping: do while (any(crystallite_todo(:,startIP:endIP,FEsolving_execELem(1):FEsolving_execElem(2))))
timeSyncing1: if (any(.not. crystallite_localPlasticity) .and. numerics_timeSyncing) then
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
! Time synchronization can only be used for nonlocal calculations, and only there it makes sense.
! The idea is that in nonlocal calculations often the vast amjority of the ips
! converges in one iteration whereas a small fraction of ips has to do a lot of cutbacks.
! Hence, we try to minimize the computational effort by just doing a lot of cutbacks
! in the vicinity of the "bad" ips and leave the easily converged volume more or less as it is.
! However, some synchronization of the time step has to be done at the border between "bad" ips
! and the ones that immediately converged.
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> crystallite iteration ',NiterationCrystallite
!$OMP END CRITICAL (write2out)
endif
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (any(crystallite_syncSubFrac)) then
! Just did a time synchronization.
! If all synchrnizers converged, then do nothing else than winding them forward.
! If any of the cynchronizers did not converge, something went completely wrong
! and its not clear how to fix this, so all nonlocals become terminally ill.
if (any(crystallite_syncSubFrac .and. .not. crystallite_converged(1,:,:))) then
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if (crystallite_syncSubFrac(i,e) .and. .not. crystallite_converged(1,i,e)) then
!$OMP CRITICAL (write2out)
write(6,'(a,i8,1x,i2)') '<< CRYST >> time synchronization: failed at el,ip ',e,i
!$OMP END CRITICAL (write2out)
endif
enddo
enddo
endif
crystallite_syncSubFrac = .false.
where(.not. crystallite_localPlasticity)
crystallite_substep = 0.0_pReal
crystallite_todo = .false.
endwhere
else
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
crystallite_clearToWindForward(i,e) = crystallite_localPlasticity(1,i,e) .or. crystallite_syncSubFrac(i,e)
crystallite_clearToCutback(i,e) = crystallite_localPlasticity(1,i,e)
enddo
enddo
!$OMP END PARALLEL DO
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> time synchronization: wind forward'
!$OMP END CRITICAL (write2out)
endif
endif
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
elseif (any(crystallite_syncSubFracCompleted)) then
! Just completed a time synchronization.
! Make sure that the ips that synchronized their time step start non-converged
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if (crystallite_syncSubFracCompleted(i,e)) crystallite_converged(1,i,e) = .false.
crystallite_syncSubFracCompleted(i,e) = .false.
crystallite_clearToWindForward(i,e) = crystallite_localPlasticity(1,i,e)
crystallite_clearToCutback(i,e) = crystallite_localPlasticity(1,i,e) .or. .not. crystallite_converged(1,i,e)
enddo
enddo
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> time synchronization: done, proceed with cutback'
!$OMP END CRITICAL (write2out)
endif
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
else
! Normal calculation.
! If all converged and are at the end of the time increment, then just do a final wind forward.
! If all converged, but not all reached the end of the time increment, then we only wind
! those forward that are still on their way, all others have to wait.
! If some did not converge and all are still at the start of the time increment,
! then all non-convergers force their converged neighbors to also do a cutback.
! In case that some ips have already wound forward to an intermediate time (subfrac),
! then all those ips that converged in the first iteration, but now have a non-converged neighbor
! have to synchronize their time step to the same intermediate time. If such a synchronization
! takes place, all other ips have to wait and only the synchronizers do a cutback. In the next
! iteration those will do a wind forward while all others still wait.
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
crystallite_clearToWindForward(i,e) = crystallite_localPlasticity(1,i,e)
crystallite_clearToCutback(i,e) = crystallite_localPlasticity(1,i,e)
enddo
enddo
!$OMP END PARALLEL DO
if (all(crystallite_localPlasticity .or. crystallite_converged)) then
if (all(crystallite_localPlasticity .or. crystallite_subStep + crystallite_subFrac >= 1.0_pReal)) then
crystallite_clearToWindForward = .true. ! final wind forward
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> final wind forward'
!$OMP END CRITICAL (write2out)
endif
else
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
crystallite_clearToWindForward(i,e) = crystallite_localPlasticity(1,i,e) .or. crystallite_subStep(1,i,e) < 1.0_pReal
enddo
enddo
!$OMP END PARALLEL DO
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> wind forward'
!$OMP END CRITICAL (write2out)
endif
endif
else
subFracIntermediate = maxval(crystallite_subFrac, mask=.not.crystallite_localPlasticity)
if (subFracIntermediate == 0.0_pReal) then
crystallite_neighborEnforcedCutback = .false. ! look for ips that require a cutback because of a nonconverged neighbor
!$OMP PARALLEL
!$OMP DO PRIVATE(neighboring_e,neighboring_i)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if (.not. crystallite_localPlasticity(1,i,e) .and. crystallite_converged(1,i,e)) then
do n = 1_pInt,FE_NipNeighbors(FE_celltype(FE_geomtype(mesh_element(2,e))))
neighboring_e = mesh_ipNeighborhood(1,n,i,e)
neighboring_i = mesh_ipNeighborhood(2,n,i,e)
if (neighboring_e > 0_pInt .and. neighboring_i > 0_pInt) then
if (.not. crystallite_localPlasticity(1,neighboring_i,neighboring_e) &
.and. .not. crystallite_converged(1,neighboring_i,neighboring_e)) then
crystallite_neighborEnforcedCutback(i,e) = .true.
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
#ifndef _OPENMP
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) &
write(6,'(a12,i5,1x,i2,a,i5,1x,i2)') '<< CRYST >> ', neighboring_e,neighboring_i, &
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
' enforced cutback at ',e,i
#endif
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
exit
endif
endif
enddo
endif
enddo
enddo
!$OMP END DO
!$OMP DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if(crystallite_neighborEnforcedCutback(i,e)) crystallite_converged(1,i,e) = .false.
enddo
enddo
!$OMP END DO
!$OMP END PARALLEL
else
crystallite_syncSubFrac = .false. ! look for ips that have to do a time synchronization because of a nonconverged neighbor
!$OMP PARALLEL
!$OMP DO PRIVATE(neighboring_e,neighboring_i)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if (.not. crystallite_localPlasticity(1,i,e) .and. crystallite_subFrac(1,i,e) == 0.0_pReal) then
do n = 1_pInt,FE_NipNeighbors(FE_celltype(FE_geomtype(mesh_element(2,e))))
neighboring_e = mesh_ipNeighborhood(1,n,i,e)
neighboring_i = mesh_ipNeighborhood(2,n,i,e)
if (neighboring_e > 0_pInt .and. neighboring_i > 0_pInt) then
if (.not. crystallite_localPlasticity(1,neighboring_i,neighboring_e) &
.and. .not. crystallite_converged(1,neighboring_i,neighboring_e)) then
crystallite_syncSubFrac(i,e) = .true.
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
#ifndef _OPENMP
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) &
write(6,'(a12,i5,1x,i2,a,i5,1x,i2)') '<< CRYST >> ',neighboring_e,neighboring_i, &
' enforced time synchronization at ',e,i
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-28 00:06:55 +05:30
#endif
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
exit
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
endif
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
endif
enddo
endif
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
enddo
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
enddo
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP END DO
!$OMP DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if(crystallite_syncSubFrac(i,e)) crystallite_converged(1,i,e) = .false.
enddo
enddo
!$OMP END DO
!$OMP END PARALLEL
endif
where(.not. crystallite_localPlasticity .and. crystallite_subStep < 1.0_pReal) &
crystallite_converged = .false.
if (any(crystallite_syncSubFrac)) then ! have to do syncing now, so all wait except for the synchronizers which do a cutback
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
crystallite_clearToWindForward(i,e) = crystallite_localPlasticity(1,i,e)
crystallite_clearToCutback(i,e) = crystallite_localPlasticity(1,i,e) .or. crystallite_syncSubFrac(i,e)
enddo
enddo
!$OMP END PARALLEL DO
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> time synchronization: cutback'
!$OMP END CRITICAL (write2out)
endif
else
!$OMP PARALLEL DO PRIVATE(myNgrains)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if(.not. crystallite_converged(1,i,e)) crystallite_clearToCutback(i,e) = .true.
enddo
enddo
!$OMP END PARALLEL DO
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,i6)') '<< CRYST >> cutback'
!$OMP END CRITICAL (write2out)
endif
endif
endif
endif
! Make sure that all cutbackers start with the same substep
where(.not. crystallite_localPlasticity .and. .not. crystallite_converged) &
crystallite_subStep = minval(crystallite_subStep, mask=.not. crystallite_localPlasticity &
.and. .not. crystallite_converged)
! Those that do neither wind forward nor cutback are not to do
!$OMP PARALLEL DO PRIVATE(myNgrains)
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
elementLooping2: do e = FEsolving_execElem(1),FEsolving_execElem(2)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
if(.not. crystallite_clearToWindForward(i,e) .and. .not. crystallite_clearToCutback(i,e)) &
crystallite_todo(1,i,e) = .false.
enddo
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
enddo elementLooping2
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP END PARALLEL DO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
endif timeSyncing1
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP PARALLEL DO PRIVATE(myNgrains,formerSubStep)
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
elementLooping3: do e = FEsolving_execElem(1),FEsolving_execElem(2)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e) ! iterate over IPs of this element to be processed
do g = 1,myNgrains
! --- wind forward ---
if (crystallite_converged(g,i,e) .and. crystallite_clearToWindForward(i,e)) then
formerSubStep = crystallite_subStep(g,i,e)
crystallite_subFrac(g,i,e) = crystallite_subFrac(g,i,e) + crystallite_subStep(g,i,e)
!$OMP FLUSH(crystallite_subFrac)
crystallite_subStep(g,i,e) = min(1.0_pReal - crystallite_subFrac(g,i,e), &
stepIncreaseCryst * crystallite_subStep(g,i,e))
!$OMP FLUSH(crystallite_subStep)
if (crystallite_subStep(g,i,e) > 0.0_pReal) then
crystallite_subF0(1:3,1:3,g,i,e) = crystallite_subF(1:3,1:3,g,i,e) ! ...def grad
!$OMP FLUSH(crystallite_subF0)
crystallite_subFp0(1:3,1:3,g,i,e) = crystallite_Fp(1:3,1:3,g,i,e) ! ...plastic def grad
crystallite_subFe0(1:3,1:3,g,i,e) = &
math_mul33x33(crystallite_subF(1:3,1:3,g,i,e), crystallite_invFp(1:3,1:3,g,i,e)) ! only needed later on for stiffness calculation
crystallite_subLp0(1:3,1:3,g,i,e) = crystallite_Lp(1:3,1:3,g,i,e) ! ...plastic velocity gradient
constitutive_subState0(g,i,e)%p = constitutive_state(g,i,e)%p ! ...microstructure
crystallite_subTstar0_v(1:6,g,i,e) = crystallite_Tstar_v(1:6,g,i,e) ! ...2nd PK stress
if (crystallite_syncSubFrac(i,e)) then ! if we just did a synchronization of states, then we wind forward without any further time integration
crystallite_syncSubFracCompleted(i,e) = .true.
crystallite_syncSubFrac(i,e) = .false.
crystallite_todo(g,i,e) = .false.
else
crystallite_todo(g,i,e) = .true.
endif
!$OMP FLUSH(crystallite_todo)
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (iand(debug_level(debug_crystallite),debug_levelBasic) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) &
write(6,'(a,f12.8,a,f12.8,a,i8,1x,i2,1x,i3,/)') '<< CRYST >> winding forward from ', &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_subFrac(g,i,e)-formerSubStep,' to current crystallite_subfrac ', &
crystallite_subFrac(g,i,e),' in crystallite_stressAndItsTangent at el ip g ',e,i,g
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
last commit also solves problem with infinite loop in case of a cutback in homogenization corrected indentation of a comment
2013-08-02 13:29:55 +05:30
else ! this crystallite just converged for the entire timestep
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
crystallite_todo(g,i,e) = .false. ! so done here
!$OMP FLUSH(crystallite_todo)
remnoved some unused fuctions from use statements
2013-08-02 11:48:41 +05:30
if (iand(debug_level(debug_crystallite),debug_levelBasic) /= 0_pInt &
.and. formerSubStep > 0.0_pReal) then
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP CRITICAL (distributionCrystallite)
debug_CrystalliteLoopDistribution(min(nCryst+1_pInt,NiterationCrystallite)) = &
debug_CrystalliteLoopDistribution(min(nCryst+1_pInt,NiterationCrystallite)) + 1_pInt
!$OMP END CRITICAL (distributionCrystallite)
endif
endif
! --- cutback ---
elseif (.not. crystallite_converged(g,i,e) .and. crystallite_clearToCutback(i,e)) then
if (crystallite_syncSubFrac(i,e)) then ! synchronize time
crystallite_subStep(g,i,e) = subFracIntermediate
else
crystallite_subStep(g,i,e) = subStepSizeCryst * crystallite_subStep(g,i,e) ! cut step in half and restore...
endif
!$OMP FLUSH(crystallite_subStep)
crystallite_Fp(1:3,1:3,g,i,e) = crystallite_subFp0(1:3,1:3,g,i,e) ! ...plastic def grad
!$OMP FLUSH(crystallite_Fp)
crystallite_invFp(1:3,1:3,g,i,e) = math_inv33(crystallite_Fp(1:3,1:3,g,i,e))
!$OMP FLUSH(crystallite_invFp)
crystallite_Lp(1:3,1:3,g,i,e) = crystallite_subLp0(1:3,1:3,g,i,e) ! ...plastic velocity grad
constitutive_state(g,i,e)%p = constitutive_subState0(g,i,e)%p ! ...microstructure
crystallite_Tstar_v(1:6,g,i,e) = crystallite_subTstar0_v(1:6,g,i,e) ! ...2nd PK stress
! cant restore dotState here, since not yet calculated in first cutback after initialization
crystallite_todo(g,i,e) = crystallite_subStep(g,i,e) > subStepMinCryst ! still on track or already done (beyond repair)
!$OMP FLUSH(crystallite_todo)
polishing
2012-11-22 15:28:36 +05:30
#ifndef _OPENMP
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if(iand(debug_level(debug_crystallite),debug_levelBasic) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
if (crystallite_todo(g,i,e)) then
write(6,'(a,f12.8,a,i8,1x,i2,1x,i3)') '<< CRYST >> cutback step in crystallite_stressAndItsTangent &
&with new crystallite_subStep: ',&
crystallite_subStep(g,i,e),' at el ip g ',e,i,g
else
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> reached minimum step size &
&in crystallite_stressAndItsTangent at el ip g ',e,i,g
endif
write(6,*)
endif
polishing
2012-11-22 15:28:36 +05:30
#endif
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
endif
! --- prepare for integration ---
if (crystallite_todo(g,i,e) .and. (crystallite_clearToWindForward(i,e) .or. crystallite_clearToCutback(i,e))) then
crystallite_subF(1:3,1:3,g,i,e) = crystallite_subF0(1:3,1:3,g,i,e) &
+ crystallite_subStep(g,i,e) &
* (crystallite_partionedF(1:3,1:3,g,i,e) &
- crystallite_partionedF0(1:3,1:3,g,i,e))
!$OMP FLUSH(crystallite_subF)
crystallite_Fe(1:3,1:3,g,i,e) = math_mul33x33(crystallite_subF(1:3,1:3,g,i,e), crystallite_invFp(1:3,1:3,g,i,e))
crystallite_subdt(g,i,e) = crystallite_subStep(g,i,e) * crystallite_dt(g,i,e)
crystallite_converged(g,i,e) = .false. ! start out non-converged
endif
enddo ! grains
enddo ! IPs
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
enddo elementLooping3
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
!$OMP END PARALLEL DO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
timeSyncing2: if(numerics_timeSyncing) then
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (any(.not. crystallite_localPlasticity .and. .not. crystallite_todo .and. .not. crystallite_converged &
.and. crystallite_subStep <= subStepMinCryst)) then ! no way of rescuing a nonlocal ip that violated the lower time step limit, ...
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
elementLooping4: do e = FEsolving_execElem(1),FEsolving_execElem(2)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
do g = 1,myNgrains
if (.not. crystallite_localPlasticity(g,i,e) .and. .not. crystallite_todo(g,i,e) &
.and. .not. crystallite_converged(g,i,e) .and. crystallite_subStep(g,i,e) <= subStepMinCryst) then
!$OMP CRITICAL (write2out)
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> nonlocal violated minimum subStep at el,ip,g ',e,i,g
!$OMP END CRITICAL (write2out)
endif
enddo
enddo
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
enddo elementLooping4
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
endif
where(.not. crystallite_localPlasticity)
crystallite_todo = .false. ! ... so let all nonlocal ips die peacefully
crystallite_subStep = 0.0_pReal
endwhere
endif
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
endif timeSyncing2
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(/,a,e12.5)') '<< CRYST >> min(subStep) ',minval(crystallite_subStep)
write(6,'(a,e12.5)') '<< CRYST >> max(subStep) ',maxval(crystallite_subStep)
write(6,'(a,e12.5)') '<< CRYST >> min(subFrac) ',minval(crystallite_subFrac)
write(6,'(a,e12.5,/)') '<< CRYST >> max(subFrac) ',maxval(crystallite_subFrac)
!$OMP END CRITICAL (write2out)
endif
! --- integrate --- requires fully defined state array (basic + dependent state)
if (any(crystallite_todo)) then
select case(numerics_integrator(numerics_integrationMode))
case(1_pInt)
call crystallite_integrateStateFPI()
case(2_pInt)
call crystallite_integrateStateEuler()
case(3_pInt)
call crystallite_integrateStateAdaptiveEuler()
case(4_pInt)
call crystallite_integrateStateRK4()
case(5_pInt)
call crystallite_integrateStateRKCK45()
end select
endif
where(.not. crystallite_converged .and. crystallite_subStep > subStepMinCryst) & ! do not try non-converged & fully cutbacked any further
crystallite_todo = .true.
NiterationCrystallite = NiterationCrystallite + 1_pInt
enddo cutbackLooping
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
! --+>> CHECK FOR NON-CONVERGED CRYSTALLITES <<+--
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
elementLooping5: do e = FEsolving_execElem(1),FEsolving_execElem(2)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e) ! iterate over IPs of this element to be processed
do g = 1,myNgrains
if (.not. crystallite_converged(g,i,e)) then ! respond fully elastically (might be not required due to becoming terminally ill anyway)
if(iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (write2out)
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
write(6,'(a,i8,1x,i2,1x,i3,/)') '<< CRYST >> no convergence: respond fully elastic at el ip g ',e,i,g
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
!$OMP END CRITICAL (write2out)
endif
invFp = math_inv33(crystallite_partionedFp0(1:3,1:3,g,i,e))
Fe_guess = math_mul33x33(crystallite_partionedF(1:3,1:3,g,i,e), invFp)
call constitutive_TandItsTangent(Tstar, junk2, Fe_guess,g,i,e)
crystallite_P(1:3,1:3,g,i,e) = math_mul33x33(Fe_guess,math_mul33x33(Tstar,transpose(invFp)))
endif
if(iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt &
fixed bug in crystallite_FPI: stateDamper always has to be defined for each grain added some OMP FLUSH statements were necessary replaced openmp do by forall construct where possible; this is much safer and perhaps even as fast for small loops
2012-11-07 21:13:29 +05:30
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite),debug_levelSelective) /= 0_pInt)) then
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
!$OMP CRITICAL (write2out)
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> central solution of cryst_StressAndTangent at el ip g ',e,i,g
write(6,'(/,a,/,3(12x,3(f12.4,1x)/))') '<< CRYST >> P / MPa', &
math_transpose33(crystallite_P(1:3,1:3,g,i,e))/1.0e6_pReal
write(6,'(a,/,3(12x,3(f14.9,1x)/))') '<< CRYST >> Fp', &
math_transpose33(crystallite_Fp(1:3,1:3,g,i,e))
write(6,'(a,/,3(12x,3(f14.9,1x)/),/)') '<< CRYST >> Lp', &
math_transpose33(crystallite_Lp(1:3,1:3,g,i,e))
!$OMP END CRITICAL (write2out)
endif
enddo
enddo
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
enddo elementLooping5
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
Tstar_v is now restored at different stages of cutbacking; we need this because preguess of state relies on consistent Tstar_v
2009-06-16 14:33:30 +05:30
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-((( * also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 22:52:48 +05:30
! --+>> STIFFNESS CALCULATION <<+--
Tstar_v is now restored at different stages of cutbacking; we need this because preguess of state relies on consistent Tstar_v
2009-06-16 14:33:30 +05:30
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
computeJacobian: if(updateJaco) then
jacobianMethod: if (analyticJaco) then
constitutive_nonlocal: - corrected flux term - multiplication is now aware of dislocation type - corrected change rate for "dipole size" dupper - corrected term for dipole dissociation by stress change - added transmissivity term in fluxes which accounts for misorientation between two neighboring grains (yet hardcoded transmissivity according to misorientation angle) - added more output variables constitutive: - 2 additional variables "previousDotState" and "previousDotState2", which are used to store the previous and second previous dotState (used in crystallite for acceleration/stabilization of state integration) - timer for dotState now measures the time for calls to constitutive_ collectState (used to reside in crystallite_updateState, which is not critical in terms of calculation time anymore) crystallite: - convergence check for nonlocal elments is now done at end of crystallite loop, not at the beginning; we simple set all elements to not converged if there is at least one nonlocal element that did not converge - need call to microstructure before first call to collect dotState for dependent states - stiffness calculation (jacobian): if there are nonlocal elements, we also have to consider changes in our neighborhood's states; so for every perturbed component in a single ip, we have to loop over all elements; since this is extremely time-consuming, we just perturb one component per cycle, starting with the one that changes the most during regular time step. - updateState gets a damping prefactor for our dotState that helps to improve convergence; prefactor is calculated according to change of dotState IO: - additional warning message for unknown crystal symmetry
2009-12-15 13:50:31 +05:30
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
! --- ANALYTIC JACOBIAN ---
!$OMP PARALLEL DO PRIVATE(dFedF,dSdF,dSdFe,myNgrains)
elementLooping6: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e) ! iterate over IPs of this element to be processed
do g = 1_pInt,myNgrains
dFedF = 0.0_pReal
forall(p=1_pInt:3_pInt, o=1_pInt:3_pInt) &
dFedF(p,o,o,1:3) = crystallite_invFp(1:3,p,g,i,e) ! dFe^T_ij/dF_kl = delta_jk * (Fp current^-1)_li
call constitutive_TandItsTangent(junk,dSdFe,crystallite_subFe0(1:3,1:3,g,i,e),g,i,e) ! call constitutive law to calculate 2nd Piola-Kirchhoff stress and its derivative
dSdF = math_mul3333xx3333(dSdFe,dFedF) ! dS/dF = dS/dFe * dFe/dF
forall(p=1_pInt:3_pInt, o=1_pInt:3_pInt) &
crystallite_dPdF(1:3,1:3,o,p,g,i,e) = math_mul33x33(math_mul33x33(dFedF(1:3,1:3,o,p),&
math_Mandel6to33(crystallite_Tstar_v)),math_transpose33(&
crystallite_invFp(1:3,1:3,g,i,e))) & ! dP/dF = dFe/dF * S * Fp^-T...
+ math_mul33x33(crystallite_subFe0(1:3,1:3,g,i,e),&
math_mul33x33(dSdF(1:3,1:3,o,p),math_transpose33(crystallite_invFp(1:3,1:3,g,i,e)))) ! + Fe * dS/dF * Fp^-T
enddo; enddo
enddo elementLooping6
!$OMP END PARALLEL DO
else jacobianMethod
! --- STANDARD (PERTURBATION METHOD) FOR JACOBIAN ---
numerics_integrationMode = 2_pInt
! --- BACKUP ---
elementLooping7: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains)
constitutive_state_backup(g,i,e)%p(1:constitutive_sizeState(g,i,e)) = &
constitutive_state(g,i,e)%p(1:constitutive_sizeState(g,i,e)) ! remember unperturbed, converged state, ...
constitutive_dotState_backup(g,i,e)%p(1:constitutive_sizeDotState(g,i,e)) = &
constitutive_dotState(g,i,e)%p(1:constitutive_sizeDotState(g,i,e)) ! ... dotStates, ...
endforall
enddo elementLooping7
F_backup = crystallite_subF ! ... and kinematics
Fp_backup = crystallite_Fp
InvFp_backup = crystallite_invFp
Fe_backup = crystallite_Fe
Lp_backup = crystallite_Lp
Tstar_v_backup = crystallite_Tstar_v
P_backup = crystallite_P
convergenceFlag_backup = crystallite_converged
! --- CALCULATE STATE AND STRESS FOR PERTURBATION ---
dPdF_perturbation1 = crystallite_dPdF0 ! initialize stiffness with known good values from last increment
dPdF_perturbation2 = crystallite_dPdF0 ! initialize stiffness with known good values from last increment
do perturbation = 1,2 ! forward and backward perturbation
if (iand(pert_method,perturbation) > 0_pInt) then ! mask for desired direction
myPert = -pert_Fg * (-1.0_pReal)**perturbation ! set perturbation step
do k = 1,3; do l = 1,3 ! ...alter individual components
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,2(1x,i1),1x,a,/)') '<< CRYST >> [[[[[[ Stiffness perturbation',k,l,']]]]]]'
!$OMP END CRITICAL (write2out)
endif
! --- INITIALIZE UNPERTURBED STATE ---
select case(numerics_integrator(numerics_integrationMode))
case(1_pInt) ! Fix-point method: restore to last converged state at end of subinc, since this is probably closest to perturbed state
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains)
constitutive_state(g,i,e)%p(1:constitutive_sizeState(g,i,e)) = &
constitutive_state_backup(g,i,e)%p(1:constitutive_sizeState(g,i,e))
constitutive_dotState(g,i,e)%p(1:constitutive_sizeDotState(g,i,e)) = &
constitutive_dotState_backup(g,i,e)%p(1:constitutive_sizeDotState(g,i,e))
endforall
enddo
crystallite_Fp = Fp_backup
crystallite_invFp = InvFp_backup
crystallite_Fe = Fe_backup
crystallite_Lp = Lp_backup
crystallite_Tstar_v = Tstar_v_backup
case(2_pInt,3_pInt) ! explicit Euler methods: nothing to restore (except for F), since we are only doing a stress integration step
case(4_pInt,5_pInt) ! explicit Runge-Kutta methods: restore to start of subinc, since we are doing a full integration of state and stress
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains)
constitutive_state(g,i,e)%p(1:constitutive_sizeState(g,i,e)) = &
constitutive_subState0(g,i,e)%p(1:constitutive_sizeState(g,i,e))
constitutive_dotState(g,i,e)%p(1:constitutive_sizeDotState(g,i,e)) = &
constitutive_dotState_backup(g,i,e)%p(1:constitutive_sizeDotState(g,i,e))
endforall
enddo
crystallite_Fp = crystallite_subFp0
crystallite_Fe = crystallite_subFe0
crystallite_Lp = crystallite_subLp0
crystallite_Tstar_v = crystallite_subTstar0_v
end select
! --- PERTURB EITHER FORWARD OR BACKWARD ---
crystallite_subF = F_backup
crystallite_subF(k,l,:,:,:) = crystallite_subF(k,l,:,:,:) + myPert
crystallite_converged = convergenceFlag_backup
crystallite_todo = crystallite_requested .and. crystallite_converged
where (crystallite_todo) crystallite_converged = .false. ! start out non-converged
select case(numerics_integrator(numerics_integrationMode))
case(1_pInt)
call crystallite_integrateStateFPI()
case(2_pInt)
call crystallite_integrateStateEuler()
case(3_pInt)
call crystallite_integrateStateAdaptiveEuler()
case(4_pInt)
call crystallite_integrateStateRK4()
case(5_pInt)
call crystallite_integrateStateRKCK45()
end select
elementLooping8: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
select case(perturbation)
case(1_pInt)
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. crystallite_converged(g,i,e)) & ! converged state warrants stiffness update
dPdF_perturbation1(1:3,1:3,k,l,g,i,e) = (crystallite_P(1:3,1:3,g,i,e) - P_backup(1:3,1:3,g,i,e)) / myPert ! tangent dP_ij/dFg_kl
case(2_pInt)
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. crystallite_converged(g,i,e)) & ! converged state warrants stiffness update
dPdF_perturbation2(1:3,1:3,k,l,g,i,e) = (crystallite_P(1:3,1:3,g,i,e) - P_backup(1:3,1:3,g,i,e)) / myPert ! tangent dP_ij/dFg_kl
end select
enddo elementLooping8
enddo; enddo ! k,l component perturbation loop
endif
enddo ! perturbation direction
! --- STIFFNESS ACCORDING TO PERTURBATION METHOD AND CONVERGENCE ---
elementLooping9: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
select case(pert_method)
case(1_pInt)
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. convergenceFlag_backup(g,i,e)) & ! perturbation mode 1: central solution converged
crystallite_dPdF(1:3,1:3,1:3,1:3,g,i,e) = dPdF_perturbation1(1:3,1:3,1:3,1:3,g,i,e)
case(2_pInt)
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. convergenceFlag_backup(g,i,e)) & ! perturbation mode 2: central solution converged
crystallite_dPdF(1:3,1:3,1:3,1:3,g,i,e) = dPdF_perturbation2(1:3,1:3,1:3,1:3,g,i,e)
case(3_pInt)
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. convergenceFlag_backup(g,i,e)) & ! perturbation mode 3: central solution converged
crystallite_dPdF(1:3,1:3,1:3,1:3,g,i,e) = 0.5_pReal* ( dPdF_perturbation1(1:3,1:3,1:3,1:3,g,i,e) &
+ dPdF_perturbation2(1:3,1:3,1:3,1:3,g,i,e))
end select
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains, &
crystallite_requested(g,i,e) .and. .not. convergenceFlag_backup(g,i,e)) & ! for any pertubation mode: if central solution did not converge...
crystallite_dPdF(1:3,1:3,1:3,1:3,g,i,e) = crystallite_fallbackdPdF(1:3,1:3,1:3,1:3,g,i,e) ! ...use (elastic) fallback
enddo elementLooping9
! --- RESTORE ---
elementLooping10: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
forall (i = FEsolving_execIP(1,e):FEsolving_execIP(2,e), g = 1:myNgrains)
constitutive_state(g,i,e)%p(1:constitutive_sizeState(g,i,e)) = &
constitutive_state_backup(g,i,e)%p(1:constitutive_sizeState(g,i,e))
constitutive_dotState(g,i,e)%p(1:constitutive_sizeDotState(g,i,e)) = &
constitutive_dotState_backup(g,i,e)%p(1:constitutive_sizeDotState(g,i,e))
endforall
enddo elementLooping10
crystallite_subF = F_backup
crystallite_Fp = Fp_backup
crystallite_invFp = InvFp_backup
crystallite_Fe = Fe_backup
crystallite_Lp = Lp_backup
crystallite_Tstar_v = Tstar_v_backup
crystallite_P = P_backup
crystallite_converged = convergenceFlag_backup
endif jacobianMethod
rateSensitivity: if (rate_sensitivity) then
!$OMP PARALLEL DO PRIVATE(dFedFdot,dSdFdot,dSdFe,Fpinv_rate,FDot_inv,counter,dFp_invdFdot,myNgrains)
elementLooping11: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e) ! iterate over IPs of this element to be processed
do g = 1_pInt,myNgrains
Fpinv_rate = math_mul33x33(crystallite_invFp(1:3,1:3,g,i,e),crystallite_Lp(1:3,1:3,g,i,e)) ! dFp^-1 = dFp^-1/dt *dt... dFp may overshoot dF by small ammount as
FDot_inv = crystallite_subF(1:3,1:3,g,i,e) - crystallite_F0(1:3,1:3,g,i,e)
counter = 0.0_pReal
do p=1_pInt,3_pInt; do o=1_pInt,3_pInt
if (abs(FDot_inv(o,p)) < relevantStrain) then
FDot_inv(o,p) = 0.0_pReal
else
counter = counter + 1.0_pReal
FDot_inv(o,p) = crystallite_dt(g,i,e)/FDot_inv(o,p)
endif
enddo; enddo
if (counter > 0.0_pReal) FDot_inv = FDot_inv/counter
forall(p=1_pInt:3_pInt, o=1_pInt:3_pInt) &
dFp_invdFdot(o,p,1:3,1:3) = Fpinv_rate(o,p)*FDot_inv
forall(p=1_pInt:3_pInt, o=1_pInt:3_pInt) &
dFedFdot(1:3,1:3,o,p) = math_transpose33(math_mul33x33(crystallite_subF(1:3,1:3,g,i,e), &
dFp_invdFdot(1:3,1:3,o,p)))
call constitutive_TandItsTangent(junk,dSdFe,crystallite_subFe0(1:3,1:3,g,i,e),g,i,e) ! call constitutive law to calculate 2nd Piola-Kirchhoff stress and its derivative
dSdFdot = math_mul3333xx3333(dSdFe,dFedFdot)
forall(p=1_pInt:3_pInt, o=1_pInt:3_pInt) &
crystallite_dPdF(1:3,1:3,o,p,g,i,e) = crystallite_dPdF(1:3,1:3,o,p,g,i,e) - &
(math_mul33x33(math_mul33x33(dFedFdot(1:3,1:3,o,p), &
math_Mandel6to33(crystallite_Tstar_v)),math_transpose33( &
crystallite_invFp(1:3,1:3,g,i,e))) + & ! dP/dFdot = dFe/dFdot * S * Fp^-T...
math_mul33x33(math_mul33x33(crystallite_subFe0(1:3,1:3,g,i,e), &
math_Mandel6to33(crystallite_Tstar_v)),math_transpose33(dFp_invdFdot(1:3,1:3,o,p))) & ! + Fe * S * dFp^-T/dFdot...
+ math_mul33x33(crystallite_subFe0(1:3,1:3,g,i,e), &
math_mul33x33(dSdFdot(1:3,1:3,o,p),math_transpose33(crystallite_invFp(1:3,1:3,g,i,e))))) ! + Fe * dS/dFdot * Fp^-T
enddo; enddo;
enddo elementLooping11
!$OMP END PARALLEL DO
endif rateSensitivity
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
endif computeJacobian
elementLooping12: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(mesh_element(3,e))
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e) ! iterate over IPs of this element to be processed
do g = 1,myNgrains
crystallite_heat(g,i,e) = 0.98_pReal* &
Coupled phase field implementation for the basic petsc solver. needs clearing up… work in progress
2013-11-12 06:14:23 +05:30
abs(math_mul33xx33(math_Mandel6to33(crystallite_Tstar_v), &
crystallite_Lp(1:3,1:3,g,i,e)))
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
enddo
enddo
enddo elementLooping12
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end subroutine crystallite_stressAndItsTangent
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
!> @brief integrate stress, state with 4th order explicit Runge Kutta method
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
2013-04-26 18:53:36 +05:30
subroutine crystallite_integrateStateRK4()
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
use numerics, only: &
numerics_integrationMode
use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_StateLoopDistribution
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems, &
mesh_maxNips
use material, only: &
homogenization_Ngrains, &
homogenization_maxNgrains
use constitutive, only: &
constitutive_sizeDotState, &
constitutive_state, &
constitutive_subState0, &
constitutive_dotState, &
constitutive_RK4dotState, &
constitutive_collectDotState, &
constitutive_deltaState, &
constitutive_collectDeltaState, &
constitutive_microstructure
doxygen comments
2013-02-22 04:38:36 +05:30
implicit none
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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real(pReal), dimension(4), parameter :: &
TIMESTEPFRACTION = [0.5_pReal, 0.5_pReal, 1.0_pReal, 1.0_pReal] ! factor giving the fraction of the original timestep used for Runge Kutta Integration
real(pReal), dimension(4), parameter :: &
WEIGHT = [1.0_pReal, 2.0_pReal, 2.0_pReal, 1.0_pReal] ! weight of slope used for Runge Kutta integration
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
2013-04-26 18:53:36 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
integer(pInt) e, & ! element index in element loop
i, & ! integration point index in ip loop
g, & ! grain index in grain loop
n, &
mySizeDotState
integer(pInt), dimension(2) :: eIter ! bounds for element iteration
integer(pInt), dimension(2,mesh_NcpElems) :: iIter, & ! bounds for ip iteration
gIter ! bounds for grain iteration
fixed out of range bug introduced with singleRun changes in rev. 2356
2013-04-30 17:44:07 +05:30
logical :: singleRun ! flag indicating computation for single (g,i,e) triple
doxygen comments
2013-02-22 04:38:36 +05:30
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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eIter = FEsolving_execElem(1:2)
do e = eIter(1),eIter(2)
iIter(1:2,e) = FEsolving_execIP(1:2,e)
gIter(1:2,e) = [ 1_pInt,homogenization_Ngrains(mesh_element(3,e))]
enddo
fixed out of range bug introduced with singleRun changes in rev. 2356
2013-04-30 17:44:07 +05:30
singleRun = (eIter(1) == eIter(2) .and. iIter(1,eIter(1)) == iIter(2,eIter(2)))
doxygen comments
2013-02-22 04:38:36 +05:30
! --- FIRST RUNGE KUTTA STEP ---
!$OMP PARALLEL PRIVATE(mySizeDotState)
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
constitutive_RK4dotState(g,i,e)%p = 0.0_pReal ! initialize Runge-Kutta dotState
if (crystallite_todo(g,i,e)) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p /= constitutive_dotState(g,i,e)%p) )then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
! --- SECOND TO FOURTH RUNGE KUTTA STEP PLUS FINAL INTEGRATION ---
do n = 1_pInt,4_pInt
! --- state update ---
!$OMP PARALLEL PRIVATE(mySizeDotState)
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
if (n < 4) then
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constitutive_RK4dotState(g,i,e)%p = constitutive_RK4dotState(g,i,e)%p &
+ weight(n)*constitutive_dotState(g,i,e)%p
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elseif (n == 4) then
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constitutive_dotState(g,i,e)%p = (constitutive_RK4dotState(g,i,e)%p &
+ weight(n)*constitutive_dotState(g,i,e)%p) / 6.0_pReal ! use weighted RKdotState for final integration
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endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_subState0(g,i,e)%p(1:mySizeDotState) &
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+ constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
* crystallite_subdt(g,i,e) * timeStepFraction(n)
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if (n == 4) then ! final integration step
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
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#ifndef _OPENMP
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g)&
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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write(6,'(a,i8,1x,i2,1x,i3,/)') '<< CRYST >> updateState at el ip g ',e,i,g
fixed some e12.6 string formats to avoid compile time warnings
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write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> dotState', constitutive_dotState(g,i,e)%p(1:mySizeDotState)
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> new state', constitutive_state(g,i,e)%p(1:mySizeDotState)
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endif
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
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#endif
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endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- state jump ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- update dependent states ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
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crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- stress integration ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e,timeStepFraction(n)) ! fraction of original times step
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- dot state and RK dot state---
if (n < 4) then
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
timeStepFraction(n)*crystallite_subdt(g,i,e), & ! fraction of original timestep
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crystallite_subFrac, g,i,e)
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p /= constitutive_dotState(g,i,e)%p)) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
endif
!$OMP END PARALLEL
enddo
! --- SET CONVERGENCE FLAG ---
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
crystallite_converged(g,i,e) = .true. ! if still "to do" then converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(4,numerics_integrationMode) = &
debug_StateLoopDistribution(4,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
enddo; enddo; enddo
! --- CHECK NONLOCAL CONVERGENCE ---
if (.not. singleRun) then ! if not requesting Integration of just a single IP
if (any(.not. crystallite_converged .and. .not. crystallite_localPlasticity)) then ! any non-local not yet converged (or broken)...
crystallite_converged = crystallite_converged .and. crystallite_localPlasticity ! ...restart all non-local as not converged
endif
endif
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
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end subroutine crystallite_integrateStateRK4
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 17:48:49 +05:30
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!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!> @brief integrate stress, state with 5th order Runge-Kutta Cash-Karp method with
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!> adaptive step size (use 5th order solution to advance = "local extrapolation")
!--------------------------------------------------------------------------------------------------
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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subroutine crystallite_integrateStateRKCK45()
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_StateLoopDistribution
use numerics, only: &
rTol_crystalliteState, &
numerics_integrationMode
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems, &
mesh_maxNips
use material, only: &
homogenization_Ngrains, &
homogenization_maxNgrains
use constitutive, only: &
constitutive_sizeDotState, &
constitutive_maxSizeDotState, &
constitutive_state, &
constitutive_aTolState, &
constitutive_subState0, &
constitutive_dotState, &
constitutive_RKCK45dotState, &
constitutive_collectDotState, &
constitutive_deltaState, &
constitutive_collectDeltaState, &
constitutive_microstructure
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implicit none
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real(pReal), dimension(5,5), parameter :: &
A = reshape([&
.2_pReal, .075_pReal, .3_pReal, -11.0_pReal/54.0_pReal, 1631.0_pReal/55296.0_pReal, &
.0_pReal, .225_pReal, -.9_pReal, 2.5_pReal, 175.0_pReal/512.0_pReal, &
.0_pReal, .0_pReal, 1.2_pReal, -70.0_pReal/27.0_pReal, 575.0_pReal/13824.0_pReal, &
.0_pReal, .0_pReal, .0_pReal, 35.0_pReal/27.0_pReal, 44275.0_pReal/110592.0_pReal, &
.0_pReal, .0_pReal, .0_pReal, .0_pReal, 253.0_pReal/4096.0_pReal], &
[5,5], order=[2,1]) !< coefficients in Butcher tableau (used for preliminary integration in stages 2 to 6)
real(pReal), dimension(6), parameter :: &
B = &
[37.0_pReal/378.0_pReal, .0_pReal, 250.0_pReal/621.0_pReal, &
125.0_pReal/594.0_pReal, .0_pReal, 512.0_pReal/1771.0_pReal], & !< coefficients in Butcher tableau (used for final integration and error estimate)
DB = B - &
[2825.0_pReal/27648.0_pReal, .0_pReal, 18575.0_pReal/48384.0_pReal,&
13525.0_pReal/55296.0_pReal, 277.0_pReal/14336.0_pReal, 0.25_pReal] !< coefficients in Butcher tableau (used for final integration and error estimate)
real(pReal), dimension(5), parameter :: &
C = [0.2_pReal, 0.3_pReal, 0.6_pReal, 1.0_pReal, 0.875_pReal] !< coefficients in Butcher tableau (fractions of original time step in stages 2 to 6)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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integer(pInt) :: &
e, & ! element index in element loop
i, & ! integration point index in ip loop
g, & ! grain index in grain loop
n, & ! stage index in integration stage loop
mySizeDotState, & ! size of dot State
s ! state index
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integer(pInt), dimension(2) :: &
eIter ! bounds for element iteration
integer(pInt), dimension(2,mesh_NcpElems) :: &
iIter, & ! bounds for ip iteration
gIter ! bounds for grain iteration
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real(pReal), dimension(constitutive_maxSizeDotState,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
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stateResiduum, & ! residuum from evolution in micrstructure
relStateResiduum ! relative residuum from evolution in microstructure
logical :: &
singleRun ! flag indicating computation for single (g,i,e) triple
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! --- LOOP ITERATOR FOR ELEMENT, GRAIN, IP ---
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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eIter = FEsolving_execElem(1:2)
do e = eIter(1),eIter(2)
iIter(1:2,e) = FEsolving_execIP(1:2,e)
gIter(1:2,e) = [ 1_pInt,homogenization_Ngrains(mesh_element(3,e))]
enddo
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fixed out of range bug introduced with singleRun changes in rev. 2356
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singleRun = (eIter(1) == eIter(2) .and. iIter(1,eIter(1)) == iIter(2,eIter(2)))
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! --- FIRST RUNGE KUTTA STEP ---
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
write(6,'(a,1x,i1)') '<< CRYST >> RUNGE KUTTA STEP',1
!$OMP END CRITICAL (write2out)
endif
!$OMP PARALLEL PRIVATE(mySizeDotState)
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p /= constitutive_dotState(g,i,e)%p)) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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enddo; enddo; enddo
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!$OMP ENDDO
!$OMP END PARALLEL
! --- SECOND TO SIXTH RUNGE KUTTA STEP ---
do n = 1_pInt,5_pInt
! --- state update ---
!$OMP PARALLEL PRIVATE(mySizeDotState)
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_RKCK45dotState(n,g,i,e)%p = constitutive_dotState(g,i,e)%p ! store Runge-Kutta dotState
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
if (n == 1) then ! NEED TO DO THE ADDITION IN THIS LENGTHY WAY BECAUSE OF PARALLELIZATION (CAN'T USE A REDUCTION CLAUSE ON A POINTER OR USER DEFINED TYPE)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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constitutive_dotState(g,i,e)%p = A(1,1) * constitutive_RKCK45dotState(1,g,i,e)%p
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elseif (n == 2) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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constitutive_dotState(g,i,e)%p = A(1,2) * constitutive_RKCK45dotState(1,g,i,e)%p &
+ A(2,2) * constitutive_RKCK45dotState(2,g,i,e)%p
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elseif (n == 3) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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constitutive_dotState(g,i,e)%p = A(1,3) * constitutive_RKCK45dotState(1,g,i,e)%p &
+ A(2,3) * constitutive_RKCK45dotState(2,g,i,e)%p &
+ A(3,3) * constitutive_RKCK45dotState(3,g,i,e)%p
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elseif (n == 4) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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constitutive_dotState(g,i,e)%p = A(1,4) * constitutive_RKCK45dotState(1,g,i,e)%p &
+ A(2,4) * constitutive_RKCK45dotState(2,g,i,e)%p &
+ A(3,4) * constitutive_RKCK45dotState(3,g,i,e)%p &
+ A(4,4) * constitutive_RKCK45dotState(4,g,i,e)%p
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elseif (n == 5) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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constitutive_dotState(g,i,e)%p = A(1,5) * constitutive_RKCK45dotState(1,g,i,e)%p &
+ A(2,5) * constitutive_RKCK45dotState(2,g,i,e)%p &
+ A(3,5) * constitutive_RKCK45dotState(3,g,i,e)%p &
+ A(4,5) * constitutive_RKCK45dotState(4,g,i,e)%p &
+ A(5,5) * constitutive_RKCK45dotState(5,g,i,e)%p
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endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_subState0(g,i,e)%p(1:mySizeDotState) &
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+ constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
* crystallite_subdt(g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
! --- state jump ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- update dependent states ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
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crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- stress integration ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e,c(n)) ! fraction of original time step
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- dot state and RK dot state---
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#ifndef _OPENMP
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
write(6,'(a,1x,i1)') '<< CRYST >> Runge--Kutta step',n+1_pInt
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#endif
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
C(n)*crystallite_subdt(g,i,e), & ! fraction of original timestep
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crystallite_subFrac, g,i,e)
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p/=constitutive_dotState(g,i,e)%p)) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
enddo
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- STATE UPDATE WITH ERROR ESTIMATE FOR STATE ---
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relStateResiduum = 0.0_pReal
!$OMP PARALLEL PRIVATE(mySizeDotState)
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_RKCK45dotState(6,g,i,e)%p = constitutive_dotState(g,i,e)%p ! store Runge-Kutta dotState
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- absolute residuum in state ---
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! NEED TO DO THE ADDITION IN THIS LENGTHY WAY BECAUSE OF PARALLELIZATION
! CAN'T USE A REDUCTION CLAUSE ON A POINTER OR USER DEFINED TYPE
stateResiduum(1:mySizeDotState,g,i,e) = &
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( DB(1) * constitutive_RKCK45dotState(1,g,i,e)%p(1:mySizeDotState) &
+ DB(2) * constitutive_RKCK45dotState(2,g,i,e)%p(1:mySizeDotState) &
+ DB(3) * constitutive_RKCK45dotState(3,g,i,e)%p(1:mySizeDotState) &
+ DB(4) * constitutive_RKCK45dotState(4,g,i,e)%p(1:mySizeDotState) &
+ DB(5) * constitutive_RKCK45dotState(5,g,i,e)%p(1:mySizeDotState) &
+ DB(6) * constitutive_RKCK45dotState(6,g,i,e)%p(1:mySizeDotState)) &
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* crystallite_subdt(g,i,e)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- dot state ---
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constitutive_dotState(g,i,e)%p = B(1) * constitutive_RKCK45dotState(1,g,i,e)%p &
+ B(2) * constitutive_RKCK45dotState(2,g,i,e)%p &
+ B(3) * constitutive_RKCK45dotState(3,g,i,e)%p &
+ B(4) * constitutive_RKCK45dotState(4,g,i,e)%p &
+ B(5) * constitutive_RKCK45dotState(5,g,i,e)%p &
+ B(6) * constitutive_RKCK45dotState(6,g,i,e)%p
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endif
enddo; enddo; enddo
!$OMP ENDDO
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- state and update ---
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_subState0(g,i,e)%p(1:mySizeDotState) &
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+ constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
* crystallite_subdt(g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
! --- relative residui and state convergence ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
forall (s = 1_pInt:mySizeDotState, abs(constitutive_state(g,i,e)%p(s)) > 0.0_pReal) &
relStateResiduum(s,g,i,e) = stateResiduum(s,g,i,e) / constitutive_state(g,i,e)%p(s)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!$OMP FLUSH(relStateResiduum)
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crystallite_todo(g,i,e) = &
( all( abs(relStateResiduum(:,g,i,e)) < rTol_crystalliteState &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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.or. abs(stateResiduum(1:mySizeDotState,g,i,e)) < constitutive_aTolState(g,i,e)%p(1:mySizeDotState) ))
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* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#ifndef _OPENMP
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt&
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g)&
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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write(6,'(a,i8,1x,i3,1x,i3,/)') '<< CRYST >> updateState at el ip g ',e,i,g
write(6,'(a,/,(12x,12(f12.1,1x)),/)') '<< CRYST >> absolute residuum tolerance', &
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stateResiduum(1:mySizeDotState,g,i,e) / constitutive_aTolState(g,i,e)%p(1:mySizeDotState)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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write(6,'(a,/,(12x,12(f12.1,1x)),/)') '<< CRYST >> relative residuum tolerance', &
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relStateResiduum(1:mySizeDotState,g,i,e) / rTol_crystalliteState
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> dotState', constitutive_dotState(g,i,e)%p(1:mySizeDotState)
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> new state', constitutive_state(g,i,e)%p(1:mySizeDotState)
doxygen comments
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endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
doxygen comments
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endif
Depending on which state integrator one uses for the stiffness calculation, the initial state has to be chosen accordingly: e.g. for FPI choose last converged state, but for explicit RK choose converged state from start of increment (in case of explicit euler no state integration at all, but only stress integration). For this purpose we also need to remember "Fe" which now follows the cutbacking procedure as it is used for "Fp".
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enddo; enddo; enddo
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!$OMP ENDDO
! --- STATE JUMP ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
Depending on which state integrator one uses for the stiffness calculation, the initial state has to be chosen accordingly: e.g. for FPI choose last converged state, but for explicit RK choose converged state from start of increment (in case of explicit euler no state integration at all, but only stress integration). For this purpose we also need to remember "Fe" which now follows the cutbacking procedure as it is used for "Fp".
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enddo; enddo; enddo
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!$OMP ENDDO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
!--------------------------------------------------------------------------------------------------
! --- UPDATE DEPENDENT STATES IF RESIDUUM BELOW TOLERANCE ---
doxygen comments
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
doxygen comments
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crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
endif
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
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enddo; enddo; enddo
doxygen comments
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!$OMP ENDDO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
!--------------------------------------------------------------------------------------------------
! --- FINAL STRESS INTEGRATION STEP IF RESIDUUM BELOW TOLERANCE ---
doxygen comments
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
!--------------------------------------------------------------------------------------------------
! --- SET CONVERGENCE FLAG ---
doxygen comments
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
crystallite_converged(g,i,e) = .true. ! if still "to do" then converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(6,numerics_integrationMode) = &
debug_StateLoopDistribution(6,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
! --- nonlocal convergence check ---
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
write(6,'(a,i8,a,i2,/)') '<< CRYST >> ', count(crystallite_converged(:,:,:)), ' grains converged'
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!$OMP END CRITICAL (write2out)
endif
if (.not. singleRun) then ! if not requesting Integration of just a single IP
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if ( any(.not. crystallite_converged .and. .not. crystallite_localPlasticity)) & ! any non-local not yet converged (or broken)...
doxygen comments
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crystallite_converged = crystallite_converged .and. crystallite_localPlasticity ! ...restart all non-local as not converged
endif
end subroutine crystallite_integrateStateRKCK45
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 17:48:49 +05:30
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
2012-05-17 20:55:21 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
!> @brief integrate stress, state with 1st order Euler method with adaptive step size
doxygen comments
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!--------------------------------------------------------------------------------------------------
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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subroutine crystallite_integrateStateAdaptiveEuler()
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_StateLoopDistribution
use numerics, only: &
rTol_crystalliteState, &
numerics_integrationMode
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems, &
mesh_maxNips
use material, only: &
homogenization_Ngrains, &
homogenization_maxNgrains
use constitutive, only: &
constitutive_sizeDotState, &
constitutive_maxSizeDotState, &
constitutive_state, &
constitutive_aTolState, &
constitutive_subState0, &
constitutive_dotState, &
constitutive_collectDotState, &
constitutive_microstructure
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implicit none
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integer(pInt) :: &
e, & ! element index in element loop
i, & ! integration point index in ip loop
g, & ! grain index in grain loop
mySizeDotState, & ! size of dot State
s ! state index
integer(pInt), dimension(2) :: &
eIter ! bounds for element iteration
integer(pInt), dimension(2,mesh_NcpElems) :: &
iIter, & ! bounds for ip iteration
gIter ! bounds for grain iteration
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real(pReal), dimension(constitutive_maxSizeDotState,homogenization_maxNgrains,mesh_maxNips,mesh_NcpElems) :: &
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stateResiduum, & ! residuum from evolution in micrstructure
relStateResiduum ! relative residuum from evolution in microstructure
logical :: &
singleRun ! flag indicating computation for single (g,i,e) triple
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! --- LOOP ITERATOR FOR ELEMENT, GRAIN, IP ---
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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eIter = FEsolving_execElem(1:2)
do e = eIter(1),eIter(2)
iIter(1:2,e) = FEsolving_execIP(1:2,e)
gIter(1:2,e) = [ 1_pInt,homogenization_Ngrains(mesh_element(3,e))]
enddo
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fixed out of range bug introduced with singleRun changes in rev. 2356
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singleRun = (eIter(1) == eIter(2) .and. iIter(1,eIter(1)) == iIter(2,eIter(2)))
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stateResiduum = 0.0_pReal
!$OMP PARALLEL PRIVATE(mySizeDotState)
if (numerics_integrationMode == 1_pInt) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- DOT STATE (EULER INTEGRATION) ---
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
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endif
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
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enddo; enddo; enddo
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!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p /= constitutive_dotState(g,i,e)%p)) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
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enddo; enddo; enddo
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!$OMP ENDDO
! --- STATE UPDATE (EULER INTEGRATION) ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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stateResiduum(1:mySizeDotState,g,i,e) = - 0.5_pReal * constitutive_dotState(g,i,e)%p &
* crystallite_subdt(g,i,e) ! contribution to absolute residuum in state
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constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_state(g,i,e)%p(1:mySizeDotState) &
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+ constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
* crystallite_subdt(g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
! --- STATE JUMP ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- UPDATE DEPENDENT STATES (EULER INTEGRATION) ---
!$OMP DO
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (crystallite_todo(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
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enddo; enddo; enddo
!$OMP ENDDO
endif
! --- STRESS INTEGRATION (EULER INTEGRATION) ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
if (numerics_integrationMode == 1_pInt) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- DOT STATE (HEUN METHOD) ---
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (crystallite_todo(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
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enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p /= constitutive_dotState(g,i,e)%p) ) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- ERROR ESTIMATE FOR STATE (HEUN METHOD) ---
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!$OMP SINGLE
relStateResiduum = 0.0_pReal
!$OMP END SINGLE
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
! --- contribution of heun step to absolute residui ---
stateResiduum(1:mySizeDotState,g,i,e) = stateResiduum(1:mySizeDotState,g,i,e) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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+ 0.5_pReal * constitutive_dotState(g,i,e)%p &
* crystallite_subdt(g,i,e) ! contribution to absolute residuum in state
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!$OMP FLUSH(stateResiduum)
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! --- relative residui ---
forall (s = 1_pInt:mySizeDotState, abs(constitutive_state(g,i,e)%p(s)) > 0.0_pReal) &
relStateResiduum(s,g,i,e) = stateResiduum(s,g,i,e) / constitutive_state(g,i,e)%p(s)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!$OMP FLUSH(relStateResiduum)
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* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#ifndef _OPENMP
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g)&
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> updateState at el ip g ',e,i,g
write(6,*)
write(6,'(a,/,(12x,12(f12.1,1x)))') '<< CRYST >> absolute residuum tolerance', &
stateResiduum(1:mySizeDotState,g,i,e) / constitutive_aTolState(g,i,e)%p(1:mySizeDotState)
write(6,*)
write(6,'(a,/,(12x,12(f12.1,1x)))') '<< CRYST >> relative residuum tolerance', &
relStateResiduum(1:mySizeDotState,g,i,e) / rTol_crystalliteState
write(6,*)
write(6,'(a,/,(12x,12(e12.5,1x)))') '<< CRYST >> dotState', constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
one line was beyond 132 characters
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- 2.0_pReal * stateResiduum(1:mySizeDotState,g,i,e) / crystallite_subdt(g,i,e) ! calculate former dotstate from higher order solution and state residuum
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write(6,*)
write(6,'(a,/,(12x,12(e12.5,1x)))') '<< CRYST >> new state', constitutive_state(g,i,e)%p(1:mySizeDotState)
write(6,*)
endif
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
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#endif
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! --- converged ? ---
if ( all( abs(relStateResiduum(:,g,i,e)) < rTol_crystalliteState &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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.or. abs(stateResiduum(1:mySizeDotState,g,i,e)) < constitutive_aTolState(g,i,e)%p(1:mySizeDotState))) then
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crystallite_converged(g,i,e) = .true. ! ... converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(2,numerics_integrationMode) = &
debug_StateLoopDistribution(2,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
elseif (numerics_integrationMode > 1) then ! stiffness calculation
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
crystallite_converged(g,i,e) = .true. ! ... converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(2,numerics_integrationMode) = &
debug_StateLoopDistribution(2,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
endif
!$OMP END PARALLEL
! --- NONLOCAL CONVERGENCE CHECK ---
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL (write2out)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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write(6,'(a,i8,a,i2,/)') '<< CRYST >> ', count(crystallite_converged(:,:,:)), ' grains converged'
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!$OMP END CRITICAL (write2out)
endif
if (.not. singleRun) then ! if not requesting Integration of just a single IP
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if ( any(.not. crystallite_converged .and. .not. crystallite_localPlasticity)) & ! any non-local not yet converged (or broken)...
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crystallite_converged = crystallite_converged .and. crystallite_localPlasticity ! ...restart all non-local as not converged
endif
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end subroutine crystallite_integrateStateAdaptiveEuler
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 17:48:49 +05:30
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!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!> @brief integrate stress, and state with 1st order explicit Euler method
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!--------------------------------------------------------------------------------------------------
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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subroutine crystallite_integrateStateEuler()
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_StateLoopDistribution
use numerics, only: &
numerics_integrationMode, &
numerics_timeSyncing
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems
use material, only: &
homogenization_Ngrains
use constitutive, only: &
constitutive_sizeDotState, &
constitutive_state, &
constitutive_subState0, &
constitutive_dotState, &
constitutive_collectDotState, &
constitutive_microstructure
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implicit none
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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integer(pInt) :: &
e, & ! element index in element loop
i, & ! integration point index in ip loop
g, & ! grain index in grain loop
mySizeDotState ! size of dot State
integer(pInt), dimension(2) :: &
eIter ! bounds for element iteration
integer(pInt), dimension(2,mesh_NcpElems) :: &
iIter, & ! bounds for ip iteration
gIter ! bounds for grain iteration
logical :: &
singleRun ! flag indicating computation for single (g,i,e) triple
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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eIter = FEsolving_execElem(1:2)
do e = eIter(1),eIter(2)
iIter(1:2,e) = FEsolving_execIP(1:2,e)
gIter(1:2,e) = [ 1_pInt,homogenization_Ngrains(mesh_element(3,e))]
enddo
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fixed out of range bug introduced with singleRun changes in rev. 2356
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singleRun = (eIter(1) == eIter(2) .and. iIter(1,eIter(1)) == iIter(2,eIter(2)))
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!$OMP PARALLEL
if (numerics_integrationMode == 1_pInt) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- DOT STATE ---
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
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enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p/=constitutive_dotState(g,i,e)%p) ) then ! NaN occured in dotState
if (.not. crystallite_localPlasticity(g,i,e) .and. .not. numerics_timeSyncing) then ! if broken non-local...
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!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
else ! if broken local...
crystallite_todo(g,i,e) = .false. ! ... skip this one next time
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- UPDATE STATE ---
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!$OMP DO PRIVATE(mySizeDotState)
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_state(g,i,e)%p(1:mySizeDotState) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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+ constitutive_dotState(g,i,e)%p(1:mySizeDotState) &
* crystallite_subdt(g,i,e)
deleted space in front of preprocessor line
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#ifndef _OPENMP
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
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write(6,'(a,i8,1x,i2,1x,i3,/)') '<< CRYST >> update state at el ip g ',e,i,g
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> dotState', constitutive_dotState(g,i,e)%p(1:mySizeDotState)
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> new state', constitutive_state(g,i,e)%p(1:mySizeDotState)
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endif
deleted space in front of preprocessor line
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#endif
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endif
enddo; enddo; enddo
!$OMP ENDDO
! --- STATE JUMP ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e) & ! if broken non-local...
.and. .not. numerics_timeSyncing) then
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- UPDATE DEPENDENT STATES ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
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crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
order of integration now same for all state integrators: first calculate the dotState and then the deltaState
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enddo; enddo; enddo
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!$OMP ENDDO
endif
! --- STRESS INTEGRATION ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e) & ! if broken non-local...
.and. .not. numerics_timeSyncing) then
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
Depending on which state integrator one uses for the stiffness calculation, the initial state has to be chosen accordingly: e.g. for FPI choose last converged state, but for explicit RK choose converged state from start of increment (in case of explicit euler no state integration at all, but only stress integration). For this purpose we also need to remember "Fe" which now follows the cutbacking procedure as it is used for "Fp".
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enddo; enddo; enddo
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!$OMP ENDDO
! --- SET CONVERGENCE FLAG ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
crystallite_converged(g,i,e) = .true. ! if still "to do" then converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(1,numerics_integrationMode) = &
debug_StateLoopDistribution(1,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
! --- CHECK NON-LOCAL CONVERGENCE ---
if (.not. singleRun) then ! if not requesting Integration of just a single IP
if (any(.not. crystallite_converged .and. .not. crystallite_localPlasticity) & ! any non-local not yet converged (or broken)...
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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.and. .not. numerics_timeSyncing) &
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crystallite_converged = crystallite_converged .and. crystallite_localPlasticity ! ...restart all non-local as not converged
endif
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
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end subroutine crystallite_integrateStateEuler
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
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!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!> @brief integrate stress, state with adaptive 1st order explicit Euler method
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!> using Fixed Point Iteration to adapt the stepsize
!--------------------------------------------------------------------------------------------------
simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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subroutine crystallite_integrateStateFPI()
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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use debug, only: &
debug_e, &
debug_i, &
debug_g, &
debug_level,&
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_StateLoopDistribution
use numerics, only: &
nState, &
numerics_integrationMode, &
rTol_crystalliteState
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems
use material, only: &
homogenization_Ngrains
use constitutive, only: &
constitutive_subState0, &
constitutive_state, &
constitutive_sizeDotState, &
constitutive_maxSizeDotState, &
constitutive_dotState, &
constitutive_collectDotState, &
constitutive_microstructure, &
constitutive_previousDotState, &
constitutive_previousDotState2, &
constitutive_aTolState
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implicit none
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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integer(pInt) :: &
NiterationState, & !< number of iterations in state loop
e, & !< element index in element loop
i, & !< integration point index in ip loop
g, & !< grain index in grain loop
mySizeDotState
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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integer(pInt), dimension(2) :: &
eIter ! bounds for element iteration
integer(pInt), dimension(2,mesh_NcpElems) :: &
iIter, & ! bounds for ip iteration
gIter ! bounds for grain iteration
real(pReal) :: &
dot_prod12, &
dot_prod22, &
stateDamper ! damper for integration of state
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real(pReal), dimension(constitutive_maxSizeDotState) :: &
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stateResiduum, &
tempState
logical :: &
singleRun ! flag indicating computation for single (g,i,e) triple
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simplified logic for single run, now not checking for extra arguments but simply checking if start and end elem/IP are the same
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eIter = FEsolving_execElem(1:2)
do e = eIter(1),eIter(2)
iIter(1:2,e) = FEsolving_execIP(1:2,e)
gIter(1:2,e) = [ 1_pInt,homogenization_Ngrains(mesh_element(3,e))]
enddo
fixed out of range bug introduced with singleRun changes in rev. 2356
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singleRun = (eIter(1) == eIter(2) .and. iIter(1,eIter(1)) == iIter(2,eIter(2)))
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! --+>> PREGUESS FOR STATE <<+--
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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! --- DOT STATES ---
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in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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!$OMP PARALLEL
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!$OMP DO
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
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constitutive_previousDotState(g,i,e)%p = 0.0_pReal
constitutive_previousDotState2(g,i,e)%p = 0.0_pReal
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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if (crystallite_todo(g,i,e)) then
call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
endif
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enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p/=constitutive_dotState(g,i,e)%p) ) then ! NaN occured in dotState
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if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken is a non-local...
!$OMP CRITICAL (checkTodo)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals done (and broken)
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!$OMP END CRITICAL (checkTodo)
else ! broken one was local...
crystallite_todo(g,i,e) = .false. ! ... done (and broken)
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- UPDATE STATE ---
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!$OMP DO PRIVATE(mySizeDotState)
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
if (crystallite_todo(g,i,e)) then
mySizeDotState = constitutive_sizeDotState(g,i,e)
constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_subState0(g,i,e)%p(1:mySizeDotState) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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+ constitutive_dotState(g,i,e)%p &
* crystallite_subdt(g,i,e)
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endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
! --+>> STATE LOOP <<+--
NiterationState = 0_pInt
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
crystalliteLooping: do while (any(crystallite_todo .and. .not. crystallite_converged) &
.and. NiterationState < nState)
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NiterationState = NiterationState + 1_pInt
!$OMP PARALLEL
! --- UPDATE DEPENDENT STATES ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_microstructure(crystallite_temperature(i,e), crystallite_Fe(1:3,1:3,g,i,e), &
doxygen comments
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crystallite_Fp(1:3,1:3,g,i,e), g, i, e) ! update dependent state variables to be consistent with basic states
constitutive_previousDotState2(g,i,e)%p = constitutive_previousDotState(g,i,e)%p ! remember previous dotState
constitutive_previousDotState(g,i,e)%p = constitutive_dotState(g,i,e)%p ! remember current dotState
enddo; enddo; enddo
!$OMP ENDDO
! --- STRESS INTEGRATION ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
crystallite_todo(g,i,e) = crystallite_integrateStress(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e) .and. .not. crystallite_localPlasticity(g,i,e)) then ! broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ... then all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP SINGLE
!$OMP CRITICAL (write2out)
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) &
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write(6,'(a,i8,a)') '<< CRYST >> ', count(crystallite_todo(:,:,:)),' grains todo after stress integration'
!$OMP END CRITICAL (write2out)
!$OMP END SINGLE
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- DOT STATE ---
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!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
call constitutive_collectDotState(crystallite_Tstar_v(1:6,g,i,e), crystallite_Fe, &
crystallite_Fp, crystallite_temperature(i,e), &
crystallite_subdt(g,i,e), crystallite_subFrac, g,i,e)
doxygen comments
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enddo; enddo; enddo
!$OMP ENDDO
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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if ( any(constitutive_dotState(g,i,e)%p/=constitutive_dotState(g,i,e)%p) ) then ! NaN occured in dotState
doxygen comments
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crystallite_todo(g,i,e) = .false. ! ... skip me next time
if (.not. crystallite_localPlasticity(g,i,e)) then ! if me is non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- UPDATE STATE ---
doxygen comments
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removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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!$OMP DO PRIVATE(dot_prod12,dot_prod22,statedamper,mySizeDotState,stateResiduum,tempState)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
doxygen comments
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if (crystallite_todo(g,i,e) .and. .not. crystallite_converged(g,i,e)) then
! --- state damper ---
dot_prod12 = dot_product( constitutive_dotState(g,i,e)%p - constitutive_previousDotState(g,i,e)%p, &
constitutive_previousDotState(g,i,e)%p - constitutive_previousDotState2(g,i,e)%p )
dot_prod22 = dot_product( constitutive_previousDotState(g,i,e)%p - constitutive_previousDotState2(g,i,e)%p, &
constitutive_previousDotState(g,i,e)%p - constitutive_previousDotState2(g,i,e)%p )
if ( dot_prod22 > 0.0_pReal &
.and. ( dot_prod12 < 0.0_pReal &
.or. dot_product(constitutive_dotState(g,i,e)%p, constitutive_previousDotState(g,i,e)%p) < 0.0_pReal) ) then
statedamper = 0.75_pReal + 0.25_pReal * tanh(2.0_pReal + 4.0_pReal * dot_prod12 / dot_prod22)
else
statedamper = 1.0_pReal
endif
! --- get residui ---
mySizeDotState = constitutive_sizeDotState(g,i,e)
stateResiduum(1:mySizeDotState) = constitutive_state(g,i,e)%p(1:mySizeDotState) &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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- constitutive_subState0(g,i,e)%p(1:mySizeDotState) &
- (constitutive_dotState(g,i,e)%p * statedamper &
+ constitutive_previousDotState(g,i,e)%p &
* (1.0_pReal - statedamper)) * crystallite_subdt(g,i,e)
doxygen comments
2013-02-22 04:38:36 +05:30
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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! --- correct state with residuum ---
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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tempState(1:mySizeDotState) = constitutive_state(g,i,e)%p(1:mySizeDotState) &
- stateResiduum(1:mySizeDotState) ! need to copy to local variable, since we cant flush a pointer in openmp
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
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#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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write(6,'(a,i8,1x,i2,1x,i3,/)') '<< CRYST >> update state at el ip g ',e,i,g
write(6,'(a,f6.1,/)') '<< CRYST >> statedamper ',statedamper
fixed some e12.6 string formats to avoid compile time warnings
2013-10-08 19:21:36 +05:30
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> state residuum',stateResiduum(1:mySizeDotState)
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> new state',tempState(1:mySizeDotState)
doxygen comments
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endif
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
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#endif
doxygen comments
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! --- store corrected dotState --- (cannot do this before state update, because not sure how to flush pointers in openmp)
constitutive_dotState(g,i,e)%p = constitutive_dotState(g,i,e)%p * statedamper &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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+ constitutive_previousDotState(g,i,e)%p &
* (1.0_pReal - statedamper)
doxygen comments
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! --- converged ? ---
if ( all( abs(stateResiduum(1:mySizeDotState)) < constitutive_aTolState(g,i,e)%p(1:mySizeDotState) &
.or. abs(stateResiduum(1:mySizeDotState)) < rTol_crystalliteState &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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* abs(tempState(1:mySizeDotState)) ) ) then
doxygen comments
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crystallite_converged(g,i,e) = .true. ! ... converged per definitionem
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionState)
debug_StateLoopDistribution(NiterationState,numerics_integrationMode) = &
debug_StateLoopDistribution(NiterationState,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionState)
endif
endif
constitutive_state(g,i,e)%p(1:mySizeDotState) = tempState(1:mySizeDotState) ! copy local backup to global pointer
endif
enddo; enddo; enddo
!$OMP ENDDO
! --- STATE JUMP ---
!$OMP DO
do e = eIter(1),eIter(2); do i = iIter(1,e),iIter(2,e); do g = gIter(1,e),gIter(2,e) ! iterate over elements, ips and grains
!$OMP FLUSH(crystallite_todo)
if (crystallite_todo(g,i,e) .and. crystallite_converged(g,i,e)) then ! converged and still alive...
crystallite_todo(g,i,e) = crystallite_stateJump(g,i,e)
!$OMP FLUSH(crystallite_todo)
if (.not. crystallite_todo(g,i,e)) then ! if state jump fails, then convergence is broken
crystallite_converged(g,i,e) = .false.
if (.not. crystallite_localPlasticity(g,i,e)) then ! if broken non-local...
!$OMP CRITICAL (checkTodo)
crystallite_todo = crystallite_todo .and. crystallite_localPlasticity ! ...all non-locals skipped
!$OMP END CRITICAL (checkTodo)
endif
endif
endif
enddo; enddo; enddo
!$OMP ENDDO
!$OMP END PARALLEL
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL(write2out)
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
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write(6,'(a,i8,a,i2,/)') '<< CRYST >> ', count(crystallite_converged(:,:,:)), &
doxygen comments
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' grains converged after state integration no. ', NiterationState
!$OMP END CRITICAL(write2out)
endif
! --- NON-LOCAL CONVERGENCE CHECK ---
if (.not. singleRun) then ! if not requesting Integration of just a single IP
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
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if (any(.not. crystallite_converged .and. .not. crystallite_localPlasticity)) & ! any non-local not yet converged (or broken)...
doxygen comments
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crystallite_converged = crystallite_converged .and. crystallite_localPlasticity ! ...restart all non-local as not converged
endif
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt) then
!$OMP CRITICAL(write2out)
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
write(6,'(a,i8,a)') '<< CRYST >> ', count(crystallite_converged(:,:,:)), &
' grains converged after non-local check'
write(6,'(a,i8,a,i2,/)') '<< CRYST >> ', count(crystallite_todo(:,:,:)), &
' grains todo after state integration no. ', NiterationState
doxygen comments
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!$OMP END CRITICAL(write2out)
endif
introduced plain mode (no ping pong) again and added test for MSC.MArc 2012 as prove that its working
2013-05-17 23:22:46 +05:30
enddo crystalliteLooping
doxygen comments
2013-02-22 04:38:36 +05:30
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end subroutine crystallite_integrateStateFPI
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp" * now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation * non-local stuff: * changed non-local kinetics (Gilman2002) * enforce zero shearrate for overall carrrier density below relevant density * enforce zero density for those states that become negative and were below relevant density before * dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 17:48:49 +05:30
doxygen comments
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!--------------------------------------------------------------------------------------------------
!> @brief calculates a jump in the state according to the current state and the current stress
!--------------------------------------------------------------------------------------------------
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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logical function crystallite_stateJump(g,i,e)
use debug, only: &
debug_level, &
debug_crystallite, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use mesh, only: &
mesh_element, &
mesh_NcpElems
use material, only: &
homogenization_Ngrains
use constitutive, only: &
constitutive_sizeDotState, &
constitutive_state, &
constitutive_deltaState, &
constitutive_collectDeltaState, &
constitutive_microstructure
doxygen comments
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implicit none
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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integer(pInt), intent(in):: &
e, & ! element index
i, & ! integration point index
g ! grain index
integer(pInt) :: &
mySizeDotState
doxygen comments
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crystallite_stateJump = .false.
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
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call constitutive_collectDeltaState(crystallite_Tstar_v(1:6,g,i,e), g,i,e)
doxygen comments
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mySizeDotState = constitutive_sizeDotState(g,i,e)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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if (any(constitutive_deltaState(g,i,e)%p(1:mySizeDotState) &
/= constitutive_deltaState(g,i,e)%p(1:mySizeDotState))) then
doxygen comments
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return
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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endif
doxygen comments
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constitutive_state(g,i,e)%p(1:mySizeDotState) = constitutive_state(g,i,e)%p(1:mySizeDotState) &
+ constitutive_deltaState(g,i,e)%p(1:mySizeDotState)
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
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#ifndef _OPENMP
doxygen comments
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if (any(constitutive_deltaState(g,i,e)%p(1:mySizeDotState) /= 0.0_pReal) &
.and. iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
write(6,'(a,i8,1x,i2,1x,i3, /)') '<< CRYST >> update state at el ip g ',e,i,g
fixed some e12.6 string formats to avoid compile time warnings
2013-10-08 19:21:36 +05:30
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> deltaState', constitutive_deltaState(g,i,e)%p(1:mySizeDotState)
write(6,'(a,/,(12x,12(e12.5,1x)),/)') '<< CRYST >> new state', constitutive_state(g,i,e)%p(1:mySizeDotState)
doxygen comments
2013-02-22 04:38:36 +05:30
endif
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
2012-06-06 20:41:30 +05:30
#endif
doxygen comments
2013-02-22 04:38:36 +05:30
crystallite_stateJump = .true.
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
2012-06-06 20:41:30 +05:30
end function crystallite_stateJump
doxygen comments
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!--------------------------------------------------------------------------------------------------
!> @brief calculation of stress (P) with time integration based on a residuum in Lp and
!> intermediate acceleration of the Newton-Raphson correction
!--------------------------------------------------------------------------------------------------
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
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logical function crystallite_integrateStress(&
doxygen comments
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g,& ! grain number
i,& ! integration point number
e,& ! element number
timeFraction &
)
use prec, only: pLongInt
use numerics, only: nStress, &
aTol_crystalliteStress, &
rTol_crystalliteStress, &
iJacoLpresiduum, &
numerics_integrationMode
use debug, only: debug_level, &
debug_crystallite, &
debug_levelBasic, &
debug_levelExtensive, &
debug_levelSelective, &
debug_e, &
debug_i, &
debug_g, &
debug_cumLpCalls, &
debug_cumLpTicks, &
debug_StressLoopDistribution
use constitutive, only: constitutive_LpAndItsTangent, &
remnoved some unused fuctions from use statements
2013-08-02 11:48:41 +05:30
constitutive_TandItsTangent
doxygen comments
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use math, only: math_mul33x33, &
math_mul33xx33, &
math_mul66x6, &
math_mul99x99, &
math_transpose33, &
math_inv33, &
math_invert33, &
math_invert, &
math_det33, &
math_norm33, &
math_I3, &
math_identity2nd, &
math_Mandel66to3333, &
math_Mandel6to33, &
math_Mandel33to6, &
math_Plain3333to99, &
math_Plain33to9, &
math_Plain9to33
implicit none
integer(pInt), intent(in):: e, & ! element index
i, & ! integration point index
g ! grain index
real(pReal), optional, intent(in) :: timeFraction ! fraction of timestep
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
doxygen comments
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!*** local variables ***!
real(pReal), dimension(3,3):: Fg_new, & ! deformation gradient at end of timestep
Fp_current, & ! plastic deformation gradient at start of timestep
Fp_new, & ! plastic deformation gradient at end of timestep
Fe_new, & ! elastic deformation gradient at end of timestep
invFp_new, & ! inverse of Fp_new
invFp_current, & ! inverse of Fp_current
Lpguess, & ! current guess for plastic velocity gradient
Lpguess_old, & ! known last good guess for plastic velocity gradient
Lp_constitutive, & ! plastic velocity gradient resulting from constitutive law
residuum, & ! current residuum of plastic velocity gradient
residuum_old, & ! last residuum of plastic velocity gradient
deltaLp, & ! direction of next guess
Tstar,& ! 2nd Piola-Kirchhoff Stress
A,&
B, &
Fe ! elastic deformation gradient
real(pReal), dimension(6):: Tstar_v ! 2nd Piola-Kirchhoff Stress in Mandel-Notation
real(pReal), dimension(9):: work ! needed for matrix inversion by LAPACK
integer(pInt), dimension(9) :: ipiv ! needed for matrix inversion by LAPACK
real(pReal), dimension(9,9) :: dLp_dT_constitutive, & ! partial derivative of plastic velocity gradient calculated by constitutive law
dT_dFe_constitutive, & ! partial derivative of 2nd Piola-Kirchhoff stress calculated by constitutive law
dFe_dLp, & ! partial derivative of elastic deformation gradient
dR_dLp, & ! partial derivative of residuum (Jacobian for NEwton-Raphson scheme)
dR_dLp2 ! working copy of dRdLp
real(pReal), dimension(3,3,3,3):: dT_dFe3333, & ! partial derivative of 2nd Piola-Kirchhoff stress
dFe_dLp3333 ! partial derivative of elastic deformation gradient
real(pReal) p_hydro, & ! volumetric part of 2nd Piola-Kirchhoff Stress
det, & ! determinant
steplength0, &
steplength, &
dt, & ! time increment
aTol
logical error ! flag indicating an error
integer(pInt) NiterationStress, & ! number of stress integrations
ierr, & ! error indicator for LAPACK
n, &
o, &
p, &
jacoCounter ! counter to check for Jacobian update
integer(pLongInt) tick, &
tock, &
tickrate, &
maxticks
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
made doxygen working for MSC.Marc again, small changes on the todo-statements for doxygen, they don't work on single lines of codes but only on module/variables
2013-06-11 22:05:04 +05:30
external :: &
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
#if(FLOAT==8)
made doxygen working for MSC.Marc again, small changes on the todo-statements for doxygen, they don't work on single lines of codes but only on module/variables
2013-06-11 22:05:04 +05:30
dgesv
#elif(FLOAT==4)
sgesv
#endif
doxygen comments
2013-02-22 04:38:36 +05:30
!* be pessimistic
crystallite_integrateStress = .false.
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> integrateStress at el ip g ',e,i,g
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!* only integrate over fraction of timestep?
if (present(timeFraction)) then
dt = crystallite_subdt(g,i,e) * timeFraction
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
Fg_new = crystallite_subF0(1:3,1:3,g,i,e) &
+ (crystallite_subF(1:3,1:3,g,i,e) - crystallite_subF0(1:3,1:3,g,i,e)) * timeFraction
doxygen comments
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else
dt = crystallite_subdt(g,i,e)
Fg_new = crystallite_subF(1:3,1:3,g,i,e)
endif
!* feed local variables
Fp_current = crystallite_subFp0(1:3,1:3,g,i,e) ! "Fp_current" is only used as temp var here...
Lpguess_old = crystallite_Lp(1:3,1:3,g,i,e) ! consider present Lp good (i.e. worth remembering) ...
Lpguess = crystallite_Lp(1:3,1:3,g,i,e) ! ... and take it as first guess
!* inversion of Fp_current...
invFp_current = math_inv33(Fp_current)
if (all(invFp_current == 0.0_pReal)) then ! ... failed?
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
write(6,'(a,i8,1x,i2,1x,i3)') '<< CRYST >> integrateStress failed on inversion of Fp_current at el ip g ',e,i,g
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
if (iand(debug_level(debug_crystallite), debug_levelExtensive) > 0_pInt) &
write(6,'(/,a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> Fp_current',math_transpose33(Fp_current(1:3,1:3))
doxygen comments
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endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#endif
doxygen comments
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return
endif
A = math_mul33x33(Fg_new,invFp_current) ! intermediate tensor needed later to calculate dFe_dLp
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
doxygen comments
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!* start LpLoop with normal step length
NiterationStress = 0_pInt
jacoCounter = 0_pInt
steplength0 = 1.0_pReal
steplength = steplength0
residuum_old = 0.0_pReal
LpLoop: do
NiterationStress = NiterationStress + 1_pInt
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
loopsExeced: if (NiterationStress > nStress) then
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) &
write(6,'(a,i3,a,i8,1x,i2,1x,i3,/)') '<< CRYST >> integrateStress reached loop limit',nStress,' at el ip g ',e,i,g
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
doxygen comments
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return
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
endif loopsExeced
doxygen comments
2013-02-22 04:38:36 +05:30
!* calculate (elastic) 2nd Piola--Kirchhoff stress tensor and its tangent from constitutive law
B = math_I3 - dt*Lpguess
Fe = math_mul33x33(A,B) ! current elastic deformation tensor
call constitutive_TandItsTangent(Tstar, dT_dFe3333, Fe, g,i,e) ! call constitutive law to calculate 2nd Piola-Kirchhoff stress and its derivative
Tstar_v = math_Mandel33to6(Tstar)
p_hydro = sum(Tstar_v(1:3)) / 3.0_pReal
forall(n=1_pInt:3_pInt) Tstar_v(n) = Tstar_v(n) - p_hydro ! get deviatoric stress tensor
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!* calculate plastic velocity gradient and its tangent from constitutive law
* enclose wall time measurement for LpAndItsTangent and count of leapfrogbreaks by CRITICAL construct * better use SINGLE (having an implicit barrier at the end) instead of MASTER construct * deleted all explicit BARRIERs after do loops since parallel loop construct implies barrier at the end
2010-11-19 22:59:29 +05:30
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
doxygen comments
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call system_clock(count=tick,count_rate=tickrate,count_max=maxticks)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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endif
doxygen comments
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in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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call constitutive_LpAndItsTangent(Lp_constitutive, dLp_dT_constitutive, Tstar_v, &
crystallite_temperature(i,e), g, i, e)
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
call system_clock(count=tock,count_rate=tickrate,count_max=maxticks)
!$OMP CRITICAL (debugTimingLpTangent)
debug_cumLpCalls = debug_cumLpCalls + 1_pInt
debug_cumLpTicks = debug_cumLpTicks + tock-tick
!$OMP FLUSH (debug_cumLpTicks)
if (tock < tick) debug_cumLpTicks = debug_cumLpTicks + maxticks
!$OMP END CRITICAL (debugTimingLpTangent)
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
write(6,'(a,i3,/)') '<< CRYST >> iteration ', NiterationStress
doxygen comments
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write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> Lp_constitutive', math_transpose33(Lp_constitutive)
write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> Lpguess', math_transpose33(Lpguess)
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
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#endif
doxygen comments
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!* update current residuum and check for convergence of loop
aTol = max(rTol_crystalliteStress * max(math_norm33(Lpguess),math_norm33(Lp_constitutive)), & ! absolute tolerance from largest acceptable relative error
aTol_crystalliteStress) ! minimum lower cutoff
residuum = Lpguess - Lp_constitutive
if (any(residuum /= residuum)) then ! NaN in residuum...
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) &
doxygen comments
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write(6,'(a,i8,1x,i2,1x,i3,a,i3,a)') '<< CRYST >> integrateStress encountered NaN at el ip g ',e,i,g,&
' ; iteration ', NiterationStress,&
' >> returning..!'
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
doxygen comments
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return ! ...me = .false. to inform integrator about problem
elseif (math_norm33(residuum) < aTol) then ! converged if below absolute tolerance
exit LpLoop ! ...leave iteration loop
elseif (math_norm33(residuum) < math_norm33(residuum_old) .or. NiterationStress == 1_pInt ) then ! not converged, but improved norm of residuum (always proceed in first iteration)...
residuum_old = residuum ! ...remember old values and...
Lpguess_old = Lpguess
steplength = steplength0 ! ...proceed with normal step length (calculate new search direction)
else ! not converged and residuum not improved...
steplength = 0.5_pReal * steplength ! ...try with smaller step length in same direction
Lpguess = Lpguess_old + steplength * deltaLp
cycle LpLoop
endif
!* calculate Jacobian for correction term
if (mod(jacoCounter, iJacoLpresiduum) == 0_pInt) then
dFe_dLp3333 = 0.0_pReal
do o=1_pInt,3_pInt; do p=1_pInt,3_pInt
dFe_dLp3333(p,o,1:3,p) = A(o,1:3) ! dFe_dLp(i,j,k,l) = -dt * A(i,k) delta(j,l)
enddo; enddo
dFe_dLp3333 = -dt * dFe_dLp3333
dFe_dLp = math_Plain3333to99(dFe_dLp3333)
dT_dFe_constitutive = math_Plain3333to99(dT_dFe3333)
dR_dLp = math_identity2nd(9_pInt) - &
math_mul99x99(dLp_dT_constitutive, math_mul99x99(dT_dFe_constitutive , dFe_dLp))
dR_dLp2 = dR_dLp ! will be overwritten in first call to LAPACK routine
work = math_plain33to9(residuum)
substituted hand written matrix inversion by LAPACK version with precision selection. also introduced check for inversion into DAMASK_spectral_Utilities.f90 for the stress BC calculation. This part is further improved by using 5% of the reference stiffness to avoid trouble in the fully plastic regime (where the stiffness is underestimated) Test for Marc 2010 is updated because the new inversion give slightly different results near 0 (order of e-13)
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#if(FLOAT==8)
doxygen comments
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call dgesv(9,1,dR_dLp2,9,ipiv,work,9,ierr) ! solve dR/dLp * delta Lp = -res for dR/dLp
substituted hand written matrix inversion by LAPACK version with precision selection. also introduced check for inversion into DAMASK_spectral_Utilities.f90 for the stress BC calculation. This part is further improved by using 5% of the reference stiffness to avoid trouble in the fully plastic regime (where the stiffness is underestimated) Test for Marc 2010 is updated because the new inversion give slightly different results near 0 (order of e-13)
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#elif(FLOAT==4)
doxygen comments
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call sgesv(9,1,dR_dLp2,9,ipiv,work,9,ierr) ! solve dR/dLp * delta Lp = -res for dR/dLp
substituted hand written matrix inversion by LAPACK version with precision selection. also introduced check for inversion into DAMASK_spectral_Utilities.f90 for the stress BC calculation. This part is further improved by using 5% of the reference stiffness to avoid trouble in the fully plastic regime (where the stiffness is underestimated) Test for Marc 2010 is updated because the new inversion give slightly different results near 0 (order of e-13)
2012-08-28 22:29:45 +05:30
#endif
doxygen comments
2013-02-22 04:38:36 +05:30
if (ierr /= 0_pInt) then
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
write(6,'(a,i8,1x,i2,1x,i3,a,i3)') '<< CRYST >> integrateStress failed on dR/dLp inversion at el ip g ',e,i,g
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g)&
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
write(6,*)
write(6,'(a,/,9(12x,9(e15.3,1x)/))') '<< CRYST >> dR_dLp',transpose(dR_dLp)
write(6,'(a,/,9(12x,9(e15.3,1x)/))') '<< CRYST >> dFe_dLp',transpose(dFe_dLp)
write(6,'(a,/,9(12x,9(e15.3,1x)/))') '<< CRYST >> dT_dFe_constitutive',transpose(dT_dFe_constitutive)
write(6,'(a,/,9(12x,9(e15.3,1x)/))') '<< CRYST >> dLp_dT_constitutive',transpose(dLp_dT_constitutive)
write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> A',math_transpose33(A)
write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> B',math_transpose33(B)
write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> Lp_constitutive',math_transpose33(Lp_constitutive)
write(6,'(a,/,3(12x,3(e20.7,1x)/))') '<< CRYST >> Lpguess',math_transpose33(Lpguess)
endif
endif
Stress integration now uses Armijo rule to find an appropriate correction of Lp: decreases step in case that residuum does not improve significantly, accelerates as usual in case of good convergence. This turned out to improve convergence behavior.
2011-08-02 16:59:08 +05:30
#endif
doxygen comments
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return
endif
deltaLp = - math_plain9to33(work)
endif
jacoCounter = jacoCounter + 1_pInt ! increase counter for jaco update
Lpguess = Lpguess + steplength * deltaLp
enddo LpLoop
!* calculate new plastic and elastic deformation gradient
invFp_new = math_mul33x33(invFp_current,B)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
invFp_new = invFp_new / math_det33(invFp_new)**(1.0_pReal/3.0_pReal) ! regularize by det
doxygen comments
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call math_invert33(invFp_new,Fp_new,det,error)
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
if (error .or. any(Fp_new /= Fp_new)) then
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
write(6,'(a,i8,1x,i2,1x,i3,a,i3)') '<< CRYST >> integrateStress failed on invFp_new inversion at el ip g ',&
e,i,g, ' ; iteration ', NiterationStress
if (iand(debug_level(debug_crystallite), debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) &
write(6,'(/,a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> invFp_new',math_transpose33(invFp_new)
doxygen comments
2013-02-22 04:38:36 +05:30
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
doxygen comments
2013-02-22 04:38:36 +05:30
return
endif
Fe_new = math_mul33x33(Fg_new,invFp_new) ! calc resulting Fe
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!* add volumetric component to 2nd Piola-Kirchhoff stress and calculate 1st Piola-Kirchhoff stress
forall (n=1_pInt:3_pInt) Tstar_v(n) = Tstar_v(n) + p_hydro
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_P(1:3,1:3,g,i,e) = math_mul33x33(Fe_new, math_mul33x33(math_Mandel6to33(Tstar_v), &
math_transpose33(invFp_new)))
doxygen comments
2013-02-22 04:38:36 +05:30
!* store local values in global variables
crystallite_Lp(1:3,1:3,g,i,e) = Lpguess
crystallite_Tstar_v(1:6,g,i,e) = Tstar_v
crystallite_Fp(1:3,1:3,g,i,e) = Fp_new
crystallite_Fe(1:3,1:3,g,i,e) = Fe_new
crystallite_invFp(1:3,1:3,g,i,e) = invFp_new
!* set return flag to true
crystallite_integrateStress = .true.
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#ifndef _OPENMP
doxygen comments
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if (iand(debug_level(debug_crystallite),debug_levelExtensive) /= 0_pInt &
.and. ((e == debug_e .and. i == debug_i .and. g == debug_g) &
.or. .not. iand(debug_level(debug_crystallite), debug_levelSelective) /= 0_pInt)) then
write(6,'(a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> P / MPa',math_transpose33(crystallite_P(1:3,1:3,g,i,e))/1.0e6_pReal
write(6,'(a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> Cauchy / MPa', &
math_mul33x33(crystallite_P(1:3,1:3,g,i,e), math_transpose33(Fg_new)) / 1.0e6_pReal / math_det33(Fg_new)
write(6,'(a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> Fe Lp Fe^-1', &
math_transpose33(math_mul33x33(Fe_new, math_mul33x33(crystallite_Lp(1:3,1:3,g,i,e), math_inv33(Fe_new)))) ! transpose to get correct print out order
write(6,'(a,/,3(12x,3(f12.7,1x)/))') '<< CRYST >> Fp',math_transpose33(crystallite_Fp(1:3,1:3,g,i,e))
endif
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization. * Also added some more openmp directives to increase percentage of parallelized code. * "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 12:57:19 +05:30
#endif
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
if (iand(debug_level(debug_crystallite), debug_levelBasic) /= 0_pInt) then
!$OMP CRITICAL (distributionStress)
debug_StressLoopDistribution(NiterationStress,numerics_integrationMode) = &
debug_StressLoopDistribution(NiterationStress,numerics_integrationMode) + 1_pInt
!$OMP END CRITICAL (distributionStress)
endif
end function crystallite_integrateStress
restructured stress integration. Double loop for stress integration (Lp and stress) with cutback step in IntegrateStress is replaced by single loop for Lp without cutback. loop counter and limits are accordingly renamed and implemented
2009-05-28 22:08:40 +05:30
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
!--------------------------------------------------------------------------------------------------
!> @brief calculates orientations and disorientations (in case of single grain ips)
!--------------------------------------------------------------------------------------------------
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
subroutine crystallite_orientations
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
use math, only: &
math_pDecomposition, &
math_RtoQ, &
math_qDisorientation, &
math_qConj
use FEsolving, only: &
FEsolving_execElem, &
FEsolving_execIP
use IO, only: &
IO_warning
use material, only: &
material_phase, &
homogenization_Ngrains, &
phase_localPlasticity, &
phase_plasticityInstance
use mesh, only: &
mesh_element, &
mesh_ipNeighborhood, &
FE_NipNeighbors, &
FE_geomtype, &
FE_celltype
use constitutive_nonlocal, only: &
constitutive_nonlocal_structure, &
constitutive_nonlocal_updateCompatibility
doxygen comments
2013-02-22 04:38:36 +05:30
implicit none
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
integer(pInt) &
e, & ! element index
i, & ! integration point index
g, & ! grain index
n, & ! neighbor index
neighboring_e, & ! element index of my neighbor
neighboring_i, & ! integration point index of my neighbor
myPhase, & ! phase
neighboringPhase, &
myInstance, & ! instance of plasticity
neighboringInstance, &
myStructure, & ! lattice structure
neighboringStructure
real(pReal), dimension(3,3) :: &
U, &
R
real(pReal), dimension(4) :: &
orientation
logical &
error
doxygen comments
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! --- CALCULATE ORIENTATION AND LATTICE ROTATION ---
!$OMP PARALLEL DO PRIVATE(error,U,R,orientation)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
do g = 1_pInt,homogenization_Ngrains(mesh_element(3,e))
added shortcuts for two do loops in the "timesyncing" procedure math_pDecomposition enclosed by omp critical statement; somehow, this subroutine is not thread safe, not clear what exactly the problem is
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!$OMP CRITICAL (polarDecomp) ! somehow this subroutine is not threadsafe, so need critical statement here; not clear, what exactly the problem is
call math_pDecomposition(crystallite_Fe(1:3,1:3,g,i,e), U, R, error) ! polar decomposition of Fe
!$OMP END CRITICAL (polarDecomp)
doxygen comments
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if (error) then
call IO_warning(650_pInt, e, i, g)
added shortcuts for two do loops in the "timesyncing" procedure math_pDecomposition enclosed by omp critical statement; somehow, this subroutine is not thread safe, not clear what exactly the problem is
2013-02-27 16:02:37 +05:30
orientation = [1.0_pReal, 0.0_pReal, 0.0_pReal, 0.0_pReal] ! fake orientation
doxygen comments
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else
orientation = math_RtoQ(transpose(R))
endif
crystallite_rotation(1:4,g,i,e) = math_qDisorientation(crystallite_orientation0(1:4,g,i,e), & ! active rotation from ori0
added shortcuts for two do loops in the "timesyncing" procedure math_pDecomposition enclosed by omp critical statement; somehow, this subroutine is not thread safe, not clear what exactly the problem is
2013-02-27 16:02:37 +05:30
orientation, & ! to current orientation
0_pInt ) ! we don't want symmetry here
doxygen comments
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crystallite_orientation(1:4,g,i,e) = orientation
enddo
enddo
enddo
!$OMP END PARALLEL DO
! --- UPDATE SOME ADDITIONAL VARIABLES THAT ARE NEEDED FOR NONLOCAL MATERIAL ---
! --- we use crystallite_orientation from above, so need a seperate loop
!$OMP PARALLEL DO PRIVATE(myPhase,myInstance,myStructure,neighboring_e,neighboring_i,neighboringPhase,&
!$OMP neighboringInstance,neighboringStructure)
do e = FEsolving_execElem(1),FEsolving_execElem(2)
do i = FEsolving_execIP(1,e),FEsolving_execIP(2,e)
myPhase = material_phase(1,i,e) ! get my phase
if (.not. phase_localPlasticity(myPhase)) then ! if nonlocal model
myInstance = phase_plasticityInstance(myPhase)
myStructure = constitutive_nonlocal_structure(myInstance) ! get my crystal structure
! --- calculate disorientation between me and my neighbor ---
neighborhood relations were screwed up for some elementtypes as of version 2318, might have caused segmentation faults with nonlocal model, now fixed
2013-04-22 19:05:35 +05:30
do n = 1_pInt,FE_NipNeighbors(FE_celltype(FE_geomtype(mesh_element(2,e)))) ! loop through my neighbors
doxygen comments
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neighboring_e = mesh_ipNeighborhood(1,n,i,e)
neighboring_i = mesh_ipNeighborhood(2,n,i,e)
if ((neighboring_e > 0) .and. (neighboring_i > 0)) then ! if neighbor exists
neighboringPhase = material_phase(1,neighboring_i,neighboring_e) ! get my neighbor's phase
if (.not. phase_localPlasticity(neighboringPhase)) then ! neighbor got also nonlocal plasticity
neighboringInstance = phase_plasticityInstance(neighboringPhase)
neighboringStructure = constitutive_nonlocal_structure(neighboringInstance) ! get my neighbor's crystal structure
if (myStructure == neighboringStructure) then ! if my neighbor has same crystal structure like me
crystallite_disorientation(:,n,1,i,e) = &
named some loops and made BUTCHER TABLEAUs parameters in crystallite_integrateStateRKCK45
2013-04-29 16:47:30 +05:30
math_qDisorientation( crystallite_orientation(1:4,1,i,e), &
crystallite_orientation(1:4,1,neighboring_i,neighboring_e), &
crystallite_symmetryID(1,i,e)) ! calculate disorientation
doxygen comments
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else ! for neighbor with different phase
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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crystallite_disorientation(:,n,1,i,e) = [0.0_pReal, 1.0_pReal, 0.0_pReal, 0.0_pReal] ! 180 degree rotation about 100 axis
doxygen comments
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endif
else ! for neighbor with local plasticity
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_disorientation(:,n,1,i,e) = [-1.0_pReal, 0.0_pReal, 0.0_pReal, 0.0_pReal] ! homomorphic identity
doxygen comments
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endif
else ! no existing neighbor
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_disorientation(:,n,1,i,e) = [-1.0_pReal, 0.0_pReal, 0.0_pReal, 0.0_pReal] ! homomorphic identity
doxygen comments
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endif
enddo
! --- calculate compatibility and transmissivity between me and my neighbor ---
call constitutive_nonlocal_updateCompatibility(crystallite_orientation,i,e)
endif
enddo
enddo
!$OMP END PARALLEL DO
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end subroutine crystallite_orientations
new subroutine crystallite_orientations: calculates the orientation matrix and the euler angles and - in case of single grain ips - the misorientation for each neighboring ip. The calculation of the misorientation is now done once in crystallite init and at the end of every FE increment. This saves a lot of time compared to doing it in dotState for every crystallite subinc.
2009-12-18 21:16:33 +05:30
in crystallite_stressAndItsTangent we now update the state first (explicit integration) and then integrate the stress (implicit integration) also inside the stress integration, it is now possible to define the frequency of the Jacobian update oin the LpLoop through iJacoLpResiduum. The frequency of the Jacobian update for the stiffness in the crystallite loop is controlled by the parameter iJacoStiffness. also updated the corresponding stuctograms in the documentation
2009-06-09 16:35:29 +05:30
doxygen comments
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!--------------------------------------------------------------------------------------------------
!> @brief return results of particular grain
!--------------------------------------------------------------------------------------------------
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
function crystallite_postResults(ipc, ip, el)
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
use math, only: &
math_qToEuler, &
grainrotation output now uses corrected rotation math
2013-06-07 15:05:00 +05:30
math_qToEulerAxisAngle, &
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
math_mul33x33, &
math_transpose33, &
math_det33, &
math_I3, &
inDeg, &
math_Mandel6to33, &
math_qMul, &
math_qConj
use mesh, only: &
mesh_element, &
mesh_ipVolume, &
mesh_ipCoordinates, &
mesh_maxNipNeighbors, &
mesh_ipNeighborhood, &
FE_NipNeighbors, &
FE_geomtype, &
FE_celltype
use material, only: &
microstructure_crystallite, &
crystallite_Noutput, &
material_phase, &
material_texture, &
homogenization_Ngrains
use constitutive, only: &
constitutive_sizePostResults, &
constitutive_postResults, &
constitutive_homogenizedC
in crystallite_stressAndItsTangent we now update the state first (explicit integration) and then integrate the stress (implicit integration) also inside the stress integration, it is now possible to define the frequency of the Jacobian update oin the LpLoop through iJacoLpResiduum. The frequency of the Jacobian update for the stiffness in the crystallite loop is controlled by the parameter iJacoStiffness. also updated the corresponding stuctograms in the documentation
2009-06-09 16:35:29 +05:30
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
implicit none
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
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integer(pInt), intent(in):: &
el, & !< element index
ip, & !< integration point index
ipc !< grain index
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
real(pReal), dimension(1+crystallite_sizePostResults(microstructure_crystallite(mesh_element(4,el)))+ &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
1+constitutive_sizePostResults(ipc,ip,el)) :: &
crystallite_postResults
real(pReal), dimension(3,3) :: &
Ee
real(pReal), dimension(4) :: &
rotation
real(pReal) :: &
detF
integer(pInt) :: &
o, &
c, &
crystID, &
mySize, &
n
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
crystID = microstructure_crystallite(mesh_element(4,el))
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
crystallite_postResults = 0.0_pReal
c = 0_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1) = real(crystallite_sizePostResults(crystID),pReal) ! size of results from cryst
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
c = c + 1_pInt
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
again: adding pInt, removing redundant use statments, chang in dble to real(,pReal)
2012-02-21 22:01:37 +05:30
do o = 1_pInt,crystallite_Noutput(crystID)
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 0_pInt
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
select case(crystallite_output(o,crystID))
case ('phase')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_postResults(c+1) = real(material_phase(ipc,ip,el),pReal) ! phaseID of grain
added "texture " as possible crystallite output => reports ID for later discrimination...
2011-03-22 19:10:27 +05:30
case ('texture')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_postResults(c+1) = real(material_texture(ipc,ip,el),pReal) ! textureID of grain
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
case ('volume')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
detF = math_det33(crystallite_partionedF(1:3,1:3,ipc,ip,el)) ! V_current = det(F) * V_reference
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_postResults(c+1) = detF * mesh_ipVolume(ip,el) &
/ homogenization_Ngrains(mesh_element(3,el)) ! grain volume (not fraction but absolute)
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
case ('heat')
mySize = 1_pInt
crystallite_postResults(c+1) = crystallite_heat(ipc,ip,el) ! heat production
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
case ('orientation')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 4_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_postResults(c+1:c+mySize) = crystallite_orientation(1:4,ipc,ip,el) ! grain orientation as quaternion
changed internal representation of orientation and misorientation from euler angles to quaternions (this should also fix some bugs in the math_misorientation subroutine). includes a couple of new functions in math.f90 and some changes in crystallite.f90. beware that crystallite output "orientation" now by default returns the orientation as quaternion. if you want euler angles instead, you have to add "eulerangles" as a crystallite output in your material.config file (see material.config template). for input of orientations in the texture block of the material.config you still have to specify the rotation in terms of euler angles, quaternions are not yet supported for input.
2010-03-18 17:53:17 +05:30
case ('eulerangles')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 3_pInt
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_postResults(c+1:c+mySize) = inDeg &
* math_qToEuler(crystallite_orientation(1:4,ipc,ip,el)) ! grain orientation as Euler angles in degree
New output can be requested from crystallite: (output) grainrotation it gives the deviation from the initial grain orientation in axis-angle representation with the angle in degrees.
2010-04-12 16:44:36 +05:30
case ('grainrotation')
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
mySize = 4_pInt
grainrotation output now uses corrected rotation math
2013-06-07 15:05:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
math_qToEulerAxisAngle(crystallite_rotation(1:4,ipc,ip,el)) ! grain rotation away from initial orientation as axis-angle in sample reference coordinates
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
crystallite_postResults(c+4) = inDeg * crystallite_postResults(c+4) ! angle in degree
new crystallite output "grainrotationX", "grainrotationY", "grainrotationZ" that gives the deviation of the initial orientation in degrees around the sample reference x/y/z axis, while "grainrotation" still gives the same as axis angle pair in crystal coordinates
2013-01-16 14:15:41 +05:30
case ('grainrotationx')
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
rotation = math_qToEulerAxisAngle(crystallite_rotation(1:4,ipc,ip,el)) ! grain rotation away from initial orientation as axis-angle in sample reference coordinates
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
crystallite_postResults(c+1) = inDeg * rotation(1) * rotation(4) ! angle in degree
new crystallite output "grainrotationX", "grainrotationY", "grainrotationZ" that gives the deviation of the initial orientation in degrees around the sample reference x/y/z axis, while "grainrotation" still gives the same as axis angle pair in crystal coordinates
2013-01-16 14:15:41 +05:30
case ('grainrotationy')
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
rotation = math_qToEulerAxisAngle(crystallite_rotation(1:4,ipc,ip,el)) ! grain rotation away from initial orientation as axis-angle in sample reference coordinates
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
crystallite_postResults(c+1) = inDeg * rotation(2) * rotation(4) ! angle in degree
new crystallite output "grainrotationX", "grainrotationY", "grainrotationZ" that gives the deviation of the initial orientation in degrees around the sample reference x/y/z axis, while "grainrotation" still gives the same as axis angle pair in crystal coordinates
2013-01-16 14:15:41 +05:30
case ('grainrotationz')
mySize = 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
rotation = math_qToEulerAxisAngle(crystallite_rotation(1:4,ipc,ip,el)) ! grain rotation away from initial orientation as axis-angle in sample reference coordinates
introduced dummy heat calculation, available as an crystallite output temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-19 00:27:28 +05:30
crystallite_postResults(c+1) = inDeg * rotation(3) * rotation(4) ! angle in degree
new substructure with 'include' and 'config' directories renaming of mpie_... to DAMASK for main usersubroutines extension of element outputs from 5 to 8 digits (FFT!!!)
2011-05-11 22:08:45 +05:30
! remark: tensor output is of the form 11,12,13, 21,22,23, 31,32,33
! thus row index i is slow, while column index j is fast. reminder: "row is slow"
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('defgrad','f')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_transpose33(crystallite_partionedF(1:3,1:3,ipc,ip,el)),[mySize])
added total Green-Lagrange strain to crystallite outputs
2012-01-20 15:55:35 +05:30
case ('e')
mySize = 9_pInt
crystallite_postResults(c+1:c+mySize) = 0.5_pReal * reshape((math_mul33x33( &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
math_transpose33(crystallite_partionedF(1:3,1:3,ipc,ip,el)), &
crystallite_partionedF(1:3,1:3,ipc,ip,el)) - math_I3),[mySize])
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('fe')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_transpose33(crystallite_Fe(1:3,1:3,ipc,ip,el)),[mySize])
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('ee')
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
Ee = 0.5_pReal *(math_mul33x33(math_transpose33(crystallite_Fe(1:3,1:3,ipc,ip,el)), &
crystallite_Fe(1:3,1:3,ipc,ip,el)) - math_I3)
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
mySize = 9_pInt
polishing: removed variable names like 'unit' and 'data' that are keywords of fortran and ensured that integer and real precision matches independent of machine standard. removed cut_off parameter for damask_spectral removed outpot of derived divergence measures and added RMS output in brackets added comments and options to the makefile
2012-02-16 00:28:38 +05:30
crystallite_postResults(c+1:c+mySize) = reshape(Ee,[mySize])
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('fp')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_transpose33(crystallite_Fp(1:3,1:3,ipc,ip,el)),[mySize])
added "Lp" as crystallite output
2011-02-25 13:45:26 +05:30
case ('lp')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_transpose33(crystallite_Lp(1:3,1:3,ipc,ip,el)),[mySize])
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('p','firstpiola','1stpiola')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_transpose33(crystallite_P(1:3,1:3,ipc,ip,el)),[mySize])
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 13:27:13 +05:30
case ('s','tstar','secondpiola','2ndpiola')
mySize = 9_pInt
some lines in crystallite.f90 exceeded limit of 132 characters fixed bug in Lib_VTK_IO.f90 (informed author as well) added zip file containing source of Lib_VTK_IO.f90
2013-05-08 23:18:00 +05:30
crystallite_postResults(c+1:c+mySize) = &
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
reshape(math_Mandel6to33(crystallite_Tstar_v(1:6,ipc,ip,el)),[mySize])
added elastic stiffness matrix as crystallite output
2012-03-01 18:36:09 +05:30
case ('elasmatrix')
mySize = 36_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_postResults(c+1:c+mySize) = reshape(constitutive_homogenizedC(ipc,ip,el),[mySize])
added crystallite output "neighboringelement" and "neighboringip" some polishing in crystallite_postResults
2013-05-08 17:32:30 +05:30
case('neighboringelement')
mySize = mesh_maxNipNeighbors
crystallite_postResults(c+1:c+mySize) = 0.0_pReal
forall (n = 1_pInt:FE_NipNeighbors(FE_celltype(FE_geomtype(mesh_element(2,el))))) &
crystallite_postResults(c+n) = real(mesh_ipNeighborhood(1,n,ip,el),pReal)
case('neighboringip')
mySize = mesh_maxNipNeighbors
crystallite_postResults(c+1:c+mySize) = 0.0_pReal
forall (n = 1_pInt:FE_NipNeighbors(FE_celltype(FE_geomtype(mesh_element(2,el))))) &
crystallite_postResults(c+n) = real(mesh_ipNeighborhood(2,n,ip,el),pReal)
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
end select
shape mismatch in crystallite, invalid names for variables(pos, size) in homogenization corrected. polishing of DAMASK_spectral_interface and makefile
2011-08-01 23:40:55 +05:30
c = c + mySize
reworked crystallite part to allow for flexible user output --> new "crystallite" part in config file --> new "crystallite" option for microstructures --> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 23:09:11 +05:30
enddo
new substructure with 'include' and 'config' directories renaming of mpie_... to DAMASK for main usersubroutines extension of element outputs from 5 to 8 digits (FFT!!!)
2011-05-11 22:08:45 +05:30
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
crystallite_postResults(c+1) = real(constitutive_sizePostResults(ipc,ip,el),pReal) ! size of constitutive results
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
c = c + 1_pInt
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
if (constitutive_sizePostResults(ipc,ip,el) > 0_pInt) &
crystallite_postResults(c+1:c+constitutive_sizePostResults(ipc,ip,el)) = &
constitutive_postResults(crystallite_Tstar_v(1:6,ipc,ip,el), crystallite_Fe, &
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate polishing: indentation level and capitalization
2013-11-21 16:28:41 +05:30
crystallite_temperature(ip,el), ipc, ip, el)
removed temperature integration and corresponding data structures and debugging options temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver. introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver. went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 18:34:59 +05:30
c = c + constitutive_sizePostResults(ipc,ip,el)
did a lot of polishing: - removed unnecessary "return" before end of subroutine or function: - changed undetermined array length (:) to (1:3) To prevent problems with some code analysing tools: - "3D oneliner loops" (with ";) only for "do" and "enddo" at the same time - removed line continuation in OMP statements made the makefile more flexible, removed heap-arrays switch
2011-09-13 21:24:06 +05:30
added new, flexible debugging scheme. now all modules have their own debug specification. compiles and runs, I hope nothing is broken did a lot of polishing
2012-03-09 01:55:28 +05:30
end function crystallite_postResults
major restructuring of code. homogenization as well as constitutive are now free to choose. the runtime got somewhat longer (25% on simple tests) compared to a hardcoded isostrain homogenization. this might be a point of further optimization at a later stage... please use homogenization_isostrain.f90 as starting point / example for future developments of homog-schemes. the homogenization scheme now can additionally output certain results. hence, the userdata structure at each integration point now looks like this: - sizeHomogPostResults - block of that size containing homogPostResults then for each grain: - sizeGrainPostResults - block of that size containing crystallitePostResults, which consist of: + phaseID + volFrac + Eulers (3) + any constitutive post results requested
2009-05-07 21:57:36 +05:30
doxygen comments
2013-02-22 04:38:36 +05:30
end module crystallite