Martin Diehl
0252fea3d7
fixed small bug in newstate
2014-07-10 08:47:00 +00:00
Martin Diehl
146d151357
disabled multiphysics output because homogenization output was not accessible anymore
2014-07-09 13:34:33 +00:00
Luv Sharma
7dfda9d8af
remved bug in phenopower law state initialization and a minor change in Makefile
2014-07-07 14:21:58 +00:00
Martin Diehl
27d861decc
fixed calculation of post results size introduced with new state
2014-07-03 13:17:29 +00:00
Luv Sharma
d5952138e3
corrected wrong dimensions of aTolstate and inclusion order of files in abaqus and marc interfaces
2014-07-03 12:52:33 +00:00
Martin Diehl
8fa2dcffbd
changed to new state, please report bugs to Luv or Martin
2014-07-02 12:27:39 +00:00
Pratheek Shanthraj
ac36190f10
no need to allocate a large array for constitutive(thermal,damage)_sizePostResults (changes apply only to new state)
2014-06-30 14:47:30 +00:00
Pratheek Shanthraj
676cba13a8
modified state integrators to perform staggered integration of plasticity damage and thermal internal variables
2014-06-24 23:21:25 +00:00
Pratheek Shanthraj
6347adcb65
fixed error in previous commit
2014-06-23 22:09:15 +00:00
Pratheek Shanthraj
d3356bde4e
moved mappings for new state layout to material
2014-06-22 18:58:29 +00:00
Martin Diehl
2160b37b1e
fixed warning message in constitutive
2014-06-17 15:24:44 +00:00
Martin Diehl
3533138936
removed delta state for J2 and phenopowerlaw when using new state
2014-06-17 06:54:49 +00:00
Martin Diehl
5bd80123b4
fixed two severe bugs in new state, now a little bit faster (399 vs. 378 sec) and more memory efficicient (251312 vs. 236832 kbytes) for Phenopowerlaw 16x16x16 example (short load only)
2014-06-16 19:19:38 +00:00
Luv Sharma
5755ed547b
applied new State for nonlocal model and a trivial changes in crystallite
2014-06-13 20:53:17 +00:00
Luv Sharma
8130f4b21f
changes to make newstate aware of damage variables
2014-06-11 16:32:09 +00:00
Luv Sharma
401b31c951
new state related changes
2014-06-11 12:27:41 +00:00
Pratheek Shanthraj
639ca89133
DAMASK (except nonlocal) now sees and interacts with FEM solver
2014-06-06 00:38:29 +00:00
Martin Diehl
164252213b
more work on the new state
2014-05-27 14:46:03 +00:00
Philip Eisenlohr
5d21ef5a84
fixed selective debugging logic flaw in crystallite_stressAndItsTangent
2014-05-19 16:43:32 +00:00
Philip Eisenlohr
88f94cbbec
increased debug threshold for some outputs (decreased verbosity level at "basic")
2014-05-15 13:01:54 +00:00
Martin Diehl
4bfced1a70
fixed small allocation flaws for new state
2014-05-12 13:00:37 +00:00
Martin Diehl
838a8be1b9
removed forgotten debug statements from last commit
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fixed material.config for abaqus example
2014-05-12 09:28:32 +00:00
Luv Sharma
d820a5aaa6
fixed some errors in changes related to newstate
2014-05-12 00:44:44 +00:00
Martin Diehl
4bb5439994
removed copyright from *.f90 and *.f files, will be added using the deployMe script for release/nightly build. Now based on presence of svn:keywords property set (usually "Id"). Similar thing will be done for .py, .sh, and .config files but more involved because they might be executable
2014-03-29 08:20:36 +00:00
Martin Diehl
7c79b31f6c
remove not needed use statement
2014-03-13 05:50:56 +00:00
Martin Diehl
9afc1e3a15
fixed wrong omp statement
2014-03-12 15:29:14 +00:00
Martin Diehl
ff1b1c1a50
fixed bug introduced with lattice_structure change nonlocal, but with DEBUG=ON OPTIMIZATION=OFF there is an FPE. Division by zero? Marked in the code
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forgot to commit dislotwin last time, now seems to work
2014-03-11 23:55:40 +00:00
Martin Diehl
2b589c3d71
moved reading in of lattice type and elastic constants to lattice module
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removed structure type for hex, fcc, bcc, now defining slip/twin systems for each phase found in material.config
constitutive modules will only be initialized if needed
homogenizedC function is only needed for models incorporating twinning in a physical way (titanmod and dislotwin)
2014-03-08 20:50:31 +00:00
Martin Diehl
a0d75ee05e
moved quaternion disorientation to lattice because it requires the knowledge of the lattice structure.
2014-02-28 13:28:27 +00:00
Martin Diehl
d45aea4467
moved reading in of lattice stru
2014-02-10 14:31:19 +00:00
Christoph Kords
b9b87a785c
added crystallite_F to debugging output
2014-02-03 13:19:49 +00:00
Christoph Kords
391d83fa2b
moved rate sensitivity block to where it belongs to, namely the analytic jacobian calculation
2014-01-22 15:34:10 +00:00
Pratheek Shanthraj
4b7890f133
fixed wrong indices in analytic jacobian calculation following christoph's changes. convergence is restored at least for the spectral solver
2014-01-22 10:16:55 +00:00
Christoph Kords
3dfdbaff5b
Fixed wrong indices in tangents dT_dFe and dFe_dLp, which however luckily did not have any effect in the perturbed stiffness since they were transposed such that the double contraction of both remained unchanged.
...
In contrast, the analytical jacobian will probably be affected by this change!
@Pratheek: Can you check with me how this can be fixed?
2014-01-22 08:38:13 +00:00
Christoph Kords
c10d0d15cb
crystallite_integrateStateFPI: convergence check always ran about all e,i,g; now checking only those specified in FEsolving_execElem, FEsolving_execIP
2014-01-21 18:45:41 +00:00
Christoph Kords
ff648492c1
perturbation calculation in crystallite_stressAndItsTangent: only backup and restore those chunks of crystallite_Fe, _Fp etc that are actually used in order to avoid pointless data copying in non ping pong mode
...
(missed some part in last commit)
2014-01-21 18:28:21 +00:00
Christoph Kords
029826d84f
perturbation calculation in crystallite_stressAndItsTangent: only backup and restore those chunks of crystallite_Fe, _Fp etc that are actually used in order to avoid pointless data copying in non ping pong mode
2014-01-21 16:35:12 +00:00
Christoph Kords
351aa6ba29
setting todo and converged flag only for those e,i,g that are to be executed (FE_elemExec etc)
...
used to spoil convergence checking in non ping pong mode and lead to slow performance
2014-01-21 16:09:00 +00:00
Christoph Kords
77cba87bf3
in crystallite_integrateStress: pass full 2nd PK stress to LpAndItsTangent instead of only the deviatoric part; otherwise constitutive laws that depend on the hydrostatic pressure do not work; constitutive laws that require a deviatoric stress need to calculate it internally (as is e.g. already done in the J2 model)
2014-01-16 10:36:40 +00:00
Martin Diehl
831e905b16
added missing lp output to crystallite
2013-12-20 11:13:12 +00:00
Martin Diehl
af075aaa9d
found bug (array index out of bounds), Philip/Franz please check if correct (Gfortran was complaining)
2013-12-20 08:33:46 +00:00
Pratheek Shanthraj
6f6bd86078
fixed bug in heat generation and analytic jacobian calculations
2013-12-18 10:19:48 +00:00
Martin Diehl
d5bdcf5a6d
some small improvements, still something wrong, probably in crystallite.f90
2013-12-13 14:14:17 +00:00
Martin Diehl
84d51d743c
fixed small issues, ATTENTION: Still a bug introduced with rev. 2783 not fixed
2013-12-13 13:19:17 +00:00
Martin Diehl
65ae979920
indroduced sourced allocation, enums where applicable (some parts still missing). fixed bug when having recursive file input
2013-12-12 17:09:59 +00:00
Martin Diehl
0bc99a9622
change latticeName to latticeID
2013-11-27 16:20:27 +00:00
Martin Diehl
2f7efa2055
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 08:04:05 +00:00
Christoph Kords
883669bd77
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate
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polishing: indentation level and capitalization
2013-11-21 10:58:41 +00:00
Pratheek Shanthraj
724380c624
Coupled phase field implementation for the basic petsc solver. needs clearing up… work in progress
2013-11-12 00:44:23 +00:00
Martin Diehl
3ecc8103f0
introduced dummy heat calculation, available as an crystallite output
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temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-18 18:57:28 +00:00