.. |
config
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Input parameter 'QedgePerSbSystem' which denotes activation energy for each shear band system is added
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2012-05-22 16:10:28 +00:00 |
include
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corrected error in apply_DAMASK_modifications
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2011-12-19 16:06:03 +00:00 |
setup
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corrected name of makefile (first letter upper case)
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2012-03-14 11:58:05 +00:00 |
CPFEM.f90
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several small corrections/polishing
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2012-04-20 11:58:41 +00:00 |
DAMASK_abaqus_exp.f
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debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working)
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2012-03-20 18:01:31 +00:00 |
DAMASK_abaqus_std.f
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debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working)
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2012-03-20 18:01:31 +00:00 |
DAMASK_marc.f90
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added new, flexible debugging scheme.
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2012-03-08 20:25:28 +00:00 |
DAMASK_spectral.f90
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using better measure (norm) of phase contrast for preconditioning
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2012-05-07 08:12:13 +00:00 |
DAMASK_spectral_AL.f90
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fixed bug (causing sigsev) concerning new functions mesh_spectral_get***
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2012-04-12 08:03:08 +00:00 |
DAMASK_spectral_interface.f90
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regridding is now working, changed the subroutine into a function
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2012-05-08 14:57:06 +00:00 |
FEsolving.f90
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corrected reading in of ABAQUS debug modes and made numbering scheme for debugging depending on variables hoping to prevent these errors in debug.f90
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2012-03-21 18:04:52 +00:00 |
IO.f90
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corrected bug causing wrong element construction when using spectral solver. Also improved error messages for invalid resolution, dimension, and homogenization.
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2012-05-21 09:06:02 +00:00 |
Makefile
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corrected NaN in prec_single.f90 (was already silent but with typo), polished output and added switch in order to check range on all files except of prec.f90 (in which NaN is defined)
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2012-05-11 12:46:17 +00:00 |
compilation_info.f90
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added "-assume byterecl" in Makefile for ifortran to specify with "recl=" the size of the file in bytes instead of 4byte chunk when opening files. (same as in gfortran per default).
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2012-03-20 12:26:21 +00:00 |
constitutive.f90
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dipole dissociation and formation by change in stress as new mechanism in deltaState; had to add dipole height to state variables, which is however updated by deltaState instead of microstructure; alternatively microstructure had to know the current stress state
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2012-05-18 14:35:52 +00:00 |
constitutive_dislotwin.f90
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Input parameter 'QedgePerSbSystem' which denotes activation energy for each shear band system is added
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2012-05-22 16:10:28 +00:00 |
constitutive_j2.f90
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all constitutive modules now contain a new function "deltaState", which in the future allows to have an instantaneous and incremental change of the state (additional to the rate based evolution with dotState).
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2012-05-16 14:43:26 +00:00 |
constitutive_nonlocal.f90
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allow minimum stable dipole height equal to zero; ensure that maximum stable dipole height is not smaller than the minimum value
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2012-05-20 13:57:35 +00:00 |
constitutive_phenopowerlaw.f90
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all constitutive modules now contain a new function "deltaState", which in the future allows to have an instantaneous and incremental change of the state (additional to the rate based evolution with dotState).
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2012-05-16 14:43:26 +00:00 |
constitutive_titanmod.f90
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all constitutive modules now contain a new function "deltaState", which in the future allows to have an instantaneous and incremental change of the state (additional to the rate based evolution with dotState).
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2012-05-16 14:43:26 +00:00 |
crystallite.f90
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small corrections for how to treat the new deltaState in FPI and euler integration; all integrators successfully tested with j2
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2012-05-18 13:00:15 +00:00 |
damask.core.pyf
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changed indices counting (fortran to python style, easier division to get rid of periodic copies)
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2012-05-09 10:09:56 +00:00 |
debug.f90
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all constitutive modules now contain a new function "deltaState", which in the future allows to have an instantaneous and incremental change of the state (additional to the rate based evolution with dotState).
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2012-05-16 14:43:26 +00:00 |
fftw3.f03
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minor changes, substituting implicit type conversions with explicit ones
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2012-02-14 12:17:47 +00:00 |
homogenization.f90
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regridding is now working, changed the subroutine into a function
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2012-05-08 14:57:06 +00:00 |
homogenization_RGC.f90
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added new, flexible debugging scheme.
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2012-03-08 20:25:28 +00:00 |
homogenization_isostrain.f90
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added new, flexible debugging scheme.
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2012-03-08 20:25:28 +00:00 |
kdtree2.f90
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fixed bug in nearest neighbor search, corrected error message for kdtree2.f90
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2012-05-08 13:16:59 +00:00 |
lattice.f90
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debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working)
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2012-03-20 18:01:31 +00:00 |
material.f90
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added "-assume byterecl" in Makefile for ifortran to specify with "recl=" the size of the file in bytes instead of 4byte chunk when opening files. (same as in gfortran per default).
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2012-03-20 12:26:21 +00:00 |
math.f90
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(likely) fixed a bug in the FFT-based geometry reconstruction. For (hopefully) correct math see Appendix B in paper.
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2012-05-22 18:35:15 +00:00 |
mesh.f90
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corrected bug causing wrong element construction when using spectral solver. Also improved error messages for invalid resolution, dimension, and homogenization.
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2012-05-21 09:06:02 +00:00 |
numerics.f90
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merged code for python and spectral solver interfacing (shared most of it anyway).
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2012-04-11 17:28:08 +00:00 |
prec.f90
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corrected NaN in prec_single.f90 (was already silent but with typo), polished output and added switch in order to check range on all files except of prec.f90 (in which NaN is defined)
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2012-05-11 12:46:17 +00:00 |
prec_single.f90
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corrected NaN in prec_single.f90 (was already silent but with typo), polished output and added switch in order to check range on all files except of prec.f90 (in which NaN is defined)
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2012-05-11 12:46:17 +00:00 |
spectral_quit.f90
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activated keyword expansion
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2012-05-22 12:45:37 +00:00 |