DAMASK_EICMD/code
Taymor El Achkar e1c5671e1f relaxed error message triggering such that purely elastic calculations and more than one constitutive instance using hex lattice are possible. no twinning possible if no slip system exists 2012-05-24 14:08:48 +00:00
..
config added missing space in makefile, made removing of old files in Makefile silent and updated files for tests to current versions 2012-05-23 18:08:34 +00:00
include corrected error in apply_DAMASK_modifications 2011-12-19 16:06:03 +00:00
setup corrected name of makefile (first letter upper case) 2012-03-14 11:58:05 +00:00
CPFEM.f90 several small corrections/polishing 2012-04-20 11:58:41 +00:00
DAMASK_abaqus_exp.f debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working) 2012-03-20 18:01:31 +00:00
DAMASK_abaqus_std.f debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working) 2012-03-20 18:01:31 +00:00
DAMASK_marc.f90 added new, flexible debugging scheme. 2012-03-08 20:25:28 +00:00
DAMASK_spectral.f90 using better measure (norm) of phase contrast for preconditioning 2012-05-07 08:12:13 +00:00
DAMASK_spectral_AL.f90 fixed bug (causing sigsev) concerning new functions mesh_spectral_get*** 2012-04-12 08:03:08 +00:00
DAMASK_spectral_interface.f90 regridding is now working, changed the subroutine into a function 2012-05-08 14:57:06 +00:00
FEsolving.f90 corrected reading in of ABAQUS debug modes and made numbering scheme for debugging depending on variables hoping to prevent these errors in debug.f90 2012-03-21 18:04:52 +00:00
IO.f90 corrected bug causing wrong element construction when using spectral solver. Also improved error messages for invalid resolution, dimension, and homogenization. 2012-05-21 09:06:02 +00:00
Makefile added missing space in makefile, made removing of old files in Makefile silent and updated files for tests to current versions 2012-05-23 18:08:34 +00:00
compilation_info.f90 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). 2012-03-20 12:26:21 +00:00
constitutive.f90 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 2012-05-18 14:35:52 +00:00
constitutive_dislotwin.f90 relaxed error message triggering such that purely elastic calculations and more than one constitutive instance using hex lattice are possible. no twinning possible if no slip system exists 2012-05-24 14:08:48 +00:00
constitutive_j2.f90 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). 2012-05-16 14:43:26 +00:00
constitutive_nonlocal.f90 allow minimum stable dipole height equal to zero; ensure that maximum stable dipole height is not smaller than the minimum value 2012-05-20 13:57:35 +00:00
constitutive_phenopowerlaw.f90 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). 2012-05-16 14:43:26 +00:00
constitutive_titanmod.f90 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). 2012-05-16 14:43:26 +00:00
crystallite.f90 small corrections for how to treat the new deltaState in FPI and euler integration; all integrators successfully tested with j2 2012-05-18 13:00:15 +00:00
damask.core.pyf changed indices counting (fortran to python style, easier division to get rid of periodic copies) 2012-05-09 10:09:56 +00:00
debug.f90 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). 2012-05-16 14:43:26 +00:00
fftw3.f03 minor changes, substituting implicit type conversions with explicit ones 2012-02-14 12:17:47 +00:00
homogenization.f90 regridding is now working, changed the subroutine into a function 2012-05-08 14:57:06 +00:00
homogenization_RGC.f90 added new, flexible debugging scheme. 2012-03-08 20:25:28 +00:00
homogenization_isostrain.f90 added new, flexible debugging scheme. 2012-03-08 20:25:28 +00:00
kdtree2.f90 fixed bug in nearest neighbor search, corrected error message for kdtree2.f90 2012-05-08 13:16:59 +00:00
lattice.f90 debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working) 2012-03-20 18:01:31 +00:00
material.f90 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). 2012-03-20 12:26:21 +00:00
math.f90 (likely) fixed a bug in the FFT-based geometry reconstruction. For (hopefully) correct math see Appendix B in paper. 2012-05-22 18:35:15 +00:00
mesh.f90 corrected bug causing wrong element construction when using spectral solver. Also improved error messages for invalid resolution, dimension, and homogenization. 2012-05-21 09:06:02 +00:00
numerics.f90 merged code for python and spectral solver interfacing (shared most of it anyway). 2012-04-11 17:28:08 +00:00
prec.f90 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) 2012-05-11 12:46:17 +00:00
prec_single.f90 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) 2012-05-11 12:46:17 +00:00
spectral_quit.f90 activated keyword expansion 2012-05-22 12:45:37 +00:00