.. |
MarcInclude
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added support for Marc 2018.1
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2018-11-07 14:11:10 +01:00 |
.gitignore
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symlinks can be handled by Git, so we can store them and simplify the installation
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2017-05-16 11:10:01 +02:00 |
CMakeLists.txt
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both solvers can share quit
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2018-09-27 20:09:59 +02:00 |
CPFEM.f90
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clearer code
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2018-10-04 06:48:33 +02:00 |
CPFEM2.f90
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Merge branch '47-save-restart-information-in-hdf5' into 'development'
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2018-11-12 08:42:22 +01:00 |
C_routines.c
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function to change working directory
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2018-05-27 14:08:23 +02:00 |
DAMASK_FEM.f90
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Merge branch 'development' into 29-rename-mesh_element-array
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2018-10-01 22:29:31 +02:00 |
DAMASK_abaqus.f
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verbose error message
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2018-07-10 09:53:20 +02:00 |
DAMASK_interface.f90
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check prerequisites as early as possible
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2018-10-15 05:03:53 +02:00 |
DAMASK_marc.f90
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Merge branch 'development' into 31_consistent_wd
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2018-08-03 00:08:16 +02:00 |
DAMASK_marc2018.1.f90
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missing link
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2018-11-07 15:13:16 +01:00 |
DAMASK_marc2018.f90
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added link for Marc2018
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2018-10-13 10:50:20 +02:00 |
DAMASK_spectral.f90
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Merge branch 'development' into 29-rename-mesh_element-array
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2018-10-01 22:29:31 +02:00 |
FEM_mech.f90
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Merge branch '38-introduce-rudimentary-PETSc-based-FEM-solver' of magit1.mpie.de:damask/DAMASK into 38-introduce-rudimentary-PETSc-based-FEM-solver
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2018-09-23 19:32:19 +02:00 |
FEM_utilities.f90
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change in tabulation order. should now be working correctly
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2018-09-23 03:14:23 +02:00 |
FEM_zoo.f90
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using shared interface for spectral and FEM solver
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2018-08-20 16:09:40 +02:00 |
FEsolving.f90
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unfified interface for spectral and FEM solver
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2018-08-20 15:59:13 +02:00 |
HDF5_utilities.f90
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close all objects of type integer(HID_T) created by native hdf5 routines
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2018-11-09 16:11:19 +01:00 |
IO.f90
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Merge branch '44-column-major-access-to-interaction-matrices' into 'development'
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2018-10-12 13:03:22 +02:00 |
commercialFEM_fileList.f90
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first step to include HDF5 in MSC.Marc
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2018-11-14 13:12:08 +01:00 |
compilation_info.f90
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compiler_options and compiler_version supported by new Intel compiler
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2018-02-02 12:36:09 +01:00 |
config.f90
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message better to understand and giving error instead of SIGSEGV
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2018-08-30 09:42:45 +02:00 |
constitutive.f90
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do concurrent not safe here
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2018-10-13 08:35:36 +02:00 |
crystallite.f90
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Merge branch '19-NewStylePhenopowerlaw' into 'development'
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2018-10-01 16:08:05 +02:00 |
damage_local.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
damage_none.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
damage_nonlocal.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
debug.f90
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inform about debug versions indenpendently of the solver
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2018-09-06 16:49:39 +02:00 |
homogenization.f90
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debug only available if compiled in debug mode
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2018-09-20 07:27:12 +02:00 |
homogenization_RGC.f90
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tensor input/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
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2018-09-27 11:53:45 +02:00 |
homogenization_isostrain.f90
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tensor input/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
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2018-09-27 11:53:45 +02:00 |
homogenization_none.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
hydrogenflux_cahnhilliard.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
hydrogenflux_isoconc.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
kinematics_cleavage_opening.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
kinematics_hydrogen_strain.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
kinematics_slipplane_opening.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
kinematics_thermal_expansion.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
kinematics_vacancy_strain.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
lattice.f90
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improved error reporting
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2018-10-10 07:42:07 +02:00 |
material.f90
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Merge branch '29-rename-mesh_element-array' into development
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2018-10-10 15:55:23 +02:00 |
math.f90
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more verbose and works for arbitrary precision
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2018-08-28 07:47:05 +02:00 |
mesh.f90
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polishing and encapsulating of Abaqus-specific local variables
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2018-10-09 17:57:10 -04:00 |
meshFEM.f90
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consistent (and better understandable) names
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2018-10-04 06:03:48 +02:00 |
numerics.f90
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foramtting of random_seed output to align with rest
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2018-10-08 17:01:56 -04:00 |
plastic_disloUCLA.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
plastic_dislotwin.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
plastic_isotropic.f90
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unused variables
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2018-08-26 11:53:18 +02:00 |
plastic_kinematichardening.f90
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Merge branch 'development' into 30_parsePhasePartOnce
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2018-06-27 21:43:09 +02:00 |
plastic_none.f90
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only doing things that are required
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2018-06-02 05:38:45 +02:00 |
plastic_nonlocal.f90
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integrationMode was always 1, very obscure code
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2018-08-16 23:33:39 +02:00 |
plastic_phenopowerlaw.f90
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using full precision
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2018-10-07 18:40:02 +02:00 |
porosity_none.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
porosity_phasefield.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
prec.f90
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not needed
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2018-09-18 05:20:08 +02:00 |
quit.f90
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initializing and closing the HDF5 library
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2018-10-09 14:13:51 +02:00 |
source_damage_anisoBrittle.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_damage_anisoDuctile.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_damage_isoBrittle.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_damage_isoDuctile.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_thermal_dissipation.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_thermal_externalheat.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_vacancy_irradiation.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_vacancy_phenoplasticity.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
source_vacancy_thermalfluc.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
spectral_damage.f90
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external statements will not work if interfaces exist
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2018-09-21 08:25:35 +02:00 |
spectral_mech_Basic.f90
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external statements will not work if interfaces exist
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2018-09-21 08:25:35 +02:00 |
spectral_mech_Polarisation.f90
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external statements will not work if interfaces exist
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2018-09-21 08:25:35 +02:00 |
spectral_thermal.f90
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external statements will not work if interfaces exist
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2018-09-21 08:25:35 +02:00 |
spectral_utilities.f90
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external statements will not work if interfaces exist
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2018-09-21 08:25:35 +02:00 |
system_routines.f90
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zero termination does not work
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2018-08-22 18:09:17 +02:00 |
thermal_adiabatic.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
thermal_conduction.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
thermal_isothermal.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
vacancyflux_cahnhilliard.f90
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using shared interface for spectral and FEM solver
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2018-08-20 16:09:40 +02:00 |
vacancyflux_isochempot.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |
vacancyflux_isoconc.f90
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more general name (should include parsing of debug and numerics)
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2018-06-14 06:39:49 +02:00 |