.. |
CPFEM.f90
|
transposed writing into t16 file (and screen/debug) did not work with just stating array(1:3,:)...
|
2011-01-24 15:02:19 +00:00 |
FEsolving.f90
|
Introducing the capability to restart jobs that crashed in the middle of sims. At the moment, this feature is exclusive for Marc.
|
2010-11-03 14:39:18 +00:00 |
IO.f90
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
concom2007r1
|
restructured the repository: renamed trunk into code, moved documentation one directory up, therefore you can now checkout either code or documentation only if you like
|
2009-06-25 07:17:59 +00:00 |
concom2008r1
|
restructured the repository: renamed trunk into code, moved documentation one directory up, therefore you can now checkout either code or documentation only if you like
|
2009-06-25 07:17:59 +00:00 |
concom2010
|
added comment on reformating to common block files
|
2010-05-06 08:50:54 +00:00 |
constitutive.f90
|
* removed calculations for dipole formation/dissociation by stress change, since it is not used anyways; also removed associated constitutive outputs from material.config
|
2011-02-25 09:53:20 +00:00 |
constitutive_dislotwin.f90
|
* former "relevantRho" and "relevantResistance" is renamed to "atol_rho" and "atol_resistance" and now used as an absolute tolerance for the state residuum. before it was used rather as significant state, so whenever the state dropped below that value it was considered converged. (In dislotwin and titanmod constitutive law there is only one value atol_rho which is used for all the states, though the state array consists not only of densities. We need further parameters here!)
|
2010-10-26 13:16:37 +00:00 |
constitutive_j2.f90
|
removed all math functions only for double precision by the more flexible counterpart, e.g. "dsqrt --> sqrt", "dsin --> sin". Should not cause any harm, as long as "implicit none" is used.
|
2011-02-25 09:25:53 +00:00 |
constitutive_nonlocal.f90
|
* removed calculations for dipole formation/dissociation by stress change, since it is not used anyways; also removed associated constitutive outputs from material.config
|
2011-02-25 09:53:20 +00:00 |
constitutive_phenopowerlaw.f90
|
removed all math functions only for double precision by the more flexible counterpart, e.g. "dsqrt --> sqrt", "dsin --> sin". Should not cause any harm, as long as "implicit none" is used.
|
2011-02-25 09:25:53 +00:00 |
constitutive_titanmod.f90
|
* former "relevantRho" and "relevantResistance" is renamed to "atol_rho" and "atol_resistance" and now used as an absolute tolerance for the state residuum. before it was used rather as significant state, so whenever the state dropped below that value it was considered converged. (In dislotwin and titanmod constitutive law there is only one value atol_rho which is used for all the states, though the state array consists not only of densities. We need further parameters here!)
|
2010-10-26 13:16:37 +00:00 |
creeps2007r1
|
restructured the repository: renamed trunk into code, moved documentation one directory up, therefore you can now checkout either code or documentation only if you like
|
2009-06-25 07:17:59 +00:00 |
creeps2008r1
|
restructured the repository: renamed trunk into code, moved documentation one directory up, therefore you can now checkout either code or documentation only if you like
|
2009-06-25 07:17:59 +00:00 |
creeps2010
|
added comment on reformating to common block files
|
2010-05-06 08:50:54 +00:00 |
crystallite.f90
|
* removed calculations for dipole formation/dissociation by stress change, since it is not used anyways; also removed associated constitutive outputs from material.config
|
2011-02-25 09:53:20 +00:00 |
debug.config
|
* 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"
|
2010-10-01 12:18:49 +00:00 |
debug.f90
|
* 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"
|
2010-10-01 12:18:49 +00:00 |
fftw3.f
|
added fftw3 as fft(library will not versioned, should be in a linkable folder) , did some corrections on the code, splitted main file up (allows use of makefile), added makefile
|
2010-08-27 16:39:38 +00:00 |
homogenization.f90
|
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-(((
|
2010-11-03 17:22:48 +00:00 |
homogenization_RGC.f90
|
1. Adding more comments
|
2010-11-26 11:50:20 +00:00 |
homogenization_isostrain.f90
|
extended output string length for init msg
|
2010-04-28 17:19:06 +00:00 |
lattice.f90
|
removed all math functions only for double precision by the more flexible counterpart, e.g. "dsqrt --> sqrt", "dsin --> sin". Should not cause any harm, as long as "implicit none" is used.
|
2011-02-25 09:25:53 +00:00 |
libfftw3.a
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
libfftw3_threads.a
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
libfftw3f.a
|
added single precision libraries for FFTW
|
2011-02-24 18:39:57 +00:00 |
libfftw3f_threads.a
|
added single precision libraries for FFTW
|
2011-02-24 18:39:57 +00:00 |
makeMe.py
|
changed common block files to release version
|
2010-04-28 07:28:12 +00:00 |
makefile
|
some polishing for single precision version.
|
2011-02-25 12:41:46 +00:00 |
material.config
|
* removed calculations for dipole formation/dissociation by stress change, since it is not used anyways; also removed associated constitutive outputs from material.config
|
2011-02-25 09:53:20 +00:00 |
material.f90
|
grain orientation shuffling was skipped for /elemhomo/. no clue why, now dropped...
|
2011-02-03 17:25:58 +00:00 |
math.f90
|
set type for acos_arg
|
2011-03-04 14:57:22 +00:00 |
mesh.f90
|
now deleted old _single files
|
2011-02-25 12:49:18 +00:00 |
mpie_cpfem_abaqus_exp.f
|
included "-heap-arrays 500000000" in remark on how to change compile command
|
2011-03-08 08:18:04 +00:00 |
mpie_cpfem_abaqus_std.f
|
included "-heap-arrays 500000000" in remark on how to change compile command
|
2011-03-08 08:18:04 +00:00 |
mpie_cpfem_marc.f90
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
mpie_spectral.f90
|
some comments (talking to Ricardo)
|
2011-02-25 16:24:23 +00:00 |
mpie_spectral2d.f90
|
changed makefile: material subroutines are now compiled using openmp, enabled linux threads for fftw3 (also did some slight changes to enable that in the fortran source code)
|
2011-01-07 12:56:45 +00:00 |
mpie_spectral_interface.f90
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
mpie_spectral_single.f90
|
removed all math functions only for double precision by the more flexible counterpart, e.g. "dsqrt --> sqrt", "dsin --> sin". Should not cause any harm, as long as "implicit none" is used.
|
2011-02-25 09:25:53 +00:00 |
numerics.config
|
* 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"
|
2010-10-01 12:18:49 +00:00 |
numerics.f90
|
sorry, forgot to commit the numerics.f90, too
|
2011-02-23 12:30:52 +00:00 |
prec.f90
|
some polishing for single precision version.
|
2011-02-25 12:41:46 +00:00 |
prec_single.f90
|
some comments (talking to Ricardo)
|
2011-02-25 16:24:23 +00:00 |
todo.txt
|
Abaqus interfaces dapted to newest version of the rest of the code
|
2011-03-07 12:49:27 +00:00 |