| .. |
|
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
|
* new global integer variable "numerics_integrationMode" (1 indicating integration of central solution, 2 indicating integration of perturbed state)
|
2011-02-23 08:29:51 +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
|
* 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_nonlocal.f90
|
* new global integer variable "numerics_integrationMode" (1 indicating integration of central solution, 2 indicating integration of perturbed state)
|
2011-02-23 08:29:51 +00:00 |
|
constitutive_phenopowerlaw.f90
|
lattice: (re)introduced _symmetryType function to replace unsafe lookup array
|
2010-11-03 14:58:11 +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
|
* new global integer variable "numerics_integrationMode" (1 indicating integration of central solution, 2 indicating integration of perturbed state)
|
2011-02-23 08:29:51 +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
|
Did not compile. Fixed missing ,
|
2011-02-15 12:29:01 +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 |
|
makeMe.py
|
changed common block files to release version
|
2010-04-28 07:28:12 +00:00 |
|
makefile
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
|
material.config
|
* now able to introduce some scatter in the initial single dislocation density (only for nonlocal model!) ; setting the parameter "rhoSglScatter" to a positive value generates a gauss distribution for the dislocation density with standard deviation equal to "rhoSglScatter"
|
2011-02-04 15:41:32 +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
|
* now able to introduce some scatter in the initial single dislocation density (only for nonlocal model!) ; setting the parameter "rhoSglScatter" to a positive value generates a gauss distribution for the dislocation density with standard deviation equal to "rhoSglScatter"
|
2011-02-04 15:41:32 +00:00 |
|
mesh.f90
|
check for twin nodes only in direction of the surface normal. this solves a problem with models of single element thickness and periodic fluxes.
|
2011-02-24 09:26:30 +00:00 |
|
mpie_cpfem_abaqus_exp.f
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +00:00 |
|
mpie_cpfem_abaqus_std.f
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +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
|
extended IO to cope with different name for solverJob and Model
|
2011-02-21 14:37:38 +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 |
|
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
|
added version information to all files
|
2009-08-31 15:09:15 +00:00 |
|
todo.txt
|
ATTENTION repository has been moved to new server!
|
2011-01-05 16:11:51 +00:00 |
8aef9b1c13