..
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
* 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
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
enclose wall time measurement for dotState and dotTemperature function by CRITICAL construct
2010-11-19 17:19:03 +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
In order to help preventing further memory leaks all array sections now have an explicit instead of assumed shape, e.g. Fe(1:3,1:3) instead of Fe(:,:).
2011-02-09 13:12:46 +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
* check convergence for nonlocals also in stiffness calculation mode
2011-02-09 08:39:07 +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
lattice: (re)introduced _symmetryType function to replace unsafe lookup array
2010-11-03 14:58:11 +00:00
makeMe.py
changed common block files to release version
2010-04-28 07:28:12 +00:00
makefile
changed ifort options back to previous ones as -fast is not working
2011-01-26 13:33:44 +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
changed format of resolution. instead of reading exponent of two, now the number given equals directly to the number of FPs. Allows us to use arbitrary number of FPs.
2010-10-01 10:42:15 +00:00
mpie_cpfem_abaqus_exp.f
cpfe_general now returns also Kirchhoff-stress P and dPdF
2010-07-07 09:58:18 +00:00
mpie_cpfem_abaqus_std.f
corrected syntax errors (long lines, line continuation by \) and logical mistake in mpie_cpfem_marc / abq_std which went unnoticed in ifort. Using SunStudio f90 surfaced those...
2010-08-03 23:47:00 +00:00
mpie_cpfem_marc.f90
added hint that extreme values of stress and tangent belong to previous cycle
2011-02-08 12:43:30 +00:00
mpie_spectral.f90
mpie_spectral.f90: changed fourier transormation, now using the advanced interface to do the tranformation both ways with just one call. now also using the same variable for pk-stress in both domains and the change of deformation gradient in both domains.
2011-02-09 17:47:28 +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
mpie_spectral and mpie_interface: changed workingdir from pathToLoadFile to pathToGeomFile
2011-02-07 14:35:42 +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
mpie_spectral and mpie_interface: changed workingdir from pathToLoadFile to pathToGeomFile
2011-02-07 14:35:42 +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
3d7fad6ba9