299d9e6bc4
fixed bug in seed initialization that didn't allow to redo calculations that started with a random seed. Now the whole random seed array is set to one value, previously only the first one was reported and the remaining ones were random
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removed old random function used by halton
2012-08-30 14:58:30 +00:00
d80b45c1d9
added relativistic correction of velocity (maximum velocity given by parameter in material.config); probability of thermal activation in velocity law not allowed to be greater than one.
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output of creation rate for edge jogs now for own system, not collinear.
check for negative densities in dotState now uses absoluteToleranceRho instead of significantRho.
2012-08-30 07:33:13 +00:00
8e3b547cbd
changed numerics.f90 back to the old openmp statement as this doesn't seem to cause the problem and is standard conforming
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corrected typo in constitutive_j2.f90 that might cause abaqus to crash
now running 20 tests of abaqus in order to have a decent statistic about the crash behavior
improved abaqus_v6.env
2012-08-29 16:16:10 +00:00
84e3f94424
added flush for easier debugging
2012-08-29 15:23:43 +00:00
d83150be1b
now capturing "terminallyIll" for basic solution, should end in a automatic cutback of time steps for the spectral solver
2012-08-29 05:50:42 +00:00
3106b8ce0c
corrected definition of integer type for gfortran
2012-08-29 05:19:35 +00:00
d089c12947
abaqus seems to have similar problems with the openmp lib as marc (use module vs. include file), i hope this fixes the crashes
2012-08-28 19:48:38 +00:00
5e9e8497e6
new solver is now compiling without a PETSc installation, however only the plain basic solver is available then.
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also removed reporting of PETSc related variables in the case it is not installed/found
2012-08-28 19:19:47 +00:00
0f64289d75
fixed bug causing trouble with ifort 11 (abaqus)
2012-08-28 19:10:54 +00:00
0959ff3299
substituted hand written matrix inversion by LAPACK version with precision selection.
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also introduced check for inversion into DAMASK_spectral_Utilities.f90 for the stress BC calculation. This part is further improved by using 5% of the reference stiffness to avoid trouble in the fully plastic regime (where the stiffness is underestimated)
Test for Marc 2010 is updated because the new inversion give slightly different results near 0 (order of e-13)
2012-08-28 16:59:45 +00:00
73349d02f5
merged precision info into the file prec.f90 and removed prec_single.f90
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precision information is now parsed as a makro, defined by the compiler, eg. -DFLOAT=8 for 8 byte long floats or -- in case no values is given -- for the FEM wrapper by the interface files.
Please don't forget to run setup_code.py !!!!!!!!!!!
abaqus_v6.env is adjusted to specify the standard precision (float=8, int=4) and got some extra compilation options, some deprecated warning supressors are removed
Optional Marc modification will follow that allow automatic selection of suitable precision
2012-08-28 16:08:17 +00:00
f3e7b3cec8
added separate output of dipole formation rate for edge and screw
2012-08-27 15:57:31 +00:00
aa380dcb08
added separate output of dipole formation rate for edge and screw
2012-08-27 15:57:22 +00:00
efd1b513cf
fixed bug in divergenceFDM
2012-08-27 15:43:17 +00:00
9214da4465
added missing labels to list of available outputs
2012-08-27 12:41:57 +00:00
96ba5ecae4
moved some more 'mesh related' functions for post processing from math.f90 to mesh.f90
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f2py functions remaining in math.f90 now uses assumed size arrays in order to have simpler interfaces. This is only working with python 2.7!
changed python pre- and postprocessing scripts.
If you encounter any problems whith core modules, try to remove the old core.so in the lib/damask
2012-08-27 08:04:47 +00:00
55a5112f36
added comments for doxygen documentation
2012-08-25 11:46:36 +00:00
e335222bd0
added constitutive none to abaqus files
2012-08-24 19:21:39 +00:00
405c3765bd
fixed bug in fiber texture component caused non-even distribution by correctly getting numbers of the halton sequence
2012-08-24 13:27:55 +00:00
3cd5fa90e8
corrected dislocation multiplication term for special case of zero density
2012-08-24 11:36:46 +00:00
4f67d04c69
new parameter "significantRho" for nonlocal constitutive law ; density below this value will hardly contribute to dislocation glide or any dislocation reaction ; old parameter "absoluteToleranceRho" is now used only for its initial purpose, namely the absolute tolerance in the state integration
2012-08-23 05:48:21 +00:00
222aed9f60
derivative of velocity with respect to resolved stress was flawed; now much better convergence of stress integration for nonlocal constitutive law
2012-08-21 14:40:01 +00:00
ad7381cfdd
maximum relative step length in stress integration cannot decrease below 1
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intermediate tensor "A" is calculated only once before the Lp loop in "integrateStress"
2012-08-21 08:53:36 +00:00
35dffd52c1
now using spectral_quit (like old spectal solver, needed because of f2py)
2012-08-20 13:22:34 +00:00
b96df9987e
fixed reading/writing of integer arrays with function for real arrays
2012-08-16 14:55:23 +00:00
453c6031a7
added functions for reading values of integer data type to binary file, corrected comment on old versions which are for real (pReal) only
2012-08-16 11:57:15 +00:00
b2aacf9ca4
rates in constitutive_results are taken directly from last converged step and not calculated again; added output of rates for annihilation of screws and deposition of edge jogs on collinear system
2012-08-16 11:03:22 +00:00
bd754dbefd
corrected debug output of evolution rates; added possibility to change the safety factor for the CFL flux condition via the material.config file; updated the example material.config due to recent changes in nonlocal constitutive
2012-08-16 09:13:38 +00:00
0434ef3daa
some comments to be seen in documentation
2012-08-15 13:38:38 +00:00
c2c31a0a59
added SolverBasicPETSC module to the new FFT solver (solves the basic scheme using PETSc when mysolver = basicpetsc in numerics.config)
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some bug fixes
2012-08-14 16:58:23 +00:00
f5e7d576f1
introduced annihilation of screw dipoles; so far no thermal activation, but immediate annihilation; each annihilated screw dipole leaves behind an edge jog of same length as the dipole height on the collinear system
2012-08-14 12:26:20 +00:00
c1c5941733
stressAndItsTangent:
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when winding forward to last substep in increment, also do the calculation if this substep is below "subStepMinCryst";
output of "wind forward" and "cutback" info only for crystallites that are still "todo"
integrateStress:
maximum component in Lp determines absolute convergence criterium:
aTol = max(maxLpComp * rTol_fromConfig , aTol_fromConfig)
this ensures that small values in Lp do not spoil the convergence, similar to the effect of the relevantStrain parameter before (not needed anymore in the stress integration)
2012-08-14 12:07:59 +00:00
eae9a34c6b
corrected debugging output: extreme values of returned stress and jacobian belong to cpfem debugging, not homogenization
2012-08-14 11:48:43 +00:00
259eb7850e
more work on array ordering in new solver. (now working but not tested)
2012-08-10 17:01:58 +00:00
cd0da03ebc
changed comments to doxygen style
2012-08-10 15:58:17 +00:00
08c7be7d15
adaptive regrid now working, updates F and F_lastInc based on mapping.
2012-08-10 15:48:27 +00:00
b324a98014
changed order of most arrays to fortran-fast, whole new solver still work in progress
2012-08-09 13:04:56 +00:00
fe4d4d9525
changed comments in prec and IO to be read by doxygen, fine tuned output of doxygen and added precompilation for documentation
2012-08-09 11:01:53 +00:00
d0933dad7b
added filter option to the spectral solver to mitigate spurious oscillations due to gibb's phenomenon. activate by setting myfilter in config file appropriately (currently only 'none' and 'cosine' options coded). more cleaning up of AL code
2012-08-07 17:23:13 +00:00
925915e30d
some cleaning up
2012-08-07 12:02:57 +00:00
32f8c9c6ea
moved petsc option string to numerics and added new numerics parameters to config file
2012-08-06 17:27:53 +00:00
93658c72db
set auto values back to auto
2012-08-06 12:44:07 +00:00
7e3a837640
moved calculation and output of geometry related data to mesh.f90, moved output of command line related information to DAMASK_spectral_interface.f90.
...
improved new solver structure (use with make SOLVER=NEW)
2012-08-06 12:43:05 +00:00
a48d180f8c
allow prefactor for self-diffusion to be equal to zero
2012-08-06 09:03:33 +00:00
e2a2621235
updates for AL version of spectral solver
2012-08-06 08:53:12 +00:00
e8df3678aa
added possibility to assign the transmissivity of grain boundaries a fixed value by use of the keyword "grainboundaryTransmissivity" in the material.config; grain boundaries are identified as interfaces between areas of different material_texture
2012-08-03 14:32:49 +00:00
948d9c03d0
new version of modular solver structure
2012-08-03 09:25:48 +00:00
3ffba037d4
Reading of euler angles from the loadcase corrected.
2012-08-02 17:52:07 +00:00
740357172a
Reading of Euler angles from the loadcase corrected.
2012-08-02 17:46:50 +00:00
ee1bde0cd7
enabling regridding more than once by introducing deallocation of arrays
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added J2 test (stub from Taymour)
2012-07-31 15:37:49 +00:00
5a89c783d4
deallocating already allocated arrays in case of regridding/restarting (i.e. when calling init more than once)
2012-07-31 14:00:15 +00:00
991a7bbd2d
reordered initialization for spectral method, corrected bug of deformation BC parsing when prescribing velocity gradient resulting in wrong average deformation
2012-07-30 15:51:48 +00:00
d4163dd16f
further work on modularization, basic scheme is now calculating the same results as DAMASK_spectral.f90
2012-07-30 14:06:22 +00:00
c341ddd855
more modularization….
2012-07-26 13:58:47 +00:00
4ed68bb4ae
next round in modularization
2012-07-25 14:01:39 +00:00
e1faad8bcf
next round in modularizzation of solvers
2012-07-24 17:07:10 +00:00
882c44a61d
changed the majority of debugging output to level "extensive"
2012-07-24 15:29:23 +00:00
15c5131874
corrected formulation of maximum height of screw dislocation dipoles
2012-07-24 14:50:11 +00:00
9c0a161ec0
in case of regridding, undeformed configuration is written out correctly. Restart improve by reading in additional data from converged step.
2012-07-24 12:21:41 +00:00
c4c00f04f4
no dipole formation by stress decrease;
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dipole dissociation rate proportional to "deltaDipoleLimit / oldDipoleLimit", not "deltaDipoleLimit / newDipoleLimit"
2012-07-24 06:57:37 +00:00
3d59fec305
further modularisation of spectral solver (only for basic scheme so far)
2012-07-23 10:12:31 +00:00
bd9e81fbec
intermediate, not working state of new solver structure
2012-07-20 15:33:13 +00:00
ad3f9d8050
removed old standalone AL solver and introduced new structure for solver zoo
2012-07-19 17:24:56 +00:00
7d4ff278cb
worked on the restart capabilities
2012-07-19 14:16:59 +00:00
13caf2d389
made linear shape reconstruction working again, pretty similar results like corrected FFT reconstruction
2012-07-18 18:39:59 +00:00
a22163c2ae
reverted unwanted commit of Makefile
2012-07-18 12:34:46 +00:00
95d292b286
2012-07-18 12:31:07 +00:00
7c6fc121fd
condensed error reporting for constitutive_XYZ_init
...
removed erroneous check for structure>3
2012-07-17 17:36:24 +00:00
0fdd43b54b
minor clarification of file content and its use
2012-07-05 10:02:20 +00:00
4d09ef0648
changed variable name "debug_what" to "debug_level"
2012-07-05 09:54:50 +00:00
b69f446caa
added constitutive_none
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added wrongly deleted "endif" statements
removed tmglib and refblas from linker command for lapack (Koen??)
xxxROOT is changed by setup_code unless commented-out... So had to delete '#' again.
2012-07-03 13:59:38 +00:00
aeb1e18268
passing of multiple make options possible now
2012-07-03 13:57:05 +00:00
7f10ab0996
corrected to consistent naming: "IMKL"
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restored xxxROOT to commented-out auto entries.
commented-out currently unused PETSC parts.
added "refblas" and "tmglib" to LAPACK library inclusion (seems to be necessary since 3.2.1).
2012-07-03 12:36:54 +00:00
823013d485
new plasticity: none
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see material.config for necessary parameters (lattice_structure, elastic constants)
2012-07-03 11:16:38 +00:00
b4103b205d
parts of the material.config can now be set to echo their content back into the log-file (i.e. STDOUT / unit 6)
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use keyword "/echo/" before first section in the respective parts that you want to see echoed back into the log file.
2012-06-26 10:24:54 +00:00
767842acbf
now real time monitoring of DAMASK_spectral output to screen
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working with GNU Fortran as well (new checking for return code)
2012-06-25 09:03:19 +00:00
0606845f15
reordered calculation of current stiffness to enable restarting with different resolution
2012-06-22 09:20:23 +00:00
bd462d12c6
fixed some bugs in the regridding routine
2012-06-20 18:33:20 +00:00
d650972904
corrected some bugs concerning the regridding
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prevented FEsolving from potentially write to a none existing file
started to introduce petsc into the make chain (nothing happens if PETSC_DIR is not set)
2012-06-20 12:49:46 +00:00
f5eb8fcb25
fixed bug caused by the inconsistent sequence of slip and twin systems
2012-06-19 16:06:25 +00:00
481268c8c2
fixed closing of file (unit 222) statement in FEsolving.f90
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added missing keyword in mesh.f90 with ifndef Spectral statement (needed for Marc and Abaqus)
2012-06-19 14:33:24 +00:00
06be437bc9
added minRes to regridding function and writing out of new geometry file
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updated f2py wrapper to enable the use of init functions.
added 2 new error messages to io
2012-06-19 13:31:15 +00:00
8537e87b7e
added shell scripts to run tests from crontab, improved numbering in spectral compile tests and added some first files for testing restart capabilities of spectral solver.
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added configuration file for generation of code documentation using doxygen
restart of spectral solver is fixed and seem to work now also for restart at significant deformation.
spectral solver now gives exit code 2 if some increments did not converge
2012-06-18 15:27:01 +00:00
d9c6f9e134
switch on restartRead logical when requested by "--restart" cmdline switch
2012-06-18 09:27:36 +00:00
380f40561b
first calculation of Tstar still used hard coded Hooke, now usese constitutive_TandItsTangent(...)
2012-06-18 07:26:34 +00:00
b2fd3e1180
introduced preprocessor identifiers Marc, Abaqus, and Spectral to enable conditional compilation. This allows deleted dummy functions that are used by one solver only.
...
Mainly affected modules are IO and mesh. Most of the changes in mesh result from reordering the functions when grouping them depending on their solver.
Further advantage is that FE solver do not need FFTW and kdtree2 anymore. The include files for these two libraries moved to DAMASKROO/lib now as I figured out how to use a include path in the Makefile.
Put all the files I got when testing compilation with abaqus in a folder which to become the abaqus compilation test.
2012-06-15 16:10:21 +00:00
eb39d332bd
ULTRA OPTIMIZATION wasnt working anymore, seems to be related to Bertholds update of ws12 and ws13. had to remove -static from optimization string to be able to link again. Added some support for IKLM, but this didn't solve the problem
2012-06-13 17:19:16 +00:00
3ef17c208b
set default lapack to lapack instead of acml, added definition of makro for spectral solver for later use in preprocessor
2012-06-13 13:45:58 +00:00
052b526bde
made compilation of spectral code a command line switch and removed interactive question
2012-06-13 13:42:00 +00:00
7754416b35
now both getSolverJobName and getSolverWorkingDirectoryName use unit 5!
2012-06-13 09:58:06 +00:00
d3d0cfdab1
common blocks from 2012
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updated setup to also create DAMASK_marc2012.f90
2012-06-13 07:30:27 +00:00
a5c27f22ca
now uses unit 5 for file name inquiery (unit 6 points to stdout in 2012, might be a bug though)
2012-06-13 07:28:43 +00:00
5b7f2e122e
fixed usage of OpenMP function library
2012-06-12 09:44:05 +00:00
fc7b4d6471
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy
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deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
2012-06-06 15:11:30 +00:00
fa7f9866df
removed phase contrast/preconditioning
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added information on itmin in output, impoved output
set exit code to 0 on successful termination (seems to be unix standard)
exit codes:
0: successful termination
1: error (using IO_error)
2: require regrid
updated the AL solver, still VERY experimental
2012-06-05 16:34:20 +00:00
4b6800b89a
removed some unwanted open statements when writing out the sizeState
2012-06-05 13:13:33 +00:00
01522cf6f2
check for valid elasticity model
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improved error message in case of unknown elaticity/plasticity model
2012-06-02 14:23:28 +00:00
3af9165b08
useless debugging inforomation (asking for elastic moduli output) is removed
2012-05-31 09:25:04 +00:00
145d971d7e
added some debug output
2012-05-30 08:05:36 +00:00
5cc73a15a9
small correction in debug output
2012-05-30 07:41:22 +00:00
0127828f70
corrected initialization order
2012-05-29 15:08:18 +00:00
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
1003cfa7f8
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
c607441717
(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
bbf790a0a5
Input parameter 'QedgePerSbSystem' which denotes activation energy for each shear band system is added
2012-05-22 16:10:28 +00:00
9201133913
activated keyword expansion
2012-05-22 12:45:37 +00:00
cec3357e8f
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
20f203f799
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
5b02d4e8eb
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
4da6907648
moved remobilization of dead dislocations from dotState to deltaState
2012-05-18 13:35:44 +00:00
a5c1624648
check for invalid mesh type once in constitutive_init and not every time constitutive_nonlocal_dotState is called
2012-05-18 13:15:23 +00:00
8c849d62ee
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
abbae76c51
instantaneous jumps in the state by constitutive_deltaState are now incorporated for all state integrators. still they (should) not influence the result, since all constitutive laws simply return zero for the deltaState
2012-05-17 15:25:21 +00:00
351c2c6e65
deltaState depends on the current state, no the state at the beginning of the timestep
2012-05-17 12:18:30 +00:00
f6d5efeed3
removed arguments Fe and Fp from collectDeltaState function call
2012-05-17 11:04:22 +00:00
a54439e3b5
dotState does not have to be reset to zero. this is a remnant from older versions when the dotState for the nonlocal model used to be updated by the neighboring integration point
2012-05-16 15:35:14 +00:00
84d4652a07
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
df2d520630
stripping abaqus comments is now aware of damask comments
2012-05-15 14:59:26 +00:00
701cf2e71b
replaced duplicated math entry by missing mesh entry
2012-05-15 14:58:47 +00:00
0d745adfa0
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
7ee368f324
check whether there is any constitutive output
2012-05-11 07:38:20 +00:00
f8f9c089d6
check for NaN in math_QuaternionInSST
2012-05-11 07:37:32 +00:00
babf2647fb
use non signaling version of NaN
2012-05-11 07:35:52 +00:00
ce83026965
corrected bug in fft based geometry reconstruction causing mirrored geometries
2012-05-09 14:56:25 +00:00
d11aa15a67
changed indices counting (fortran to python style, easier division to get rid of periodic copies)
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corrected f2py pyf file
2012-05-09 10:09:56 +00:00
fbd075dc6e
corrected automatic determination of resolution
2012-05-08 15:12:43 +00:00
c752dd5474
regridding is now working, changed the subroutine into a function
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changed order of arrays in nearest neighbor search to make it fortran fast
constitutive.f90 and homogenization.f90 write state size out during initialization
setup/setup_processing.py is using byterecl to be compatible with binary files written out by solver
2012-05-08 14:57:06 +00:00
a9a72cee97
fixed bug in nearest neighbor search, corrected error message for kdtree2.f90
2012-05-08 13:16:59 +00:00
eb8265b914
fixed potential division by zero error discovered by our American friends
2012-05-08 07:16:00 +00:00
bdc46a8828
using better measure (norm) of phase contrast for preconditioning
2012-05-07 08:12:13 +00:00
4b18278781
reworked neares neigbor search subroutine, now also works for voronoi tesselation (general nn search in periodic cell)
2012-05-04 13:07:37 +00:00
863f0c766e
removed line continuation causing trouble
2012-05-04 08:19:12 +00:00
b4775249e8
corrected standard check to make f2py working with gfortran
2012-05-03 17:12:36 +00:00
26c6063a2c
utf8 encoding output to screen now for all solvers using intel ifort>10 or any gfortran (old versions might not support it, but we don't use them anyway)
2012-04-28 10:46:41 +00:00
dbeac18df6
no more dropping of comments in Abaqus input file assembly
2012-04-27 14:33:39 +00:00
83e89fba3c
improved regridding, especially interfacing to python (also for nearest neighbor search)
2012-04-24 17:02:27 +00:00
e33c34d86b
corrected wrong integer arithmetics in calculation of coordinates in DAMASK_spectral.f90
2012-04-24 16:59:38 +00:00
83e22c00a2
added missing allocation of slopeLnRate array.
...
changed parsing to lowercase name.
2012-04-20 12:18:38 +00:00
d2c4874db3
several small corrections/polishing
2012-04-20 11:58:41 +00:00
c889d20ba0
added simple preconditioning to improve convergence for high phase contrast materials in standard algorithm
2012-04-20 09:42:57 +00:00
caff3124fd
changed multiplier keyword from "times" to "copies of" to prevent ambiguity.
2012-04-17 10:05:49 +00:00
dbc5a3a3ce
subnodeparent check is now running only over actual number (not max) of parent nodes...
2012-04-17 09:19:44 +00:00
f905a97cdf
fixed bug (causing sigsev) concerning new functions mesh_spectral_get***
2012-04-12 08:03:08 +00:00
8c559cbdc9
fixed bug concerning file handling.
2012-04-11 18:46:36 +00:00
37fa6c2e14
merged code for python and spectral solver interfacing (shared most of it anyway).
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put functionality for getting header information (dimension, homogenization, resolution) in functions in mesh.f90
2012-04-11 17:28:08 +00:00
a18e5e48dc
added 'times' keyword in function for continuous int values: "4 times 1 => 1 1 1 1", mainly for geom files of spectral solver.
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corrected name for contin"U"ousIntValues functions
2012-04-11 17:24:50 +00:00
91cfd21c88
corrected some copy and paste errors
2012-04-11 14:12:30 +00:00
9a92d343dc
added Onurs modified description for tausat in j2 law.
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Polishing phenopowerlaw
2012-04-11 14:01:02 +00:00
f2da887899
added missing ":" in mesh.f90, introduced absolute stress tolerance for spectral solver in numerics.config/numerics.f90
2012-04-11 12:57:25 +00:00
f20cecd421
integrated subroutine for regridding into mesh.f90 and made it available for python
2012-04-10 15:15:46 +00:00
Martin Diehl