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.
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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
Martin Diehl