c4c27860b2
renamed script
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updated to recent standard in io processing
introduced "primitive" bicontinuous structure in addition to "diamond" and "gyroid"
2012-11-07 16:52:10 +00:00
7cf2024be3
fixed buggy parameter checking
2012-11-07 16:51:17 +00:00
e11d107956
fixed reporting to STDOUT/STDERR
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fixed buggy parameter checking
2012-11-07 16:49:47 +00:00
dad9922f54
fixed bug in crystallite_FPI: stateDamper always has to be defined for each grain
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added some OMP FLUSH statements were necessary
replaced openmp do by forall construct where possible; this is much safer and perhaps even as fast for small loops
2012-11-07 15:43:29 +00:00
bbcffa668b
some small changes in including PETSc *.h90 files to prevent warnings.
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It seems that a bug in old gfortran 4.5.0 causes the problems, at least with 4.7.3 it seems to work after fixing the bugs in IO.f90
2012-11-07 13:11:41 +00:00
9e20149c6f
updated reference results, differ because changes in crystallite (matrix inversion removed)
2012-11-07 09:57:34 +00:00
9b99825ac6
preventing array index out of bounds in case of empty line, removed to goto statements
2012-11-07 09:31:46 +00:00
5214b93342
fixed bug when reading in geometry for spectral solver
2012-11-06 17:16:01 +00:00
3ada4897fb
reordered PETSc initialization (now first part done in interface, setting of parameters done in numerics), removed unnecessary includes for PETSc
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still not running with gfortran, use at own risk!
2012-11-06 16:00:51 +00:00
a86d528a4a
replaced call flush(6) by flush(6), slightly improved formating for output of gfortran version
2012-11-06 15:50:20 +00:00
e0dc2710b5
now works in "sourcing" mode.
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still have to worry about figuring out the lib/pathinfo details and setting LD_LIBRARY_PATH accordingly...
2012-11-06 15:40:45 +00:00
5b6baa7c0d
introduced distinction between ip coordinates and cell center coordinates; the former can be globally calculated by subroutine mesh_build_ipCoordinates, the latter locally by the function mesh_cellCenterCoordinates; renamed mesh_ipCenterOfGravity to mesh_ipCordinates
2012-11-06 14:37:13 +00:00
bb033c5fe7
Simplified algorithm of crystallite_integrateStress while preserving (almost) same functionality.
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Removed "leapfrogging" (increase of step for next guess, when last guess was ok); Replaced Armijo rule testing for step size by simple check if the residuum got better, since the former virtually did not have any effect; consistently using the 2-norm of the residuum rather than infinity-norm for the convergence check throughout the function
2012-11-06 12:35:45 +00:00
1583ae74c3
adopted new naming scheme
2012-11-06 08:49:48 +00:00
cfc8823328
missed those three in former commit...
2012-11-05 21:28:01 +00:00
1bd4262cfb
renaming of (loosely related) "spectral" scripts to (more tightly related) "geom" versions.
2012-11-05 21:19:12 +00:00
639d6e0655
inserted missing flush(crystallite_todo) in parallel section; might have caused trouble in parallel calculations before
2012-11-05 14:45:52 +00:00
1fc59107fa
removed debug statement in averageDown.py, deleted obsolete spectral_iterationCount.py (new solver will report statistics anyway and most probably the current count does not work as the screen output was modified)
2012-10-31 10:06:11 +00:00
689b64e3f5
updated geom pack/unpack test to new definition
2012-10-31 10:04:53 +00:00
086fe138b1
substituted matrix inversion to solve equation by direct solution routine from LAPACK
2012-10-31 09:56:26 +00:00
c0b83bd554
exported PDF versions as 300dpi PNG
2012-10-31 09:28:46 +00:00
afaf1f4e8c
made errors report to STDERR.
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maxMicrostructure remains silent if not present.
2012-10-30 16:32:00 +00:00
f2229883b5
exchanged "maxGrainCount" for "maxMicrostructure", since this is what it really means...
2012-10-30 16:15:10 +00:00
ff164c9209
changed packing syntax from "N copies of x" to "N of x" (now consistent with IO.f90)
2012-10-30 15:53:46 +00:00
2d36d52cf7
changed packing syntax from "N copies of x" to "N of x" (now consistent with geomPack and IO.f90)
2012-10-30 15:47:11 +00:00
be5d072e2d
Added report of SUCCESSFUL test for Revision 1848
2012-10-30 03:59:17 +00:00
55dc286be2
corrected limit for upper stable dipole distance; fixed a bug in the postResults where division by zero might happen
2012-10-29 13:02:01 +00:00
f666f8dcf3
added possibility to scale the plastic shearrate by the ratio of mobile to total density; keyword in material.config is "deadZone"
2012-10-29 12:49:28 +00:00
b9aa50c59a
improved performance for large packing values
2012-10-26 12:59:43 +00:00
4e5ae4056b
did a mistake during last update of this test, now it should run again
2012-10-25 13:16:48 +00:00
78aa010565
now just comparing substring to figure out if setup_processing was importing the core module
2012-10-25 12:40:06 +00:00
ca596bc7af
error messages are now printed, added svn properties
2012-10-25 09:16:17 +00:00
339205c890
added missing quotes
2012-10-25 07:56:58 +00:00
868984cb89
import of damask.core will not complain any more if done in setup_processing.py, however setup_processing.py will check if core.so exist after compilation and delete it before compilation
2012-10-25 07:55:27 +00:00
b212da5928
this version of the env script maybe works
2012-10-24 15:22:30 +00:00
d6f69568ad
Dynamically create DAMASK_ROOT and DAMASK_BIN
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by sourcing this script.
also documents the changes to .bashrc if one wants to
'install' DAMASK permanently
2012-10-24 15:19:41 +00:00
93cc466749
third entry in mesh_ipNeighborhood stores the neighbor_index that points from each neighbor back to the central ip; needed in nonlocal model
2012-10-24 14:03:02 +00:00
13b55275b1
documented utilities and structured, worked on the restart capabilities of the new basic solver
2012-10-24 11:31:40 +00:00
aefe8d7e32
added a test for compiling all spectral solver variants with gfortran
2012-10-24 09:26:21 +00:00
265a03d32a
new references, as the results are slightly different for corrected phenopowerlaw
2012-10-23 16:25:36 +00:00
5ad0eda1b6
switched saturation behavior!!
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was \dot s_alpha = (1-s_alpha/s_inf)^a h_alphabeta \dot gamma_beta
now \dot s_alpha = h_alphabeta (1-s_beta/s_inf)^a \dot gamma_beta
current form is consistent with the genmat implementation (and appears to make more physical sense). Kalidindi_etal1992 suggested this form, but altered it to the alpha-one in Bachu+Kalidindi1998... By now, it seems that some groups use alpha, others beta approach.
introduced two new absolute tolerance values for "shears" and "twinFrac" (default 1e-6).
2012-10-22 14:55:07 +00:00
2be331b74d
In crystallite for state integrators 2 and 3: now that "stateJump" is called before integrating dotState, we have to do state = state + dotState *dt instead of state = subState0 + dotState * dt; otherwise the deltaState is lost
2012-10-22 13:34:15 +00:00
2c0c3e35bb
found some figures that have not yet been committed
2012-10-22 08:25:25 +00:00
263f316344
added ./ in case current path is not in path
2012-10-22 08:18:44 +00:00
0980920b66
In crystallite: for state integrators 2 and 3 the deltaState always has to be done at the beginning of the integration, not at the end; otherwise the stiffness calculation can be completely wrong, when the state is changed after the stress integration for the central solution.
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Also changed some debugging levels in crystallite and mainly in constitutive_nonlocal
2012-10-22 07:59:35 +00:00
cb770000b9
added test to check creation of core module with ifort and gfortan
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added test to see if all spectral solvers compile (and get the same results independently of make options)
polished spectral utilities
2012-10-19 16:31:40 +00:00
68476f2102
resetting reference to old status after fixing bug in new basic scheme
2012-10-19 12:12:27 +00:00
3ecaa9e371
modified multiplication term in order to mimic a discrete distribution of dislocation sources; namely, at high resolution, when there is (on average) less than one source per integration point, a random generator decides whether there is a source in the finite volume or not; if there is one, then the multiplication turns independent of the density and depends only on the velocity/volume times a scalar factor; recovers density*velocity/lambda for large finite volumes
2012-10-19 11:40:17 +00:00
36676029e1
for state integrator 2 (explicit euler) and 3 (adaptive 2nd order euler): don't do any state evolution during stiffness perturbation, but only stress integration, since for those cases the state is not restored after every perturbation step
2012-10-19 11:20:31 +00:00
b9f97ba5da
unified naming scheme, fixed a bug in the new basic scheme, and added a statistic file similar to abaqus to store the information on needed cut backs and iterations for each inc
2012-10-19 08:44:21 +00:00
Philip Eisenlohr