7484849b22
Merge remote-tracking branch 'origin/development' into 42-new-coding-style-for-homogenization-NEW
2019-01-27 08:44:46 +01:00
221c587362
using separate functions for stress and tangent
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extensively tested in 46-simplification-of-crystallite-f90-NEW3 already
2019-01-18 15:30:50 +01:00
54bb6a5eb6
more verbose name
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credits to Franz
2019-01-14 16:36:08 +01:00
adb68ff792
avoid converstions and use of global variables
2019-01-14 12:45:07 +01:00
f82a422e21
do concurrent causes problems on matesting/Intel 18.0.1
2019-01-14 09:34:14 +01:00
01a2fffd3c
clearer naming for vector <-> tensor conversion
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and a bunch of other improvements
2019-01-14 07:27:18 +01:00
619baefe19
some comments
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calling a conversion "Mandel" that does not follow the Mandel convention
(at least according to wikipedia) is not really intuitive
2019-01-13 18:54:20 +01:00
fe28e0d739
better follow the same conventions everywhere
2019-01-13 08:47:01 +01:00
cd8ee4503b
Merge branch '22-NewStyle_disloUCLA-2' into 'development'
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Resolve "New coding style for plastic_disloUCLA"
See merge request damask/DAMASK!51
2018-12-18 15:02:12 +01:00
5768356642
PGI compatible
2018-12-06 01:12:15 +01:00
91a2748131
simplifying
2018-12-04 20:33:28 +01:00
94695f773e
more verbose and works for arbitrary precision
2018-08-28 07:47:05 +02:00
241b2ade8b
more portable way to define PI
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https://software.intel.com/en-us/forums/intel-visual-fortran-compiler-for-windows/topic/490432
and compiler will not complain about truncation
2018-08-26 11:40:38 +02:00
0a6bde70c5
Merge branch 'development' into 19-NewStylePhenopowerlaw
2018-08-03 06:56:43 +02:00
449449b500
does the same as numpy.clip
2018-07-28 01:31:02 +02:00
d7da70cefb
Merge branch '30_parsePhasePartOnce' into 19-NewStylePhenopowerlaw
2018-06-19 19:30:01 +02:00
32d481020f
Merge branch 'development' into 30_parsePhasePartOnce
2018-06-16 14:49:57 +02:00
f8ae0ec925
list does tokenizing automatically
2018-06-10 11:07:17 +02:00
c903880d19
using on unitialized error caused segfault in some cases
2018-06-04 12:38:28 +02:00
804febe7f9
WIP: separate reading in and parsing
2018-05-31 18:31:44 +02:00
72b69959de
Merge branch 'development' into 19-NewStylePhenopowerlaw
2018-05-31 17:02:45 +02:00
f0309ac4dd
Bessel functions not used
2018-05-24 07:51:16 +02:00
6b27460a3b
Merge branch 'development' into 12-fixOrientationSampling
2018-05-05 19:03:51 +02:00
235b2fe3c8
ntwin = [0] cause problems
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math_expand now works for sum(how) == 0
2018-05-02 16:44:27 +02:00
81cab02d7a
simplified reading in and initialization
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init of absolute tolerances and state0 done on the fly
reading in array type parameters in the param structure
:
2018-04-25 19:43:03 +02:00
8509b13f16
avoid numerical noise
2018-03-13 09:21:41 +01:00
302a5017d4
Merge branch 'development' into 12-fixOrientationSampling
2018-03-13 04:12:03 +01:00
2ceb3aeea0
not all variables were consistently renamed
2018-03-13 03:56:02 +01:00
44e5644e78
fixed random Gaussian sampling
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sampling needs to be performed from unfiform misorientation, NOT uniformly distributed rotations
for Fiber, compute uniform tilt of Fiber axis
2018-03-13 03:36:24 +01:00
361cf680a5
merged more recent development
2018-03-09 18:19:41 -05:00
f26fd1d1dc
Fixed a physics issue: sense change with respect to difference between resolved stress and backstress
2018-03-09 18:01:09 -05:00
0ccce7facc
fixed missing angle initialization, simplified and commented
2018-03-08 17:33:54 +01:00
e716441787
indexing now follows description
2018-02-26 20:18:38 +01:00
cd4115bada
now using the correct rotation formula
2018-02-26 11:14:02 +01:00
e1c4c7e6e8
wrong indices in matrix rotation
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fixing this resolves issue 14: "Poor performance after load case rotation"
now inline with http://www.continuummechanics.org/rotationmatrix.html
C'_mnop = R_mi R_nj R_ok R_pl C_ijkl
2018-02-25 21:01:23 +01:00
4f4fa5daf8
simplified
2018-02-22 14:54:49 +01:00
e51de7ffd8
explicitly select halton bases in call
2018-02-22 14:16:36 +01:00
c6c66bb653
using proper Gauss sampling also for the fiber components
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function most probably still contains a bu
2018-02-22 00:42:06 +01:00
5c908e44ec
correct scaling for FWHM
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FWHM was wrong by a factor of approx 2.
Analytic expression can be found in https://en.wikipedia.org/wiki/Gaussian_function
2018-02-22 00:10:38 +01:00
9173d12d14
correct algorithm for sampling of uniform orientations and fix for Halton series
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Halton series gives strange results for large prime numbers, now always starting with 2 for first dimension, 3 for second etc.
Consecutive Halton numbers for rejection sampling seem to cause problems (i.e. introduce patterns).
Algorithm for uniformly distributed orientations with FWHM specified is taken from https://math.stackexchange.com/questions/131336 .
WIP: Gauss filtering is currently not implemented!
2018-02-21 20:32:52 +01:00
ae27660e86
simplified halto procedure (still needs testing)
2018-02-21 18:47:39 +01:00
98df2d1427
better description and names
2018-02-21 16:49:29 +01:00
a52f54a9a0
fixed typo in prime number list and extended to 1600 values
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source https://people.sc.fsu.edu/~jburkardt/f_src/halton/halton.f90
2018-02-21 14:37:02 +01:00
6b1c1af609
no early return required here
2018-02-21 08:55:33 +01:00
9b1e72e7bc
more sensible cutoff for scatter
2018-02-15 11:26:19 +01:00
230ffe8f35
Bessel functions for Gaussian scatter
2018-02-14 13:03:50 +01:00
fe07a34c69
source code should not be executable
2018-02-12 12:42:18 +01:00
b6abbfca9d
early return not needed here
2018-02-12 11:45:42 +01:00
2254746177
Merge branch 'development' of magit1.mpie.de:damask/DAMASK into development
2018-02-12 11:23:05 +01:00
7f487bb77b
merge development into kinematic hardening branch
2018-02-07 11:30:57 -05:00
Martin Diehl