b429068aa4
adopted new reference result for grainGrowth test
2018-03-30 11:54:15 -04:00
1b12457fe6
vicinityOffset to specific triggering IDs instead of just any other ID
2018-03-30 11:48:02 -04:00
d17debbd5e
Merge branch 'development' of magit1.mpie.de:damask/DAMASK into development
2018-03-27 16:54:08 -04:00
0570a49ed5
fixed broken logic of restoring and preventing immutable microstructures
2018-03-27 16:53:49 -04:00
8509b13f16
avoid numerical noise
2018-03-13 09:21:41 +01:00
ff2c950d20
Merge branch 'development' into 12-fixOrientationSampling
2018-03-13 04:37:41 +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
005c9f80c5
include updated test
2018-03-13 03:52:17 +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
fb710dda0a
[skip ci] updated version information after successful test of v2.0.1-1110-g52c9954
2018-03-12 22:56:52 +01:00
52c9954ca4
Revert "more work to get testing to work"
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This reverts commit 63c104b374
2018-03-12 17:44:37 +01:00
63c104b374
more work to get testing to work
2018-03-12 17:35:54 +01:00
12adcec41e
updated PRIVATE submodule to new state
2018-03-09 18:36:34 -05:00
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
8fa8427c99
simple test, only ensures that scatter is not bigger than 2 FWHM (hard max)
2018-03-08 17:35:59 +01:00
0ccce7facc
fixed missing angle initialization, simplified and commented
2018-03-08 17:33:54 +01:00
48fce3a49e
[skip ci] updated version information after successful test of v2.0.1-1107-g2c3eae6
2018-03-08 10:15:17 +01:00
2c3eae6bf0
fixed tests and bug for very small unit cube fractions when grid is also small
2018-03-07 18:59:27 -05:00
32c34457c2
direct selection of valid seed coordinates within subfraction of unit cube instead of check and repeat
2018-03-07 17:45:22 -05:00
03c643c433
[skip ci] updated version information after successful test of v2.0.1-1104-g88c46d5
2018-03-01 06:25:54 +01:00
88c46d500e
Merge branch '13-higher-order-thermal-expansion' into 'development'
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Resolve "higher-order thermal expansion"
Closes #13
See merge request damask/DAMASK!19
2018-02-28 21:08:01 +01:00
f18f076a09
[skip ci] Merge branch 'master' into development
2018-02-27 19:18:42 +01:00
35e4244887
Merge commit 'v2.0.1-1098-g5c2aeed'
2018-02-27 19:18:18 +01:00
5c2aeedb73
[skip ci] updated version information after successful test of v2.0.1-1097-gcb073fe
2018-02-27 19:18:18 +01:00
f5f5791b39
[skip ci] Merge branch 'master' into development
2018-02-27 10:01:09 +01:00
3a4506c5ae
[skip ci] updated version information after successful test of v2.0.1-1088-gf35a88d
2018-02-27 10:01:02 +01:00
cb073fe127
Merge branch '14_LoadCaseRotationPerformance' into 'development'
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14 load case rotation performance
See merge request damask/DAMASK!20
2018-02-27 00:41:20 +01:00
f35a88d2c4
it's 2018 already
2018-02-26 23:51:23 +01:00
1bbaa7cefe
reverted last commit, scipy.linalg is different from numpy.linalg
2018-02-26 23:50:44 +01:00
6046a7ae3d
there is no scipy.linalg (at least on my system)
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numpy.linalg is automatically imported together with numpy
2018-02-26 20:22:57 +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
30d66c2d67
[skip ci] updated version information after successful test of v2.0.1-1084-gb078234
2018-02-26 09:50:06 +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
b078234644
added scipy and scipy.linalg as known modules for calculations
2018-02-25 14:19:22 -05:00
bc998846ab
thermal expansion coefficient alpha = a + b(T-T_0) + c(T-T_0)^2
2018-02-25 14:14:03 -05:00
c2ced6a274
not needed anymore
2018-02-25 14:45:35 +01:00
d5d71d2321
math_transpose33 has no benefit here
2018-02-25 13:42:02 +01:00
42500eabff
simplified (math_transpose33 does not provide any benefit here)
2018-02-25 12:48:58 +01:00
eedec74a6a
correct debug reporting
2018-02-25 12:31:23 +01:00
86768c38d9
source code should not be executable
2018-02-25 10:16:27 +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
Philip Eisenlohr