Martin Diehl
|
464375a54e
|
pInt does not add any value
|
2019-03-27 22:12:31 +01:00 |
|
Martin Diehl
|
761dcb0358
|
no need for explicit loop
|
2019-03-25 18:04:53 +01:00 |
|
Martin Diehl
|
18fe8c34ee
|
fortran fast storage of interaction matrices
|
2019-03-11 22:41:59 +01:00 |
|
Martin Diehl
|
34660599a1
|
dummy HDF5 output for all plasticity laws
|
2019-03-09 20:43:31 +01:00 |
|
Martin Diehl
|
0d08659b2a
|
general cleaning
|
2019-03-09 11:11:40 +01:00 |
|
Martin Diehl
|
e9087f83fe
|
small improvements
checking size of arguments (not shape)
length of lattice structure not limited to 3 any more
|
2019-01-25 14:01:17 +01:00 |
|
Philip Eisenlohr
|
f81c25bb58
|
[skip ci] allow strain softening in phenopowerlaw, i.e. xi_sat might be less than xi_0
|
2019-01-17 17:51:38 -05:00 |
|
Martin Diehl
|
aaea11d96b
|
make similarity of state/param structure clear
|
2019-01-13 17:03:49 +01:00 |
|
Martin Diehl
|
070952dbb8
|
Merge branch 'NewStyleKinematicHardening-3' into development
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2019-01-08 01:12:05 +01:00 |
|
Martin Diehl
|
995122504e
|
cross comparing
|
2019-01-07 08:04:02 +01:00 |
|
Martin Diehl
|
4037085f6c
|
whitespace not needed
|
2019-01-07 07:24:02 +01:00 |
|
Martin Diehl
|
705d55a3a5
|
re-enabled sanity checks + slight adjustments to layout
|
2019-01-07 07:20:13 +01:00 |
|
Martin Diehl
|
2aa2373432
|
Merge branch 'development' into NewStyleKinematicHardening-3
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2019-01-07 07:09:28 +01:00 |
|
Martin Diehl
|
15d1789a19
|
following best practise from phenopowerlaw
|
2019-01-06 21:55:33 +01:00 |
|
Martin Diehl
|
ebf028421b
|
corrected unit
|
2019-01-06 20:57:40 +01:00 |
|
Martin Diehl
|
1192f16582
|
Merge remote-tracking branch 'origin/development' into 56-parallel-hdf5
|
2019-01-06 20:56:36 +01:00 |
|
Martin Diehl
|
19df6f8a71
|
general polishing
|
2019-01-05 23:55:10 +01:00 |
|
Martin Diehl
|
dc64841f15
|
mutual best practise phenopowerlaw <-> disloUCLA
|
2019-01-05 23:40:59 +01:00 |
|
Martin Diehl
|
c5dd8d1265
|
unified style
|
2018-12-30 18:11:03 +01:00 |
|
Martin Diehl
|
311b8be715
|
simplifying
|
2018-12-30 15:14:43 +01:00 |
|
Martin Diehl
|
226bbad013
|
don't waste character space
|
2018-12-22 08:31:13 +01:00 |
|
Martin Diehl
|
d8a7fdd01d
|
function description was wrong
|
2018-12-21 18:14:54 +01:00 |
|
Martin Diehl
|
dcd22ccb6a
|
put private functions at the end
for easy separation
|
2018-12-21 14:56:32 +01:00 |
|
Martin Diehl
|
8832c04dd0
|
more sanity checks
number of arguments for values per system needs to match the number of
systems that are defined
|
2018-12-21 11:52:23 +01:00 |
|
Martin Diehl
|
3f3e23c2c8
|
polished addAttribute and use it to store meta data
|
2018-12-17 16:15:16 +01:00 |
|
Martin Diehl
|
4dd064a275
|
polishing
|
2018-12-14 09:23:52 +01:00 |
|
Martin Diehl
|
2aa6b12126
|
IMPORTANT Behavior change: Slip (Lp) happens in twinned volume fraction
aliases for associate do not have to be defined
|
2018-12-12 16:13:57 +01:00 |
|
Martin Diehl
|
fd2d4d856b
|
cleaned + suggested structure to write data
|
2018-12-12 07:45:20 +01:00 |
|
Martin Diehl
|
cb28d10d79
|
dummy structure to write plasticity results
|
2018-12-12 06:40:57 +01:00 |
|
Martin Diehl
|
cf4a0a69fd
|
Intel compiler detected use of unallocated variable
bug was in for a while
|
2018-11-26 09:15:44 +01:00 |
|
Martin Diehl
|
7cc2892e64
|
no need to calculate twinned volume fraction as state
|
2018-11-25 16:14:46 +01:00 |
|
Martin Diehl
|
8a253856f1
|
no need to perform the state integration
|
2018-11-25 15:38:14 +01:00 |
|
Martin Diehl
|
1808b37357
|
can be easily computed during postprocessing
|
2018-11-25 11:17:12 +01:00 |
|
Martin Diehl
|
7ac96bd630
|
polishing
|
2018-10-17 00:01:21 +02:00 |
|
Martin Diehl
|
be8d7e19fe
|
missing use statement caused compilation error
|
2018-10-15 22:38:34 +02:00 |
|
Martin Diehl
|
ad1a64c338
|
rename was missing
|
2018-10-15 06:01:38 +02:00 |
|
Martin Diehl
|
767ca0edd4
|
avoid code repetition
|
2018-10-14 20:16:30 +02:00 |
|
Martin Diehl
|
6599aa487c
|
kinetics_slip does not seem to be the problem
|
2018-10-14 15:53:24 +02:00 |
|
Martin Diehl
|
4c780226d1
|
polishing
|
2018-10-14 09:27:34 +02:00 |
|
Martin Diehl
|
513faa2218
|
investigating the reason for the poor performance
|
2018-10-13 11:29:07 +02:00 |
|
Martin Diehl
|
0e17b17b90
|
using full precision
|
2018-10-07 18:40:02 +02:00 |
|
Martin Diehl
|
3a2f86df1c
|
non-schmid is always bcc
|
2018-10-05 23:04:06 +02:00 |
|
Martin Diehl
|
2a51e528bd
|
Merge branch 'development' into 44-column-major-access-to-interaction-matrices
|
2018-10-05 11:11:20 +02:00 |
|
Martin Diehl
|
47a748831f
|
Cannot write out resolved stress including non schmid
Would need to write out tau_pos and tau_neg separately, so limit to
resolved stress in the sense of Schmid
|
2018-10-05 07:26:13 +02:00 |
|
Martin Diehl
|
6ccbc5e4e6
|
characteristing shear is defined per system
|
2018-10-05 07:20:51 +02:00 |
|
Martin Diehl
|
e74a852ef7
|
new style is noticable slower
runtime (polycrystal example) increased from 70s to 90s.
Need to figure out how to write readable AND fast code
|
2018-10-05 06:38:20 +02:00 |
|
Martin Diehl
|
3a00fcde16
|
WIP: characteristic shear calculated in lattice
|
2018-10-05 05:09:31 +02:00 |
|
Martin Diehl
|
fda2676365
|
calculate only if required
|
2018-10-05 04:54:47 +02:00 |
|
Martin Diehl
|
79b0efc678
|
also using nonSchmid matrix from lattice
|
2018-10-04 21:20:42 +02:00 |
|
Martin Diehl
|
35956ce0c8
|
needs to be multiplikative
|
2018-10-04 21:06:57 +02:00 |