28ea09050d
polishing
2022-10-25 23:18:22 +02:00
ff3e08531e
including test
2022-10-23 12:42:17 +02:00
0c83245d4b
example files for TWIP/TRIP
...
I'm not able to reproduce the results from https://doi.org/10.1016/j.actamat.2016.07.032 ,
but these parameters give results that are qualitatively ok
2022-09-22 16:39:23 +02:00
576c79a619
following DAMASK paper
2022-06-13 14:08:45 +02:00
9b94aca09f
new example file
2022-06-08 23:28:54 +02:00
b3992e0ff0
test new example files
2022-05-16 23:24:29 +02:00
37eb567451
dataset for Platinum
2022-05-13 11:10:02 +02:00
4d808335de
polishing
2022-02-12 18:55:01 +01:00
3bdfc29fb2
Parameter set for beta-Sn
2022-02-12 15:42:39 +01:00
0f0108f603
polishing
2022-01-09 08:14:31 +01:00
a884b99aa9
Merge remote-tracking branch 'origin/development' into physics-based-hex-interactions
2022-01-08 20:45:46 +01:00
4a0a1f7ac9
paper is online
2022-01-02 22:29:48 +01:00
d66b9e1896
subdivision of interaction matrix for hcp
2021-12-06 16:51:18 +01:00
fe2123bae4
2. order prismatic systems are not needed
...
not clear for which material they have been introduced, according to
T.R. Bieler and P. Eisenlohr they are typicall not active in any
material of interest
2021-12-06 12:23:24 +01:00
5ba59dead2
polish
2021-11-25 14:07:41 -05:00
97ffb8c88e
guide the user
...
+ needed for consistent indentation (make YAMLlint happy)
2021-11-24 20:02:08 +01:00
719996f285
trailing definitions not needed
2021-11-24 15:52:38 +01:00
56bc3bc71d
simplify counting, emphasize floating point values
2021-11-24 15:48:11 +01:00
2e3de727cc
hint at issues with the current parametrization
2021-11-02 07:27:08 +01:00
3f3224a9cb
found better source
2021-10-31 18:59:57 +01:00
737eff9179
bugfix: change of behavior
...
v_0 was erroneously introduced
use tau = (tau_pos+tau_neg)/2
2021-10-31 18:59:51 +01:00
a352f8deeb
reasonable convergence
2021-10-31 16:05:22 +01:00
fbc4865c30
mathematically equivalent re-formulation
...
allows to disable contribution from grain size by setting it to a large
value
2021-10-31 15:42:18 +01:00
25ca77c38e
parameters from original paper (mostly)
2021-10-31 13:34:48 +01:00
0107acff16
original data was given in min^-1
2021-08-14 13:12:21 +02:00
809365cd72
reference for 1.4/1
2021-08-14 13:01:37 +02:00
931dc99557
not used
...
climb formulation was updated a while ago
2021-07-24 11:21:07 +02:00
6f906647eb
documenting hex
2021-07-24 09:35:27 +02:00
6936ecb091
sl is the subscript for slip
2021-07-23 21:36:26 +02:00
c873123e6d
reference can now include comments!
2021-07-13 20:46:50 +02:00
562a84bc30
quick hack for YAML issue with :
2021-07-09 11:12:17 +02:00
6e4fe5b1c3
consistent citation style
...
should be used for Fortran, python, YAML
2021-07-08 16:56:41 +02:00
cd9d704aae
bug fixes:
...
invalid material.yaml, detect such errors in future
2021-07-05 11:30:52 +02:00
b465a6d615
new style examples
2021-07-05 05:38:47 +02:00
300431d2b0
correct conversion to float
2021-06-29 11:22:42 +02:00
4dcd249bf3
python YAML is too picky/following v1.1
...
https://stackoverflow.com/questions/30458977
2021-06-29 10:14:59 +02:00
b1f4c06f9c
takeover from Christophs thesis
2021-06-26 13:25:13 +02:00
62e5cab440
polishing example configurations
2021-06-25 15:25:35 +02:00
eddb65d796
should not be part of the repository
2021-06-24 11:43:55 +02:00
452da977b0
cleaning up example files
2021-06-24 08:55:44 +02:00
0a22916aba
not a double subscript
2021-06-19 15:13:27 +02:00
ab070a3c13
data for thermal expansion
2021-05-24 10:31:56 +02:00
16cba043c9
update BCC examples, old_coef=new_coef/ 1=1 - 2=3 - 3=2,8,9 - 4=4,5,10,11,12,13 - 5=7,20,23 - 6=6,14,15,16,17,18,19,21,22,24
2021-05-07 11:46:29 +02:00
2d50a5de7f
update examples FCC
2021-05-07 10:59:17 +02:00
3977e230b3
documenting and ensuring consistent argument names
...
'name' for a dataset matches the analogy to a file name
2021-04-24 14:47:45 +02:00
a2b2f8fb13
include latest results
2021-03-29 07:07:11 +02:00
33b601461b
modularizing further
...
steepens the learning curve. But ensures that ther IS a learning curve
2021-03-27 19:25:36 +01:00
cc72fad86a
split configuration per physics
2021-03-27 15:12:29 +01:00
Martin Diehl