f68f4c6edf
marked wrong entries as unused
2024-01-17 12:45:17 +01:00
68d5acc645
PETSc options can be defined for every field solver
2024-01-02 14:46:35 +01:00
bd0eb0f154
load -> yaml
2023-12-18 17:23:05 +01:00
7fc09d3413
adjusted to current situation
2023-12-07 13:30:20 +01:00
5c87435f1a
small examples for testing purposes
2023-12-07 13:29:10 +01:00
255017d5be
examples are too large and don't compile
2023-12-07 13:06:41 +01:00
80c6823777
new temperature-dependent elastic constants
2023-10-30 00:40:41 +01:00
4de21b5f86
more systematic name
2023-09-15 00:28:40 +02:00
af955df891
added phi_min back to example; more consistency in code syntax
2023-09-06 15:11:48 -04:00
925da8aad4
Merge remote-tracking branch 'origin/numerics-comment-format' into restructure-numerics
2023-09-06 20:14:58 +02:00
2434c322ca
more sensible sorting of sections; additional polish
2023-09-05 13:14:20 -04:00
8399a11703
more extensive numerics.yaml documentation
2023-09-04 11:39:45 -04:00
09f3b2063d
Merge remote-tracking branch 'origin/development' into restructure-numerics
2023-08-17 12:09:10 +02:00
e161ef40b3
per-family parameters for kinehardening
2023-08-11 10:36:03 -04:00
81d0002a49
corrected remaining instances of phenopowerlaw configuration
2023-08-05 11:50:03 -04:00
ffdf478b62
all parameters as slip family-dependent
2023-08-04 13:07:42 -04:00
ac63ee3600
marc and other minor changes
2023-08-02 14:18:54 +02:00
482ba98b18
mesh numerics changes
2023-08-02 13:28:50 +02:00
485839b651
consistent names
2023-08-01 18:03:00 +02:00
4191762a41
seems redundant
2023-08-01 11:07:07 +02:00
6b85ee47d4
new names
2023-08-01 10:49:43 +02:00
a113492600
example file updated
2023-07-28 11:21:27 +02:00
af2a4c6e72
more readable
2023-07-26 16:32:47 +02:00
2547d4a25c
clear names
2023-07-25 23:04:29 +02:00
c4134f2358
updated examples
2023-07-25 11:04:38 +02:00
8117e9f54c
correct hierarchy
2023-07-17 19:07:03 +02:00
9651f3e486
examples follow current implementation
...
small polishing/consistent capitalization
2023-07-17 18:03:31 +02:00
96de1abc04
forest projection of both edge and screw character with adjustment parameter f_edge
2023-06-22 14:16:27 -04:00
289765cae3
better values and documentation
2023-04-28 00:39:52 +02:00
eeb0825e63
adjusting to original publication
...
Our implementation is using synonymous names for parameters compared to the paper by J.A. Wollmershauser, B. Clausen, and S.R. Agnew.
'xi_inf' and 'chi_inf' are not strictly "asymptotic values", but stresses that correspond to the back-extrapolation from the terminal linear hardening stage (characterized by 'h_inf_xi/chi').
All parameters are referenced back to their counterparts in the paper by J.A. Wollmershauser, B. Clausen, and S.R. Agnew.
2023-03-31 17:54:25 +00:00
13630325c3
notation following paper
...
https://doi.org/10.1016/j.jmps.2016.10.012
DAMASK paper
2023-03-13 17:23:28 +01:00
e5b7ad335f
debug.yaml causes more work than it saves
2023-02-13 22:26:58 +01:00
f427b85967
re-fit for new phenopowerlaw formulation
2023-01-23 21:51:08 +01:00
1174e94486
re-fit
...
- new phenopowerlaw formulation for hardening
- physics-based interactions (scaled DDD results such that
self-hardening is 1.0)
2023-01-15 01:34:30 +01:00
6c1edaeaac
new data for Aluminum
2023-01-15 01:33:50 +01:00
695d78eb35
have EOL and EOF
2023-01-08 14:32:13 +01:00
47e29f47fb
re-fit
...
using higher order polynomial where appropriate. Code for fitting in
"parameters" repository
2023-01-08 14:31:54 +01:00
976cfd501a
thermal expansion coefficients for SiC
...
this material was the initial motivation for adding fourth order
polynomials, but I could not find a reliable source for the graphs send
to damask@mpie.de . It seems that the CTE levels off for even higher
temperature which calls for a higher order polynomial
2023-01-08 14:31:43 +01:00
eb74d5a097
polishing
2023-01-08 11:54:42 +01:00
64fbfbb206
re-fit with correct conversion between Celsius and Kelvin
...
procedure is documented in the 'parameters' repository
2023-01-08 10:58:01 +01:00
b9195a121f
commonly used scaling
2023-01-08 10:57:36 +01:00
1711bf3220
re-fit using correct scaling
...
code is in 'parameters' repository
2023-01-08 10:57:06 +01:00
81870a6111
re-fit data
...
some small adjustments, procedure is now reproducible using "parameters"
repository
2023-01-08 00:25:43 +01:00
8d9df30090
legacy example
...
- undocumented
- not atomic
2023-01-07 22:01:03 +01:00
cca5d6d495
impoved naming
2022-12-09 06:48:16 +01:00
9d71ffa3ee
better naming
2022-11-24 11:23:10 +01:00
ef435ee7d1
commonly used variable name
2022-11-20 09:40:15 +01:00
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
Martin Diehl