Martin Diehl
|
8af0c8dbc3
|
using initial temperature from load case file
|
2021-02-28 21:51:07 +01:00 |
|
Sharan Roongta
|
9679c5403e
|
continue with cell based map (solver + homog)
|
2021-02-23 15:44:58 +01:00 |
|
Sharan Roongta
|
e249168189
|
modifying storing of orientations;
needed for nonlocal, and also to remove the use if ip,el at homogenization level.
ip, el should be used only for looping eventually.
|
2021-02-22 20:38:49 +01:00 |
|
Martin Diehl
|
e855083964
|
systematic names
|
2021-02-11 14:19:04 +01:00 |
|
Martin Diehl
|
0d3b9b9f2a
|
correct reporting
|
2021-01-27 10:44:03 +01:00 |
|
Martin Diehl
|
69f6de0e4f
|
consistent access pattern and naming
|
2021-01-26 23:44:11 +01:00 |
|
Martin Diehl
|
17ec5f378e
|
short names
|
2021-01-26 20:30:47 +01:00 |
|
Martin Diehl
|
26c7969837
|
not needed anymore
|
2021-01-24 17:12:34 +01:00 |
|
Martin Diehl
|
599dc2a2c6
|
base HDF5 output on new data
|
2021-01-24 16:34:51 +01:00 |
|
Martin Diehl
|
c2ae2c919b
|
use new structure
|
2021-01-24 15:19:57 +01:00 |
|
Martin Diehl
|
e22d76be9e
|
using new structure for thermal
|
2021-01-24 13:26:01 +01:00 |
|
Martin Diehl
|
a933fe57e7
|
data structures for storing T at the homogenization level
similar to thermal_conduction, better than homogenization_T
|
2021-01-24 12:15:18 +01:00 |
|
Martin Diehl
|
9a7017484d
|
wrapper for homogenization of temperature rate
|
2021-01-17 15:10:43 +01:00 |
|
Martin Diehl
|
833d25420b
|
using new mapping
discrimination of integration point and element makes only sense for the
solver
|
2021-01-17 14:52:52 +01:00 |
|
Martin Diehl
|
ca5409f0f1
|
similar structure as for mechanics
|
2021-01-17 13:20:17 +01:00 |
|
Martin Diehl
|
27f4e4ce2a
|
separate state for thermal
|
2021-01-07 22:23:13 +01:00 |
|
Martin Diehl
|
0dac5f84ef
|
dummy data layout
|
2020-12-30 12:00:47 +01:00 |