0cddf36106
typo, using value of p_slip for q
2018-10-05 17:47:46 +02:00
2a51e528bd
Merge branch 'development' into 44-column-major-access-to-interaction-matrices
2018-10-05 11:11:20 +02:00
40cf7f134d
Merge branch '44-column-major-access-to-interaction-matrices' of magit1.mpie.de:damask/DAMASK into 44-column-major-access-to-interaction-matrices
2018-10-05 11:08:29 +02:00
aa34b83978
avoid array out of bounds
...
allows to handle un- or partly defined non schmid coefficients
2018-10-05 10:36:44 +02:00
a560fff2ac
[skip ci] [skip sc] generic interfaces for HDF5 operations
...
most existing HDF5 functions are only designed for writing output files
and more general functionality is needed for storing the restart data
2018-10-05 09:03:20 +02:00
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
6ccbc5e4e6
characteristing shear is defined per system
2018-10-05 07:20:51 +02:00
e74a852ef7
new style is noticable slower
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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
3a00fcde16
WIP: characteristic shear calculated in lattice
2018-10-05 05:09:31 +02:00
fda2676365
calculate only if required
2018-10-05 04:54:47 +02:00
79b0efc678
also using nonSchmid matrix from lattice
2018-10-04 21:20:42 +02:00
35956ce0c8
needs to be multiplikative
2018-10-04 21:06:57 +02:00
a6ebdfc1ff
Reading and writing not very efficient method
2018-10-04 17:00:24 +02:00
edb94b8bc9
using the same kinetics for slip everywhere
2018-10-04 16:12:14 +02:00
12d053d123
strange parameter caused simulation not to start if not defined
...
probably a leftover. now only bothers you if twin systems are defined
2018-10-04 14:54:00 +02:00
f1750b4eef
avoiding use of unitialized arrays
2018-10-04 14:51:32 +02:00
cd7f285686
prevent use of unallocated array
...
interaction matrices are used even if no slip/twin systems defined
2018-10-04 07:17:00 +02:00
dc289a278b
clearer code
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homogenization is defined per element, not per IP
hence, use material_homogenizationAt instead of deprecated
material_homog which pretends a dependency on the integration point
2018-10-04 06:48:33 +02:00
df473302f4
consistent (and better understandable) names
2018-10-04 06:03:48 +02:00
f494803c76
fixed tangent calculation
2018-10-03 16:40:40 +02:00
ec77d4450b
checking for required things
2018-10-03 09:17:06 +02:00
db645efda7
function to calculate nonSchmid matrix
2018-10-03 08:49:23 +02:00
103b46ecbb
don't repeate code over different plastic_xxx modules
2018-10-03 07:58:02 +02:00
89e03be699
also building interactions for slip-twin and twin-slip
2018-10-03 07:51:11 +02:00
0cac6ce0d2
allocating to wrong size
2018-10-03 07:36:57 +02:00
ba383336f5
only one projection matrix required for all (non)schmid projections
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following the example from plastic_nonlocal
2018-10-03 07:23:18 +02:00
d718521890
polishing
2018-10-03 07:13:30 +02:00
67c55965e9
segmentation fault, tried LHS with scalar
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Nxx per system is stored in LATTICE_yyy_NxxxSYSTEM
Using CAPITALS for parameters improves readbility
2018-10-03 06:45:42 +02:00
97d2c2b353
mesh_element(1) has a size of 4
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fixed sigsegv
2018-10-02 22:54:44 +02:00
014c7894bf
Merge branch 'development' into 29-rename-mesh_element-array
2018-10-02 20:38:19 +02:00
740325165d
Merge branch 'development' into 20-NewStyleDislotwin
2018-10-02 20:37:11 +02:00
64a160eaab
[skip ci] Merge branch 'master' into development
2018-10-02 18:15:05 +02:00
3394d39c44
Merge commit 'v2.0.2-701-g7ac6a5e7'
2018-10-02 18:14:32 +02:00
7ac6a5e739
[skip ci] updated version information after successful test of v2.0.2-700-g27bde055
2018-10-02 18:14:32 +02:00
0047e6c14c
correct calculation of dGdot_dTau
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needs to take drag coefficient into account for the derivative
2018-10-02 18:09:57 +02:00
9cc3a77e01
mean velocity of dislocation corrected for higher temperatures
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- v_wait: obstacle spacing over waiting time (effective velocity)
- v_run: 'true' velocity of a dislocation moving between obstacles
for higher temperatures v_run becomes important and bounds the velocity
2018-10-02 15:56:18 +02:00
5d1e648d17
drag coefficient B introduced and read in
2018-10-02 15:25:40 +02:00
7ac07f3d99
[skip ci] Merge branch 'master' into development
2018-10-02 02:53:39 +02:00
b59b6523b4
[skip ci] updated version information after successful test of v2.0.2-638-gd5cf7d21
2018-10-02 02:53:01 +02:00
384a785805
more sevice functions use
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still trying
2018-10-01 23:02:31 +02:00
ff2614b757
using 'service functions' from lattice
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get rid of many global array on the long run
2018-10-01 22:48:14 +02:00
a943940760
Merge branch 'development' into 44-column-major-access-to-interaction-matrices
2018-10-01 22:32:38 +02:00
98296a978e
Merge branch 'development' into 29-rename-mesh_element-array
2018-10-01 22:29:31 +02:00
e7b8adadd0
passing in instance and of is much easier
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also using always the full Mandel stress tensor to avoid repeated
conversion
2018-10-01 22:14:54 +02:00
ddfbe19f02
Merge branch 'development' into 20-NewStyleDislotwin
2018-10-01 21:16:11 +02:00
27bde05529
Merge branch '38-introduce-rudimentary-PETSc-based-FEM-solver' into 'development'
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Resolve "Introduce Rudimentary PETSc based FEM solver"
Closes #38
See merge request damask/DAMASK!41
2018-10-01 21:10:03 +02:00
d5cf7d2144
Merge branch '19-NewStylePhenopowerlaw' into 'development'
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Resolve "New coding style for phenopowerlaw"
See merge request damask/DAMASK!39
2018-10-01 16:08:05 +02:00
bd882bb39e
[skip ci] updated version information after successful test of v2.0.2-591-ga00d15b8
2018-09-30 00:12:50 +02:00
a00d15b889
geom files are not labeled
2018-09-29 11:18:35 +02:00
49a4202e26
not needed here
2018-09-29 10:31:45 +02:00
Martin Diehl