Commit Graph

9535 Commits

Author SHA1 Message Date
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
Vitesh Shah a6ebdfc1ff Reading and writing not very efficient method 2018-10-04 17:00:24 +02:00
Martin Diehl edb94b8bc9 using the same kinetics for slip everywhere 2018-10-04 16:12:14 +02:00
Martin Diehl 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
Martin Diehl f1750b4eef avoiding use of unitialized arrays 2018-10-04 14:51:32 +02:00
Martin Diehl 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
Martin Diehl dc289a278b clearer code
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
Martin Diehl df473302f4 consistent (and better understandable) names 2018-10-04 06:03:48 +02:00
Martin Diehl f494803c76 fixed tangent calculation 2018-10-03 16:40:40 +02:00
Martin Diehl ec77d4450b checking for required things 2018-10-03 09:17:06 +02:00
Martin Diehl db645efda7 function to calculate nonSchmid matrix 2018-10-03 08:49:23 +02:00
Martin Diehl 103b46ecbb don't repeate code over different plastic_xxx modules 2018-10-03 07:58:02 +02:00
Martin Diehl 89e03be699 also building interactions for slip-twin and twin-slip 2018-10-03 07:51:11 +02:00
Martin Diehl 0cac6ce0d2 allocating to wrong size 2018-10-03 07:36:57 +02:00
Martin Diehl ba383336f5 only one projection matrix required for all (non)schmid projections
following the example from plastic_nonlocal
2018-10-03 07:23:18 +02:00
Martin Diehl d718521890 polishing 2018-10-03 07:13:30 +02:00
Martin Diehl 67c55965e9 segmentation fault, tried LHS with scalar
Nxx per system is stored in LATTICE_yyy_NxxxSYSTEM
Using CAPITALS for parameters improves readbility
2018-10-03 06:45:42 +02:00
Martin Diehl 97d2c2b353 mesh_element(1) has a size of 4
fixed sigsegv
2018-10-02 22:54:44 +02:00
Martin Diehl 014c7894bf Merge branch 'development' into 29-rename-mesh_element-array 2018-10-02 20:38:19 +02:00
Martin Diehl 740325165d Merge branch 'development' into 20-NewStyleDislotwin 2018-10-02 20:37:11 +02:00
Test User 64a160eaab [skip ci] Merge branch 'master' into development 2018-10-02 18:15:05 +02:00
Test User 3394d39c44 Merge commit 'v2.0.2-701-g7ac6a5e7' 2018-10-02 18:14:32 +02:00
Test User 7ac6a5e739 [skip ci] updated version information after successful test of v2.0.2-700-g27bde055 2018-10-02 18:14:32 +02:00
Martin Diehl 0047e6c14c correct calculation of dGdot_dTau
needs to take drag coefficient into account for the derivative
2018-10-02 18:09:57 +02:00
Martin Diehl 9cc3a77e01 mean velocity of dislocation corrected for higher temperatures
- 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
Martin Diehl 5d1e648d17 drag coefficient B introduced and read in 2018-10-02 15:25:40 +02:00
Test User 7ac07f3d99 [skip ci] Merge branch 'master' into development 2018-10-02 02:53:39 +02:00
Test User b59b6523b4 [skip ci] updated version information after successful test of v2.0.2-638-gd5cf7d21 2018-10-02 02:53:01 +02:00
Martin Diehl 384a785805 more sevice functions use
still trying
2018-10-01 23:02:31 +02:00
Martin Diehl ff2614b757 using 'service functions' from lattice
get rid of many global array on the long run
2018-10-01 22:48:14 +02:00
Martin Diehl a943940760 Merge branch 'development' into 44-column-major-access-to-interaction-matrices 2018-10-01 22:32:38 +02:00
Martin Diehl 98296a978e Merge branch 'development' into 29-rename-mesh_element-array 2018-10-01 22:29:31 +02:00
Martin Diehl e7b8adadd0 passing in instance and of is much easier
also using always the full Mandel stress tensor to avoid repeated
conversion
2018-10-01 22:14:54 +02:00
Martin Diehl ddfbe19f02 Merge branch 'development' into 20-NewStyleDislotwin 2018-10-01 21:16:11 +02:00
Martin Diehl 27bde05529 Merge branch '38-introduce-rudimentary-PETSc-based-FEM-solver' into 'development'
Resolve "Introduce Rudimentary PETSc based FEM solver"

Closes #38

See merge request damask/DAMASK!41
2018-10-01 21:10:03 +02:00
Franz Roters d5cf7d2144 Merge branch '19-NewStylePhenopowerlaw' into 'development'
Resolve "New coding style for phenopowerlaw"

See merge request damask/DAMASK!39
2018-10-01 16:08:05 +02:00
Test User bd882bb39e [skip ci] updated version information after successful test of v2.0.2-591-ga00d15b8 2018-09-30 00:12:50 +02:00
Martin Diehl a00d15b889 geom files are not labeled 2018-09-29 11:18:35 +02:00
Martin Diehl 49a4202e26 not needed here 2018-09-29 10:31:45 +02:00
Martin Diehl 14509876d4 error == 0 is normal termination 2018-09-29 09:57:53 +02:00
Test User bdc0051c19 [skip ci] Merge branch 'master' into development 2018-09-29 00:50:15 +02:00
Test User 813b22da49 Merge commit 'v2.0.2-584-g56c7b2e4' 2018-09-29 00:49:44 +02:00
Test User 56c7b2e433 [skip ci] updated version information after successful test of v2.0.2-583-gb391ad30 2018-09-29 00:49:43 +02:00
Martin Diehl 637544509e rewind needed
the file is read twice from beginning to end
2018-09-28 10:06:21 +02:00
Vitesh Shah 8619b49e20 made it nonexecutable 2018-09-28 08:47:00 +02:00
Vitesh Shah 8bd0cb3b25 Made it non executable 2018-09-28 08:45:52 +02:00
Vitesh Shah 6efde5f4ce Combined the dataset creation and writing dataset in single subroutine. Created group for looped writing. 2018-09-28 08:41:29 +02:00
Martin Diehl b141252f1f doing the same things in the same way in both solvers 2018-09-28 08:06:22 +02:00