Commit Graph

1233 Commits

Author SHA1 Message Date
Martin Diehl 7f3c24e1f1 fixed some buggy last minute changes in the last commit 2013-08-08 09:13:29 +00:00
Pratheek Shanthraj 23e8fcbc51 updated config file with new convergence parameters 2013-08-08 09:12:12 +00:00
Martin Diehl ac92b90e0b fixed al and pol solver, now checking for div(p) = curl(f) = 0 2013-08-07 17:20:05 +00:00
Christoph Kords f2d6703148 multiplication now sensitive of crystal structure, yet multiplication in bcc identical to fcc except for the contribution of edges which is completely dropped for bcc 2013-08-05 09:26:37 +00:00
Christoph Kords 813ed130b0 nonSchmid behavior now ready to use for bcc with phenopowerlaw and nonlocal constitutive model.
nonSchmid tensors according to Koester,Ma,Hartmaier,2012.
extended lattice_Sslip with non-Schmid tensors (the full non-symmetric tensors are required for the tangent and cannot be retrieved from the symmetrized Mandel notation)
2013-08-05 09:23:21 +00:00
Christoph Kords 9f0fe873ba plain mode (no ping pong) now seems to work for marc, further testing needed
regular sequence of computation modes is
inc 0: 1,1,1,…
inc 1: 0,0,0,…
          7,1,1,…
          0,0,0,…
          1,1,1,…
and so on

after a cutback the computation modes follow as
inc 5: 8,0,0,…
          1,1,1,…
          0,0,0,…
          1,1,1,…
2013-08-02 16:19:45 +00:00
Christoph Kords fa3be9a967 corrected lastLovl introduced in rev2593 2013-08-02 15:44:28 +00:00
Martin Diehl 5b80ef3a4c fixed wrong error calculation in Polarisation and AL solvers, and strictened tolerances for tests 2013-08-02 13:55:44 +00:00
Christoph Kords 8d6b840802 removed variable lastMode from FE_solving, used to be used for detection of first call after ping pong; now this is done by checking for a change in the lovl (macro) or a change in the calculation step (abaqus) 2013-08-02 13:28:50 +00:00
Martin Diehl 74791a6686 corrected invalid error for mismatch_p 2013-08-02 11:48:24 +00:00
Christoph Kords 3d687be8b0 Changed order of blocks associated with different tasks:
backup jacobian
restore jacobian
age results
collect 
calc
This becomes important if multiple tasks are requested by one call to CPFEM_general. In plain mode this could, e.g., be 
1) backup jaco, 2) age results, 3) calc
2013-08-02 11:36:51 +00:00
Christoph Kords 7d2206356e parallelExecution flag now passed as input variable by CPFEM_general; flag is set on the solver level (DAMASK_abaqus_exp.f, DAMASK_marc.f90, etc.) 2013-08-02 11:20:11 +00:00
Franz Roters 4f9dbfa193 last commit also solves problem with infinite loop in case of a cutback in homogenization
corrected indentation of a comment
2013-08-02 07:59:55 +00:00
Franz Roters a08d263865 remnoved some unused fuctions from use statements 2013-08-02 06:18:41 +00:00
Christoph Kords a7f0f4ed79 moved some small part of the code that remembers maximum and minimum stress/stiffness values to different location 2013-08-01 16:27:37 +00:00
Christoph Kords 728facd451 corrected indentation level of parts of the code
moved debugging output of stress and stiffness to different position in code
2013-08-01 16:10:56 +00:00
Martin Diehl ac2ca43cfc added svn properties 2013-08-01 09:13:46 +00:00
Martin Diehl 2dc985f558 set tolerances to useful values and renamed them.
allowed "keyword = value" in numerics.config (simply removing "=" from line)
2013-07-31 15:03:38 +00:00
Martin Diehl b5a11f9d31 fixed bug in AL, weakened correction slightly 2013-07-30 21:04:41 +00:00
Martin Diehl 81531097f1 changes on convergence tolerances of AL and Polarisation, switched back to immediate correction of stress bc but only when last two average stresses are close to each other (cosine decay) 2013-07-30 15:32:55 +00:00
Pratheek Shanthraj 03d8f14a98 introduced dynamics for high strain rate simulations. so far only works for materials with homogeneous density. the density is read in as an optional argument in the load file using the keyword 'den' or 'density'. if density > 0 then inertial terms are added to the stress equilibrium. an implicit euler time discretisation is used to calculate the inertial terms.
dynamic problems are length scale dependent so make sure the geometry size is meaningful (1 m^3 or N m^3 for example is too big for a RVE!).

not specifying a density (density = 0) will perform a quasi static simulation as before.
2013-07-26 16:25:37 +00:00
Martin Diehl 216063fe36 added Polarisation scheme as solver 2013-07-24 13:06:16 +00:00
Franz Roters 4f7cd76b29 renamed texture_rotation into texture_transformation
changed keyword for material.config to axes in line with geom_fromAng.py
former keyword rotation is still recognized for compatibility
2013-07-24 11:09:39 +00:00
Franz Roters f896b4a01e updated Marc/Mentat integration once more to minimze interference with original instal
added support for Marc2013, which is now default in apply_DAMASK_modifications
2013-07-24 08:41:58 +00:00
Martin Diehl ebe8361af0 decoupled compatibility/equilibrium calculation from stress BC correction. needs more iteration for mildly contrasted materials, but there the basic scheme is better suited anyway. but now converges better for highly contrasted VEs 2013-07-23 17:42:15 +00:00
Christoph Kords 3749cd5564 changed "math_AxisAngleToR" to "math_axisAngleToR" to be consistent with spelling in math.f90 2013-07-22 09:43:35 +00:00
Martin Diehl bbb0803ce4 itmin was always +1 2013-07-17 19:58:48 +00:00
Martin Diehl 74a7840a59 wrong intent(in) statement fixed 2013-07-15 10:13:28 +00:00
Martin Diehl 8210b14e90 comments for doxygen 2013-07-12 06:57:15 +00:00
Martin Diehl 4407edd802 checked convergence reporting for AL and BasicPETSc, seems to be ok now. 2013-07-08 15:48:13 +00:00
Martin Diehl 27c64ba4ad corrected line breaking for /echo/ tag 2013-07-08 09:46:38 +00:00
Franz Roters 1db24d2a72 removed duploicate writes
changed last occurences of old mode syntax
one more change in the direction of a plain mode, i.e. when there is no collect cycle
2013-07-04 11:59:45 +00:00
Pratheek Shanthraj 8f146ad385 fixed bug in cosine filter 2013-07-02 04:38:18 +00:00
Philip Eisenlohr 8ccdfb27f3 reworked the hexagonal slip system order and adjusted interaction matrices to a logic that facilitates later system additions without altering existing structure. 2013-07-01 14:01:42 +00:00
Franz Roters 4a291dc372 implementation of twin nucleation criteria according to Davids PhD thesis
applies for fcc crystal structure only
2013-07-01 13:06:01 +00:00
Martin Diehl 6ec57db0c6 fixed writing out of initial configuration for spectral solver in case of ngrains != 1, small formating improvements in other files 2013-07-01 06:40:09 +00:00
Martin Diehl 40ace5c666 more documentation and parameters capitalization unified and using ipc in all modules (sometimes called gr)
nonlocal: only missing line continuation in string fixed
2013-07-01 06:10:42 +00:00
Philip Eisenlohr f408ea3381 corrected error msg typos 2013-06-30 00:17:58 +00:00
Martin Diehl 5f20c86905 small documentation and output fixes 2013-06-28 18:59:21 +00:00
Martin Diehl ef2c2af471 doxygen documentation for J2 2013-06-28 18:58:10 +00:00
Philip Eisenlohr fd8d85896a error msg in case of unknown keyword was not properly trimmed --> 64kB of spaces... 2013-06-27 16:41:00 +00:00
Philip Eisenlohr f9f76fa158 missed these three files in last commit!
[added possibility for multi-level inclusion of files in *.config and loadcase files.
include subfiles by stating

{path/to/include}
]
2013-06-26 19:19:41 +00:00
Philip Eisenlohr 98528f9a89 added possibility for multi-level inclusion of files in *.config and loadcase files.
include subfiles by stating

{path/to/include}
2013-06-26 19:19:00 +00:00
Martin Diehl 0f1bb4f555 corrected doxygen documentation tags 2013-06-25 06:08:33 +00:00
Harsha Phukan aea8ab144a changed all file reads consistently to 65536 bytes length 2013-06-24 13:33:30 +00:00
Franz Roters 9a1ad7e089 added third value for slip twin interaction in fcc dislotwin example 2013-06-24 12:53:56 +00:00
Pratheek Shanthraj 7b2e48df68 new 'gradient' filter based on greens function from gradient elasticity theory. work in progress 2013-06-21 17:26:05 +00:00
Philip Eisenlohr 81cdd2b1cc added second type prismatic slip system for hexagonal lattices as 6th slip family.
consequently, 4 new interaction types (21,22,23,24) available for slip/twin and twin/slip.

interaction of slip/slip got rearranged and now has 42 types...
list of former --> new:
6	7
7	8
8	9
9	10
10	11
11	13
12	14
13	15
14	16
15	18
16	19
17	20
18	22
19	23
20	25
21	28
22	29
23	30
24	31
25	33
26	34
27	35
28	37
29	38
30	40
2013-06-14 10:20:31 +00:00
Franz Roters a78f91311e added svn properties: line ending: LF and keywords: ID 2013-06-14 09:49:33 +00:00
Pratheek Shanthraj 1c25403b5b changed default values of AL spectral solver tolerances. should've been done along with commit 2254. 2013-06-12 10:06:04 +00:00