Commit Graph

1277 Commits

Author SHA1 Message Date
Philip Eisenlohr 0a292d8d8b fixed final bug in hex twintwin matrix 2013-10-15 22:02:39 +00:00
Franz Roters 4d184b1ee4 improved comments 2013-10-14 14:35:41 +00:00
Martin Diehl 295d0cd28e removed a bunch of dummy functions (delta state for all constitutive_XXX except nonlocal, microstructure for none, j2 and phenopowerla), additional simplifications for none, averageBurgers is only relevant for RGC 2013-10-14 10:54:45 +00:00
Martin Diehl 029502c12e fixed typo causing compilation error 2013-10-14 06:11:50 +00:00
Martin Diehl b651f334fe set useful default values to remove dummy functions in individual homogenization schemes (stateInit, averageTemperature, and updateState (isostrain only)) 2013-10-11 16:01:53 +00:00
Franz Roters 80cb78c1fd corrected activation of slipbands; both velocity and resistance have to be non zero 2013-10-11 13:52:00 +00:00
Martin Diehl 3b5a5ab812 changed error in case of number of found interaction types is less than expected to warning 2013-10-11 09:17:03 +00:00
Martin Diehl bb0b35e466 made compilation_info.f90 windows compatible and added abaqus_v6_windows.env as a template for using DAMASK with windows.
Deleted old fftw and ACML installation instruction (can be found on damask.mpie.de)
2013-10-10 09:38:31 +00:00
Martin Diehl ed47d25adc remove dotTemperature (returned always 0 anyway) to make it easier to replace it with a heating rate funtction
remove potentially dangerous short circuiting in homogenization files
added doxygen comment for nonlocal (giving the functions a name)
fixed wrong definition of maxnchungs introcuded into dislotwin with last commit, causes trouble with hex
2013-10-09 06:12:16 +00:00
Martin Diehl 82faf74363 added doxygen documentation and unified variable names and some common parts of the code 2013-10-08 16:27:26 +00:00
Philip Eisenlohr 0a7052a7da fixed two errors in hexagonal slipslip and twintwin interaction matrix 2013-10-08 13:52:19 +00:00
Philip Eisenlohr 42cd4eb38f fixed some e12.6 string formats to avoid compile time warnings 2013-10-08 13:51:36 +00:00
Philip Eisenlohr a2169e338f fixed type-casting problems (mainly with Lib_VTK_IO) 2013-09-26 17:21:46 +00:00
Martin Diehl ca2a8d0a03 fixed typos in Abaqus related functions 2013-09-23 09:01:46 +00:00
Martin Diehl 595c8860a2 renamed myInstance -> matID, myStructure -> structID to be consistent with other constitutive models 2013-09-20 17:03:11 +00:00
Martin Diehl ad32aa3ced fixed calculation of CurlRMS when grid(1)==1 2013-09-20 16:17:25 +00:00
Martin Diehl a0f304021f fixed restarting for Polarisation and AL, updated corresponding test and polished output in python (some statements are screwed up when making them Python3 compatible) 2013-09-20 14:22:37 +00:00
Martin Diehl 40c399bf2e fixed bug in last commit and remove one more goto marker 2013-09-19 15:28:55 +00:00
David Mercier ce926aaf1f Minor contribution :
- add SVN keyword to the material.config file for cp-Ti
- add comments in lattice file
2013-09-19 09:17:09 +00:00
Martin Diehl ca0b3b7b81 changed name of some variables to be in accordance with constitutive_none,j2,phenopowerlaw 2013-09-19 07:46:01 +00:00
Martin Diehl 70c888f6ea fixed a typo in documentation 2013-09-18 19:54:39 +00:00
Martin Diehl 56d21286a6 fixed comment on values changed automatically 2013-09-18 14:33:40 +00:00
Martin Diehl 3eec0ecdcd introduced #EOF# as module wide parameter in IO.f90
renamed read/write binary file to read/write real/int
removed suffix job from readFile functions as the name of the model is needed as an argument
2013-09-18 14:07:55 +00:00
Martin Diehl 19a353edb4 made error in case of invalid precision more verbose 2013-09-18 13:59:42 +00:00
David Mercier a8eb6a985e - Addition of an example of a material.config file for hcp material (cp-Ti).
- New Error Message #214 when elastic constants are not correctly defined.
- Error message when the c/a ratio for hcp is higher than 2 (no physical sense).
2013-09-17 12:20:50 +00:00
Martin Diehl cb16b30409 set output order of spectral parameters to more reasonable one 2013-09-17 09:19:16 +00:00
Martin Diehl 3bf0ed84c8 some comments and minor improvements.
removed tol_gravityNodePos from prec because it's not used
tol_math_check is now used by spectral driver to check rotation
2013-09-14 10:59:35 +00:00
Christoph Kords 5f973a21c0 require all hardening coefficients/ non schmid coefficients to be specified in material.config, do not silently ignore any
warning message now more meaningful (?) when using less than maximum number of slip families
2013-09-12 14:47:09 +00:00
Martin Diehl ddfc40afe6 improve restart test, deletion of results was messed up. fixed restart for BasicPETSc, AL and Polarization currently don't run when restarting 2013-09-05 12:07:58 +00:00
Christoph Kords 4ebf46d2ac nonSchmidProjection was reset to zero each time during instance loop in init, so entries from previous instances got lost; fixed that 2013-08-23 13:53:03 +00:00
Christoph Kords 1f77594ca0 dislocation velocity was not correctly stored to state in last version 2013-08-21 13:54:36 +00:00
Christoph Kords 4f8664baa3 in kinetics: non schmid stresses only influence peierls mechanism, but not solid solution hardening; as a result the derivative of the velocity with respect to the resolved stress has to be split into a Schmid and a non-Schmid part 2013-08-21 12:21:52 +00:00
Christoph Kords ec377a6e8e removed obsolete "dead zone" scaling 2013-08-21 08:39:43 +00:00
Christoph Kords f706ba3ff9 rearranged arguments of "constitutive_nonlocal_kinetics", got "tauTreshold" as argument, not complete state
don't call "constitutive_nonlocal_kinetics" twice for edges in case of nonSchmid behavior, but just call once and copy results from positive to negative edges
2013-08-21 07:55:34 +00:00
Christoph Kords 277972edbd "dv_dtau" argument in "constitutive_nonlocal_kinetics" not optional anymore
renamed "screwStressProjection" to "nonSchmidProjection"
2013-08-21 07:23:02 +00:00
Christoph Kords 39c05e0d9e for bcc: exchanged 2nd and third hardening coefficient to be consistent with fcc; now 2nd is coplanar and 3rd is collinear; added newer reference concerning the bcc hardening coefficients 2013-08-14 11:47:03 +00:00
Christoph Kords e909b825cc correction of hardening coefficients also enabled for bcc
for fcc: now applied to all hardening coefficients, not only hirth, lomer, and glissile
2013-08-14 11:44:30 +00:00
Martin Diehl b8d5f3124f added citation on phenopowerlaw aluminum parameters 2013-08-09 21:24:42 +00:00
Pratheek Shanthraj e62b760a6e added F_avg = F_aim in boundary condition convergence check 2013-08-09 16:25:13 +00:00
Martin Diehl 822fa3d97c forgotten line continuation 2013-08-09 04:16:16 +00:00
Martin Diehl c93373a4ac removed long lines 2013-08-08 19:33:21 +00:00
Martin Diehl 3bb5a5e7b5 line too long in DAMASK_spectral_solverPolarisation.f90, reordered curl calculation for clearer look, fixed test for Marc 2013 2013-08-08 18:10:58 +00:00
Franz Roters 591a3023e8 made plain mode work with Abaqus
ATTENTION plain mode (Marc and Avaqus) does not support writung out the deformed geometries
2013-08-08 15:00:22 +00:00
Christoph Kords 3fcc00910c fixed bug that occured under marc (and abaqus?) with openmp:
"lastLovl" (for marc) and "lastStep" (for abaqus) have to be global module variables in FEsolving.f90 instead of local variables in the respective DAMASK_* files; otherwise they are initialized with zero each time hypela2/umat is called.
2013-08-08 12:53:03 +00:00
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