2f7efa2055
introduced named constants for homogenization_type, phase_plasticitiy, and phase_elasticity to replace expensive string comparison. Labels for different schemes need to be stored in material.f90 because they are needed when parsing the config file
2013-11-27 08:04:05 +00:00
c9ce8d2c52
some improvements on HDF5 test, polishing math
2013-11-22 10:31:52 +00:00
e8de8f69a8
renaming of "maxNinstance" to be consistent with naming scheme introduced in rev2662
2013-11-21 13:40:14 +00:00
3cc6781eaf
renaming of "instance" and thelike to be consistent with naming scheme introduced in rev2662
2013-11-21 13:35:43 +00:00
883669bd77
in preguess of FPintegrator: resetting of previous dotstates can be done in same loop as collectdotstate
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polishing: indentation level and capitalization
2013-11-21 10:58:41 +00:00
9083aa53fb
fixed long lines due to makro expansion
2013-11-19 16:06:53 +00:00
9c34c1b871
error reporting for phase fields only if there are active phase fields
2013-11-14 10:36:49 +00:00
f51c600189
convergence check for phase field only if there are active phase fields
2013-11-14 10:32:41 +00:00
3b113f6a62
more errors :)
2013-11-13 19:38:25 +00:00
8444b4116d
corrected error in previous commit
2013-11-13 19:26:36 +00:00
50db944c0c
reworked phase field interface to damask spectral solvers. now specify 'thermal a b c' or 'fracture a b c' to activate either phase field where a b c are the initial value, diffusion coefficient and mobility respectively.
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Right now only thermal and fracture phase fields implemented and only in the basic petsc solver
2013-11-13 19:21:35 +00:00
724380c624
Coupled phase field implementation for the basic petsc solver. needs clearing up… work in progress
2013-11-12 00:44:23 +00:00
9ac8846e41
compiling with hdf5 is now working for DAMASK (if HDF5=ON) and for playground example in private
2013-11-07 12:52:36 +00:00
c857381881
added "-d", "--directory" as possible cmd switches for working directory.
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fixed (sometimes?) non-working check for valid working directory path.
2013-10-24 18:56:56 +00:00
ea980f428e
fixed long line coming from PETSc macro expansion
2013-10-23 17:52:58 +00:00
57cf472982
Improved convergence checking when using newton solver (does not oversolve the problem like before)
2013-10-23 15:22:12 +00:00
eb0d2b7e24
fixed bug that (sometimes, always?) prevented reading in of debug.config, when variable 'line' was still '#EOF#' from former IO_read...
2013-10-23 11:23:41 +00:00
bdafc6f1b8
condensed error msg numbering,
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introduced new error for "microstructure without any constituent"
2013-10-23 11:21:48 +00:00
205eb66ba8
bugfix for last commit, too many variables declared as private
2013-10-23 10:29:38 +00:00
96b03841e8
redefined macro for intel compiler, should work with windows (but Nicolo had some problems)
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made configure verbose
2013-10-23 08:38:14 +00:00
7b28dedfe3
removed temperature calculation and debugging statements
2013-10-22 15:52:58 +00:00
ea664688f8
introduced dummy temperature calculation.
2013-10-18 20:56:10 +00:00
3ecc8103f0
introduced dummy heat calculation, available as an crystallite output
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temperature, avgP and avgF are available as homogenization output. move crystallite output of ipcoordinates to homogenization
2013-10-18 18:57:28 +00:00
1c7ed337d7
corrected linebreak in comment
2013-10-17 12:52:46 +00:00
03e26af37b
small bufix, didn't compile
2013-10-16 20:44:04 +00:00
dc95c82d4a
removed temperature integration and corresponding data structures and debugging options
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temperature is stored in crystallite, but homogeneous on one IP (not an component (grain) quantity and an input value parsed in by the BVP solver.
introduced heat, a component (grain) quantity which is homogenized before returned to the heat transfer solver.
went ahead with removal of dummy functions in homogenization and constitutive, this time mainly reduced function signatures to reflect actually needed quantities.
2013-10-16 13:04:59 +00:00
6a1c40d540
introduced error when element/IP/component(grain) selected for debugging does not exist
2013-10-16 12:38:00 +00:00
0a292d8d8b
fixed final bug in hex twintwin matrix
2013-10-15 22:02:39 +00:00
4d184b1ee4
improved comments
2013-10-14 14:35:41 +00:00
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
029502c12e
fixed typo causing compilation error
2013-10-14 06:11:50 +00:00
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
80cb78c1fd
corrected activation of slipbands; both velocity and resistance have to be non zero
2013-10-11 13:52:00 +00:00
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
bb0b35e466
made compilation_info.f90 windows compatible and added abaqus_v6_windows.env as a template for using DAMASK with windows.
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Deleted old fftw and ACML installation instruction (can be found on damask.mpie.de)
2013-10-10 09:38:31 +00:00
ed47d25adc
remove dotTemperature (returned always 0 anyway) to make it easier to replace it with a heating rate funtction
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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
82faf74363
added doxygen documentation and unified variable names and some common parts of the code
2013-10-08 16:27:26 +00:00
0a7052a7da
fixed two errors in hexagonal slipslip and twintwin interaction matrix
2013-10-08 13:52:19 +00:00
42cd4eb38f
fixed some e12.6 string formats to avoid compile time warnings
2013-10-08 13:51:36 +00:00
a2169e338f
fixed type-casting problems (mainly with Lib_VTK_IO)
2013-09-26 17:21:46 +00:00
ca2a8d0a03
fixed typos in Abaqus related functions
2013-09-23 09:01:46 +00:00
595c8860a2
renamed myInstance -> matID, myStructure -> structID to be consistent with other constitutive models
2013-09-20 17:03:11 +00:00
ad32aa3ced
fixed calculation of CurlRMS when grid(1)==1
2013-09-20 16:17:25 +00:00
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
40c399bf2e
fixed bug in last commit and remove one more goto marker
2013-09-19 15:28:55 +00:00
ce926aaf1f
Minor contribution :
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- add SVN keyword to the material.config file for cp-Ti
- add comments in lattice file
2013-09-19 09:17:09 +00:00
ca0b3b7b81
changed name of some variables to be in accordance with constitutive_none,j2,phenopowerlaw
2013-09-19 07:46:01 +00:00
70c888f6ea
fixed a typo in documentation
2013-09-18 19:54:39 +00:00
56d21286a6
fixed comment on values changed automatically
2013-09-18 14:33:40 +00:00
3eec0ecdcd
introduced #EOF# as module wide parameter in IO.f90
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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
19a353edb4
made error in case of invalid precision more verbose
2013-09-18 13:59:42 +00:00
a8eb6a985e
- Addition of an example of a material.config file for hcp material (cp-Ti).
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- 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
cb16b30409
set output order of spectral parameters to more reasonable one
2013-09-17 09:19:16 +00:00
3bf0ed84c8
some comments and minor improvements.
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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
5f973a21c0
require all hardening coefficients/ non schmid coefficients to be specified in material.config, do not silently ignore any
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warning message now more meaningful (?) when using less than maximum number of slip families
2013-09-12 14:47:09 +00:00
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
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
1f77594ca0
dislocation velocity was not correctly stored to state in last version
2013-08-21 13:54:36 +00:00
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
ec377a6e8e
removed obsolete "dead zone" scaling
2013-08-21 08:39:43 +00:00
f706ba3ff9
rearranged arguments of "constitutive_nonlocal_kinetics", got "tauTreshold" as argument, not complete state
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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
277972edbd
"dv_dtau" argument in "constitutive_nonlocal_kinetics" not optional anymore
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renamed "screwStressProjection" to "nonSchmidProjection"
2013-08-21 07:23:02 +00:00
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
e909b825cc
correction of hardening coefficients also enabled for bcc
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for fcc: now applied to all hardening coefficients, not only hirth, lomer, and glissile
2013-08-14 11:44:30 +00:00
b8d5f3124f
added citation on phenopowerlaw aluminum parameters
2013-08-09 21:24:42 +00:00
e62b760a6e
added F_avg = F_aim in boundary condition convergence check
2013-08-09 16:25:13 +00:00
822fa3d97c
forgotten line continuation
2013-08-09 04:16:16 +00:00
c93373a4ac
removed long lines
2013-08-08 19:33:21 +00:00
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
591a3023e8
made plain mode work with Abaqus
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ATTENTION plain mode (Marc and Avaqus) does not support writung out the deformed geometries
2013-08-08 15:00:22 +00:00
3fcc00910c
fixed bug that occured under marc (and abaqus?) with openmp:
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"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
7f3c24e1f1
fixed some buggy last minute changes in the last commit
2013-08-08 09:13:29 +00:00
23e8fcbc51
updated config file with new convergence parameters
2013-08-08 09:12:12 +00:00
ac92b90e0b
fixed al and pol solver, now checking for div(p) = curl(f) = 0
2013-08-07 17:20:05 +00:00
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
813ed130b0
nonSchmid behavior now ready to use for bcc with phenopowerlaw and nonlocal constitutive model.
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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
9f0fe873ba
plain mode (no ping pong) now seems to work for marc, further testing needed
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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
fa3be9a967
corrected lastLovl introduced in rev2593
2013-08-02 15:44:28 +00:00
5b80ef3a4c
fixed wrong error calculation in Polarisation and AL solvers, and strictened tolerances for tests
2013-08-02 13:55:44 +00:00
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
74791a6686
corrected invalid error for mismatch_p
2013-08-02 11:48:24 +00:00
3d687be8b0
Changed order of blocks associated with different tasks:
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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
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
4f9dbfa193
last commit also solves problem with infinite loop in case of a cutback in homogenization
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corrected indentation of a comment
2013-08-02 07:59:55 +00:00
a08d263865
remnoved some unused fuctions from use statements
2013-08-02 06:18:41 +00:00
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
728facd451
corrected indentation level of parts of the code
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moved debugging output of stress and stiffness to different position in code
2013-08-01 16:10:56 +00:00
ac2ca43cfc
added svn properties
2013-08-01 09:13:46 +00:00
2dc985f558
set tolerances to useful values and renamed them.
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allowed "keyword = value" in numerics.config (simply removing "=" from line)
2013-07-31 15:03:38 +00:00
b5a11f9d31
fixed bug in AL, weakened correction slightly
2013-07-30 21:04:41 +00:00
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
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.
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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
216063fe36
added Polarisation scheme as solver
2013-07-24 13:06:16 +00:00
4f7cd76b29
renamed texture_rotation into texture_transformation
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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
f896b4a01e
updated Marc/Mentat integration once more to minimze interference with original instal
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added support for Marc2013, which is now default in apply_DAMASK_modifications
2013-07-24 08:41:58 +00:00
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
3749cd5564
changed "math_AxisAngleToR" to "math_axisAngleToR" to be consistent with spelling in math.f90
2013-07-22 09:43:35 +00:00
bbb0803ce4
itmin was always +1
2013-07-17 19:58:48 +00:00
74a7840a59
wrong intent(in) statement fixed
2013-07-15 10:13:28 +00:00
8210b14e90
comments for doxygen
2013-07-12 06:57:15 +00:00
Martin Diehl