Christoph Kords
875abcd06f
replaced some array assignments, which might have caused trouble when using the "timeSyncing" option, by parallelized loops of scalar value assignments
2013-02-27 16:36:12 +00:00
Christoph Kords
3736ab1d97
added shortcuts for two do loops in the "timesyncing" procedure
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math_pDecomposition enclosed by omp critical statement; somehow, this subroutine is not thread safe, not clear what exactly the problem is
2013-02-27 10:32:37 +00:00
Pratheek Shanthraj
07ff1f7c93
reporting current time for most module inits
2013-02-25 16:34:59 +00:00
Martin Diehl
393c60565d
one line was beyond 132 characters
2013-02-22 05:38:02 +00:00
Martin Diehl
42b96354db
doxygen comments
2013-02-21 23:08:36 +00:00
Martin Diehl
f0b4281400
removed unused variables, added pure statements, and declared external functions as external (using gfortrans debug option)
2013-02-11 10:43:45 +00:00
Martin Diehl
e74b5da19a
changed all remaining routines to fortran-fast arrays (geometry reconstruction etc.)
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changed all remaining routines in f2py to more clever determination of array size (requires f2py >= 2.0)
enabled 3D visualize to work with odd resolution by switching to linear reconstruction
PLEASE NOTE: Redefinition of routines for f2py might cause trouble -> DELETE DAMASK_ROOT/lib/damask/core.so in this case
further changes: added pure statement where possible, polished, unified use of "Q" for "Quaternion" and reordered math to have similar routines together
2013-01-31 16:28:08 +00:00
Martin Diehl
3ffd6499b1
change bash-only "let" to "`expr`", abaqus_v6.env now suppresses warnings about long lines (there are only comments anyway)
2013-01-28 15:30:51 +00:00
Pratheek Shanthraj
fd94c786f0
moved stiffness tensor calculation to lattice
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introduced 'isotropic' and 'orthorhombic' lattice types to use corresponding symmetries in stiffness tensor. intended to be used with non-crystal plasticity models (j2, constitutive_none with isotropic, cubic or orthotropic elasticity).
2013-01-21 21:57:26 +00:00
Christoph Kords
8a45a90775
new crystallite output "grainrotationX", "grainrotationY", "grainrotationZ" that gives the deviation of the initial orientation in degrees around the sample reference x/y/z axis, while "grainrotation" still gives the same as axis angle pair in crystal coordinates
2013-01-16 08:45:41 +00:00
Christoph Kords
7dd1130e92
reset syncSubFrac flag when turning terminallyIll
2012-12-16 16:18:36 +00:00
Christoph Kords
92d2c83334
more debugging info for timesyncing
2012-12-16 11:30:19 +00:00
Christoph Kords
4f12073dcb
once again corrected parallelization statements
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added some debugging writes for timesyncing
2012-12-16 10:54:13 +00:00
Christoph Kords
f744fc1d47
fixed bug in parallelization: flushing of crystallite_todo was missing at a couple of places
2012-12-11 15:05:08 +00:00
Christoph Kords
6a9b19e4c0
fixed bug in timesyncing procedure: if any ip that synchronizes its time step did not converge, all nonlocals become terminally ill; before, this led to an infinite loop in crystallite
2012-12-11 13:42:22 +00:00
Christoph Kords
35a0483507
fixed bug in last revision: FE_geomType was not in namespace
2012-12-10 17:22:16 +00:00
Philip Eisenlohr
10ed848258
fixed 2 bugs: missing mapping with FE_geomtype(mesh_element(2,...))
2012-12-10 17:03:28 +00:00
Christoph Kords
98d02dcffb
removed call to microstructure in stateJump function, since this is already done in the state integrator subroutine
2012-12-07 07:50:41 +00:00
Christoph Kords
0986a66449
accidentally also included some changes in crystallite_integrateStress in last commit; reverted these changes in this revision
2012-12-03 16:34:41 +00:00
Christoph Kords
f2dacb5f40
polished debugging output
2012-12-03 16:29:54 +00:00
Christoph Kords
f92d34dd22
removed some unused variables
2012-11-29 18:44:00 +00:00
Christoph Kords
e10000a338
Introduced an alternative cutback scheme for the nonlocal model, that allows to keep the results of most of the ips that immediately converged, and only do cutbacks in regions where some ips are in big trouble. Only works for nonlocal model and state integrator 2.
2012-11-27 18:36:55 +00:00
Christoph Kords
e584c0e6e8
deleted space in front of preprocessor line
2012-11-22 20:04:33 +00:00
Christoph Kords
38ec462f4a
order of integration now same for all state integrators: first calculate the dotState and then the deltaState
2012-11-22 13:04:19 +00:00
Philip Eisenlohr
7d196fbb25
polishing
2012-11-22 09:58:36 +00:00
Philip Eisenlohr
d189a6a7a0
polishing
2012-11-21 16:57:57 +00:00
Christoph Kords
760af1fbbf
crystallite_requested now masked by execIP, now elemhomogeneous works again
2012-11-19 15:13:48 +00:00
Christoph Kords
9fb94cd707
breaking crystallite loop in case of terminally ill (this functionality was probably lost since rev1886)
2012-11-19 08:39:48 +00:00
Philip Eisenlohr
d9a98417ca
switched element library to geomType based.
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saves to copy same geometry description for different elements that are essentially similar regarding the IP number but differ in total node count.
introduced quadratic tetrahedron (Marc element 127 -- element 157 might also work, but did not perform well in fully elastic calc so far)
2012-11-15 22:45:20 +00:00
Christoph Kords
11264f3fe4
forgot to check for convergence flag in FPI integrator
2012-11-08 20:15:19 +00:00
Christoph Kords
60438cdbcc
criterion for crystallite cutback loop changed from crystallite_subStep to crystallite_todo; this avoids problems when the last substep of the crystallite increment is below subStepMinCryst (which is allowed during last wind forward)
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fixed bug in the adaptive Euler integrator and the RK4 integrator, which could not reach the stateJump function, because of erroneous check for converged flag; also corrected the state counter for the RK4 integrator
2012-11-08 20:00:29 +00:00
Christoph Kords
c775edaa6d
better avoid initialization of residuum_old with huge, since it posed problems in Abaqus
2012-11-08 13:26:22 +00:00
Christoph Kords
dad9922f54
fixed bug in crystallite_FPI: stateDamper always has to be defined for each grain
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added some OMP FLUSH statements were necessary
replaced openmp do by forall construct where possible; this is much safer and perhaps even as fast for small loops
2012-11-07 15:43:29 +00:00
Christoph Kords
bb033c5fe7
Simplified algorithm of crystallite_integrateStress while preserving (almost) same functionality.
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Removed "leapfrogging" (increase of step for next guess, when last guess was ok); Replaced Armijo rule testing for step size by simple check if the residuum got better, since the former virtually did not have any effect; consistently using the 2-norm of the residuum rather than infinity-norm for the convergence check throughout the function
2012-11-06 12:35:45 +00:00
Christoph Kords
639d6e0655
inserted missing flush(crystallite_todo) in parallel section; might have caused trouble in parallel calculations before
2012-11-05 14:45:52 +00:00
Martin Diehl
086fe138b1
substituted matrix inversion to solve equation by direct solution routine from LAPACK
2012-10-31 09:56:26 +00:00
Christoph Kords
2be331b74d
In crystallite for state integrators 2 and 3: now that "stateJump" is called before integrating dotState, we have to do state = state + dotState *dt instead of state = subState0 + dotState * dt; otherwise the deltaState is lost
2012-10-22 13:34:15 +00:00
Christoph Kords
0980920b66
In crystallite: for state integrators 2 and 3 the deltaState always has to be done at the beginning of the integration, not at the end; otherwise the stiffness calculation can be completely wrong, when the state is changed after the stress integration for the central solution.
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Also changed some debugging levels in crystallite and mainly in constitutive_nonlocal
2012-10-22 07:59:35 +00:00
Christoph Kords
36676029e1
for state integrator 2 (explicit euler) and 3 (adaptive 2nd order euler): don't do any state evolution during stiffness perturbation, but only stress integration, since for those cases the state is not restored after every perturbation step
2012-10-19 11:20:31 +00:00
Philip Eisenlohr
dd5f453994
mainly cosmetics. added some comments. changed debug levels for some outputs. corrected (probably non-essential) check for NaN in FPI stressIntegrator.
2012-10-18 09:53:26 +00:00
Christoph Kords
5f0440fde3
crystallite_integrateStress now raises an error if Fp becomes NaN
2012-10-17 16:19:42 +00:00
Martin Diehl
0bcb8f59db
added doxygen comments, some polishing, added "protected" statements where applicable
2012-10-02 12:53:25 +00:00
Martin Diehl
22812c9a91
some minor improvement on precision detection: checking only once (in prec and no longer in math and crystallite), added one more 4/8 switch for LAPACK, as there is no single precision FFTW, stopping compilation for spectral method if FLOAT=4
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new function in IO to print integers without leading zeros, implemented it at some places in the new spectral solver (reporting still needs some serious polishing)
updated preprocessing for documentation to handle precision correctly
2012-08-30 20:26:28 +00:00
Martin Diehl
0959ff3299
substituted hand written matrix inversion by LAPACK version with precision selection.
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also introduced check for inversion into DAMASK_spectral_Utilities.f90 for the stress BC calculation. This part is further improved by using 5% of the reference stiffness to avoid trouble in the fully plastic regime (where the stiffness is underestimated)
Test for Marc 2010 is updated because the new inversion give slightly different results near 0 (order of e-13)
2012-08-28 16:59:45 +00:00
Christoph Kords
ad7381cfdd
maximum relative step length in stress integration cannot decrease below 1
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intermediate tensor "A" is calculated only once before the Lp loop in "integrateStress"
2012-08-21 08:53:36 +00:00
Christoph Kords
c1c5941733
stressAndItsTangent:
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when winding forward to last substep in increment, also do the calculation if this substep is below "subStepMinCryst";
output of "wind forward" and "cutback" info only for crystallites that are still "todo"
integrateStress:
maximum component in Lp determines absolute convergence criterium:
aTol = max(maxLpComp * rTol_fromConfig , aTol_fromConfig)
this ensures that small values in Lp do not spoil the convergence, similar to the effect of the relevantStrain parameter before (not needed anymore in the stress integration)
2012-08-14 12:07:59 +00:00
Philip Eisenlohr
4d09ef0648
changed variable name "debug_what" to "debug_level"
2012-07-05 09:54:50 +00:00
Franz Roters
380f40561b
first calculation of Tstar still used hard coded Hooke, now usese constitutive_TandItsTangent(...)
2012-06-18 07:26:34 +00:00
Christoph Kords
fc7b4d6471
new function stateJump, which takes care of immediate changes in the state (deltaState); this introduces discontinuities in the state evolution; therefore this is always and only once done after each integration step, so no evaluation of deltaState for intermediate steps of e.g. the Runge-Kutta integrator; otherwise integration becomes a pain without significant gain in accuracy
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deltaState now successfully tested for nonlocal model; was not correct for integrators 1,4,5 before
2012-06-06 15:11:30 +00:00
Christoph Kords
8c849d62ee
small corrections for how to treat the new deltaState in FPI and euler integration; all integrators successfully tested with j2
2012-05-18 13:00:15 +00:00