Christoph Kords
c36968fc68
distance for periodic images in internal stress calculation was incorrect
2011-03-30 11:57:41 +00:00
Franz Roters
08da2b5e4d
added minimum abaqus_v6.env file containing all changes necessary for the use of the MPIE subroutine
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changed comments in interface routines to refelect this
2011-03-29 13:49:50 +00:00
Franz Roters
e9e6abbdaf
introduced variables for compiler options
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added -fpp switch to invoke precompiler
2011-03-29 07:55:38 +00:00
Christoph Kords
314ca3fe7f
Internal stress calculation in nonlocal model: instead of integration of excess gradients (->Bayley) we now sum up contributions from adjacent superdislocations within a certain radius R. When periodicity is used, also periodic images are considered in stress evaluation.
2011-03-29 07:34:33 +00:00
Christoph Kords
3d51dd36fa
* Introduced preprocessor directives in order to suppress compilation of most write statements when using openmp. This tremendously improves efficiency of parallelization.
...
* Also added some more openmp directives to increase percentage of parallelized code.
* "implicit none" was missing in two subroutines of homogenization and constitutive.
2011-03-29 07:27:19 +00:00
Philip Eisenlohr
5c05c5d068
corrected mixed up array size for hardeningMatrices (twin/slip)
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added explicit array range 1:lattice_maxNslip/twinFamily
2011-03-24 17:20:35 +00:00
Franz Roters
fa323f3f0b
removed division by zero from debug_reset(), uses huge() now
2011-03-24 07:38:56 +00:00
Franz Roters
78d4e7d1dc
mpie_cpfem_abaqus_std.f: first call is with kinc==1
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mesh: allow multiple element sets with identical material
2011-03-23 16:20:12 +00:00
Franz Roters
8467c91dab
moved setup scripts back to subdirs where they are needed
2011-03-22 15:42:53 +00:00
Christoph Kords
31a570768b
new error 237: singularity in internal stress calculation
2011-03-22 13:58:42 +00:00
Nan Jia
7be2edb10e
added "texture
...
" as possible crystallite output => reports ID for later discrimination...
2011-03-22 13:40:27 +00:00
Christoph Kords
b8b75edd7d
no changes to previous version, just wanted to add some comment to the previous commit:
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subroutine "constitutive_nonlocal_dotState" only affects the current dotState, so no need to pass the whole array as argument
2011-03-21 15:23:36 +00:00
Christoph Kords
9b1e1e35ea
dotState
2011-03-21 15:18:09 +00:00
Christoph Kords
462eda6736
split parallel region in integrateStateFPI into two
2011-03-21 14:30:10 +00:00
Christoph Kords
5ee73dee72
age dotState before resetting it to zero, otherwise the statedamping does not work.
2011-03-21 13:06:11 +00:00
Christoph Kords
fc6f2ae68f
No need to call constitutive_microstructure at the beginning of each crystallite step, since it's already been done at the end of the previous step. Just do it once after initialization to start with correct values for the dependent state variables.
2011-03-21 10:35:42 +00:00
Christoph Kords
11138e3ee2
debugging output is now controlled by the "verbosity" parameter in the debug.config ranging from 0 (=almost no output) to 8 (=very detailed output)
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0 : only version infos and all from "hypela2"/"umat"
1 : basic outputs from "CPFEM.f90", basic output from initialization routines, debug_info
2 : extensive outputs from "CPFEM.f90", extensive output from initialization routines
3 : basic outputs from "homogenization.f90"
4 : extensive outputs from "homogenization.f90"
5 : basic outputs from "crystallite.f90"
6 : extensive outputs from "crystallite.f90"
7 : basic outputs from the constitutive files
8 : extensive outputs from the constitutive files
If verbosity is equal to zero, all counters in debug are not set during calculation (e.g. debug_StressLoopDistribution or debug_cumDotStateTicks). This might speed up parallel calculation, because all these need critical statements which extremely slow down parallel computation.
2011-03-21 10:31:17 +00:00
Christoph Kords
9d7ede7e03
extreme values of stress and jacobian now recorded in CPFEM_general. variable declaration and generation of output moved to debug module.
2011-03-17 13:13:13 +00:00
Christoph Kords
235266b169
openmp parallelization working again (at least for j2 and nonlocal constitutive model).
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In order to keep it like that, please follow these simple rules:
DON'T use implicit array subscripts:
example: real, dimension(3,3) :: A,B
A(:,2) = B(:,1) <--- DON'T USE
A(1:3,2) = B(1:3,1) <--- BETTER USE
In many cases the use of explicit array subscripts is inevitable for parallelization. Additionally, it is an easy means to prevent memory leaks.
Enclose all write statements with the following:
!$OMP CRITICAL (write2out)
<your write statement>
!$OMP END CRITICAL (write2out)
Whenever you change something in the code and are not sure if it affects parallelization and leads to nonconforming behavior, please ask me and/or Franz to check this.
2011-03-17 10:46:17 +00:00
Franz Roters
97a0146672
deactivated one debug statement at the end of crystallite_updateState(g,i,e) as it leads to division by zero if constitutive_state(g,i,e)%p(1:mySize) contains zero values
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statement should be changed to check for zero values
2011-03-11 10:05:30 +00:00
Philip Eisenlohr
1f0569230b
new installation/setup dir to hold all top-level make_*-scripts
2011-03-11 09:20:37 +00:00
Franz Roters
bdc17f7d72
extended comment on modification of abaqus_v6.env
2011-03-11 09:05:09 +00:00
Franz Roters
6475235fb4
included "-heap-arrays 500000000" in remark on how to change compile command
2011-03-08 08:18:04 +00:00
Franz Roters
18e668340f
Abaqus interfaces dapted to newest version of the rest of the code
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does not yet check for restart, have to check out first how restarts work in Abaqus
explicit code not checked as we do not have a license
2011-03-07 12:49:27 +00:00
Franz Roters
654b5ea987
set type for acos_arg
2011-03-04 14:57:22 +00:00
Franz Roters
2975c99144
now the maybe not perfect quartenions caused trouble in math_QuaternionToEuler
2011-03-03 14:23:39 +00:00
Franz Roters
e7c7ccdcdd
improper rotation matrix from pdecomposition could cause negative arguments in squareroot
2011-03-03 10:47:07 +00:00
Franz Roters
6667e94238
abaqus routines VGETOUTDIR and GETOUTDIR do not return the trailing slash, which we assume to be there, so it has to be appended
2011-03-03 10:29:59 +00:00
Martin Diehl
138e9c43eb
some comments (talking to Ricardo)
2011-02-25 16:24:23 +00:00
Martin Diehl
a6d1e5c911
now deleted old _single files
2011-02-25 12:49:18 +00:00
Martin Diehl
8cae4d609a
some polishing for single precision version.
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Now only prec and mpie_spectral are needed in different versions
2011-02-25 12:41:46 +00:00
Christoph Kords
ad4706673b
* removed calculations for dipole formation/dissociation by stress change, since it is not used anyways; also removed associated constitutive outputs from material.config
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* removed input variables in constitutive_collectDotState and constitutive_postResults that are not needed anymore (because of recent changes in constitutive_nonlocal)
2011-02-25 09:53:20 +00:00
Martin Diehl
cd5407b08b
removed all math functions only for double precision by the more flexible counterpart, e.g. "dsqrt --> sqrt", "dsin --> sin". Should not cause any harm, as long as "implicit none" is used.
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Now it is possible to compile a single precision spectral solver/crystal plasticity by replacing mesh.f90 and prec.f90 with mesh_single.f90 and prec_single.f90.
For the spectral method, just call "make precision=single" instead of "make". Use "make clean" evertime you switch precision
2011-02-25 09:25:53 +00:00
Christoph Kords
2f503f5cdb
added "Lp" as crystallite output
2011-02-25 08:15:26 +00:00
Christoph Kords
e022810e66
fixed problem in internal stress calculation for periodic neighborhood
2011-02-25 08:10:11 +00:00
Martin Diehl
f525c02ded
added single precision libraries for FFTW
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First try of implement single precision crystal plasticity, not working yet.
polishing text about geometry construction.
polishing postResults, still having problems concerning machines without MSC installation
2011-02-24 18:39:57 +00:00
Christoph Kords
e49e5e13af
* in flux calculation: take care of special case for single element model
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* do not overwrite "constitutive_nonlocal_rhoDotFlux" when doing a state perturbation, so we can use it for output
2011-02-24 10:01:41 +00:00
Christoph Kords
8aef9b1c13
check for twin nodes only in direction of the surface normal. this solves a problem with models of single element thickness and periodic fluxes.
2011-02-24 09:26:30 +00:00
Christoph Kords
fed53a7e60
in subroutine "mesh_marc_get_mpieOptions": need at least one additional string after keywords "$mpie" and "periodic", not two as it used to be
2011-02-23 12:33:51 +00:00
Christoph Kords
430966eb20
sorry, forgot to commit the numerics.f90, too
2011-02-23 12:30:52 +00:00
Christoph Kords
96d3682d5e
* new global integer variable "numerics_integrationMode" (1 indicating integration of central solution, 2 indicating integration of perturbed state)
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* combined "integrator" and "integratorStiffness" in new global variable "numerics_integrator"
2011-02-23 08:29:51 +00:00
Christoph Kords
d835380bc0
* "constitutive_nonlocal_flux" is set to zero in "constitutive_nonlocal_dotState", not in "constitutive_nonlocal_microstructure"
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* dislocation flux and internal stress calculation now consistent with new definition of slip system lattice according to paper (polarity of screws inverted)
2011-02-23 08:08:06 +00:00
Martin Diehl
8dd1a694a3
extended IO to cope with different name for solverJob and Model
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polishing, added error codes
added FFTW library files
2011-02-21 14:37:38 +00:00
Christoph Kords
b21c153761
restructured constitutive_nonlocal_compatibility and incorporated the "surfaceTransmissivity" in the compatibility calculation
2011-02-16 16:38:18 +00:00
Christoph Kords
24d33bf2ff
* added a new material parameter "surfaceTransmissivity" (default value 1.0) which allows to change the transmissivity of the material surface between 0 and 1
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* now complaining when encountering an unknown nonlocal parameter in material.config
* use same error ID for all material parameters out of bounds
* symmetric flux calculation in side dotState can now be omitted (because of new treatment of periodicity)
* switching back to "local flux balance" (add leaving and entering fluxes at central MP, don't touch neighbor) instead of "flux distribution" (subtract leaving fluxes from central MP and add them at neighboring MP). This has the advantage that there is almost no need for CRITICAL statements in parallelization, so hopefully this results in some speed up.
2011-02-16 16:35:38 +00:00
Christoph Kords
8f626c8989
Now able to have real periodicity for fluxes (fluxes leaving the model on one side enter on the other side).
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To enable this feature one has to add the following somewhere in the marc input file:
$mpie periodic x y z
for having periodicity in all directions
$mpie periodic z x
for having periodicity in x and z direction
etc.
Note that this only works for regular meshes!!!
2011-02-16 16:23:08 +00:00
Alankar Alankar
89ed6f5f66
Did not compile. Fixed missing ,
2011-02-15 12:29:01 +00:00
Alankar Alankar
c39e04644b
Sorting of hex slip-systems done in update 659 was missing. Included again.
2011-02-15 12:21:54 +00:00
Martin Diehl
438bf95105
added ft-based reconstruction of deformed configuration to postprocessingMath.f90 and postprocessingMath.pyf
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also added function to calculate average of tensor
some polishing in mpie_spectral.f90, added sanity check to see im resolution is power of 2
2011-02-14 17:21:31 +00:00
Philip Eisenlohr
171f5375f1
shearrate output now with sign (no |abs| as before)
2011-02-11 10:19:41 +00:00
Martin Diehl
3d7fad6ba9
mpie_spectral.f90: changed fourier transormation, now using the advanced interface to do the tranformation both ways with just one call. now also using the same variable for pk-stress in both domains and the change of deformation gradient in both domains.
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postprocessing: renamed name of python/f2py modul from "reconstruct" to "postprocessingMath", added some numerical operations to use for postprocessing.
2011-02-09 17:47:28 +00:00
Christoph Kords
803e1a8c05
In order to help preventing further memory leaks all array sections now have an explicit instead of assumed shape, e.g. Fe(1:3,1:3) instead of Fe(:,:).
2011-02-09 13:12:46 +00:00
Christoph Kords
466ced911e
* check convergence for nonlocals also in stiffness calculation mode
2011-02-09 08:39:07 +00:00
Christoph Kords
921967c2ba
* found memory leak in nonlocal model! "constitutive_nonlocal_rhoDotFlux" has to have upper index bound of 10 for second dimension, not 8.
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* need to recalculate dislocation velocity in postResults, otherwise we take values of last perturbed state! So the following outputs were up to now showing the perturbed state: shearrate, dislocation velocity, all density rates!
2011-02-09 08:28:47 +00:00
Christoph Kords
17a6c0e59b
enhanced comment on dislocation kinetics
2011-02-08 12:48:50 +00:00
Christoph Kords
6731659aa4
added hint that extreme values of stress and tangent belong to previous cycle
2011-02-08 12:43:30 +00:00
Christoph Kords
0a30fb739a
now reporting extreme values of stress and tangent, that were returned to marc, in output file
2011-02-08 10:25:51 +00:00
Martin Diehl
7a7ca1aab7
mpie_spectral and mpie_interface: changed workingdir from pathToLoadFile to pathToGeomFile
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mpie_spectral and numerics: added switch to prevent pre calculation of gamma_hat. slower, but saves memory
3Dvisualize: started to add support for gmsh (not fully working yet)
reconstruct: new version of f2py/Fortran subroutines for output of results from spectral method
2011-02-07 14:35:42 +00:00
Christoph Kords
faba13f7fd
* now able to introduce some scatter in the initial single dislocation density (only for nonlocal model!) ; setting the parameter "rhoSglScatter" to a positive value generates a gauss distribution for the dislocation density with standard deviation equal to "rhoSglScatter"
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* dislocation stress calculation is only done for nonlocal constitution ("/nonlocal/" keyword is present in material.config)
2011-02-04 15:41:32 +00:00
Alankar Alankar
b362755457
grain orientation shuffling was skipped for /elemhomo/. no clue why, now dropped...
2011-02-03 17:25:58 +00:00
Martin Diehl
fec2c14a4e
removed hard-coded tolerances from mpie_spectral and put them to numerics/IO
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removed storage of full cauchy stres field from mpie_spectral.f90, only average is stored now
added cauchy stress and von mises equivalent calculation to spectral post.
2011-01-31 17:07:42 +00:00
Christoph Kords
b72d75ed05
corrected indices in flux density output
2011-01-28 12:49:58 +00:00
Philip Eisenlohr
c00a42a9a4
fixed last remaining tensor outputs to their transposed versions
2011-01-27 14:29:06 +00:00
Martin Diehl
aa7d5afd94
changed ifort options back to previous ones as -fast is not working
2011-01-26 13:33:44 +00:00
Christoph Kords
05d4d5fef2
* kinetics now according to Mohles; enables solid solution hardening
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* changed example in material.config accordingly
2011-01-26 10:17:42 +00:00
Philip Eisenlohr
6ac06af517
sorry, forgot to alter the most important part: post_results..! eventually, the t16 has defgrads and friends in correct format: du_i/dx_j is listed as linear array (1,1),(1,2),(1,3),(2,1),...
2011-01-24 16:23:37 +00:00
Philip Eisenlohr
4ee40df5ba
transposed writing into t16 file (and screen/debug) did not work with just stating array(1:3,:)...
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fixed by using math_transpose3x3 (and similar) instead.
2011-01-24 15:02:19 +00:00
Philip Eisenlohr
794aeb253b
crystallite and CPFEM now print/output tensors in ij notation (used to be, particularly in the t16, ji, i.e. transposed...)
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math reports random seed used for rnd() generation
2011-01-20 19:25:45 +00:00
Martin Diehl
b546d3bb91
some corrections regarding Multicore-support on mpie_spectral.f90 and makefile
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slight changes on mpie_spectral.f90 regarding file output
2011-01-12 17:02:42 +00:00
Christoph Kords
062c6b3d54
* allow zero cutoff radius
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* added missing error codes
2011-01-12 12:36:48 +00:00
Christoph Kords
d92f992eb7
if nonlocal ip has local neighbor assume perfect transparency of the (perhaps virtual) phase boundary. this is only a quick fix! need to rethink the way constitutive and real boundaries are treated!
2011-01-11 18:00:29 +00:00
Christoph Kords
6a3dd78259
fluxes are disabled when keyword "/nonlocal/" is omitted in the material.config (this is a way to use the constitutive_nonlocal model as a local dislocation based model)
2011-01-11 14:55:36 +00:00
Martin Diehl
ccc6aac10b
did not delete mpie_spectral2.f90 properly
2011-01-07 13:11:32 +00:00
Martin Diehl
71fb5eedf2
changed makefile: material subroutines are now compiled using openmp, enabled linux threads for fftw3 (also did some slight changes to enable that in the fortran source code)
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renamed mpie_spectral2.f90 to mpie_spectral2d.f90 (testing file, not properly working at the moment)
changed file extension and variable names in mpie_spectral.f90 and mpie_spectral_interface.f90 from "mesh" to "geom". Removed direct output from mpie_spectral.f90, all output is now base on materialpoint_results(:,1,:)
2011-01-07 12:56:45 +00:00
Franz Roters
9447330ab0
ATTENTION repository has been moved to new server!
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Now at musvn1:/home/svn/repos/cpfem
2011-01-05 16:11:51 +00:00
Franz Roters
096a4803b0
some polishing concerning openMP initialization
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number of threads is now written to *.out file
2010-12-02 11:04:29 +00:00
Denny Tjahjanto
36f27edd75
1. Adding more comments
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2. Changing 'subroutine' into 'function' for optimizing the computation time
2010-11-26 11:50:20 +00:00
Christoph Kords
6b199e7830
allow 2digit values to be read in for MPIE_NUM_THREADS
2010-11-25 10:34:55 +00:00
Christoph Kords
ea6a6c9503
* environment variable MPIE_NUM_THREADS now determines number of threads used in parallel regions
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* default value of the OMP_NUM_THREADS variable has to be restored at the end of mpie subroutine, since marc also seems to use and change(!) this
* usage: "export MPIE_NUM_THREADS=<number of threads>" to set variable in shell, then restart mentat and compile with option 3 (at the moment this does only work on ws 6, since all other workstations use compiler option "-save"; this puts all local variables by default in static memory, which is a killer for parallelization!)
2010-11-19 17:45:27 +00:00
Christoph Kords
b9b226548c
* enclose wall time measurement for LpAndItsTangent and count of leapfrogbreaks by CRITICAL construct
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* better use SINGLE (having an implicit barrier at the end) instead of MASTER construct
* deleted all explicit BARRIERs after do loops since parallel loop construct implies barrier at the end
2010-11-19 17:29:29 +00:00
Christoph Kords
15728d3305
enclose wall time measurement for dotState and dotTemperature function by CRITICAL construct
2010-11-19 17:19:03 +00:00
Christoph Kords
4f267f4375
parallelization now works properly (not yet tested extensively though):
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* had to add some BARRIER constructs
* only the master thread is allowed to increase the state counter
yet parallelization seems not to give a significant decrease in calculation time with nonlocal model (because of too many CRITICAL statements?)
2010-11-11 16:16:05 +00:00
Christoph Kords
14594dc9e2
* OpenMP does not like unbounded array subscripts in function calls
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* some write statements were still not enclosed by CRITICAL construct, some needed a MASTER construct
2010-11-11 13:14:53 +00:00
Christoph Kords
bca951325d
* cpfem will now produce a warning if all components of the stiffness tensor are close to zero
2010-11-04 18:18:01 +00:00
Philip Eisenlohr
54748bb6a5
cycleCounter reset was 0 now -1 ==> occurence of jacobian calculation is now correct, i.e. always calc at start of new increment
2010-11-04 18:15:50 +00:00
Christoph Kords
405d5529e7
* checked and corrected parallelization of code. compiles now successfully, but simply aborts computation with first parallel directive without any comment :-(((
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* also put a call to constitutive_microstructure at the start of each crystallite_integration subroutine like it was before. need that for nonlocal model in case of crystallite cutback
2010-11-03 17:22:48 +00:00
Philip Eisenlohr
0dd99cb965
lattice: (re)introduced _symmetryType function to replace unsafe lookup array
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numerics: polishing
mpie_cpfem_marc: polishing
..powerlaw: aware of symmetryType function
crystallite: aware of symmetryType function, smaller leapfrog acceleration
IO: new warning 101
CPFEM: range of odd stress is now -1e15...+1e15, H_sym is used for stiffness
2010-11-03 14:58:11 +00:00
Denny Tjahjanto
763c20b302
Introducing the capability to restart jobs that crashed in the middle of sims. At the moment, this feature is exclusive for Marc.
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Major changes:
CPFEM.f90 =>
1. Moving the initialization out of CPFEM_general into a separate subroutine, which is directly called by the hypela2 (Beware, the Abaqus version must also be modified in order to adapt with this change).
2. Restore primary state variables in CPFEM_init from binary files when requested (Marc flag: restart read).
3. Writing primary state variables into binary files (Marc flag: restart write).
FEsolving.f90 =>
1. Adding functions to recognize Marc restart flags: read and write and the corresponding restart file (parent job).
2. Change the initial value of cycleCounter = -1 in conjuction with the change made the ping-pong scheme
homogenization_RGC.f90 =>
1. Just syntax polishing.
IO.f90 =>
1. Adding functions/subroutines to open binary files for writing the primary state variables for restart purpose.
mpie_cpfem_marc.f90
1. Modification of the general scheme for collection and calculation in order to accommodate the newly added restart feature.
2010-11-03 14:39:18 +00:00
Christoph Kords
4c20daa00d
state loop count was wrong for adaptive euler integration
2010-10-28 12:22:17 +00:00
Martin Diehl
17812c1f9e
added raw output, gmsh output is still included
2010-10-27 17:15:49 +00:00
Christoph Kords
9320d48305
in RKCK45 state integration: dotState was not saved in last Runge-Kutta step
2010-10-27 08:48:04 +00:00
Christoph Kords
f5f3ef5ecc
* have to reset dotState to zero before call to collectDotState (only important for nonlocal calculation)
...
* in Fixed Point Iteration: update dependent states after state preguess was missing; on the other hand, the first call to constitutive_microstructure was obsolete
2010-10-26 14:04:33 +00:00
Christoph Kords
4439282239
no change to previous version, just forget to mention one important change of the last revision:
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* fluxes are now again calculated and distributed only! by the originating material point. this means that the central MP might change the dotState of its neighbor. have to see whether locks slow down parallel computation
2010-10-26 13:49:58 +00:00
Christoph Kords
62d06001ea
* corrected compatibility for screws (always positive)
...
* detection of grain boundary in constitutive_nonlocal_microstructure with the help of transmissivity
* enforce positive densities in constitutive_nonlocal_microstructure (needed because dotState does not create cutbacks for negative densities anymore)
* reset single mobile densities below certain threshold to zero (also done in constitutive_nonlocal_microstructure)
* constitutive_nonlocal_kinetics only gets local state variable as input, no need for the entire array here
* dv_dtau is always positive
* multiplication is only active when there is already some initial density of the respective type
2010-10-26 13:42:18 +00:00
Christoph Kords
366d52bd71
* former "relevantRho" and "relevantResistance" is renamed to "atol_rho" and "atol_resistance" and now used as an absolute tolerance for the state residuum. before it was used rather as significant state, so whenever the state dropped below that value it was considered converged. (In dislotwin and titanmod constitutive law there is only one value atol_rho which is used for all the states, though the state array consists not only of densities. We need further parameters here!)
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* somewhat simplified convergence check for adaptive euler and runge-kutta
2010-10-26 13:16:37 +00:00
Martin Diehl
26cb618b6d
changed calculation to small strain/cauchy stress
2010-10-20 11:27:10 +00:00
Martin Diehl
da35eaa8a1
changed spectral algorithm to version proposed by Ricardo 2001 (using tau_field instead of stress_field).
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Still using largestrain-formulation
2010-10-20 09:27:47 +00:00
Martin Diehl
3837dad51e
fixed bug in mpie_spectral.f90 concerning spectral method (now deltaF hat get the right value)
...
added mpie_spectral2.f90, a version that should get the new algorithm proposed in 2010. until now, it is the same as mpie_spectral.f90 (large strain formulation by suquet et al) but with c2c, c2c FFT
2010-10-20 08:59:00 +00:00
Christoph Kords
e49de75fe3
stiffness calculation now only needs a single function call to the respective integrator method instead of one call per grain (which seems to heavily slow down the computation). also no special treatment for non-local material points anymore.
2010-10-15 14:57:13 +00:00
Christoph Kords
fffe731447
* had to correct nonlocal slip system compatibility and flux calculation. last update gave wrong results.
2010-10-15 13:19:26 +00:00
Philip Eisenlohr
61f8a5fcbe
corrected UpperCase "SolidSolutionStrength" in config file parsing.
2010-10-15 12:59:00 +00:00
Martin Diehl
3c502561ee
added matrix multiplication 3333x33 to math.f90
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added some parameters for spectral method to numerics.f90 (tolerance)
changed error message concerning spectral method in IO.f90
corrected calculation of stress BC in mpie_spectral.f90
2010-10-13 16:04:44 +00:00
Christoph Kords
724960686f
* in nonlocal model: dislocation flux now with valid description also for large angle grain boundaries; transfer of dislocations from one slip system to the other according to new variable "constitutive_nonlocal_compatibility" which depends on the angle between slip plane normals and slip directions and is updated once per cycle in function "crystallite_orientations"
...
* reactivated debugging functionality for "non-standard" integration methods
2010-10-12 13:08:54 +00:00
Christoph Kords
efd92d9b51
allocation of special state variables for "non-standard integration" was erroneous. used to produce segmentation fault for integration method 4 and 5.
2010-10-12 12:11:24 +00:00
Christoph Kords
fce7590c17
* now able to choose method for state integration (integrator and integratorStiffness in numerics.config); standard is "Fixed Point Iteration", which is basically the same as before; others available are "Explicit Euler", "AdaptiveEuler", "Classical Runge-Kutta" and "Runge-Kutta Cash-Karp"
...
* now remembering stiffness similar to how we do it for Lp etc.; avoids undefined stiffness values for nonconverged stiffness calculation
* non-local stuff:
* changed non-local kinetics (Gilman2002)
* enforce zero shearrate for overall carrrier density below relevant density
* enforce zero density for those states that become negative and were below relevant density before
* dislocation velocity is not limited by V^(1/3) / dt anymore
2010-10-01 12:18:49 +00:00
Martin Diehl
9927cd7adb
changed format of resolution. instead of reading exponent of two, now the number given equals directly to the number of FPs. Allows us to use arbitrary number of FPs.
...
example:
OLD: reading 5 results in 2^5=32 FPs
NEW: reading 33 results in 33 FPs
2010-10-01 10:42:15 +00:00
Alankar Alankar
2cc7bc38d7
Fixed a missing ','. Assigned plane and direction names.
2010-10-01 06:32:44 +00:00
Philip Eisenlohr
1ae252c1ce
altered hexagonal slip systems
...
(needs comparison to former set, which is potentially wrong)
2010-09-30 17:31:19 +00:00
Claudio Zambaldi
b85f9b0770
material.config: changed texture of microstructure 1 from 1 to 3, because 1 needs a ODF file which is not in the repository and makes the one_element_model.proc complain.
2010-09-30 12:55:38 +00:00
Philip Eisenlohr
a8dfdc6487
added _mul33xx33 double contraction: A_ij * B_ij = scalar
2010-09-30 09:32:49 +00:00
Christoph Kords
cb4b4afc88
corrected header for math_qRot
2010-09-30 08:46:58 +00:00
Philip Eisenlohr
b259fbd9c6
1) added distribution of leapfrog breaks
...
2) lattice_symmetryType is now a function (former lookup array was buggy)
3) stricter check of state var values (>0!) and memory deallocation done
2010-09-30 07:31:53 +00:00
Alankar Alankar
e562df35a9
Added more state dependent variables in post results.
2010-09-29 06:35:08 +00:00
Martin Diehl
5a51082977
polishing, changed calculation of stress BC.
...
prevent updating of gamma hat in case of perfect plasticity
2010-09-24 13:27:53 +00:00
Alankar Alankar
d94236b2d6
Declaration of filename etc. was missing. Fixed now.
2010-09-23 09:13:46 +00:00
Philip Eisenlohr
83a921eec2
crystallite: polishing
...
rest: added "$ID" and line ending settings...
2010-09-23 08:05:50 +00:00
Philip Eisenlohr
a467fb4ae3
forgot "$ID" and setting line endings...
2010-09-23 08:03:00 +00:00
Philip Eisenlohr
89136afade
debug now has config file, too
2010-09-23 08:01:41 +00:00
Martin Diehl
6ea8623f65
added functions math_mul33x3_complex math_Plain99to3333 to math.f90.
...
mpie_spectral.f90 uses both functions
math_Plain99to3333 is used for inversion of c0
math_mul33x3_complex is used for equilibrium check in fourier space
also did some cleaning up on mpie_spectral.f90
2010-09-22 12:04:43 +00:00
Alankar Alankar
80618c9814
Cleaned-up, rearranged state variables
2010-09-22 09:00:40 +00:00
Alankar Alankar
7548858ffa
Some useful changes in damper for quicker convergence.
2010-09-22 08:54:36 +00:00
Martin Diehl
604992a9e1
fixes bugs in screen output, changed gmsh output, now the deformed mesh is written out
2010-09-22 08:51:34 +00:00
Martin Diehl
6920d8d939
cleaning up, added new output to gmsh and to screen, prepared calculation of deformed mesh
...
new convergence criteria: divergence of stressfield (in fourier space)
2010-09-21 15:38:25 +00:00
Alankar Alankar
8488cafe3a
now consistent with numerics.f90 values
2010-09-21 14:37:52 +00:00
Alankar Alankar
18c86ca0b1
Updated corresponding files for titanmod constitutive
2010-09-13 09:29:03 +00:00
Philip Eisenlohr
9a20f742ea
leaner memory requirement to store states and their rates when calculating the crystallite stiffness
2010-09-13 09:13:25 +00:00
Martin Diehl
1693bfca47
changed calculation of defgrad from cauchy-stress to pk-stress, now working in large-strain-formulation.
...
output of msh-file changed to deformed configuration, removed output of defgrad as a field
2010-09-07 16:37:55 +00:00
Alankar Alankar
3c5f38643d
Brushed up accountability of twinning to Lp
2010-09-07 14:44:37 +00:00
Christoph Kords
7d4c7f7fa7
corrected bug in debug: stressloop info was erroneous
...
mesh init now showing much more ip statistics in verbose mode
2010-09-07 09:06:02 +00:00
Philip Eisenlohr
a3c92061f9
1) terminallyIll was reset before FE did cutback --> useless extra calculations of same problem over and over...
...
2) local stiffness calculation is now standard for non-local grains
3) stressLoopDistribution discriminates between (a) central solution and (b) stiffness perturbation
4) debugger is switched on as standard... (but verboseDebugger not!)
2010-09-06 16:06:41 +00:00
Martin Diehl
00922705eb
now using current average stiffness for reference material stiffness
2010-09-06 10:00:59 +00:00
Philip Eisenlohr
c19524f264
1) fixed terminallyIll bug occurring with Ngrains=1 homogenization
...
2) brushed up the output to be more easily readable/understandable
2010-09-01 21:04:02 +00:00
Alankar Alankar
4f29e8c2fe
Introduced twinning. Twinning based on accumulated shear on twin systems. No slip-twin interactions yet.
2010-09-01 10:07:52 +00:00
Martin Diehl
a5c228fd02
changed back transform to complex-to-real, removed redundant variables, reduced size of arrays where possible
2010-09-01 08:05:11 +00:00
Martin Diehl
85febf0803
added fftw3 as fft(library will not versioned, should be in a linkable folder) , did some corrections on the code, splitted main file up (allows use of makefile), added makefile
...
changes on mpie_spectral.f90:
new structure, changed variable names, now using defgrad instead of disgrad, cleaned up, removed augmented Lagrange.
ToDo: Implement Augmented Lagrange again (but then a working version), implement Large strain, think about complex-to real-transform backwards, try to implement MP-support
2010-08-27 16:39:38 +00:00
Christoph Kords
05568ef73b
calculation of state damper was erroneous for use with nonlocal and other constitution at the same time
2010-08-26 12:54:31 +00:00
Christoph Kords
197d7ea8d9
rearranged output statements in crystallite init for better readability in output file
2010-08-26 09:52:40 +00:00
Alankar Alankar
ec4269bdd8
Added 'dislocation-type' dependent interactions. Ideal for hexagonal and BCC structures.
2010-08-23 11:36:51 +00:00
Philip Eisenlohr
da53656c9a
added C3D20R (type 9) to list of possible non-local elements (Christoph, should we invent a reasonable error number for this? "-1" may not be optimal...)
2010-08-19 23:00:26 +00:00
Philip Eisenlohr
c352146fe6
exchanged forall (warning causers) to nested do loops
...
deleted (currently unused) symmetrization of H tensor in CPFEM.f90 --> Denny pls advise?
2010-08-19 21:35:38 +00:00
Franz Roters
f78b07448f
some modifications in line with Davids analytical model
...
input some additional variables via material.config
2010-08-17 14:23:55 +00:00
Philip Eisenlohr
bb9899e7de
1) added element type 57 (C3D20R) reduced quadratic hexahedral
...
2) need discussion about the present omission of the FE_nodesAtIP for type 8 --> added comment into source code
2010-08-16 22:53:24 +00:00
Alankar Alankar
9f071c3e01
Added kink-pair pre-factor for screw dislocation mobilities on non-basal slip systems in hex
2010-08-06 15:53:45 +00:00
Philip Eisenlohr
298cecbfec
corrected syntax errors (long lines, line continuation by \) and logical mistake in mpie_cpfem_marc / abq_std which went unnoticed in ifort. Using SunStudio f90 surfaced those...
2010-08-03 23:47:00 +00:00
Alankar Alankar
60decea760
Calibration (Prismatic slip) of the new dislocation density based CPFE model for single crystal alpha-Ti (Titanmod). Formulated edge and screw dislocations mobilities in presence of kink pairs. Updated comments. The model shows the plateau in stress evolution in prismatic orientation which is observed in experiments.
2010-07-15 07:16:15 +00:00
Martin Diehl
49926d5d66
F77 --> F90 polishing/condensation as far as possible.
...
next step is change of Re/Im FFT to Re only...
2010-07-13 15:29:26 +00:00
Philip Eisenlohr
4d110126da
adopted improvements done by Arun Prakash.
...
mesh:
elemType identification based on lower case
Abaqus now reports more errors
IO:
new function to inquire whether inputfile contains "parts"
new function to assemble multiply included inputfile into a flat one
awareness of range generation in element numbers
error reporting
2010-07-13 10:26:07 +00:00
Alankar Alankar
eb7830dc8f
New Titanium CPFE model based on dislocation density. Running but calibration and changes needed.
2010-07-13 08:19:25 +00:00
Martin Diehl
397db06fb3
cpfe_general now returns also Kirchhoff-stress P and dPdF
...
added dummy variables P and dPdF to mpie_cpfe_* to be able to call cpfem_general correctly
2010-07-07 09:58:18 +00:00
Martin Diehl
80016f8429
added P and dPdF for the call to cpfem_general, made some comments in the code, aligned some loops
2010-07-07 09:10:54 +00:00
Martin Diehl
f9834bc612
changed types of integers and reals in fourier transform, changed some variables and cleaned up code to make it easier to understand
2010-07-05 16:01:36 +00:00
Ricardo Lebensohn
c3e222dbbd
errs added etc.
2010-07-05 11:33:48 +00:00
Philip Eisenlohr
4f76eada31
started suggestions for F77 --> F90 style
...
xkdyad useful..?
looking for error calculation (Ricardo to rescue here)
2010-07-02 17:15:53 +00:00
Martin Diehl
d6ba9d54b6
changed declaration of two variables from real to int, spectral method is now working.
...
started to commend Ricardos code, layoutet loops and removed some redundant variables.
until now, no error calculation is done. at the moment calculations are in an infinite loop
2010-07-02 14:10:36 +00:00
Martin Diehl
661bb97800
corrected some problems in building mesh
2010-07-01 15:20:39 +00:00
Martin Diehl
2ec39c936c
added first version of spectral method, changed corrected functions to get correct path to files
2010-07-01 15:20:06 +00:00
Martin Diehl
c3e51e5330
added functions to read out resolution, dimension and homogenization from mesh file
2010-06-25 11:31:05 +00:00
Christoph Kords
eb0cc24a8e
no need for material parameter "a" anymore, dislocation stress calculation now works without "core spreading"
2010-06-21 16:01:05 +00:00
Christoph Kords
7d6e52067b
dislocation stress based on dislocation density gradients
2010-06-21 15:58:56 +00:00
Christoph Kords
6d874e2c1f
nonlocal stiffness calculation:
...
rather perturb all components at once (and optionally decrease the frequency of the Jacobian update with the iJaco parameter) than perturbing only a single component per cycle
2010-06-17 06:32:56 +00:00
Philip Eisenlohr
1c72439350
first shot at init with CPFEM_general
...
better would be to manually read the mesh resolution, set up Spectral solution strategy and call CPFEM_general just during BVP solution.
2010-06-10 15:32:06 +00:00
Philip Eisenlohr
8ea52ac495
mpie_spectral now can read loadcase data
...
adapted error codes
2010-06-10 14:51:10 +00:00
Martin Diehl
386ca7ebc3
added some basic I/O functions to mpie_spectral.f90
2010-06-10 08:50:04 +00:00
Christoph Kords
740db98090
- use upwind differences scheme for fluxes instead of central differences
...
- introduced possibility to "reflect" fluxes at free surfaces in order to have quasi-periodic fluxes
2010-06-09 08:56:00 +00:00
Philip Eisenlohr
11b98fbfa6
added ID functionality and correct line endings
2010-06-08 10:10:57 +00:00
Philip Eisenlohr
82687d31c8
first shot at mpie_spectral wrapper
2010-06-08 10:08:15 +00:00
Philip Eisenlohr
7e78932976
renamed "mpie_cpfem_init" subroutine within mpie_interface module to more general name "mpie_interface_init"
2010-06-08 09:35:13 +00:00
Christoph Kords
71c6179ee5
dislocation stress had wrong sign in some components
2010-06-08 09:34:23 +00:00
Christoph Kords
3ce1882d29
when calculating dislocation stress at grain boundaries, densities are now extrapolated similarly to like it was already done at free surfaces
2010-06-07 16:01:37 +00:00
Christoph Kords
3989cc2688
dislocation stress now considers dislocation segments of length V^(1/3) and ensures non-singular solution for points that are collinear to the dislocation line by means of a core spreading parameter "a". stress is scaled by a reference cutoff radius "r" to avoid mesh-dependent stress values.
...
corrected formula for conversion of anisotropic elastic constants to isotropic Youngs modulus and poissons ratio
2010-06-07 14:32:23 +00:00
Franz Roters
5283ba5546
if it is pReal it should be 1.0 not just 1
2010-05-31 07:12:45 +00:00
Christoph Kords
76b392e12f
dislocation stress calculation in constitutive_nonlocal_microstructure: corrected mapping from lattice to slip system frame and the neighboring dislocation density formulation
2010-05-28 13:12:36 +00:00
Franz Roters
bb73a74325
there was a line break missing so that it did not compile
2010-05-26 17:10:26 +00:00
Denny Tjahjanto
9932c90c73
restoring the crystallite.f90, IO.f90 and material.f90 to the version 575. the version 576 of these files contain some uncleared debugging statements.
2010-05-26 16:34:44 +00:00
Denny Tjahjanto
d114a600c3
fixed some errors in QuaternionToEuler, RToQuaternion to get the correct texture representation in the output.
2010-05-26 15:52:54 +00:00
Christoph Kords
e5f0af638e
fixed calculation of dislocation stress for elements with a single ip and no neighbors; used to get segmentation fault
2010-05-26 09:17:10 +00:00
Christoph Kords
0c5bc83469
in nonlocal_microstructure: at the model surface the excess density is now extrapolated from opposite neighbor instead of assuming zero density; this results in better modeling of the dislocation stress at the surface
...
restructured nonlocal_dotstate, to be able to easily switch on and off particular effects in the microstructure evolution
nonlocal_dotstate now enforces a cutback when single density runs the risk of becoming negative; in the case of a state already below the relevantState dotState is set to zero
introduced two new output variables: rho_dot_edge and rho_dot_screw
2010-05-21 08:51:15 +00:00
Christoph Kords
dba4ae7ef1
new numerics parameter "defgradTolerance" replaces "relevantStrain" in cpfem, since "relevantStrain" is also used in crystallite but in a different context.
...
"defgradTolerance" gets the same standard value as "relevantStrain" so calculations should be consistent with older ones
2010-05-20 14:55:11 +00:00
Christoph Kords
3a23dc4bbd
first call to hypela2 in inc 0 is done with computation mode 2 (=plain calc), but since rev. 539 the second call was done with computation mode 6 (=only return values) instead of 2. This doesnt work, because computation mode 2 might calculate stress and tangent for all materialpoints, but the mapping from lattice to current configuration is only done for the element/IP that triggers the call.
...
So switched back to the former order of calls which also works for marc2010:
el 1 IP 1 | el 1 IP 2
|
inc mode lovl | inc mode lovl
------------------ | ------------------
0 2 6 | 0 2 6
1 6 4 | 1 6 4
1 4 6 | 1 3 6
1 6 4 | 1 6 4
1 1 6 | 1 2 6
Still to be checked:
according to Franz the lovl order could be different in contact analysis (e.g. starting with lovl 4 instead of 6)
2010-05-20 09:14:59 +00:00
Christoph Kords
51da3b6242
sorry, in rev 568 some variables were not declared in crystallite_postResults
2010-05-18 12:36:09 +00:00
Christoph Kords
472684c30e
make element type 8 (= hex8 reduced integration) available for nonlocal constitutive law
2010-05-18 08:13:23 +00:00
Christoph Kords
19b6fae88b
added a missing exclamation mark in front of an $OMP directive
2010-05-18 08:07:55 +00:00
Christoph Kords
d96780967b
added some output variables in crystallite: F, Fe, Fp, Ee, P, S
2010-05-18 07:57:13 +00:00
Claudio Zambaldi
15328e51cf
Like this Euler angles AND grain rotation should be OK.
2010-05-11 15:06:21 +00:00
Franz Roters
483584ceb3
improved version of general I/O functions
...
renamed module cpfem_interface to mpie_interface
2010-05-11 06:57:15 +00:00
Franz Roters
e810e5cfa1
changed fileopen routines in IO.f90 to use solver dependant functions defined in the interface routines
...
DID NOT test ABAQUS versions yet, not shure whether (V)GETOUTDIR returns path with or without terminating slash
2010-05-10 15:02:59 +00:00
Philip Eisenlohr
0416c9a616
reworked build_ipNeighborhood
...
added C3D8R reduced integration hexahedral element
2010-05-10 14:54:59 +00:00
Claudio Zambaldi
2405a51042
crystallite:
...
- grainrotation calculation now is done with symmetryID 0, i.e. without symmetry reduction since we want the absolute misorientation.
- While math has everything in radians, post results eulerangles and axisangle are given in degrees.
And: grain rotation seems OK after the previous changes in math module.
2010-05-07 12:01:46 +00:00
Philip Eisenlohr
97f206d0bc
new errors regarding Spectral method input file parsing
...
mesh setup from Spectral input file
$Id$ in FEsolving activated
2010-05-06 16:40:47 +00:00
Philip Eisenlohr
e4067f2d26
debugged zoo of rotation operations and transformations
...
all angles now in radians
introduced a rudimentary check in math_init to complain (IO_error) about broken transformations (e.g. quat --> R --> quat)
2010-05-06 14:07:21 +00:00
Franz Roters
f23b4d16d1
updated section with dislotwin paramters
2010-05-06 09:01:54 +00:00
Franz Roters
383a36b226
added comment on reformating to common block files
...
added modifications necessary for running the subroutine with Marc/Mentat2010
2010-05-06 08:50:54 +00:00
Alankar Alankar
393a67e587
now stating instance when sanity checks run into trouble
2010-05-05 13:36:59 +00:00
Christoph Kords
0a36527f61
fixed bugs in math_quaternionDisorientation
...
though running, there still seem to be some problems with the quaternion functions, since crystallite_grainRotation gives some dubious results!
2010-05-04 16:02:05 +00:00
Philip Eisenlohr
ba48e5d3ab
fixed syntax errors in last commit -- hopefully no further ones...
2010-05-04 13:03:35 +00:00
Philip Eisenlohr
cecffffe2b
disorientation with symmetryType == 0 returns plain misorientation
...
complain about unknown symmetryType
2010-05-04 12:54:13 +00:00
Claudio Zambaldi
adaeb0e1ef
rotation axis is undefined for small angles and therefore gets a NaN
2010-05-03 18:27:19 +00:00
Christoph Kords
ea718573ef
return 180° disorientation about 100 for neighbors with different phases
2010-04-29 12:28:51 +00:00
Christoph Kords
8ab101da50
safe use of acos function in math_QuaternionToAxisAngle
2010-04-29 10:33:39 +00:00
Philip Eisenlohr
15e5dcf8f2
math_QuaternionToAxisAngle now safe for small or close to 2pi rotations.
2010-04-29 10:01:09 +00:00