Commit Graph

225 Commits

Author SHA1 Message Date
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
Franz Roters e8719cb6b8 Table driven input works wirh 2010!
That leaves DDM to do for tomorrow ;-)
2010-04-29 09:43:31 +00:00
Franz Roters aaf1bf0edf fixed (first) problem with Marc2010 single job with old style input and extended precision should work now! 2010-04-29 08:15:29 +00:00
Christoph Kords c34c07a6ff statedamper has to be local (specific for each e,i,g); with a global damping we may produce spurious convergence 2010-04-29 07:41:29 +00:00
Christoph Kords 77dc16d15f print aged state of 1 1 1, which always exists, to avoid segmentation fault 2010-04-29 07:34:20 +00:00
Claudio Zambaldi 79f286f24c small typo 2010-04-28 17:45:30 +00:00
Claudio Zambaldi 0b83fa0fb2 corrected (?) disorientation calc and introduced some new assisting functions 2010-04-28 17:19:58 +00:00
Claudio Zambaldi 35cebfb132 extended output string length for init msg 2010-04-28 17:19:06 +00:00
Franz Roters a36951a6ac changed common block files to release version 2010-04-28 07:28:12 +00:00
Claudio Zambaldi e8ab495a6c Introduced new parameter NaN, not a number. It should be assigned for invalid results, such as currently for misorientation of unknown crystal symmetry. 2010-04-19 13:40:22 +00:00
Claudio Zambaldi cab2261693 New array crystallite_symmetryID(i,g,e) is now filled during initialization run with 1 for bcc and fcc phase and 2 for hexagonal phase. The values are needed for misorientation calculations to apply the correct symmetry operators for cubic and hexagonal phases. 2010-04-19 10:03:34 +00:00
Claudio Zambaldi 249042c2d3 New output can be requested from crystallite:
(output) grainrotation
it gives the deviation from the initial grain orientation 
in axis-angle representation with the angle in degrees.
2010-04-12 11:14:36 +00:00
Claudio Zambaldi 653837046e new: math_QuaternionToAxisAngle 2010-04-12 11:07:25 +00:00
Christoph Kords adf6206b71 corrected symmetry operations for hex. 2010-04-12 08:04:26 +00:00
Claudio Zambaldi fc3f35cf3b debugger = .false. 2010-04-08 09:30:25 +00:00
Christoph Kords 1730a90e12 corrected ip numbers in FE_ipNeighbor for element type 21; used to get wrong neighborhood for this element type 2010-04-06 11:45:23 +00:00
Philip Eisenlohr 9b5047c828 corrected two OMP CRITICAL terminations 2010-04-06 06:47:15 +00:00
Christoph Kords 1bf740eb9d an allocation statement was deleted from rev 518 to rev 520!!! 2010-03-30 13:15:18 +00:00
Christoph Kords 67c523e4b1 enclosed output statements in an "if (verboseDebugger)" 2010-03-25 08:27:42 +00:00
Denny Tjahjanto 9026cc4016 again corrections. but this version must work. 2010-03-24 16:23:21 +00:00
Denny Tjahjanto 414050303b forgotten: the change in the input config 2010-03-24 13:28:46 +00:00
Denny Tjahjanto 40b1478dac the latest RGC model + corrections for "element homogeneous" feature 2010-03-24 13:20:12 +00:00
Franz Roters 3aa2dd5fef removed special characters from twip steel section in material.config
changed crirtical twin stress in constitutive_dislotwin.f90
2010-03-24 08:17:27 +00:00
Christoph Kords 2c6c8fa04e ensure positive eulerangles in math_QuaternionToEuler 2010-03-19 16:11:53 +00:00
Christoph Kords f4e5d32cde added flag verboseDebugger to debug in order to have more control about debugging statements
set this to true if you want extended debugging info in the output file
2010-03-19 14:14:08 +00:00
Claudio Zambaldi 418bb9ecbe small improvement in readability 2010-03-19 12:56:00 +00:00
Christoph Kords 948c119ee9 changed internal representation of orientation and misorientation from euler angles to quaternions (this should also fix some bugs in the math_misorientation subroutine). includes a couple of new functions in math.f90 and some changes in crystallite.f90.
beware that crystallite output "orientation" now by default returns the orientation as quaternion. if you want euler angles instead, you have to add "eulerangles"  as a crystallite output in your material.config file (see material.config template).

for input of orientations in the texture block of the material.config you still have to specify the rotation in terms of euler angles, quaternions are not yet supported for input.
2010-03-18 12:23:17 +00:00
Christoph Kords e6fdfdfc36 iJacoStiffness belongs to numerics, not debug
sorry for not having checked that before
2010-03-17 17:00:54 +00:00
Christoph Kords 1a992e1aef nonlocal stiffness calculation produced segmentation fault for cycle number > 16. Corrected calculation of perturbation indices k and l. 2010-03-10 09:53:41 +00:00
Christoph Kords e3dd7551dc added output for dislocation evolution rate associated with flux: "rho_dot_flux" 2010-03-10 09:49:40 +00:00
Philip Eisenlohr 4752bbe42e deleted unused <global> part from file 2010-03-09 15:36:07 +00:00
Christoph Kords 61bd0224c1 - corrected an if statement in the state loop
- nonlocal stiffness calculation: we perturb all material points at the same time, so instead of N^2 loops we just need N
- set "forceLocalStiffnessCalculation" to false as standard
2010-03-04 17:27:39 +00:00
Christoph Kords a0d28ebc18 - flux calculation is now also compatible to neighborhood of local constitution
- flux density interpolation now depends on the position of the interface between ttwo neighboring material points
- simplified flux calculation scheme
- introduced sanity check for dislocation velocity to ensure v*dt< cellsize
2010-03-04 17:14:47 +00:00
Christoph Kords 947af80a2e removed old debugging statements 2010-02-26 12:02:49 +00:00
Philip Eisenlohr 8c8ed34356 reworked crystallite part to allow for flexible user output
--> new "crystallite" part in config file
--> new "crystallite" option for microstructures
--> new output file "...job.outputCrystallite" to be used in conjunction with marc_addUserOutput for meaningful naming of User Defined Vars.
2010-02-25 17:39:11 +00:00
Christoph Kords 538faecf45 new output "dislocationvelocity" 2010-02-23 17:23:07 +00:00
Christoph Kords c1717329ac only need 2 logicals in crystallite_stressAndItsTangent to reflect all possible integration states, so crystallite_onTrack was obsolete and replaced by crystallite_todo; broken state update now directly produces a cutback 2010-02-23 09:46:39 +00:00
Claudio Zambaldi 7526a24a1b now with functionality to output a "JOB.outputHomogenization". This contains size descriptions of all requested output variables to be parsed by a further script to generate meaningful names for user defined vars... (watch out!) 2010-02-19 18:03:16 +00:00
Christoph Kords aab5598d96 detabbed file for better readability 2010-02-19 13:44:38 +00:00
Philip Eisenlohr 8c5852dedf corrected messed up output of grain orientation in t16-file.
this bug affected at least all calculations done after revision 480 (Dec 18, 2009)
2010-02-18 16:09:45 +00:00
Denny Tjahjanto e9aac0c4af (1) change phaseOfGrain from real to integer and (2) introducing a condition to switch off the grain reshuffling when element homogeneous is requested. 2010-02-18 15:54:10 +00:00
Claudio Zambaldi d60d8a4103 small readability improvement 2010-02-18 15:06:08 +00:00
Franz Roters 7e632e8132 corrcected definition of forceLocalStiffnessCalculation 2010-02-18 14:43:40 +00:00
Philip Eisenlohr e1a25e0f73 renaming of abaqus to _std and adding of VUMAT interface for explicit. 2010-02-18 10:23:42 +00:00
Philip Eisenlohr af06e8e58f fixed some dangerous constructs in computation mode assignments
introduction of separate stress and stiffness variables to pass on to CPFEM_general (of dimension 6)
2010-02-18 10:23:02 +00:00
Philip Eisenlohr 78808a7d47 corrected corrupted header $id 2010-02-18 10:18:15 +00:00
Philip Eisenlohr 4cb7254a21 added new computation modes 8 and 9 for Abaqus_exp. These correspond to mode 1 and 2 but do collection and calculation in one step.
stress and stiffness are always of dimension 6 in CPFEM_general, hence, variable "ngens" useless by now
2010-02-18 10:15:08 +00:00
Philip Eisenlohr c3cd75c2c2 small polishing 2010-02-18 10:12:45 +00:00
Franz Roters 9c63005c8f allow for longer pathes when openening files
corrected error messages concerning file openening
2010-02-18 08:29:57 +00:00
Christoph Kords 97db70cf23 constitutive_nonlocal:
- reworked contribution of immobile dislocation density for rate equations
- flux is now calculated on the basis of interpolated velocities and densities at the interface; both incoming and outgoing fluxes are considered, so every material point only changes his own dotState
- dislocation velocity is now globally defined and calculated by subroutine constitutive_nonlocal_kinetics; the subroutine is called inside _LpAndItsTangent as well as _microstructure; therefore, microstructure now needs Tstar_v as additional input; in the future one should perhaps create a subroutine constitutive_kinetics that calls constitutive_nonlocal_kinetics separately, to clearly distinguish between microstructural and kinetic variables 
- better use flux density vector as output variable instead of scalar flux values for each interface
- added output variables internal and external resolved stress

crystallite:
- added flag to force local stiffness calculation in case of nonlocal model
- misorientation angle is explicitly set to zero when no neighbor can be found

debug:
- added flag "selectiveDebugger" that is used when debugging statements should only affect a specific element, ip and grain; these are specified with the new variables debug_e, debug_i and debug_g
- debugger can now be used in its original sense
2010-02-17 13:21:36 +00:00
Christoph Kords a2037db9c6 corrected sign of screw part of dislocation stress 2010-02-12 12:54:00 +00:00
Claudio Zambaldi f1daf9f2e7 added comment, my first 'test' SVN commit 2010-02-10 16:40:50 +00:00
Philip Eisenlohr f186c83068 introduced racing condition breaker for the case of multithreaded CPFEM init. 2010-02-02 15:00:08 +00:00
Franz Roters 101d4c6bb4 updated list 2010-02-02 13:05:17 +00:00
Franz Roters 02b98100d1 added / updated files for use with marc2010r1 2010-01-11 08:35:28 +00:00
Christoph Kords ed8446e0f3 - corrected contribution of immobile singles to dipole formation and annihilation rates
- remobilization of immobile singles immediately increases the mobile single dislocation density and therefore directly affects all other mechanisms in dotState
2010-01-06 09:54:00 +00:00
Christoph Kords dce840c0a5 - introduction of immobile (used) single dislocation densities as new state variables
- changed nomenclature (rho -> rhoSgl) to distinguish precisely between single dislocation density and total dislocation density
- changed material.config accordingly
2010-01-05 16:07:24 +00:00
Christoph Kords 2098c106ad misorientation is set to 400 degrees if our neighbor has a different phase 2010-01-05 16:03:45 +00:00
Christoph Kords aee0721ab2 corrected math_misorientation 2010-01-05 16:02:00 +00:00
Christoph Kords ac080e0b52 corrected small mistake in calculation for ip center of gravity / ip coordinates; used to ignore subnodes that had coordinates (0.0, 0.0, 0.0) 2009-12-22 13:23:20 +00:00
Denny Tjahjanto 043356e8a9 homogenization_RGC.f90 >> just switching-off one of the debugging statement.
crystallite.f90 >> optimizing the perturbation algorithm for local tangent.
2009-12-22 12:28:02 +00:00
Christoph Kords 1f7aebfa4d new subroutine crystallite_orientations: calculates the orientation matrix and the euler angles and - in case of single grain ips - the misorientation for each neighboring ip.
The calculation of the misorientation is now done once in crystallite init and at the end of every FE increment. This saves a lot of time compared to doing it in dotState for every crystallite subinc.
2009-12-18 15:46:33 +00:00
Denny Tjahjanto 3ab5cdc770 Additional feature to the RGC scheme: The volumetric consistency constraint. This is implemented by penalizing any volumetric discrepancy which occurs due to severe relaxation. The penalty for volume inconsistency is described using a power-law model. The setting for this function can be done in the numerics.config via three new parameters, i.e., maxvoldiscrepancy_RGC, voldiscrepancymod_RGC and discrepancypower_RGC. For monintoring, an extra output variable in prescribed in the material.config in the RGC section, namely "(output) volumediscrepancy".
IO.f90 and numerics.f90 has been modified accordingly to accommodate these changes
2009-12-16 16:20:53 +00:00
Franz Roters 39d1932e2b corrected line parsing now counts all parts 2009-12-15 16:03:53 +00:00
Christoph Kords 01b7e88e5f adapted the material.config file to last changes in constitutive_nonlocal 2009-12-15 10:22:17 +00:00
Christoph Kords 26e9056f90 added stiffness state loop counter to nonlocal stiffness calculation 2009-12-15 09:03:04 +00:00
Christoph Kords d784153e0c constitutive_nonlocal:
- corrected flux term
- multiplication is now aware of dislocation type
- corrected change rate for "dipole size" dupper
- corrected term for dipole dissociation by stress change
- added transmissivity term in fluxes which accounts for misorientation between two neighboring grains (yet hardcoded transmissivity according to misorientation angle)
- added more output variables

constitutive:
-  2 additional variables "previousDotState" and "previousDotState2", which are used to store the previous and second previous dotState (used in crystallite for acceleration/stabilization of state integration)
- timer for dotState now measures the time for calls to constitutive_ collectState (used to reside in crystallite_updateState, which is not critical in terms of calculation time anymore) 

crystallite:
- convergence check for nonlocal elments is now done at end of crystallite loop, not at the beginning; we simple set all elements to not converged if there is at least one nonlocal element that did not converge
- need call to microstructure before first call to collect dotState for dependent states
- stiffness calculation (jacobian): if there are nonlocal elements, we also have to consider changes in our neighborhood's states; so for every perturbed component in a single ip, we have to loop over all elements; since this is extremely time-consuming, we just perturb one component per cycle, starting with the one that changes the most during regular time step.
- updateState gets a damping prefactor for our dotState that helps to improve convergence; prefactor is calculated according to change of dotState

IO:
- additional warning message for unknown crystal symmetry
2009-12-15 08:20:31 +00:00
Christoph Kords 07303d9506 - corrected math_misorientation subroutine 2009-12-15 07:34:53 +00:00
Christoph Kords 596b7f3727 - rearranged array with symmetry operations
- new subroutine "math_misorientation" which calculates misorientations (based on old subroutine "misorientation", which was not used previously)
- rendered some functions pure
2009-12-14 11:02:10 +00:00
Denny Tjahjanto cad278c3bc Introduce a randomness in the odd stress, using pre-factor rnd. 2009-12-09 10:33:00 +00:00
Franz Roters 9b1b612f67 added some examples 2009-12-08 15:31:50 +00:00
Denny Tjahjanto 1bf3b978eb modifying the criteria for the sum of microstructure fraction.
previously was:
if (the_sum /= 1.0_pReal) then (error 170)
this condition is too strict. it may give problem with some numerical truncation error.

now becomes:
if (abs(the_sum - 1.0_pReal) >= 1.0e-10_pReal) then (error 170)
2009-12-02 13:08:14 +00:00
Denny Tjahjanto 59d22d47b2 introduction of a possibility to have homogeneous element (all ips in one element are identical, sort of reduced integration)
and bugs-fixing in crystallite.f90, homogenization_RGC.f90, numerics.f90.
2009-11-24 15:00:25 +00:00
Denny Tjahjanto 6702cb3baa Introduction of a numerical viscosity into the RGC scheme to improve the convergent behavior and the numerical stability of the scheme (see: homogenization_RGC.f90). These changes have been incorporated in all related subroutines (homogenization.f90, IO.f90, numerics.config and numerics.f90). 2009-11-17 13:42:38 +00:00
Denny Tjahjanto cb88019aa6 introduced a flexibility in cut-backing scheme in homogenization.f90 and in crystallite.f90:
(1) subStepSizeHomog and subStepSizeCryst := size of substep when cut-back is applied (initially was hard-coded).
(2) stepIncreaseHomog and stepIncreaseCryst := step increase when calculation for substep converge (was also hardcoded).

introduced a possibility to choose different finite difference scheme, i.e., forward-, backward- and central-difference, for computing grain numerical tangent. note that central-difference scheme will slow down the computation significantly. please use it only if necessary.

parameters to set these new features have been included in numerics.f90 and numerics.config, whereas corresponding error messages have been introduced in the IO.f90
2009-11-10 13:36:27 +00:00
Luc Hantcherli 67f87486b1 in constitutive_dislotwin.f90:
in constitutive_nonlocal.f90:

Derivatives of shear rates w.r.t. resolved shear stress HAVE to be positive.
Computation of dgdot_dtauslip is now correct.
2009-11-06 17:46:12 +00:00
Philip Eisenlohr f96f9332cf added some comments and made sure that texture distribution among a large number of IPs is statistically sound. 2009-11-02 08:03:14 +00:00
Denny Tjahjanto 8f40c516bb added to the previous one 2009-10-30 10:00:17 +00:00
Denny Tjahjanto 2068346f6d just small changes in the 'default' value of RGC numerical parameters. 2009-10-30 09:54:52 +00:00
Christoph Kords 1e5a0318f3 don't do any cutbacks in homogenization when my materialpoint consists of only one grain. 2009-10-27 08:31:45 +00:00
Christoph Kords c766ba2e3a minimum substepping size in homogenization and crystallite is now controlled by two independent parameters subStepMinHomog and subStepMinCryst respectively.
deleted flush statements where they are not needed, since they seriously slow down computation.
2009-10-26 16:43:43 +00:00
Denny Tjahjanto f50d3291f9 sorry, back to the previous version. grain deformation output is part of crystallite.f90, no longer done by homogenization. material.config reflects the changes. 2009-10-22 16:59:24 +00:00
Denny Tjahjanto d344aaf3a0 added possibility to output individual grain deformation gradient in homogenization_RGC.f90 and the homogenization.f90 has been modified accordingly. see material.config for the key-words to output the individual grain deformation gradient in the homogenization block. 2009-10-22 09:24:05 +00:00
Philip Eisenlohr 1dcb80753c tidying up code and reversing order in debug timing output 2009-10-22 09:14:17 +00:00
Philip Eisenlohr 67f4bdfaa0 volume fraction where new twins may form is now limited to (1-F) instead of 1...
"relevantResistance" is set to 1 Pa as default
2009-10-22 08:58:14 +00:00
Philip Eisenlohr 5d01e30f77 deleted debugging statements that print out interaction/hardening matrixes 2009-10-21 13:41:49 +00:00
Philip Eisenlohr 5d5e7eb8f8 corrected uncritical mix-up of Ntwin and Nslip in reshaping fcc interaction (slip--twin) 2009-10-21 13:41:09 +00:00
Philip Eisenlohr 4e98935287 changed lattice_interaction matrices to (other:me) notation
fixed small mistake in hexagonal twin--slip interaction matrix

adopted above switched notation for hardening matrix calculation
shortened dotState by introducing dot_product notation
2009-10-21 13:10:12 +00:00