Commit Graph

285 Commits

Author SHA1 Message Date
Christoph Kords 5f973a21c0 require all hardening coefficients/ non schmid coefficients to be specified in material.config, do not silently ignore any
warning message now more meaningful (?) when using less than maximum number of slip families
2013-09-12 14:47:09 +00:00
Christoph Kords 4ebf46d2ac nonSchmidProjection was reset to zero each time during instance loop in init, so entries from previous instances got lost; fixed that 2013-08-23 13:53:03 +00:00
Christoph Kords 1f77594ca0 dislocation velocity was not correctly stored to state in last version 2013-08-21 13:54:36 +00:00
Christoph Kords 4f8664baa3 in kinetics: non schmid stresses only influence peierls mechanism, but not solid solution hardening; as a result the derivative of the velocity with respect to the resolved stress has to be split into a Schmid and a non-Schmid part 2013-08-21 12:21:52 +00:00
Christoph Kords ec377a6e8e removed obsolete "dead zone" scaling 2013-08-21 08:39:43 +00:00
Christoph Kords f706ba3ff9 rearranged arguments of "constitutive_nonlocal_kinetics", got "tauTreshold" as argument, not complete state
don't call "constitutive_nonlocal_kinetics" twice for edges in case of nonSchmid behavior, but just call once and copy results from positive to negative edges
2013-08-21 07:55:34 +00:00
Christoph Kords 277972edbd "dv_dtau" argument in "constitutive_nonlocal_kinetics" not optional anymore
renamed "screwStressProjection" to "nonSchmidProjection"
2013-08-21 07:23:02 +00:00
Christoph Kords e909b825cc correction of hardening coefficients also enabled for bcc
for fcc: now applied to all hardening coefficients, not only hirth, lomer, and glissile
2013-08-14 11:44:30 +00:00
Martin Diehl c93373a4ac removed long lines 2013-08-08 19:33:21 +00:00
Christoph Kords f2d6703148 multiplication now sensitive of crystal structure, yet multiplication in bcc identical to fcc except for the contribution of edges which is completely dropped for bcc 2013-08-05 09:26:37 +00:00
Christoph Kords 813ed130b0 nonSchmid behavior now ready to use for bcc with phenopowerlaw and nonlocal constitutive model.
nonSchmid tensors according to Koester,Ma,Hartmaier,2012.
extended lattice_Sslip with non-Schmid tensors (the full non-symmetric tensors are required for the tangent and cannot be retrieved from the symmetrized Mandel notation)
2013-08-05 09:23:21 +00:00
Martin Diehl 40ace5c666 more documentation and parameters capitalization unified and using ipc in all modules (sometimes called gr)
nonlocal: only missing line continuation in string fixed
2013-07-01 06:10:42 +00:00
Philip Eisenlohr fd8d85896a error msg in case of unknown keyword was not properly trimmed --> 64kB of spaces... 2013-06-27 16:41:00 +00:00
Philip Eisenlohr 98528f9a89 added possibility for multi-level inclusion of files in *.config and loadcase files.
include subfiles by stating

{path/to/include}
2013-06-26 19:19:00 +00:00
Christoph Kords daf89806b1 fixed bug in deltaState; used to lead to unpredictable values in accumulated shear, since deltaState was not defined at this state position 2013-06-11 21:03:23 +00:00
Martin Diehl 296a5040b9 fixed bug in initialization when reading in material.config.
Fortran does not short-circuit, e.g. (if a>0 .and. b(a) ==c) might cause an out-of-bounds error when a=-1 it'll try to access b(-1)!
2013-06-11 20:16:40 +00:00
Christoph Kords a6361738fb (again!) fixed bug that was introduced in rev 2085: messed up indices of stiffness matrix in calculation of Poisson's ratio 2013-05-26 14:31:31 +00:00
Christoph Kords ab997f19ac fixed bug in nonlocal state init that was introduced in rev 2438 and used to reset states from other constitutions 2013-05-24 13:43:44 +00:00
Christoph Kords c0539d2383 replaced all remaining occurrences of state indices 2013-05-24 11:48:34 +00:00
Christoph Kords e2d970ce57 combined some state indices to an array with a more generic name 2013-05-24 09:02:30 +00:00
Christoph Kords ad4a66cb4e use named state variable indices in "deltaState" 2013-05-23 21:46:15 +00:00
Christoph Kords 332b207270 use named state variable indices in "kinetics" and "microstructure" 2013-05-23 21:40:00 +00:00
Christoph Kords 5900076d72 rename state variable index for critical resolved shear stress from "iTau" to "iTauF" 2013-05-23 21:32:36 +00:00
Christoph Kords ad2a245cdf use named state variable indices in "microstructure" 2013-05-23 21:28:45 +00:00
Christoph Kords c02645c996 use named state variable indices in "aTolState" 2013-05-23 21:13:56 +00:00
Christoph Kords f04a531e9b use named state variable indices in "stateInit" 2013-05-23 21:10:31 +00:00
Christoph Kords 65524b7f84 corrected named indices for state variables; however, not yet used 2013-05-23 20:30:06 +00:00
Christoph Kords e249366ded introduced named indices for state variables; however, not yet used 2013-05-23 20:15:23 +00:00
Christoph Kords 72129cae00 removed prefix "constitutive_nonlocal_" from all private variables 2013-05-23 19:56:36 +00:00
Christoph Kords b559666436 replaced FE_maxNipNeighbors with mesh_maxNipNeighbors, which is sufficient for memory allocation, since this gives the maximum of neighbors in all cp elements 2013-05-23 17:46:21 +00:00
Christoph Kords 77e9b80a16 bug fix for calculation of fluxdensity and slipnormal/direction in constitutive_nonlocal_postResults: indices for Fe were missing 2013-05-23 14:52:57 +00:00
Christoph Kords 41faa60323 fixed bug in backstress calculation for elements with periodic neighbors 2013-05-23 12:36:48 +00:00
Christoph Kords 3aaf60cffe polishing 2013-05-23 12:25:56 +00:00
Christoph Kords ec2503253e added output of slip direction and slip normal
changed name of fluxdensity outputs
2013-05-23 08:19:36 +00:00
Christoph Kords e758ee32be improved accuracy of accumulated shear output: take shear rate from LpAndItsTangent for time integration 2013-05-21 10:04:52 +00:00
Christoph Kords 3759024b42 forgot to set neighboring_rho (also reverting changes made in rev 2384) 2013-05-19 19:23:31 +00:00
Christoph Kords 0504fb3b21 reverted changes made in rev2384 2013-05-17 12:54:47 +00:00
Christoph Kords 6fac7c347c fixed bug in constitutive_nonlocal_kinetics that was introduced in rev2088 along with the non-Schmid behavior: nonSchmid matrix of last slip system was used for all slip systems; led to extremely bad convergence due to flawed dLp_dT 2013-05-10 22:29:12 +00:00
Christoph Kords d9cc42daef slight change in flux formulation: no flux to neighbor, not only if there is a sign change in the velocity, but also if the neighboring velocity is exactly zero 2013-05-10 08:42:42 +00:00
Martin Diehl b2a3c9235b fixed some warnings issued by gfortran (type conversion, not needed use statements) 2013-05-08 09:23:47 +00:00
Christoph Kords 6e64b5c476 better not allow for deads to contribute to flux, since not clear at which interface they got stuck 2013-05-07 18:47:17 +00:00
Christoph Kords a7706090d2 neighborhood relations were screwed up for some elementtypes as of version 2318, might have caused segmentation faults with nonlocal model, now fixed 2013-04-22 13:35:35 +00:00
Christoph Kords ad879ebcf9 forgot to delete all occurrences of obsolete "constitutive_nonlocal_ accumulatedShear" in last commit 2013-04-08 08:51:12 +00:00
Christoph Kords 10e50bf41d improved accuracy of "accumulated shear": now added as a state variable, which facilitates integration (dotstate=shearrate); needs absolute tolerance value for state integration in material.config 2013-04-04 13:37:14 +00:00
Christoph Kords 3c25723139 - make sure that formerly blocked density is not able to move to neighbor until it is remobilized
- added some explicit indices instead of ":"
2013-04-03 16:29:48 +00:00
Christoph Kords 6d3f05b387 small changes in nonlocal constitutive model:
- make sure neighboring density is always greater equal zero
- no extra Bauschinger in postResults
2013-04-03 16:22:55 +00:00
Christoph Kords b8f8d66f82 total density used in backstress calculation now based on average of neighborhood
fixed small bug in state_init: random distribution of density was probably not working correctly, as some variables were not properly initialized
2013-03-27 13:04:01 +00:00
Christoph Kords 19655c2d92 significantRho check was flawed for dipole density 2013-03-25 17:36:04 +00:00
Franz Roters 02f092492e updated copyright header 2013-03-22 17:35:05 +00:00
Christoph Kords cee90bbdb3 simplified dislocation kinetics: dropped relativistic correction of velocity, since the infinite attack frequency already sets a limit for the velocity; dropped second; also dropped the correction term for backward jumps, since it was probably not meaningful 2013-03-21 12:52:29 +00:00
Pratheek Shanthraj 07ff1f7c93 reporting current time for most module inits 2013-02-25 16:34:59 +00:00
Philip Eisenlohr c1cf446774 parsing of material.config file now expects adequate number of (slip/twin) family entries according to given lattice type.
used to read up to maxN, but that caused unnecessary IO_warnings...
2013-02-14 22:24:55 +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
Mahesh Balasubramaniam 362cbf3359 Made corresponding changes in the constitutive files and DAMASK_spectral_driver and interface files with respect to the changes made to IO.f90 2013-02-06 16:45:34 +00:00
Martin Diehl e74b5da19a changed all remaining routines to fortran-fast arrays (geometry reconstruction etc.)
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
Pratheek Shanthraj 50e874f887 fixed bug in elasticity matrix calculation 2013-01-22 15:48:47 +00:00
Martin Diehl df089b94bd line break in lines > 132 2013-01-22 11:06:39 +00:00
Martin Diehl 2b319f02e6 small corrections on changes related to non-schmid systems 2013-01-22 10:04:15 +00:00
Pratheek Shanthraj f3bd920c23 added non-schmid structure 2013-01-21 23:50:28 +00:00
Pratheek Shanthraj 60fec0e8ec added code structure for non-schmid mechanics. work in progress… 2013-01-21 23:11:16 +00:00
Pratheek Shanthraj fd94c786f0 moved stiffness tensor calculation to lattice
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
Martin Diehl 093cf92338 remove omp statements during initialization, "line" for reading in from material.config now has a default (empty) value to prevent conditional jump depend on this value 2013-01-08 22:11:59 +00:00
Christoph Kords f14fd45ce1 new material parameter "egdejog": fraction of annihilated screw dipoles that forms edge jogs 2012-12-23 12:56:15 +00:00
Christoph Kords 03a88d4798 fixed timesyncing for special case of ip that synchronizes its time step, but does not have a neighbor 2012-12-11 13:38:36 +00:00
Christoph Kords 37028455e9 always use the current state for leaving flux calculation when no neighbor is present 2012-12-09 12:24:32 +00:00
Christoph Kords 149c747688 use non-corrected densities for rate check in dotState 2012-12-06 17:14:35 +00:00
Christoph Kords 1f5a30d6f0 corrected typo in random multiplication term 2012-12-06 14:04:18 +00:00
Christoph Kords 20f7053ad3 correction of interaction coefficients due to line tension effect only applies to coefficients 3, 4 and 5 2012-12-04 18:23:46 +00:00
Christoph Kords 9eb89b0050 made random multiplication switchable via material.config 2012-12-03 12:59:38 +00:00
Christoph Kords 62ddbf26df slightly changed the multiplication term in the nonlocal model for the starvation case 2012-11-29 18:50:25 +00:00
Christoph Kords f92d34dd22 removed some unused variables 2012-11-29 18:44:00 +00:00
Christoph Kords 29618df550 annihilate only part of the screw dipoles (specified by minimumDipoleHeight), not all; moved annihilation of screws from deltaState back to dotState 2012-11-28 12:09:48 +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 4195d53d11 message of last commit was incomplete: moved annihilation of screw dipoles from dotstate to deltaState, since it is not a rate 2012-11-17 13:54:22 +00:00
Christoph Kords 467c186f0f annihilation of screws 2012-11-17 13:50:20 +00:00
Philip Eisenlohr d9a98417ca switched element library to geomType based.
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 5b6baa7c0d introduced distinction between ip coordinates and cell center coordinates; the former can be globally calculated by subroutine mesh_build_ipCoordinates, the latter locally by the function mesh_cellCenterCoordinates; renamed mesh_ipCenterOfGravity to mesh_ipCordinates 2012-11-06 14:37:13 +00:00
Christoph Kords 55dc286be2 corrected limit for upper stable dipole distance; fixed a bug in the postResults where division by zero might happen 2012-10-29 13:02:01 +00:00
Christoph Kords f666f8dcf3 added possibility to scale the plastic shearrate by the ratio of mobile to total density; keyword in material.config is "deadZone" 2012-10-29 12:49:28 +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.
Also changed some debugging levels in crystallite and mainly in constitutive_nonlocal
2012-10-22 07:59:35 +00:00
Christoph Kords 3ecaa9e371 modified multiplication term in order to mimic a discrete distribution of dislocation sources; namely, at high resolution, when there is (on average) less than one source per integration point, a random generator decides whether there is a source in the finite volume or not; if there is one, then the multiplication turns independent of the density and depends only on the velocity/volume times a scalar factor; recovers density*velocity/lambda for large finite volumes 2012-10-19 11:40:17 +00:00
Christoph Kords e4054c116d fixed problem with gnu compiler: allocation of variables in constitutive_nonlocal_stateInit was not safe when not using any nonlocal constitution
put header of debugging output in constitutive_init at the start of the function in order to make debugging easier
2012-10-09 12:34:57 +00:00
Christoph Kords a84e0529c3 make correction of hardening coefficients thread safe 2012-10-05 16:05:51 +00:00
Christoph Kords 40a2e652e7 introduced material parameter "linetension", which indicates how strong the effect of the line tension on the hardening coefficients is 2012-10-05 14:42:41 +00:00
Christoph Kords 7cc6108a04 hardening coefficients for fcc are density dependent (line tension effect, Devincre, Kubin, Hoc; 2006; Physical analyses of crystal plasticity by DD simulations)
fixed bug with thermal annihilation producing negative density in case of very small dipole density and high climb velocity
2012-10-04 18:08:40 +00:00
Christoph Kords bce8012c89 random distribution of initial dislocation density now really independent of meshsize 2012-10-02 15:26:58 +00:00
Christoph Kords 91b7883c2a random distribution of initial dislocation density now independent of mesh size 2012-10-02 13:35:34 +00:00
Christoph Kords 1502a71f0c added possibility to start with an initial random distribution of dislocation segments with specific overall density 2012-10-02 12:57:24 +00:00
Christoph Kords 29023cea3c minor correction of debugging output 2012-09-05 11:19:46 +00:00
Christoph Kords f153866030 introduced factor to control edge contribution to multiplication;
dislocation density below a single dislocation per IP considered not significant
2012-09-04 16:56:37 +00:00
Christoph Kords d80b45c1d9 added relativistic correction of velocity (maximum velocity given by parameter in material.config); probability of thermal activation in velocity law not allowed to be greater than one.
output of creation rate for edge jogs now for own system, not collinear.
check for negative densities in dotState now uses absoluteToleranceRho instead of significantRho.
2012-08-30 07:33:13 +00:00
Christoph Kords f3e7b3cec8 added separate output of dipole formation rate for edge and screw 2012-08-27 15:57:31 +00:00
Christoph Kords 9214da4465 added missing labels to list of available outputs 2012-08-27 12:41:57 +00:00
Christoph Kords 3cd5fa90e8 corrected dislocation multiplication term for special case of zero density 2012-08-24 11:36:46 +00:00
Christoph Kords 4f67d04c69 new parameter "significantRho" for nonlocal constitutive law ; density below this value will hardly contribute to dislocation glide or any dislocation reaction ; old parameter "absoluteToleranceRho" is now used only for its initial purpose, namely the absolute tolerance in the state integration 2012-08-23 05:48:21 +00:00
Christoph Kords 222aed9f60 derivative of velocity with respect to resolved stress was flawed; now much better convergence of stress integration for nonlocal constitutive law 2012-08-21 14:40:01 +00:00
Christoph Kords b2aacf9ca4 rates in constitutive_results are taken directly from last converged step and not calculated again; added output of rates for annihilation of screws and deposition of edge jogs on collinear system 2012-08-16 11:03:22 +00:00
Christoph Kords bd754dbefd corrected debug output of evolution rates; added possibility to change the safety factor for the CFL flux condition via the material.config file; updated the example material.config due to recent changes in nonlocal constitutive 2012-08-16 09:13:38 +00:00
Christoph Kords f5e7d576f1 introduced annihilation of screw dipoles; so far no thermal activation, but immediate annihilation; each annihilated screw dipole leaves behind an edge jog of same length as the dipole height on the collinear system 2012-08-14 12:26:20 +00:00
Christoph Kords a48d180f8c allow prefactor for self-diffusion to be equal to zero 2012-08-06 09:03:33 +00:00