Commit Graph

172 Commits

Author SHA1 Message Date
Su Leen Wong c2ee6ff299 Renaming transformation input variables to more logical names 2014-09-23 15:38:41 +00:00
Pratheek Shanthraj 556d485ca4 typo: diffusion not difusion 2014-09-23 12:30:52 +00:00
Pratheek Shanthraj 5ce49387f6 added history variable for brittle damage to prevent healing. renamed/removed some lattice damage tensors and symmetrize them. 2014-09-23 12:22:34 +00:00
Pratheek Shanthraj 6ace12be0c removed unused variables 2014-09-22 20:34:42 +00:00
Luv Sharma e83a0fb3f7 polished field state related changes and brittle damage 2014-09-22 18:15:19 +00:00
Martin Diehl 7cb7815176 polishing style 2014-09-13 10:04:44 +00:00
Su Leen Wong f8646daf85 Added projection matrix for strain-induced transformation 2014-09-12 09:10:19 +00:00
Martin Diehl 5b6f143fb0 intel fortran behaves strange for standard check:
https://software.intel.com/en-us/forums/topic/506419
worked around that
2014-09-11 16:02:05 +00:00
Luv Sharma dc406a01c0 added funtions to get averged properties at integration points. 2014-09-10 08:37:12 +00:00
Su Leen Wong 5f1e49c053 Cleaner way of calculating the Bain strain 2014-09-01 10:47:48 +00:00
Su Leen Wong 565e703f49 Minor fix for now 2014-09-01 09:30:33 +00:00
Pratheek Shanthraj fc941a6436 fixed some bugs in previous commit 2014-09-01 08:57:34 +00:00
Su Leen Wong e8a3b7ed19 Pitsch orientation relationship for phase transformation 2014-08-29 13:03:48 +00:00
Su Leen Wong 1da874a6db Modification of basic states for phase transformation 2014-08-14 13:18:33 +00:00
Su Leen Wong 591a82de26 Fixed issue with previous commit 2014-08-14 12:21:51 +00:00
Su Leen Wong 5719987f95 Calculation of eigendeformation tensor for phase transformation 2014-08-14 10:04:13 +00:00
Su Leen Wong 1707f7d367 updated to read in TRIP parameters 2014-07-22 07:43:03 +00:00
Pratheek Shanthraj 4af3459424 fixed bug in symmetrizing 2nd order tensor 2014-07-08 01:02:29 +00:00
Martin Diehl 8fa2dcffbd changed to new state, please report bugs to Luv or Martin 2014-07-02 12:27:39 +00:00
Pratheek Shanthraj 0c66204904 reference temperature for thermal problems parsed and stored in lattice 2014-06-24 22:54:19 +00:00
Pratheek Shanthraj 9cdee47500 now parsing thermal conductivity, thermal expansion coeff and damage tensor from material config if present and symmetrizing according to lattice structure. setting up for multi physics 2014-06-24 13:48:29 +00:00
Pratheek Shanthraj bf24bd83f2 fixed error check for CoverA ratio 2014-06-18 13:26:16 +00:00
Martin Diehl eaa3e32f21 improved warning and error messages 2014-06-18 09:10:16 +00:00
Martin Diehl 488927a231 worked on phenopowerlaw test, made material.config writer case insensitive, polished lattice, removed deprecated part of documentation 2014-06-16 13:11:26 +00:00
Martin Diehl da8f10fe6f consistency checks for lattice type improved 2014-06-13 08:57:00 +00:00
Martin Diehl d9e8e8fc10 added consitency check: At least one phase must be present 2014-05-21 13:03:59 +00:00
Christoph Kords c027e8e1a8 added comment and citation for non-Schmid matrices for bcc 2014-04-30 09:56:30 +00:00
Martin Diehl 4bb5439994 removed copyright from *.f90 and *.f files, will be added using the deployMe script for release/nightly build. Now based on presence of svn:keywords property set (usually "Id"). Similar thing will be done for .py, .sh, and .config files but more involved because they might be executable 2014-03-29 08:20:36 +00:00
Martin Diehl ef8fbf4dda introduced case in dislotwin for bcc (peierls stress as critical stress)
renamed some parameters, now exponents (p,q) for slip are per family, shear band got own ones. exponent for twin (r) now per family

fixed bugs in lattice ("empty" interactions should be 1 not zero)

see both Phase examples to check what is needed
2014-03-11 17:40:59 +00:00
Martin Diehl 721183e702 removed some forgotten debug statements 2014-03-08 22:51:32 +00:00
Martin Diehl 2b589c3d71 moved reading in of lattice type and elastic constants to lattice module
removed structure type for hex, fcc, bcc, now defining slip/twin systems for each phase found in material.config
constitutive modules will only be initialized if needed
homogenizedC function is only needed for models incorporating twinning in a physical way (titanmod and dislotwin)
2014-03-08 20:50:31 +00:00
Martin Diehl 32493675d6 fixed bug in constitutive introduced in rev 2988 causing wrong names in *.outputConstitutive 2014-03-05 08:06:21 +00:00
Martin Diehl a0d75ee05e moved quaternion disorientation to lattice because it requires the knowledge of the lattice structure. 2014-02-28 13:28:27 +00:00
Martin Diehl fe13bb16fe added some consistency check and remove unnamed constants 2014-02-27 18:57:46 +00:00
Martin Diehl 69992638a8 added missing covera_ration in hex test. was not necessary before for constitutive_none, now it is 2014-02-17 09:45:54 +00:00
Martin Diehl 4efb1e5617 fixed bug: wrong initialization of lattice structure, had effect on j2 and phenopowerlaw 2014-02-14 18:05:59 +00:00
Martin Diehl d45aea4467 moved reading in of lattice stru 2014-02-10 14:31:19 +00:00
Martin Diehl 9f3a17b1b6 fixed bug in hexagonal slip system definition 2014-01-15 12:08:46 +00:00
Martin Diehl 95d6430b09 improved on enums (introduced them for output in j2), fixed wrong recursion depth bug in IO, fixed a bug in reading in for none, j2, phenopowerlaw 2013-12-11 22:03:09 +00:00
Martin Diehl 7885ebaf8f added 'reset' flag for recursive function IO_read, need to reset stack when stopping exectution (will be used by constitutive and homogenization) 2013-12-11 16:49:20 +00:00
Martin Diehl 0bc99a9622 change latticeName to latticeID 2013-11-27 16:20:27 +00:00
Philip Eisenlohr 0a292d8d8b fixed final bug in hex twintwin matrix 2013-10-15 22:02:39 +00:00
Martin Diehl ed47d25adc remove dotTemperature (returned always 0 anyway) to make it easier to replace it with a heating rate funtction
remove potentially dangerous short circuiting in homogenization files
added doxygen comment for nonlocal (giving the functions a name)
fixed wrong definition of maxnchungs introcuded into dislotwin with last commit, causes trouble with hex
2013-10-09 06:12:16 +00:00
Philip Eisenlohr 0a7052a7da fixed two errors in hexagonal slipslip and twintwin interaction matrix 2013-10-08 13:52:19 +00:00
David Mercier ce926aaf1f Minor contribution :
- add SVN keyword to the material.config file for cp-Ti
- add comments in lattice file
2013-09-19 09:17:09 +00:00
David Mercier a8eb6a985e - Addition of an example of a material.config file for hcp material (cp-Ti).
- New Error Message #214 when elastic constants are not correctly defined.
- Error message when the c/a ratio for hcp is higher than 2 (no physical sense).
2013-09-17 12:20:50 +00:00
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 39c05e0d9e for bcc: exchanged 2nd and third hardening coefficient to be consistent with fcc; now 2nd is coplanar and 3rd is collinear; added newer reference concerning the bcc hardening coefficients 2013-08-14 11:47:03 +00:00
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
Christoph Kords 3749cd5564 changed "math_AxisAngleToR" to "math_axisAngleToR" to be consistent with spelling in math.f90 2013-07-22 09:43:35 +00:00
Philip Eisenlohr 8ccdfb27f3 reworked the hexagonal slip system order and adjusted interaction matrices to a logic that facilitates later system additions without altering existing structure. 2013-07-01 14:01:42 +00:00
Franz Roters 4a291dc372 implementation of twin nucleation criteria according to Davids PhD thesis
applies for fcc crystal structure only
2013-07-01 13:06:01 +00:00
Philip Eisenlohr 81cdd2b1cc added second type prismatic slip system for hexagonal lattices as 6th slip family.
consequently, 4 new interaction types (21,22,23,24) available for slip/twin and twin/slip.

interaction of slip/slip got rearranged and now has 42 types...
list of former --> new:
6	7
7	8
8	9
9	10
10	11
11	13
12	14
13	15
14	16
15	18
16	19
17	20
18	22
19	23
20	25
21	28
22	29
23	30
24	31
25	33
26	34
27	35
28	37
29	38
30	40
2013-06-14 10:20:31 +00:00
Martin Diehl 85d4a37d95 moved public data res,size and homog from mesh to DAMASK_spectral_utilities (as grid and geomSize) 2013-05-08 15:52:29 +00:00
Franz Roters 02f092492e updated copyright header 2013-03-22 17:35:05 +00:00
Martin Diehl 3e2ecbe0a3 added time stamp to init of lattice 2013-03-07 22:45:00 +00:00
Martin Diehl 7e0ea5dd04 hickups in doxygen documentation fixed 2013-03-05 14:35:26 +00:00
Christoph Kords 62e55483f7 fixed bug in lattice: line continuation character was missing 2013-02-27 10:49:23 +00:00
Martin Diehl bac186c5b7 removed 2003 standard initialization expression not supported by ifort so far 2013-02-27 07:35:53 +00:00
Martin Diehl 0be6706483 some more detailed doxygen comments 2013-02-26 19:01:31 +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 e644c6dbc5 improved reading in of values, now only warnings in case of problematic entries in material.config
divergence calculation sqrt scaling optionally introduced for basic scheme spectral solver
2013-02-08 15:55:53 +00:00
Martin Diehl 2b319f02e6 small corrections on changes related to non-schmid systems 2013-01-22 10:04:15 +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
Philip Eisenlohr 1e32eb560e corrected buggy calculation of Schmid matrix for twins introduced in rev1809.
(stress acting on twin systems was overestimated by factor of sqrt(3) due to that!!)

additional polishing.
2012-11-23 17:02:50 +00:00
Nader Zaafarani dc5cd8a4c4 A modified twin-twin interaction matrix for BCC is introduced.
An introduction of a third parameter at the interactionTwinTwin in the material.config for BCC-dislotwin materials is essential.
2012-11-16 13:39:08 +00:00
Nader Zaafarani c0a5a1dfd1 Formation of the Slip-Slip interaction matrix for BCC. 2012-11-14 17:35:33 +00:00
Martin Diehl 1896c07c70 corrected some bugs in the last commits 2012-11-14 14:33:41 +00:00
Nader Zaafarani c8be3a03bd The twin system <111>{112} for BCC is introduced. 2012-11-14 13:43:59 +00:00
Nader Zaafarani 6b010b4a46 Twin-slip interaction matrix for BCC is set to 0. 2012-11-14 11:53:22 +00:00
Nader Zaafarani b0464ad176 A modified slip-twin interaction matrices for FCC and BCC are introduced.
The shear twin value for BCC is corrected.
An introduction of a third parameter at the interactionSlipTwin in the material.config for dislotwin materials is essential.
2012-11-14 11:13:16 +00:00
Philip Eisenlohr fb2981b4c4 switched matrix indices in SlipSlip, SlipTwin, TwinSlip, and TwinTwin such that first index refers to first name and second to second... 2012-11-14 10:27:23 +00:00
Philip Eisenlohr 79a5a30a90 removed now obsolete vectorproduct variables st, tt... 2012-10-18 07:25:49 +00:00
Philip Eisenlohr 31f20e51da just to be able to tell about the bug I found in the hex slip systems---which I actually forgot to mention during the last commit---I slipped in a syntax error that now is fixed, too... 2012-10-12 20:31:50 +00:00
Philip Eisenlohr 82a13af474 tidied up the Schmid matrix calculations.
added internal check against dilatation in Schmid matrices.
2012-10-12 17:59:50 +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 0434ef3daa some comments to be seen in documentation 2012-08-15 13:38:38 +00:00
Philip Eisenlohr 4d09ef0648 changed variable name "debug_what" to "debug_level" 2012-07-05 09:54:50 +00:00
Martin Diehl dbdc7ddfa2 debug.config, debug.f90, DAMASK_abaqus_exp.f, DAMASK_abaqus_std.f: changed to new debug scheme (wasn't working)
lattice.f90, FEsolving.f90: explicitly defined public functions and variables, all others are now private
numerics.f90: changed output format of real numbers, now instead of 0.1eX 1.0e(X-1) is printed to screen
Makefile: now using correct Optimization flags for OPTIMIZATION=AGGRESSIVE
DAMASK_spectral_AL.f90: improved, but still testing. Stress BCs now seem to be handled correctly
2012-03-20 18:01:31 +00:00
Martin Diehl bd9667bd4b added new, flexible debugging scheme.
now all modules have their own debug specification.
compiles and runs, I hope nothing is broken
did a lot of polishing
2012-03-08 20:25:28 +00:00
Martin Diehl 23cda48709 cleaning up, removing includes not needed 2012-02-21 15:42:47 +00:00
Martin Diehl 6c0f9d163b polishing: removed variable names like 'unit' and 'data' that are keywords of fortran and ensured that integer and real precision matches independent of machine standard.
removed cut_off parameter for damask_spectral
removed outpot of derived divergence measures and added RMS output in brackets
added comments and options to the makefile
2012-02-15 18:58:38 +00:00
Christoph Kords c786336af3 reordered (and partly redistributed) error message identifiers, deleted those which are not in use anymore.
all constitutive as well numerics now raises an error, if an unknown keyword is found in the respective config file
2012-02-13 17:41:27 +00:00
Martin Diehl 37ac7bf1b4 fixing inconsistencies in variable assignments 2012-02-10 11:56:05 +00:00
Martin Diehl 800e291240 made code standard conform to Fortran 2008 (ignoring warning concerning comments beyond character 132). Basically, changing "x" format specifier to "Nx" ("1x") plus removing $ format specifier
added compiler switches for gfortran and ifort to check for standard conformity
old gnu compilers <4.4 are not longer supported because they don't provide the c binding for fftw
2012-01-31 19:18:55 +00:00
Martin Diehl 80583fefb5 added compilation_info.f90, to store compilation date,time and compiler info in each file
added #include statement at each init() routine
2012-01-31 14:54:49 +00:00
Christoph Kords 1330576a01 added new math function "math_deviatoric33" which returns the deviatoric part of a 3x3 tensor
renamed some math functions, so that we have a universal naming scheme: for matrix multiplications use an "x" (e.g. math_mul33x3); don't use the "x" to describe the shape of the tensor that the function is applied to (e.g. math_invert33 instead of math_invert3x3)
2012-01-26 13:50:00 +00:00
Philip Eisenlohr a7d9d711f6 edited lines exceeding 132 chars (before any comment started) 2012-01-11 16:56:35 +00:00
Martin Diehl c35ea33f8e did a lot of polishing:
- removed unnecessary "return" before end of subroutine or function:
- changed undetermined array length (:) to (1:3)

To prevent problems with some code analysing tools:
- "3D oneliner loops" (with ";) only for "do" and "enddo" at the same time
- removed line continuation in OMP statements

made the makefile more flexible, removed heap-arrays switch
2011-09-13 15:54:06 +00:00
Martin Diehl fe9754a41c previous commit was wrong file 2011-09-02 10:46:37 +00:00
Martin Diehl 43e2684cfb added new glide system for hex lattice 2011-09-02 10:43:49 +00:00
Martin Diehl 75c67f53f7 introduced alternative location for material configuration.
If present, the >>>JOB.materialConfig<<< file takes precedence over the standard >>>material.config<<<
2011-08-02 10:14:16 +00:00
Franz Roters 7d84a0911e removed unused variables 2011-04-13 14:16:22 +00:00
Franz Roters c1b8391110 changed enconding of all source files to UTF-8 without BOM (signature) Codepage 65001 2011-04-07 07:20:28 +00:00
Franz Roters fcdb805225 added copyright text to all f90 (free) format files 2011-04-04 14:09:54 +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)
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 235266b169 openmp parallelization working again (at least for j2 and nonlocal constitutive model).
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
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.
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