a329a9b91d
added flags for ifort and gfortran to use preprocessor
2012-02-09 13:30:59 +00:00
dced3f9430
changed FFT reporting of dimension and resolution to one line each.
2012-02-09 13:18:59 +00:00
0f7c74e02d
set ID flag and line endings
2012-02-09 13:06:22 +00:00
195491aaaa
added missing pInts
2012-02-09 12:35:55 +00:00
a26456f9c0
now handling capitals in restart argument correctly
2012-02-09 12:20:14 +00:00
d2bb7c10e5
new test for addCurl
2012-02-09 08:58:45 +00:00
e909efdad6
removed accidently inserted comments
2012-02-09 08:54:09 +00:00
aad69a6b7c
with the min # recycles set to 1 the compile-check (1101) runs now
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started to get hex-elastic (2101) up and running again with new test class
postprocessing to be done for both
2012-02-08 16:38:29 +00:00
eec2af6505
set min number of recycles to 1 for one-element Marc calculations
2012-02-08 15:19:47 +00:00
5a6cd1fc8f
slightly prettified handling of finite difference accuracy requesting
2012-02-08 12:01:38 +00:00
56ce779f57
generalized slip system idea of Christoph to field data of "special" dimension (i.e. not 3 or 9).
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dropped "norm"-suffix from input names of norms.
ASCIItable output is now called "normType" with type being Abs, Frobenius, or Max...
2012-02-08 12:00:31 +00:00
282e4a0360
scripts now figure out dimension and resolution on their own...
2012-02-08 11:18:15 +00:00
9c35e4e148
small polishing of help output.
2012-02-08 09:12:08 +00:00
51e8981ba3
not specifying the location of python executable directly, but rather getting it from $path, otherwise the scripts won't work on every machine
2012-02-07 13:09:10 +00:00
2f07faa0e2
norm capable of using different p-norms (abs norm, frobenius norm, and max norm). also able to handle "slipsystem" outputs (use option -s). number of slip systems can be set by option -i, if not 12 is default.
2012-02-07 13:02:56 +00:00
e7d407c2f6
crystallite_Fp has to be initialized in crystallite_init, cause it is used by constitutive_microstructure
2012-02-03 14:52:09 +00:00
5ddade27fc
changed Peierls stress to more realistic values for fcc
2012-02-03 13:12:45 +00:00
d62eddc0cd
corrected kinetics law and changed parameters. For solid solution hardening there are 3 parameters: the activation energy, the concentration of obstacles that determines the activation length and meanfreepath, and the obstacle size that determines the activation volume. For the Peierls mechanism there is: the width of doublekinks that determines the activation volume and the Peierls stress for edge and screw.
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Still testing needed to check whether the current formulation makes sense or not.
2012-02-03 12:50:54 +00:00
bbf4f25898
renamed subroutine "mesh_marc_get_mpieOptions" to "mesh_get_damaskOptions" which is now also used for abaqus and spectral input files. The only available option so far is "periodic", which allows for periodic fluxes in the specified direction. Examples for usage (add the following lines to the respective input file, in case of spectral file this goes into the header):
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- periodicity in x and z direction for marc:
$damask periodic x z
- periodicity in y direction for abaqus:
**damask periodic y
- periodicity in x and y direction for spectral:
periodic y x
2012-02-03 12:37:52 +00:00
a3e47b2d65
added method to return data as list of floats.
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safer check whether ASCII file has ended.
2012-02-02 17:13:51 +00:00
bffc22fbe1
major restructuring. packing stencil can be shifted to allow for element or nodal value averaging.
2012-02-02 17:12:48 +00:00
7e23f84d2c
new subroutine find_nearest_neigbor, basically a wrapper function for our purpose to kdtree2
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split up kdtree2.f90 again from math.f90 to make the files better accessible
2012-02-02 15:57:22 +00:00
72aeb2113a
minor improvement on the still not working long (polarization field based) algorithm
2012-02-02 13:20:09 +00:00
faed4ec232
added deallocation of arrays (fftw_free)
2012-02-02 13:19:35 +00:00
2e4f2f3d9c
added _pInt where appropriate
2012-02-02 13:19:02 +00:00
683384681a
doing average correction now in Fourier space, now sure that the constant term is correct.
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changed order of stress BC calculation/spectral method to avoid average calculation of stress in real space
2012-02-01 20:30:27 +00:00
c6fb2122be
added some comments for further debuggin/compliance with standard checking
2012-02-01 20:28:58 +00:00
c5128e94eb
some f2008 standard related correction i didn't check in last time
2012-02-01 20:20:05 +00:00
7dd67e3ebb
improved creation of material.config files, mostly done by Philip
2012-02-01 19:44:36 +00:00
590b10ee3e
not much
2012-02-01 19:43:11 +00:00
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
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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
93f311f2b9
now skips environment variables in comments, i.e. after '#'
2012-01-31 15:43:39 +00:00
80583fefb5
added compilation_info.f90, to store compilation date,time and compiler info in each file
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added #include statement at each init() routine
2012-01-31 14:54:49 +00:00
e87296b10a
added debug output for tests, corrected bug reporting number of successful tests
2012-01-31 13:10:14 +00:00
9b679c3c0b
switched to damask include instead of outdated damask_tools
2012-01-31 13:08:25 +00:00
8cf67e1be6
corrected weighting of difference divergence measures, added some additional output and introduced exit code 0 for successful termination.
2012-01-30 20:25:04 +00:00
9464937db7
merge declaration and initialization with standard values
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corrected handling of $DAMASK_NUM_THREADS
2012-01-30 20:16:19 +00:00
eeda357710
N^2 initialization loop (former spectralPictureMode) rewritten in material.f90
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additional output in DAMASK_spectral_interface.f90
132 character cut off in constitutive_nonlocal.f90
rounding error in math.f90 complex number initialization (1.0_pReal)*2.0_pReal*pi
new $DAMASK_NUM_THREADS warning in numerics.f90 / IO.f90
polishing in DAMASK_spectral.f90
2012-01-30 13:52:41 +00:00
7731926fec
two step renaming because otherwise svn get confused
2012-01-27 09:58:08 +00:00
2a89d9b81a
simplified compilation testing by introducing some small helper functions for common tasks, continued to rename
2012-01-27 09:55:19 +00:00
7c35e5a1cd
renamed to new numbering scheme, added first test cases for addDivergence
2012-01-26 17:29:26 +00:00
20a775e8d1
small improvements (more output to screen)
2012-01-26 15:26:21 +00:00
c6c9fd71de
marc compile test is compiling and running again, postprocess still not working
2012-01-26 15:23:41 +00:00
4edd824d8c
forgot homogenization.f90 in last commit
2012-01-26 13:51:01 +00:00
1330576a01
added new math function "math_deviatoric33" which returns the deviatoric part of a 3x3 tensor
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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
df931890e0
corrected typos
2012-01-26 12:50:04 +00:00
6fec57bbd7
replaced variable fraction by "timefraction"
2012-01-26 12:48:59 +00:00
27a976c04f
changed to new structure (using damask module)
2012-01-26 12:46:38 +00:00
5a658d1b82
dislocation velocity output for each dislocation type (edge+,edge-,screw+,screw-)
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for fcc constitutive_nonlocal_kinetics is called only once and the result is used for each dislocation type, for all other lattice structures we have one call for each dislocation type
2012-01-26 07:43:36 +00:00
e5407894b5
Reworked kinetics. Now there is a universal law which can be used for both fcc and bcc (and probably even hcp). It mainly consists of an athermal forest cutting part , solid solution and peierls as thermally activated processes, and viscous glide. Therefore, lots of new parameters in the material.config. Not sure yet if the values make sense though.
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Also renamed some of the old parameters.
Unknown constitutive output raises error.
2012-01-25 17:04:37 +00:00
Martin Diehl