Pratheek Shanthraj
|
197ae53553
|
lots of memory savings (~ stateside + 250 pReals per integration point) when using analytic jacobian
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2015-08-28 10:55:38 +00:00 |
Martin Diehl
|
6848d83d13
|
behavior of IO_stringPos was unsafe in some situations, also took the chance to rename the variables used in its context to a more meaningful name.
functions in the core module are not used, including kdTree
|
2015-08-28 07:38:48 +00:00 |
Martin Diehl
|
1171dc4344
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MPI has a 2GB limit for writing at once, now chunking
|
2015-08-21 17:51:05 +00:00 |
Martin Diehl
|
8474da26d9
|
empty line
|
2015-08-18 16:31:47 +00:00 |
Martin Diehl
|
bae5cfcf89
|
named if
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2015-08-18 16:07:01 +00:00 |
Tias Maiti
|
53c574033a
|
size of MAXCHUNKS same as maximum allocated size for “heat_time” & “heat_rate”
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2015-08-18 03:20:16 +00:00 |
Martin Diehl
|
f64a5e7552
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output safe for 64bit integer
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2015-08-14 05:03:54 +00:00 |
Martin Diehl
|
31ea4dadf1
|
IO_stringPos replacement not needing MAXNCHUNKS but making use of new Fortran features for dynamic allocation
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2015-08-13 14:54:34 +00:00 |
Martin Diehl
|
563d9e64dd
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MAXNCHUNKS capitalized since it is a parameter
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2015-08-06 09:24:56 +00:00 |
Pratheek Shanthraj
|
3d94ae4074
|
finite strain correction for respective expansions
|
2015-08-05 14:12:54 +00:00 |
Tias Maiti
|
09c7affbbc
|
more efficient rate calculation in updateState when subdt is zero
|
2015-08-05 11:09:38 +00:00 |
Tias Maiti
|
7928ce3ac3
|
fixed erroneous rate calculation in updateState when time increment (subdt) was zero during initialization.
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2015-08-04 21:27:30 +00:00 |
Tias Maiti
|
65d114e4f0
|
improved debug statements
|
2015-08-04 21:26:22 +00:00 |
Pratheek Shanthraj
|
905b9f8f42
|
petsc update (now v3.6.1)
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2015-08-04 15:04:53 +00:00 |
Pratheek Shanthraj
|
5b57ea7d16
|
fluctuations proportional to thermal equilibrium concentration
|
2015-08-03 11:08:59 +00:00 |
Pratheek Shanthraj
|
a01d7d8d66
|
corrections to crystallite_push33ToRef function
|
2015-08-03 11:07:19 +00:00 |
Pratheek Shanthraj
|
1ed276ce2d
|
quadratic softening for finite dissipation energy
|
2015-07-30 10:29:25 +00:00 |
Pratheek Shanthraj
|
c97b83c9a1
|
added user defined external heat source
|
2015-07-27 11:09:37 +00:00 |
Pratheek Shanthraj
|
4bb6664de9
|
tightened default thermal tolerance
|
2015-07-27 11:08:43 +00:00 |
Pratheek Shanthraj
|
c82c4b74f1
|
updated config files to reflect recent changes in input parameters
|
2015-07-24 17:14:03 +00:00 |
Pratheek Shanthraj
|
5e09954575
|
remove deprecated spectral load case definition of temperature
|
2015-07-24 14:57:29 +00:00 |
Pratheek Shanthraj
|
7554647c8e
|
more control over initialisation of field values. specify initial field value in the homogenisation part of the material config file using the appropriate tags
|
2015-07-24 14:53:50 +00:00 |
Pratheek Shanthraj
|
87d42bf447
|
initialise Fi correctly for initial field values away from equilibrium
|
2015-07-24 14:47:18 +00:00 |
Pratheek Shanthraj
|
0a5ccb3d91
|
possibility to set damage potential order
|
2015-07-24 14:43:05 +00:00 |
Tias Maiti
|
7c101cdc31
|
fixed issues causing compilation errors
|
2015-07-23 19:22:03 +00:00 |
Tias Maiti
|
7f8a8d5b0f
|
new function to report initial thermal strain based on current temperature deviation from reference.
to be used in constitutive_initialFi, which collects from all kinematics, derives and sums Li terms to report initial Fi.
|
2015-07-23 15:59:25 +00:00 |
Philip Eisenlohr
|
25a03e128a
|
added remark to include looping over sources of same type within one phase. (for instance to accommodate different activity periods.)
|
2015-07-16 17:20:18 +00:00 |
Su Leen Wong
|
d2c748e716
|
TRIP input parameters for fcc to hex
|
2015-07-10 09:02:48 +00:00 |
Luv Sharma
|
1e9682eef9
|
corrected upper bound for spectral damage solver as well.
|
2015-07-09 15:51:34 +00:00 |
Shaokang Zhang
|
d2bfd26937
|
1) added the error message of all MPI plans 2) deleted the suffix (MPI) for all MPI plans
|
2015-07-09 13:38:21 +00:00 |
Su Leen Wong
|
7a4415b28a
|
Sanity checks for SFE
|
2015-07-08 15:37:16 +00:00 |
Su Leen Wong
|
df5cdb6b01
|
Elasticity matrices for transformed phase
|
2015-07-08 11:58:52 +00:00 |
Su Leen Wong
|
66564c1f75
|
Read in elastic constants for transformed phase
|
2015-07-07 13:23:56 +00:00 |
Luv Sharma
|
4435244681
|
corrected missing initialization. newState = oldState + deltaState. But for irreversibility driving force must be compared with last converged subState.
|
2015-07-06 09:34:43 +00:00 |
Luv Sharma
|
3d5a85e4af
|
corrected implementation of deltaState for isoBrittle damage
|
2015-07-06 08:47:40 +00:00 |
Martin Diehl
|
72b7df34a3
|
save some space
|
2015-07-02 09:45:25 +00:00 |
Aritra Chakraborty
|
74af77a81f
|
formatted the interaction matrix for beta-Sn
|
2015-07-02 05:45:56 +00:00 |
Aritra Chakraborty
|
0e6ac411bb
|
further modified to add longer lines for (bct) beta-Sn in lattice
|
2015-07-02 05:44:45 +00:00 |
Martin Diehl
|
6272129f01
|
formatted code and modified Makefile to have long lines in lattice
|
2015-07-02 05:09:07 +00:00 |
Aritra Chakraborty
|
e61050dcde
|
added lattice for (bct) beta- Sn.
|
2015-06-27 14:55:30 +00:00 |
Shaokang Zhang
|
a40d247f7f
|
lower bound for damage is residual stiffness
|
2015-06-22 14:27:32 +00:00 |
Su Leen Wong
|
12bc4f01ef
|
fcc to hex orientation relationship (Shoji-Nishiyama)
|
2015-06-22 13:47:15 +00:00 |
Su Leen Wong
|
ad17c40d92
|
Renamed variables to denote fcc to bcc transformation
|
2015-06-22 08:33:48 +00:00 |
Su Leen Wong
|
5114e0b43e
|
Cleaning up
|
2015-06-22 08:10:20 +00:00 |
Philip Eisenlohr
|
3e0e187b14
|
clarified meaning of symEulers function in help
|
2015-06-19 07:29:01 +00:00 |
Franz Roters
|
b1c036daab
|
added some comments on possible code changes
|
2015-06-17 06:53:00 +00:00 |
Franz Roters
|
0e48fb8fc7
|
removed double entry in use list
|
2015-06-16 07:57:42 +00:00 |
Su Leen Wong
|
081bc33159
|
Read in c/a ratio for transformed hcp phase
|
2015-06-12 08:59:39 +00:00 |
Su Leen Wong
|
a370372c1b
|
transformed lattice structure should not be mandatory
|
2015-06-11 17:03:34 +00:00 |
Pratheek Shanthraj
|
40701cedc4
|
damage driving force is a history variable and damage field is strictly bounded between 0 and 1
|
2015-06-11 09:03:51 +00:00 |