Nan Jia
211f66a728
added elastic stiffness matrix as crystallite output
2012-03-01 13:06:09 +00:00
Christoph Kords
8dc6e256c0
choose textures and phases of example materials according to what the labels suggest
2012-02-21 13:16:59 +00:00
Christoph Kords
5ddade27fc
changed Peierls stress to more realistic values for fcc
2012-02-03 13:12:45 +00:00
Christoph Kords
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
Christoph Kords
df931890e0
corrected typos
2012-01-26 12:50:04 +00:00
Christoph Kords
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
Christoph Kords
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
Christoph Kords
4980f57fd5
added total Green-Lagrange strain to crystallite outputs
2012-01-20 10:25:35 +00:00
Christoph Kords
8739b9522e
dislocation stress does not add to stress field anymore, but is only available as constitutive output for purposes of postprocessing. instead, we now use a backstress term (which is added to the resolved shear stress) that depends on the gradient of excess density on the same slip system.
2012-01-17 10:26:57 +00:00
Franz Roters
515986c4d6
renamed w0 and w0_slip to a and a_slip
2011-11-23 14:48:39 +00:00
Christoph Kords
7033e84fc7
new outputs "accumulatedshear", "velocity_edge", and "velocity_screw" (the latter two replace the output "dislocationvelocity")
2011-11-09 09:22:52 +00:00
Franz Roters
58917b5abe
corrected error messages
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you can now switch of shear banding by seting sb_velocity to zero
stacking fault energy parameters are now read from material.config
2011-09-26 09:55:08 +00:00
Franz Roters
9d091bdc3f
added parameters for shear band model
2011-09-14 13:35:28 +00:00
Christoph Kords
9a64f3dd85
* comments are now recognized by IO even when they do not appear at the beginning of the line
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* no need for the zero entries in the material.config anymore
2011-05-30 09:09:19 +00:00
Christoph Kords
bbf75f3fb5
cannot omit entries for second to fourth slip system family, though they are zero
2011-05-30 07:53:41 +00:00
Franz Roters
08d39342e4
reworked restarting for compatibility with abaqus (not yet fully working)
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added new orientation feature for direct simulation:
component type (random) asigns random orientation to an entire grain
2011-05-28 09:44:43 +00:00
Christoph Kords
a910c469df
update of nonlocal material parameters
2011-05-20 08:11:22 +00:00
Philip Eisenlohr
1baae024cb
added two more <crystallite> examples
2011-05-13 16:54:08 +00:00
Philip Eisenlohr
e5a2d829b0
new substructure with 'include' and 'config' directories
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renaming of mpie_... to DAMASK for main usersubroutines
extension of element outputs from 5 to 8 digits (FFT!!!)
2011-05-11 16:38:45 +00:00