Go to file
Achal H P f0694312f2
Update README.md
2024-02-19 10:16:30 +05:30
.github/workflows Intel (classic) has issues on GitHub actions 2022-10-08 20:07:56 +02:00
PRIVATE@8c0a24006f add read-in init phi, correct write-out damage result 2022-09-21 08:50:00 +02:00
cmake avoid trapping of underflows 2022-09-14 00:27:49 +02:00
env python(2) is not available on newer systems 2021-09-01 08:07:55 +02:00
examples following DAMASK paper 2022-06-13 14:08:45 +02:00
img nicer formatting (official plain text download) 2022-01-25 08:33:53 +01:00
install/MarcMentat standard format 2022-09-29 20:52:31 +02:00
processing grain growth not maintained and has issues 2022-01-12 07:48:09 +01:00
python fix grid add primitive bug 2022-08-29 11:44:50 +00:00
src 27-Oct-23-1 2023-10-27 18:37:16 +05:30
.gitattributes matches other short names (src, img, ..) 2021-07-10 13:41:19 +02:00
.gitignore only ignore temporary files in the respective folders 2020-03-16 22:50:09 +01:00
.gitlab-ci.yml new Marc version 2022-05-09 14:05:30 +02:00
.gitmodules master was rename to development 2021-08-29 20:46:46 +02:00
CMakeLists.txt PETSc 3.18.0 compatibility 2022-10-02 12:48:54 +02:00
COPYING using AGPL instead of GPL 2022-01-15 00:20:29 +01:00
DAMASK_prerequisites.sh also test for new Intel compilers 2021-09-06 09:02:14 +02:00
LICENSE original layout from official page 2022-06-28 20:00:39 +02:00
Makefile modern CMake shortcut 2022-01-09 20:48:58 +01:00
README.md Update README.md 2024-02-19 10:16:30 +05:30
VERSION v3.0.0-alpha7 2022-10-10 10:48:36 +02:00

README.md

DAMASK - The Düsseldorf Advanced Material Simulation Kit

Visit damask.mpie.de for installation and usage instructions

DAMASK_EICMD

This is a DAMASK fork with "Discrete deformation twinning model" implementation based on work done by Dr. Satyapriya Gupta and Dr. Philip Eisenlohr at MSU.)

The Discrete deformation twinning model

  • We introduce stochasticity for the nucleation and growth events of twinning through random sampling, similar to Monte Carlo Methods.

  • The ease or difficulty of a twinning event is controlled by adjusting the frequency of sampling.

  • At each voxel, the state of twinning is treated as a discrete quantity, unlike the approach based on diffused volume fraction.

  • The kinetics of twinning occur in the form of a “jump,” rather than following a rate equation as in the “pseudo-slip” approach.

  • The jumped state is evaluated using the correspondence matrix from Niewczas, Acta Materialia, 2010.

Contact Information

Max-Planck-Institut für Eisenforschung GmbH
Max-Planck-Str. 1
40237 Düsseldorf
Germany

damask@mpie.de
https://damask.mpie.de
https://git.damask.mpie.de

( EICMD Team, IIT Dharwad https://sites.google.com/view/eicmd/home )