TY - JOUR
T1 - Discrete dislocation dynamics for crystal RVEs. Part 1
T2 - Periodic network kinematics
AU - Pachaury, Yash
AU - Po, Giacomo
AU - El-Azab, Anter
N1 - Funding Information:
A. El-Azab acknowledges support from the U. S. Department of Energy, Division of Materials Sciences and Engineering, through award number DE-SC0017718 at Purdue University. Y. Pachaury was supported by the US Department of Energy, Office of Nuclear Energy, contract DE-NE0008758 at Purdue University. G. Po acknowledges the support of the U.S. Department of Energy, Office of Fusion Energy Sciences (FES), under award number DE-SC0019157 with UCLA, and subaward number 019GXA906 with the University of Miami.
Publisher Copyright:
© 2022 Elsevier Ltd
PY - 2022/6
Y1 - 2022/6
N2 - A novel implementation of the dislocation flux boundary condition in discrete dislocation dynamics is presented. The continuity of the individual dislocation loops in a periodic representative crystal volume (RVE) is enforced across the boundary of the RVE with the help of a dual topological description for representing dislocation line kinematics in two equivalent spaces representing the deforming crystal, the RVE and the unbounded crystal spaces. The former describes the motion of the dislocations in the simulated crystal RVE whereas the latter represents the motion of dislocations in an infinite space containing all replicas of the RVE. A mapping between the two spaces forms the basis of the implementation of flux boundary condition. The implementation details are discussed in the context of statistical homogeneity of bulk crystals undergoing macroscopically homogeneous plastic deformation. In this case, the boundary nodes associated with dislocation segments bear no relevance in the motion of the dislocations. Some test cases are presented and discussed to establish the proposed approach.
AB - A novel implementation of the dislocation flux boundary condition in discrete dislocation dynamics is presented. The continuity of the individual dislocation loops in a periodic representative crystal volume (RVE) is enforced across the boundary of the RVE with the help of a dual topological description for representing dislocation line kinematics in two equivalent spaces representing the deforming crystal, the RVE and the unbounded crystal spaces. The former describes the motion of the dislocations in the simulated crystal RVE whereas the latter represents the motion of dislocations in an infinite space containing all replicas of the RVE. A mapping between the two spaces forms the basis of the implementation of flux boundary condition. The implementation details are discussed in the context of statistical homogeneity of bulk crystals undergoing macroscopically homogeneous plastic deformation. In this case, the boundary nodes associated with dislocation segments bear no relevance in the motion of the dislocations. Some test cases are presented and discussed to establish the proposed approach.
KW - Bulk crystal plasticity
KW - Discrete dislocation dynamics
KW - Representative volume element (RVE)
KW - Statistical homogeneity
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U2 - 10.1016/j.jmps.2022.104861
DO - 10.1016/j.jmps.2022.104861
M3 - Article
AN - SCOPUS:85127151337
VL - 163
JO - Journal of the Mechanics and Physics of Solids
JF - Journal of the Mechanics and Physics of Solids
SN - 0022-5096
M1 - 104861
ER -