2006
DOI: 10.1002/nme.1896
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A new fast finite element method for dislocations based on interior discontinuities

Abstract: SUMMARYA new technique for the modelling of multiple dislocations based on introducing interior discontinuities is presented. In contrast to existing methods, the superposition of infinite domain solutions is avoided; interior discontinuities are specified on the dislocation slip surfaces and the resulting boundary value problem is solved by a finite element method. The accuracy of the proposed method is verified and its efficiency for multi-dislocation problems is illustrated. Bounded core energies are incorp… Show more

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Cited by 77 publications
(61 citation statements)
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“…This problem can be posed as the analysis of a body containing an embedded surface of discontinuity where the relative displacements (or jump in displacements) across the surface of discontinuity are prescribed according to the Burgers vector b of the dislocation. XFEM has been applied to the mesoscale modeling of dislocations in two dimensions [109,50,12,49], three dimensions [49,82] and in thin shells such as carbon nanotubes [82].…”
Section: Dislocationsmentioning
confidence: 99%
“…This problem can be posed as the analysis of a body containing an embedded surface of discontinuity where the relative displacements (or jump in displacements) across the surface of discontinuity are prescribed according to the Burgers vector b of the dislocation. XFEM has been applied to the mesoscale modeling of dislocations in two dimensions [109,50,12,49], three dimensions [49,82] and in thin shells such as carbon nanotubes [82].…”
Section: Dislocationsmentioning
confidence: 99%
“…Nevertheless, fine-scale features can also be incorporated "hierarchically" through enrichment. For example, Gracie et al [321,322], Belytschko and Gracie [323] developed special enrichment functions for dislocations.…”
Section: Isrn Applied Mathematicsmentioning
confidence: 99%
“…S ∞ is the set of nodes within a given number of element layers from the glide plane or core, as shown in Figure 6(a). is defined by (17), where d i and d e are defined to be constant distances from the glide plane, as shown in Figure 13(a). We label this enrichment EEL because it corresponds to the enriched element layers scheme used in [8] with the standard XFEM.…”
Section: Singular Enrichment Without Heaviside Enrichment and With A mentioning
confidence: 99%