2015
DOI: 10.1016/j.mechmat.2015.01.013
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A line-tension model of dislocation networks on several slip planes

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Cited by 8 publications
(7 citation statements)
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“…Indeed, relaxation phenomena may be present, and straight dislocations with certain Burgers vectors and orientations may spontaneously decompose into several parallel dislocations, and in some cases a zig-zag structure is optimal, see [11,12,14]. The relaxation formula for (2.2) involves the H 1 -elliptic envelope…”
Section: Variational Models Of Dislocations and Plasticity In Crystalsmentioning
confidence: 99%
See 1 more Smart Citation
“…Indeed, relaxation phenomena may be present, and straight dislocations with certain Burgers vectors and orientations may spontaneously decompose into several parallel dislocations, and in some cases a zig-zag structure is optimal, see [11,12,14]. The relaxation formula for (2.2) involves the H 1 -elliptic envelope…”
Section: Variational Models Of Dislocations and Plasticity In Crystalsmentioning
confidence: 99%
“…Numerical results were first presented in [26,28], in situations in which individual dislocations are resolved. A mathematical analysis of the model was performed in [21,22] for the scalar case in which all dislocations have the same Burgers vector, in [11,13] for the vectorial situation with multiple Burgers vectors, and in [12] for dislocations localized to two parallel planes. The asymptotic analysis results in a line tension model associated to a Caccioppoli partition of the type (1.2), where the energy density ψ is obtained by the H 1 -elliptic envelope of the pre-logarithmic factor ψ 0 , as defined in (2.3).…”
Section: Variational Models Of Dislocations and Plasticity In Crystalsmentioning
confidence: 99%
“…For the intermediate case, the limit energy of a mollified straight jump w b,ν,ε = b1 {x·ν>0} * ν ε is (1 − β)ϕ short (b, ν) + βϕ long (b, ν). The double relaxation is achieved by first replacing the straight jump by a large-scale exterior microstructure and then replacing all straight jumps in the microstructure by interior microstructures at scale h. For an example of a non-trivial optimal two-scale microstructure, see [5]. The proof of the theorem will appear in [6].…”
Section: The Limit Energy For Multiple Planesmentioning
confidence: 99%
“…Macroscopic line-tension models have been rigorously derived from the KCO model for single slip [28,29], for multipleslip [16,19] and for multi-planar slip [20]. A remarkable result of the analysis of Conti et al [19] is that the effective self-energy may be strictly smaller than the classical self-energies of straight dislocations (cf., for example [11]) as a result of fine reconstruction of the dislocation line.…”
Section: Introductionmentioning
confidence: 99%