2015
DOI: 10.1016/j.amc.2015.01.102
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Verification of a multiscale surface stress model near voids in copper under the load induced by external high electric field

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Cited by 5 publications
(8 citation statements)
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“…30 However, the formation process of such protrusions in a metal subject to an electric field has not yet been adequately described theoretically or observed experimentally. 19,25,28,29 Our model, based on mobile dislocation density fluc- tuations (MDDF), 16 complements these previous models by proposing that surface features appear as a result of a critical increase in the mobile dislocation density ρ. According to this model, prior to breakdown, the mobile dislocation density is in a long-lived metastable state, fluctuating around a deterministically stable value ρ * .…”
Section: Introductionsupporting
confidence: 53%
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“…30 However, the formation process of such protrusions in a metal subject to an electric field has not yet been adequately described theoretically or observed experimentally. 19,25,28,29 Our model, based on mobile dislocation density fluc- tuations (MDDF), 16 complements these previous models by proposing that surface features appear as a result of a critical increase in the mobile dislocation density ρ. According to this model, prior to breakdown, the mobile dislocation density is in a long-lived metastable state, fluctuating around a deterministically stable value ρ * .…”
Section: Introductionsupporting
confidence: 53%
“…This early stage evolution can nucleate consequent dynamics, which are described by other models. [25][26][27][28][29]53 In addition, the model defines some unique features of breakdown nucleation, which have not been directly treated by previous models. First, breakdown is a critical process, which develops within several tens of nanoseconds for parameter values around those of the nominal parameters, see Section VI.…”
Section: Discussionmentioning
confidence: 99%
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“…This protrusion would then enhance the electric current on the surface, leading to heating and thus to plasma formation and arc nucleation. However, molecular dynamics and finite element simulations showed these processes occurring only at E 1 GV/m [11,12], significantly more than the observed BD fields, in the range of 100-200 MV/m [4,10]. It is well established that plasticity in metals close to the yield is controlled by stochastic dislocation reactions [13].…”
mentioning
confidence: 99%