2016
DOI: 10.1016/j.na.2016.02.001
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On the quenching of a nonlocal parabolic problem arising in electrostatic MEMS control

Abstract: Abstract. We consider a nonlocal parabolic model for a micro-electro-mechanical system. Specifically, for a radially symmetric problem with monotonic initial data, it is shown that the solution quenches, so that touchdown occurs in the device, in a situation where there is no steady state. It is also shown that quenching occurs at a single point and a bound on the approach to touchdown is obtained. Numerical simulations illustrating the results are given.

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Cited by 19 publications
(23 citation statements)
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“…The quenching behavior of the nonlocal Equation () associated with Dirichlet boundary ( β=+) has been treated in Kavallaris et al 20 and in references therein as well as in previous works 21–23 . Also, non‐local alterations of parabolic and hyperbolic problems arising in MEMS technology were tackled in previous works 5,7,20–22,24,25 .…”
Section: Introductionmentioning
confidence: 99%
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“…The quenching behavior of the nonlocal Equation () associated with Dirichlet boundary ( β=+) has been treated in Kavallaris et al 20 and in references therein as well as in previous works 21–23 . Also, non‐local alterations of parabolic and hyperbolic problems arising in MEMS technology were tackled in previous works 5,7,20–22,24,25 .…”
Section: Introductionmentioning
confidence: 99%
“…The quenching behavior of the nonlocal Equation () associated with Dirichlet boundary ( β=+) has been treated in Kavallaris et al 20 and in references therein as well as in previous works 21–23 . Also, non‐local alterations of parabolic and hyperbolic problems arising in MEMS technology were tackled in previous works 5,7,20–22,24,25 . However, to the best of our knowledge, there are not similar studies available in the literature for the Robin problem (0 < β < + ∞ ,) so in the current work we study problem (1.1) and we extend some of the results given in Guo 1 for the local problem, but we also deliver a further investigation related to the steady‐state problem and the quenching behavior of the time‐dependent problem.…”
Section: Introductionmentioning
confidence: 99%
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“…In case σ ( u ) ≡ 0, then problem ()–() is reduced to its deterministic counterpart ut=normalΔu+λ(1u)2,1emin1emQT, u=01emon1emnormalΓT, 0u(x,0)=ξ(x)<1,1emxnormalΩ. Actually, ()–() and its non‐local variations have attracted the attention of many researchers , because this kind of equations can model the operation of some (idealized) electrostatic actuated micro‐electro‐mechanical systems (MEMS), which have a wide variety of applications.…”
Section: Introductionmentioning
confidence: 99%