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DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS

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ON QUENCHING FOR SEMILINEAR PARABOLIC EQUATIONS<br />

WITH DYNAMIC BOUNDARY CONDITIONS<br />

JOAKIM H. PETERSSON<br />

We present a quenching result for semilinear parabolic equations with dynamic boundary<br />

conditions in bounded domains with a smooth boundary.<br />

Copyright © 2006 Joakim H. Petersson. This is an open access article distributed under<br />

the Creative Commons Attribution License, which permits unrestricted use, distribution,<br />

and reproduction in any medium, provided the original work is properly cited.<br />

1. Introduction<br />

For semilinear partial differential equations, a particular type of blow-up phenomenon<br />

may arise when the nonlinearity has a pole at a finite value of the solution. Namely, the<br />

solution itself remains bounded while some derivative of it blows up. This is referred<br />

to by saying that the solution “quenches.” The study of quenching phenomena for parabolic<br />

differential equations with singular terms and classical boundary conditions (of<br />

Dirichlet- or Neumann-type) was initiated by Kawarada [7] in connection with the study<br />

of electric current transients in polarized ionic conductors, and has attracted much attention<br />

since then (see the survey [8]). Recently, parabolic differential equations with dynamic<br />

boundary conditions aroused the interest of several researchers (see [1, 3, 6]). The<br />

question of the occurrence of quenching phenomena in the case of dynamic boundary<br />

conditions comes up naturally. In this paper, we provide a simple example.<br />

In Section 2, we present some recent results on parabolic equations with dynamic<br />

boundary conditions in bounded domains with a smooth boundary and we prove some<br />

needed facts about the behavior of the solutions. Section 3 is devoted to a simple criterion<br />

(positivity of the nonlinearities) for the appearance of quenching for certain semilinear<br />

equations of this type.<br />

2. Preliminary considerations<br />

We will consider the semilinear problem with dynamic boundary conditions<br />

u t − Δu = f (x,u), t>0, x ∈ Ω,<br />

u t + u ν = g(x,u), t>0, x ∈ ∂Ω,<br />

u(0,x) = u 0 (x), x ∈ Ω,<br />

(2.1)<br />

Hindawi Publishing Corporation<br />

Proceedings of the Conference on Differential & Difference Equations and Applications, pp. 935–941

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