DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS
DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS
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