Blow–up for the wave equation with hyperbolic dynamical boundary conditions, interior and boundary nonlinear damping and sources

Enzo Vitillaro
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引用次数: 5

Abstract

The aim of this paper is to give global nonexistence and blow–up results for the problem

where \begin{document}$ \Omega $\end{document} is a bounded open \begin{document}$ C^1 $\end{document} subset of \begin{document}$ {\mathbb R}^N $\end{document}, \begin{document}$ N\ge 2 $\end{document}, \begin{document}$ \Gamma = \partial\Omega $\end{document}, \begin{document}$ (\Gamma_0,\Gamma_1) $\end{document} is a partition of \begin{document}$ \Gamma $\end{document}, \begin{document}$ \Gamma_1\not = \emptyset $\end{document} being relatively open in \begin{document}$ \Gamma $\end{document}, \begin{document}$ \Delta_\Gamma $\end{document} denotes the Laplace–Beltrami operator on \begin{document}$ \Gamma $\end{document}, \begin{document}$ \nu $\end{document} is the outward normal to \begin{document}$ \Omega $\end{document}, and the terms \begin{document}$ P $\end{document} and \begin{document}$ Q $\end{document} represent nonlinear damping terms, while \begin{document}$ f $\end{document} and \begin{document}$ g $\end{document} are nonlinear source terms. These results complement the analysis of the problem given by the author in two recent papers, dealing with local and global existence, uniqueness and well–posedness.

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The aim of this paper is to give global nonexistence and blow–up results for the problem \begin{document}$ \begin{cases} u_{tt}-\Delta u+P(x,u_t) = f(x,u) \qquad &\text{in $(0, \infty) \times\Omega$,}\\ u = 0 &\text{on $ (0, \infty) \times\Gamma _0 $,}\\ u_{tt}+\partial_\nu u-\Delta_\Gamma u+Q(x,u_t) = g(x,u)\qquad &\text{on $ (0, \infty) \times\Gamma _1$,}\\ u(0,x) = u_0(x),\quad u_t(0,x) = u_1(x) & \text{in $\overline{\Omega}$,} \end{cases} $\end{document} where \begin{document}$ \Omega $\end{document} is a bounded open \begin{document}$ C^1 $\end{document} subset of \begin{document}$ {\mathbb R}^N $\end{document}, \begin{document}$ N\ge 2 $\end{document}, \begin{document}$ \Gamma = \partial\Omega $\end{document}, \begin{document}$ (\Gamma_0,\Gamma_1) $\end{document} is a partition of \begin{document}$ \Gamma $\end{document}, \begin{document}$ \Gamma_1\not = \emptyset $\end{document} being relatively open in \begin{document}$ \Gamma $\end{document}, \begin{document}$ \Delta_\Gamma $\end{document} denotes the Laplace–Beltrami operator on \begin{document}$ \Gamma $\end{document}, \begin{document}$ \nu $\end{document} is the outward normal to \begin{document}$ \Omega $\end{document}, and the terms \begin{document}$ P $\end{document} and \begin{document}$ Q $\end{document} represent nonlinear damping terms, while \begin{document}$ f $\end{document} and \begin{document}$ g $\end{document} are nonlinear source terms. These results complement the analysis of the problem given by the author in two recent papers, dealing with local and global existence, uniqueness and well–posedness.
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