656 research outputs found

    Decay of semilinear damped wave equations:cases without geometric control condition

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    We consider the semilinear damped wave equation ∂tt2u(x,t)+γ(x)∂tu(x,t)=Δu(x,t)−αu(x,t)−f(x,u(x,t))\partial_{tt}^2 u(x,t)+\gamma(x)\partial_t u(x,t)=\Delta u(x,t)-\alpha u(x,t)-f(x,u(x,t)). In this article, we obtain the first results concerning the stabilization of this semilinear equation in cases where γ\gamma does not satisfy the geometric control condition. When some of the geodesic rays are trapped, the stabilization of the linear semigroup is semi-uniform in the sense that ∥eAtA−1∥≤h(t)\|e^{At}A^{-1}\|\leq h(t) for some function hh with h(t)→0h(t)\rightarrow 0 when t→+∞t\rightarrow +\infty. We provide general tools to deal with the semilinear stabilization problem in the case where h(t)h(t) has a sufficiently fast decay

    Asymptotic stability and blow up for a semilinear damped wave equation with dynamic boundary conditions

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    In this paper we consider a multi-dimensional wave equation with dynamic boundary conditions, related to the Kelvin-Voigt damping. Global existence and asymptotic stability of solutions starting in a stable set are proved. Blow up for solutions of the problem with linear dynamic boundary conditions with initial data in the unstable set is also obtained

    Global Stabilization of the Navier-Stokes-Voight and the damped nonlinear wave equations by finite number of feedback controllers

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    In this paper we introduce a finite-parameters feedback control algorithm for stabilizing solutions of the Navier-Stokes-Voigt equations, the strongly damped nonlinear wave equations and the nonlinear wave equation with nonlinear damping term, the Benjamin-Bona-Mahony-Burgers equation and the KdV-Burgers equation. This algorithm capitalizes on the fact that such infinite-dimensional dissipative dynamical systems posses finite-dimensional long-time behavior which is represented by, for instance, the finitely many determining parameters of their long-time dynamics, such as determining Fourier modes, determining volume elements, determining nodes , etc..The algorithm utilizes these finite parameters in the form of feedback control to stabilize the relevant solutions. For the sake of clarity, and in order to fix ideas, we focus in this work on the case of low Fourier modes feedback controller, however, our results and tools are equally valid for using other feedback controllers employing other spatial coarse mesh interpolants
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