Stability w.r.t. Disturbances for the Global Attractor of Multi-Valued Semiflow Generated by Nonlinear Wave Equation (original) (raw)

Global attractors for multivalued semiflows with weak continuity properties

Nonlinear Analysis: Theory, Methods & Applications, 2014

A method is proposed to deal with some multivalued semiflows with weak continuity properties. An application to the reaction-diffusion problems with nonmonotone multivalued semilinear boundary condition and nonmonotone multivalued semilinear source term is presented.

Attractors and their structure for semilinear wave equations with nonlinear boundary dissipation

2004

Long time behavior of a semilinear wave equation with nonlinear boundary dissipation is considered. It is shown that weak solutions generated by the wave dynamics converge asymptotically to a flnite dimensional attractor. It is known (CEL1) that the attractor consists of all full trajectories emanating from the set of stationary points. Under the additional assumption that the set of stationary

On Global Attractors for Autonomous Damped Wave Equation with Discontinuous Nonlinearity

Continuous and Distributed Systems, 2013

We consider autonomous damped wave equation with discontinuous nonlinearity. The long-term prognosis of the state functions when the conditions on the parameters of the problem do not guarantee uniqueness of solution of the corresponding Cauchy problem are studied. We prove the existence of a global attractor and investigate its structure. It is obtained that trajectory of every weak solution defined on [0; +→) tends to a fixed point.

Attractors for the semiflow associated with a class of doubly nonlinear parabolic equations

2008

A doubly nonlinear parabolic equation of the form α(u t ) − ∆u + W ′ (u) = f , complemented with initial and either Dirichlet or Neumann homogeneous boundary conditions, is addressed. The two nonlinearities are given by the maximal monotone function α and by the derivative W ′ of a smooth but possibly nonconvex potential W ; f is a known source. After defining a proper notion of solution and recalling a related existence result, we show that from any initial datum emanates at least one solution which gains further regularity for t > 0. Such regularizing solutions constitute a semiflow S for which uniqueness is satisfied for strictly positive times and we can study long time behavior properties. In particular, we can prove existence of both global and exponential attractors and investigate the structure of ω-limits of single trajectories.

Attractors and their structure for semilinear wave equations with nonlinear boundary dissipation-doi: 10.5269/bspm. v22i1. 7494

2004

Long time behavior of a semilinear wave equation with nonlinear boundary dissipation is considered. It is shown that weak solutions generated by the wave dynamics converge asymptotically to a finite dimensional attractor. It is known [CEL1] that the attractor consists of all full trajectories emanating from the set of stationary points. Under the additional assumption that the set of stationary points is finite it is proved that every solution converges to some stationary points at an exponential rate.

STURM GLOBAL ATTRACTORS OF HAMILTONIAN TYPE FOR SEMILINEAR PARABOLIC EQUATIONS (Nonlinear Partial Differential Equations, Dynamical Systems and Their Applications)

数理解析研究所講究録, 2014

Dedicated to Hiroshi Matano on the occasion of his 60th birthday ABSTRACT. In this note we review the characterization of global attractors for dissipative semiflows generated by scalar semilinear parabolic equations of the form ut=uxx+f(x,u−ux)u_{t}=u_{xx}+f(x, u-u_{x})ut=uxx+f(x,uux) defined on the interval 0leqxleqpi0\leq x\leq\pi0leqxleqpi with Neumann boundary conditions. We outline the characterization results for these global attractors-the Sturm attractors-obtained by a permutation of the equilibrium solutions-the Sturm permutation-associated to the second order ODEODEODE satisfied by the stationary solutions of the parabolic equation. In particular we consider the characterization results for the class of nonlinearities of the form f=f(u)f=f(u)f=f(u)-the Hamiltonian class. Using this characterization we then outline some results on the geometry of Sturm attractors for the case of periodic boundary conditions.