Attractors for damped semilinear wave equations with a Robin–acoustic boundary perturbation. (December 2019)

• Record Type: Journal Article
• Authors: Shomberg, Joseph L.
• Is Part Of: Nonlinear analysis. Volume 189(2019)
• Publication Date: 2019-12
• Subjects: primary 35B25 35B41 -- secondary 35L20 35Q72; Damped semilinear wave equation -- Acoustic boundary condition -- Robin boundary condition -- Singular perturbation -- Global attractor -- Upper-semicontinuity -- Exponential attractor; Mathematical analysis -- Periodicals; Functional analysis -- Periodicals; Nonlinear theories -- Periodicals; Analyse mathématique -- Périodiques; Analyse fonctionnelle -- Périodiques; Théories non linéaires -- Périodiques; Functional analysis; Mathematical analysis; Nonlinear theories; Periodicals; Electronic journals; 515.7248
• DOI: 10.1016/j.na.2019.111582
• Languages: English
• ISSNs: 0362-546X

Abstract

Abstract: Under consideration is the damped semilinear wave equation u t t + u t − Δ u + u + f ( u ) = 0 on a bounded domain Ω in R 3 with a perturbation parameter ε > 0 occurring in an acoustic boundary condition, limiting ( ε = 0 ) to a Robin boundary condition. With minimal assumptions on the nonlinear term f, the existence and uniqueness of global weak solutions is shown for each ε ∈ [ 0, 1 ] . Also, the existence of a family of global attractors is shown to exist. After proving a general result concerning the upper-semicontinuity of a one-parameter family of sets, the result is applied to the family of global attractors. Because of the complicated boundary conditions for the perturbed problem, fractional powers of the Laplacian are not well-defined; moreover, because of the restrictive growth assumptions on f, the family of global attractors is obtained from the asymptotic compactness method developed by J. Ball for generalized semiflows. With more relaxed assumptions on the nonlinear term f, we are able to show the global attractors possess optimal regularity and prove the existence of an exponential attractor, for each ε ∈ [ 0, 1 ] . This result insures that the corresponding global attractor inherits finite (fractal) dimension, however, the dimension is not necessarily uniform in ε .