Abstract

We propose a generalized finite element method for the strongly damped wave equation with highly varying coefficients. The proposed method is based on the localized orthogonal decomposition introduced in Målqvist and Peterseim [Math. Comp. 83 (2014) 2583–2603], and is designed to handle independent variations in both the damping and the wave propagation speed respectively. The method does so by automatically correcting for the damping in the transient phase and for the propagation speed in the steady state phase. Convergence of optimal order is proven in L2(H1)-norm, independent of the derivatives of the coefficients. We present numerical examples that confirm the theoretical findings.

Highlights

  • This paper is devoted to the study of numerical solutions to the strongly damped wave equation with highly varying coefficients

  • A and B represent the system’s damping and wave propagation respectively, f denotes the source term, and the solution u is a displacement function. This equation commonly appears in the modelling of viscoelastic materials, where the strong damping −∇ · A∇uarises due to the stress being represented as the sum of an elastic part and a viscous part [6, 13]

  • We propose a novel multiscale method based on the localized orthogonal decomposition (LOD) method

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Summary

Introduction

This paper is devoted to the study of numerical solutions to the strongly damped wave equation with highly varying coefficients. Multiscale, localized orthogonal decomposition, finite element method, reduced basis method. Multiscale methods, as the localized orthogonal decomposition, are usually designed to handle problems with a single multiscale coefficient In this sense, the strongly damped wave equation is different, as an extra coefficient appears due to the strong damping. In this paper we present a generalized finite element method (GFEM), with a backward Euler time stepping for solving the strongly damped wave equation. The method uses both the damping and diffusion coefficients to construct a generalized finite element space, similar to those in e.g.

Weak formulation and classical FEM
Generalized finite element method
Ideal method
Localized method
Error estimates
Auxiliary problem
The damped wave equation
Error bound for the ideal method
Initial data
Reduced basis method
Academic example
Marmousi model

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