Abstract

A space-time fully decoupled wavelet integral collocation method (WICM) with high-order accuracy is proposed for the solution of a class of nonlinear wave equations. With this method, wave equations with various nonlinearities are first transformed into a system of ordinary differential equations (ODEs) with respect to the highest-order spatial derivative values at spatial nodes, in which all the matrices in the resulting nonlinear ODEs are constants over time. As a result, these matrices generated in the spatial discretization do not need to be updated in the time integration, such that a fully decoupling between spatial and temporal discretization can be achieved. A linear multi-step method based on the same wavelet approximation used in the spatial discretization is then employed to solve such a semi-discretization system. By numerically solving several widely considered benchmark problems, including the Klein/sine–Gordon equation and the generalized Benjamin–Bona–Mahony–Burgers equation, we demonstrate that the proposed wavelet algorithm possesses much better accuracy and a faster convergence rate than many existing numerical methods. Most interestingly, the space-associated convergence rate of the present WICM is always about order 6 for different equations with various nonlinearities, which is in the same order with direct approximation of a function in terms of the proposed wavelet approximation scheme. This fact implies that the accuracy of the proposed method is almost independent of the equation order and nonlinearity.

Highlights

  • IntroductionWe consider a numerical solution of the general nonlinear wave problem

  • I =1 in which ei = uexact (xi ) − unum (xi ) with the exact solution uexact and the numerical solution unum, and M is the total number of nodes in space

  • wavelet integral collocation method (WICM) was employed to execute the spatial discretization of nonlinear wave equations

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Summary

Introduction

We consider a numerical solution of the general nonlinear wave problem The general form (1) covers several types of well-known wave problems arising in many scientific and engineering fields, such as nonlinear optics [1,2,3], solid state physics [4,5,6,7,8], and quantum field theory [9,10,11]. When α = 1, γ = 0, β= 0, λ= 1, ρ = 0, and g(u) = au + buc with constants a, b, and c, Equation (1) degrades to the so-called nonlinear.

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