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
Summary
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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