Abstract

Meshfree methods based on radial basis function (RBF) approximation are of interest for numerical solution of partial differential equations because they are flexible with respect to the geometry of the computational domain, they can provide high order convergence, they are not more complicated for problems with many space dimensions and they allow for local refinement. The aim of this paper is to show that the solution of the Rosenau equation, as an example of an initial-boundary value problem with multiple boundary conditions, can be implemented using RBF approximation methods. We extend the fictitious point method and the resampling method to work in combination with an RBF collocation method. Both approaches are implemented in one and two space dimensions. The accuracy of the RBF fictitious point method is analyzed partly theoretically and partly numerically. The error estimates indicate that a high order of convergence can be achieved for the Rosenau equation. The numerical experiments show that both methods perform well. In the one-dimensional case, the accuracy of the RBF approaches is compared with that of the corresponding pseudospectral methods, showing similar or slightly better accuracy for the RBF methods. In the two-dimensional case, the Rosenau problem is solved both in a square domain and in an irregular domain with smooth boundary, to illustrate the capability of the RBF-based methods to handle irregular geometries.

Highlights

  • The Rosenau equation has become an established research subject in the field of mathematical physics since its introduction in the late 80s by Philip Rosenau [31]

  • The objective of this paper is to derive numerical methods based on radial basis function (RBF) collocation methods [14,22] for the Rosenau equation, that can be applied to problems in one, two, and three space dimensions, for non-trivial geometries

  • The Rosenau equation, which is used as an application throughout this paper, is an example of a non-linear PDE with multiple boundary conditions as well as mixed space-time derivatives

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Summary

Introduction

The Rosenau equation has become an established research subject in the field of mathematical physics since its introduction in the late 80s by Philip Rosenau [31]. The equation is intended to overcome shortcomings of the already famous Korteweg–de Vries (KdV) equation [15] in describing phenomena of solitary wave interaction. Knowledge about this interaction, when two or more wave packets called solitons are colliding with one another, is indispensable in digital transmission through optical fibers. One may consult [7] for a fascinating history behind this subject.

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