Multiple-soliton solutions and multiple-singular soliton solutions for two higher-dimensional shallow water wave equations

https://doi.org/10.1016/j.amc.2009.01.071Get rights and content

Abstract

Two (3 + 1)-dimensional shallow water wave equations are studied for complete integrability. The Hirota’s bilinear method is used to determine the multiple-soliton solutions for these equations. Moreover, multiple-singular soliton solutions will also be determined for each model. The analysis highlights the capability of the direct method in handling completely integrable equations.

Introduction

The (3 + 1)-dimensional shallow water wave equations [1]uyzt+uxxxyz-6uxuxyz-6uxzuxy=0anduxzt+uxxxyz-2(uxxuyz+uyuxxz)-4(uxuxyz+uxzuxy)=0will be studied. Both equations reduce to the potential KdV equation for z=y=x. The difference between the first terms of the two models is that x replaces y in the term uyzt. The generalized shallow water wave equations studied by Ablowitz [2] and Hirota and Satsuma [3], and by Mansfield and Clarkson [1] arise as reduction of these two equations.

A variety of distinct methods are used for classification of integrable equations. The Painlevé analysis, the inverse scattering method, the Bäcklund transformation method, the conservation laws method, and the Hirota bilinear method [4], [5], [6], [7], [8], [9], [10], [11], [12], [13] are mostly used in the literature for investigating complete integrability. The Hirota’s bilinear method is rather heuristic and possesses significant features that make it ideal for the determination of multiple-soliton solutions for a wide class of nonlinear evolution equations.

Two goals are set for this work. We first aim to use Hirota’s bilinear method to emphasize its power and reliability for handling integrable equations. We second aim to determine multiple-soliton solutions and multiple-singular soliton solutions [14], [15], [16], [17], [18], [19], [20], [21], [22] for these Eqs. (1), (2). The Hereman’s simplified form [12], [13] will be combined with the Hirota’s method to achieve these two goals.

Section snippets

The Hirota’s bilinear method

To formally derive N-soliton solutions for completely integrable equations, we will use the Hirota’s direct method combined with the simplified version of Hereman et al. [12], [13]. It was proved by many that soliton solutions are just polynomials of exponentials. This will be also confirmed in the coming discussions.

We first substituteu(x,y,z,t)=ekx+ry+sz-ct,into the linear terms of the equation under discussion to determine the dispersion relation between k, r, s and c. We then substitute the

The first (3 + 1)-dimensional equation

In this section, we apply the Hirota’s bilinear method to the (3 + 1)-dimensional shallow water wave equationuyzt+uxxxyz-6uxuxyz-6uxzuxy=0.It is interesting to point out that this equation can be reduced to the potential KdV equation by setting z=y=x and integrating twice with respect to x.

The second (3 + 1)-dimensional equation

In this section, we apply the Hirota’s bilinear method to the (3 + 1)-dimensional shallow water wave equationuxzt+uxxxyz-2(uxxuyz+uyuxxz)-4(uxuxyz+uxzuxy)=0.It is interesting to point out that this equation can be reduced to the potential KdV equation by setting z=y=x and integrating twice with respect to x.

Discussion

A combination of Hirota’s method and Hereman’s method were used to formally derive multiple-soliton solutions and multiple-singular soliton solutions of two completely integrable (3 + 1)-dimensional equations. The Hirota’s bilinear method possesses significant features that make it ideal for the determination of multiple-soliton solutions for a wide class of nonlinear evolution equations. The study revealed the power of the bilinear method.

Cited by (20)

  • Some new nonlinear wave solutions for two (3+1)-dimensional equations

    2015, Applied Mathematics and Computation
    Citation Excerpt :

    In these references, none of the solutions contains arbitrary function. In [14], Wazwaz investigated multiple soliton solutions and multiple singular soliton solutions of Eqs. (1.8) and (1.9) respectively. This paper is organized as follows.

View all citing articles on Scopus
View full text