Multiple-soliton solutions and multiple-singular soliton solutions for two higher-dimensional shallow water wave equations
Introduction
The (3 + 1)-dimensional shallow water wave equations [1]andwill be studied. Both equations reduce to the potential KdV equation for . The difference between the first terms of the two models is that x replaces y in the term . 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 substituteinto 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 equationIt is interesting to point out that this equation can be reduced to the potential KdV equation by setting 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 equationIt is interesting to point out that this equation can be reduced to the potential KdV equation by setting 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.
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2015, Applied Mathematics and ComputationCitation 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.