Integrability classification and exact solutions to generalized variable-coefficient nonlinear evolution equation
Liu Han-Ze, Zhang Li-Xiang
School of Mathematical Sciences, Liaocheng University, Liaocheng 252059, China

 

† Corresponding author. E-mail: bzliuhanze@163.com

Abstract

This paper is concerned with the generalized variable-coefficient nonlinear evolution equation (vc-NLEE). The complete integrability classification is presented, and the integrable conditions for the generalized variable-coefficient equations are obtained by the Painlevé analysis. Then, the exact explicit solutions to these vc-NLEEs are investigated by the truncated expansion method, and the Lax pairs (LP) of the vc-NLEEs are constructed in terms of the integrable conditions.

PACS: ;02.30.Jr;;02.30.Ik;
1. Introduction

The Painlevé test could to provide useful information for the identification of completely integrable PDEs, which are of importance in nonlinear theory and physical applications. In addition, they also appear to yield other integrable properties such as Lax pairs (LPs), Bäcklund transformations (BTs), rational solutions, and so on (see e.g., Refs. [13] and the references therein).

On the other hand, to find exact solutions to the nonlinear evolution equations (NLEEs) is always one of the themes in mathematics and physics. In the past few decades, there are noticeable progresses in this field, and various methods have been developed, such as the inverse scattering method,[4,5] Darboux and Bäcklund transformations,[68] Lie symmetry analysis,[913] dynamical system method,[14,15] trial function method (direct method),[11,16] Painlevé test,[13,12,1719] and so on. In the present paper, we consider the generalized variable-coefficient nonlinear evolution equation (vc-NLEE) as follows: where u = u(x,t) denotes the unknown function of space variable x and time t, the exponent p is a positive integer, the coefficient functions f = f(t), g = g(t), h = h(t), and l = l(t) are all arbitrary analytic functions, is assumed throughout this paper (otherwise this equation is linear and excluded from our discussion).

This equation is also called the variable-coefficient generalized Burgers–KdV type equation sometimes. Such vc-NLEE plays a significant role in mathematical physics, integrable system, and physical applications, etc.[17,18] However, to obtain the exact solutions and integrability of the variable-coefficient equation in generalized form are more involved. By the equivalent transformation, the variable-coefficient equation can be transformed into constant-coefficient equation under some conditions, so the exact solutions are obtained accordingly.[20] This is a useful method for dealing with exact solutions to the vc-NLEEs, but the integrability of the vc-NLEE may be different from the constant-coefficient equation. In Ref. [12], the Painlevé test and Lie group analysis are performed for the variable-coefficient nonlinear evolution equations (including the cylindrical KdV type equations), but the equation is not the generalized form and it differs greatly from Eq. (1) in the present paper.

The main purpose of this paper is to investigate the complete integrability classification of the generalized vc-BKdV equation by Painlevé test. The remainder of this paper is organized as follows. In Section 2, the Painlevé test is performed, the complete Painlevé integrability classification of Eq. (1) is given, and the integrable conditions for the vc-NLEEs are obtained accordingly. Then, the exact explicit solutions to the equations are investigated by the truncated expansion method, and the Lax pairs of the vc-NLEEs are constructed in terms of the integrable conditions. Finally, the conclusion and some remarks will be given in Section 3.

2. Painlevé test for vc-NLEEs

In this section, we employ the Kruskal’s simplified method[13] to carry out the Painlevé test for Eq. (1). Then, the integrable conditions, exact solutions, and other properties of the vc-NLEEs are obtained.

First of all, we assume that where , ( ) are analytic functions in a neighborhood of the noncharacteristic singular manifold, , ρ is a positive integer.

Then, by using the leading order analysis, we obtain the following results:

(i) . In this case, equation (1) reduces to the variable-coefficient generalized Burgers’ equation (vc-GBE) where . In this case, we have with p being a positive integer, we choose p = 1, that is ρ = 1 and . So the condition is satisfied.

(ii) . In the general case, we have In view of p being a positive integer, we choose p = 1 or p = 2, respectively.

When p = 1, we have ρ = 2 and . So the condition is satisfied.

When p = 2, we have and . So the condition is satisfied also.

Summarizing the above discussion, we obtain a necessary condition of integrability as follows:

In what follows, under the integrable conditions, we perform the Painlevé analysis completely, so the Painlevé integrability classification of Eq. (1) is obtained.

2.1. Painlevé test for Eq. (1) in the case h = h(t) = 0

In this case, equation (1) becomes Eq. (3). Furthermore, if it is integrable, then p = 1.

Thus, substituting Eq. (2) into Eq. (3), we have

By using Eqs. (6a), (6b), and (6d), we can obtain uj (j = 0,1,3) in a unique manner. But from Eq. (6c), we cannot obtain u2 definitely. In general, we have the recursion relations for Eq. (3) as follows: for all .

In view of Eq. (8), we can see that the resonances occur at . In particular, if j = 2, then from Eq. (8) we have Eq. (6c), that is, u2 is arbitrary.

Thus, let , the other coefficients uj ( ) can be determined successively from Eq. (8) in a unique manner. This implies that for Eq. (3), there exists a Laurent series (2) with the coefficients given by Eq. (8). Moreover, setting , that is, Then, by the induction method, it is easy to see that , for all .

So, we can say that equation (3) possesses the Painlevé property (PP) under the conditions p = 1 and Eqs. (6c).

Thus, we have the following result.

Furthermore, the complete classification in terms of Eq. (6c) is as follows:

Summarizing the above discussion, we have

To sum up, we have

2.2. Painlevé test for Eq. (1) in the case

From Eq. (5), we have to discuss the following two cases, respectively.

Summarizing the above discussions, we achieve the following result.

Summarizing the above argument, we achieve the following result.

3. Conclusion and remarks

In this paper, the complete integrability classification of the generalized variable-coefficient nonlinear evolution equation is investigated by the Painlevé analysis method. The integrable conditions for the vc-NLEEs are obtained in the sense of simplified Painlevé test, and the exact explicit solutions are obtained by the truncated expansion method. Then the Lax pairs of the equations are given under the integrable conditions. Moreover, for the integrable equations, the other properties, such as Bäcklund transformations, infinite generalized symmetries, and conservation laws (CLs) can be considered through other methods, the details are omitted in this paper.

Remark 1 In fact, the Painlevé analysis is a powerful method for dealing with intrinsic properties and exact solutions to the nonlinear equations. But the simplified Painlevé test differs from the general Painlevé test[13,19] for dealing with integrable properties and exact solutions sometimes.

Reference
[1] Conte R Musette M 2008 The Painlevé handbook Dordrecht Springer
[2] Weiss J Tabor M Carnevale G 1983 J. Math. Phys. 24 522
[3] Weiss J 1983 J. Math. Phys. 24 1405
[4] Ablowitz M Segur H 1981 Solition and the inverse scattering transform Philadelphia SIAM
[5] Wang D S Lou S Y 2009 J. Math. Phys. 50 123513
[6] Matveev V Salle M 1991 Darboux transformations and solitions Berlin Springer
[7] Rogers C Shadwick W 1982 Bäcklund transformations and their applications New York Academic Press
[8] Liu H Z Xin X P Wang Z G Liu X Q 2017 Commun. Nonlinear. Sci. Numer Simulat 44 11
[9] Bluman G Anco S 2002 Symmetry and integration methods for differential equations New York Springer-Verlag
[10] Olver P 1993 Applications of Lie groups to differential equations New York Springer-Verlag
[11] Liu H Z Xin X P 2016 Commun. Theor. Phys. 66 155
[12] Liu H Z Yue C 2017 Nonlinear. Dyn. 89 1989
[13] Ma W X Bullough R K Caudrey P J 1997 J. Nonlinear Math. Phys. 4 293
[14] Kou K Li J B 2017 Int. Bifur. Chaos. 27 1750058
[15] Feng D H Li J B 2007 Phys. Lett. 369 255
[16] Wang M L Li X Zhang J 2008 Phys. Lett. 372 417
[17] Zhang Y Li J B Lv Y N 2008 Ann. Phys. 323 3059
[18] Wei G M Gao Y T Hu W Zhang C Y 2006 Eur. Phys. J. 53 343
[19] Ma W X 1994 J. Fudan Univ. 33 319
[20] Vaneeva O 2012 Commun. Nonlinear Sci. Numer. Simulat 17 611
[21] Zhang Y P Liu J Wei G M 2015 Appl. Math. Lett. 45 58
[22] Newell A 1985 Solitions in mathematics and physics Philadelphia SIAM
[23] Ma Z Y Fei J X Chen Y M 2014 Appl. Math. Lett. 37 54
[24] Xia Y R Xin X P Zhang S L 2017 Chin. Phys. 26 030202