Abstract and Applied Analysis

Volume 2014 (2014), Article ID 264049, 4 pages

http://dx.doi.org/10.1155/2014/264049

Letter to the Editor

Comment on “Conservation Laws of Two (2 + 1)-Dimensional Nonlinear Evolution Equations with Higher-Order Mixed Derivatives”

Long Wei and Yang Wang

Department of Mathematics, Hangzhou Dianzi University, Zhejiang 310018, China

Received 30 October 2013; Accepted 28 November 2013; Published 28 January 2014

Academic Editor: Chaudry M. Khalique

Copyright © 2014 Long Wei and Yang Wang. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

In a recent paper (Zhang (2013)), the author claims that he has proposed two rules to modify Ibragimov’s theorem on conservation laws to “ensure the theorem can be applied to nonlinear evolution equations with any mixed derivatives.” In this letter, we analysis the paper. Indeed, the so-called “modification rules” are needless and the theorem of Ibragimov can be applied to construct conservation laws directly for nonlinear equations with any mixed derivatives as long as the formal Lagrangian is rewritten in symmetric form. Moreover, the conservation laws obtained by the so-called “modification rules” in the paper under discussion are equivalent to the one obtained by Ibragimov’s theorem.

1. Introduction

Noether’s famous theorem about symmetries and conservation laws is now almost a century old and has been discussed in literally hundreds of papers and is covered in many textbooks, for example, in [1, 2]. Noether’s theorem allows one to construct conservation laws for differential equations following a straightforward algorithm. Although Noether’s approach provides an elegant algorithm for finding conservation laws, it possesses a strong limitation: it can only be applied to equations having variational structure. However, a large number of differential equations without variational structure admit conservation laws. Recently, Ibragimov proved a result in [3] which allows one to construct conservation laws for equations without variational structure. Essentially, Ibragimov’s theorem is an extension of Noether’s theorem by introducing formal Lagrangian to get rid of the variational limitation. There have been abundant papers on constructing conservation laws using Ibragimov’s theorem; see [4–9] and references therein.

In [10], to construct conservation laws for some nonlinear equations with higher-order mixed derivatives, the author proposed two so-called “modification rules” to modify Ibragimov’s theorem and gave “new” formulae of conservation laws for ANNV equation and KP-BBM equation. The two rules in [10] are uncalled for and illusive; indeed, Ibragimov’s theorem can be applied to construct conservation laws directly for nonlinear equations with higher-order mixed derivatives. To do so, we only need to rewrite the corresponding form Lagrangian in symmetric form. Moreover, by direct calculations, we find that the conservation laws obtained by so-called “modification rules” in [10] are equivalent to the one obtained by Ibragimov’s theorem.

For simplicity, we only illuminate our statement for the ANNV equation [10, ] in the following section.

2. Formulae of Conservation Laws for ANNV Equation and the Equivalence

In this section, we first apply Ibragimov’s theorem to construct conservation laws for ANNV equation [10, ]

The form Lagrangian of (1) and the corresponding adjoint equation is

where is the solution of the adjoint equation. We rewrite in the symmetric form as follows:

For any Lie point, Lie-Bäcklund, and nonlocal symmetry of (1),

from Ibragimov’s theorem, we obtain the general formulae of conservation laws for the system consisting of (1) and the adjoint equation as follows:

where is the Lie characteristic function, is the formal Lagrangian in the symmetric form given by (3), and . Thus, the conservation laws for (1) can be derived from above formulae (5), (6), and (7) if Lie symmetries of (1) are known. For example, let us construct the conserved vector corresponding to the generator

as follows:

We should point out here that the conservation laws obtained in [10] , , , () are equivalent to our result given above if we transfer the terms , from , to each other and transfer the terms , from , to each other, respectively.

To explain the fact, in general, we show the equivalence of the formulae of conservation laws (5), (6), (7), and the ones in Theorem 3.1 in [10].

Now let us consider the formulae of conserved vector of (1). Observe the facts that in (5)

in (6)

and in (7)

Thus, we have that

Therefore, we can deduce the conserved quality as follows:

Rewriting above result in , we have

this is the result in [10].

Similarly, if we rewrite (5), (6), and (7) in the following way:

then the conservation law can be deduced in as follows:

this is the conservation law in [10].

Adopting the same procedure as above, we see that all the conservation laws obtained in Theorem 3.1 in [10] can be deduced from our result given by (5), (6), and (7); we have checked them and omit the details here.

3. Conclusions

In this letter, we have analyzed the paper [10]. We see that the two so-called “modification rules” in [10] are needless and Ibragimov’s theorem can be applied to construct conservation laws directly for nonlinear equations with higher-order mixed derivatives. By direct calculations, we have found that the conservation laws obtained by the so-called “modification rules” in [10] are equivalent to the one obtained by Ibragimov’s theorem. Therefore, Ibragimov’s theorem on conservation laws need not be modified.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The first author is partly supported by Zhejiang Provincial Natural Science Foundation of China under Grant no. LY12A01003 and subjects research and development foundation of Hangzhou Dianzi University under Grant no. ZX100204004-6. The second author is partly supported by NSFC under Grant no. 11101111.

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