# Exact solutions of two nonlinear partial differential equations by using the first integral method

Hossein Jafari12*, Rahmat Soltani1, Chaudry Masood Khalique2 and Dumitru Baleanu345

### Author affiliations

1 Department of Mathematics, University of Mazandaran, P.O. Box 47416-95447, Babolsar, Iran

2 International Institute for Symmetry Analysis and Mathematical Modelling, Department of Mathematical Sciences, North-West University, Mafikeng Campus, Private Bag X 2046, Mmabatho, 2735, South Africa

3 Department of Mathematics and Computer Sciences, Faculty of Art and Sciences, Çankaya University, Balgat, Ankara, 0630, Turkey

4 Department of Chemical and Materials Engineering, Faculty of Engineering, King Abdulaziz University, P.O. Box 80204, Jeddah, 21589, Saudi Arabia

5 Institute of Space Sciences, P.O. Box MG-23, Magurele, Bucharest, 76900, Romania

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Boundary Value Problems 2013, 2013:117  doi:10.1186/1687-2770-2013-117

 Received: 22 August 2012 Accepted: 12 April 2013 Published: 7 May 2013

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

### Abstract

In recent years, many approaches have been utilized for finding the exact solutions of nonlinear partial differential equations. One such method is known as the first integral method and was proposed by Feng. In this paper, we utilize this method and obtain exact solutions of two nonlinear partial differential equations, namely double sine-Gordon and Burgers equations. It is found that the method by Feng is a very efficient method which can be used to obtain exact solutions of a large number of nonlinear partial differential equations.

##### Keywords:
first integral method; double sine-Gordon equation; Burgers equation; exact solutions

### 1 Introduction

With the availability of symbolic computation packages like Maple or Mathematica, the search for obtaining exact solutions of nonlinear partial differential equations (PDEs) has become more and more stimulating for mathematicians and scientists. Having exact solutions of nonlinear PDEs makes it possible to study nonlinear physical phenomena thoroughly and facilitates testing the numerical solvers as well as aiding the stability analysis of solutions. In recent years, many approaches to solve nonlinear PDEs such as the extended tanh function method [1-6], the modified extended tanh function method [7,8], the exp-function method [9-11], the Weierstrass elliptic function method [12], the Laplace decomposition method [13,14] and so on have been employed.

Among these, the first integral method, which is based on the ring theory of commutative algebra, due to Feng [15-19] has been applied by many authors to solve different types of nonlinear equations in science and engineering [20-23]. Therefore, in the present article, the first integral method is applied to analytic treatment of some important nonlinear of partial differential equations.

The rest of this article is arranged as follows. In Section 2, the basic ideas of the first integral method are expressed. In Section 3, the method is employed for obtaining the exact solutions of double sine-Gordon (SG) and Burgers equations, and finally conclusions are presented in Section 4.

### 2 The first integral method

Let

(1)

be a nonlinear partial differential equation (PDE) with as its solution. We introduce the transformation

(2)

where c is constant. Then we have

(3)

Thus PDE (1) is then transformed to the ordinary differential equation (ODE)

(4)

We now introduce a new transformation, namely

(5)

and this gives us the system of ODEs

(6)

If we can find the integrals of (6) under the same conditions, the qualitative theory of differential equations [24] tells us that the general solutions of (6) can be obtained directly. But in general, it is very difficult even for a single first integral. Since for a plane autonomous system, there is no methodical theory which gives us first integrals, we will therefore apply the division theorem to find one first integral (6), which will reduce (4) to a first-order integral for an ordinary differential equation. By solving this equation, exact solutions of (1) will be obtained. We recall the division theorem.

Theorem 2.1 (Division theorem, see [25])

Letandbe polynomials of two variablesxandyin, and letbe irreducible in. Ifvanishes at all zero points of, then there exists a polynomialinsuch that.

The division theorem follows immediately from the Hilbert-Nullstellensatz theorem [26].

Theorem 2.2 (Hilbert-Nullstellensatz theorem)

LetKbe a field andLbe an algebraic closure ofK. Then:

(i) Every idealγofnot containing 1 admits at least one zero in.

(ii) Let, be two elements of; for the set of polynomials ofzero atxto be identical with the set of polynomials ofzero aty, it is necessary and sufficient that there exists a K-automorphismSofLsuch thatfor.

(iii) For an idealαofto be maximal, it is necessary and sufficient that there exists anxinsuch thatαis the set of polynomials ofzero atx.

(iv) For a polynomialQofto be zero on the set of zeros inof an idealγof, it is necessary and sufficient that there exists an integersuch that.

### 3 Applications

#### 3.1 Exact solutions to the double sine-Gordon equation

Consider the double sine-Gordon (SG) equation [27,28]

(7)

In order to apply the first integral method described in Section 2, we first introduce the transformations

(8)

Using (2) and (3), Eq. (7) becomes

(9)

We next use the transformation

(10)

We obtain

(11)

Next, we introduce new independent variables , which change (11) to the system of ODEs

(12)

Assume that , then (12) becomes

(13)

where .

According to the first integral method, we suppose that and are nontrivial solutions of Eq. (13) and

is an irreducible polynomial in the complex domain such that

(14)

where () are polynomials in X and . Equation (14) is called the first integral to Eq. (13). Applying the division theorem, one sees that there exists a polynomial in the complex domain such that

(15)

Suppose that in (14), and then, by comparing with the coefficients of () on both sides of (15), we have

(16)

(17)

(18)

Since is a polynomial in X, from (16) we conclude that is a constant and . For simplicity, we take . Then Eq. (17) indicates that . Thus, from Eq. (18) we conclude that . Now suppose that

(19)

where , , , , , are all constants to be determined. Substituting Eq. (19) into Eq. (17), we obtain

Then

Substituting , and in (18) and setting all the coefficients of powers X to be zero, we obtain a system of nonlinear algebraic equations, and by solving it, we obtain

(20)

Substituting (20) in (14), we obtain

(21)

Combining Eq. (21) with (13), second-order differential Eq. (11) can be reduced to

(22)

Solving Eq. (22) directly and changing to the original variables, we obtain the exact solutions to Eq. (7):

(23)

(24)

where is an arbitrary constant and .

Therefore, the exact solutions to the double sine-Gordon (SG) equation can be written as

(25)

(26)

where is an arbitrary constant.

#### 3.2 Exact solutions to the Burgers equation

The Burgers equation [29]

(27)

is one of the most famous nonlinear diffusion equations. The positive parameter a refers to a dissipative effect.

Using (2) and (3), Eq. (27) becomes

(28)

We rewrite (28) as follows:

(29)

By introducing new variables and , Eq. (29) changes into a system of ODEs

(30)

Now, the division theorem is employed to seek the first integral to (30). Suppose that and are nontrivial solutions to (30), and is an irreducible polynomial in such that

(31)

where () are polynomials in X and . Equation (31) is called the first integral to Eq. (30). Due to the division theorem, there exists a polynomial in such that

(32)

Suppose that in (31). By comparing the coefficients of () on both sides of (32), we have

(33)

(34)

(35)

Since is a polynomial in X, from (33) we conclude that is a constant and . For simplicity, we take , and balancing the degrees of and , we conclude that or 1. If , suppose that , then from (34), we find

where B is an arbitrary integration constant.

Substituting and in (35) and setting all the coefficients of powers X to be zero, we obtain a system of nonlinear algebraic equations, and by solving it, we obtain

(36)

Using (36) in (31), we obtain

(37)

Combining Eq. (37) with the first part of (30), we obtain the exact solutions of Eq. (29) as follows:

(38)

where is an arbitrary constant.

Therefore, the exact solutions to the Burgers equation can be written as

(39)

where is an arbitrary constant and .

Now suppose that . By an application of the division theorem, we can conclude that there exists a polynomial in such that

(40)

Comparing the coefficients of () of both sides of (40) yields

(41)

(42)

(43)

(44)

Since is a polynomial of X, from (41) we conclude that is a constant and . For simplicity, we take , and balancing the degrees of , and , we conclude that or 1. If , suppose that . Then from (42), we find

where B is an arbitrary constant of integration. From (43) we have

where D is an arbitrary constant of integration. Substituting and in (44) and setting all the coefficients of powers of X to zero, we obtain a system of nonlinear algebraic equations. Solving these equations, we obtain

(45)

Now using (45) in (31), we get

(46)

Combining Eq. (46) with the first part of (30), we obtain the exact solutions to Eq. (29) in the form

(47)

where is an arbitrary constant of integration. Therefore, the exact solutions to the Burgers equation can be written as

(48)

where is an arbitrary constant and .

### 4 Conclusions

The first integral method was employed successfully to solve some important nonlinear partial differential equations, including the double sine-Gordon and Burgers equations, analytically. Some exact solutions for these equations were formally obtained by applying the first integral method. Due to the good performance of the first integral method, we feel that it is a powerful technique in handling a wide variety of nonlinear partial differential equations. Also, this method is computerizable, which permits us to accomplish difficult and tiresome algebraic calculations on a computer with ease.

### Competing interests

The authors declare that they have no competing interests.

### Authors’ contributions

The authors declare that the manuscript was realized in collaboration with the same responsibility. All authors read and approved the final version of the manuscript.

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