General Solution of Two Generalized Form of Burgers Equation by Using the (G'/G)-Expansion Method ()
1. Introduction
Nonlinear evolution equations (NLEEs) have been the subject of study in various branches of mathematicalphysical sciences such as physics, biology, chemistry, etc. The analytical solutions of such equations are of fundamental importance since a lot of mathematical-physical models are described by NLEEs. Among the possible solutions to NLEEs, certain special form solutions may depend only on a single combination of variables such as traveling wave variables. In the literature, there is a wide variety of approaches to nonlinear problems for constructing traveling wave solutions. Some of these approaches are the Jacobi elliptic function method [1], inverse scattering method [2], Hirotas bilinear method [3], homogeneous balance method [4], homotopy perturbation method [5], Weierstrass function method [6], symmetry method [7], Adomian decomposition method [8], sine/cosine method [9], tanh/coth method [10], the Exp-function method [11-16] and so on. But, most of the methods may sometimes fail or can only lead to a kind of special solution and the solution procedures become very complex as the degree of nonlinearity increases.
Recently, the 
-expansion method, firstly introduced by Wang et al. [17], has become widely used to search for various exact solutions of NLEEs [17-27]. The 
-expansion method is based on the assumptions that the travelling wave solutions can be expressed by a polynomial in
, and that
, satisfies a second order linear ordinary differential equation
(1)
where 
are arbitrary constants and 
The degree of the polynomial can be determined by considering the homogeneous balance between the highest order derivative and nonlinear terms appearing in the given nonlinear evolution equations. The coefficients of the polynomial can be obtained by solving a set of algebraic equations resulted in from the process of using the method. The 
-expansion method is direct, conciseelementary and effective, and can be used for nonlinear partial differential equation involving higher-order nonlinear terms.
As we know, much work has been done on developing and extending the 
-expansion method for solving nonlinear evolution equations (see, for example [17-27] and their references). But in generalized cases, a small amount of work has been done (see, for example [28,29]). In this paper, we restrict our attention to the study of the following generalized forms of Burgers equation,
(2)
(3)
where 
and 
and 
are constants. These equations are the generalized combined forms of Burgers equation
(4)
Equation (4) is the lowest order approximation for the one-dimensional propagation of weak shock waves in a fluid [30,31]. It is also used in the description of the variation in vehicle density in highway traffic [32]. It is one of the fundamental model equations in fluid mechanics. The Burgers equation demonstrates the coupling between diffusion 
and the convection process
. Burgers introduced this equation to capture some of the features of turbulent fluid in a channel caused by the interaction of the opposite effects of convection and diffusion [33]. It is also used to describe the structure of shock waves, traffic flow, and acoustic transmission [34].
The generalized Burgers-KdV Equation (2) are models for the propagation of waves on an elastic tube (see [28, 29,35,36] and their references). It can be regarded as a combination of the Burgers equation (
, 
,
) and the KdV equation
. EspeciallyIsmail Aslan in [26] applied the 
-expansion method for the Burgers-KdV equation (
) and in [36] Ahmet Bekir applied the tanh method to modified form of Burgers-KdV equation (
). In addition, the generalized Burgers-Fisher Equation (3), see [37], has a wide range of applications in plasma physics, fluid physics, capillary-gravity waves, nonlinear optics and chemical physics [38].
Our first interest in the present work is in implementing the 
-expansion method to stress its power in handling nonlinear equations, so that one can apply it to models of various types of nonlinearity. The next interest is in the determination of exact travelling wave solutions for the generalized form of Equations (2) and (3) especially the modified form of them 
Searching for exact solutions of nonlinear problems has attracted a considerable amount of research work where computer symbolic systems facilitate the computational work.
2. Description of the 
-Expansion Method
The objective of this section is to outline the use of the 
-expansion method for solving certain nonlinear partial differential equations (PDEs). Suppose we have a nonlinear PDE for 
in the form
(5)
where 
is a polynomial in its arguments, which includes nonlinear terms and the highest order derivatives. The transformation 
reduces Equation (5) to the ordinary differential equation (ODE)
(6)
where 
and prime denotes derivative with respect to ξ. We assume that the solution of Equation (6)
can be expressed by a polynomial in 
as follows:
(7)
where
, and 
are constants to be determined later, and 
satisfies the second order linear ordinary differential Equation (1):
(8)
where 
and 
are arbitrary constants. It follows from (7) and (8), that
(9)
(10)
and so on, here the prime denotes the derivative with respective to
.
To determine 
explicitly, we take the following three steps:
Step 1. Determine the integer 
by substituting Equation (7) into Equation (6) and balancing the highest order nonlinear term(s) and the highest order derivative.
Step 2. Substitute Equation (7) along with Equation (8) into Equation (6) and collect all terms with the same order of 
together, the left-hand side of Equation (6) is converted into a polynomial in
. Then set each coefficient of this polynomial to zero to derive a set of algebraic equations for 
and
.
Step 3. Solve the system of algebraic equations obtained in Step 2, for 
and 
by use of Maple, along with the general solutions of Equation (8), we can have more travelling wave solutions of Equation (5).
3. Application
In this section, we will demonstrate the 
-expansion method on the generalized equations listed in (2) and (3).
3.1. Generalized Burgers-KdV Equation
Considering the generalized Burgers-KdV equation with higher-order nonlinear terms
(11)
Now,using the wave variable 
in (11) and integrating the resulting equation and neglecting the constant of integration, we find
(12)
To achieve our goal, we use the transformation
that will carry (12) into the ODE
(13)
According to Step 1, we get
, hence 
We then suppose that Equation (13) has the following formal solutions:
(14)
where 
and 
are constants which are unknown to be determined later.
Substituting Equation (14) into Equation (13) and collecting all terms with the same order of
, togetherthe left-hand sides of Equation (13) are converted into a polynomial in
. Setting each coefficient of each polynomial to zero, we derive a set of algebraic equations for 
and 
(collecting the coefficients of 
and setting it to zeroAppendix I) and solving them by use of Maple, we get the following general result:
(15)
Substitute the above general case in (10), we get
(16)
then use the transformation 
the hyperbolic function solutions of Equation (11), becomes:
(17)
and the trigonometric function solutions of Equation (11), will be:
(18)
where
and 
and 
are arbitrary constants and 
If 
and 
take up special values, the various known results in the literature can be rediscovered, for instance, setting 
then the general solutions (17)- (18) reduces, respectively,
(19)
(20)
and when 
then we deduce from general solutions (17)-(18) that, respectively
(21)
(22)
where
and 
and 
are arbitrary constants and 
In particulars cases, if 
and 
then
and
are the four solitary wave solutions of the particular Burgers-KdV equation
(23)
where 
is arbitrary constant and 
Different real solutions of the general Burgers-KdV Equation (2) were obtained by Ahmet Bekir in [36] using the extended tanh method.
3.2. Generalized Burgers-Fisher Equation
Now considering the generalized Burgers-Fisher equation with higher-order nonlinear terms
(24)
Using the wave variable
, in (24), we find
(25)
To achieve our goal, we use the transformation
that will carry (25) into the ODE
(26)
According to Step 1, we get
, hence 
We then suppose that Equation (26) has the following formal solutions:
(27)
where 
and 
are constants which are unknown to be determined later.
Similar on previous section, substituting Equation (29) into Equation (26) and collecting all terms with the same order of
, together, we derive a set of algebraic equations for 
and 
(collecting the coefficients of 
and setting it to zeroAppendix II) and solving them by use of Maple, we get the following general result:
(28)
Substitute the above general case in (25), we get
(29)
then use the transformation 
the hyperbolic and the trigonometric function solutions of Equation (11), will be:
(30)
(31)
where 
and 
are arbitrary constants and
.
If 
and 
take up special values, the various known results in the literature can be rediscovered, for instance, setting 
then the general solutions (30)-(31) reduces, respectively,
(32)
(33)
and when 
then we deduce from general solutions (30)-(31) that, respectively
(34)
(35)
where 
is arbitrary constant and
.
In particular, if 
then
and
are the four solitary wave solutions of the particular Burgers-Fisher equation
(36)
is arbitrary constant and
.
Different real solutions of the general Burgers-Fisher Equation (3) were obtained by Wazwaz in [39] using the tanh method and by El-Wakil in [38] using a modified tanh-function method and recently by Luwai Wazzan in [28] using a modified tanh-coth method.
4. Conclusions
This study shows that the 
-expansion method is quite efficient and practically well suited for use in finding exact solutions for the generalized form of BurgersKorteweg-de Vries (Burgers-KdV) and Burger-Fisher equations. The results show that this method is a powerful Mathematical tool for obtaining exact solutions for the general B-Fisher and B-KdV equations. With the aid of Maple, we have assured the correctness of the obtained solutions by putting them back into the original equation. It is also a promising method to solve other nonlinear partial differential equations arising in engineering sciences.
5. Acknowledgements
This work is partially supported by Grant-in-Aid from the university of Mohaghegh Ardabili, Ardabil, Iran.
Appendix I
Appendix II
NOTES