Abstract and Applied Analysis

Volume 2013 (2013), Article ID 742643, 11 pages

http://dx.doi.org/10.1155/2013/742643

## Classification of Exact Solutions for Generalized Form of Equation

Department of Mathematics, Faculty of Science, Firat University, 23119 Elazig, Turkey

Received 24 May 2013; Revised 1 August 2013; Accepted 18 August 2013

Academic Editor: Santanu Saha Ray

Copyright © 2013 Hasan Bulut. 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

The classification of exact solutions, including solitons and elliptic solutions, to the generalized equation by the complete discrimination system for polynomial method has been obtained. From here, we find some interesting results for nonlinear partial differential equations with generalized evolution.

#### 1. Introduction

In science and engineering applications, it is often very difficult to obtain analytical solutions of partial differential equations. Recently, many exact solutions of partial differential equations have been examined by the use of trial equation method. Also there are a lot of important methods that have been defined such as Hirota method, tanh-coth method, sine-cosine method, the trial equation method, and the extended trial equation method [1–15] to find exact solutions to nonlinear partial differential equations. There are a lot of nonlinear evolution equations that are solved by the use of various mathematical methods. Soliton solutions, singular solitons, and other solutions have been found by using these approaches. These obtained solutions have been encountered in various areas of applied mathematics and are very important.

In Section 2, we introduce an extended trial equation method for nonlinear evolution equations with higher order nonlinearity. In Section 3, as applications, we procure some exact solutions to nonlinear partial differential equations such as the generalized form of equation [16–18]: where are constants since , and . Here, the first term is the generalized evolution term, while the second term represents the nonlinear term and the third term is the dispersion term. This equation is the generalized form of the KdV equation, where, in particular, the case leads to the KdV equation. The Korteweg de Vries equation is one of the most important equations in applied mathematics and physics. There have been several kinds of solutions, such as compactons, that are studied in the context of equation, for various situations. We now offer a more general trial equation method for discussion as follows.

#### 2. The Extended Trial Equation Method

*Step 1. *For a given nonlinear partial differential equation
take the general wave transformation
where and . Substituting (3) into (2) yields a nonlinear ordinary differential equation:

*Step 2. *Take the finite series and trial equation as follows:
where
Using (5) and (6), we can write
where and are polynomials. Substituting these relations into (4) yields an equation of polynomial of :
According to the balance principle, we can find a relation of , , and . We can calculate some values of , , and .

*Step 3. *Letting the coefficients of all be zero will yield an algebraic equations system:
Solving this system, we will determine the values of ; ; and .

*Step 4. *Reduce (6) to the elementary integral form
Using a complete discrimination system for polynomial to classify the roots of , we solve (10) and obtain the exact solutions to (4). Furthermore, we can write the exact traveling wave solutions to (2), respectively.

#### 3. Application to the Generalized Form of Equation

In order to look for travelling wave solutions of (1), we make the transformation , , where is the wave speed. Therefore it can be converted to the ODE where prime denotes the derivative with respect to . Then, integrating this equation with respect to one time and setting the integration constant to zero, we obtain Let , applying balance and using the following transformation: Equation (12) turns into the following equation: Substituting (7) into (14) and using balance principle yield After this solution procedure, we obtain the results as follows.

*Case 1. *If we take , , and , then
where and . Respectively, solving the algebraic equation system (9) yields
Substituting these results into (6) and (10), we havewhere
Integrating (18), we obtain the solutions to (1) as follows:
where
Also , , and are the roots of the polynomial equation
Substituting solutions (20) into (5) and (13), we have
If we take and , then solutions (23) can reduce to rational function solution
1-soliton wave solution
singular soliton solution
and elliptic soliton solution
where , , , , , , , and /. Here, and are the amplitudes of the solitons, while and are the inverse widths of the solitons and is the velocity. Thus, we can say that the solitons exist for .

*Remark 1. *If we choose the corresponding values for some parameters, solution (25) is in full agreement with solution (21) mentioned in [17].

*Case 2. *If we take , , and , then
where and . Respectively, solving the algebraic equation system (9) yields
Substituting these results into (6) and (10), we get
where . Integrating (30), we obtain the solutions to (1) as follows:
where
Also , , , and are the roots of the polynomial equation
Substituting solutions (31) into (5) and (13), we have

For simplicity, if we take , then we can write solutions (34) as follows:
where , , , , and . Here, is the amplitude of the soliton, while is the velocity and and are the inverse widths of the solitons. Thus, we can say that the solitons exist for .

*Case 3. *If we take , , and , then
where and . Respectively, solving the algebraic equation system (9) yields
Substituting these results into (6) and (10), we get
where . Integrating (38), we obtain the solutions to (1) as follows:
where
where
Also , , , , and are the roots of the polynomial equation

*Case 4. *If we take , , and , then
where and . Respectively, solving the algebraic equation system (9) yields
where . Substituting these results into (6) and (10), we get
where . Integrating (45), we obtain the solution to (1) as follows:
where
where
where

*Case 5. *If we take , , and , then
where and . Respectively, solving the algebraic equation system (9) yields
Substituting these results into (6) and (10), we get
where . Integrating (52), we obtain the solution to (1) as follows:
where
where

#### 4. Discussion

Thus we introduce a more general extended trial equation method for nonlinear partial differential equations as follows.

*Step 1. *Extended trial equation (6) can be reduced to the following more general form:
where
Here, , , , and are the constants to be specified.

*Step 2. *Taking trial equations (56) and (57), we derive the following equations:
and other derivation terms such as .

*Step 3. *Substituting , , and other derivation terms into (5) yields the following equation:
According to the balance principle we can determine a relation of , , , and .

*Step 4. *Letting the coefficients of all be zero will yield an algebraic equations system . Solving this equations system, we will determine the values ; ; ; and .

*Step 5. *Substituting the results obtained in Step 4 into (57) and integrating (57), we can find the exact solutions of (3).

#### 5. Conclusions and Remarks

In this study, we proposed an extended trial equation method and used it to obtain some soliton and elliptic function solutions to the generalized equation. Otherwise, we discussed a more general trial equation method. The proposed method can also be applied to other nonlinear differential equations with nonlinear evolution.

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