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# Solving the fractional nonlinear Klein-Gordon equation by means of the homotopy analysis method

- Muhammet Kurulay
^{1, 2}Email author

**2012**:187

https://doi.org/10.1186/1687-1847-2012-187

© Kurulay; licensee Springer 2012

**Received:**23 September 2012**Accepted:**19 October 2012**Published:**2 November 2012

## Abstract

In this paper, the homotopy analysis method is applied to obtain the solution of nonlinear fractional partial differential equations. The method has been successively provided for finding approximate analytical solutions of the fractional nonlinear Klein-Gordon equation. Different from all other analytic methods, it provides us with a simple way to adjust and control the convergence region of solution series by introducing an auxiliary parameter *ħ*. The analysis is accompanied by numerical examples. The algorithm described in this paper is expected to be further employed to solve similar nonlinear problems in fractional calculus.

## Keywords

- fractional nonlinear Klein-Gordon equations
- homotopy analysis method
- analytical solutions

## 1 Introduction

where *u* is a function of *x* and *t*, *a* and *b* are real, *g* is a nonlinear function, and *f* is a known analytic function. The Klein-Gordon equation plays an important role in mathematical physics.

The homotopy perturbation method (HPM) has been successively applied for finding approximate analytical solutions of the fractional nonlinear Klein-Gordon equation which can be used as a numerical algorithm [1]. Analytical approach that can be applied to solve nonlinear differential equations is to employ the homotopy analysis method (HAM) [2–5]. Chowdhury and Hashim have employed HPM for solving Klein-Gordon equations [6]. The main aim of this work is to apply the HPM to solve the nonlinear Klein-Gordon equations of fractional order. An account of the recent developments of HAM was given by Liao [7]. HAM has been successfully applied in engineering fields. The method has been applied to give an explicit solution for the Riemann problem of the nonlinear shallow-water equations [8]. The homotopy analysis method is applied to solve linear and nonlinear fractional partial differential equations (fPDEs) [9]. The obtained Riemann solver has been implemented into a numerical model to simulate long waves, such as storm surge or tsunami, propagation and run-up. Differential equations and nonlinear mechanics very recently, Song and Zhang [10] solved the fractional KdV-Burgers-Kuramoto equation using HAM. Cang *et al.* [11] solved nonlinear Riccati differential equations of fractional order using HAM. Hashim *et al.* [12] employed HAM to solve fractional initial value problems (fIVPs) for ordinary differential equations. In [13] the applicability of HAM was extended to construct a numerical solution for the fractional BBM-Burgers equation. The homotopy analysis method is implemented to give approximate and analytical solutions for the Klein-Gordon equation [14]. The HAM solutions for systems of nonlinear fractional differential equations were presented by Bataineh *et al.* [15]. A specific linear, nonhomogeneous time fractional partial differential equation (fPDE) with variable coefficients was first transformed into two fractional ordinary differential equations, which were then solved by HAM in [16]. Recently, Xu *et al.* [17] applied HAM to linear, homogeneous one- and two-dimensional fractional heat-like PDEs subject to the Neumann boundary conditions. They implemented relatively new, exact series method of solution known as the differential transform method for solving linear and nonlinear Klein-Gordon equations [18]. Jafari and Seifi [19] applied HAM to linear and nonlinear homogeneous fractional diffusion-wave equations. Very recently, HAM was shown to be capable of solving linear and nonlinear systems of fPDEs [20].

## 2 Definitions

### 2.1 The Mittag-Leffler function

*m*th derivatives of Mittag-Leffler functions [21] are given

### 2.2 Laplace’s transform of fractional order

### 2.3 Fractional calculus

We have well-known definitions of a fractional derivative of order $\alpha >0$ such as Riemann-Liouville, Grunwald-Letnikow, Caputo, and generalized functions approach [23, 24]. The most commonly used definitions are those of Riemann-Liouville and Caputo. We give some basic definitions and properties of the fractional calculus theory, which are used throughout the paper.

**Definition 2.1** A real function $f(x)$, $x>0$, is said to be in the space ${C}_{\mu}$, $\mu \in R$, if there exists a real number ($p>\mu $) such that $f(x)={x}^{p}{f}_{1}(x)$, where ${f}_{1}(x)\in C[0,\mathrm{\infty})$, and it is said to be in the space ${C}_{\mu}^{m}$ iff ${f}^{m}\in {C}_{\mu}$, $m\in N$.

**Definition 2.2**The Riemann-Liouville fractional integral operator of order $\alpha \ge 0$ of a function $f\in {C}_{\mu}$, $\mu \ge -1$, is defined as

- 1.
${J}^{\alpha}{J}^{\beta}f(x)={J}^{\alpha +\beta}f(x)$,

- 2.
${J}^{\alpha}{J}^{\beta}f(x)={J}^{\beta}{J}^{\alpha}f(x)$,

- 3.
${J}^{\alpha}{x}^{\gamma}=\frac{\mathrm{\Gamma}(\gamma +1)}{\mathrm{\Gamma}(\alpha +\gamma +1)}{x}^{\alpha +\gamma}$.

The Riemann-Liouville fractional derivative is mostly used by mathematicians, but this approach is not suitable for physical problems of the real world since it requires the definition of fractional order initial conditions which have no physically meaningful explanation yet. Caputo introduced an alternative definition which has the advantage of defining integer order initial conditions for fractional order differential equations.

**Definition 2.3**The fractional derivative of $f(x)$ in the Caputo sense is defined as

for $m-1<v<m$, $m\in N$, $x>0$, $f\in {C}_{-1}^{m}$.

*The Caputo fractional derivative is used here because it allows traditional initial and boundary conditions to be included in the formulation of the problem*.

**Definition 2.5**For

*m*to be the smallest integer that exceeds

*α*, the Caputo time-fractional derivative operator of order $\alpha >0$ is defined as

## 3 Homotopy analysis method

*L* is an auxiliary linear integer order operator and it possesses the property $L(C)=0$, *U* is an unknown function.

*U*in Taylor series with respect to

*q*, one has

*m*times with respect to the embedding parameter

*q*, then setting $q=0$, and finally dividing them by

*m*!, we have the

*m*th-order deformation equation

These equations can be easily solved using software such as Maple, Mathlab and so on.

## 4 Application

*m*th-order deformation equation for $m\ge 1$ becomes

## 5 Conclusion

In this study, the homotopy analysis method with new strategies has been employed to obtain an approximate analytical solution of fractional nonlinear Klein-Gordon equations. It is quite important to notice that a higher number of iteration and higher order of *p* are needed to gain more accuracy.

This work illustrates the validity and great potential of the homotopy analysis method for nonlinear fractional partial differential equations. The basic ideas of this approach are expected to be further employed to solve other nonlinear problems in fractional calculus.

## Declarations

### Acknowledgements

This work was supported by the scientific and technological research council of Turkey (TUBITAK).

## Authors’ Affiliations

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