Solving the Fisher s Equation by Means of Variational Iteration Method
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1 Int. J. Contemp. Math. Sciences, Vol. 4, 29, no. 7, Solving the Fisher s Equation by Means of Variational Iteration Method M. Matinfar 1 and M. Ghanbari 1 Department of Mathematics, University of Mazandaran Babolsar, , Iran 1 m.matinfar@umz.ac.ir Abstract In this paper, we consider variational iteration method (VIM) to obtain exact solution to the Fisher s equation. The variational iteration method is based on Lagrange multipliers for identification of optimal value of parameters in a functional. Using this method, it is possible to find the exact solution or an approximate solution of the problem. Keywords: Variational iteration method(vim); Fisher s equation 1 Introduction In this work, we consider the Fisher s equation u t = u xx + u(1 u), (1) where u t = u,u t xx = 2 u. x 2 Fisher proposed Eq. (1) as a model for the propagation of a mutantgene, with u denoting the density of an advantageous. This equation is encountered in chemical kinetics [7] and population dynamics which includes problems such as nonlinear evolution of a population in a one-dimensional habitat, neutron population in a nuclear reaction. Moreover, the same equation occurs in logistic population growth models [1], flame propagation, neurophysiology, autocatalytic chemical reactions, and branching Brownian motion processes. Ji-Huan He proposed the well-known variational iteration method (VIM) to have a series solution of a nonlinear differential equation using an iterative formula [2, 3, 4]. In this paper, we solve the Fisher s equation via variational iteration method.
2 344 M. Matinfar and M. Ghanbari 2 Variational iteration method To illustrate the basic concepts of VIM, consider the following general nonlinear partial differential equation: Lu(x, t)+ru(x, t)+nu(x, t) =g(x, t), u(x, ) = f(x), (2) where L,R is a linear operator which has partial derivatives with respect t to x, Nu(x, t) is a nonlinear term and g(x, t) is an inhomogeneous term. According to the VIM [2, 3, 4], we can construct the following iteration formula: u n+1 (x, t) =u n (x, t)+ λ{lu n + Rũ n + Nũ n g}dτ, (3) where λ is called a general Lagrange multiplier [5] which can be identified optimally via variational theory, ũ n is considered as restricted variations [2], i.e. δũ n =. Calculating variation with respect to u n, the following stationary conditions are obtained: λ (τ) =, (4) 1+λ(τ) τ=t =, (5) The Lagrange multiplier, therefore, can be identified as λ = 1. Substituting the identified multiplier into Eq. (3) results in the following iteration formula: u n+1 (x, t) =u n (x, t) {Lu n + Ru n + Nu n g}dτ. (6) The second term on the right is called the correction term. Eq. (6) can be solved iteratively using u (x, t) =f(x) as an initial approximation. 3 Variational iteration method (VIM) To illustrate the basic concepts of VIM, consider the following general nonlinear partial differential equation: Lu(x, t)+ru(x, t)+nu(x, t) =g(x, t), u(x, ) = f(x), (7) where L,R is a linear operator which has partial derivatives with respect t to x, Nu(x, t) is a nonlinear term and g(x, t) is an inhomogeneous term. According to the VIM [2, 3, 4], we can construct the following iteration formula: u n+1 (x, t) =u n (x, t)+ λ{lu n + Rũ n + Nũ n g}dτ, (8)
3 Solving the Fisher s equation by means of VIM 345 where λ is called a general Lagrange multiplier [5] which can be identified optimally via variational theory, ũ n is considered as restricted variations [2], i.e. δũ n =. Calculating variation with respect to u n, the following stationary conditions are obtained: λ (τ) =, (9) 1+λ(τ) τ=t =, (1) The Lagrange multiplier, therefore, can be identified as λ = 1. Substituting the identified multiplier into Eq. (3) results in the following iteration formula: u n+1 (x, t) =u n (x, t) {Lu n + Ru n + Nu n g}dτ. (11) The second term on the right is called the correction term. Eq. (6) can be solved iteratively using u (x, t) =f(x) as an initial approximation. 4 Implementation of the VIM in this section, we consider the Fisher s equation u t = u xx + u(1 u), (12) subject to the initial condition u(x, ) = α. To solve Eq. (7) by means of the VIM, substitute in Eq. (6) by Lu = u nτ, Ru n = u nxx, Nu n = u n (1 u n ), and g =, and obtain the following iteration formula: u n+1 (x, t) =u n (x, t) {u nτ u nxx u n (1 u n )}dτ, (13) with the initial approximation u (x, t) =α. The iteration formula (8) will give several approximations, and the exact solution is obtained at the limit of the resulting successive approximations. By using iteration formula (8) and MATLAB software, we can obtain u 1 (x, t) = α + α(1 α)t, u 2 (x, t) = α + α(1 α)t + α(1 α)(1 2α) t2 2! +[ α2 (1 α) 2 t3 3! ],
4 346 M. Matinfar and M. Ghanbari u 3 (x, t) = α + α(1 α)t + α(1 α)(1 2α) t2 2! + α(1 α)(1 6α +6α2 ) t3 3! + [ α 2 (1 2α)(1 α) 2 t4 3 α2 (1 α) 2 (3 2α +2α 2 ) t5 6 + α 3 (1 2α)(1 α) 3 t6 18 α4 (1 α) 4 t7 63 ], u 4 (x, t) = α + α(1 α)t + α(1 α)(1 2α) t2 2! + α(1 α)(1 6α +6α 2 ) t3 3! + α(1 α)(1 2α)(1 12α +12α2 ) t4 4! + [ α 2 (1 α) 2 (11 52α +52α 2 ) t5 6 α 2 (1 2α)(13 12α + 12α 2 )(1 α) 2 t6 36 α 2 (5 148α + 728α 2 116α α 4 )(1 α) 2 t α 3 (1 2α)(23 142α + 142α 2 )(1 α) 3 t α 3 (21 476α α 2 344α α 4 )(1 α) 3 t α 4 (1 2α)(49 33α + 33α 2 )(1 α) 4 t1 945 α 4 ( α α 2 44α α 4 )(1 α) 3 t 11 + α 5 (1 2α)(7 6α +6α 2 )(1 α) 5 t α 6 (1 2α)(1 α) 7 t α 7 (1 2α)(1 α) 7 t α8 (1 α)68 t ], and so on. The solution in a closed form is given by 8316 u(x, t) = α + α(1 α)t + α(1 α)(1 2α) t2 2! + α(1 α)(1 6α +6α2 ) t3 3! + = αe t 1 α + αe, t which is in full agreement with the results in [6]. Fig. 1 shows the comparison between the 7-iterative of VIM and the exact solution.
5 Solving the Fisher s equation by means of VIM Exact solution Approx. solution u t Fig. 1. The exact solution and the 7-iterate VIM for the Fisher s equation (α = 2). 5 Conclusion In this paper, exact solution for the Fisher s equation has been obtained by variational iteration method. The results show that the Variational iteration method is a powerful mathematical tool for finding the exact and approximate solutions of nonlinear equations. In our work we use the MATLAB to calculate the series obtained from the variational iteration method. References [1] P. Brazhnik, J. Tyson, On traveling wave solutions of Fisher s equation in two spatial dimensions, SIAM J. Appl. Math. 6 (2) (1999) [2] J.H. He, A new approach to nonlinear partial differential equations, Commun. Nonlinear Sci. Numer. Simulation, 2 (4) (1997) [3] J.H. He, Variational iteration method-a kind of non-linear analytical technique: some examples, Int. J. Non-Linear Mech. 34 (4) (1999)
6 348 M. Matinfar and M. Ghanbari [4] J.H. He, Some asymptotic methods for strongly nonlinear equations, Int. J. Mod. Phys. B, 2 (1) (26) [5] M. Inokuti, H. Sekine,T. Mura, General use of the Lagrange multiplier in non-linear mathematical physics, in: S. Nemat-Nasser (Ed.),Variational Method in the Mechanics of Solids, Pergamon Press, Oxford, 1978, pp [6] D.S. Jone, B.D. Sleeman, Differential Equations and Mathematical Biology, Chapman and Hall/ CRC, New York, 23. [7] W. Malfliet, Solitary wave solutions of nonlinear wave equations, Am. J. Phys. 7 (1992) Received: July, 28
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