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Journal of Computational and Applied Mathematics journal homepage: www.elsevier.com/locate/cam
Numerical solution of nonlinear Fredholm integral equations of the second kind using Haar wavelets E. Babolian ∗ , A. Shahsavaran Science and Research Campus, Islamic Azad University of Tehran, Tehran, Iran
article
a b s t r a c t
info
Article history: Received 28 December 2007 Received in revised form 4 June 2008
Keywords: Nonlinear Fredholm integral equation Haar wavelet Error analysis Haar coefficient matrix Block-pulse function Collocation points
1. Introduction Beginning from 1991 the wavelet method has been applied for solving integral equations. A short survey of these papers can be found in [3]. The solutions are often quite complicated and the advantages of the wavelet method get lost. Therefore any kind of simplification is welcome. One possibility for it is to make use of the Haar wavelets, which are mathematically the most simple wavelets. Also, many different basis functions have been used to solve and reduce integral equations to a system of algebraic equations [1–12]. The aim of this work is to present a numerical method for approximating the solution of nonlinear Fredholm integral equation of the second kind: u( t ) −
Z
1
K (t , y)[u(y)]m dy = f (t ),
m>1
0
where, f ∈ L2 [0, 1), K ∈ L2 [0, 1)2 and u is the unknown function to be determined and m is a positive integer [2]. Definition. The Haar wavelet is the function defined on the real line R as: