Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation

Metzler et al. introduced a fractional Fokker-Planck equation (FFPE) describing a subdiffusive behavior of a particle under the combined influence of external nonlinear force field and a Boltzmann thermal heat bath. In this paper, we present an interval Shannon wavelet numerical method for the FFPE....

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Main Authors: Shu-Li Mei, De-Hai Zhu
Format: Article
Language:English
Published: Hindawi Limited 2013-01-01
Series:Advances in Mathematical Physics
Online Access:http://dx.doi.org/10.1155/2013/821820
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spelling doaj-e0023a54093542c78650c3a09ddd213b2021-07-02T06:39:13ZengHindawi LimitedAdvances in Mathematical Physics1687-91201687-91392013-01-01201310.1155/2013/821820821820Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck EquationShu-Li Mei0De-Hai Zhu1College of Information and Electrical Engineering, China Agricultural University, Beijing 100083, ChinaCollege of Information and Electrical Engineering, China Agricultural University, Beijing 100083, ChinaMetzler et al. introduced a fractional Fokker-Planck equation (FFPE) describing a subdiffusive behavior of a particle under the combined influence of external nonlinear force field and a Boltzmann thermal heat bath. In this paper, we present an interval Shannon wavelet numerical method for the FFPE. In this method, a new concept named “dynamic interval wavelet” is proposed to solve the problem that the numerical solution of the fractional PDE is usually sensitive to boundary conditions. Comparing with the traditional wavelet defined in the interval, the Newton interpolator is employed instead of the Lagrange interpolation operator, so, the extrapolation points in the interval wavelet can be chosen dynamically to restrict the boundary effect without increase of the calculation amount. In order to avoid unlimited increasing of the extrapolation points, both the error tolerance and the condition number are taken as indicators for the dynamic choice of the extrapolation points. Then, combining with the finite difference technology, a new numerical method for the time fractional partial differential equation is constructed. A simple Fokker-Planck equation is taken as an example to illustrate the effectiveness by comparing with the Grunwald-Letnikov central difference approximation (GL-CDA).http://dx.doi.org/10.1155/2013/821820
collection DOAJ
language English
format Article
sources DOAJ
author Shu-Li Mei
De-Hai Zhu
spellingShingle Shu-Li Mei
De-Hai Zhu
Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
Advances in Mathematical Physics
author_facet Shu-Li Mei
De-Hai Zhu
author_sort Shu-Li Mei
title Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
title_short Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
title_full Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
title_fullStr Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
title_full_unstemmed Interval Shannon Wavelet Collocation Method for Fractional Fokker-Planck Equation
title_sort interval shannon wavelet collocation method for fractional fokker-planck equation
publisher Hindawi Limited
series Advances in Mathematical Physics
issn 1687-9120
1687-9139
publishDate 2013-01-01
description Metzler et al. introduced a fractional Fokker-Planck equation (FFPE) describing a subdiffusive behavior of a particle under the combined influence of external nonlinear force field and a Boltzmann thermal heat bath. In this paper, we present an interval Shannon wavelet numerical method for the FFPE. In this method, a new concept named “dynamic interval wavelet” is proposed to solve the problem that the numerical solution of the fractional PDE is usually sensitive to boundary conditions. Comparing with the traditional wavelet defined in the interval, the Newton interpolator is employed instead of the Lagrange interpolation operator, so, the extrapolation points in the interval wavelet can be chosen dynamically to restrict the boundary effect without increase of the calculation amount. In order to avoid unlimited increasing of the extrapolation points, both the error tolerance and the condition number are taken as indicators for the dynamic choice of the extrapolation points. Then, combining with the finite difference technology, a new numerical method for the time fractional partial differential equation is constructed. A simple Fokker-Planck equation is taken as an example to illustrate the effectiveness by comparing with the Grunwald-Letnikov central difference approximation (GL-CDA).
url http://dx.doi.org/10.1155/2013/821820
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