Research Article  Open Access
Chunye Gong, Weimin Bao, Guojian Tang, Yuewen Jiang, Jie Liu, "A Domain Decomposition Method for Time Fractional ReactionDiffusion Equation", The Scientific World Journal, vol. 2014, Article ID 681707, 5 pages, 2014. https://doi.org/10.1155/2014/681707
A Domain Decomposition Method for Time Fractional ReactionDiffusion Equation
Abstract
The computational complexity of onedimensional time fractional reactiondiffusion equation is compared with for classical integer reactiondiffusion equation. Parallel computing is used to overcome this challenge. Domain decomposition method (DDM) embodies large potential for parallelization of the numerical solution for fractional equations and serves as a basis for distributed, parallel computations. A domain decomposition algorithm for time fractional reactiondiffusion equation with implicit finite difference method is proposed. The domain decomposition algorithm keeps the same parallelism but needs much fewer iterations, compared with Jacobi iteration in each time step. Numerical experiments are used to verify the efficiency of the obtained algorithm.
1. Introduction
Fractional equations can be used to describe some physical phenomenon more accurately than the classical integer order differential equation. The reactiondiffusion equations play an important role in dynamical systems of mathematics, physics, chemistry, bioinformatics, finance, and other research areas. There has been a wide variety of analytical and numerical methods proposed for fractional equations [1–7], for example, finite difference method [8], finite element method [9], Adomian decomposition method [10], and spectral technique [11]. Interest in fractional reactiondiffusion equations has increased [12].
Domain decomposition methods (DDM) solve a boundary value problem by splitting it into smaller boundary value problems on subdomains and iterating it to coordinate the solution between adjacent subdomains [13]. A coarse problem with one or few unknowns per subdomain is used to further coordinate the solution between the subdomains globally. The DDM can be divided into two categories: the overlapping and nonoverlapping [14]. Chan and Mathew [15] gave a survey on iterative domain decomposition techniques that had been developed for solving several kinds of partial differential equations, including elliptic, parabolic, and differential systems such as the Stokes problem and mixed formulations of elliptic problems. The problems on the subdomains are almost independent, which makes domain decomposition methods suitable for parallel computing. Parallel computing is used to solve intensive computation applications simultaneously [16], such as particle transport [17, 18] and fast multipole methods [19]. It is time consuming to numerically solve fractional differential equations for long time tail. Parallel computing [20–22] can be used to overcome the computational challenge of fractional approximation. DDM will embody large potential for a parallelization of the numerical solution for fractional equations. Until today the power of DDM for approximating fractional derivatives and solving fractional differential equations has not been recognized.
This paper focuses on the Caputo fractional reactiondiffusion equation: on a finite domain and . The and are constants. If equals 1, (1) is the classical reactiondiffusion equation. The fractional derivative is in the Caputo form.
2. Background
2.1. Numerical Solution
The fractional derivative of in the Caputo sense is defined as [23]
If is continuous bounded derivatives in for every , we can get
Define , , , and for , . Define , , and as the numerical approximation to , , and . We can get [12] where , , and
By using center difference scheme for , we can get
The implicit finite difference approximation for (1) is
Define , , , and as
Equation (7) evolves as where matrix is a tridiagonal matrix, defined by
Because , , the elements of matrix satisfy . This means that matrix is strictly diagonally dominant.
2.2. Computational Challenge
In order to get , the rightsided computation of (9) should be performed and tridiagonal linear system should be solved. There are mainly many constant vector multiplications and many vector vector additions in the rightsided computation.(1)The constant vector multiplications are , , and .(2)The vector vector additions are .(3)After solving tridiagonal linear system , we get .
The Thomas algorithm for tridiagonal systems needs multiplications and additions. The computational complexity of is . The total computation of (9) is determined by , which means multiplications and additions for each time step; The computational complexity of (1) is , while the computational complexity of classical onedimensional reactiondiffusion equation is only . The computational cost of (11) varies linearly along the number of grid points but squares with the number of time steps.
3. Domain Decomposition Method
3.1. DDM with Two Subdomains
Similar to the classical alternating Schwarz method [13, 24], the domain can be divided into two subdomains and . There are grid points for . and , where . The global physical boundary is defined in (1). (the right boundary of ) and (the left boundary of ) are called artificial internal boundary.
In order to approximate the time fractional equation on the two subdomains separately, the following iterative procedure can be performed. For each time step, the right hand side of (9) is calculated at first and the is given as initial guess , where . The better approximation of can be obtained iteratively. During each iteration, which is inside of a time step, the time fractional equation is solved in the subdomain , using the approximation of the previous iteration from on as follows: where stands for the previous solution of grid point in subdomain . The better approximation is obtained. is defined as . is defined as . The definitions for and are similar.
Then, we solve the time fractional equation within the subdomain of , using the approximation of the previous iteration from on as follows: where stands for the previous solution of grid point in subdomain .
The two local time fractional equations in and are connected by the artificial boundary condition. The artificial boundary condition on the internal boundary of subdomain is provided by from subdomain , and vice versa. The approximation and may change until converged to the true solution. So, in an inner iteration of each time step, the two time fractional equations need to exchange two sets of data (send one and receive one) to update the artificial boundary conditions.
3.2. A Domain Decomposition Algorithm
Section 3.1 shows the procedure of DDM for time fractional equation with two subdomains. It is not hard to extend the method of Section 3.1 to more than two subdomains. The domain can be decomposed into a set of subdomains with . For time step , has one global boundary and one artificial inner boundary . has one global boundary and one artificial inner boundary . The () has two artificial inner boundaries and . means that the neighboring subdomains have explicit overlap.
The iterative procedure for the time step is similar to Section 3.1. The current iteration of uses the data of previous iteration of its neighboring subdomains. Assuming is divisible with , the domain decomposition algorithm is shown in Algorithm 1.

In Algorithm 1, there are some fast algorithms to solve the tridiagonal matrix , such as Thomas algorithm. is a threshold, such as . The signal is used to count how many iterations are needed in each time step. The data exchange between neighboring iterations is shown in lines 19–22. From the view of computer science, lines 2–6, lines 7–30, and lines 3132 are preprocessing procedure, numerical solver, and postprocessing procedure.
3.3. Analysis
The presented DD algorithm updates the artificial boundary condition in a Jacobi fashion, using approximation from all the relevant neighboring subdomains from the previous iteration for each time step. A subdomain only exchanges two sets of data for one artificial boundary with its neighbor. Therefore, the subdomain solved in Algorithm 1 can be carried out almost completely independently, thus making the method inherently as parallel as the Jacobi iteration. The DD algorithm keeps the good parallelism of Jacobi iteration but needs fewer inner iterations in each time step; see Section 4. Equation (9) can be regarded as approximation of a special integer order reactiondiffusion equation. The stability and convergence analysis of integer order reactiondiffusion equation can refer to Mathew’s book [25].
4. Numerical Example
The following Caputo fractional reactiondiffusion equation [12] was considered, as shown in (14): with , , and
The exact solution of (14) is
With , , , and , the comparison between exact solution and the presented DD algorithm is shown in Table 1. We can find that the DD algorithm compares well with the exact solution.

We can replace the DDM (lines 16–27 of Algorithm 1) with Jacobi method. The Jacobi method for a time step has the same parallelism with the DD algorithm. But the Jacobi method needs more iterations. With and , the comparison between Jacobi method and the presented DD algorithm is shown in Table 2. The sum of “count” (total iterations) for all time steps is recorded. We can see that the DDM needs much less iterations than Jacobi method.

As a part of the future work, we would like to implement an efficient DDM for time fractional equations on parallel computer systems, for example, Tianhe1A supercomputer [26].
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This research work is supported by the National Natural Science Foundation of China under Grant no. 11175253. The authors would like to thank the anonymous reviewers for their helpful comments as well.
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Copyright © 2014 Chunye Gong et al. 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.