11
Adomian Decomposition Method

11.1 Introduction

The Adomian Decomposition Method (ADM) was first introduced by Adomian in the early 1980s [1,2]. It is an efficient semi‐analytical technique used for solving linear and nonlinear differential equations. It permits us to handle both nonlinear initial value problems (IVPs) and boundary value problems (BVPs).

The solution technique of this method [3,4] is mainly based on decomposing the solution of nonlinear operator equation to a series of functions. Each presented term of the obtained series is developed from a polynomial generated in the expansion of an analytic function into a power series. Generally, the abstract formulation of this technique is very simple, but the actual difficulty arises while calculating the required polynomials and also in proving the convergence of the series of functions. In this chapter, we present procedures for solving linear as well as nonlinear ordinary/partial differential equations by the ADM along with example problems for clear understanding.

The following section addresses the ADM for handling ordinary differential equations (ODEs).

11.2 ADM for ODEs

The ADM mainly depends on decomposing the governing differential equation 5,6] viz. F(x, p(x), p′(x)) = 0 into two components

(11.1)equation

where images and N are the linear and nonlinear parts of F, respectively. The operator Lx is assumed as an invertible operator. Solving for Lx(p(x)), Eq. (11.1) leads to

(11.2)equation

Applying the inverse operator images on both sides of Eq. (11.2) yields

(11.3)equation

where p(0) = φ(x) is the constant of integration which satisfies the given initial conditions. Now assume that the solution “p(x)” can be represented as an infinite series of the form

(11.4)equation

Furthermore, from Eq. (11.4) the nonlinear term N(p(x)) is written as infinite series [ 1 , 2 ] in terms of the Adomian polynomials An(x) of the form

(11.5)equation

where An Adomian polynomials of p0, p1, p2, …, pn are given by the following formula [ 3 , 4 ]:

(11.6)equation

Then, substituting Eqs. ( 11.4 ) and (11.5) in Eq. (11.3) gives

(11.7)equation

From Eq. (11.6), one may find the Adomian polynomials as below [ 4 , 5 ]

(11.8)equation

In order to get the solution images, the process is longer but in practice all the terms of the series may not be required and the solution may be approximated by the truncated series images (by using the convergence of the series).

Next, we present linear and nonlinear IVPs for clear understanding of the ADM for ODEs.

11.3 Solving System of ODEs by ADM

A system of first‐order ordinary differential equations can be considered as [7,8],

(11.21)equation

We can present the system of equations 11.21) as

(11.22)equation

where Lx is the linear operator images with inverse linear operator, images. Applying the inverse operator on Eq. (11.22), we get the following canonical form which is suitable for applying the ADM.

(11.23)equation

where ui(0) are the initial conditions of Eq. ( 11.22 ).

As mentioned earlier, the solution of Eq. ( 11.22 ) using the ADM is considered as the sum of a series

(11.24)equation

and the integrand in Eq. (11.23) reduces to

(11.25)equation

where Ai, j(fi, 0, fi, 1, …, fi, n) are the Adomian polynomials. Substituting Eqs. (11.24) and (11.25) in Eq. ( 11.23 ), we get

(11.26)equation

From Eq. (11.26), we have the following recursive relations as

11.27equation

By solving Eq. ( 11.26 ), we obtain fi, j and images.

11.4 ADM for Solving Partial Differential Equations

Let us consider a general nonlinear partial differential equations (PDEs) in the following form [9]:

(11.29)equation

The linear term of nonlinear PDE is represented as Lu + Ru, while the nonlinear term is represented by Nu. Here, L is the invertible linear operator and R is the remaining linear part. By applying inverse operator images, Eq. (11.29) can be written as

(11.30)equation

where φ(x) is the constant of integration which satisfies the given initial conditions.

Then, the solution may be represented by the decomposition method given in Eq. (11.30) by the following infinite series:

(11.31)equation

The nonlinear operator Nu is then decomposed as

(11.32)equation

where An's are Adomian polynomials defined as

(11.33)equation

By substituting Eqs. (11.31) and (11.32) in Eq. ( 11.30 ), we have

(11.34)equation

Consequently, Eq. (11.34) can be written in terms of recursive relations as

(11.35)equation

Hence, all the terms of “u” may be calculated using the above recursive relations and the general solution obtained according to the ADM images.

11.5 ADM for System of PDEs

ADM transforms system of PDEs into a set of recursive relation that can easily be handled [ 9 ,10]. To understand the method, we now consider the following system of linear PDEs:

(11.38)equation

subject to the initial conditions, p(x, 0) = g1(x); q(x, 0) = g2(x).

The system of linear PDEs, given in Eq. (11.38), can be further written as

(11.39)equation

where Lt and Lx are first‐order partial operators, and f1 and f2 are homogeneous terms. Now, by applying the inverse operator images to Eq. (11.39) and then using the initial conditions we get

(11.40)equation
(11.41)equation

The ADM suggests that the linear terms p(x, t) and q(x, t) are decomposed by infinite series,

(11.42)equation

and

(11.43)equation

By substituting Eqs. (11.42) and (11.43) in Eqs. (11.40) and (11.41), respectively, we obtain

(11.44)equation

and

(11.45)equation

The system is then transformed into a set of following recursive relations:

equation

and

equation

Exercise

  1. 1 Solve the following IVPs by using the ADM
    equation
    equation
  2. 2 Solve the linear system of PDEs
    equation

    with the initial data

    equation
  3. 3 Solve the problem
    equation

    with the initial condition

    equation

References

  1. 1 Wazwaz, A.M. (1998). A comparison between Adomian decomposition method and Taylor series method in the series solutions. Applied Mathematics and Computation 97 (1): 37–44.
  2. 2 Adomian, G. (1990). A review of the decomposition method and some recent results for nonlinear equations. Mathematical and Computer Modelling 13 (7): 17–43.
  3. 3 Momani, S. and Odibat, Z. (2006). Analytical solution of a time‐fractional Navier–Stokes equation by Adomian decomposition method. Applied Mathematics and Computation 177 (2): 488–494.
  4. 4 Evans, D.J. and Raslan, K.R. (2005). The Adomian decomposition method for solving delay differential equation. International Journal of Computer Mathematics 82 (1): 49–54.
  5. 5 Jafari, H. and Daftardar‐Gejji, V. (2006). Revised Adomian decomposition method for solving systems of ordinary and fractional differential equations. Applied Mathematics and Computation 181 (1): 598–608.
  6. 6 Batiha, B., Noorani, M.S.M., and Hashim, I. (2008). Numerical solutions of the nonlinear integro‐differential equations. International Journal of Open Problems in Computer Science 1 (1): 34–42.
  7. 7 Dehghan, M., Shakourifar, M., and Hamidi, A. (2009). The solution of linear and nonlinear systems of Volterra functional equations using Adomian–Pade technique. Chaos, Solitons, and Fractals 39 (5): 2509–2521.
  8. 8 Jafari, H. and Daftardar‐Gejji, V. (2006). Revised Adomian decomposition method for solving a system of nonlinear equations. Applied Mathematics and Computation 175 (1): 1–7.
  9. 9 Bildik, N. and Konuralp, A. (2006). The use of variational iteration method, differential transform method and Adomian decomposition method for solving different types of nonlinear partial differential equations. International Journal of Nonlinear Sciences and Numerical Simulation 7 (1): 65–70.
  10. 10 Wazwaz, A.M. (1999). A reliable modification of Adomian decomposition method. Applied Mathematics and Computation 102 (1): 77–86.
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