Solution of the Nonlinear Mixed Volterra-Fredholm Integral Equations by Hybrid of Block-Pulse Functions and Bernoulli Polynomials

A new numerical method for solving the nonlinear mixed Volterra-Fredholm integral equations is presented. This method is based upon hybrid functions approximation. The properties of hybrid functions consisting of block-pulse functions and Bernoulli polynomials are presented. The operational matrices of integration and product are given. These matrices are then utilized to reduce the nonlinear mixed Volterra-Fredholm integral equations to the solution of algebraic equations. Illustrative examples are included to demonstrate the validity and applicability of the technique.

The available sets of orthogonal functions can be divided into three classes. The first class includes sets of piecewise constant basis functions (PCBF's) (e.g., block-pulse, Haar, and Walsh). The second class consists of sets of orthogonal polynomials (e.g., Chebyshev, Laguerre, and Legendre). The third class is the set of sine-cosine functions in the Fourier series.
Orthogonal functions have been used when dealing with various problems of the dynamical systems. The approach is based on converting the underlying differential equation into an integral equation through integration, approximating various signals involved in the equation by truncated orthogonal functions, and using the operational matrix of integration to eliminate the integral operations. The matrix can be uniquely determined based on the particular orthogonal functions (see [15] and references therein). Among orthogonal polynomials, the shifted Legendre polynomial is computationally more effective [16]. The Bernoulli polynomials and Taylor series are not based on orthogonal functions; nevertheless, they possess the operational matrices of integration. However, since the integration of the cross product of two Taylor series vectors is given in terms of a Hilbert matrix [17], which is known to be ill-conditioned, the applications of Taylor series are limited.
Recently, different types of hybrid functions have been used for solving integral equations and proved to be a mathematical power tool [8,11,14].
In the present paper we introduce a new direct computational method to solve nonlinear mixed Volterra-Fredholm integral equations in (1). We approximate the solution not to the equation in its original form but rather to an equivalent equation 1 ( ) = 1 ( , ( )) and 2 ( ) = 2 ( , ( )), ∈ [0, 1]. The functions 1 ( ) and 2 ( ) are approximated by hybrid functions with unknown coefficients. These hybrid functions, which consist of block-pulse functions and Bernoulli polynomials together with their operational matrices of integration and product, are given. These matrices are then used to evaluate the coefficients of the hybrid functions for solution of nonlinear mixed Volterra-Fredholm integral equations.
The outline of this paper is as follows. In Section 2, we introduce properties of Bernoulli polynomials and hybrid functions. In Section 3, the numerical method is used to approximate the nonlinear mixed Volterra-Fredholm integral equations, and in Section 4, we report our numerical findings and demonstrate the accuracy of the proposed numerical scheme by considering five numerical examples.

Properties of Bernoulli Polynomials.
The Bernoulli polynomials of order are defined in [18] by where , = 0, 1, . . . , are Bernoulli numbers. These numbers are a sequence of signed rational numbers, which arise in the series expansion of trigonometric functions [19] and can be defined by the identity The first few Bernoulli numbers are with 2 +1 = 0, = 1, 2, 3, . . .. The first few Bernoulli polynomials are According to [20], Bernoulli polynomials form a complete basis over the interval [0, 1].

Hybrid of Block-Pulse Functions and Bernoulli Polynomials
where and are the order of block-pulse functions and Bernoulli polynomials, respectively.

Function Approximation. Let
with being an arbitrary element in . Since is a finite dimensional vector space, has the unique best approximation out of such as 0 ∈ , that is, Since 0 ∈ , there exist unique coefficients 10 , 20 , . . . , such that Further, by using (9), we can obtain where is a sparse invertible matrix [21].

Function of Two Variables
Approximation. Let ( , ) be a function of two independent variables defined for ∈ [0, 1] and ∈ [0, 1]. Then can be expanded as Let the matrix be given by ] .
From (13), we get Also, ( ) can be expanded as where can be obtained similar to (15).

Operational Matrices of Integration and Product.
The integration of the hybrid functions ( ) defined in (10) is given by where is the ( + 1) × ( + 1) operational matrix of integration. The product of two hybrid functions with the vector is given by wherẽis the ( + 1) × ( + 1) product operational matrix. The matrices and̃are given in [22].

Approximation Errors.
In this section we obtain bounds for the error of best approximation in terms of Sobolev norms. This norm is defined in the interval ( , ) for ≥ 0 by where ( ) denotes the th derivative of . The symbol | | ; (0,1) which is introduced in [23] is defined by is the best approximation of then and, for 1 ≤ ≤ , where depends on .

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Illustrative Example
In this section, five examples are given to demonstrate the applicability and accuracy of our method. Example 1 is a nonlinear mixed Volterra-Fredholm-Hammerstein integral equation which was considered in [13] by using rationalized Haar functions (RHF) and also solved in [24] by applying Chebyshev approximation. Examples 2 and 3 are the integral equations reformulation of the nonlinear two-point boundary value problems considered in [13,25] by using RHF and Adomian method, respectively. Although the reformulated integral equations in Examples 2 and 3 are Fredholm-Hammerstein integral equations, the method described here can be used. Examples 1-3 were also solved in [14] by using hybrid of block-pulse functions and Lagrange polynomials. For Examples 1-3, we compare our findings with the numerical results in [14] which have been shown to be superior to those of [13,24,25]. Examples 4 and 5 are Fredholm and Volterra integral equations of the second kind, respectively, which were considered in [7] by using RHF which were also solved in [8] by using hybrid of block-pulse functions and Legendre polynomials. For Examples 4 and 5, we compare our findings with the numerical results in [8] which have been shown to be superior to those of [7].
(c) The coefficients of individual terms in Bernoulli polynomials ( ) are smaller than the coefficient of individual terms in the Lagrange polynomials ( ). Since the computational errors in the product are related to the coefficients of individual terms, the computational errors are less by using Bernoulli polynomials.
sin ( − ) cos 2 = ( ) 1 ( ) , Table 3 Adomian method Method in [14] P where 1 can be calculated similar to (12). We collocate (38) Solving (40) we obtain in (35). Table 1 shows the absolute errors of exact and approximate solutions in some points of the interval [0, 1] obtained by the present method for = 1 and = 4 together with the method of [14]. In this Table 1 is order of Lagrange polynomials.
Here, is the root of the equation 6 The Scientific World Journal Equation (41) can be reformulated as the integral equation where  [14]. In Table 2, and denote the approximate and exact solutions, respectively. Example 3. In this example we consider the mathematical model for an adiabatic tubular chemical reactor discussed in [27,28], which, in the case of steady state solutions, can be stated as the ordinary differential equation The problem can be converted into a Hammerstein integral equation of the form [28] ( ) = ∫ 1 0 ( , ) ( , ( )) , 0 ≤ ≤ 1, where ( , ) is defined by The existence and uniqueness of the solution for this Hammerstein integral equation with respect to the value of parameters , , and are given in [28]. In [25] the Adomian method is used to solve the integral equation (48) for the particular values of the parameters = 10, = 0.02, and = 3 which guarantee the existence and uniqueness of the solution for this integral equation [28]. Table 3 gives a comparison between the numerical results of ( ) in some points of the interval [0, 1] obtained by the Adomian method given in [25], together with the method in [14] for = 4 and 1 = 7 and by the present method for = 4 and = 4.
with the exact solution ( ) = 2 . Table 4 gives a comparison between the numerical results of ( ) in some points of the interval [0, 1] obtained by the method given in [8] for = 2 and 3 = 11 and by the present method for = 2 and = 4. In this Table 3 is order of Legendre polynomials.
with the exact solution ( ) = (1/3)(2 cos √ 3 + 1). Table 5 gives a comparison between the numerical results of ( ) in some points of the interval [0, 1] obtained by the method given in [8] for = 2 and 3 = 11 and by the present method for = 2 and = 4.
The Scientific World Journal 7 Table 5 Method in [8] P r e s e n t m e t h o d Exact solution with = 2 and 3 = 11 with = 2 and = 4 0.0 1.0000000000

Conclusion
In the present work, the hybrid of block-pulse functions with Bernoulli polynomials is used to solve nonlinear mixed Volterra-Fredholm integral equations. The problem has been reduced to a problem of solving a system of algebraic equations. The matrices and in (17) and (12) have large numbers of zero elements and are sparse matrices, hence, the present method is very attractive and reduces the computer memory. Illustrative examples are given to demonstrate the validity and applicability of the proposed method.