Received 15 May 2016; accepted 27 June 2016; published 30 June 2016
The Volterra-Fredholm integral equation (V-FIE) arises from parabolic boundary value problems. The integral equations appear in many problems of physics and engineering. The Adomian decomposition method (ADM) was proposed by George Adomian in   . A lot of examination work has been put as of late in applying this method to a wide range of ordinary differential equations, partial differential equations and integral equations, linear and nonlinear. Many authors discussed solutions of linear and nonlinear integral equations by utilizing different methods. What’s more, others interested singular integral equation.
We consider the linear (V-FIE) with singular kernel given by
There are several techniques that have been utilized to handle the integral Equation (1) in  -  ; a few techniques, for example, the projection method, time collocation method, the trapezoidal Nystrom method, and furthermore analytical or numerical techniques were utilized to treated this equation, but this techniques experienced troubles as far as computational work utilized. In  treated Maleknejad and Hadizadeh Equation (1) by using the Adomian decomposition method presented in   introduced Wazwaz  the modified Adomian decomposition method for solving the Volterra-Fredholm integral equations.
In this work, we display numerical techniques to obtain numerical solution for linear mixed integral equation with Hilbert kernel. In Section 2, we talk about the existence and uniqueness of the solution. In Section 3, we discuss the Adomian decomposition method, as one of the well known technique and we note that the Adomian polynomials do not appear in this work because we handle linear problems. In Section 4, we present the Laplace Adomian decomposition method and apply this method to linear mixed integral equation with Hilbert kernel. In Sections 5 and 6, we display the Toeplitz matrix method.
2. The Existence and Uniqueness of the Solution 
Consider the integral Equation (1), the functions, and are given and called the kernel of Fredholm integral term, Volterra integral term and the free term respectively and is a real parameter (may be complex and has physical meaning). Also, Ω is the domain of integration with respect to position,
and the time t,. While is the unknown function to be determined in the space
In order to guarantee the existence of a unique solution of Equation (1) we assume through this work the following conditions:
(i) The kernel of position ,
Satisfies the discontinuity condition
(ii) The kernel of time satisfies, is a constant,
(iii) The given function with its partial derivatives with respect to position and time t is conti-
nuous in the space, and its norm is defined as
(iv) The unknown function it behaves in this space, as the known function.
3. The Adomian Decomposition Method for Solving Volterra-Fredholm Integral Equation  
Adomian decomposition method   defines the unknown function by an infinite series
where the components will be determined recurrently and the nonlinear term decomposed into an infinite series of Adomian polynomials
The polynomials are produced for all kinds of nonlinearity so that depends just on, relies on upon and, and so on. The Adomian polynomial   , , is given by,
Substituting Equation (2) into Equation (1) to get
The components are computed using the following recursive relations
4. The Combined Laplace-Adomian Decomposition Method Applied to Volterra-Fredholm Integral Equation with Hilbert Kernel  - 
We consider the kernel of Equation (1) take the form and applying the
Laplace transform to both sides of Equation (1) gives:
The linear term will be represented by the Adomian decomposition from Equation (2). Substituting Equation (2) into Equation (7) leads to
The Adomian decomposition method introduces the recursive relation
Applying the inverse Laplace transform to the first part of Equation (9) gives. Utilizing will empower us to evaluate, and so on. This will prompt the complete determination of the components of upon utilizing the second part of Equation (9). The series solution follows promptly after utilizing Equation (2). The obtained series solution may converge to an exact solution if such a solution exists.
5. The System of Fredholm Integral Equations (SFIEs)  
In this part, a numerical technique is used, in the integral Equation (1) to obtain a system of linear integral equa-
tions with singular kernel, so we divide the interval, as
, where Then the formula (1) reduces to SFIEs of the second kind, in the form:
where is the error.
6. The Toeplitz Matrix Method (TMM)  - 
In this section, we apply (TMM) to obtain the numerical solution of the SFIEs (10) with singular kernel, each equation in this system can be written in a simplify form
The integral term in Equation (12) can be written as
We approximate the integral in the right hand side of Equation (13) by
where and are two arbitrary functions to be determined and is the estimate error which depends on and on the way that the coefficients are chosen. Putting in Equation (14) yields a set of two equations in terms of the two functions and. For choosing the values of, the error, in this case, must vanish.
We can, clearly solve the result set of two equations for and, to obtain
Hence, Equation (13) takes the form
The integral Equation (12), after putting, becomes
The formula (18) represents a linear system of algebraic equation , where u is a vector of elements, while is a matrix whose elements are given by
The matrix is a Toeplitz matrix of order, where.
The solution of the system (18) can be obtained in the form
The error term is determined from Equation (14) by letting , to get
7. Numerical Example
Example 1: Consider the linear mixed integral equation with Hilbert kernel
, the exact solution
we obtain Table 1.
In this paper, we applied (LADM) for solution two dimensional linear mixed integral equations of type Volterra- Fredholm with Hilbert kernel. Additionally, comparison was made with Toeplitz matrix method (TMM). It could be concluded that (LADM) was an effective technique and simple in finding very good solutions for these sorts of equations.
Table 1. Results obtained for example 1 and error.
Figure 1. The exact value of u and the value of u using (LADM).
The authors would like to thank the King Abdulaziz city for science and technology.
 Han, G.Q. and Zhang, L.Q. (1994) Asymptotic Expansion for the Trapezoidal Nystrom Method of Linear Volterra-Fredholm Equations. Journal of Computational and Applied Mathematics, 51, 339-348.
 Maleknejad, K. and Hadizadeh, M. (1999) A New Computational Method for Volterra-Fredholm Integral Equations. Journal of Computational and Applied Mathematics, 37, 1-8.
 Adomian, G. (1991) A Review of the Decomposition Method and Some Recent Results for Nonlinear Equation. Computers & Mathematics with Applications, 21, 101-127.
 Cherruault, Y., Saccomandi, G. and Some, B. (1992) New Results for Convergence of Adomian’s Method Applied to Integral Equations. Mathematical and Computer Modelling, 16, 85-93.
 Jafari, H., Tayyebi, E., Sadeghi, S. and Khalique, C.M. (2014) A New Modification of the Adomian Decomposition Method for Nonlinear Integral Equations. International Journal of Advances in Applied Mathematics and Mechanics, 1, 33-39.
 Hendi, F.A. and Bakodah, H.O. (2012) Numerical Solution of Fredholm-Volterra Integral Equation in Two Dimensonal Space By Using Discrete Adomian Decomposition Method”, IJRRAS, 10(3), pp. 466-471,.
 Wazwaz, A.M. (2012) The Combined Laplace Transform-Adomian Decomposition Method for Handling Nonlinear Volterra Integro-Differential Equations. Applied Mathematics and Computation, 216, 1304-1309.
 Abdou, M.A., El-Kalla, I.L. and Al-Bugami, A.M. (2011) Numerical Solution for Volterra-Ferdholm Integral Equation with a Generalized Singular Kernel. Journal of Modern Methods in Numerical Mathematics, 2, 1-15.
 Abdou, M.A., Mohamed, K.I. and Ismail, A.S. (2003) On the Numerical Solution of Fredholm-Voltrra Integral Equation. Journal of Applied Mathematics and Computing, 146, 713-728.