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Journal of Applied Sciences

Year: 2010 | Volume: 10 | Issue: 9 | Page No.: 781-783
DOI: 10.3923/jas.2010.781.783
Solution of Pseudoparabolic Equation by Finite-Element Method
R. Lotfikar and A. Farmany

Abstract: In this study, an approximate solution for the initial-boundary value problem for the pseudoparabolic equation using finite-element method is obtained. It is proved that the constructed sequence converges to the exact solution is possible.

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How to cite this article
R. Lotfikar and A. Farmany, 2010. Solution of Pseudoparabolic Equation by Finite-Element Method. Journal of Applied Sciences, 10: 781-783.

Keywords: initial boundary problem, approximate solution, monotone operators, pseudoparabolic equations, Finite-element method and exact solution

INTRODUCTION

Let, Ω⊂Rn be a bounded domain with the smooth boundary and t>0.

The following initial-boundary value problem (Showalter, 1996):

(1)

(2)

(3)

Where:

and bij(x) = bji(x), aij(x) = aji(x) (i,j = 1,2,...,n) are continuous functions in and the following inequality is valid:

For ∀x ∈ , ∀ξ ∈ ℝn was investigated by Petrosyan and Hakobyan (2008).

The problem in Eq. 1-3 was investigated in the case in which L is linear, M is nonlinear where, L and M are degenerated operators (Petrosyan and Hakobyan, 2008). The solution of a general case in which L and M are nonlinear is considered by Gaevskii et al. (1978). Quarteroni et al. (2000) proved (using Galerkin’s method) that the solution of the problem 1-3 exists (Mamikonyan, 2006).

In this study, we construct an approximate solution of the problem 1-3 using finite-element method for the case in which Ω∈(0,1)x(0,1)⊂ℝ2, Lu = -Δu,

Definition: The function:

may be a weak solution of the problem in Eq. 1-3 if:

and for:

the Eq. 4 is valid:

(4)

Petrosyan and Hakobyan (2008) proved that the Eq. 4 has a unique solution.

Let, we construct an approximate solution for the problem in Eq. 4 using the finite-element method.

Suppose the partition domain Ω = (0,1)2 with a uniform triangulation of mesh size h with respect to x and y as Fig. 1.

Fig. 1: Partition domain Ω = (0,1)2 with a uniform triangulation of mesh size h with respect to x and y

xi+1 -xi = h,i,j = 1,2,...,n,
yj+1-yj = hh = 1/n

We construct the piecewise linear functions φij(x,y) by the following rule:

and linear in the domain of every triangle. In the remained triangles of the square [0,1]x[0,1] we assume φij (x,y) = 0.

In continue, we set N = (n-1)2 as the basis functions. Let, ωn = {(ih, jh); i, j = 1,2,...,n-1}. If we number the points of the set ωn for example:

then, the basis functions φij will be renumbered, i.e., by constructing ψk(Ar) δkr (k,r = 1,2,...,n-1) we get the system ψ12,...,ψn.

Note that Sn is the linear space generated by the functions ψi = (i = 1,2,...,N) and dimSn = N and where, v is linear in every triangle and v = 0 on ∂Ω}.

It is easy to see that:

is a subspace. To calculate,

we use the Table 1.

Table 1: The derivatives of the basis functions ψi

Denote:

To find the weak solution of the problem 1-3 we use the Galerkins method:

which is equivalent to:

(5)

We can rewrite the Eq. 5 in the matrix form:

(6)

where, βN = (α12,...,αN),

It is easy to check that the matrix MN has the following form:

where, E is the unit matrix and A is the following matrix of order of (n-1)x(n-1):

The solution of the system of differential Eq. 6 with the conditions:

(7)

where, ci are the coefficients of the expansion of the function u0(x,y) by the basis ψi(x,y) (i =1,...,N) may be denoted by using αi(t) (i = 1,...,). Thus, we obtain the following sequence of the functions:

This sequence:

converges in:

norm to the weak solution of the problem in Eq. 1-3.

To find the numerical solution of the system 6 we use the θ method (Braess, 2001). Suppose the partition [0,T] into equal parts with the step Δt denote by:

Now we replace the system 6 by the following different system:

(8)

where,

For every k, we get the linear system of equations.

We choose the parameter θ such that the matrix:

will be positive,

Then we can represent the system of Eq. 8 in the following form:

(9)

where, K = HTH.

Denote by:

It is easy to verify that:

CONCLUSION

The initial boundary value problem is investigated for the pseudoparabolic equation with nonlinear operators. An approximate solution for this problem is obtained using the finite element method. Finally it is proved that the constructed sequence converges to the exact solution is possible.

REFERENCES

  • Braess, D., 2001. Finite Elements. Cambridge University Press, Cambridge


  • Gaevskii, K., K. Greger and K. Zakharis, 1978. Nonlinear operator equations and operator differential equations. Mir, Moscow, (In Russian).


  • Mamikonyan, H.A., 2006. The Galerkin Method for Some Class of Nonlinear Degenerate Pseudoparabolic Equations. EGU, Austria, pp: 33-40


  • Petrosyan, A.A. and G.S. Hakobyan, 2008. On a generalization of nonlinear pseudoparabolic variational inequalities. J. Contemporary Math. Anal., 43: 118-125.
    CrossRef    Direct Link    


  • Quarteroni, A., R. Sacco and F. Saleri, 2000. Numerical Mathematics. 1st Edn., Springer, USA


  • Showalter, R.E., 1996. Monotone Operators in Banach space and Nonlinear Partial Differential Equations (Mathematical Surveys and Monographs). American Mathematical Society, Amrica, pp: 278
    Direct Link    

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