Polynomial and nonpolynomial spline approaches to the numerical solution of second order boundary value problems
Introduction
Many problems in science and technology are formulated mathematically in boundary value problems for second order differential equations as in heat transfer and deflection in cables.We shall consider a numerical solution of the following linear second order two-point boundary value problem, see [6]subjected to Neumann boundary conditions:where Ai, i = 1, 2 are finite real constants. The functions f(x) and g(x) are continuous on the interval [a, b]. The analytical solution of (1.1) subjected to (1.2) can not be obtained for arbitrary choices of f(x) and g(x).
The numerical analysis literature contains little on the solution of second order two-point boundary value problems (1.1) subjected to Neumann boundary conditions (1.2). Albasiny and Raghavarao [1], [4] solved linear second order two-point boundary problem (1.1) subjected to Dirichlet boundary conditions using cubic polynomial spline. Blue [5] solved this problem using quintic polynomial spline. While, Caglar et al. [3] solved this problem using cubic B-spline. Arshad Khan solved it using parametric cubic spline. Zahra [6], also solved this problem using quadratic polynomial spline at midknots.
In this paper, we use both polynomial and nonpolynomial spline functions to develop numerical methods for obtaining smooth approximations for the solution of the problem (1.1) subjected to Neumann boundary conditions (1.2).
Section snippets
Derivation of the methods
We introduce a finite set of grid points xi by dividing the interval [a, b] into n equal parts.
Let y(x) be the exact solution of the system (1.1) and Si be an approximation to yi = y(xi) obtained by the spline function Qi(x) passing through the points (xi, Si) and (xi+1, Si+1).
Spline solutions
The spline solution of (1.1) with the boundary condition (1.2) is based on the linear equations given by (2.9), (2.10), (2.11) for quadratic polynomial spline and (2.16), (2.17), (2.18) for cubic spline solution and (2.25), (2.26), (2.27) for nonpolynomial spline.
Let Y = (yi+1/2), S = (Si+1/2), C = (Ci), T = (ti), E = (ei+1/2) = Y − S be n-dimensional column vectors. Then we can write the standard matrix equations for nonpolynomial spline method in the form.
Convergence analysis
Our main purpose now is to derive a bound on ∥E∥∞. We now turn back to the error equation (iii) in (3.1) and rewrite it in the formwe getprovided .
It was shown in [2] that, Lemma 4.1 The matrix N given by (3.2) is nonsingular, provided thatwhere .
The proof of Lemma 4.1 follows from the following statement. If T is square matrix
Numerical examples and discussion
We now consider two numerical examples illustrating the comparative performance of nonpolynomial spline method (ii) in (3.1) over quadratic and cubic polynomials spline methods. All calculations are implemented by MATLAB 6. Example 1 Consider the boundary value problemThe analytical solution of (5.1) is Example 2 Consider the boundary value problemThe analytical solution of (5.3)
Conclusion
Table 5, Table 6 show that the accuracy of the nonpolynomial spline method is better than the two polynomial spline methods (quadratic and cubic splines) and is less than half the errors due to quadratic and cubic polynomial splines. Moreover, Nonpolynomial spline method has less computational cost over other polynomial spline methods and by arbitrary choices of α and ω we get the other two methods. So the results obtained by nonpolynomial spline method are very encouraging over other existing
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