Quintic B-Spline Technique for Numerical Treatment of Third Order Singular Perturbed Delay Differential Equation

Author:

Vaid Mandeep Kaur,Arora Geeta

Abstract

In this paper, a class of third order singularly perturbed delay differential equation with large delay is considered for numerical treatment. The considered equation has discontinuous convection-diffusion coefficient and source term. A quintic trigonometric B-spline collocation technique is used for numerical simulation of the considered singularly perturbed delay differential equation by dividing the domain into the uniform mesh. Further, uniform convergence of the solution is discussed by using the concept of Hall error estimation and the method is found to be of first-order convergent. The existence of the solution is also established. Computation work is carried out to validate the theoretical results.

Publisher

International Journal of Mathematical, Engineering and Management Sciences plus Mangey Ram

Subject

General Engineering,General Business, Management and Accounting,General Mathematics,General Computer Science

Reference17 articles.

1. Andargie, A., & Reddy, Y. N. (2013). Parameter fitted scheme for singularly perturbed delay differential equations. International Journal of Applied Science and Engineering, 11(4), 361-373.

2. Cimen, E. (2017). A priori estimates for solution of singularly perturbed boundary value problem with delay in convection term. Journal of Mathematical Analysis, 8(1), 202-211.

3. Hall, C.A. (1968). On error bounds for spline interpolation. Journal of Approximation Theory, 1(2), 209-218.

4. Kellogg, R.B., & Tsan, A. (1978). Analysis of some difference approximations for a singular perturbation problem without turning points. Mathematics of Computation, 32(144), 1025-1039.

5. Kumar, D., & Kadalbajoo, M.K. (2012). Numerical treatment of singularly perturbed delay differential equations using B-Spline collocation method on Shishkin mesh. Journal of Numerical Analysis, Industrial and Applied Mathematics, 7(3-4), 73-90.

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