Abstract

In this article, a numerical solution is proposed for singularly perturbed delay parabolic reaction-diffusion problem with mixed-type boundary conditions. The problem is discretized by the implicit Euler method on uniform mesh in time and extended cubic B-spline collocation method on a Shishkin mesh in space. The parameter-uniform convergence of the method is given, and it is shown to be ε -uniformly convergent of O Δ t + N − 2 ln 2 N , where Δ t and N denote the step size in time and number of mesh intervals in space, respectively. The proposed method gives accurate results by choosing suitable value of the free parameter λ . Some numerical results are carried out to support the theory.

Highlights

  • IntroductionMany researchers have proposed different numerical methods to solve singularly perturbed time delay parabolic reaction-diffusion equations; for instance, see [3,4,5,6,7,8]

  • Let Ω = ð0, 1Þ, D = Ω × ð0, TŠ, and Γ = Γl ∪ Γb ∪ Γr, where Γl and Γr are the left and right sides of the rectangular domain D corresponding to x = 0 and x = 1, respectively, and Γb is the base of the domain and given by Γb=1⁄20, 1Š × 1⁄2−τ, 0Š

  • To see the applicability and efficiency of the proposed method, an example is considered from the literature

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Summary

Introduction

Many researchers have proposed different numerical methods to solve singularly perturbed time delay parabolic reaction-diffusion equations; for instance, see [3,4,5,6,7,8]. The authors in [11] studied singularly perturbed time delay parabolic reaction-diffusion equation subject to mixed-type boundary conditions, yet to the best of our knowledge, no further study has been done. We apply the extended form of cubic B-spline collocation method for singularly perturbed time delay parabolic reaction-diffusion problem subject to mixed boundary conditions. The authors in [17, 18] studied singularly perturbed semilinear differential equation of reaction-diffusion and convection-diffusion type, respectively, using cubic B-spline collocation method on a piecewise Shishkin mesh.

Properties of Continuous Problem
Description of the Numerical Method
Error Analysis
G Á: ð56Þ
Numerical Results and Discussions
Conclusion

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