Abstract

A higher-order blended compact difference (BCD) scheme is proposed to solve the general two-dimensional (2D) linear second-order partial differential equation. The distinguishing feature of the present method is that methodologies of explicit compact difference and implicit compact difference are blended together. Sixth-order accuracy approximations for the first- and second-order derivatives are employed, and the original equation is also discretized based on a 9-point stencil, which is different from the work of Lee et al. (J. Comput. Appl. Math. 264:23–37, 2014). A truncation error analysis is performed to show that the scheme is of sixth-order accuracy for the interior grid points. Simultaneously, sixth-order accuracy schemes are proposed to compute the grid points on the boundaries for the first- and second-order derivatives. Numerical experiments are conducted to demonstrate the accuracy and efficiency of the present method.

Highlights

  • In this paper, we consider the general two-dimensional (2D) linear partial differential equation in the form a(x, y)uxx + b(x, y)uyy + c(x, y)uxy + p(x, y)ux + q(x, y)uy + r(x, y)u = f (x, y). (1)Here the unknown function u, the variable coefficient functions a, b, c, p, q, r, and the forcing function f are assumed to be continuously differentiable and have the required partial derivatives on Ω

  • We can clearly see that the blended compact difference (BCD) scheme obtains sixth-order accuracy and gets a more accurate solution than the CCD2 scheme

  • It is seen that the BCD and CCD2 schemes are almost not influenced by the increase of Reynolds number, while the FOC scheme gradually loses its fourth-order accuracy

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Summary

Introduction

For the general 2D linear second-order equations with variable coefficients and the mixed derivative term like (1), it is impossible to get an explicit fourthorder compact difference scheme with 9 grid points except under certain conditions mentioned above. Equation (25) is the new BCD scheme we developed It involves the values of the unknown function on 9 grid points (like explicit compact difference scheme) and their first- and second-order derivatives on 3 grid points on each coordinate direction (like implicit compact difference scheme). With more than 4 grid points along one direction, the above boundary difference equations are not strictly compact in the traditional sense, but they are necessary to retain the high-order accuracy of the BCD scheme.

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