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Approximation of a System of Singularly Perturbed Reaction—Diffusion Parabolic Equations in a Rectangle

机译:矩形奇摄动反应扩散方程组的逼近

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摘要

The Dirichlet problem for a system of singularly perturbed reaction–diffusion parabolicequations in a rectangle is considered. The higher order derivatives of the equations are multiplied by aperturbation parameter c2, where e takes arbitrary values in the interval (0, 1]. When £ vanishes, the sys-tem of parabolic equations degenerates into a system of ordinary differential equations with respect tot. When c tends to zero, a parabolic boundary layer with a characteristic width c appears in a neighbor-hood of the boundary. Using the condensing grid technique and the classical finite difference approxi-mations of the boundary value problem, a special difference scheme is constructed that converges c-uni- formly at a rate of O(N~(-2)In~2N + N_0~(-1) ), whereN =minN_s, N_s+ 1 and N_0 + 1 are the numbers of meshpoints on the axes x_s andt,respectively.
机译:考虑了矩形中奇摄动反应扩散方程的Dirichlet问题。方程的高阶导数乘以扰动参数c2,其中e在(0,1]区间中取任意值。当£消失时,抛物方程的系统退化为关于t的常微分方程组当c趋于零时,具有特征宽度c的抛物线边界层出现在边界的邻域中,利用凝聚网格技术和经典的边值问题的有限差分近似,一种特殊的差分方案是构造为以O(N〜(-2)In〜2N + N_0〜(-1))的速率均匀收敛c,其中N = minN_s,N_s + 1和N_0 + 1是轴上的网格点数x_s andt分别。

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