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Grid Approximations of the Solution and Diffusion Flux for Singularly Perturbed Equations with Neumann Boundary Conditions

机译:具有Neumann边界条件的奇摄动方程解和扩散通量的网格逼近

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Neumann problems for singularly perturbed parabolic equations ae considered on a segment and on a rectangle #epsilon#~2. When #epsilon#=0, the parabolic equation degenerates, and only the time derivative remains. The normalized diffusion flux, i.e., the product of #epsilon# and the derivative in the direction of normal, is given on the boundary. The solution of a classical discretization method on a uniform grid does not convergo #epsilon# uniformly. Moreover, we show with numerical examples that, in the case of a Neumann problem, the approximate solution and, thereupon, the discretization error may increase without bound for a vanishing #epsilon#. The error can exceed the real solution many times for small #epsilon#. For the solution of the boundary value problems allow us to approximate the solution and the normalized diffusion fluxes #epsilon#-uniformly.
机译:在段上和矩形#epsilon#〜2上考虑奇异摄动抛物方程的Neumann问题。当#epsilon#= 0时,抛物线方程退化,仅保留时间导数。在边界上给出归一化的扩散通量,即,εε与导数在法线方向上的乘积。在均匀网格上经典离散化方法的解决方案不能均匀地收敛。此外,我们通过数值示例表明,在诺伊曼(Neumann)问题的情况下,近似解以及随即的离散化误差可能会增加而不会消失#epsilon#。对于较小的#epsilon#,该错误可能超出实际解多次。对于边值问题的解,我们可以统一近似地求解该解和归一化扩散通量。

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