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Grid approximation of a singularly perturbed boundary value problem modelling heat transfer in the case of flow over a flat plate with suction of the boundary layer

机译:奇异摄动边值问题的网格近似,用于模拟在边界层具有吸力的情况下在平板上流动时的传热

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摘要

In the present paper we consider a boundary value problem on the semiaxis (0, ∞) for a singularly perturbed parabolic equation with the two perturbation parameters ε_1 and ε_2 multiplying, respectively, the second and first derivatives with respect to the space variable. Depending on the relation between the parameters, the differential equation can be either of reaction–diffusion type or of convection–diffusion type. Correspondingly, the boundary layer can be either parabolic or regular. For this problem we consider the case when the boundary layer can be controlled by continuous suction of the fluid out of the boundary layer (model problems of this type appear in the mathematical modelling of heat transfer processes for flow past a flat plate). Errors in the approximations generated by standard numerical methods can be unsatisfactorily large for small values of the parameter 1. We construct a monotone finite difference scheme on piecewise uniform meshes which generates numerical solutions converging ε-uniformly with order O(N~(-1) ln N + N_0~(-1)), where N0 is the number of nodes in the time mesh and N is the number of meshpoints on a unit interval of the semiaxis in x. Although the solution of problem has a singularity only for ε_1 → 0, the character of the boundary layer depends essentially on the vector-valued parameter ε = (ε_1, ε_2). This prevents us from constructing an ε-uniformly convergent scheme having a transition parameter which is independent of the parameter ε_2.
机译:在本文中,我们考虑了一个奇摄动抛物方程的半轴(0,∞)上的边值问题,其中两个摄动参数ε_1和ε_2分别乘以相对于空间变量的二阶和一阶导数。根据参数之间的关系,微分方程可以是反应扩散型或对流扩散型。相应地,边界层可以是抛物线的或规则的。对于这个问题,我们考虑可以通过从边界层连续吸出流体来控制边界层的情况(这种类型的模型问题出现在流经平板的传热过程的数学模型中)。对于参数1的较小值,通过标准数值方法生成的近似值中的误差可能会不令人满意地大。我们在分段均匀网格上构造了一个单调有限差分方案,该方案生成数值解以O(N〜(-1)阶均匀收敛)。 ln N + N_0〜(-1)),其中N0是时间网格中的节点数,N是x中半轴单位间隔上的网格点数。尽管问题的解决方案仅对于ε_1→0具有奇异性,但边界层的特征基本上取决于矢量值参数ε=(ε_1,ε_2)。这使我们无法构造一个过渡参数与参数ε_2独立的ε一致收敛方案。

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