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首页> 外文期刊>RAIRO. Mathematical Modelling and Numerical Analysis. = Modelisation Mathematique et Analyse Numerique >Theoretical analysis of the upwind finite volume scheme on the counter-example of Peterson
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Theoretical analysis of the upwind finite volume scheme on the counter-example of Peterson

机译:以彼得森为例的逆风有限体积方案的理论分析

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摘要

When applied to the linear advection problem in dimension two, the upwind finite volume method is a non consistent scheme in the finite differences sense but a convergent scheme. According to our previous paper [Bouche et al., SIAM J. Numer. Anal. 43 (2005) 578-603], a sufficient condition in order to complete the mathematical analysis of the finite volume scheme consists in obtaining an estimation of order p, less or equal to one, of a quantity that depends only on the mesh and on the advection velocity and that we called geometric corrector. In [Bouche et al., Hermes Science publishing, London, UK (2005) 225-236], we prove that, on the mesh given by Peterson [SIAM J. Numer. Anal. 28 (1991) 133-140] and for a subtle alignment of the direction of transport parallel to the vertical boundary, the infinite norm of the geometric corrector only behaves like h1/2 where h is a characteristic size of the mesh. This paper focuses on the case of an oblique incidence i.e. a transport direction that is not parallel to the boundary, still with the Peterson mesh. Using various mathematical technics, we explicitly compute an upper bound of the geometric corrector and we provide a probabilistic interpretation in terms of Markov processes. This bound is proved to behave like h, so that the order of convergence is one. Then the reduction of the order of convergence occurs only if the direction of advection is aligned with the boundary.
机译:当应用于二维的线性对流问题时,迎风有限体积法是有限差分意义上的非一致方案,而是收敛方案。根据我们之前的论文[Bouche等,SIAM J. Numer。肛门43(2005)578-603]中,为了完成对有限体积方案的数学分析,一个充分的条件在于获得仅依赖于网格并依赖于p的数量的p阶估计,小于或等于1。平流速度,我们称之为几何校正器。在[Bouche等人,爱马仕科学出版社,伦敦,英国(2005)225-236]中,我们证明了在彼得森给出的网格上[SIAM J. Numer。肛门28(1991)133-140],并且对于平行于垂直边界的传输方向进行细微对齐,几何校正器的无穷范数仅表现为h1 / 2,其中h是网格的特征尺寸。本文重点关注倾斜入射的情况,即与彼得森网格仍然不平行于边界的传输方向。使用各种数学技术,我们显式计算了几何校正器的上限,并根据马尔可夫过程提供了概率解释。证明此边界的行为类似于h,因此收敛的阶数为1。然后,仅在对流方向与边界对齐的情况下才会发生收敛阶数的减小。

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