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Numerical approximation of the boundary control for the wave equation with mixed finite elements in a square

机译:正方形有限元混合波动方程边界控制的数值逼近

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摘要

This paper studies the numerical approximation of the boundary control for the wave equation in a square domain. It is known that the discrete and semi-discrete models obtained by discretizing the wave equation with the usual finite-difference or finite-element methods do not provide convergent sequences of approximations to the boundary control of the continuous wave equation as the mesh size goes to zero. Here, we introduce and analyse a new semi-discrete model based on the space discretization of the wave equation using a mixed finite-element method with two different basis functions for the position and velocity. The main theoretical result is a uniform observability inequality which allows us to construct a sequence of approximations converging to the minimal L2-norm control of the continuous wave equation. We also introduce a fully discrete system, obtained from our semi-discrete scheme, for which we conjecture that it provides a convergent sequence of discrete approximations as both h and Δt, the time discretization parameter, go to zero. We illustrate this fact with several numerical experiments.
机译:本文研究了平方域中波动方程边界控制的数值逼近。众所周知,随着网格尺寸的增大,通过通常的有限差分法或有限元方法离散化波动方程而获得的离散和半离散模型无法为连续波动方程的边界控制提供收敛的近似序列。零。在这里,我们介绍并分析一种基于波动方程空间离散化的新半离散模型,该模型使用混合有限元方法,具有两个不同的位置和速度基函数。理论上的主要结果是一致的可观测性不等式,这使我们能够构造一个收敛到连续波方程的最小L 2 -范数控制的逼近序列。我们还介绍了一个完全离散的系统,该系统是从我们的半离散方案中获得的,我们可以推测,由于h和Δt(时间离散参数)都为零,它提供了一个离散近似的收敛序列。我们通过几个数值实验来说明这一事实。

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  • 来源
    《IMA Journal of Numerical Analysis》 |2008年第1期|186-214|共29页
  • 作者

    Carlos Castro†;

  • 作者单位

    Departmento de Matemática e Informática Aplicadas a la Ingeniería Civil Escuela Técnica Superior de Ingenieros de Caminos Canales y Puertos Universidad Politécnica de Madrid 28040 Madrid Spain Laboratoire de Mathématiques de Besançon UMR CNRS 6623 Université de Franche-Comte 16 route de Gray 25030 Besançon cedex France;

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