On the quadratic finite element approximation of one-dimensional waves: Propagation, observation, and control
We study the propagation, observation, and control properties of the quadratic P 2-classical finite element semidiscretization of the one-dimensional wave equation on a bounded interval. A careful Fourier analysis of the discrete wave dynamics reveals two different branches in the spectrum: the acou...
| Autores: | , |
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| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2012 |
| País: | España |
| Institución: | Basque Center for Applied Mathematics (BCAM) |
| Repositorio: | BIRD. BCAM's Institutional Repository Data |
| OAI Identifier: | oai:bird.bcamath.org:20.500.11824/559 |
| Acceso en línea: | http://hdl.handle.net/20.500.11824/559 |
| Access Level: | acceso abierto |
| Palabra clave: | Acoustic/optic mode Bi-grid algorithm Fourier truncation method Observability/controllability property Quadratic finite element method Uniform mesh Vanishing group velocity |
| Sumario: | We study the propagation, observation, and control properties of the quadratic P 2-classical finite element semidiscretization of the one-dimensional wave equation on a bounded interval. A careful Fourier analysis of the discrete wave dynamics reveals two different branches in the spectrum: the acoustic one, of physical nature, and the optic one, related to the perturbations that this second-order finite element approximation introduces with respect to the P 1 one. On both modes there are high frequencies with vanishing group velocity as the mesh size tends to zero. This shows that the classical property of continuous waves of being observable from the boundary fails to be uniform for this discretization scheme. As a consequence of this, the controls of the discrete waves may blow up as the mesh size tends to zero. To remedy these high-frequency pathologies, we design filtering mechanisms based on the Fourier truncation method or on a bi-grid algorithm, for which one can recover the uniformity of the observability constant in a finite time and, consequently, the possibility to control with uniformly bounded L 2-controls appropriate projections of the solutions. This also allow us to show that, by relaxing the control requirement, the controls are uniformly bounded and converge to the continuous ones as the mesh size tends to zero. |
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