Using a mathematical framework originally developed for the development of PML schemes in computational electromagnetics, we develop a set of strongly well-posed PML equations for the absorption of acoustic and vorticity waves in two-dimensional convective acoustics under the assumption of a spatial
Evaluation of the Perfectly Matched Layer for Computational Acoustics
โ Scribed by Quan Qi; Thomas L. Geers
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 315 KB
- Volume
- 139
- Category
- Article
- ISSN
- 0021-9991
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โฆ Synopsis
The perfectly matched layer (PML) recently formulated by Berenger for the absorption of radiated/scattered waves in computational electromagnetics is adapted to computational acoustics, and its effectiveness as a nonreflecting boundary is examined. The excellent absorbing ability of the PML is demonstrated by its small reflection coefficient for a plane wave incident on a plane interface. However, additional frequency-domain and time-domain solutions show that the PML may not be an appropriate computational boundary if the analyst is only interested in the response of the radiator/scatterer and/or the acoustic field in the vicinity of the radiator/scatterer.
๐ SIMILAR VOLUMES
nates, the six components yield 12 subcomponents denoted as E xy , E xz , E yz , E yx , E zx , E zy , H xy , H xz , H yz , The perfectly matched layer is a technique of free-space simulation developed for solving unbounded electromagnetic problems H yx , H zx , H zy , and the Maxwell equations are r
The perfectly matched layer PML absorbing boundary condition has been used for a wide range of applications since its introduction in 1994. Most of these applications haยจe used the PML in a uniform air-filled zone around a nonair scatterer. This paper describes the application of the PML to a geophy
## Abstract A modified __Z__โtransformโbased algorithm for implementing the DโH anisotropic perfectly matched layer (APML) is presented for truncating the finiteโdifference timeโdomain (FDTD) lattices. The main advantage is that, as compared with the previous __Z__โtransformโbased implementation fo
The terms on the right sides of (5) 1 and (5) 2 are mutually exclusive. Whereas A แ ( x แ , ) and ( x แ , ) are some fields that are not necessarily electromagnetic, the six scalars โฃ ฯฎ (), and so on, are uniform in the respective regions and may be considered as constitutive scalars. A blind appli