THE THREE-DIMENSIONAL DtN FINITE ELEMENT METHOD FOR RADIATION PROBLEMS OF THE HELMHOLTZ EQUATION
β Scribed by D. Giljohann; M. Bittner
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 254 KB
- Volume
- 212
- Category
- Article
- ISSN
- 0022-460X
No coin nor oath required. For personal study only.
β¦ Synopsis
A finite element method is presented for solving three-dimensional radiation problems in time-harmonic acoustics. This is done by introducing a so-called ''Dirichlet-to-Neumann'' boundary condition on the outer boundary of the domain discretized with finite elements. This DtN boundary condition is an exact non-reflecting boundary condition. It has been developed by Givoli and Keller [1,2] for two and three dimensions. Calculations, however, have been carried out only for simple two-dimensional cases [2][3][4][5][6]. In this paper, the Dirichlet-to-Neumann boundary condition for problems in three dimensions is dealt with. From the strong form given by Givoli and Keller, the weak form is derived. Numerical examples show the applicability and performance of the DtN boundary condition.
π SIMILAR VOLUMES
The standard "nite element method (FEM) is unreliable to compute approximate solutions of the Helmholtz equation for high wave numbers due to the dispersion, unless highly re"ned meshes are used, leading to unacceptable resolution times. The paper presents an application of the element-free Galerkin
A new finite element method for Nwogu's (O. Nwogu, ASCE J. Waterw., Port, Coast., Ocean Eng., 119, 618 -638 (1993)) one-dimensional extended Boussinesq equations is presented using a linear element spatial discretisation method coupled with a sophisticated adaptive time integration package. The accu
## Abstract Convectionβdominated problems are typified by the presence of strongly directional features such as shock waves or boundary layers. Resolution of numerical solutions using an isotropic mesh can lead to unnecessary refinement in directions parallel to such features. This is particularly