## Abstract In this study, the electromagnetic scattering from a highβorder inhomogeneous impedance cylinder is investigated. The method presented in this paper is based on the series representation of incident and scattering fields. The inhomogeneousβsurface impedance functions are also expressed
High-Order Nonreflecting Boundary Conditions without High-Order Derivatives
β Scribed by Dan Givoli
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 139 KB
- Volume
- 170
- Category
- Article
- ISSN
- 0021-9991
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β¦ Synopsis
A wave problem in an unbounded domain is often treated numerically by truncating the infinite domain via an artificial boundary B, imposing a so-called nonreflecting boundary condition (NRBC) on B, and then solving the problem numerically in the finite domain bounded by B. A general approach is devised here to construct highorder local NRBCs with a symmetric structure and with only low (first-or second-) order spatial and/or temporal derivatives. This enables the practical use of NRBCs of arbitrarily high order. In the case of time-harmonic waves with finite element discretization, the approach yields a symmetric C 0 finite element formulation in which standard elements can be employed. The general methodology is presented for both the time-harmonic case (Helmholtz equation) and the time-dependent case (the wave equation) and is demonstrated numerically in the former case.
π SIMILAR VOLUMES
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When solvinglinear scattering problems, one typically first solves for the impinging wave in the absence of obstacles. Then, using the linear superposition principle, the original problem is reduced to one which involves only the scattered wave (which is driven by the values of the impinging field a
## Abstract In this study, electromagnetic scattering from inhomogeneous impedance cylinder of arbitrary shape have been solved by means of transformation of problem into equivalent problem, that is scattering from circle represented by high order inhomogeneous impedance boundary condition (IBC). H