TABLE 3 Simulation Results of Parallel Adding Method Number of P -Code 1 2 3 3 Successful Number of P -Code 15044 77 0 7 Total Number of P -Code 823543 823543 823543 7 creases. The interference between the P -code and P -code 7 3 is more serious in VAD. That is, the interference from K is more impo
Perfectly matched anisotropic layer for the numerical analysis of unbounded eddy-current problems
β Scribed by Kosmanis, T.I.; Yioultsis, T.V.; Tsiboukis, T.D.
- Book ID
- 114549413
- Publisher
- IEEE
- Year
- 1999
- Tongue
- English
- Weight
- 166 KB
- Volume
- 35
- Category
- Article
- ISSN
- 0018-9464
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π SIMILAR VOLUMES
Perfectly matched anisotropic absorbers are introduced in two-and three-dimensional beam propagation methods. The anisotropic perfectly matched layer does not require the modification of Maxwell's equations, and can be easily implemented in codes which deal with anisotropic materials. Finite-element
In this paper we analyze a finite element method for the numerical solution of an eddy current problem in a bounded conducting domain. We use a weak formulation in terms of the electric field and impose non-local non-standard boundary conditions. The unique data are the input current intensities whi