## Abstract In this article, the iterative alternating‐direction‐implicit finite‐difference time‐domain (ADI‐FDTD) method is used to simulate the resonator in electromagnetic field. This method is exactly the same as the original Crank–Nicolson (CN) method, while recognizing the ADI‐FDTD method as
A three-dimensional analysis of planar discontinuities by an iterative method
✍ Scribed by M. Azizi; M. Boussouis; H. Aubert; H. Baudrand
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 511 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
✦ Synopsis
torboat (VCA = 47. Curve b; VCA = 0, Curve c) calculated by the segments with duration about 30 s (solid line), and their approximation by ( 5 ) within the spectrum half-width 0.25 of the vessel velocity, and n = 3 for Curves a and b and 2 for Curve c. Figure shows good agreement between the approximations and the experimental data.
The presented analysis reveals the following:
Receiued 5-14-96
📜 SIMILAR VOLUMES
## Abstract In this paper, electromagnetic wave scattering is formulated in terms of the electric‐field integral equation (EFIE) for a dielectric body of general shape, inhomogeneity, and anisotropy. Applying the pulse‐function expansion and the point‐matching technique, the integral equation can b