## 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
Analysis of planar circuits using an unconditionally stable 3D ADI-FDTD method
✍ Scribed by Y. Yang; R. S. Chen; W. C. Tang; K. Sha; Edward K. N. Yung
- Publisher
- John Wiley and Sons
- Year
- 2005
- Tongue
- English
- Weight
- 190 KB
- Volume
- 46
- Category
- Article
- ISSN
- 0895-2477
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📜 SIMILAR VOLUMES
## Abstract In this article two special considerations or notes on the implementation of the alternating direction implicit finite‐difference–time‐domain (ADI‐FDTD) method are discussed. In particular, the two notes are (a) the mathematical algorithm used to solve the tridiagonal matrix equation, a
## Abstract In this paper, an improved finite‐difference time‐domain (FDTD) algorithm is proposed in order to eliminate the restraint by the Courant–Friedrich–Levy condition. The new algorithm is developed based on an alternating‐direction implicit (ADI) approach. In this method, the conventional t
## Abstract In this article, an accurate numerical dispersion relationship is developed for 3‐D alternating direction implicit finite difference time domain (ADI FDTD) with artificial anisotropy. The numerical dispersion relation with accurate mathematical model helps to calculate the anisotropic p
## Abstract In this paper, by analyzing the numerical dispersion property of an unconditionally stable three‐dimensional alternating direction implicit finite‐difference time‐domain (ADI‐FDTD) method, the influence of the time steps on the numerical dispersion error of the method is investigated. I