## Abstract We present a parallel implementation of the three‐dimensional alternating direction implicit finite‐difference time‐domain (ADI‐FDTD) method in Cartesian coordinates using the message passing interface (MPI) library. Parallel implementations not only speed up computations but also incre
Two special notes on the implementation of the unconditionally stable ADI-FDTD method
✍ Scribed by An Ping Zhao
- Publisher
- John Wiley and Sons
- Year
- 2002
- Tongue
- English
- Weight
- 168 KB
- Volume
- 33
- Category
- Article
- ISSN
- 0895-2477
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✦ Synopsis
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, and (b) the way to apply the excitation. First, it is found that the ADI‐FDTD method is not always stable if the algorithm (for solving the tridiagonal matrix equation) proposed in the book Numerical Recipes in C is adopted. Consequently, a simple, efficient, and stable mathematical algorithm for solving the tridiagonal matrix equation of the ADI‐FDTD method is presented. Second, it is demonstrated that, to obtain more accurate results for all the field components, the excitation function should be applied to both the first subiteration and the second subiteration, rather than forced in the first subiteration only. The theory proposed in this article is validated through numerical examples. © 2002 Wiley Periodicals, Inc. Microwave Opt Technol Lett 33: 273–277, 2002; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.10295
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