## 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
PEC condition implementation for the ADI-FDTD method
✍ Scribed by Juan Chen; Jianguo Wang
- Publisher
- John Wiley and Sons
- Year
- 2007
- Tongue
- English
- Weight
- 308 KB
- Volume
- 49
- Category
- Article
- ISSN
- 0895-2477
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✦ Synopsis
Abstract
The perfect‐electric‐conductor (PEC) condition implementation for the alternating‐direction‐implicit finite‐difference time‐domain (ADI‐FDTD) method is discussed in this article. By comparing different implementation strategies, it shows that the most accurate implementation method is that the PEC condition is directly incorporated within the tridiagonal matrix. Compared with the other two methods commonly used in conventional FDTD, this method is unconditionally stable and has higher accuracy. The theory proposed in this article is validated through numerical examples. © 2007 Wiley Periodicals, Inc. Microwave Opt Technol Lett 49: 526–530, 2007; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.22185
📜 SIMILAR VOLUMES
## Abstract Current implementations of the Mur 1st‐order absorbing boundary condition (Mur1) in the alternating‐direction implicit finite‐difference time‐domain (ADI‐FDTD) method treat the intermediate (half‐step) variables as electromagnetic field quantities that are an approximate solution to Max
## Abstract Bilinear approximation is employed to implement the perfectly matched layer (PML) absorbing boundary condition in the alternating direction implicit (ADI) finite‐difference time‐domain (FDTD) method. Numerical examples show that this implementation is effective and unconditionally stabl
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