In this paper a parallel algorithm is created for solving electromagnetic wave scattering problems. The algorithm based on the finite difference time-domain (FDTD) representation of the Maxwell's equations written in 3L Parallel Fortran for use on a transputer array. The problem simulated consists
A comparison of the performance of the finite difference time-domain, finite element time-domain, and planar generalized Yee algorithms of high-performance parallel computers
β Scribed by Stephen D. Gedney; Umesh Navsariwala
- Publisher
- John Wiley and Sons
- Year
- 1995
- Tongue
- English
- Weight
- 814 KB
- Volume
- 8
- Category
- Article
- ISSN
- 0894-3370
No coin nor oath required. For personal study only.
β¦ Synopsis
Parallel algorithms for the finite difference time-domain (FDTD), the planar generalized Yee (PGY), and the finite element time-domain (FETD) methods are presented. The FDTD and the PGY algorithms are both explicit time-domain solutions of Maxwell's equations, while the PGY algorithm is based on an unstructured grid. The FETD algorithm is a semi-implicit solution of Maxwell's equations using variational principles, and thus requires a matrix inversion for every time iteration. The three parallel algorithms are based on spatial decompositions of the discrete three-dimensional problem spaces. A comparative analysis of the parallel algorithms is presented based on their memory and computational efficiency as well as their parallel efficiency.
π SIMILAR VOLUMES
An efficient algorithm for implementing the finite-element ( ) time-domain FETD method on parallel computers is presented. An unconditionally stable implicit FETD algorithm is combined with the ( ) finite-element tearing and interconnecting FETI method. This domain decomposition algorithm con¨erges
A comprehensive simulation procedure is presented for describing the behaviour of high-frequency "eld e!ect transistors (FETs). It combines a circuit model of the intrinsic part of the device with a hybrid "nite elements/"nite di!erences (FE/FD) technique directly implemented in time domain (TD). Th
## Abstract In this paper we investigate the performances of firstβ and secondβorder timeβdomain absorbing boundary conditions (ABCs) when introduced in a finiteβelement algorithm to solve electromagnetic scattering problems. Attention is focused on the analysis of the ABC's absorbing characteristi
and is divided into five uniform segments. For the explicit scheme, the time sample was chosen as 0.053 LM. The Ε½ . current at the location 0.0; y0.1 is shown in Figure 4. Again, the agreement is good, and it is seen that for the implicit scheme, one can make β¬ t large and violate the Courant stabil