A simple preconditioner for electric-field integral equations
✍ Scribed by Yongjun Xie; Jiangqi He; Anders Sullivan; Lawrence Carin
- Publisher
- John Wiley and Sons
- Year
- 2001
- Tongue
- English
- Weight
- 129 KB
- Volume
- 30
- Category
- Article
- ISSN
- 0895-2477
- DOI
- 10.1002/mop.1218
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
A preconditioner is applied to the electric‐field integral equation, to improve the convergence of iterative integral‐equation solvers, such as the conjugate‐gradient (CG) method. The preconditioner accounts for (expansion function)–(testing function) interactions in the vicinity of a given basis function, requiring order N complexity for N unknowns. Example results are presented for microwave scattering calculations for targets in the vicinity of a half space (soil), with results computed via a multilevel fast multipole algorithm. © 2001 John Wiley & Sons, Inc. Microwave Opt Technol Lett 30: 51–54, 2001.
📜 SIMILAR VOLUMES
## Abstract The super‐hyper singularity treatment is developed for solving three‐dimensional (3D) electric field integral equations (EFIE). EFIE usually takes two forms: one of which includes a super‐hyper singular kernel generated by the double gradient of the Green's function. So far, there is no
In this paper, we consider solving potential equations by the boundary integral equation approach. The equations so derived are Fredholm integral equations of the ÿrst kind and are known to be ill-conditioned. Their discretized matrices are dense and have condition numbers growing like O(n) where n
## Abstract The conventional electric field integral equation (EFIE) is augmented by including charge as the extra unknown, so that the contributions of the vector potential and the scalar potential are separated to avoid the imbalance at low frequencies. With the frequency scaling and the direct e
## Abstract In this paper, we present a new formulation using the time‐domain electric‐field integral equation (TD–EFIE) to obtain a transient scattering response from arbitrarily shaped conducting bodies. The time derivative of the magnetic vector potential is approximated with a central finite di