Abstract
The properties of different forms of the combined field integral equation (CFIE) formulation of electromagnetic scattering from convex, perfect electrically conducting geometries are considered. Several difficulties encountered in the numerical implementation of the traditional CFIEs of electromagnetic scattering theory are discussed. An alternate form of the CFIE is introduced which is free of many of the deficiencies of traditional formulations for smooth, convex geometries. The improved numerical properties of the new formulation are illustrated with numerical examples.
Original language | English |
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Pages (from-to) | 1294-1303 |
Number of pages | 10 |
Journal | IEEE Transactions on Antennas and Propagation |
Volume | 52 |
Issue number | 5 |
DOIs | |
State | Published - May 2004 |
Bibliographical note
Funding Information:Manuscript received October 30, 2000; revised June 4, 2003. This work was supported in part by a Bradley postdoctoral fellowship while the author was with the Electrical and Computer Engineering Department, Virginia Polytechnic Institute and State University, and in part by the Lawrence Livermore National Laboratory under Contract B522019.
Funding
Manuscript received October 30, 2000; revised June 4, 2003. This work was supported in part by a Bradley postdoctoral fellowship while the author was with the Electrical and Computer Engineering Department, Virginia Polytechnic Institute and State University, and in part by the Lawrence Livermore National Laboratory under Contract B522019.
Funders | Funder number |
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The Pennsylvania State University | |
Lawrence Livermore National Laboratory | B522019 |
Virginia Polytechnic Institute and State University |
Keywords
- Integral equations
- Scattering
ASJC Scopus subject areas
- Electrical and Electronic Engineering