DocumentCode
2869195
Title
FVTD applied to dielectric or wire structures
Author
Bonnet, P. ; Ferrieres, X. ; Grando, J. ; Alliot, J.C.
Author_Institution
Office Nat. d´Etudes et de Recherches Aerospatiales, Chatillon, France
Volume
3
fYear
1996
fDate
21-26 July 1996
Firstpage
2126
Abstract
We have used the well known property that curl Maxwell equations for the electric and magnetic fields can be transformed in a condensed equation. For dielectric structures it is assumed that the permittivities have constant values inside the elementary volume cells. As an illustration of the method, we have computed the far scattered field of a dielectric sphere in a transient plane wave. A comparison with results obtained by a time domain integral method is shown. A current injection technique is used to analyse the wire structure, where a wire located above a perfectly conducting plate is fed by a current generator with an infinite impedance. The waveform of the injected current corresponds to a Gaussian pulse. The results of the current along the wire are compared with results obtained when the FDTD method is applied.
Keywords
Maxwell equations; electromagnetic fields; electromagnetic wave scattering; finite difference time-domain analysis; permittivity; wires (electric); FDTD method; FVTD; Gaussian pulse waveform; curl Maxwell equations; current generator; current injection technique; dielectric sphere; dielectric structures; electric fields; elementary volume cells; far scattered field; infinite impedance; magnetic fields; perfectly conducting plate; permittivities; time domain integral method; transient plane wave; wire structures; Dielectrics; Finite difference methods; Impedance; Integral equations; Magnetic fields; Magnetic properties; Maxwell equations; Permittivity; Scattering; Wire;
fLanguage
English
Publisher
ieee
Conference_Titel
Antennas and Propagation Society International Symposium, 1996. AP-S. Digest
Conference_Location
Baltimore, MD, USA
Print_ISBN
0-7803-3216-4
Type
conf
DOI
10.1109/APS.1996.550029
Filename
550029
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