DocumentCode
2704022
Title
Elimination of FDTD Numerical Dispersion by using Geometrical Optics
Author
Çiydem, Mehmet ; KOç, S. Sencer
Author_Institution
HVL-USA, Kent, WA
fYear
2006
fDate
9-14 July 2006
Firstpage
3817
Lastpage
3820
Abstract
The ray based time domain (RBTD) method for the computation of time-dependent electromagnetic fields is introduced. RBTD deals with discontinuities of field quantities, transports them along the rays and then constructs time-dependent field by using Taylor series with coefficients being discontinuities at the point of interest. The presented theory of RBTD handles propagation, reflection and refraction of finite jump discontinuities but not diffraction. Transport equations are 1D and RBTD implements xutri=nuxutrit along the ray. Hence in effect, RBTD reduces all higher dimensional problems to 1D along the ray. Honoring directional signal propagation and ODE nature of transport equations provide RBTD to eliminate numerical dispersion and superluminal effect of FDTD, which result from discretization of PDEs
Keywords
differential equations; electromagnetic fields; electromagnetic wave propagation; electromagnetic wave reflection; electromagnetic wave refraction; finite difference time-domain analysis; geometrical optics; series (mathematics); FDTD numerical dispersion elimination; Taylor series; directional signal propagation; finite difference time domain; finite jump discontinuities; geometrical optics; propagation; ray based time domain method; reflection; refraction; time-dependent electromagnetic fields; transport equations; Electromagnetic fields; Electromagnetic propagation; Electromagnetic reflection; Electromagnetic refraction; Equations; Finite difference methods; Geometrical optics; Optical reflection; Taylor series; Time domain analysis;
fLanguage
English
Publisher
ieee
Conference_Titel
Antennas and Propagation Society International Symposium 2006, IEEE
Conference_Location
Albuquerque, NM
Print_ISBN
1-4244-0123-2
Type
conf
DOI
10.1109/APS.2006.1711455
Filename
1711455
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