On the analysis of resonators using finite-difference time-domain techniques

被引:7
作者
Wagner, CL [1 ]
Schneider, JB [1 ]
机构
[1] Washington State Univ, Sch Elect Engn & Comp Sci, Pullman, WA 99164 USA
关键词
finite-difference time-domain (FDTD);
D O I
10.1109/TAP.2003.817572
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Because a resonator with perfect electrically conducting (PEC) walls has no complications with absorbing boundary conditions and, for canonical geometries, the resonant frequencies are trivial to find, resonators are often used for analyzing the performance of finite-difference time-domain (FDTD) methods. However, when testing the performance of boundary implementations in an FDTD scheme, one should compare to the resonant frequencies of a "perfect" discretized resonator (not to the mode frequencies in the continuous world). On the other hand, when testing the dispersion properties of a method, the resonant frequencies for some structures can be obtained directly from the dispersion relation, thus obviating the need for any simulation. Here, we demonstrate how the dispersion relation can be used to obtain all the resonant frequencies of a rectangular resonator modeled with the Yee algorithm. Furthermore, it is shown that modes that are degenerate in the continuous world can split into distinct modes in FDTD resonators, while modes that are separate in the continuous world can combine in FDTD resonators, thus yielding extra or missing modes. Analytic results are verified using numerical simulations.
引用
收藏
页码:2885 / 2890
页数:6
相关论文
共 10 条
[1]   A locally conformal finite-difference time-domain (FDTD) algorithm for modeling three-dimensional perfectly conducting objects [J].
Dey, S ;
Mittra, R .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1997, 7 (09) :273-275
[2]   A time-domain method with isotropic dispersion and increased stability on an overlapped lattice [J].
Forgy, EA ;
Chew, WC .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 2002, 50 (07) :983-996
[3]   Application of biorthogonal interpolating wavelets to the Galerkin scheme of time dependent Maxwell's equations [J].
Fujii, M ;
Hoefer, WJR .
IEEE MICROWAVE AND WIRELESS COMPONENTS LETTERS, 2001, 11 (01) :22-24
[4]   Reducing the phase error for finite-difference methods without increasing the order [J].
Nehrbass, JW ;
Jevtic, JO ;
Lee, R .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 1998, 46 (08) :1194-1201
[5]   An analytical and numerical analysis of several locally conformal FDTD schemes [J].
Railton, CJ ;
Schneider, JB .
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, 1999, 47 (01) :56-66
[6]   FDTD dispersion revisited: Faster-than-light propagation [J].
Schneider, JB ;
Wagner, CL .
IEEE MICROWAVE AND GUIDED WAVE LETTERS, 1999, 9 (02) :54-56
[7]   Dispersion of homogeneous and inhomogeneous waves in the Yee finite-difference time-domain grid [J].
Schneider, JB ;
Kruhlak, RJ .
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, 2001, 49 (02) :280-287
[8]   NUMERICAL-SOLUTION OF STEADY-STATE ELECTROMAGNETIC SCATTERING PROBLEMS USING TIME-DEPENDENT MAXWELLS EQUATIONS [J].
TAFLOVE, A ;
BRODWIN, ME .
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, 1975, 23 (08) :623-630
[9]   Divergent fields, charge, and capacitance in FDTD simulations [J].
Wagner, CL ;
Schneider, JB .
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, 1998, 46 (12) :2131-2136
[10]  
YOUNG JL, 1999, P IEEE ANT PROP SOC, V1, P176