TY - GEN
T1 - Analysis of the FDTD method via the discrete oscillator
AU - Schutt-Ainé, José E.
N1 - Publisher Copyright:
© 1999 IEEE.
PY - 1999
Y1 - 1999
N2 - The analysis of the FDTD method is usually performed by assuming an e/sup j/spl omega/t/ time dependence for the field quantities as the response due to a steady-state monochromatic wave excitation. This continuous dependence, when combined with the discrete nature of the Yee grid leads to solution errors and dispersion relations that do not describe accurately the propagation properties in the grid for all frequencies. In this article, the discrete oscillator is introduced and used to study the numerical properties of the FDTD method. Formulas are derived for the propagation characteristics in the one- and two-dimensional cases.
AB - The analysis of the FDTD method is usually performed by assuming an e/sup j/spl omega/t/ time dependence for the field quantities as the response due to a steady-state monochromatic wave excitation. This continuous dependence, when combined with the discrete nature of the Yee grid leads to solution errors and dispersion relations that do not describe accurately the propagation properties in the grid for all frequencies. In this article, the discrete oscillator is introduced and used to study the numerical properties of the FDTD method. Formulas are derived for the propagation characteristics in the one- and two-dimensional cases.
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U2 - 10.1109/APS.1999.789113
DO - 10.1109/APS.1999.789113
M3 - Conference contribution
AN - SCOPUS:85039996922
T3 - IEEE Antennas and Propagation Society International Symposium: Wireless Technologies and Information Networks, APS 1999 - Held in conjunction with USNC/URSI National Radio Science Meeting
SP - 188
EP - 191
BT - IEEE Antennas and Propagation Society International Symposium
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 1999 IEEE Antennas and Propagation Society International Symposium, APSURSI 1999
Y2 - 11 July 1999 through 16 July 1999
ER -