1992
DOI: 10.1007/bf01009054
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Transient analysis of microstrip lines with ferrite substrate by extended FD-TD method

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Cited by 14 publications
(6 citation statements)
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“…Earlier FDTD algorithms for ferrites are described in [1], [203]- [211] based on either a frequency-dependent (Polder) tensor as above or on the Gilbert's equation of motion, describing the interaction between the magnetic intensity and the magnetization . An improved FDTD algorithm for ferrite based on the Gilbert's equation of motion and space synchronism is discussed in [212].…”
Section: Combined Effectsmentioning
confidence: 99%
“…Earlier FDTD algorithms for ferrites are described in [1], [203]- [211] based on either a frequency-dependent (Polder) tensor as above or on the Gilbert's equation of motion, describing the interaction between the magnetic intensity and the magnetization . An improved FDTD algorithm for ferrite based on the Gilbert's equation of motion and space synchronism is discussed in [212].…”
Section: Combined Effectsmentioning
confidence: 99%
“…Thus, the algorithm proceeds as follows: first, compute from (3)-(5); second, compute from (14)- (16); and finally compute using the difference equations resulting from discretizing (2) [7]. To solve the above difference equations, a value for has to be selected first as an input parameter.…”
Section: Assumingmentioning
confidence: 99%
“…Thus, the DI schemes presented to date have accomplished the task of simulating electromagnetic effects within magnetic materials but have introduced certain errors in their chosen approximations. For example, Zheng and Chen [2] make the assumption that H n H n01=2 to update magnetization. This assumption leads to a quite simple implementation, but introduces significant inaccuracies in the resulting scheme.…”
Section: Introductionmentioning
confidence: 99%
“…This method begins with the basic Maxwell equations, but leaves Faraday's law dependent on B rather than expressing the solution in terms of H as commonly done. These equations are combined with the Landau-Lifschitz form Manuscript (1) @Bac @t = 0 r 2 E ac (2) where currents are neglected, the electric constitutive relation (D = r E) was used, and the subscript ac is used to indicate that only time-varying fields are considered here. In addition to the curl equations above, the magnetic constitutive relation must be considered H ac = 1 B ac 0 M ac : …”
Section: Introductionmentioning
confidence: 99%