2001
DOI: 10.2528/pier00011001
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Space-Harmonic Effects in Helical Slow-Wave Structure --- an Equivalent Circuit Analysis

Abstract: The analysis of a lossless helical slow-wave structure (SWS) using equivalent circuit approach, reported elsewhere, had been carried out for the fundamental mode only. This is essentially used to predict the transmission line parameters. Moreover, in the analysis the

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Cited by 7 publications
(8 citation statements)
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“…For the analysis, in the structure model ( Fig. 1(b)), the rectangular-shaped discrete dielectric support rods are azimuthally smoothed out into a single (or a number of) continuous dielectric tube regions, between the helix and the metal segments tip (b ≤ r ≤ c) of an effective permittivity value ε r which is found from the relative volume of the dielectric support rods in the structure [1][2][3]. For practical helical SWS, the dielectric support rods are usually made of APBN (anisotropic pyrolytic boron nitride ε r = 5.1), quartz (ε r = 3.78), beryllia (ε r = 6.65).…”
Section: Discussionmentioning
confidence: 99%
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“…For the analysis, in the structure model ( Fig. 1(b)), the rectangular-shaped discrete dielectric support rods are azimuthally smoothed out into a single (or a number of) continuous dielectric tube regions, between the helix and the metal segments tip (b ≤ r ≤ c) of an effective permittivity value ε r which is found from the relative volume of the dielectric support rods in the structure [1][2][3]. For practical helical SWS, the dielectric support rods are usually made of APBN (anisotropic pyrolytic boron nitride ε r = 5.1), quartz (ε r = 3.78), beryllia (ε r = 6.65).…”
Section: Discussionmentioning
confidence: 99%
“…1) is field analyzed here to find its dispersion relation and interaction impedance [1][2][3][4][5][6][7][8][9]. The analysis of a loaded helix in the conventional tape model is quite encumbered [5].…”
Section: Dispersion Relationmentioning
confidence: 99%
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“…In addition to the dominant T + 1 mode, there are also other modes including T + 0 , T + 2 as well as the corresponding reflected components T − 1 , T − 0 and T − 2 from the open end of the helix. These modes can be studied rigorously by considering the helix as an infinite periodic structure [6,7]. However, the excitation strength of these modes cannot be obtained in this manner.…”
Section: Introductionmentioning
confidence: 99%