1966
DOI: 10.1002/rds19661131
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Slots in Dielectrically Loaded Waveguide

Abstract: Simple modifications of formulas presented by A. A. Oliner are found to allow the determination of the impedance and resonant length of a slot in rectangular waveguide when the guide is filled with dielectric material. The modifications are justified by reference to earlier work by Oliner and others, and are verified by experimental results.

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Cited by 8 publications
(4 citation statements)
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“…A shunt conductance in a transmission line can be utilized directly to present the long slot inside the planar surface of an air-filled rectangular waveguide [25]. For a filled rectangular waveguide, the single slot normalized resistance is calculated by [26]…”
Section: Single-element Designmentioning
confidence: 99%
“…A shunt conductance in a transmission line can be utilized directly to present the long slot inside the planar surface of an air-filled rectangular waveguide [25]. For a filled rectangular waveguide, the single slot normalized resistance is calculated by [26]…”
Section: Single-element Designmentioning
confidence: 99%
“…From HFSS simulations, the cut-off frequency of the SIW is about 42.8 GHz, a little higher than calculated. As a longitudinal slot in the broad face of an air-filled rectangular waveguide can be represented by a shunt conductance in an equivalent transmission line [12], Oliner's theory [13] can be directly used for the dielectric-filled rectangular waveguide to its calculate normalized resistance [14] by…”
Section: Design Proceduresmentioning
confidence: 99%
“…As a longitudinal slot in the broad face of an air‐filled rectangular waveguide can be represented by a shunt conductance in an equivalent transmission line , Oliner's theory can be directly used for the dielectric‐filled rectangular waveguide to its calculate normalized resistance by RZ0=8πa3b3λ3λnormalg·true[ 1true(2aλnormalgtrue)2 true]2true[ 10.374true(aλtrue)2+0.130true(aλtrue)4 true]sin2true(πxatrue)cos2true(πaλnormalgtrue) where λ is the free space wavelength, λ g is the guide wavelength, x is the offset of the slot from the center line of the rectangular waveguide, a is slot length, and a and b are the width and the length of the rectangular waveguide. In this design, the slot length is chosen to be approximately a half free space wavelength, that is, a=0.48λ.…”
Section: Design Proceduresmentioning
confidence: 99%
“…It was first proposed by Larson et al [12] that filling the SWA with a dielectric material can reduce the waveguide size needed, increase the flexibility in slots location, reduce the slot length that allows spacing the shunt slots entirely in the narrow wall, and prevent electrical breakdown when working with high power microwaves. Larson used Babinet's principle to modify the equations of the radiation resistance, guide wavelength, slots conductance, and slot resonant length for dielectric-filled SWAs, previously presented by Elliott and Oliner in [7], [11].…”
Section: Introductionmentioning
confidence: 99%