2012
DOI: 10.1049/iet-map.2011.0446
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Perfectly conducting tape-helix model for guided electromagnetic wave propagation

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Cited by 12 publications
(7 citation statements)
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“…By enforcing the boundary conditions E z = 0 and E j = 0 at ρ = b, the arbitrary constants C n ′ and D n ′ , n ∈ ℤ in (5) and (6) have been evaluated in terms of C n and D n to be C n ′ = − C n σ bn and…”
Section: Problem Formulationmentioning
confidence: 99%
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“…By enforcing the boundary conditions E z = 0 and E j = 0 at ρ = b, the arbitrary constants C n ′ and D n ′ , n ∈ ℤ in (5) and (6) have been evaluated in terms of C n and D n to be C n ′ = − C n σ bn and…”
Section: Problem Formulationmentioning
confidence: 99%
“…where J (f, z) and J ⊥ (f, z) are the parallel and the perpendicular components of the surface current density, which is confined only to the tape surface, characterised by the axial and the angular components as J J ⊥ = sin cos cos −sin J z J f and the function g(f, z), defined in terms of the indicator functions of the disjoint (for the same value of f) intervals [3][4][5][6][7],…”
Section: Boundary Conditionsmentioning
confidence: 99%
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“…This method has subsequently been extended to solving the problem of guided electromagnetic wave propagation through an open tape helix for the perfectly conducting model in [3]. Beginning with the fundamental work of Sensiper [4] until the publication of [1], all the published derivations [5][6][7][8] of the propagation characteristics of electromagnetic waves guided by an open helical slow-wave structure, modeled invariably to be an anisotropically conducting tape helix, were based on some ad hoc assumption about the tape-current distribution.…”
Section: Introductionmentioning
confidence: 99%