1989
DOI: 10.1109/8.24187
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Diffraction of high-frequency electromagnetic waves by curved strips

Abstract: A bstract-The construction of a high-frequency solution in the geometrical theory of diffraction (GTD) format for the generation of edge-diffracted space rays and edge-excited surface waves by an electromagnetic wave normally incident on the edge of a curved impedance strip is discussed. The transformation coefficients necessary for the analysis of the diffraction on curved surfaces with equal or vanishing face impedances are tabulated in a form appropriate for numerical applications. The procedure for evaluat… Show more

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Cited by 9 publications
(3 citation statements)
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“…7(c). Edge diffraction of these WG rays as discussed in [15] can be summarized as v s ∼ṽ i (E1) ·Tew (ϕ k ) ·Πw12 (E1, E2) ·Twe (ϕ) ·Πo2p (E2, p) (28) where from (1) and Fig. 1(c) v i (E1) = exp(j · ka · cos(θ + θo)) (29a) Fig.…”
Section: Appendix B Cwutd Diffraction Coefficientmentioning
confidence: 99%
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“…7(c). Edge diffraction of these WG rays as discussed in [15] can be summarized as v s ∼ṽ i (E1) ·Tew (ϕ k ) ·Πw12 (E1, E2) ·Twe (ϕ) ·Πo2p (E2, p) (28) where from (1) and Fig. 1(c) v i (E1) = exp(j · ka · cos(θ + θo)) (29a) Fig.…”
Section: Appendix B Cwutd Diffraction Coefficientmentioning
confidence: 99%
“…The creeping to creeping coefficientTcc and the surface to observation phase factorΠoMp is given as [15] Tcc = jka/(4 ·υn · (υn − ka)) (33a)…”
Section: Appendix B Cwutd Diffraction Coefficientmentioning
confidence: 99%
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