1970
DOI: 10.1049/piee.1970.0176
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Obstacle gain in radio-wave propagation over inhomogeneous earth

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Cited by 11 publications
(15 citation statements)
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“…9(b). The first-order perturbation solution of the integral equation for this case can easily be shown to be 1161, [231 (38) where C = cos 6 and H P ) is the Hankel function of the second kind. Here E is chosen to be sufficiently large that f(x) C= 0…”
Section: Near Coastline Effectsmentioning
confidence: 99%
See 1 more Smart Citation
“…9(b). The first-order perturbation solution of the integral equation for this case can easily be shown to be 1161, [231 (38) where C = cos 6 and H P ) is the Hankel function of the second kind. Here E is chosen to be sufficiently large that f(x) C= 0…”
Section: Near Coastline Effectsmentioning
confidence: 99%
“…In what follows, we introduce a dimensionless quantity G(a) where a = kCx such that f(x) = ~( a ) (39) With a change of variable from x to d , (38) …”
Section: We Choosef(x) = [ Z ' ( X ) -Z] /To T O Be a Continuous Funcmentioning
confidence: 99%
“…For more screens the Kirchhoff-Huygens integral has to be solved numerically Manuscript which, for example, was done to develop the Walfisch-Bertoni model [8]. Based on a series representation pertaining to propagation over irregular terrain given in [9], Vogler derived an integral representation for multiple screen diffraction in case of grazing incidence [10]. Regarding computation, Vogler found a more suitable solution of this multiple integral in terms of sums over repeated integrals of the error function.…”
Section: Introductionmentioning
confidence: 99%
“…An explicit expression of the attenuation was obtained in a series of papers [Furutsu, 1957a, b-I for a radio wave propagation over a class of terrains consisting, along the wave path, of several sections of different heights and different electrical properties, with discontinuous boundaries of the sections and the possible existence of a ridge of arbitrary height at each boundary (as shown in Figure 5). Some of the results were also reviewed by Furutsu [1963a], Furutsu et al [1964], and Furutsu [1965], where some numerical illustrations and sets of graphs for practical application are also added, but a strict version of the equation formulation was not given, although one was to some extent in the original paper [Furutsu, 1957a]. Later, in the work by Wait, [1968], essentially the same problems were considered in two-dimensional space, and an equivalent result was obtained based on the Fresnel-Kirchhoff principle and also an eigenfunction expansion technique.…”
Section: Introductionmentioning
confidence: 99%