1966
DOI: 10.6028/nbs.tn.335
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Zonal harmonics in low frequency terrestrial radio wave propagation.

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Cited by 8 publications
(4 citation statements)
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“…The ELF or VLF frequencies are not, however, the upper limit of usefulness for spherical wave functions in terrestrial radio wave problems. It has been shown [Johler, 1964[Johler, , 1966] that this spherical wave solution can be reformulated as a geometric series to improve the slow convergence of the series of zonal harmonics.…”
mentioning
confidence: 99%
“…The ELF or VLF frequencies are not, however, the upper limit of usefulness for spherical wave functions in terrestrial radio wave problems. It has been shown [Johler, 1964[Johler, , 1966] that this spherical wave solution can be reformulated as a geometric series to improve the slow convergence of the series of zonal harmonics.…”
mentioning
confidence: 99%
“…The waveguide-mode representations normally employed to describe VLF propagation around the earth below an azimuthally symmetric ionosphere (Watson, 1919;Bremmer, 1949;Budden, 1951Budden, , 1952Budden, , 1961Wait, 1960Wait, , 1962Wait, , 1963Wait, , 1964aJohler andBerry, 1962, 1964;Galejs, 1964), involve basically only two coordinates, the vertical and the outward (parallel to the earth's surface) directions relative to the source. These correspond to the z and the p coordinates here.…”
Section: Discussionmentioning
confidence: 99%
“…The source is assumed to be a vertical electric dipole (current moment = Iol amp-m = 1) located in the wave guide. The wave number kj, j = 1, 2, 3, is With the source at the earth's surface, b --a, the vertical electric field E•, for example, can be written [Johler, 1966] At this point it would be instructive to depart from the present development and consider a very crude model. Let us seek a quasi-static approximation to the boundary problem of a dipole source at the earth's surface oscillating at ELF.…”
Section: Theory Of I:)ropagationmentioning
confidence: 99%