1964
DOI: 10.1109/tap.1964.1138203
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Radiation resistance of an electric dipole in a magnetoionic medium

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Cited by 27 publications
(6 citation statements)
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“…Our work differs from that of other workers who have considered similar or identical problems [Bun- kin, 1957;Kogelnik, 1960a, b;Kuehl, 1962;Mittra and Deschamps, 1963;Arbel and Felsen, 1963;Balmain, 1964;Ament et al, 1964;Staras, 1964;Weil and Walsh, 1964;Blair, 1964;$eshadri, 1965; 167 WANG AND BELL Gale]s, 1966a, b] in that we have started from a full-wave treatment of the problem and have derived approximate closed form expressions for the radiation resistance which are valid for a wide range of antenna lengths. Using these expressions, we are able to define for the first time the range of antenna length for which a quasi-static analysis, such as that employed by Balmain [1964] and Blair [1964], accurately predicts the radiation resistance of the antenna.…”
Section: Introductioncontrasting
confidence: 54%
“…Our work differs from that of other workers who have considered similar or identical problems [Bun- kin, 1957;Kogelnik, 1960a, b;Kuehl, 1962;Mittra and Deschamps, 1963;Arbel and Felsen, 1963;Balmain, 1964;Ament et al, 1964;Staras, 1964;Weil and Walsh, 1964;Blair, 1964;$eshadri, 1965; 167 WANG AND BELL Gale]s, 1966a, b] in that we have started from a full-wave treatment of the problem and have derived approximate closed form expressions for the radiation resistance which are valid for a wide range of antenna lengths. Using these expressions, we are able to define for the first time the range of antenna length for which a quasi-static analysis, such as that employed by Balmain [1964] and Blair [1964], accurately predicts the radiation resistance of the antenna.…”
Section: Introductioncontrasting
confidence: 54%
“…10. This figure agrees with the results of H. Weil and D. Walsh [12]. When the wave normal surfaces are plotted for each region shown in Fig.…”
Section: Clemmow-mually-allis (Cma) Diagramsupporting
confidence: 91%
“…It can be shown that, for very slight losses (i.e., Z • 0), this increase in the real part of the impedance corresponds to true radiation as opposed to being an intrinsic loss in the medium, i.e., it appears in the far field. Therefore, although a small circular loop is an extremely inefficient transmitting antenna in free space [Weeks, 1968], the enhancement of its radiating characteristics [Weil and Walsh, 1964] due to the magneto-. plasma suggest that it may well be used as a transmitting antenna on board extraterrestrial vehicles.…”
Section: The Plasma Dependence Of the Second Term Of (42) Is Not Of Tmentioning
confidence: 99%