2003
DOI: 10.2298/sjee0301027s
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Symmetrical linear antennas driven by two-wire lines

Abstract: A new theoretical approach to the problem of the symmetrical linear antenna driven by a two-wire line is presented. Then symmetrical linear antenna and the feeder line are treated as a unique boundary-value problem leading to a system of two simultaneous integral equations containing antenna and line currents as unknown sub-integral functions. The integral equations are approximately solved by the so-called point-matching method. Due to the mutual coupling between the antenna and the line, a new conveniently d… Show more

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Cited by 3 publications
(2 citation statements)
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“…The electric field out of the metal oil tank, in accordance with Maxwell's postulate, originates from the positive induced electric charges and spreads through the surrounding area, as presented in Fig. 5 [22][23][24][25][26][27][28]. Since the surface of the Earth in different circumstances acts practically as an ideal conductor plane, the electrostatic system of charged oil tank -earth, acts as a loaded capacitor, in which the oil tank surface represents a positive coating and its reflection in the mirror with regard to the surface of the earth a negative coating [1,2,18].…”
Section: Generating Of Static Electricity Of Transportation and Storamentioning
confidence: 99%
“…The electric field out of the metal oil tank, in accordance with Maxwell's postulate, originates from the positive induced electric charges and spreads through the surrounding area, as presented in Fig. 5 [22][23][24][25][26][27][28]. Since the surface of the Earth in different circumstances acts practically as an ideal conductor plane, the electrostatic system of charged oil tank -earth, acts as a loaded capacitor, in which the oil tank surface represents a positive coating and its reflection in the mirror with regard to the surface of the earth a negative coating [1,2,18].…”
Section: Generating Of Static Electricity Of Transportation and Storamentioning
confidence: 99%
“…Furthermore, partial tangential and radial components of the magnetic field intensity phasors at the arbitrary field point M k , due to the filament current at the source point T i , could be respectively obtained from the following expressions: along the local coordinate axis ξ could be computed as follows, e.g., [22,23]…”
Section: Figurementioning
confidence: 99%