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Re: Topband: Grounding the ends of radials

To: <topband@contesting.com>
Subject: Re: Topband: Grounding the ends of radials
From: "Richard Fry" <rfry@adams.net>
Date: Sat, 25 Jan 2014 19:34:03 -0600
List-post: <topband@contesting.com">mailto:topband@contesting.com>
Elevated radial wires perform much differently than buried radial wires.

Elevated, horizontal radial wires having self-resonant 1/4 wavelength used as all, or part of an elevated counterpoise for a monopole, tee, or inverted L should NOT have a low-Z (direct) path to the earth at the operating frequency at either end of those horizontal conductors -- such as provided by wired connections using ground rods.

If so, then those elevated, horizontal conductors no longer will have the characteristics of opposing, end-fed 1/4-wave conductors -- which have about zero r-f current at the ends opposite their feedpoints and maximum r-f current at their feedpoints, and which produce the best radiation efficiencies from such antenna systems.

The reason for this is that the r-f current flowing in to and out of the ground plane from the end(s) of such grounded, elevated radials constitutes loss that otherwise would add to the fields radiated by that antenna system.
_____

Depending on their wavelengths, number, and geometry, buried radial wires concentric with the base of a monopole provide a relatively low loss path for r-f currents flowing in the earth within about 1/2 wavelength of the monopole (due to its near-field radiation into the ground plane) to flow between the r-f ground connection of the transmit system and the feedpoint of the monopole.

The lower the r-f losses in that path, the greater the radiation efficiency of that antenna system.

As shown by well-documented physical experiments going back to 1937 and many subsequent real-world tests and measurements also accepted by the FCC, a monopole of about 55-deg electrical height or more driven against a set of ~120 buried horizontal radials at equal azimuth spacing and each having a free-space wavelength of about 90 degrees produces a peak inverse-distance groundwave field at 1 km that is within several percent of the maximum theoretical field possible for that applied power when radiated by a perfect monopole of such electrical heights when driven against a perfect ground plane.

R. Fry
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