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Re: LF: Re: modeling a loop

To: [email protected]
Subject: Re: LF: Re: modeling a loop
From: John Andrews <[email protected]>
Date: Fri, 29 May 2009 19:42:28 -0400
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Jim,

Here is a little hard data which may be of some use. The antenna still exists in somewhat distorted form due to an ice storm last winter.

Conductor height: 23 Meters
Horizontal length: 51 Meters
Perimeter approx. 147 Meters
Conductor: Single 5.7 mm dia. stranded copper, plus plastic insulation.
Lower conductor clearance above ground: 3 Meters, average.

The ground here is made up of glacial droppings -- lots of rocks and boulders, with gravel and sand. Typical conductivity would be 1 mS/M.

RF bridge measured impedances at 137 kHz showed a fairly constant +j213 Ohms reactance over a wide temperature range. Resistance varied from 1.7 Ohms in winter to 2.05 Ohms in summer, representing a temperature range from -4C to 23C.

The impedances at 508 kHz were considerably higher, with about +j1100 Ohms reactance year-round, and a winter to summer resistance range of 52 to 62 Ohms. The perimeter of the loop is close to a quarter wave at this frequency, and the feed point is near the center of the baseline, if that's of any help.

At 137 kHz, a number of far-field (>5 km) measurements in the pattern maxima showed about 1 watt ERP (not EIRP) for 400 watts into the antenna. No measurements were taken at 500 kHz, and the unfortunate events of last winter would prevent any direct comparison.

Hope this might be of some help in the discussion.

John, W1TAG


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