[TowerTalk] Fixed Quads
L. B. Cebik
cebik@utkux.utcc.utk.edu
Mon, 31 Jan 2000 08:45:13 -0500 (EST)
On Sat, 29 Jan 2000 n4kg@juno.com wrote:
>
>Re: Full Wave Loop antenna elements de N4KG
>
>Chapter 4 in the W2PV Yagi Antenna Design book
>discusses loop antennas.
>
>Table 4.5, estimated gain and self resistance vs shape,
>is especially interesting.
>
>Shape Sides Gain R (ohms)
> dBi
>
>Triangle 3 2.70 105
>Square 4 2.99 120 (same as diamond)
>Pentagon 5 3.10 126
>Hexagon 6 3.16 129
>Octagon 8 3.22 132
>Circle oo 3.28 135
>
Out of curiosity, I modeled free space loops of the main entries above to
see how well NEC-4 compared to Jim's estimates. Everything is #12 copper
wire. The remnant reactance can be pruned out of the table, but that
would not change anything significantly. Everything is fed bottom center,
but that makes no difference in free space.
Shape Perimeter in ft F-S Gain dBi R+/-jX
Triangle 145.2' 2.85 116.5 - j 4.8
Square 144.0' 3.18 125.7 - j 6.8
Diamond 144.3' 3.10 128.7 - j 2.7
Hexagon 143.4' 3.39 134.5 + j 5.0
Octagon 143.0' 3.45 137.4 + j 7.7
There will be a very slight difference in gain and impedance if you feed a
"shape" at the corner rather than mid-side, but that difference will not
make a performance difference.
Note that for maximum gain with horizontal polarization, a single loop
should have the form of a vertically tall rectangle fed on the shorter
horizontal side. The impedance will also come down closer to 50 Ohms. On
the lower HF bands, the max gain shape and the 50-Ohm shape are not far
apart. Free-space gain may reach the 4.0 to 4.5 dBi range for a single
loop. Of course, structural feasibility at lower HF is always a concern.
For most purposes, then, Jim's table remains a reliable guide.
-73-
LB, W4RNL
L. B. Cebik, W4RNL /\ /\ * / / / Tel: (423) 938-6335
1434 High Mesa Drive / \/ \/\ ----/\---
Knoxville, Tennessee /\ \ \ \ / / || / http://www.cebik.com
37938-4443 USA / \ \ \ \ || e-mail: cebik@utk.edu
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