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C h a p t e r 1 3 : C u b i c a l Q u a d s a n d D e l t a L o o p s 327<br />

especially in the case of multielement delta loops, where the elements are often suspended<br />

from a long boom fixed-mounted near the top of the tallest tower in an antenna<br />

installation.<br />

Make no mistake—because of its triangular shape and acute interior angles, the<br />

delta loop is a compromise compared to the square quad loop. Modeling the free-space<br />

difference between a square loop and an equilateral triangle indicates about 0.25 dB<br />

difference in the gain of the main lobe (in favor of the square loop) when the length of<br />

each loop is adjusted for a purely resistive feedpoint impedance at the design frequency.<br />

Nonetheless, the delta loop can do a passable job at providing low-angle gain on the<br />

lower HF bands.<br />

Diamond Loop<br />

The diamond loop consists of a square loop rotated around its broadside axis by 45 degrees.<br />

When fed at a top or bottom corner, as shown in Fig. 13.9, it delivers 1.5 dB more<br />

forward gain in free space than a delta loop designed with the same rules. The extra<br />

gain is the direct result of the greater spacing and better physical layout of the two inverted<br />

vees that form the array. However, that’s not really a fair comparison, since the<br />

height of the diamond loop is twice that of the delta loop for the same frequency. Thus,<br />

the diamond loop is not usually a candidate for the lower HF bands, but single-element<br />

and multielement versions might warrant consideration as fixed arrays at 20 m and<br />

above if the user has a single tall support or can stretch a catenary line between two<br />

such supports.<br />

<br />

4<br />

<br />

4<br />

<br />

4<br />

<br />

4<br />

X 1 X 2<br />

Figure 13.9 Horizontally polarized diamond loop.

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