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216 P a r t I I I : H i g h - F r e q u e n c y B u i l d i n g - B l o c k A n t e n n a s<br />

Each side is <br />

/<br />

2 2<br />

L side = 480<br />

F MHz<br />

}<br />

/<br />

<br />

Matching section<br />

4<br />

1:1 BALUN<br />

transformer<br />

52 Coaxial<br />

cable to receiver<br />

except that each side is now l/2 in length. If the<br />

reactance is canceled out through slight shortening<br />

or lengthening of the total loop, the feedpoint<br />

impedance is a good match for either<br />

52-Ω or 75-Ω cable directly. The difference in<br />

feedpoint impedances between the 2l diamond<br />

loop and the 2l quad loop is a direct result of<br />

changing the location of the feedpoint from the<br />

midpoint of a side to the corner between two<br />

sides.<br />

When operated at its design frequency and<br />

fed as shown in Fig. 7.8, the bisquare antenna<br />

offers maximum horizontally polarized radiation<br />

in free space at a 45-degree elevation angle<br />

broadside to the plane of the antenna (42 degrees<br />

when the feedpoint is l/4 above ground).<br />

The peaks of the vertically polarized radiation<br />

pattern are as before—that is, in the plane of the<br />

wire (to the left and right on the page), but the<br />

gain is 2 dB or so less than that of a single vertical<br />

l/2 dipole, thus proving that “more” is not<br />

always “better”!<br />

In general, there is little to recommend the<br />

added mechanical complexity of a 2l loop unless<br />

the phase relationship between opposing<br />

sections is “corrected” with the use of phasing<br />

lines or inductors.<br />

Near-Vertical Incidence Skywave<br />

(NVIS) <strong>Antenna</strong><br />

The preceding descriptions of large loop operation<br />

in the presence of ground are based on<br />

hanging each loop from one or two high supports.<br />

However, these loop antennas can instead<br />

be suspended so that the plane of the loop of wire is parallel to the ground beneath<br />

it. When that is done, at practical heights above ground these loops will send most of<br />

their radiation straight up in the air, since the innate array pattern of the 1l loops generates<br />

maximum radiation at right angles to the plane of the loop.<br />

Figure 7.8 Bisquare 2l square loop antenna.<br />

Given<br />

0111057<br />

the<br />

FIG<br />

high-angle<br />

14-10<br />

horizontal polarization of the bisquare loop, which favors<br />

short-haul communications links, comparable results can be obtained by laying the<br />

same amount of wire “on its side”, supported at a more practical height. A 2l loop of<br />

wire arranged in a diamond of uniform height l/8 or more can provide nearly the same<br />

gain as the bisquare, albeit in a more omnidirectional pattern. Actually, the pattern of<br />

the 2l NVIS antenna consists of two separate four-lobed cloverleafs: one with horizontally<br />

polarized lobes at right angles to the four wires, and the other with vertically polarized<br />

lobes midway in between.

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