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296 P a r t I V : D i r e c t i o n a l H i g h - F r e q u e n c y A n t e n n a A r r a y s<br />

diameter step at the junction of certain pairs of tubes. Some commercial antenna manufacturers<br />

accomplish this by swaging one end of each tube, but most of us do not have<br />

the tools or the skills to do this at home. The other approach is to insert a few inches of<br />

tubing having the right “in-between” diameter at the junction of the two tubing segments.<br />

But if we’re going to have to obtain tubing for the “unused” diameters to avoid<br />

having to swage joints, we might as well use it for element segments, instead.<br />

Caution The half-element taper schedule of Fig. 12.4A has good wind and ice survival<br />

characteristics only because critical regions of the half-element are double thickness by<br />

virtue of inserting the next smaller diameter inside the larger tube for at least the distances<br />

shown in the figure. If you attempt to scrimp on tubing material and do not overlap tubes at<br />

least as much as shown in the drawing, your Yagi will fail at very low wind speeds! All<br />

telescoping joints and doubled thickness regions must be pinned so as to prevent relative<br />

slippage between any two tubes. Popular techniques for pinning include dimpling “hidden”<br />

reinforcing tubes with a punch, stainless steel sheet metal screws, and pop rivets. Unless<br />

you’re extremely proficient at slitting the ends of tubing and properly applying hose clamps,<br />

using hose clamps on telescoping sections is not recommended by the author.<br />

An important design decision is whether to shunt-feed the driven element. If so, the<br />

element can be continuous metal tubing across its center point as it passes over or under<br />

the boom, but the added complexity of a gamma match or other shunt-feeding system<br />

may be a potential deterrent to the backyard builder.<br />

Instead, this beam employs a split driven element, thus allowing the use of a simple<br />

feed technique, the 4:1 balun. This is not exactly a trivial decision because an 18-ft length<br />

of tubing, whether tapered or not, supported only at one end represents quite a cantilevered<br />

beam. The penalty for choosing this approach is that the boom-to-element bracket for<br />

the driven element must be long enough to allow proper spacing of four U-bolts (two<br />

properly spaced on each side of the driven element) along its length and the U-bolts and<br />

bracket must be strong enough to withstand the moment arm created by the force of the<br />

wind over the entire length of the element half. Also, insulating “tubes” must surround<br />

the element halves where they are grasped by the U-bolts, and the insulation must extend<br />

to just beyond the outer edges of the bracket. Purchase of appropriate boom-to-element<br />

insulating bracket assemblies from the antenna manufacturers or accessory suppliers<br />

listed in App. B may be the best option for the first-time builder of an HF Yagi.<br />

For the director and reflector brackets, flat aluminum plates that are at least ¼-in<br />

thick, 3.5 in wide (the edge dimension that is parallel to the boom length) and 6 to 8 in<br />

long (the edge dimension parallel to the element length) should be fine for normal wind<br />

speeds. Alternatively, obtain aluminum rectangular (bathtub) channel of roughly the same<br />

dimensions for vastly increased strength.<br />

Table 12.2 is used in conjunction with the element taper drawing of Fig. 12.4A to<br />

assemble each element of the 20-m Yagi. The table includes three separate sets of dimensions,<br />

each having a distinct focus:<br />

• The “CW” column emphasizes performance across the 14.000 to 14.100 end of<br />

the 20-m band. In particular, when fed with 50-Ω transmission line, the SWR is<br />

less than 1.5:1 across that 100-kHz range and the F/B ratio exceeds 30 dB over<br />

the bottom 80 kHz or so.<br />

• The “Mid” column is a design that maximizes SWR bandwidth while maintaining<br />

reasonably flat gain across the entire 20-m band. As a result, maximum gain at the

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