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402 p a r t V I : a n t e n n a s f o r O t h e r F r e q u e n c i e s<br />

greatly increases absorption of these near-vertical signals in the lower layers of<br />

the ionosphere, making daytime short-haul communication problematic. Further,<br />

during periods of very low sunspot activity, the critical frequency, f C , can in<br />

fact drop below 1.8 MHz, with the result that nighttime skip entirely disappears<br />

on the topband. An efficient vertically polarized antenna can cover the same<br />

region with a strong ground wave that is present 24/7 and is not dependent<br />

upon conditions in the ionosphere.<br />

What, then, is a “decent” vertical installation? Surprising to many who are wrestling<br />

with antenna space requirements for the first time, vertical antennas require nearly<br />

as much backyard space (or footprint) as l/2 dipoles! Although a 40-m vertical (33 ft<br />

high) is not an unreasonable mechanical assembly and has modest guying requirements,<br />

a full-size quarter-wave vertical for 160 stands 125 to 140 ft tall, and will likely<br />

require a guy wire footprint having a diameter of 200 ft or greater. In addition, local<br />

building codes may not require any special inspections or permits for the 33-ft antenna<br />

but may impose rigid and very exacting requirements on the higher structure. Worse<br />

yet, an antenna with overall height substantially taller than the maximum allowed for<br />

a principal structure (often 35 or 40 ft in the United States) may not be allowed at all by<br />

the local zoning ordinance! On suburban or urban lots, a typical 40-m vertical might<br />

well be able to fall over without crossing the property line or landing on power lines.<br />

Not so the 160-m vertical!<br />

Thus, the biggest problem for most topband DXers, as you can see, is the size of<br />

antennas for those frequencies; but there are ways to shorten an antenna—not without<br />

penalty, mind you, because the TANSTAAFL* principle still applies—to the point<br />

where an antenna for 160 becomes feasible with limited yard space. In return, the user<br />

typically gives up a few decibels of distant signal strength for a given power delivered<br />

to the antenna and suffers a narrower VSWR bandwidth before retuning of the antenna<br />

is necessary.<br />

As discussed in Chap. 16, to get the most (radiated field) from an antenna we must<br />

maximize the area under its current-versus-length curve while simultaneously minimizing<br />

the portion of the RF energy from the transmitter that is wasted in feedline losses<br />

and ground system losses. In general, this means that our preferred antennas are those<br />

that give maximum exposure to the natural high-current portions of the antenna<br />

element(s), exhibit a high radiation resistance relative to other losses in the system, and<br />

are a reasonably close match to available feedlines. Further, if the antenna is a monopole<br />

(such as a ground-mounted or ground-plane vertical) being operated against ground, we<br />

must not neglect the design of the RF ground system in the immediate vicinity of the<br />

antenna.<br />

l/4 Vertical Monopole<br />

By far the conceptually simplest way to give maximize exposure to the high-current<br />

portion of the antenna is to make sure that horizontal dipoles are l\2 or slightly longer<br />

and verticals are l/4 or slightly longer. Since the title of this book includes the word<br />

“practical”, we will concentrate on the l/4 ground-mounted vertical instead of l/2<br />

dipoles erected at heights of 300 ft or more!<br />

*TANSTAAFL = There ain’t no such thing as a free lunch!

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