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Practical_Antenna_Handbook_0071639586

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188 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 />

suspended from the same center support, eliminating any downward pull on the center<br />

of the antenna. Another mechanical advantage of the inverted-vee is that there is no<br />

need for substantial tension in the antenna wires themselves, since they are not being<br />

called upon to support the weight of the feedline or the center insulator. Hence, there is<br />

no reason an inverted-vee can’t be constructed from #18 or smaller gauge wire.<br />

Figure 6.6 shows a typical inverted-vee installation. The operating frequency and<br />

the height of the center support will determine the approximate height above ground of<br />

the ends, but there is no reason the ends can’t come almost to the ground if provision<br />

for preventing people and animals from touching the antenna is included. Angle a can<br />

be almost anything convenient, provided that a > 90 degrees; typically, a is between 90<br />

and 120 degrees. On 80 m, the minimum practical height for the center support is about<br />

35 ft for a = 120 degrees and the overall length of the antenna’s footprint is about 110 ft.<br />

Conversely, if backyard space is at a premium, reducing the included angle to 90 degrees<br />

leads to a minimum center support height of nearly 50 ft, but the footprint is only<br />

slightly more than 90 ft. An inverted-vee for 40 m could have minimum dimensions—<br />

both height and footprint—of approximately 50 percent to 60 percent of these figures.<br />

Sloping the antenna elements down from the horizontal to an angle (as shown in<br />

Fig. 6.6) lowers the resonant frequency for a given length of wire. Thus, the wire lengths<br />

may need to be cut slightly shorter for any given frequency than for a true horizontal<br />

dipole cut for the same frequency. There is no precise equation for calculation of the<br />

overall length of the antenna elements; the concept of “absolute” length holds even less<br />

for the inverted-vee than it does for regular dipoles. There is, however, a rule of thumb<br />

that can be followed for a starting point: Make the antenna about 6 percent shorter than<br />

a dipole for the same frequency. The initial cut of the antenna element lengths (each<br />

quarter-wavelength) is then<br />

<br />

L<br />

Coaxial<br />

cable to<br />

transmitter<br />

L<br />

S<br />

R<br />

I<br />

Insulated<br />

support<br />

L 220<br />

F MHz<br />

Feet<br />

I<br />

R<br />

S<br />

I Insulator<br />

S Support stake<br />

R Rope<br />

Figure 6.6 Inverted-vee dipole.

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