Practical_Antenna_Handbook_0071639586

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260 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 Figure 10.8 Gain versus length of vee beam and rhombic beam antennas. The gain of a vee beam is about 3 dB higher than the gain of the single-wire longwire antenna of the same wire length, and it is considerably higher than the gain of a dipole (see Fig. 10.8). At three wavelengths, for example, the gain is 7 dB over a dipole. In addition, there may be some extra gain because of mutual impedance effects—which can be about 1 dB at 5l and 2 dB at 8l. Nonresonant Vee Beams Like single-wire longwire antennas, the vee beam can be made nonresonant by terminating each wire in a resistance that is equal to the antenna’s characteristic impedance (Fig. 10.9). Although the regular vee is a standing wave antenna, the terminated version is a traveling wave antenna and is thus unidirectional. Traveling wave antennas achieve unidirectionality because the terminating resistor absorbs the incident wave after it has propagated to the end of the wire. In a standing wave antenna, any energy reaching the far end is reflected back toward the source, so it can radiate oppositely from the incident wave. Rhombics The rhombic antenna, also called the double vee, consists of two vee beams positioned to face each other with their corresponding tips connected. The unidirectional, nonresonant (terminated) rhombic shown in Fig. 10.10 develops approximately the same gain and directivity as a vee beam of the same size. The nonresonant rhombic has a gain of about 3 dB over a vee beam of the same size (see Fig. 10.8 again).

C h a p t e r 1 0 : W i r e A r r a y s 261 R } Resultant pattern R Figure 10.9 Nonresonant vee beam antenna. The layout of the rhombic antenna is characterized by two angles. One-half of the included angle of the two legs of one wire is the tilt angle (f), while the angle between the two wires is the apex angle (q). But the two are not independent; from Fig. 10.10 it should be obvious that q/2 = 90 - f. A common rhombic design uses a tilt angle of 70 degrees, a length of 6l for each leg (two legs per side), and a height above the ground of 1.1l. q for this antenna must necessarily be 40 degrees. The termination resistance for the nonresonant rhombic is 600 to 800 Ω, and it must be noninductive across the entire range of operating frequencies. For transmitting rhombics, the resistor should be capable of dissipating at least one-third of the average power of the transmitter. For receive-only rhombics, the termination resistor can be a 2W carbon composition or metal-film type. Such an antenna works nicely over an octave (2:1) frequency range.

C h a p t e r 1 0 : W i r e A r r a y s 261<br />

R<br />

}<br />

Resultant pattern<br />

R<br />

Figure 10.9 Nonresonant vee beam antenna.<br />

The layout of the rhombic antenna is characterized by two angles. One-half of the<br />

included angle of the two legs of one wire is the tilt angle (f), while the angle between<br />

the two wires is the apex angle (q). But the two are not independent; from Fig. 10.10 it<br />

should be obvious that q/2 = 90 - f. A common rhombic design uses a tilt angle of 70<br />

degrees, a length of 6l for each leg (two legs per side), and a height above the ground<br />

of 1.1l. q for this antenna must necessarily be 40 degrees.<br />

The termination resistance for the nonresonant rhombic is 600 to 800 Ω, and it must<br />

be noninductive across the entire range of operating frequencies. For transmitting<br />

rhombics, the resistor should be capable of dissipating at least one-third of the average<br />

power of the transmitter. For receive-only rhombics, the termination resistor can be a<br />

2W carbon composition or metal-film type. Such an antenna works nicely over an octave<br />

(2:1) frequency range.

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