Practical_Antenna_Handbook_0071639586
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.
- Page 227 and 228: C h a p t e r 7 : L a r g e W i r e
- Page 229 and 230: C h a p t e r 7 : L a r g e W i r e
- Page 231 and 232: C h a p t e r 7 : L a r g e W i r e
- Page 233 and 234: C h a p t e r 7 : L a r g e W i r e
- Page 235 and 236: CHAPTER 8 Multiband and Tunable Wir
- Page 237 and 238: C h a p t e r 8 : M u l t i b a n d
- Page 239 and 240: C h a p t e r 8 : M u l t i b a n d
- Page 241 and 242: C h a p t e r 8 : M u l t i b a n d
- Page 243 and 244: C h a p t e r 8 : M u l t i b a n d
- Page 245 and 246: C h a p t e r 8 : M u l t i b a n d
- Page 247 and 248: CHAPTER 9 Vertically Polarized Ante
- Page 249 and 250: C h a p t e r 9 : V e r t i c a l l
- Page 251 and 252: C h a p t e r 9 : V e r t i c a l l
- Page 253 and 254: Quarter-wave vertical radiator Insu
- Page 255 and 256: C h a p t e r 9 : V e r t i c a l l
- Page 257 and 258: C h a p t e r 9 : V e r t i c a l l
- Page 259 and 260: C h a p t e r 9 : V e r t i c a l l
- Page 261 and 262: C h a p t e r 9 : V e r t i c a l l
- Page 263 and 264: C h a p t e r 9 : V e r t i c a l l
- Page 265 and 266: C h a p t e r 9 : V e r t i c a l l
- Page 267 and 268: C h a p t e r 9 : V e r t i c a l l
- Page 269 and 270: Directional High-Frequency Antenna
- Page 271 and 272: CHAPTER 10 Wire Arrays When a singl
- Page 273 and 274: C h a p t e r 1 0 : W i r e A r r a
- Page 275 and 276: C h a p t e r 1 0 : W i r e A r r a
- Page 277: Wire 2 C h a p t e r 1 0 : W i r e
- Page 281 and 282: C h a p t e r 1 0 : W i r e A r r a
- Page 283 and 284: CHAPTER 11 Vertical Arrays Despite
- Page 285 and 286: C h a p t e r 1 1 : V e r t i c a l
- Page 287 and 288: C h a p t e r 1 1 : V e r t i c a l
- Page 289 and 290: C h a p t e r 1 1 : V e r t i c a l
- Page 291 and 292: C h a p t e r 1 1 : V e r t i c a l
- Page 293 and 294: C h a p t e r 1 1 : V e r t i c a l
- Page 295 and 296: CHAPTER 12 The Yagi-Uda Beam Antenn
- Page 297 and 298: C h a p t e r 1 2 : T h e Y a g i -
- Page 299 and 300: C h a p t e r 1 2 : T h e Y a g i -
- Page 301 and 302: C h a p t e r 1 2 : T h e Y a g i -
- Page 303 and 304: C h a p t e r 1 2 : T h e Y a g i -
- Page 305 and 306: C h a p t e r 1 2 : T h e Y a g i -
- Page 307 and 308: C h a p t e r 1 2 : T h e Y a g i -
- Page 309 and 310: C h a p t e r 1 2 : T h e Y a g i -
- Page 311 and 312: C h a p t e r 1 2 : T h e Y a g i -
- Page 313 and 314: C h a p t e r 1 2 : T h e Y a g i -
- Page 315 and 316: C h a p t e r 1 2 : T h e Y a g i -
- Page 317 and 318: C h a p t e r 1 2 : T h e Y a g i -
- Page 319 and 320: C h a p t e r 1 2 : T h e Y a g i -
- Page 321 and 322: C h a p t e r 1 2 : T h e Y a g i -
- Page 323 and 324: C h a p t e r 1 2 : T h e Y a g i -
- Page 325 and 326: C h a p t e r 1 2 : T h e Y a g i -
- Page 327 and 328: C h a p t e r 1 2 : T h e Y a g i -
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.