Practical_Antenna_Handbook_0071639586
504 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 The horizontal section is an open-circuited loop of diameter D, which varies with frequency. The optimum conductor diameter E for the DDRR is at least 0.5 in at 28 MHz, increasing to 4 in at 4 MHz. Thus, for monitoring Jupiter, a diameter of 1 in or slightly less is appropriate. Because of the loop, some people call this the hula hoop antenna. One author recommends using a 2-in automobile exhaust pipe bent into the correct shape by a cooperative automobile muffler mechanic. The far end of the loop is connected to ground through a small-value tuning capacitor C 1 . The actual value of C 1 , which is used to resonate the antenna at a particular operating frequency, is found experimentally. The feedline of the DDRR antenna is coaxial cable; its shield is grounded at the bottom end of the vertical section. The center conductor is connected to the ring radiator a distance F from the vertical section in a circular variant of the autotransformer or gamma match. The length F is determined by the impedance that must be matched. The radiation resistance is approximated by R H = 2620 2 (22.1) l RAD 2 where R RAD = radiation resistance, in ohms H = height of antenna above ground plane l = wavelength H and l must be in the same units. The approximate values for the various dimensions of the DDRR are given as follows in general terms, with examples in Table 22.1: D 0.078l H 0.11D F 0.25H E 0.5 to 4 in G See Table 22.1 Band (MHz) Dimension 1.8 4 7.5 15 22 30 50 150 G (in) 16 7 5 3 2.5 2 1.5 1 C 1 (pF) 150 100 75 35 15 12 10 6 F (in) 12 6 6 1.5 1.5 1 1 0.5 H (in) 48 24 11 6 4.75 3 1.5 1 D (ft) 36 18 9 4.5 3.33 2.33 1.4 6 E (in) 5 4 2 1 0.75 0.75 0.5 0.25 Table 22.1 Examples of Dimensions for DDRR
C h a p t e r 2 2 : R a d i o A s t r o n o m y A n t e n n a s 505 The construction details of the DDRR are so similar to those of the ring radiator that the same diagram can be used (see Fig. 22.3 again). The normal attitude of the DDRR for communications is horizontal. However, for maximum signal when monitoring Jupiter, the entire antenna assembly, including the ground-plane screen, can be tilted to track Jupiter’s position in the sky. Helical Antennas The helical antenna (Fig. 22.5) provides moderately wide bandwidth and circular polarization. Thanks to the latter, some find the helical antenna particularly well suited to radio astronomy reception. The antenna (of diameter D) will have a circumference C of 0.75l to 1.3l. The pitch of the helix (S) is the axial length of a single turn, while the overall length L = NS (where N is the number of turns). The ratio S/C should be 0.22l to 0.28l. At least three turns are needed to produce axial-mode main lobe maxima. The diameter or edge of the ground plane G should be on the order of 0.8l to 1.1l if the conducting surface is circular or square, respectively. The offset between the ground plane and the first turn of the helix is 0.12l. The approximate gain of the helical antenna is found from 2 Gain = 11.8 + 10 log ( C NS) dBi (22.2) The pitch angle f and turn length g for the helical antenna are given by –1 ⎛ πD ⎞ φ = tan ⎜ ⎟ (22.3) ⎝ S ⎠ and 2 2 g = (π D) + S (22.4) Figure 22.5 Helical antenna.
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504 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 />
The horizontal section is an open-circuited loop of diameter D, which varies with frequency.<br />
The optimum conductor diameter E for the DDRR is at least 0.5 in at 28 MHz, increasing<br />
to 4 in at 4 MHz. Thus, for monitoring Jupiter, a diameter of 1 in or slightly less<br />
is appropriate.<br />
Because of the loop, some people call this the hula hoop antenna. One author recommends<br />
using a 2-in automobile exhaust pipe bent into the correct shape by a cooperative<br />
automobile muffler mechanic. The far end of the loop is connected to ground<br />
through a small-value tuning capacitor C 1 . The actual value of C 1 , which is used to resonate<br />
the antenna at a particular operating frequency, is found experimentally.<br />
The feedline of the DDRR antenna is coaxial cable; its shield is grounded at the bottom<br />
end of the vertical section. The center conductor is connected to the ring radiator a<br />
distance F from the vertical section in a circular variant of the autotransformer or gamma<br />
match. The length F is determined by the impedance that must be matched. The radiation<br />
resistance is approximated by<br />
R<br />
H<br />
= 2620 2 (22.1)<br />
l<br />
RAD 2<br />
where R RAD = radiation resistance, in ohms<br />
H = height of antenna above ground plane<br />
l = wavelength<br />
H and l must be in the same units.<br />
The approximate values for the various dimensions of the DDRR are given as follows<br />
in general terms, with examples in Table 22.1:<br />
D 0.078l<br />
H 0.11D<br />
F 0.25H<br />
E 0.5 to 4 in<br />
G See Table 22.1<br />
Band (MHz)<br />
Dimension 1.8 4 7.5 15 22 30 50 150<br />
G (in) 16 7 5 3 2.5 2 1.5 1<br />
C 1 (pF) 150 100 75 35 15 12 10 6<br />
F (in) 12 6 6 1.5 1.5 1 1 0.5<br />
H (in) 48 24 11 6 4.75 3 1.5 1<br />
D (ft) 36 18 9 4.5 3.33 2.33 1.4 6<br />
E (in) 5 4 2 1 0.75 0.75 0.5 0.25<br />
Table 22.1 Examples of Dimensions for DDRR