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8 Direction of main lobe (S1 closed) Direction of main lobe (S1 open) 14-1 Half-wave square loop antenna with reversal switch

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Neither /2 loop configuration shows gain over a dipole The figure usually quoted is 1-dB forward gain (ie, a loss compared with a dipole), and about 6-dB front-to-back ratio (FBR) Such low values of FBR indicate that there is no deep notch ( null ) in the pattern A lossy antenna with a low FBR seems like a born loser, and in most cases it is But the /2 loop finds a niche where size must be constrained, for one reason or another In those cases, the /2 loop can be an alternative These antennas can be considered limited-space designs, and can be mounted in an attic, or other limitedaccess place, as appropriate A simple trick will change the gain, as well as the direction of radiation, of the closed version of the /2 loop In Fig 14-2, a pair of inductors (L1 and L2) are inserted into the circuit at the midpoints of the sides adjacent to the side containing the feedpoints These inductors should have an inductive reactance XL of about 360 in the center of the band of operation The inductance of the coil is

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[141]

where L H is the coil inductance, in microhenrys ( H) FHz is the midband frequency, in hertz (Hz) Example Find the inductance for the coils in a loaded half-wavelength closedloop antenna that must operate in a band centered on 10125 MHz Solution: [Note: 10125 MHz 10,125,000 Hz] L H 36 108 2 (10,125,000 Hz) 57 H

The coils force the current antinodes toward the feedpoint, reversing the direction of the main lobe, and creating a gain of about 1 dB over a half-wavelength dipole The currents flowing in the antenna can be quite high, so when making the coils, be sure to use a size that is sufficient for the power and current levels anticipated The 2- to 3-in B&W Air-Dux style coils are sufficient for most amateur radio use Smaller coils are available on the market, but their use is limited to low-power situations

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L2 XL = 370 14-2 Use of inductive loading to reduce the size of antenna, and make the pattern more uniform

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If size is not forcing you to a /2 loop, then a 1 loop might be just the ticket It produces a gain of about 2 dB over a dipole in the directions that are perpendicular to the plane of the loop The azimuth patterns formed by these antennas are similar to the figure-8 pattern of the dipole Three versions are shown: the square loop (Fig 14-3), the diamond loop (Fig 14-4), and the delta loop (aka D-loop and triangle Fig 14-5) The square and diamond loops are built with /4 on each side, and the delta loop is /3 on each side The overall length of wire needed to build these antennas is Lfeet 1005 FMHz [142]

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The polarization of the three loop antennas is horizontal, because of the location of the feedpoints On the square loop, moving the feedpoint to the middle of either vertical side will provide vertical polarization Similarly, on the diamond loop vertical polarization is realized by moving the feedpoint to either of the two adjacent apexes On the delta loop, placing the feedpoint at either of the two other apexes produces a diagonal polarization that offers approximately equal vertical and horizontal polarization components

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X1 X2 4 14-3 Quarter-wavelength square loop (single-element quad)

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