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168 High-frequency dipole and other doublet antennas pass the wire, that are the dimension W apart (19 in for 40 m) Once the spreaders are in place, take about a foot of spare antenna wire and make jumpers to hold the dowels in place The jumper is wrapped around the antenna wire on either side of the dowel, and then soldered The two end supports can be made of 1 2 in wood treated with varnish or urethane spray The wire is passed through screw eyes fastened to the supports A support rope is passed through two holes on either end of the 1 2 and then tied off at an end insulator The TCFTFD antenna is noticeably quieter than the random-length wire antenna, and somewhat quieter than the half-wavelength dipole When the tilt angle is around 30 , the pattern is close to omnidirectional Although a little harder to build than dipoles, it offers some advantages that ought not to be overlooked These dimensions will suffice when the bottom end frequency is the 40-m band, and it will work well on higher bands

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The vee-sloper antenna is shown in Fig 6-22 It is related to the vee beam (covered in Chap 9), but it is built like a sloper (ie, with the feed end of the antenna high above ground) The supporting mast height should be about half (to three-fourths) of the length of either antenna leg The legs are sloped downward to terminating

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Multiband fan dipole 169 resistors at ground level Each wire should be longer than 1 at the lowest operating frequency The terminating resistors should be on the order of 270 (about one-half of the characteristic impedance of the antenna), with a power rating capable of dissipating one-third of the transmitter power Like other terminating resistors, these should be noninductive (carbon composition or metal film) The advantage of this form of antenna over the vee beam is that it is vertically polarized, and the resistors are close to the earth, so they are easily grounded

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A variation on the theme is the vertically polarized rhombic of Fig 6-23 Although sometimes called an inverted vee not to be confused with the dipole variant of the same name this antenna is half a rhombic, with the missing half being mirrored in the ground (similar to a vertical) The angle at the top of the mast ( ) is typically 90 , and 120 to 145 is more common Each leg (A) should be , with the longer lengths being somewhat higher in gain, but harder to install for low frequencies A requirement for this type of antenna is a very good ground connection This is often accomplished by routing an underground wire between the terminating resistor ground and the feedpoint ground

The basic half-wavelength dipole antenna is a very good performer, especially when cost is a factor The dipole yields relatively good performance for practically no in-

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170 High-frequency dipole and other doublet antennas vestment A standard half-wavelength dipole offers a bidirectional figure-8 pattern on its basic band (ie, where the length is a half-wavelength), and a four-lobe cloverleaf pattern at frequencies for which the physical length is 3 /2 Thus, a 40-m halfwavelength dipole produces a bidirectional pattern on 40 m, and a four-lobe cloverleaf pattern on 15 m The dipole is not easily multibanded without resorting to traps (covered in Chap 8) One can, however, tie several dipoles to the same center insulator or balun transformer Figure 6-24 shows three dipoles cut for different bands, operating from a common feedline and balun transformer: A1 A2, B1 B2, and C1 C2 Each of these antennas is a half-wavelength (ie, Lfeet = 468/FMHz) There are two points to keep in mind when building this antenna First, try to keep the ends spread a bit apart, and second, make sure that none of the antennas is cut as a half-wavelength for a band for which another is 3 /2 For example, if you make A1 A2 cut for 40 m, then don t cut any of the other three for 15 m If you do, the feedpoint impedance and the radiation pattern will be affected

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