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Perhaps the most common form of multiband wire antenna is the trap dipole shown in Fig 8-1A In this type of antenna, one (or more) pairs of parallel resonant traps are placed in series with the quarter-wavelength elements of the dipole The purpose of the traps is to block their own resonant frequency, while passing all other frequencies In the example of Fig 8-1A, a 10-m trap isolates the first 8 ft or so (quarterwavelength on 10 m) so that the antenna resonates on that band A 40-m or 15-m signal, on the other hand, passes through the traps and uses the whole length of the antenna (Note: A half-wavelength 40-m dipole works as a 3/2-wavelength antenna on 15 m) The overall length of the trap dipole will be a little less than the natural nontrap length for the lowest frequency of operation At the low frequencies, the traps add a little inductance to the circuit so that the resonant point is lower than the natural resonant frequency In general, most trap dipoles are just a few percent shorter than nontrap dipoles at the same band The actual amount of shortening depends upon the values of the components in the traps, so consult the data for each trap purchased Where more than one pair of traps is used in the antenna, make sure they are of the same brand and are intended to work together Another solution to this problem is shown in Fig 8-1B This type of antenna actually has two or more half-wavelength dipoles fed from the same transmission line In this illustration, a total of three dipoles are fed from the same 75- transmission line There is no theoretical limit to how many dipoles can be accommodated, although there is certainly a practical limit For one thing, there is a mechanical limit to how many wires are supportable (or desirable) hanging from any given support There is also an electrical limit, although it is less defined Having a lot of dipoles increases the possibility of radiating harmonics and other spurious emissions from your transmitter The 75- coaxial cable is connected to the center feedpoint of the multidipole either directly or through a 1:1 balun transformer, as shown in Fig 8-1B Each an-.

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tenna (A-A, B-B, or C-C) is a half-wavelength Therefore, the overall length is found approximately from the standard dipole expressions: Overall length (A + A, B + B, or C + C): Lft = or, for each element alone (A, B, or C): Lft = 234 FMHz [82] 468 FMHz [81]

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As always, close to the earth s surface, these equations are approximations, and are not to be taken too literally Some experimentation will probably be necessary to optimize resonance on each band Also, be aware that the drooping dipoles (B and C in this case) may act more like an inverted-vee antenna (see Chap 7) than a straight dipole, so the equation length will be just a few percent too short In any event, a little spritzing with this antenna will yield results Some amateurs build the multiple dipole from four- or five-wire TV rotator lead That type of wire is used to control antenna rotators, and has either four or five parallel wires in a flat arrangement similar to lamp cord Cut each wire to the length required for a band, and strip off any unused portions Another possibility is the link-tuned dipole shown in Fig 8-1C In this situation, a single conductor is used for each half of the dipole, or actually inverted vee The conductors are broken into segments A, B, and C (or more, if desired) Each segment is separated from the two adjacent sections by inline insulators (standard end insulators are suitable) Segment A is a quarter-wavelength on the highest frequency band of operation, A + B is a quarter-wavelength on the next highest band of operation, and A + B + C is a quarter-wavelength on the lowest frequency band of operation The antenna is tuned to a specific band by either connecting, or disconnecting, a similar wire (see inset) jumper across the insulator that breaks the connection between the segments Either a switch or an alligator clip jumper will short out the insulator to effectively lengthen the antenna for a lower band Some amateurs use single-pole 110-Vac power line switches to jumper the insulator Although I have not tried this method, it should work.

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