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On Thu, 11 Nov 2010 16:31:35 +1100, "VK2KC Gmail"
wrote: But what I want to know is how the Arrow manages to match the antenna to the 50 ohm feed. I am thinking its in the spacing of the two elements? Hi OM, Both styles are the same basic method. You are using a length of transmission line (the paired section) to match one Z to another Z. The line Z is part of the equation (the spacing, as you asked). One method (most observed) uses a tapped feed which for the shorted section is located at the line's translation to 50 Ohms, the open end is a higher Z matching to the half-wave radiator (I won't go into the difficulties and considerations of the matching section also radiating). The mystery feed point (do I connect my "hot" lead to the long wire, or the short one?), its magic position, all contribute to a religious lockstep of praise. In itself, it has virtually nothing to offer but complexity. The other method (infrequently observed) simply approaches the situation in the classic application of a line transformer. Think of the smith chart. It's amazing how often this method is used at HF, but draws blank stares when we shift to UHF. I have built, measured, and tested antennas employing the second method because, frankly, it is far simpler to construct on a SO-239 connector: one wire in the center conductor, one wire from any of the four holes - end of story (neglecting the precautionary tales of decoupling everything). The practical side of this home-brew is you build one "close enough," and then with the aid of a SWR meter, you clip off 1/8th inch portions of wire (either side until you get the drift of it) until you have flattened it out the pesky SWR - and then walk away. Anyone versed in using the Smith Chart will immediately recognize that there are many possible satisfactory solutions. As is common with cautioning children not to run with scissors, not all Z-match solutions are preferred radiators. The free version of EZNEC is eminently suited to exploring this. 73's Richard Clark, KB7QHC |
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