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![]() "Richard Clark" wrote in message news ![]() On Fri, 05 Nov 2004 10:45:57 -0800, Jim Kelley wrote: I have a question. Can you express the mathematical and/or physical relationship between Rr and antenna gain? It would sure help to clarify the point you were trying to make. Hi Jim, I would have thought someone else could, given the bandwidth of discussion in making the current taper shorter and the constant current section longer. Testing does not bear their facile relationship out however, and for the topic of a short antenna (otherwise, why are we talking about loading coils?) it would seem that antenna gain is immutable over several octaves below a quarterwave length. Of course, I coulda done something wrong. I did use a commonly available design. I did use a commonly available modeler. I even may have done the wrong thing in choosing a design that could be evaluated for free. Perhaps I erred in providing the cogent details of construction. It took all of 20 minutes to accomplish (far less time than that expended in theories of current-in/current-out). These technical hurdles appear to have set the bar too high for my work's refutation in kind. I appreciate that "it's hard work!" ;-) To answer your question, if you just abandon the perfect load, then you stand to achieve a higher gain. If you shorten the antenna, then you stand to achieve a higher gain. There is no change in Rr with the addition of Xl. Hence the mathematical relationship for an antenna shorter than quarterwave would be suggested as: gain ~ 1/Rr gain ~ 1/Xl Rr Z Don't take this gain to the bank however. 73's Richard Clark, KB7QHC Oh... This is about gain? No wonder I'm confused about the subject. |
#2
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John Smith wrote:
"Oh...This is about gain?" Don`t think so. This is about unequal currents into and out of an antenna loading coil. The effect a loading coil has on received signals is due at least in part to its effect on radiation resistance versus total (radiation + loss) resistance. If you increase radiation resistance as comared with loss resistance you increase effective radiated power. Directive gain has nothing to do with loss. Here is Terman`s comment on gain in Note 2 on page 870 of his 1955 edition: "Directive gain depends entirely on the distribution in space of radiated power. The power input to the antenna, the antenna losses, or the power consumed in a terminating resistance have nothing to do with directive gain. Such factors are taken into account in terms of the power gain of the antenna which is defined as the ratio of the power input to the comparison antenna required to develop a particular field strength in the direction of maximum radiation, to the power input that must be delivered to the directional antenna to obtain the same field strength in the same direction. Unless otherwise specified the comparison antenna is a lossless isotropic radiator." Best regards, Richard Harrison, KB5WZI |
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