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Richard Clark wrote in message . ..
On 20 Apr 2004 09:06:35 -0700, (N2EY) wrote: These apologies ring false. The issue of gaps is desperate and the selection of tubular has no basis in special characteristics. All such considerations MUST yield to simple scaling. For instance, if you need 0.8 and have 0.9, there is no magic formula beyond proportions necessary to achieve "what should be." I disagree! In the QST article, Lattin describes an 80/40 dipole using his method. It has wires dangling from the stub junctions to get 40 meter resonance. Hi Jim, OK, you disagree, but with what? With the idea that scaling answers all questions. Scaling will ALWAYS answer everything but the mystical apologies. The two-band 80/40 dipole in the QST article has extra wires at the junctions of the 80 and 40 sections because (according to the author) the velocity factor of the tubular Twin Lead makes it necessary. Those wires might or might not be required with a unity velocity factor. Most important to me is that the antenna offers no real advantages over, say, a conventional trap dipole. Yet it offers many disadvantages, such as mechanical frailty and difficulty of duplication. This is more pilot error than design error (which has its own problems, of course). In a perfect world, maybe. But in the real world of ham radio, most hams have limited materials, test equipment, time and space. An antenna made out of unobtainable materials, which requires unobtainable tools and test equipment to build and adjust is only of academic interest to a ham. And again - what advantages does it have over, say, a W3DZZ trap dipole? I see no such issues if the theory were hammered out. It is plainly these readings of tea leaves that frustrate construction, because when a design is described, it is most clear and concise - it just doesn't work is all. Exactly! If it cannot be easily duplicated by a ham with typical resources, what good is it? Like I said, I've done some measures and added a dozen more since. The results are interesting. I can come up with a four band antenna without too much trouble; however, getting those bands into Ham regions (all of them) is another matter. I can do this with a simple run of twin lead, and one strategically placed short between them. Which is not what Lattin did at all. Your design sounds far superior. Is it on the web anywhere? This antenna (usefully resonant or otherwise) is no worse than any wire strung between poles - just two wires instead of one, hardly what I would call fragile. If it has an advantage over your W3DZZ trap dipole, I leave that strictly in the eye of the beholder as I have full faith it won't be any worse. All depends on the wires. I use recycled #12 house wire, which stands up under ice loading and high winds here in EPA. Yet it is hardly noticed by the neighbors. Any way, such work offers a step towards an antenna with MORE gain (and more wire, a third one) by constructing a Franklin Array style of antenna. True, not a multi bander, but I am not particularly nailed to the floor over that. The main attraction of the Lattin is its claim to multiband operation. Otherwise one might as well go with a plain dipole. 73 de Jim, N2EY |
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Scaling is a powerful analytical technique(*), but in some cases it can
be a little trickier than meets the eye. Consider, for example, scaling a piece of TV twinlead to twice the frequency so it'll behave exactly the same (both as a transmission line and as a radiator) at the new frequency. The wire diameters have to be reduced by a factor of two. The spacing between the wires has to be reduced by a factor of two. Luckily, if the scale model and the original are both in free space, then The dielectric constant of the insulator remains unchanged. And, almost always overlooked, The wire conductivity has to be increased by a factor of two. The dielectric conductivity has to be increased by a factor of two. Fortunately, these last factors are usually unimportant. If the original is made from copper, it isn't possible to scale to a much higher frequency. But it's something to be kept in mind if loss is significant and an accurate assessment of loss is necessary. Permeability, incidentally, remains unchanged with frequency when scaling. But even if you can neglect the conductivity scaling, you wouldn't be able to run down to the store and buy a piece of the scaled twinlead to use in your antenna for another band. (*) Antennas are often scaled to higher frequencies for testing because the scale model is a more convenient size. When I was involved in the development of very high-speed sampling circuits, we often made scale models of various structures (for example, coax connector to microstrip transitions) at *lower* frequencies, so they'd be large enough to measure and physically adjust. Roy Lewallen, W7EL |
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#7
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Hi, all concerned:
Here's some anecdata (sic) ... : OUAT, after reading something some where about the Lattin Labs antenna, I put an 8-ft stub on the side of a 33-ft verticaloverlotsaradials. I got a "new" indication of low-Z near 10M which wasn't there B4, to go along with the 40M low-Z reading. Received noise on 10M went up, from a well-defined nearby source, suggesting that the el pattern might have come down some. I moved the stub nearer the top, and found what I remember as a 3/4-wave low-Z indication on 10M. I think the KT-XX series of "diametrically opposed designs" use this method of multibanding, as well. Might even try this anecdata in Roy's Toy3, to see if its gui-ed algorithm-ized academic mumblings prove this scandalous anecdata. Shucks, if it can't be modeled, it can't be made to happen ;o) Right? 73, Dave, N3HE "Richard Clark" wrote in message ... On 22 Apr 2004 07:19:37 -0700, (N2EY) wrote: Like I said, I've done some measures and added a dozen more since. The results are interesting. I can come up with a four band antenna without too much trouble; however, getting those bands into Ham regions (all of them) is another matter. I can do this with a simple run of twin lead, and one strategically placed short between them. Which is not what Lattin did at all. Your design sounds far superior. Is it on the web anywhere? Hi Jim, You should take care with my perverse generalizations, especially when you follow it with: BIGSNIP Frankly, the Lattin has yet to prove to me that the notion of a longitudinal stub as "trap" really holds any water. I've seen the same "theory" applied to diametrically opposed designs. It is pleasing to the arm-chair designer to mutter these ideas, but these so-called streamers needed to make it work just yell foul on every street corner. It is an ad-hoc design draped with academic mumblings to lend it the appearance of legitimacy. To extend my quote above, I have added yet another dozen measurements to have nailed down patterns that emerged with the basis of a consistent building paradigm (yeah, I know, gobbldygook). I seek to generalize such claims as the Lattin makes and reduce them to a practical minimum that are robust and repeatable. This is not to say entirely useful, nor optimal. I did the same thing with the fractal with 300 or more measurements and reduced that junk science to a simple observation: you can push more resonances into a length of wire, the more you kink it. Useful? The test of time has shown that no one has made any money from those same published 300 pages - why would I expect the Lattin to emerge from 5 decades of neglect to eclipse that record? Frankly, the Lattin simply confirms this simple observation, but is more controlled. It may mature to a more repeatable design, but I doubt its inventor would recognize it. 73's Richard Clark, KB7QHC |
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#8
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On Fri, 23 Apr 2004 06:19:29 -0400, "David J Windisch"
wrote: Shucks, if it can't be modeled, it can't be made to happen ;o) Right? Hi Dave, More the issue is if it can be made to happen, and it can't be modeled - what happened? [After that we can then stare at our navels and ask "what is IT?"] 73's Richard Clark, KB7QHC |
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