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#51
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Yuri Blanarovich wrote:
What I was looking for is to see 1. if anyone else MEASURED the current in loading coils, and what results they arrived at (and if we are wrong, then where did we go wrong). 2. If this is right than to have modeling software implement it with least error. I would like to use that for optimizing, say, loaded elements for receiving arrays on low bands, optimizing mobile antennas, loaded multielement beams, etc. Hi Yuri, try this out for your argument in the other group. Using EZNEC: Example 1: 102' CF dipole with loading coils in the center of each arm to cause the antenna to resonate on 3.76 MHz. I get XL=j335 ohms. Example 2: Replace the above loading coils with series inductive stubs hanging down. Ten foot stubs with six inch spacing between the wires is what I used. What happens to the current across that six inch gap is obvious from the current plot using EZNEC. Hint: There is a step function across that six inch gap just as there will be with a six inch coil. Then ask: Why doesn't EZNEC treat these two cases the same way? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#52
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Yuri Blanarovich wrote:
There is too much reliance now going on modeling program results, ignoring some realities. Yuri, here is a modeling result that you might like. :-) I took a 102' dipole and loaded it in the center of each leg with an inductive stub that made the dipole resonant on 3.76 MHz. I added a one ohm series 'load' to each side of the stub. Drawing one leg of the dipole, it looks like this: ----------R2-+ +-R1----------FP--- ... other half | | | | inductive | | stub +-+ EZNEC reports 0.85 amps through R1 and 0.57 amps through R2, a difference of 33%. If one could model the inductive loading reactance as an actual physical coil instead of a lumped single point impedance, results would be similar to the above. Now here is something that might blow some minds. The inductive stub above is ten feet long. That's about 1/8WL on 20m. A 1/8WL shorted stub equals +jZ0. The results of running the above antenna on 20m is that the current through R1 is 185 degrees out of phase with the current through R2. At the time when the current through R2 is flowing toward the end of the antenna, the current through R1 is flowing toward the feedpoint. Wonder what Kirchhoff would say about that. If you replace the stub with a coil of the same reactance, not much changes. Tell W8JI to stop using lumped circuit analysis when he should be using distributed circuit analysis. :-) -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#53
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Thank you Cecil and Fred!
(Where is Roy? We could use expert guidance in modeling the case.) I will post your comments on eHam.net. The analogy using stubs is excellent. That brings the question of using nice coils, vs. stubs, vs. toroids in shortened antennas. But we will save that for another thread with proper name. Now watch for W8JI twisting into: "I said that all along" see him changing his web page and become a guru who "discovered" that current accross the loading coil in the antenna is significantly different and Yuri (et al) will remain the idiot who can't get the things right :-).... Happened many times before :-( Thanks again! Yuri, K3BU/m As Ken, K7GCO keeps saying: "Don't they get tired of being wrong?" |
#54
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Yuri Blanarovich wrote:
Thank you Cecil and Fred! (Where is Roy? We could use expert guidance in modeling the case.) I sent Roy a copy of the EZNEC file that I sent to you. Anyone else who wants a copy of those files, send me an email. I will post your comments on eHam.net. Which forum/topic? -- 73, Cecil, W5DXP |
#55
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Cecil wrote,
Tell W8JI to stop using lumped circuit analysis when he should be using distributed circuit analysis. :-) -- 73, Cecil http://www.qsl.net/w5dxp You know, it's against the law to kill people, Cecil. I almost choked to death on my morning cup of Bo Lee when I read that. :-) 73, Tom Donaly, KA6RUH |
#56
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#57
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Tdonaly wrote:
Cecil wrote, Tell W8JI to stop using lumped circuit analysis when he should be using distributed circuit analysis. :-) You know, it's against the law to kill people, Cecil. I almost choked to death on my morning cup of Bo Lee when I read that. :-) I apologize for that, Tom. If you had choked to death, would there have been enough evidence to convict me? :-) -- 73, Cecil, W5DXP |
#58
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Cecil wrote,
I apologize for that, Tom. If you had choked to death, would there have been enough evidence to convict me? :-) -- 73, Cecil, W5DXP Not in California, Cecil. It would have been the perfect crime. 73, Tom Donaly, KA6RUH |
#59
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![]() "Mark Keith" wrote I beat Reg's vertload program to death finding the best overall coil height for my mobile antenna. Basically I ended up putting it as high as I could. Which ended up a center load at 5 ft up, with a 10 ft whip. =============================== There are 3 losses - coil loss resistance, ground loss resistance and radiation resistance. To calculate and maximise efficiency all 3 values must be transformed to a common point - the base feedpoint. The length of radiator between coil and base behaves is a transmission line transformer which transforms the coil loss resistance (XL/Q) to another value at the base. Would-be modellers should take this into account. The Cosine current distribution along the radiator is a direct consequence of its behaviour as a lossy line. (Actually, it is not an exact cosine shape because of end-effect) Efficiency = Rrad / ( Rrad+Rcoil+Rground ). Rground is constant. For short antennas Rrad is the smallest of the 3 resistances. As the coil is moved further up the antenna both Rrad and Rcoil increase. But even if the coil is located at the extreme top of the antenna, radiation resistance cannot increase to more than 4 times the radiation resistance when the coil is located at the base feedpoint. Usually it is considerably less than 4. So the rapidly increasing coil loss resistance very soon overtakes the increase in radiation resistance. Even if coil Q remains constant, coil loss resistance increases just by virtue of its necessary increase in inductive reactance. To maintain resonance coil inductance increases inversely proportional to the length of the whip above it. So when the coil is located 95% of the way to the top of the antenna its loss resistance is TWENTY times greater than that of a base loading coil even when Q is unchanged. In practice, a coil having 20 times the inductance but with the same overall dimensions will very likely have a lower Q and an even higher resistance. Its easy to see the fixed value of Rground in the above efficiency formula has the following effects - When coil loss is less than ground loss, higher radiating efficiency is achieved by placing the coil nearer to the top of the antenna. And vice-versa. When ground loss is very small (zero if antenna is a pair of two back-to-back radiators to form a dipole) efficiency is relatively high anyway, maximumum efficiency perhaps occurring with the coil located in the lower half of the antenna. The slight improvement relative to base loading (as part of a tuner) may not then be worth the mechanical inconvience of fitting a coil in the antenna anyway. An important factor, not considered quantitatively by anybody, is that a mobile antenna is not just a loaded vertical - the vehicle body, just by looking at it, obviously forms the major portion of the antenna and is floating above ground. The vehicle body plus loaded whip should be considered to be an off-centre-fed, short, 1/2-wave resonant vertical dipole and modelled as such. --------------------------------------------------------- Regarding antenna modelling - program LOADCOIL considers all 3 parts parts of the antenna, the mast, loading coil and whip, as consecutive lengths of transmission line each with its own Zo and loss resistance. It is obliged to do this because it covers actual antenna heights approaching 1/4-wavelength as may be erected in your backyard. And it continues to do this for very short antennas with very short loading coils even where there would be negligible error by assuming the current going into one end of the coil is the as what comes out of the other. There's a companion program TOPHAT2. There's no coil in it. ---- ======================= Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.g4fgq.com ======================= |
#60
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NM5K snip, snip and...
Besides, I've never really worried about it much. I don't think it would have any effect on how I build my short verticals. Good for you :-) Granted, we are close to optimum with mobile verticals. If I understand how and why things work, I can do better job on optimizing and maximizing the performance of the antennas, especially when it comes to more element loaded arrays. You would see significant difference in designing/optimizing say 3 element loaded beam. Modeling software uses currents in elements and calculates mutual interaction between the elements. If the current distribution and magnitude are off by 50% then we have major problem. Yuri |
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