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Cecil Moore wrote in message ...
Yes, that's true. Now try it with a thin wire on HF. I believe what you will find is that at the maximum reactance point, the resistance is approximately half of the one-wavelength (anti)resonant value. At the maximum reactance point, the resistance and reactance are approximately equal. Since the maximum reactance value lies between two points of pure resistance, doesn't it make sense that it might be approximately where the resistance is half of the maximum value of resistance? That's pretty approximate, Cecil. From EZNec for a 10 meter 1mm diam wire, I got about 2570+j2277 at 27.00MHz. The resistive and reactive parts differ by over ten percent. Be that as it may, if you evaluate the SWR tangency thing for a high reference impedance, you will see that it's a GROSS error, not a tiny one. You said it wouldn't change with changes in reference impedance, but it does, and in a major way. Yes, the error is tiny for your assumed 2500+j2500 evaluated against Z0 of 50 ohms, but the error is huge if you evaluate against Z0 of, say, 2000 ohms. And we're still back to not having said anything about _why_ the reactance peaks at the frequency it does relative to the half- and full-wave resonances. Cheers, Tom |
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