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Current through coils
On Wed, 15 Mar 2006 20:08:18 GMT, Cecil Moore wrote:
Richard Clark wrote: Provide the Velocity Factor and Characteristic Impedance per the formulas you offered: Tom Donaly has graciously volunteered to provide those values. Please stand by. You have nothing to show of your own work employing your own references? I can do this myself, as certainly Tom can too; but it says nothing about your well coming up dry when we ask you to carry your own water in supporting your claims. |
Current through coils
Richard Clark wrote:
.. I can do this myself, as certainly Tom can too; but it says nothing about your well coming up dry when we ask you to carry your own water in supporting your claims. Pure humor with zero technical content follows: So sue me for being lazy. :-) -- 73, Cecil http://www.qsl.net/w5dxp |
Current through coils
On Wed, 15 Mar 2006 20:57:21 GMT, Cecil Moore wrote:
So sue me for being lazy. :-) The legacy of Xerox research. |
Current through coils
Richard Clark wrote:
Cecil Moore wrote: So sue me for being lazy. :-) The legacy of Xerox research. Please remind us of the technical content of your posting. Do you think experimental technical results depend upon whom is doing the experiment? If I dropped dead, could Tom's results change from valid to invalid? -- 73, Cecil http://www.qsl.net/w5dxp |
Current through coils
On Wed, 15 Mar 2006 21:29:14 GMT, Cecil Moore wrote:
Do you think experimental technical results depend upon whom is doing the experiment? Clearly you have nothing to offer that conflicts in that respect. If I dropped dead, could Tom's results change from valid to invalid? are you asking would you be technically dead, or clinically dead, or dead lazy? This appears to be a reverse progression question. None of your work appears by your admitted laxity. None of your testing appears by lack of its accomplishment. No pulse can be discerned through the evidence of correspondence (classic result of The Chinese Room Argument). Diagnosis: Xerox induced narcosis. |
Current through coils
Cecil Moore wrote: Richard Clark wrote: Cecil Moore wrote: So sue me for being lazy. :-) The legacy of Xerox research. Please remind us of the technical content of your posting. Do you think experimental technical results depend upon whom is doing the experiment? If I dropped dead, could Tom's results change from valid to invalid? 73, Cecil http://www.qsl.net/w5dxp Probably, since it appears you are the only one finding fault with them. It appears you have painted yourself into a corner by trying o apply a paper about Tesla coils that specifically states it applies only to inductors at self-resonance to inductors operating away from self-resonance. For example, if you look at this time-delay plot: http://www.w8ji.com/inductor_current_time_delay.htm you'll see time delay is essentially flat except near the 16MHz self-resonant frequency and a higher-frequency resonance at 26 MHz. If I coupled that inductor to a oscillator like a Telsa coil has, it would indeed oscillate near the frequency where the inductor has considerable time delay. That time delay is largely because the inductor looks like a combination of shunt C and series L, and is indeed in mode similar to what we find in a transmission line. It is a narrow bandwidth effect because the resonance is high-Q. It does not surprise me at all. 73 Tom |
Current through coils
Richard Clark wrote:
None of your work appears by your admitted laxity. None of your testing appears by lack of its accomplishment. My testing results have been reported. Here are the results of the VF calculation for my 75m bugcatcher coil. The test for physical structure is met. The paper asserts that the expression gives acceptable results with errors less than 10%. The VF of my 75m bugcatcher coil calculates out to be VF = 0.0175 at 6.6 MHz where it measured to be self- resonant. That self-resonant measurement included a length of coax and a one foot bottom section so the actual self-resonant frequency will be somewhat higher than I measured. I could probably make a calculation to adjust for the coax and bottom section. The VF calculated directly from the too-low self- resonant frequency was 0.015 which is 14% different from Dr. Corum's equation. Given the uncertainly in the exact self-resonant frequency in my measurements, that's pretty reasonable. Ballpark is all we need to understand the concepts. Working backward, Dr. Corum's VF would make the coil self-resonant at 7.7 MHz. There's probably enough slop in my measurement configuration to account for the 1.1 MHz difference. -- 73, Cecil http://www.qsl.net/w5dxp |
Current through coils
Cecil, W5DXP wrote:
"How is it possible to use a signal (standing wave current) that is known not to change phase, to measure the phase delay through a wire or coil?" Ignore it. Lissajous figures result from applying signals to the vertical and horizontal deflection circuits of an oscilloscope simultaneously. Phase difference between signals of the same frequency make a distinctive pattern. One can use coax lines with identical delays to couple the inputs with phase sampling loops. Take samples of the currents at the two points where the phase difference would be known. Amplitudes can be adjusted for a suitable pattern. It will be destinctive. Then take samples from the same source. Add a known delay to one channel until you have reproduced the distinctive pattern you had observed when testing the felay between the points that have the unknown phase difference. With a few elaborations, that`s how a phase monitor works. Best regards, Richard Harrison, KB5WZI |
Current through coils
Richard Harrison wrote:
Cecil, W5DXP wrote: "How is it possible to use a signal (standing wave current) that is known not to change phase, to measure the phase delay through a wire or coil?" Ignore it. Lissajous figures result from applying signals to the vertical and horizontal deflection circuits of an oscilloscope simultaneously. Phase difference between signals of the same frequency make a distinctive pattern. One can use coax lines with identical delays to couple the inputs with phase sampling loops. Take samples of the currents at the two points where the phase difference would be known. Amplitudes can be adjusted for a suitable pattern. It will be destinctive. Then take samples from the same source. Add a known delay to one channel until you have reproduced the distinctive pattern you had observed when testing the felay between the points that have the unknown phase difference. With a few elaborations, that`s how a phase monitor works. Many analog scopes aren't capable of producing a meaningful Lissajous figure at HF because of the limited bandwidth of the horizontal channel. Significant phase delays occur at frequencies well below the nominal cutoff frequency, which is often much lower than the vertical channel. Before believing in the validity of any figure, you should look at the figure you get when you apply the signal to both axes at the same time. If it deviates significantly from a single diagonal line, you won't be able to trust other patterns. It would be a simple matter for a digital scope to present a good Lissajous figure, since the bandwidth is determined solely by the input samplers rather than a series of amplifiers and the CRT deflection structure as in an analog scope. I haven't looked closely at digital scopes lately, but I'd be surprised if most don't have the capability of making a good Lissajous figure at HF. It would be simply a matter of internal firmware programming. Of course, a dedicated phase monitor would be designed for good phase and amplitude match between channels at the frequencies it's specified to be used at. Roy Lewallen, W7EL |
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