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wrote :
That is incorrect for the conditions we are outlining, and it is misleading Cecil. It has him lost in a world of reflections. What is causing the misleading part is: THE LUMPED-CIRCUIT MODEL FAILS IN THE PRESENCE OF STANDING WAVES! There is no virtually no difference in phase delay in current at each end of a relatively compact inductor. Is a 75m bugcatcher coil a "relatively compact indictor"? If you say yes, you are stuck with its measured delay. If you say no, then we are not discussing the typical amateur radio mobile loading coil. Of course, one turn on a toroid is going to exhibit the characteristics you are presenting. But that is not a typical bugcatcher coil either. The Tesla coil, by definition of how it works, violates all boundaries of the examples myself and others are giving Cecil. It does not apply to the discussion at all. False: A 75m bugcatcher coil used as a 1/4WL resonator on 9-10 MHz meets the minimum requirements for a Tesla coil. It uses 1/6 wavelength of wire on 75m. I'll bet it would certainly arc at a kilowatt. The typical minimum Tesla system is a coil with a top hat sphere. It looks a lot like your 160m mobile antenna. :-) It is not operated at a fraction of self-resonance as people SHOULD know a good mobile loading coil is. A 75m bugcatcher coil is operating close enough to its self-resonant frequency that the self-resonant effects are certainly present. A 75m bugcatcher coil can be considered to be a lumped circuit impedance at 60 Hz but certainly not at 4000000 Hz. In fact, that is the whole question. At what frequency can the lumped circuit model be validly used on a 75m bugcatcher coil? I'm willing to bet that frequency is lower than 1000000 Hz. It has no bearing at all on the discussion, ... Wishful thinking on your part. .. In fact, a Tesla coil has more in common with a cavity resonator than it does with a conventional inductor." A 75m bugcatcher coil has more in common with a cavity resonator than it does with your lumped circuit inductance. "at its operating frequency, a Tesla coil is NOT a lumped-element induction coil". Neither is a 75m bugcatcher coil. Everyone in the conversation has been very careful to clearly establish the boundary conditions that the behavior we are talking about is significantly below self-resonance, an inductor of compact form factor, and an inductor of good design. A 75m bugcatcher coil used on 4 MHz is NOT significantly below the self-resonant frequency of 9-10 MHz. THE LUMPED-CIRCUIT MODEL FAILS IN A STANDING WAVE ENVIRONMENT! In the face of that simple technical fact, all other discussion is moot. Anyone wishing to validly model a 75m bugcatcher coil used on a mobile antenna is forced to choose a model that does not presuppose faster than light wave travel through a 75m bugcatcher coil. It's as simple as that. Tom, with a straight face, I want you to assert that the RF waves on a 75m bugcatcher mobile antenna are traveling faster than the speed of light. If it takes 125 nanoseconds for the forward current wave to make it from the end of the antenna and back to the feedpoint, then the lumped-circuit model yields invalid results. TDR anyone? -- 73, Cecil, W5DXP |
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#2
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Cecil Moore wrote: A 75m bugcatcher coil used on 4 MHz is NOT significantly below the self-resonant frequency of 9-10 MHz. Yes it is, but no so far as to have perfectly equal currents at each end an zero phase shift in current. It is in the neither land between a Tesla coil (which is still nothing like my mobile antenna, but at least getting closer) and a idealized lumped component. THE LUMPED-CIRCUIT MODEL FAILS IN A STANDING WAVE ENVIRONMENT! In the face of that simple technical fact, all other discussion is moot. Anyone wishing to validly model a 75m bugcatcher coil used on a mobile antenna is forced to choose a model that does not presuppose faster than light wave travel through a 75m bugcatcher coil. It's as simple as that. Nonsense. You are ignoring the coupling mechanisim inside the inductor. Tom, with a straight face, I want you to assert that the RF waves on a 75m bugcatcher mobile antenna are traveling faster than the speed of light. If it takes 125 nanoseconds for the forward current wave to make it from the end of the antenna and back to the feedpoint, then the lumped-circuit model yields invalid results. TDR anyone? They are not travelling faster than light. What you (and the one or two others who seem to agree with you) repeatedly ignore or forget is magnetic flux couples one turn to another. A real inductor is always someplace between the two extremes of something like a radial mode helice (helically loaded whip) and an ideal lumped component. Since you have taken the path of totally forgetting or ignoring flux coupling, you are reaching incorrect conclusions. Using the Tesla coil model is a good example. Everyone is freely admitting there is *some* transmission line effect going on. There is some distrbuted component (a series of inductors shunted by capacitors) going on. Everyone (except you) is being careful to qualify remarks by specifying the inductor is operating well below self-resonance. If you weren't so pig-headed you could look at the measured data at: http://www.w8ji.com/mobile_antenna_c...ts_at_w8ji.htm ....and see that as inductors move towards self-resonance they do begin to display characteristics of transmission lines. It's too bad in three years you have claimed others made a measurement error, when in fact the error is in thinking all of the current in a loading coil slowly winds its way around turn by turn and the magnetic field linking turns does not cause charges in other turns to move long before current traveleing at light speed would wind through the copper path. Until you stop, put the beer away, and think about this a while you'll continue to butt your head up against people who KNOW how inductors behave. 73 Tom |
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#4
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Cecil Moore wrote: You measured standing wave current, Tom. Your measurements are meaningless! Standing wave current has the same constant phase whether the coil exists or not. Your measurements prove absolutely nothing that is not already known. Nothing I have said has changed from what I've said for years. Now you have magnetic fields traveling slower than light speed in air, and have gone right back to the same nonsense of standing wave current. Please tell us all how you would measure the "traveling current" while ignoring "standing wave current". This ought to be good..... |
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#5
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Please tell us all how you would measure the "traveling current" while ignoring "standing wave current". Good question. One would ideally do it in a system without reflections. I am struggling with that concept right now. The best thought I have come up with so far is simple: coil +----////----+ | | source --- cap | --- | | +--/\/\/\/\--+ resistor I'm not a measurements guy so I could use some help. What's wrong with just reporting the measured the delay through your test coils? Your measured data already shows the current on one side of the coil to be different from the current on the other side of the coil. All we have to worry about now is the delay through the coils. If I've got your attention, let me repeat something I posted days ago. The forward current through the coil can indeed be assumed to be equal magnitude at both ends of the coil without much error. That should make you happy. The delay through the coil is whatever it is but it is nowhere near zero. I assume that makes you unhappy. The reflected current through the coil can indeed be assumed to be equal magnitude at both ends of the coil without much error. That should make you happy. The delay through the coil is whatever it is but it is nowhere near zero. I assume that makes you unhappy. The standing wave is the phasor sum of the forward wave and reflected wave. Its magnitude can vary from about double the forward current at a current loop to close to zero at a current node. I assume that makes you unhappy. The standing wave phase is close to constant and fixed near zero degrees within 1/4WL of the feedpoint. I assume that makes you happy. So three out of six results should make you happy and that's about all any mere mortal can hope for. :-) -- 73, Cecil http://www.qsl.net/w5dxp |
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#6
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Cecil Moore wrote: What's wrong with just reporting the measured the delay through your test coils? Your measured data already shows the current on one side of the coil to be different from the current on the other side of the coil. All we have to worry about now is the delay through the coils. What measurement are you talking about? The one I did over two years ago that has been up on my web site since that time? Something on a bench? |
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#7
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wrote:
What measurement are you talking about? The one I did over two years ago that has been up on my web site since that time? Something on a bench? That one on your web site measured the standing wave current. We know the phase of the standing wave current is irrelevent since it is essentially the same whether the coil is in or out of the circuit. i.e. there is no such thing as standing wave current "delay" since the phase of the standing wave current is essentially fixed at (or near) zero degrees. You have measured the S12 delay for 100uH at 1 MHz to be -60 to -70 degrees. What we need is the equivalent of the S12 delay for current, rather than for voltage. What is the current delay througn the coil when no reflections are present? In other words, if the coil were installed in a traveling-wave antenna, like a terminated rhombic, what would the delay be through the coil? -- 73, Cecil http://www.qsl.net/w5dxp |
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