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#1
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Cecil Moore wrote:
Jim Kelley wrote: What difference would it make, Cecil? One that is short compared to the delay. What difference would it make if the frequency of the pulse is far removed from the operating frequency? What difference would it make if the frequency is far above the self-resonant frequency? What difference would it make if the inductance is completely swamped by the capacitance? Shirley, you jest. The advantage to using pulses is that they are 'broadband' - they don't have "A" frequency. The inductance and capacitance of the system are unaffected by the small signals one impresses upon it. What's different about the 'situ' during steady state that causes electromagnetic fields to propagate differently than at other times? They don't propagate differently but how does one separate the forward wave from the reflected wave on a standing-wave antenna? If you can do that, you will have solved the measurement problem. The antenna behaves physically in exactly the same way whether or not it happens to be 'occupied' by waves, standing, sitting, or whatever during measurement. If you want to know how long it take an electromagnetic wave to traverse a conductor in any shape or configuration, you pulse it and measure how long it takes, either to get from one end to the other, or to be reflected back from the other end. There are of course dispersion effects, and by studying the change in the waveshape it is possible to deconvolve the frequency dependent components. This is a matter of routine for practicioners. 73, ac6xg |
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#2
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Jim Kelley wrote:
The advantage to using pulses is that they are 'broadband' - they don't have "A" frequency. The inductance and capacitance of the system are unaffected by the small signals one impresses upon it. But we are not interested in the phase delay for all those other frequencies. We are only interested in the phase delay at one particular frequency. And since we are talking about distributed networks and not lumped circuits, the inductance and capacitance of the coil does change with frequency. Whatever measurements we make need to be made at the frequency of operation. The antenna behaves physically in exactly the same way whether or not it happens to be 'occupied' by waves, standing, sitting, or whatever during measurement. If you want to know how long it take an electromagnetic wave to traverse a conductor in any shape or configuration, you pulse it and measure how long it takes, either to get from one end to the other, or to be reflected back from the other end. If the pulse is not at the frequency of operation, the results are hardly useful at all since the response of the loading coil is frequency dependent. So we are back to the original question. How can the delay through a mobile loading coil be measured at the frequency of operation in a standing-wave antenna? -- 73, Cecil, w5dxp.com |
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#3
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Cecil Moore wrote: If the pulse is not at the frequency of operation, the results are hardly useful at all since the response of the loading coil is frequency dependent. So we are back to the original question. It's clear that you are still back at that question. That doesn't necessarily apply to everyone else though. What I would suggest is that you go back, re-read, and try to undertstand the post, in particular the parts you deleted. 73, ac6xg |
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#4
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Jim Kelley wrote:
It's clear that you are still back at that question. That doesn't necessarily apply to everyone else though. What I would suggest is that you go back, re-read, and try to undertstand the post, in particular the parts you deleted. What's to understand? If the measurements are not made at the operating frequency, there is no way to prove that they are valid. Both the velocity factor and the characteristic impedance of a loading coil change dramatically with frequency. What is wrong with using a sinusoidal traveling wave to measure the phase shift through a coil at its frequency of operation? -- 73, Cecil, w5dxp.com |
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#5
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Cecil Moore wrote:
Jim Kelley wrote: It's clear that you are still back at that question. That doesn't necessarily apply to everyone else though. What I would suggest is that you go back, re-read, and try to undertstand the post, in particular the parts you deleted. What's to understand? If the measurements are not made at the operating frequency, there is no way to prove that they are valid. It appears that you would benefit from an understanding of the spectral nature of broadband pulses. Both the velocity factor and the characteristic impedance of a loading coil change dramatically with frequency. What is wrong with using a sinusoidal traveling wave to measure the phase shift through a coil at its frequency of operation? You need to be able to demonstrate that attaching a load resistor to a standing wave antenna in order to turn it into a traveling wave antenna does not dramatically change the characteristics. 73, Jim AC6XG |
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#6
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Jim Kelley wrote:
It appears that you would benefit from an understanding of the spectral nature of broadband pulses. I understand Fourier analysis. What is the benefit of using a lot of frequencies when you could use the frequency of interest? You need to be able to demonstrate that attaching a load resistor to a standing wave antenna in order to turn it into a traveling wave antenna does not dramatically change the characteristics. Proving a negative is impossible. If you are asserting that attaching a load resistor to a loading coil dramatically changes the characteristics, the onus of proof is upon you. -- 73, Cecil, w5dxp.com |
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#7
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Cecil Moore wrote:
What is the benefit of using a lot of frequencies when you could use the frequency of interest? Your memory is growing short. Do you not remember challenging me to do that very thing - claiming it was impossible? I said I would use pulses, then you said it wouldn't work, bla bla bla. Circuitious, isn't it. If you are asserting that attaching a load resistor to a loading coil dramatically changes the characteristics, the onus of proof is upon you. It should be readily apparent to just about anyone that one does in fact significantly alter the characteristics of a system by changing it from one which has a reflection at the end to one which doesn't. 73, ac6xg |
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