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#1
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Roy Lewallen wrote:
A standing wave is the result of, and the sum of, two or more traveling waves. There aren't points which are "on" one or the other. If you can separately measure or calculate the values of the traveling current waves at any point, you can add them to get the total current (what Cecil calls "standing wave current") at that point. If you add the traveling current waves at each point along the line and plot the amplitude of the sum (that is, of the total current) versus position, you see a periodic relationship between the amplitude and position. It's this relationship which is called a "standing wave". It's so called because its position relative to the line stays fixed. It's simply a graph of the total current (the sum of the traveling waves) vs. position. And there's no such thing as current imbalance based on standing wave currents being different at each end of a loading coil. "Current imbalance" is a concept that doesn't apply to standing waves. "Phase rotation with position" is a concept that doesn't apply to standing waves. Standing wave current is NOT ordinary current. It is the superposition of two ordinary currents. -- 73, Cecil http://www.qsl.net/w5dxp |
#2
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Cecil Moore wrote:
And there's no such thing as current imbalance based on standing wave currents being different at each end of a loading coil. "Current imbalance" is a concept that doesn't apply to standing waves. "Phase rotation with position" is a concept that doesn't apply to standing waves. Standing wave current is NOT ordinary current. It is the superposition of two ordinary currents. You two are so close to agreement. Standing waves have a current that varies with position. The fact that the EZNEC simulation of a loading coil shows differing current in a situation that is a fairly pure standing wave situation (more energy bouncing up and down the antenna than is radiating from it) means that the RMS current will vary along the standing wave. And, since the simulation shows a different current magnitude at the two ends of the coil, a significant part of a standing wave cycle must reside inside the coil (more than the physical length between the two ends of the coil would account for). In one case (the highest frequency one) the phase of the current even reverses from one end of the coil to the other, as well as an amplitude variation, indicating that a standing wave node occurs some where inside the coil, and the two ends are on opposite ends of that node. If the two currents had been equal, but 180 degrees out of phase, the node would have been in the center of the coil. |
#3
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John Popelish wrote:
You two are so close to agreement. Standing waves have a current that varies with position. The fact that the EZNEC simulation of a loading coil shows differing current in a situation that is a fairly pure standing wave situation (more energy bouncing up and down the antenna than is radiating from it) means that the RMS current will vary along the standing wave. And, since the simulation shows a different current magnitude at the two ends of the coil, a significant part of a standing wave cycle must reside inside the coil (more than the physical length between the two ends of the coil would account for). No, you're misinterpreting what you're seeing. Imagine an LC L network with theoretically lumped series L and shunt C. If you look at the currents at the input and output of the perfect inductor, you'll find that they're exactly the same. If, however, you look at the currents in and out of the *network* you'll see that they're different, because of current going to ground through the C. And, as I said before, you can even pretend it's a transmission line and measure forward and reverse traveling waves and a standing wave ratio. But with zero length, there can be no standing waves inside the inductor. Yet the terminal characteristics of the network are the same as a transmission line. You don't need to imagine standing waves residing inside the inductor in the LC circuit, and you don't need to imagine them inside the inductor in Cecil's model, either. When you look at the currents reported by EZNEC for the model on Cecil's web page, the current at the top of the coil is the equivalent to the *network* current described above. It's the current flowing through the inductance minus the current being shunted to ground via the C between the coil and ground. You can tell just how much this is by looking at my modified model and subtracting the current going into the coil from ground from the current going into ground from the added wire. They're not the same -- the difference is the displacement current through the C from the inductor to ground. When I removed the ground, you could then see the current flowing through the inductor, by itself, without the current being shunted off. And lo and behold, it's nearly the same at both ends of the inductor, showing that the inductor is behaving very much like a lumped L. Only in conjunction with the C to ground does the combination mimic a transmission line -- just like any other lumped LC circuit. Of course, at some length and/or poorness of interturn coupling, a coil will start behaving in a way we can't adequately model as a lumped L. But that's not the case here. . . . Roy Lewallen, W7EL |
#4
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Roy Lewallen wrote:
If, however, you look at the currents in and out of the *network* you'll see that they're different, because of current going to ground through the C. The main effect in a standing wave environment are the forward and reflected phasors rotating in opposite directions. The standing wave current is ZERO when those phasors are 180 degrees out of phase. The standing wave current is maximum when those phasors are in phase. "Current going to ground through the C" is not even required. But with zero length, there can be no standing waves inside the inductor. You keep saying stuff like this as if a zero length inductor actually existed in reality. Wake up, Roy, and smell the roses. That zero length inductor exists only in human minds. When you look at the currents reported by EZNEC for the model on Cecil's web page, the current at the top of the coil is the equivalent to the *network* current described above. It's the current flowing through the inductance minus the current being shunted to ground via the C between the coil and ground. Huh? How do you explain the current at the top being greater than the current at the bottom of the coil? Is the coil sucking current from the ground? -- 73, Cecil http://www.qsl.net/w5dxp |
#5
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![]() Cecil Moore wrote: Roy Lewallen wrote: If, however, you look at the currents in and out of the *network* you'll see that they're different, because of current going to ground through the C. The main effect in a standing wave environment are the forward and reflected phasors rotating in opposite directions. The standing wave current is ZERO when those phasors are 180 degrees out of phase. The standing wave current is maximum when those phasors are in phase. "Current going to ground through the C" is not even required. That's utter nonsense Cecil, and why people aren't buying into your misconceived theories. Maybe you can take some time to rethink your position while on vacation. A two-terminal network that transforms impedance, now there's a concept! An inductor behaves exactly the same way in or out of your so-called standing wave environment. It follows the same rules all the time. Since your theory says otherwise, it has to be wrong. Wave theory is just another way of analyzing a complex system. It doesn't change how things inside the system behave. 73 Tom |
#7
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#8
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John Popelish wrote:
wrote: A two-terminal network that transforms impedance, now there's a concept! (My opinion follows, please correct me. Dang, I should put that in my sig.) In reality, there is no such thing as a two terminal network, unless one of those terminals is grounded. For all other cases, there is an unavoidable implied ground terminal that covers all the stray capacitance of the device. So the bug catcher coil is recognized as a 3 terminal device, with ground being the third terminal. It can be modeled as a pi, T or transmission line structure, as long as you want to understand what to quantify it at only one frequency (or a narrow band), and the choice is arbitrary. If you are concerned with modeling a large frequency range (that goes well past the first self resonance), one of those models (or a more complicated one) will be superior. You fellows lack imagination. As long as you're trying to morph a coil into a transmission line, why not just imagine it as a shorted stub? There's more than one way to make an inductive reactance. 73, Tom Donaly, KA6RUH |
#9
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Roy Lewallen wrote:
John Popelish wrote: No, you're misinterpreting what you're seeing. Imagine an LC L network with theoretically lumped series L and shunt C. Okay, I am imagining an idealized, network made of perfect, impossible components that is simple to analyze. Got it. If you look at the currents at the input and output of the perfect inductor, you'll find that they're exactly the same. Right. If, however, you look at the currents in and out of the *network* you'll see that they're different, because of current going to ground through the C. Got it. Same for any pi, T, or more complicated LC network. And, as I said before, you can even pretend it's a transmission line and measure forward and reverse traveling waves and a standing wave ratio. Yes. Under some specific conditions. But with zero length, there can be no standing waves inside the inductor. Yes. There are no waves in a single ideal lumped component, so there can be no waves inside any of them, only a phase shift between the voltage across them and the current through them. But a network made of them can mimic lots of processes that internally involve propagation of waves, including the phase shift between voltages across the terminals and current into the terminals, and even group delay, but only over narrow frequency range. It is a model with this severe limitation. Yet the terminal characteristics of the network are the same as a transmission line. You don't need to imagine standing waves residing inside the inductor in the LC circuit, and you don't need to imagine them inside the inductor in Cecil's model, either. (snip) Whether or not we need to imagine them to picture what is happening at the terminals is not the question at hand. The question in my mind is what is the actual mechanism, inside the device in question that is causing the effects we see at the terminals. I am not interested in the full range of models that predict the effect, but in the actual cause. I accept that my motivation is not necessarily the same as yours. |
#10
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John Popelish wrote:
Standing waves have a current that varies with position. The fact that the EZNEC simulation of a loading coil shows differing current in a situation that is a fairly pure standing wave situation (more energy bouncing up and down the antenna than is radiating from it) means that the RMS current will vary along the standing wave. And, since the simulation shows a different current magnitude at the two ends of the coil, a significant part of a standing wave cycle must reside inside the coil (more than the physical length between the two ends of the coil would account for). And since a significant part of a standing wave cycle resides inside the coil, it occupies a non-negligible percentage of a wavelength. By every valid method, measured or calculated, a 75m bugcatcher coil occupies tens of degrees of a wavelength (out of 360 degrees). My best estimate is 60 degrees in a 75m mobile antenna. In one case (the highest frequency one) the phase of the current even reverses from one end of the coil to the other, as well as an amplitude variation, indicating that a standing wave node occurs some where inside the coil, and the two ends are on opposite ends of that node. If the two currents had been equal, but 180 degrees out of phase, the node would have been in the center of the coil. Yes, if a current node exists inside a coil, the standing wave currents are flowing into the coil at the same time from both ends and 1/2 cycle later they are both flowing out of the coil at the same time. Wonder how a lumped-circuit inductance handles that? :-) -- 73, Cecil http://www.qsl.net/w5dxp |
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