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Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 4:24*pm, Cecil Moore wrote:
On Jan 12, 3:25 pm, Keith Dysart wrote: But, of course, V(t) and I(t) are general functions of time. In particular, the discusion was regarding pulses. Pulses can be analyzed as Fourier sinusoidal functions with multiple frequencies. Point is that you could have saved a month of grief on this newsgroup if you had initially said your power equation applied only to real voltage and real current. If you had done that, nobody would have argued with you. An earlier post suggested that you "had got it", but these last two posts leave me wondering. P(t) = V(t) * I(t) where V(t) and I(t) are functions describing the actual measureable voltage and current at a point on the line. Examples of V(t) would be V(t) = 10 V(t) = A cos(wt + a) These functions all yield real results since the voltage measureable at a point on the line is a real function of time. When the latter example is written in complex exponential form it becomes V(t) = Re[A*e^j(wt+a)] Re[] is not there because there is some imaginary part to be ignored, but because this is how one writes the function for V(t) in this notation. Thus Re[V(t)] is non-sensical since the Re[] is already in the expression describing the function. My apologies for not detecting this subtle bit of misleading thinking when I wrote my earlier reply. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 8:45 pm, Keith Dysart wrote:
P(t) = V(t) * I(t) where V(t) and I(t) are functions describing the actual measureable voltage and current at a point on the line. Apparently, the measurable *instantaneous* voltage and current. We could have avoided a lot of wasted time if you had stated those conditions a month ago. None of my references contain that equation. Re[] is not there because there is some imaginary part to be ignored, but because this is how one writes the function for V(t) in this notation. Where is it? You have never explained your assumptions before now. Please provide a reference. -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 12, 11:23*pm, Cecil Moore wrote:
On Jan 12, 8:45 pm, Keith Dysart wrote: P(t) = V(t) * I(t) where V(t) and I(t) are functions describing the actual measureable voltage and current at a point on the line. Apparently, the measurable *instantaneous* voltage and current. We could have avoided a lot of wasted time if you had stated those conditions a month ago. None of my references contain that equation. I am curious. What other interpretation than 'voltage as a function of time' did you have for "V(t)"? And, of course, when you plug any particular time into a function describing xxxx as a function of time, you get the value of xxxx at that time; the instantaneous value of xxxx. Or is there another possible interpretation? ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 13, 7:58 am, Keith Dysart wrote:
I am curious. What other interpretation than 'voltage as a function of time' did you have for "V(t)"? Strange question. My interpretation is not the "other interpretation". My interpretation is the (apparently) standard one from "Fields and Waves", by Ramo&Whinnery - begin quote: V(t) = Re[Vm*e^jwt] Because of the inconvenience of this notation, it is usually not written explicitly but is understood. - end quote When you used the term, "V(t)", I understood it to represent the Ramo&Whinnery definition applying to exponential notation. Your interpretation is the one that differs from that definition. What other interpretation than the Ramo&Whinnery equation do *YOU* have for V(t)? Or is there another possible interpretation? Apparently there is and you can prove it by providing a reference that extends V(t) in the Ramo&Whinnery definition above to something other than exponential notation. I am not doubting your word, just (pretty please) asking again for a reference that agrees with your statement that V(t) is used for something else. If "V(t)" is commonly used outside of the Ramo&Whinnery definition above, I apologize for being confused by the notation being used. -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 13, 8:54*am, Cecil Moore wrote:
If "V(t)" is commonly used outside of the Ramo&Whinnery definition above, I apologize for being confused by the notation being used. Apology accepted. As a cautionary note.... It is unwise to take the notation used in one text and blindly substitute into another, especially when the text is deriving for a specific case. The IEEE dictionary (see 'instantaneous power') starts with p = ei and then goes on to derive the special case for sinusoids. Desoer and Kuh, "Basic Circuit Theory", start with p(t) = v(t)i(t) then derive the special case for sinusoids by substituting v(t) = Vm * cos(wt+a) = Re[Vm * e^ja * e^jwt] {taking some liberties to make it ascii} Note that Re[] is only needed when using the exponential form and not the trigonometric form. And, from your post, it appears that Ramo and Whinnery start with W(t) = V(t) I(t) and do the derivation for the special case of sinusoids by substituting V(t) = Re[Vm*e^j(wt+A1)] These are all equivalent derivations using different notations. A key point is that they all start with "instanteous power being equal to instantaneous voltage times instantaneous current" as the general case and derive the special case by appropriate substitution. And a second key point is that Re[] is not needed in the general expression for power, (choose the form you like) p = ei p(t) = v(t) i(t) P(t) = V(t) I(t) , because it is already in the expressions for voltage and current when the exponential form is used. ...Keith |
Standing-Wave Current vs Traveling-Wave Current
On Jan 13, 12:02 pm, Keith Dysart wrote:
It is unwise to take the notation used in one text ... Unfortunately, I only brought one book with me. Ramo&Whinnery don't discuss non sinusoidal signals. Even their square waves are analyzed as a Fourier series whose total voltage is f(t), not V(t). -- 73, Cecil, w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote: You don't need Poynting vectors to realize that when the instantaneous power is always 0, no energy is flowing. And when the instantaneous power is always 0, it is unnecessary to integrate and average to compute the net energy flow, because no energy is flowing at all. And if by your response you really do mean that energy can be flowing when the instantaneous power is always 0, please be direct and say so. But then you will have to come up with a new definition of instantaneous power for it can not be that it is the rate of energy transfer if energy is flowing when the instantaneous power is zero. The little program I wrote shows that, on the line being analyzed, the energy is changing -- moving -- on both sides of a point of zero power. Energy is flowing into that point from both directions at equal rates, then flowing out at equal rates. This causes the energy at that point to increase and decrease. What zero power at a given point means is that there is no *net* energy moving in either direction past that point. Roy Lewallen, W7EL |
Standing-Wave Current vs Traveling-Wave Current
Roy Lewallen wrote:
... What zero power at a given point means is that there is no *net* energy moving in either direction past that point. Roy Lewallen, W7EL A black hole? :-D JS |
Standing-Wave Current vs Traveling-Wave Current
Comments interspersed. . .
Keith Dysart wrote: Thanks for offering the two capacitor/one capacitor view of the middle of the line. It took a bit of time to decide whether the commingling of the charge in the single capacitor at the middle of the line would solve my dilemma. So I considered this one capacitor in the exact center of a perfect transmission line. It is the perfect capacitor, absolutely symmetrical. So as the exactly equal currents flow into it on the exactly symmetrical leads, the charge is perfectly balanced so that the charge coming from each side exactly occupies its side of the conductor. As the two flows of charge flow over the perfectly symmetrical plates, they meet in the exact center, and flow no more. I conclude that a surface can be found exactly in the center of this capacitor across which no charge flows. Thus (un)happily returning me exactly to where I was before; there is a line across which no charge, and hence no energy, flows. I'm ok with that. To me, it's the same as splitting the capacitor into two separate ones, each with its own charge from one direction. More comments below. On Jan 2, 7:38 pm, Roy Lewallen wrote: I'm top posting this so readers won't have to scroll down to see it, but so I can include the original posting completely as a reference. Keith, you've presented a very good and well thought out argument. But I'm not willing to embrace it without a lot of further critical thought. Some of the things I find disturbing a 1. There are no mathematics to quantitatively describe the phenomenon. 2. I don't understand the mechanism which causes waves to bounce. I take this to imply that you are not happy with the simple "like charge repels"? That's right. Although it's a true statement, I haven't seen any explanation of why it would cause waves to bounce off each other. 3. No test has been proposed which gives measurable results that will be different if this phenomenon exists than if it doesn't. (I acknowledge your proposed test but don't believe it fits in this category.) 4. I'm skeptical that this mechanism wouldn't cause visible distortion when dissimilar waves collide. But without any describing mathematics or physical basis for the phenomenon, there's no way to predict what should or shouldn't occur. 5. Although the argument about no energy crossing the zero-current node is compelling, I don't feel that an adequate argument has been given to justify the wave "bouncing" theory over all other possible explanations. I would really appreciate seeing some other possible explanations. How about this: During the initial turn-on of the system, energy does cross the magic node. It's only in the theoretical limiting case of steady state that the energy goes into and out of the node but doesn't cross it. I'll argue that the limiting case can never be reached -- since this whole setup is a perfect construct to begin with. Or, if that's not adequate by itself, what's the problem with energy being trapped between nodes once the line is charged and steady state is reached? One other one which I have seen and am not confortable with is the explanation that energy in the waves pass through the point in each direction and sum to zero. But this is indistinguishable from superposing power which most agree is inappropriate. As well, this explanation means that P(t) is not equal to V(t) times I(t), something that I am quite reluctant to agree with. I won't go there either. The other explanation seen is that the voltage waves or the current waves travel down the line superpose, yielding a total voltage and current function at each point on the line which can be used to compute the power. This is done and graphically shown with the TLVis1 program demo. The energy at each point is also calculated and shown. With this explanation, P(t) is definitely equal to V(t) time I(t), which I do appreciate. The weakness of this explanation is that it seems to deny that the wave moves energy. And yet before the pulses collide it is easy to observe the energy moving in the line, and if a pulse was not coming in the other direction, there would be no dispute that the energy travelled to the end of the line and was absorbed in the load. Yet when the pulses collide, no energy crosses the middle of the line. Yet energy can be observed travelling in the line before and after the pulses collide. I think the basic problem here is assigning energy to each traveling wave. It's taking you into exactly the same morass that Cecil constantly finds himself in. He also concluded some time back that two waves which collide had to reverse direction in order to conserve power, energy, momentum, or something. Energy in the system is conserved; but nowhere is it written that each wave has to have individually conserved energy. So... I can give up on pulses (or waves) moving energy. I am not happy doing that. I'm afraid you might have to. I can give up on P(t) = V(t) * I(t). I am not happy doing that either. Fortunately, that's not necessary. So the (poorly developped) "charge bouncing" explanation seems like a way out, but I certainly would appreciate other explanations for consideration. I think you need to take a closer look at what it's getting you out from. I believe the problem lies there. None of these make an argument with your logical development, although I think I might be able to do that too. But I'm very reluctant to accept a view of wave interaction that's apparently contrary to established and completely successful theory and one, if true, might have profound effects on our understanding of how things work. So frankly I'm looking hard for a flaw in your argument. And I may have found one. So I am not convinced that it any way goes against established theory. I have not seen established theory attempt an explanation of how the waves can both transport energy as well as not do so when waves of equal energy collide. Perhaps that's because individual waves don't transport energy that has to be conserved? . . . It would be instructive to see what happens as, for example, the load resistance is increased toward infinity or decreased toward zero arbitrarily closely, but not at the point at which it's actually there. If the "bouncing" phenomenon is necessary only to explain the limiting case of infinite SWR on a perfect line but no others, then an argument can be made that it's not necessary at all. I suspect this is the case. The same concern that arises for pulses of equal voltage also occurs for pulses of different voltage. While the mid-point no longer has zero current, the actual current is only the difference of the two currents in the pulses, the charge that crosses is only the difference in the charge between the two pulses, and the power at the mid-point is exactly the power that is needed to move the difference in the energy of the two pulses. Sorry, I'm having trouble following that. Voltage, current, charge, and energy all in two sentences has too high a concept density for me to handle. So the challenge is not so starkly obvious as it is when the power at the mid-point is always 0, but P(t) = V(t) * I(t) can still be computed and it will not be sufficient to allow the energy in the two pulses to cross the mid-point (unless one likes superposing power, in which case it will be numerologically correct). No, it'll have to be done without superposing power. Simple calculations clearly show where the power is and where the energy is going, without the need to superpose power or assign power or energy to individual waves. I agree with your argument about two sources energized in turn, and have used that argument a number of times myself to refute the notion of superposing powers. Once two voltage or current waves occupy the same space, the only reality is the sum. We're free to split them up into traveling waves or any other combination we might dream up, with the sole requirement being that the sum of all our creations equals the correct total. (And the behavior of waves you're describing seemingly go beyond this.) I sometimes think that this may actually be a debate about the conceptual view of waves. If waves consist only of voltage and current, then all is well, superposition works, the correct answers are achieved. And if the power is computed after the voltages and currents are arrived at, all is well. But if one conceives waves as also including energy, then it seems that the question 'where does the energy go' is valid and the common explanations do not seem to hold up well. I think you're partially right about that. Partially, because I think there's an underlying assumption that the power in an individual wave has to be conserved. If you do insist on assigning energy to individual traveling waves, I think you have to be willing to deal with the fact that the energy can be swapped and shared among different waves, and stored and returned as well. Our common analytical techniques deal with E and H fields which we can superpose. In a transmission line, these are closely associated with voltages and currents. They add nicely to make a total with properties we can measure and characterize, and the total can neatly be created as the sum of individual traveling waves from turn on until steady state. It all works very well. Two fields, voltages or currents can easily add to zero simply by being oriented in opposite directions -- and they do, all along a transmission line. But how are the energies they supposedly contain going to add to zero? You'll have to construct a whole new model if you're going to require conservation of energy of individual traveling waves. I'm absolutely certain that after all the work of developing a self-consistent model with all interactions quantitatively and mathematically explained and accounted for, we'll find a testable case where some measurable result will be different from the conventional viewpoint. (Google "ultraviolet catastrophe".) That would then establish the validity of the new model. But I'm just as certain that no such mathematical model will ever be forthcoming. The advantage to the non-interacting traveling wave model is that it so neatly predicts transient phenomena such as TDR and run-up to steady state. I spent a number of years designing TDR circuitry, interfacing with customers, and on several occasions developing and teaching classes on TDR techniques, without ever encountering any phenomena requiring explanations beyond classical traveling wave theory. So you can understand my reluctance to embrace it based on a problem with energy transfer across a single infinitesimal point in an ideal line. Yes, indeed. Though any (new) explanation would have to remain consistent with the existing body of knowledge which works so well. Either that, or be able to demonstrate where the existing knowledge fails. I'm not holding my breath. Roy Lewallen, W7EL |
Standing-Wave Current vs Traveling-Wave Current
Roy Lewallen wrote:
What zero power at a given point means is that there is no *net* energy moving in either direction past that point. Exactly! But that does not preclude the forward Poynting vector being equal in magnitude to the reflected Poynting vector. -- 73, Cecil http://www.w5dxp.com |
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