W5DXP wrote:
You will never understand the present topic unless you understand that EM wave interference doesn't affect the flow of energy in the individual waves. That is true for light and RF. I should have added: "in the absence of a physical impedance discontinuity." If a physical impedance discontinuity exists, then of course, the flow of energy in the individual waves is affected by reflections. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
I wrote:
"As energy can`t be destroyed it had to be reflected by a hard short or open." Keith replied: "Or just stopped and stored." Wave energy is energy in motion. No motion, no waves. Keith also wrote: "All of this is easily visualized by observing the amplitude of the P(t) function at various points along the line." Power as a function of time has the same amplitude in the forward wave everywhere along the line. Same is true of the reflected wave. Interference as demonstrated by standing waves has no effect on this. Keith wrote: "I would strongly suggest that no energy crosses these points in the line where the voltage and current are always zero since p(t) is always zero." See my comment above on power as a function of time. Keith erred in saying "points in the line where the voltage and current are always zero", as where SWR volts are zero, amps are max, and vice versa. I wrote: "If energy were turned around before it reached the end of the line, nulls more distant from the source than the turnaround point would not exist." Keith wrote: "Not so,---." There is no argument that can make wave interference where there are no waves. In a lossless line, pre-existing waves could circulate forever. But, our discussion relates to effects on actual lines. Keith wrote: "Try visualizing how a step function charges the line." Totally irrelevant. SWR nulls are the result of phase opposition at specific points produced by alternating waves. A step function changes only when it starts or stops. Only during the changes does Zo apply unless a line is terminated in its Zo. In this case there`s no reflected wave to make a null. As Reg once said, "If your line were infinite in length, you could measure Zo with your ohmmeter. Best regards, Richard Harrison, KB5WZI |
Keith wrote:
"I do not find that step 7) is in error." Step 7) declares power is zero at quarter wave points where volts or amps are zero in the standing wave pattern. Power flow does not stop at an actual short or open in a line. It merely changes direction. At zero volt or amp points, where there is no actual short or open, no reversal of direction occurs. Power flow is affected in no way by standing wave nulls or maxima where no impedance discontinuity exists. Energy exists in every SWR null. It is in the two waves which produce the null as these experience no change in energy due to standing waves. Best regards, Richard Harrison, KB5WZI |
What is missing here, IMO, is that the physics of energy flow has not
been adequately explained. Cecil provided a reference to it but did not elaborate for the general readership. The energy in forward and reflected waves has been well documented for many years. From Kraus, Electromagnetics, McGraw Hill, 1953, Chapter 9, Section 9-13, "Energy Relations in a Standing Wave": EQ 9-145 We = 2eEo^2[cos^2wt*sin^2Bx] EQ 9-147 Wm = 2uHo^2[sin^2wt*cos^2Bx] Note: The energy in the E field [We] is a function of the sin^2(Bx). The energy in the H field [Wm] is a function of the cos^2(Bx). You will remember from trigonometry the the maxima [or minima] of a sin and cos are displaced by 90 degrees. Conclusion: when the E field is zero the H field is maximum; when the H field is zero the E field is maximum. Ergo! Energy is conserved and propagates through the zero E field as an H field; also, when the H field is zero the energy is in the E field. This is what Cecil is referring to when he refers to the Poynting vector. It is analogous to a parallel tuned circuit. When the instantaneous voltage across the capacitor is zero we don't claim there is no energy in the circuit. We know that the energy is stored in the inductor. Conversely, when the instantaneous current in the inductor is zero we don't claim there is no energy in the circuit. We know the energy is stored in the capacitor. In a TEM wave the energy cycles between the E field and the H field and the energy components are 90 degrees out of phase. Deacon Dave, W1MCE |
wrote:
What about Ramo and Whinnery's forward Poynting vector and reflected Poynting vector? Why do you choose to ignore them? I haven't used them because I don't need them to arrive at an answer. Yes, but you need them to arrive at the correct answer. :-) Basic electricity, a dash of circuit theory, a bit of knowledge of trigonometry, some basic calculus and the ability to think is all that is required. Apparently, that is not all that is required. Here's a neat web page that will allow you to visualize what is happening. Note the forward and reflected waves do not change energy or momentum at a zero voltage point. http://www.gmi.edu/~drussell/Demos/s....html#standing -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
Keith wrote:
"Basic electricity, a dash of circuit theory, a bit of knowledge of trigonometry, some basic calculus, and the ability to think is all that is required." An electrical education limited to d-c familiarity leads to mistaken assumptions when dealing with a-c in Keith`s case it seems. Best regards, Richard Harrison, KB5WZI |
Richard Harrison wrote:
Keith wrote: "I do not find that step 7) is in error." Step 7) declares power is zero at quarter wave points where volts or amps are zero in the standing wave pattern. Unfortunately, probably due to my poor description, you have missed the point I was trying to make. You are, I think, disagreeing with the RESULT of step 7. Even though the result may be wrong, step 7) can be correct. Step 7) again: "7) From 6), the energy crossing quarter wave points is 0" This is saying that if the result of step 6) is correct, then the result of step 7) is correct. The transformation from 6) to 7) merely integrated power to get energy; a common and correct thing to do. So if you disagree with the result of step 7), it is in step 6) which you must search for the error since step 7) is correct. If step 6) is correct, then search in step 2) and step 5) for the error. I suspect that like Cecil, you will end up at step 2) as the source of what you perceive to be an error. Then, when we resolve whether 2) is in error, we will know whether the result of 7) is in error. ....Keith |
W5DXP wrote:
wrote: Seems to me that the sinusoidal standing wave with minima and maxima at the quarter wave points can only arise with single frequency sinusoidal excitation of the line. Are there other signals which will produce this result? Probably not, but that makes sinusoids unique, not magic. Magic was your moniker not mine. But I am glad that you agree. What about Ramo and Whinnery's forward Poynting vector and reflected Poynting vector? Why do you choose to ignore them? I haven't used them because I don't need them to arrive at an answer. You need them to keep from making the same mistakes over and over. I've being using p(t) = v(t) * i(t) and simply arguing that when v(t) or i(t) is zero for all t, then there is no power. Poynting won't change a thing. There is no P when E or H is zero. So the debate can be had with the simpler p(t) = v(t) * i(t). There is no need to complexify. ....Keith |
Richard Harrison wrote:
Keith wrote: "Are there other signals which would produce this result?" A short-circuit produces a voltage inversion. The plus volts and the minus volts make a zero in a short. Imagine a couple of identical positive pulses separated by some distance and traveling in the same direction along a long transmission line which has a short approached by the pulses. When the first pulse hits the short it is inverted and reflected to travel back toward its source as a minus voltage pulse. When the first pulse encounters the second pulse they disappear at the instant of coincidence, but otherwise, travel on their merry ways. What happens at coincidence is transfer of the energy associated with volts to the energy wave associated with amps as energy can`t be obliterated while the volts disappear. I do like pulses. Thinking about pulses on the line certainly helped clarify my understanding of how lines worked. So what happens when two pulses collide? I don't think you will like this answer either, but here goes. First, remember that power and energy are not the same. Power can become zero while the energy remains. It simply means that the energy is now stored in the capacitance or inductance (or equally, the E field or H field) but is not moving. So no energy is lost or destroyed when the power goes to zero. So what happens to these two pulses? They bounce off of each other and return whence they came. This must happen since the voltage on the region of the line where the two pulses collide remains zero and since p(t) = v(t) * i(t) there is no power in this region so there must be no energy flowing. You would observe exactly the same result were you to short the line at the point of collision just before the collision occurred. Two pulses colliding is just like a reflection. As a simple analogue, consider two identical elastic balls rolling towards each other. They bounce back after the collision. On a line this is easier to visualize with two negative pulses colliding. Each pulse consists of a clump of charge. When these clumps of charge collide, remembering that like charge repels, they bounce back. What actually happens during the collision? With balls, the energy is stored in the deformation of the ball and then released as the balls separate. With pulses, the power stops (current is zero), and the energy is stored in the capacitance of the line in the region of the collision. After all the energy has stopped flowing (no power, zero current, all energy in the E field), the energy is released into the reflected pulses and once again, there is energy moving (power) on the line. ....Keith |
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