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Standing-Wave Current vs Traveling-Wave Current
Roy Lewallen wrote:
People who are having trouble with the concept of a -1 voltage reflection coefficient for a perfect voltage source might benefit from the following exercise: Look at my first analysis, where the perfect source was connected directly to the transmission line. Make no assumptions about the impedance or reflection coefficient it presents. Then, when the reflection of the initial forward wave returns, calculate the value the re-reflected wave must have in order to make the sum of the waves present, which is the line input voltage, equal to the perfect source voltage. The voltage of the perfect source can't change, by definition. The ratio of the re-reflected wave to the returning wave is the voltage reflection coefficient (since we're dealing with voltage waves). I'll do it for you: The forward wave was vf(t, x) = sin(wt - x) The returning wave was vr(t, x) = sin(wt + x) The returning wave will strike the input end of the line and create a new forward wave with value vf2(t, 0) = Gs * vr(t, 0) at the input, where Gs is the source voltage reflection coefficient. Before the first forward wave returns, we have only vf(t, 0) = sin(wt) at the input end of the line. This is of course the source voltage. After the wave arrives and re-reflects, we have at the input end vtot(t, 0) = vf(t, 0) + vr(t, 0) + vf2(t, 0) = vf(t, 0) + vr(t, 0) * (1 + Gs) This must equal the source voltage, which is the line input voltage, and cannot change. So plugging in values: sin(wt) = sin(wt) + sin(wt) * (1 + Gs) Solving for Gs = Gs = -1 I have made no statement about the "impedance" of the perfect source. The only thing I've required is that the voltage remains constant, which is the very definition of a perfect source. You can do a similar exercise to show that the voltage reflection coefficient of a perfect current source is +1. Roy Lewallen, W7EL I see your example as identical to Keith's example of two wave pulses traveling in opposite directions. At the point of interaction, Keith's example has a reflection factor of 1 or zero, depending upon whether the waves bounce or pass. Keith's example is not a short circuit because two pulses of identical polarity are interacting so a reflection factor of -1 could never exist. In your example, the presence of voltage from the ideal source creates conditions identical to Keith's example for the returning reflected wave. Accepting this premise, then the reflection factor must be either 1 or zero, depending upon whether the waves bounce or pass. By assuming that the waves reflect at the ideal source, you proved that the reflection factor is -1, which is the factor for a short circuit. This can not be the case, so waves must not reflect at the ideal voltage source, they must pass. vtot(t, 0) = vf(t, 0) + vr(t, 0) = sin(wt)tot = sin(wt) + sin(wt) = 2*sin(wt) Someone will certainly say the the vtot(t,0) at the source location is the source voltage, because it is defined that way. The conditions at point (t,0) itself is actually unknown (because vf mysteriously appears, and vr disappears by going off the transmission line), but point (t, 0) is defined by assumptions. Therefore, at vtot(t, 0) = vf(t, 0) + vr(t, 0) = sin(wt)tot = sin(wt) + sin(wt) = 2*sin(wt) 73, Roger, W7WKB |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
Can photons explain the state of a transmission line driven with a step function after the line has settled to a constant voltage? Of course, photons can be used to explain all EM wave action. A step function accelerates electrons which then emit photons as EM waves. Hint: electrons cannot move at the speed of light. EM waves move at the speed of light. -- 73, Cecil http://www.w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
So there is NO reference that claims that the output impedance can not be used to compute the reflection coefficient. If I say I am not going to look for a reference to "creation" in The Bible, are you going to assert there are no references to creation in The Bible? Good luck on your ridiculous assertions. So that settles it, then. No, it is not settled. Please reply to my posting where I proved the reflection coefficient is plus or minus one, the exact opposite of what you assert. And the arguments that I have seen between Mr. Maxwell and Dr. Bruene are on a completely different matter. If you think that, it's prima facie evidence that you are really confused. -- 73, Cecil http://www.w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
My attempt to confuse!? We were discussing the determination of reflection coefficients for Thevenin equivalent circuits. No, we were discussing destructive and constructive interference. Sorry about your confusion. But in another post, you have agreed that there is a complete lack of references supporting your position, ... No, I said I am not going to look for them. Sorry about your confusion. Enjoy the new ability to solve problems that were previously outside your grasp. I'm sorry, Keith, delusions of grandeur are a problem outside of my field of expertise. Perhaps a professional shrink could help you better than I. -- 73, Cecil http://www.w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Thu, 3 Jan 2008 06:28:19 -0500, "David J Windisch"
wrote: You were writing of Tesla over Edison, a-c over d-c power transmission, and I was reminded that Prez Kennedy started some work years ago somewhere in the West, involving hvdc transmission. I wasn't intentionally obscuring things in that earlier post. 73 Dave N3HE Hi Dave, I am well practiced mixing it up with the masters of obscurity, and I certainly don't confuse you with Prior Art, or Cecileo. However, the HVDC project you allude to is new to me (even if it is/was decades old). As an aside, I have worked with the lawyer who was instrumental in closing down WPPS (a nuclear power consortium we generally called WHOOPS). That consortium agonized that Washington's credit rating would go down the toilet if we defaulted - barely a blip in the interest rate resulted when we mothballed several nuclear reactors. Even further aside, I lived in Japan in the early 50s when they used DC residential power (and we had to be careful to buy AC/DC appliances). Woe to those living at the end of the block where the street lights were dim. Edison used to portray AC as being the killer current (eventually selected for use on death row). Actually there were a mix of characteristics that lent either the death potentiality. DC will cause the muscles to clamp, and if you seized a hazardous wire, you could never let go. AC, on the other hand (no pun), would cause fibrillation, and you stood some chance of releasing the same hazardous wire. AC, on the third hand (again, no pun), would also cause the sweat glands to excrete (due to the same fibrillation) and lower your path resistance (more lethal current). 73's Richard Clark, KB7QHC |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
Excellent. So there is NO reference that claims that the output impedance can not be used to compute the reflection coefficient. That is probably a false statement. I just haven't wasted my time looking for a reference that uses those exact words. There are many references that do. I seriously doubt that they say what you are asserting. Please produce those references. In another thread, I proved your assertion wrong. A Bird wattmeter placed at the output of your source will read forward power = reflected power. The reflection coefficient can be calculated from that. rho = SQRT(Pref/Pfor) = plus or minus 1.0 -- 73, Cecil http://www.w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On 3 Jan, 09:51, Cecil Moore wrote:
Keith Dysart wrote: If such analysis is appropriate, then it seems to me that a pulse can be viewed as a chunk of charge moving down the line. Q2. Is this an appropriate view? No. Q3. If so, then what happens when two such chunks of charge collide in the middle of the line? They don't "collide". Clouds of photons collide and their behavior is well known. Q5. If no charge crosses the mid-point, then how do the pulses, made up of chunks of charge. pass the mid-point? How can two water waves pass through each other while the water molecules are only moving up and down? -- 73, Cecil *http://www.w5dxp.com Cecil The current only changes direction at the behest of the frequency. I know you think that the current changes at the behest of the length of radiator used i.e. at the top but frankly that is lunacy. It is only when the capacitor charge starts to move to the inductance and starts to store energy which generates a diamagnetic field can propagation can occur You must get a pencil and paper and think things out for yourself instead of relying on books. With your IQ it should be a cake walk because unlike some others you are able to get back to first principles instead of learning by rote. No personal offence intended. Being stubborn is not all that bad but only if you are willing to think out alternatives given. Otherwise it is a not invented in my back yard aproach which amounts to an over inflation of one's ability Best regards Art |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
The example was carefully chosen to illustrate the point, of course. But that is the value of particular examples. When the pulses are not identical, the energy that crosses the point is exactly sufficient to turn one pulse into the other. The remainder of the energy must bounce because it does not cross the mid-point. ...Keith So it really is almost as though the pulses travel through one another, rather than bounce off one another. I have seen the concept that energy doesn't cross nodal points alluded to in some texts. However there are so many exceptions to it found in physical systems as to render it a dubious notion at best. Useful perhaps for illustration purposes. In the discussion of standing waves on a string, Halliday and Resnick says "It is clear that energy is not transported along the string to the right or to the left, for energy cannot flow past the nodal points in the string, which are permanently at rest. Hence the energy remains "standing" in the string, although it alternates between vibrational kinetic energy and elastic potential energy." So the idea is valid for a simple harmonic oscillator in which there are no losses. In such a case, once the system begins oscillating, no further input of energy is required in order to maintain oscillation. Clearly there is no flow of energy into or out of such a system. What is clear is that energy doesn't pass through the nodes. It is less clear that there exists an inherent mechanism which prevents the movement of energy. And so it appears in cases where there is no transfer of energy that one might claim that waves bounce off of one another. There are no other examples, and no supporting mechanism for it of which I am aware, and so one might be equally justified in claiming that waves pass through each other in all cases. 73, ac6xg |
Standing-Wave Current vs Traveling-Wave Current
Keith Dysart wrote:
Good answers. Exactly as I expected. Now please explain the applicability of EM waves to the state of an open circuited line excited with a step function, especially after it settles to a constant voltage (where only an E field will be present). Before it settles to a constant voltage, there is acceleration of electrons that results in an EM photonic wave. After it settles to a constant voltage, there is no acceleration of electrons and the EM photonic wave disappears. Please see Maxwell's equations for further enlightenment. -- 73, Cecil http://www.w5dxp.com |
Standing-Wave Current vs Traveling-Wave Current
On Jan 3, 1:48*pm, Cecil Moore wrote:
Keith Dysart wrote: Can photons explain the state of a transmission line driven with a step function after the line has settled to a constant voltage? Of course, photons can be used to explain all EM wave action. A step function accelerates electrons which then emit photons as EM waves. Hint: electrons cannot move at the speed of light. EM waves move at the speed of light. Please describe the final state of the step excited open circuited line using photons. Thanks, Keith |
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