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#1
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On Jun 11, 12:09*pm, Roy Lewallen wrote:
But why would you expect the "reflected power" to have a different effect when the transmission line is a quarter wavelength than when it's a half wavelength? If reflected power is fictitious, and the number wavelengths of transmission line of any random impedance compared to the load connected to it makes no difference in the load seen by the transmitter, the output power produced by the transmitter, and the power dissipated in the far-end termination, then what is the reason you chose a 1/2 wavelength of transmission line in your quoted post? RF |
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#2
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On Jun 11, 12:29*pm, Richard Fry wrote:
If reflected power is fictitious, etc Followup: Those denying the existence of reflected signals within an antenna system may wish to view the measurement of such signals, at the link below. http://i62.photobucket.com/albums/h8...easurement.gif RF |
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#3
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On Jun 11, 12:56*pm, Richard Fry wrote:
Followup: *Those denying the existence of reflected signals within an antenna system may wish to view the measurement of such signals, at the link below. Or at this link. Scroll down to "Using Dielectric Beamsplitters to find the "missing energy" in destructive interference". http://www.teachspin.com/instruments...eriments.shtml I guarantee that every optical physicist who is reading this thread is laughing at the ignorance of the alleged RF gurus. -- 73, Cecil, w5dxp.com |
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#4
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On 11 jun, 16:27, Cecil Moore wrote:
On Jun 11, 12:56*pm, Richard Fry wrote: Followup: *Those denying the existence of reflected signals within an antenna system may wish to view the measurement of such signals, at the link below. Or at this link. Scroll down to "Using Dielectric Beamsplitters to find the "missing energy" in destructive interference". http://www.teachspin.com/instruments...eriments.shtml I guarantee that every optical physicist who is reading this thread is laughing at the ignorance of the alleged RF gurus. -- 73, Cecil, w5dxp.com Hello, here we are...! :) At the risk of naïve and conciliatory I still thinking that to some extent this is a problem of "same cat seen from different points of view". What if the question is formulated in terms apart, for example = generator responses to load differences, and by what mechanism a transmission line transforms impedances to presents to the generator those different loads? In that formulation I think there are room to simple, basic, and understandable electrical laws to account for generator behaviour and TL travelling waves interference phenomenom to account for Z transformings. From my perspective your main differences are reducible 73 Miguel Ghezzi - LU6ETJ |
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#5
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On Jun 11, 10:03*pm, lu6etj wrote:
On 11 jun, 16:27, Cecil Moore wrote: On Jun 11, 12:56*pm, Richard Fry wrote: Followup: *Those denying the existence of reflected signals within an antenna system may wish to view the measurement of such signals, at the link below. Or at this link. Scroll down to "Using Dielectric Beamsplitters to find the "missing energy" in destructive interference". http://www.teachspin.com/instruments...eriments.shtml I guarantee that every optical physicist who is reading this thread is laughing at the ignorance of the alleged RF gurus. -- 73, Cecil, w5dxp.com Hello, here we are...! *:) At the risk of naïve and conciliatory I still thinking that to some extent this is a problem of "same cat seen from different points of view". What if the question is formulated in terms apart, for example = generator responses to load differences, and by what mechanism a transmission line transforms impedances to presents to the generator those different loads? In that formulation I think there are room to simple, basic, and understandable electrical laws to account for generator behaviour and TL travelling waves interference phenomenom to account for Z transformings. From my perspective your main differences are reducible 73 Miguel Ghezzi - LU6ETJ of course, but that is no fun! |
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#6
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On Jun 11, 5:03*pm, lu6etj wrote:
From my perspective your main differences are reducible The basic argument revolves around what math shortcuts can be used to solve a particular problem vs what is actually happening in reality according to the accepted laws of physics. I agree one doesn't necessarily need to understand the laws of physics to solve a problem but one should probably know enough physics to recognize when those laws of physics are being violated by one's argument. -- 73, Cecil, w5dxp.com |
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#7
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On 11 jun, 23:26, Cecil Moore wrote:
On Jun 11, 5:03*pm, lu6etj wrote: From my perspective your main differences are reducible The basic argument revolves around what math shortcuts can be used to solve a particular problem vs what is actually happening in reality according to the accepted laws of physics. I agree one doesn't necessarily need to understand the laws of physics to solve a problem but one should probably know enough physics to recognize when those laws of physics are being violated by one's argument. -- 73, Cecil, w5dxp.com ............ of course, but that is no fun! I agree ![]() ...... As a courtesy to me, a foreigner tourist ham, would you mind stop for a brief moment your more general differences and tell me if you agree on the behavior of a Thevenin generator with a series resistance of 50 ohms in relation to changes in impedance of a lossless TL predicted by the Telegrapher's equations solutions in terms of the power dissipated on the load resistance and series resistence of Thevenin source? I am pretty serious about this: until today I could not know if you agree in that!! :) |
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#8
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On Jun 12, 4:24*am, lu6etj wrote:
On 11 jun, 23:26, Cecil Moore wrote: On Jun 11, 5:03*pm, lu6etj wrote: From my perspective your main differences are reducible The basic argument revolves around what math shortcuts can be used to solve a particular problem vs what is actually happening in reality according to the accepted laws of physics. I agree one doesn't necessarily need to understand the laws of physics to solve a problem but one should probably know enough physics to recognize when those laws of physics are being violated by one's argument. -- 73, Cecil, w5dxp.com ........... of course, but that is no fun! I agree ![]() ..... As a courtesy to me, a foreigner tourist ham, would you mind stop for a brief moment your more general differences and tell me if you agree on the behavior of a Thevenin generator with a series resistance of 50 ohms in relation to changes in impedance of a lossless TL predicted by the Telegrapher's equations solutions in terms of the power dissipated on the load resistance and series resistence of Thevenin source? I am pretty serious about this: until today I could not know if you agree in that!! :) sure, if you properly apply the telegrapher's equations and the thevenin equivalent methods. The real problem is that if you try to do that for most amateur radio transmitters the source impedance is not linear, and even worse may be time varying, which renders the thevenin equivalent source substitution invalid. Note though that in real world cases you need to use the full set of equations, usually called by engineers the 'general transmission line equations'. beware, some places may over simplify the telegrapher's equations which may make them invalid in some cases. The Telegrapher's equations (http://en.wikipedia.org/wiki/Telegrapher %27s_equations), are often considered a subset of the 'General transmission line equations (http://en.wikipedia.org/wiki/ Transmission_line) that are taught in distributed circuits and fields and waves courses in engineering schools. |
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#9
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On Jun 11, 11:24*pm, lu6etj wrote:
As a courtesy to me, a foreigner tourist ham, would you mind stop for a brief moment your more general differences and tell me if you agree on the behavior of a Thevenin generator with a series resistance of 50 ohms in relation to changes in impedance of a lossless TL predicted by the Telegrapher's equations solutions in terms of the power dissipated on the load resistance and series resistence of Thevenin source? I am pretty serious about this: until today I could not know if you agree in that!! :) Miguel, I don't think there is much disagreement about things that are easily measured, like voltage and current. One solution to the telegrapher's equations involves forward and reflected waves of voltage and current. The conventional way of handling power (energy/ unit-time) is to use the voltages and currents to calculate the power at certain points of interest. The telegrapher's equations do not tell us *why* the power is what it is and the energy is where it is. To obtain the why, one must study the behavior of electromagnetic waves. How does the energy in electromagnetic waves behave? The telegrapher's equations and Thevenin source do not answer that question. For instance: Most readers here seem to think that the only phenomenon that can cause a reversal of direction of energy flow in a transmission line is a simple EM wave reflection based on the reflection model. When they cannot explain what is happening using that model, they throw up their hands and utter crap like, "Reflected wave energy doesn't slosh back and forth between the load and the source". But not only does it "slosh back and forth", it sloshes back and forth at the speed of light in the medium because nothing else is possible. These are the people who have allowed their math models to become their religion. They will not change their minds even when accepted technical facts are presented. One response was, "Gobblydegook". (sic) There is another phenomenon, besides a simple reflection, that causes reflected energy to be redistributed back toward the load and that is wave cancellation involving two wavefronts. If the two wavefronts are equal in magnitude and opposite in phase, total wave cancellation is the result which, in a transmission line, redistributes the wave energy in the only other direction possible which is, surprise, the opposite direction. This is a well known, well understood, mathematically predictable phenomenon that happens all the time in the field of optics, e.g. at the surface of non-reflective glass. It also happens all the time in RF transmission lines when a Z0-match is achieved. Using the s-parameter equations (phasor math) at a Z0-match point in a transmission line: b1 = s11*a1 + s12*a2 = 0 = reflected voltage toward the source Square this equation to get the reflected power toward the source. These are the two wavefronts that undergo total wave cancellation, i.e. total destructive interference. b2 = s21*a1 + s22*a2 = forward voltage toward the load s22*a2 is the re-reflection. Square this equation to get the forward power toward the load. If one squares both of those equations, one can observe the interference terms which indicate why and where the energy goes. All of the energy in s11*a1 and s12*a2 reverses direction at the Z0-match and flows back toward the load. All the things that Roy is confused about in his food-for-thought article on forward and reflected power are easily explained by the power density equation (or by squaring the s-parameter equations). Ptot = P1 + P2 + 2*SQRT(P1*P2)*cos(A) -- 73, Cecil, w5dxp.com |
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#10
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On Jun 12, 2:26*am, Cecil Moore wrote:
On Jun 11, 5:03*pm, lu6etj wrote: From my perspective your main differences are reducible The basic argument revolves around what math shortcuts can be used to solve a particular problem vs what is actually happening in reality according to the accepted laws of physics. I agree one doesn't necessarily need to understand the laws of physics to solve a problem but one should probably know enough physics to recognize when those laws of physics are being violated by one's argument. -- 73, Cecil, w5dxp.com rather than worrying about basic physics, the real problem here is that analysis of a non-linear circuit is being attempted using techniques that are only valid for linear circuits. |
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