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#71
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Derivation of Reflection Coefficient vs SWR
On Feb 8, 9:15*am, Cecil Moore wrote:
Keith Dysart wrote: When we analyze this circuit we find that there is no voltage re-reflection when the wave gets back to the generator. This is clear because Vf does not change, which it would have to do if any of Vr was re-reflected. Nope, Vf doesn't have to change for there to be a reflection. Looking at what happens to the power dissipation in the source resistor, Rs, when the reflected wave arrives, we see that the energy being supplied by the source drops by 99.85%. Most of the energy in the forward wave is supplied by the reflected wave, starting at the time the reflected wave arrives and causes destructive interference. And yet it appears that you are claiming that power is reflected at the generator. How can power be reflected if voltage is not? To be technically correct, reflected energy is redistributed back toward the load during the process of destructive interference. The conditions before the reflected wave arrives and after the reflected wave arrives are extremely different. Before the reflected wave arrives, the source resistor, Rs, is dissipating 25 watts. After the reflected wave arrives, the source resistor, Rs, is dissipating 0.03845 watts. Clearly, something drastic has happened and that is: 99.85% of the forward energy originally supplied by the source has been replaced with reflected energy being redistributed back toward the load. Because of destructive interference, reflected energy *never* flows through the source resistor, Rs, and is instead redistributed back toward the load. Nothing else is possible since the source is supplying only 1.9608 watts during steady-state. 92.3% of the forward power is not being supplied by the source during steady-state. The energy incident upon a point must equal the energy exiting the point. The energy incident upon the generator terminals is 1.92234 joules/sec from the source and 23.0777 joules/sec from the reflected wave. The energy exiting that point is 25 joules/sec. The reflected wave energy obviously reverses direction and joins the forward wave and that is what we call a "reflection". Are you sure? I thought a reflection was something that occurred at an impedance discontinuity and the magnitude of the voltage reflection was defined by Vr = Vincident * ReflectionCoefficient = Vincident * (Z2-Z1)/(Z2+Z1) and that the reflected voltage then added to any wave already travelling in that direction. But you are claiming that power can be reflected when voltage is not. I have never encountered this claim before. Are you sure? ...Keith |
#72
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Derivation of Reflection Coefficient vs SWR
Keith Dysart wrote:
Are you sure? I thought a reflection was something that occurred at an impedance discontinuity and the magnitude of the voltage reflection was defined by Vr = Vincident * ReflectionCoefficient = Vincident * (Z2-Z1)/(Z2+Z1) That's true for normal reflections which involve only one wave. Wave cancellation is a different kind of energy reflection involving two waves. The energy flow is canceled in one direction and therefore flows in the other direction. In optics, it is known as a redistribution of energy in directions that allow constructive interference. In a transmission line, there are only two possible directions so any redistribution of energy due to destructive interference can be considered to be a reflection in the opposite direction, the only direction available to constructive interference. and that the reflected voltage then added to any wave already travelling in that direction. True for a single wave reflection. For two interacting waves, the voltage in one of the waves can simply replace the voltage in the other wave. In our example, the reflected voltage simply replaces the source voltage component. But you are claiming that power can be reflected when voltage is not. I have never encountered this claim before. When the reflected wave arrives, it cancels most of the existing forward wave from the source. The reflected voltage exactly equals the canceled source voltage in our example because the source resistance is the same as the Z0 of the line. Are you sure? It is obvious that reflected energy never flows in the source resistor so it must go in the only other direction possible. Yes, I am sure. The conservation of energy principle will allow nothing else. -- 73, Cecil http://www.w5dxp.com |
#73
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Derivation of Reflection Coefficient vs SWR
Keith Dysart wrote:
Are you sure? Rs Vg Pfor--25w Vl +----/\/\/-----+----------------------+ | 50 ohm 23.08w--Pref | | 48.08w / 1.92w Vs 45 degrees \ Rl 100 cos(wt) 50 ohm line / 1 ohm 50w \ load | | +--------------+----------------------+ gnd As a matter of interest, let's return to the 45 degree line, the one to which I objected previously. The forward power and reflected power are the same as in the previous example but now the dissipation in Rs is equal to the sum of the forward power and reflected power. (It would be nice if all cases were as straight forward as this special case.) This is indeed the one special case where everything you have been saying is true. There is no redistribution of energy because there is no interference. There is no interference because at Vg, Vfor and Vref are 90 degrees out of phase. These concepts are covered in my magazine article at: http://www.w5dxp.com/energy.htm -- 73, Cecil http://www.w5dxp.com |
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