Home |
Search |
Today's Posts |
|
#1
![]() |
|||
|
|||
![]()
On Thu, 17 Apr 2008 18:43:41 GMT
Cecil Moore wrote: Roger Sparks wrote: Yes, in nature the returning power will affect the frequency of the source. If the reflected wave is a sine wave coherent with the forward wave, why would the frequency change when they are superposed? I grant that the case for true frequency change was overstated. There is a one time phase change, causing a frequency "bump" for one cycle. This phase change is a one time event, occuring for each successive and diminishing reflected wave. GND--Vs--x--Rs--------45deg 50 ohm----short 100v 50ohm This circuit has an impedance of 73.5 + J44.1 ohms at the point x. Energy sinking into the source occurs during the cycle. It is not an illusion. I got a different impedance value but for purposes of discussion, all that matters is that the impedance is NOT 50 ohms. Right, in my haste, I picked up the impedance for a 12.5 ohm load. Sorry. The impedance should be 50 + 50j ohms. Let's assume your impedance is correct. That means the ratio of reflected power to forward power at point 'x' is 0.1452 in the 50 ohm environment. Why would reflected energy flowing back through the source be considered "energy sinking". Why cannot the reflected energy flow back through the source unimpeded by the 0+j0 impedance and be reflected by the short to ground on the other side? That same thing happens all the time to standing wave current on the outside of the coax braid. Why do the laws of physics change inside a source? It is the arbitrariness that I object to. As you say, you chose 50 ohms to calculate the reflection factor. So we have a 50 ohm transmission line zero length long, reflecting from a short circuit. This does nothing for us. We still have the source absorbing power, but now we have now added a mechanism for how the absorbed power behaves within the source. In this example, we are delivering 100 watts to Rs. With a power reflection coefficient of 0.1452, the forward power has to be 117 watts making the reflected power equal to 17 watts at point 'x'. That reflected power of 17 watts is not absorbed by the source. It flows back through the source, unimpeded by the 0+j0 impedance, and is reflected by the short to ground. It joins the 100 watts being generated by the source to become the forward wave of 117 watts. No absorbing of energy required - just good old distributed network physics. Once this 17 watt wave is tracked back through the source, reflected, and superposed with the 100 watts being generated by the source, all will become clear without any power absorption by the source being necessary. Here's a diagram of what's happening. 100w 100w GND--------Vs----------Rs--------45deg----------short 17w-- 117w-- 50w-- --17w --17w --50w All energy flows balance perfectly and there is no absorption by the source. -- This is much too arbitrary for me. -- 73, Roger, W7WKB |
#2
![]() |
|||
|
|||
![]()
Roger Sparks wrote:
This is much too arbitrary for me. It's not arbitrary at all - it's the result of very carefully chosen boundary conditions including specifying a 100% 50 ohm system with ideal components. It agrees with Roy's posting about ideal source impedances and short-circuits. The bottom line is: If the distributed network model is used to the right of Rs, it must also be used to the left of Rs. Once the distributed network principles are applied to the source, the results are the posted values. Since no other values are possible, it is certainly not arbitrary. What *is* arbitrary is willy-nilly using the distributed network model for part of the network and using the lumped circuit model for the other part. I have updated the diagram to the values that I calculated for the shorted 45 degree line. 100v 50ohm 45deg GND--------Vs----------Rs--------50ohm----------short 25w-- 125w-- 50w-- --25w --25w --50w The net voltages and currents are the result of the superposition of the component voltages and currents. The forward and reflected power readings are what an ideal directional wattmeter would indicate. -- 73, Cecil http://www.w5dxp.com |
#3
![]() |
|||
|
|||
![]()
On Fri, 18 Apr 2008 10:57:24 -0500
Cecil Moore wrote: Roger Sparks wrote: This is much too arbitrary for me. It's not arbitrary at all - it's the result of very carefully chosen boundary conditions including specifying a 100% 50 ohm system with ideal components. It agrees with Roy's posting about ideal source impedances and short-circuits. It is arbitrary because when using the short circuit model, you limit the discussion to only one example of transmission line termination--the example of a low impedance on one end of the line and a higher impedance on the other. As you well know, two additional examples of transmission line termination are possible--the transmission line impedance is higher (or lower) than the termination at either end. It is also arbitrary because the reflected wave information is useless. Any reflection from the source is folded into the sine wave to form one wave, which becomes the forward wave. The only real accomplishment from the exercise to to shift the frequency for a one cycle "bump", and that accomplishment does more to introduce confusion than contribute to better understanding. -- 73, Roger, W7WKB |
#4
![]() |
|||
|
|||
![]()
Roger Sparks wrote:
It is arbitrary because when using the short circuit model, you limit the discussion to only one example of transmission line termination ... It is not arbitrary - it is what it is. All of the source impedance, Rs, is separated from Vs. That leaves only a 0+j0 dead short impedance possible for the series source. If it was some other value, the distributed network model would still work. Any reflection from the source is folded into the sine wave to form one wave, which becomes the forward wave. Yes, in exact accordance with the distributed network model. What it means is that the source is not delivering the folded-in reflected energy at the time the reflected energy joins the source signal. Since I don't see that energy in Keith's equations, chances are that is why they didn't balance. -- 73, Cecil http://www.w5dxp.com |
#5
![]() |
|||
|
|||
![]()
On Sat, 19 Apr 2008 13:02:08 GMT
Cecil Moore wrote: Roger Sparks wrote: Any reflection from the source is folded into the sine wave to form one wave, which becomes the forward wave. Yes, in exact accordance with the distributed network model. What it means is that the source is not delivering the folded-in reflected energy at the time the reflected energy joins the source signal. Since I don't see that energy in Keith's equations, chances are that is why they didn't balance. -- You are missing an important observation here. When the energy from the reflected wave folds into the forward wave, any further analysis is a replication of the first analysis. Nothing new is learned. I think what you want to see is a source matched to the load, so that all the energy flows one way, to the resistor Rs. Your proposal is to allow/force reflectons from the source Vs so that effectively, the resistor Rs becomes the only load. This is then a demonstration/proof for what? -- 73, Roger, W7WKB |
#6
![]() |
|||
|
|||
![]()
Roger Sparks wrote:
You are missing an important observation here. When the energy from the reflected wave folds into the forward wave, any further analysis is a replication of the first analysis. Nothing new is learned. I'm posting steady-state values. If it is already steady-state, nothing new is needed. The point is that some of the steady-state forward energy is not being delivered by the source. Your proposal is to allow/force reflectons from the source Vs so that effectively, the resistor Rs becomes the only load. No, the resistor Rs is not the only load. The resistor plus the rest of the network is the load. With a 45 deg shorted stub the load is 50+j50 as you previously reported. -- 73, Cecil http://www.w5dxp.com |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Now for the rest of the story! | General | |||
Now for the rest of the story! | Policy | |||
Now for the rest of the story! | General | |||
Now for the rest of the story! | Policy | |||
WTD: Paul Harvey Rest of the Story broadcasts from Sep 1 thru 6 | Broadcasting |