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#1
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One word answers...
Owen Duffy wrote in
: You could devise an example with an AC source that had exactly the same outcome, more complicated mathematics to solve it, but the exactly the same outcome. But you don't need to do that, the example is in the set of the general, and stands against a general statement that power reflected from a source is necessarily dissipated in the source. This wasn't so well written, let me move a word around: You could devise an example with an AC source that had exactly the same outcome, more complicated mathematics to solve it, but the exactly the same outcome. But you don't need to do that, the example is in the set of the general, and stands against a general statement that reflected power from a source is necessarily dissipated in the source. Owen |
#2
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One word answers...
Owen Duffy wrote:
You could devise an example with an AC source that had exactly the same outcome, more complicated mathematics to solve it, but the exactly the same outcome. But the point is that I can devise an example with an AC source that has the opposite outcome simply by using a Norton equivalent source. When the reflection arrives, the dissipation doubles. -- 73, Cecil, w5dxp.com |
#3
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One word answers...
Cecil Moore wrote in news:KGhKh.7646$yW.5893
@newssvr11.news.prodigy.net: Owen Duffy wrote: You could devise an example with an AC source that had exactly the same outcome, more complicated mathematics to solve it, but the exactly the same outcome. But the point is that I can devise an example with an AC source that has the opposite outcome simply by using a Norton equivalent source. When the reflection arrives, the dissipation doubles. Your Norton equivalent doesn't pretend to replicate my (real) source in every way, it only pretends to supply the same voltage and current to its load... and it does that. Owen |
#4
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One word answers...
Owen Duffy wrote:
Your Norton equivalent doesn't pretend to replicate my (real) source in every way, ... I thought we were discussing general principles, not replicating a special case example in every way. -- 73, Cecil, w5dxp.com |
#5
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One word answers...
Owen Duffy wrote:
Cecil Moore wrote in news:96hKh.483$rj1.92 @newssvr23.news.prodigy.net: Owen Duffy wrote: Are the principles that apply to this example inconsistent with the general case (eg dc, ac, transient, steady state etc)? Of course, pure DC principles are not adequate to cover general case distributed network problems. Else, there The principles are those of the behaviour of transmission lines and the theory applying to solving the source circuit. In the 'DC' case, the analysis becomes trivial, but IMHO there were no underlying principles that do not apply in the general case. But your underlying principle is that the source steps and doesn't change. So any general case where the source is at some different level is now not covered. Best, Dan. |
#6
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One word answers...
Dan Bloomquist wrote in news:xYhKh.5014$ya1.2122
@news02.roc.ny: But your underlying principle is that the source steps and doesn't change. So any general case where the source is at some different level is now not covered. It semantics Dan, the excitation is part of the scenario or example, it is not a principle of circuits or transmisssion lines. Owen |
#7
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One word answers...
Owen Duffy wrote:
Dan Bloomquist wrote in news:xYhKh.5014$ya1.2122 @news02.roc.ny: But your underlying principle is that the source steps and doesn't change. So any general case where the source is at some different level is now not covered. It semantics Dan, the excitation is part of the scenario or example, it is not a principle of circuits or transmisssion lines. Like saying the impedance of a capacitor is the same no matter what the frequency...... From here, I'll let you have the last word. I'm not into hand waving.... Owen Best, Dan. |
#8
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One word answers...
Owen Duffy wrote in
: .... When the switch is closed, current flows into the line. Until t=2T seconds, the current If that flows into the line equals 100V/(100+100 ohms) = 0.5A, during which time the resistor dissipates heat at the rate of I^2*R = 100W. The voltage of the wave Vf travelling from the source is I*Zo = 50V. This situation is constant until t=2T seconds. .... David Ryeburn is awake, even if I wasn't at 5.38 when I wrote this. should be ...during which time the resistor dissipates heat at the rate of I^2*R = 25W... It doesn't materially change anything, but I messed up! Owen |
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