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On Jun 13, 12:00*am, Cecil Moore wrote:
On Jun 12, 4:34*pm, K1TTT wrote: ok, so you defined a case where the superposition of the reflected and refracted waves at a discontinuity results in a zero sum. *is that supposed to prove something? *did i ever say that you could not define such a case?? I would call two waves superposing to zero indefinitely, "wave cancellation". If that is not wave cancellation, where did the reflected and refracted wavefronts go along with their energy components? The answer to that question will reveal exactly what happens to the reflected energy. i don't care, i know that the superimposed voltage or current is zero. from that i can calculate the power or energy anywhere i want. why does anyone care about 'energy' anyway, that is even worse to think about in transmission lines than power. at least you can measure, or at least calibrate your meters, in power units. have you ever seen an amateur station that had an energy meter on their transmitter? and isn't the term 'reflected energy' kind of an oxymoron anyway? for energy to be reflected it has to be moving, so isn't that just another word for power? Here's a brain teaser for you and others. Given a Z01 to Z02 impedance discontinuity with a power reflection coefficient of 0.25 at the '+' discontinuity: ------Z01------+------Z02-------load Pfor1 in the Z01 section is 100 watts. Pref1 in the Z01 section is zero watts. What is Pfor2, Pref2, and the SWR in the Z02 section? -- 73, Cecil, w5dxp.com so? what does this special case prove that hundreds of others doesn't? |
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