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On Jun 14, 9:00*pm, walt wrote:
In his Nov 1991 QST article Warren Bruene, W5OLY, used what I believe is a similar procedure, in which he claims he measured the Rs that he called the 'source impedance' of the RF amp. *He used his measurements in asserting that because his Rs didn't equal RL there could be no conjugate match when the source is an RF power amp. I have never believed his procedure and measurements were valid, and I still don't. IMO, the error that Bruene made is similar in concept to the some of the errors being made here in this thread. Many people assume that a simple reflection is the only way to change the direction and momentum of an EM wave in a transmission line. In "Reflections", Sec 4.3, Reflection Mechanics of Stub Matching, you describe the role of wave cancellation associated with interference as a mechanism for redistributing reflected energy back toward the load. You said, "Wave interference between these two complimentary waves at the stub point causes a cancellation of energy flow in the direction toward the generator." It seems obvious to me that your "virtual short" reflection at a Z0-match point is a combination of ordinary wave reflection and interference patterns adding up to zero energy flowing toward the source. Obviously, interference can also happen inside a source. Redistribution of energy can occur associated with destructive/ constructive interference inside the source and has an effect on the V/ I ratios, i.e. on the impedances. Bruene's pinging method completely ignores the role of interference at the source. The Z = (Vfor+Vref)/ (Ifor+Iref) impedance for coherent waves may be a completely different value than for the non-coherent pinging waves. -- 73, Cecil, w5dxp.com |
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