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On Jun 1, 1:52*pm, Cecil Moore wrote:
On Jun 1, 8:10*am, K1TTT wrote: what exactly is the 'interaction' *and why is it unique to that special coherent, collimated, etc, case? Is it not obvious that when two reflected waves cancel in one direction, as at the surface of a 1/4WL thin-film coating on glass, and their combined EM energy is redistributed in the opposite direction, that those two waves have interacted, i.e. have suffered a permanent change and have lost their original identities? Is it not obvious that when two waves are traveling two different paths where the incident angle is, e.g. two degrees, that those two waves will superpose and interfere throughout a certain space after which they emerge intact, unaffected, and have obviously not interacted, i.e. they suffered no permanent change and have maintained their original identities? no, it is not obvious. where do you draw the line... 1 degree, .1 degree, .001 degree? at what point is the angle small enough to say that they have 'interacted' and the energy is redistributed? Did superposition occur in both cases? Yes. Did interference occur in both cases? Yes. Did wave cancellation occur in both cases? No, just in the non-reflective glass case. i propose that 'cancellation' is just a special case of interference where the waves are 'close enough' to collinear that you never see the interference pattern. this would of course always apply in a transmission line because they are confined. closely analyze the transient response of your non-reflective glass in the case where the wave is not incident perpendicular to the glass. do each reflection from each interface separately as the wave travels in the coating at an angle. then reduce the angle to very near perpendicular and you should see that there are indeed reflections that should very nearly 'cancel' each other out as the number of reflections gets bigger. |
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