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On Dec 1, 9:25*am, Lostgallifreyan wrote:
Art Unwin wrote in news:15904250-69bb-4aba-8a3f- : If you go back to the arbitary boundary of the Gaussian law of statics and view it as a Faraday shield it all becomes quite simple. If one adds a time varying field you have the duplicate of Maxwells laws for radiation, *where the outside of the boundary is the radiator. The Faraday shield supplies the transition from a static to a dynamic field for xmission and the reverse action *for receiving. Very basic my dear Watson, and a vindication that particles and not waves create radiation which puts it in line with deductions when other methods are applied. Doesn't look basic, and I suspect it never will to me. The only thing I can get from this is the idea that a particle model will do what the wave one does, which isn't surprising but I've been told that particle based models are usually best left to situations (usually atomic scale quantum mechanical) where the wave model won't do, and I've never seen anyone suggest that wave-based theories of electromagnetics were inadequate (or inefficient) for scales involving obviously large numbers of particles. The other explanations seemed to grip, but not this one. I'll leave well alone now, but if anyone else takes up the discussion, I'll read it and only comment if I can't stop myself.. Yep, that's about right. In fact, my advice if you do get into that situation (where quantization of energy is important), is to NOT think of particles or waves, but realize that quanta of electromagnetic radiation behave exactly as they behave, which is neither exactly like waves nor exactly like particles. One of Richard Feynman's physics lectures covered what I think is a lovely example of this: how you can NOT explain the results of the experiment he sets up, using EITHER wave OR particle behaviour. I highly recommend it, to arm yourself against people who get into the particle-vs-wave battle. I believe it's the sixth of what has been published as Feynman's "Six Easy Pieces." Cheers, Tom |
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On Dec 3, 12:25*am, Lostgallifreyan wrote:
( Richard Feynman lectures) ... I don't know if he's written anything a layman can easily work through, that doesn't come with lots of maths without which accompanying text doesn't help much, but if he has I'll try to read it. I think one of the key things that made his physics lectures popular is that they were delivered without a whole lot of math. You could get into that if you wanted, but you could also get a lot out of just listening to the _ideas_. If you drop me an email, perhaps I can send you a bit more about this particular lecture... Cheers, Tom |
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On Dec 3, 6:52*pm, K7ITM wrote:
On Dec 3, 12:25*am, Lostgallifreyan wrote: ( *Richard Feynman lectures) ... I don't know if he's written anything a layman can easily work through, that doesn't come with lots of maths without which accompanying text doesn't help much, but if he has I'll try to read it. I think one of the key things that made his physics lectures popular is that they were delivered without a whole lot of math. *You could get into that if you wanted, but you could also get a lot out of just listening to the _ideas_. If you drop me an email, perhaps I can send you a bit more about this particular lecture... Cheers, Tom That is oh so true! The masters started with an observation of an occurence and not from a rendering of mathematics. With more observations it became natural to align the Universe via mathematics which, as with a jig saw puzzle, fits together nicely., It would seem today that scientists today are using mathematics via a computer to churn out bundles of equations leaving the operator to think of an observation that would fit the math. Of course, mathematics provide imaginary answers similar to a quadratic equation that finish up as multiple of false leads and deductions which eventually requires the multiple use of constants to provide a semblance of understanding of what has been provided. |
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