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07-01-2002, 07:34 PM | #21 |
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I'd be very interrsted to hear whether other phenomena seem to acquire velocity instantaneously. Gravity for example - I've read a couple of articles claiming that the effect of gravitation is instantaneous over any distance with one stating that this is necessary to for the coherenece of newtonian physics to explain how centrifugal (or is it centripetal) force is balanced by gravity. On the other hand, another article seemed to say that measurements on GPS satellites confirmed general relativity results that the time of any effect at a distance would need to take into account the different inertial frames of reference. I'm curious about magnetism also.
Cheers, John BTW the Cereneko Effect link was fascinating and pretty much made sense - if we don't have a means of detecting anything exceeding the speed of light then of course it would appear that c is an absolute limit. I've been trying to imagine if we had no knowledge of light whether physics would have concluded that the speed of sound could not be exceeded (absent clues from the sonic boom of a meteorite). Cheers, John |
07-02-2002, 03:18 AM | #22 | ||
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Boro Nut |
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07-02-2002, 03:22 AM | #23 | |
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07-02-2002, 08:21 AM | #24 |
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Yes, it is true that light travels slower in a medium such as water or air, but this has nothing to do with photons traveling faster than the speed of light. When light travels slower through a medium, it is due to the fact that the photons which make up the light are constantly being absorbed and reemitted by the atoms in the medium. It’s like having a car that instantly acquires 60 miles an hour when you hit the gas and instantly goes back to zero when you hit the breaks – you won’t waste anytime speeding up or slowing down, but you still might have to stop at traffic lights.
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07-02-2002, 08:39 AM | #25 | |
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God Bless, Kenny [ July 02, 2002: Message edited by: Kenny ]</p> |
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07-02-2002, 08:53 AM | #26 |
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One utterly useless implication of light's instantaneous acceleration is that the light you see from distant stars is liable to be the exact same "age" as it was when it was created. That's brand spankin' new light!
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07-02-2002, 08:59 AM | #27 | ||
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Kenny, I'm a little confused. You said:
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07-02-2002, 09:08 AM | #28 | |
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God Bless, Kenny |
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07-02-2002, 10:00 AM | #29 |
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Kenny:
Is this really the best way to describe it? If you really do have absorption, i.e. destruction of the photon, and re-emission, i.e. creation of a new one, how do you maintain the direction of the photon, and more importantly, its phase? |
07-02-2002, 01:03 PM | #30 | |
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<a href="http://www.wikipedia.com/wiki/refractive+index" target="_blank">http://www.wikipedia.com/wiki/refractive+index</a> Alternatively... The quantum description is given by quantum field theory of solids: The approximate Hamiltonian of the coupled system is in terms of the creation and annihilation operators of light and electron modes with interaction terms describing absorption of a photon and creation of an electron mode and vice versa. This Hamiltonian may be diagonalized by a Bogoliubov transformation replacing photon and electron operators by a linear combination of them, which may be interpreted as quasi particle operators of "polaritons", the quanta of the coupled oscillation. The dispersion relation of the polaritons is a mixture of the dispersion relations of the light and the polarization wave and is approximately linear for small wavenumbers / large wavelengths with \omega \approx ck/n while the dispersion relation for photons and electrons remains unchanged. Therefore I'd say one never measures a photon with \omega = ck/n for n \neq 1 but one could measure polaritons with this relation. (from <a href="http://www.lns.cornell.edu/spr/2001-04/msg0032182.html" target="_blank">http://www.lns.cornell.edu/spr/2001-04/msg0032182.html</a> ) I couldn't have put it better myself |
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