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Length contraction of falling things |
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| Jun21-12, 09:01 AM | #35 |
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Length contraction of falling thingsSay for a cubical cavity resonator, resolve cavity field into three mutually orthogonal sets of counterpropagating travelling waves. Two sets propagating transverse to radial direction, one along that axis. Sets need not be equal amplitude. It should be obvious the two transverse sets have no appreciable coupling to the only conceivable factor that hauling-up process could bring to bear as locally measured - a changing gravity/tidal gravity. In the radial set case, it is equally obvious whatever is conceivably gained/lost by a travelling wave component in one direction is reversed during the other half trip. Perhaps for an exceedingly rapid 'snatch' process a tiny disequilibrium would occur, but up to critics to prove that matters here imo. And incidentally this kind of thing can be extended to say a box full of hot gas or whatever - there is no reason to suppose any such form of trapped energy acts differently to a dead lump of rest mass. Assuming varying gravity/tidal gravity is all there is to consider. And yet...... There is a possible caveat, stemming from my own earlier considerations in a thread dealing with angular momentum of a flywheel lowered into a potential well. We had assumed the flywheel's own angular momentum was invariant wrt potential, a reasonable assumption in keeping with conservation of angular momentum. Yet from a Machian pov that seems suspect. Time dilation demands that the coordinate determined spin-rate declines with lowering potential, and this in turn naively implies an increased coordinate flywheel mass to compensate. Problem is that would conflict with the two assumptions that rest mass/energy declines with lower potential and that EP holds true (inertial mass = active gravitational mass = passive gravitational mass). A redefinition of angular momentum in gravity well is thus necessary to at all reconcile these factors. There is however an additional possibility - that angular momentum becomes progressively redistributed between flywheel proper and the rest of the gravitating mass system. Which is in keeping with the Machian position that inertia is a mutual effect between all mass/energy. Thus build a shell of mass around a flywheel and it's coordinate spin-rate declines, but one must expect an action of flywheel's motion back on the shell. And that seems at least roughly in line with a strictly GR 'frame dragging'. One might then conclude a varying gravitational and/or gravitational tidal force is not the only possible influence on 'light in a box'. So yes I'm having it a bit both ways here!
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| Jun21-12, 09:24 AM | #36 |
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Different people have different definitions they like, and they often will say (as the Okun paper that harrylin mentioned does--btw, harrylin, do you have a link to the paper itself?) that other definitions besides theirs are "misleadinng" or some such. The key thing IMHO is to remember that in GR, "energy" is not a fundamental concept; it's a way of interpreting the physics, but you don't need it to actually calculate what happens. You can calculate everything using covariant geometric objects like vectors and tensors, which have unambiguous definitions and behave in well-defined, unambiguous ways.For example, take the photon free-falling radially towards a gravitating body. It has a 4-momentum vector [itex]p^{a}[/itex] which is parallel transported along its worldline. Since parallel transport is one common way in GR of defining what it means for a geometric object to "not change" along a curve, this implies that the photon's 4-momentum does not change. And since the norm of the 4-momentum can be defined as the "energy at infinity" of the photon, some people interpret this as saying that the energy of the photon does not change. However, the energy that the photon will be *observed* to have depends on the 4-velocity of the observer, via the equation: [tex]E_{obs} = g_{ab} p^{a} u^{b}[/tex] Even if we interpret what I said above as [itex]p^{a}[/itex] not changing as the photon falls, [itex]g_{ab} u^{b}[/itex] *will* change, in general, for different observers. In particular, it will change for static observers at different altitudes, who will therefore observe the photon to have different energies, and therefore different frequencies, i.e., gravitational redshift/blueshift. Some people interpret this as saying that the energy of the photon *does* change. Which interpretation is "right"? Does it matter? It depends on what you are using the interpretation for. Both interpretations agree on the actual physical observables, so as far as physics is concerned, they're equivalent. One may lead to more understanding and less confusion for some people, in some situations. But IMHO that's not a question of physics. |
| Jun21-12, 11:00 AM | #37 |
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| Jun21-12, 11:34 AM | #38 |
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| Jun21-12, 11:37 AM | #39 |
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Perhaps you meant a link to a freely downloadable (=pirated) version, but no I don't have that. On the other hand, a personal message can have good results (hint). ![]() |
| Jun21-12, 02:08 PM | #40 |
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| Jun21-12, 03:37 PM | #41 |
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| Jun21-12, 03:57 PM | #42 |
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Could you elaborate on the assumption that "rest mass/energy declines with lower potential " ? |
| Jun21-12, 04:58 PM | #43 |
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![]() Perhaps it's better to give a crystal clear example: Put an atomic clock in a high tower and synchronise1 it with the ECI frame, as is commonly done. Tune a crystal oscillator to exactly 1.000 GHz with that atomic clock as reference, and use it for a radio emitter. There is a similarly tuned atomic clock and a radio receiver with frequency analyser on the ground. Send during exactly 24h a 1.000 GHz radio signal to the ground, 500 m below. According to GR the received signal as read on the frequency analyser will be exactly 1.000 GHz and the emission time exactly 24 h (in an ideal2 situation). That should be clear and obvious to everyone. Harald ADDENDUM, notes: 1. tune it to run in sync, as is commonly done for time keeping 2. also overlooking that the ECI frame isn't perfectly inertial |
| Jun21-12, 05:04 PM | #44 |
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PeterDonis:
In any case, I had been thinking that slowly raising photons from varying gravitational potential depths would result in a different characteristic of light at the surface versus them following null geodesics as when freely emitted; that some changes in characteristics would result. Can you comment about what you think happens? |
| Jun21-12, 05:21 PM | #45 |
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![]() And I think that we have largely covered the topic of this thread. |
| Jun21-12, 07:06 PM | #46 |
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| Jun21-12, 07:08 PM | #47 |
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| Jun21-12, 07:46 PM | #48 |
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So here's what happens in the box that contains light and is being lifted:
Let us examine light in a mirror lined box, which is being lifted at a constant coordinate speed. The coordinate speeds of the ceiling mirror and the floor mirror are the same. The coordinate speeds of the light near the ceiling and the light near the floor are different. Now we must study Doppler shift. When an EM-wave pulse and a mirror collide, the mirror receives wave crests at average frequency: the number of crests in the wave / time that the collision lasts Now, in the Doppler shift effect there is no change of number of wave crests in a wave pulse, so the change of the duration of the collision between the wave and the mirror is the thing that determines the Doppler shift. An observer who is staying at constant altitude, and observing our box being lifted, says that near the ceiling the light has a larger coordinate speed, and therefore the duration of the collision between the ceiling mirror and the light is determined by the motion of the light in a greater degree as compared to the collision between the light and the floor mirror, so near the floor mirror the duration of the light-mirror collision is determined by the coordinate speed of the mirror in a greater degree, as compared to the situation near the ceiling. So this observer at constant altitude says that light blue shifts, when being reflected from the floor mirror, more than it red shifts when reflected from the ceiling mirror, and therefore the observer observes a frequency increase of the light. |
| Jun21-12, 09:29 PM | #49 |
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| Jun21-12, 09:40 PM | #50 |
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![]() First of all, when you say "synchronise it with the ECI frame", I assume you mean not just adopting the standard of simultaneity of the ECI frame, but also its clock rate, correct? In other words, you are artificially setting the frequency of *both* oscillators, at different heights, to different clock rates than they would normally run at, similar to what is done with the clocks on board the GPS satellites. Only if you do this does your prediction of unchanged "frequency" with height make sense. But of course this "frequency" that you are saying does not change with height is really a "coordinate frequency", not a "proper frequency"; it's not the "natural" frequency that at least one of the oscillators (and probably both) would measure if you hadn't artificially set them to the ECI clock rate. In other words, you are artifically tuning each oscillator so that the "frequency" that it measures is *not* the "natural" frequency that would be measured by an observer with the same 4-velocity. The "effective" 4-velocity of the oscillator for purposes of measuring frequency, what you would contract with the 4-momentum of the photon to compute its observed frequency, is some *other* 4-vector, a 4-vector that is associated with "coordinate time" in the ECI frame. All of which illustrates that it's tough to be clear, even when you are really trying to be.
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| Jun21-12, 09:50 PM | #51 |
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The simplest assumption is that the walls of the box are perfectly reflecting mirrors; this means that each collision of a photon with a box wall can be modeled as perfectly elastic, with the photon's momentum perpendicular to the box wall reversing direction (and a corresponding change in the momentum of the box). In another thread I used this type of model to describe how one could extract work from a box filled with photons by slowly lowering it instead of letting it freely fall, and how extracting the work would lower the "photon temperature" inside the box, whereas a freely falling box of photons would have the same "photon temperature" inside as it fell (relative to the box, in both cases). But in either case, the "average" motion of the photons inside the box is no longer null, but timelike--it's just the motion of the center of mass of the box+photons. One could try more complicated models, but I'm not sure what the point would be. The key point is already clear from the above simple model: the behavior of light inside a box, when the interaction with the box is included, does change. |
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