Length contraction of falling things

In summary: But I can tell you that the result would be proportional to the blue shift of the light pulse. In summary, the contraction happens because the font of the light pulse moves slower than the rear of the light pulse.
  • #71
Naty1 said:
Q-reeus: "Now lower (not free-fall drop) the same positron-electron pair down into the potential well of some gravitating mass..."

This means lower the pair and then place them at rest at some point down in the potential well? Is this different than letting the pair free fall, stopping their fall, then letting them annihilate?? I don't see how the gamma ray energy is any different at the top and bottom of the well: local observers each see the same energy locally, top and bottom, right?; but such an observer at the top will see redshift from the bottom gammas, at the bottom, blue shift from the top gammas.
No real difference in outcome Naty1 - that process is 'path independent'. Just making sure no-one unreasonably seized on any lack of specificity to infer it might have referred to annihilation during a free-fall situation (which would have resulted in a further redshift factor reduction in received frequency 'out there'). I find it pays to have a lawyer's attitude to wording on occasion!
[Oops - just to further clarify that last bit about further redshift in free-fall. Was meant to refer to that ray received by a distant observer inline with radial in-fall. There is also blueshift of the other ray and overall there would actually be no net redshift at all. I'l make a lawyer yet!]
 
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  • #72
Naty1 said:
[..] "Now lower (not free-fall drop) the same positron-electron pair down into the potential well of some gravitating mass..."

This means lower the pair and then place them at rest at some point down in the potential well? Is this different than letting the pair free fall, stopping their fall, then letting them annihilate?? [..]
I did not linger on that part... but it might have been better to not include that! I guessed that Q-reeus wanted to avoid any issues with thermal energy.
Oh OK, the reason was different, as I see now. But the conclusion remains the same, sometimes less is better. :wink:
 
  • #73
No real difference in outcome Naty1 - that process is 'path independent'.

good..forgot to ask about paths...

yeah:

I find it pays to have a lawyer's attitude to wording on occasion!

you mean always!
One tough thing about these forums is that our posts don't get objective editing before posts like a textbook does...even when the poster really knows the facts. I am writing myself an explanation of some of this and thought I really had it down...until I read my own notes the next day and realized.."oops that's not quite right' and 'fixed' it..only to discover upon checking on a third day 'oops,again, did not think about this/that issue...It makes one appreciate a clearly written textbook...though not the pirces!
 
  • #74
Originally Posted by Austin0

Does this not mean that its 4-momentum vector (energy) remains constant (stays the same)along that worldline?
DaleSpam said:
First, the four momentum is not the energy. Energy is the timelike component of the four momentum. So even if you interpret parallel transport as keeping the four momentum constant you cannot conclude that the same applies for energy.
How are you distinguishing between momentum and energy in this context. Both are just a function of frequency and the same constant (reduced Planck).
So if the momentum remains the same then the frequency must remain the same. If the frequency remains the same how could the energy vary??

DaleSpam said:
Second, it is hard to interpret parallel transport as keeping a four vector constant. If you parallel transport a vector on a closed loop it does not generally wind up in the same orientation. It is an interpretation that can be useful over small regions of spacetime where you can neglect curvature, but it can cause problems if taken too far.

Austin0
the definitions of 4-momentum and vector transport in this context.

This context being; along a geodesic. Free falling photon.

I notice you did not comment on the actual point of the post. Or the logic leading to the expressed conclusion.
 
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  • #75
DaleSpam said:
Second, it is hard to interpret parallel transport as keeping a four vector constant. If you parallel transport a vector on a closed loop it does not generally wind up in the same orientation. It is an interpretation that can be useful over small regions of spacetime where you can neglect curvature, but it can cause problems if taken too far.

Hmm, this is a good point which I hadn't considered when I was talking about parallel transport before. You're right that the effects of curvature mean that even parallel transported vectors don't "stay the same", in the sense that there is a change around a closed curve. However, parallel transport is as close as we can come to a vector "not changing" along a curve in any invariant sense; we don't have any better definition to use. Also, in the cases we've been discussing, parallel transport does at least preserve properties "at infinity", such as constant energy at infinity along a geodesic.
 
  • #76
DaleSpam said:
Where do these equations come from? I don't recognize any of them as standard SR or GR equations.
With those equations I describe what a static observer sees, when observing a light pulse that bounces up and down in a box that is being lifted.

And what the observer sees is:
1: Light moving down contracts and slows down.
2: Light moving up expands and speeds up.
3: The frequency of light bouncing off a mirror changes by an amount that is proportional to change of collision time caused by the motion of the mirror.

collision time = collision start time - collision end timeWhether falling light blue shifts or not, doesn't matter here, because the observer does not see any blue shift actually happening anyway.
 
  • #77
jartsa said:
With those equations I describe what a static observer sees, when observing a light pulse that bounces up and down in a box that is being lifted.

And what the observer sees is:
1: Light moving down contracts and slows down.
2: Light moving up expands and speeds up.
3: The frequency of light bouncing off a mirror changes by an amount that is proportional to change of collision time caused by the motion of the mirror.

collision time = collision start time - collision end time

Whether falling light blue shifts or not, doesn't matter here, because the observer does not see any blue shift actually happening anyway.
That is nice that you are sticking to your story, but none of that answers the question: where did those equations come from? I have never seen any of them. Did you read them in a manuscript that you can reference? Did you derive them from the Schwarzschild metric, or the parallel transport equation? Did you just pull them out of thin air because they sounded cool? To me, it looks like the last.
 
  • #78
Austin0 said:
How are you distinguishing between momentum and energy in this context. Both are just a function of frequency and the same constant (reduced Planck).
So if the momentum remains the same then the frequency must remain the same. If the frequency remains the same how could the energy vary??
The energy is the timelike component of the four-momentum and the momentum is the spacelike component of the four-momentum. The four-momentum of a photon is a null vector, so the spacelike components must vary together with the timelike components, as is indeed implied by the fact that they are both proportional to the frequency. All three (energy, momentum, frequency) vary together.

Austin0 said:
I notice you did not comment on the actual point of the post. Or the logic leading to the expressed conclusion.
True. I rarely reply to an entire post when I think that replying to one key misconception is sufficient (or I run out of time). I don't do it to be rude, it is just a mental "triage". If there is a short specific point that you would like me to address and I neglected, then please mention it.
 
  • #79
DaleSpam said:
That is nice that you are sticking to your story, but none of that answers the question: where did those equations come from? I have never seen any of them. Did you read them in a manuscript that you can reference? Did you derive them from the Schwarzschild metric, or the parallel transport equation? Did you just pull them out of thin air because they sounded cool? To me, it looks like the last.

I don't know what Schwartschild metrics is.

This equeation from physics book I did find very useful: time = distance / speed

There is also the inverse of time dilation factor k. That kind of takes care of the General Relativity part.EDIT: k is time dilation factor, not the inverse of it
 
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  • #80
jartsa said:
I don't know what Schwartschild metrics is.

This equeation from physics book I did find very useful: time = distance / speed

There is also the inverse of time dilation factor k. That kind of takes care of the General Relativity part.

time = distance / speed works very well in an inertial frame. In General Relativity calculating distance becomes rather involved, and the relation time = distance / speed won't work with the usual definition of speed, which is usually defined by local measurements.
 
  • #81
Naty1 said:
[..] One tough thing about these forums is that our posts don't get objective editing before posts like a textbook does...even when the poster really knows the facts. I am writing myself an explanation of some of this and thought I really had it down...until I read my own notes the next day and realized.."oops that's not quite right' and 'fixed' it..[..] It makes one appreciate a clearly written textbook..[..]!
I thought exactly the same when I clarified my example in post #43. Happily the time to edit has been increased, so that it's sometimes still possible after a night's sleep to "fix" things for the benefit of later readers :smile:
 
  • #82
jartsa said:
With those equations I describe what a static observer sees, when observing a light pulse that bounces up and down in a box that is being lifted.
[..]
3: The frequency of light bouncing off a mirror changes by an amount that is proportional to change of collision time caused by the motion of the mirror.

collision time = collision start time - collision end time [..].
Like Dalespam, I don't think so. Common theory of moving mirrors gets by fine neglecting "collision time" which is thought not to affect frequency. As I remarked in post #70, you can easily infer the frequency change from Doppler shift (qualitatively that is very easy).
 
  • #83
PeterDonis said:
[..] The simplest assumption is that the walls of the box are perfectly reflecting mirrors; [..]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 [..]
Could you find back that post by you? I ask, because now, when I went swimming, I realized that I too hastily :redface: agreed with your following explanation:
PeterDonis said:
[..] Consider a photon that bounces off the upper wall of the box, travels to the lower wall, and bounces off it. Look at this process in the instantaneous rest frame of the box, which, by our underlying assumption, can cover both "bounce" events in a single local inertial coordinate patch.

If the box is in free fall, then it can be considered to be at rest in the local inertial frame for both bounce events, so the momentum exchange of the two events cancels. So there is no energy exchange between the photons and the box.

If the box is accelerated upward, then it is moving upward for one of the bounce events. That means that there is more momentum exchanged when the photon hits the lower wall of the box than when it hits the upper wall of the box.[..]
If I now correctly understand you, here you are effectively using the equivalence principle, so that you transformed (and I'm making it more concrete) to the frame of a space shuttle with a box inside. If the box is free falling together with the shuttle then the local observation should be as in an inertial frame of SR. OK so far.

Next its gets tricky: you say that when accelerating the box upward, more momentum and thus no energy is exchanged when the photon hits the lower wall of the box than when it hits the upper wall of the box. But you did not really show this, and I'm not sure if you mean relative to the Earth (as I originally thought) or relative to the falling frame.
Relative to the falling frame, a box in rest on Earth is also accelerating, and I think that no energy should be exchanged.
And contrary to my earlier thinking, that analysis doesn't yet answer the question of moving a box to a different height whereby the box accelerates, has a speed and decelerates.
 
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  • #84
harrylin said:
Like Dalespam, I don't think so. Common theory of moving mirrors gets by fine neglecting "collision time" which is thought not to affect frequency. As I remarked in post #70, you can easily infer the frequency change from Doppler shift (qualitatively that is very easy).

By time I meant duration.

Pick A collides with 6 guitar strings during 0.1 seconds time,
Pick B collides with 6 guitar strings during 0.2 seconds time

different sound results from these two collisions
 
  • #85
jartsa said:
By time I meant duration.

Pick A collides with 6 guitar strings during 0.1 seconds time,
Pick B collides with 6 guitar strings during 0.2 seconds time

different sound results from these two collisions
Well, what can I say? :biggrin:
 
  • #86
harrylin said:
Well, what can I say? :biggrin:


When you are sawing a log, the frequency of the vibrations changes if the speed of the saw changes. If the log does its own motion that also changes the frequency, if the saw contracts or expands that changes the frequency too.

But we can calculate the frequency in a simple way:

number of saw teeth / duration of one sawing stroke
 
  • #87
jartsa said:
I don't know what Schwartschild metrics is.
Well, once you learn some GR then please come back and try your derivation again.
 
  • #88
DaleSpam said:
Well, once you learn some GR then please come back and try your derivation again.

How much does a metric really matter when we are discussing light? Light only has 2 spatial dimensions to deal with since distance for it has completely contracted. Keeping it symmetrical then requires a second time dimension at C, making it 2+2 spacetime dimensions. Relativity means symmetry, right?
 
  • #89
Cosmoknot said:
How much does a metric really matter when we are discussing light?
Since the metric is what determines which paths are null geodesics, it matters a lot. The rest of your post is really nonsense.
 
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