Rotating a laser beam faster than light?

Click For Summary

Discussion Overview

The discussion centers around the concept of rotating a laser beam and whether the spot created by the laser can move faster than the speed of light. Participants explore theoretical scenarios involving lasers, rotating objects, and the implications of relativity on the movement of light and information transfer.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that rotating a laser beam could cause the spot to travel faster than light, particularly when considering vast distances.
  • Others argue that while the angular movement of the laser can point to different locations quickly, the actual movement of the light spot does not exceed the speed of light due to the nature of light propagation.
  • There is mention of the lighthouse paradox, where a sweeping beam does not transfer information faster than light, as the beam itself does not carry tangible information from one point to another.
  • Some participants question the definition of "information" in this context, suggesting that it relates to knowledge that can be conveyed or received.
  • A hypothetical scenario involving a metal disc with a radius of a billion light years is raised, questioning whether its outer edge could rotate faster than light.
  • Concerns are expressed about the nature of photons and whether they possess any tangential velocity in addition to their radial speed.
  • Participants discuss the implications of rigid objects in relativity, noting that no rigid object can exist theoretically, which affects the discussion of rotating bodies.
  • Some participants clarify that the light beam does not actually curve but suggest that the perception of movement can lead to misunderstandings about its behavior over large distances.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the movement of the laser spot and the implications of relativity. There is no consensus on whether the spot can move faster than light, and the discussion remains unresolved.

Contextual Notes

Limitations include the dependence on definitions of information and the theoretical nature of the scenarios discussed. The discussion also highlights the complexities of light behavior and the assumptions made about rigid bodies in relativistic contexts.

  • #91
My apologies. I should have worded that better. My question isn't about the intensity, nor arrival timing of photons, nor how far photons can travel.

You said that for an "individual photon ... E=h/f"
I assumed you meant E(individual photon) = h / f. Is that correct?
If that is correct it would imply that one cycle of light through a point (or a wavelength) corresponds to a self-contained single photon.
 
Physics news on Phys.org
  • #92
gonegahgah said:
I assumed you meant E(individual photon) = h / f. Is that correct?

That is correct.

If that is correct it would imply that one cycle of light through a point (or a wavelength) corresponds to a self-contained single photon.

No, it doesn't. Why would you think it does?
 
  • #93
Fredrik said:
Yes, it's incorrect. In the original rest frame, the rocket keeps getting shorter due to Lorentz contraction. This means that the front and rear can't have the same acceleration profile. The rear must accelerate faster than the front for the rocket to get shorter. What a clock measures is the integral of \sqrt{dt^2-dx^2} along its world line, and since the rear is accelerating faster, the integral along its world line gets a bigger contribution from the dx2 term. Because of the minus sign in front of it, that makes the integral smalller. That's why the clock in the rear will be behind the clock in the front.

Fredrik --thanks for your responce but I am still confused.
As I understand it, the desynchronuzation of clocks is responcible for the invariance of the measured speed of light? The only way this seems to make sense is if the clocks at the rear are running ahead of the clocks in front. Ie: showing a later time.
This seems to mean that if you have distributed , synchronized clocks in a rest frame and then accelerate the frame , the clock in the rear would end up running ahead of one in the front. Does this make sense or am I seriously missing something??
 
  • #94
gonegahgah said:
You said that for an "individual photon ... E=h/f"
I assumed you meant E(individual photon) = h / f. Is that correct?
If that is correct it would imply that one cycle of light through a point (or a wavelength) corresponds to a self-contained single photon.
Why would it imply that? Can you explain your reasoning?
 
  • #95
Austin0 said:
As I understand it, the desynchronuzation of clocks is responcible for the invariance of the measured speed of light?
I don't know if it works that way, i.e. if you can prove the invariance using only what we know about desynchronization of clocks attached to the same solid object. Maybe you can, but it seems to be an unnecessarily complicated way to think about it. I think of SR as a physical theory that consists of a mathematical model (Minkowski space) and a set of postulates that identifies things in the model with things in the real world. The metric can be used to derive anything about the model, so I'd rather say that the Minkowski metric is the cause of both desynchronization and invariance.

Anyway, Einstein's second "postulate" says that the speed of light is the same in all inertial frames. It's not the same in arbitrary coordinate systems.

Austin0 said:
The only way this seems to make sense is if the clocks at the rear are running ahead of the clocks in front. Ie: showing a later time.
I don't see why.

Austin0 said:
This seems to mean that if you have distributed , synchronized clocks in a rest frame and then accelerate the frame , the clock in the rear would end up running ahead of one in the front. Does this make sense or am I seriously missing something??
If the red "this" refers to what I said, then the red "ahead" should be "behind". Anyway, if you take a grid of rulers and synchronized clocks and accelerate them by starting a tiny rocket attached to each clock when they all show the same time, and then shut them off when they have reached velocity v in the original rest frame, then they will be doing inertial motion again, but they won't be synchronized, so the numbers you can read off the grid won't agree with the coordinates assigned by an inertial frame.
 
  • #96
JesseM said:
Why would it imply that? Can you explain your reasoning?

Well, you said that E=hc/λ.
I assume you were transfering that through (by the progression of the paragraph) as meaning E(individual photon) = hc/λ. So constant divided by wavelength.

I read your words and this to say that one photon = one wavelength. If the photon were multiple wavelengths joined end to end then the total energy of an individual photon would be (number of wavelengths) * hc / λ as the equation implies that it is per wavelength.

Maybe you could clarify it for me by showing how you would work out how many photons arrived given the energy and time.
 
  • #97
russ_watters said:
Expansion: Again, think of the rod as a spring. If you accelerate the rod, it will shorten the way a spring does until the force of the coiled spring equals the force of the acceleration and the pressure wave of the start of the acceleration propagates through it. Then it will continue to accelerate as a shortened rod.
___________________________________________________________________________
Hi One question.
Given that the rate of propagation [speed of sound] is very slow compared to intermolecular elastic reactions , wouldn't both the force and the compression move as a reciprocal occilation with no net compaction or actual motion at the point of acceleration until the whole system attained sufficient energy to begin moving as a body?

In the spring context; Wouldn't continuous acceleration result in continued expansion /compression of the spring with the force of acceleration never reaching equilibrium with the intermolecular tensile force in a state of maximum compression?

This is assuming that the magnitude of the force does not exceed the systems ability to distribute it fast enough.

This is a question I have mulled over before in other contexts so would appreciate any clarification.
 

Similar threads

  • · Replies 90 ·
4
Replies
90
Views
4K
  • · Replies 128 ·
5
Replies
128
Views
7K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 26 ·
Replies
26
Views
2K
Replies
15
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 52 ·
2
Replies
52
Views
6K