Is the Speed of Light Consistent Across Rotating Reference Frames?

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Discussion Overview

The discussion centers around the consistency of the speed of light across rotating reference frames, examining implications for the postulates of special relativity. Participants explore the nature of light's velocity, its components, and how these relate to different transformations in physics.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question whether the invariance of the speed of light is violated in rotating reference frames.
  • There is a discussion about dividing the speed of light into vector components, with some asserting that while the components may change, the magnitude remains invariant.
  • One participant suggests that the invariance of the interval can be used to demonstrate the constancy of light's speed across different frames.
  • Another participant raises a question about whether the second postulate of special relativity holds true under coordinate shifts that involve rotation.
  • Some argue that while all inertial frames agree on the speed of light, they may not agree on its direction due to effects like aberration.
  • A participant introduces the concept of the wave-fourvector and its transformation properties, noting that the speed of light remains constant as a null vector across frames.
  • There is a reiteration that the spacetime interval is invariant under various transformations, including rotations and Lorentz boosts.

Areas of Agreement / Disagreement

Participants express differing views on the implications of rotating reference frames for the speed of light, with no consensus reached on whether the second postulate of special relativity is upheld in such cases.

Contextual Notes

Some discussions involve assumptions about the definitions of velocity vectors and the nature of light's propagation, which may not be universally agreed upon. The mathematical steps involved in transformations are also noted as potentially unresolved.

phymath7
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TL;DR
Can we divide the speed of light into components?
Does it violate the postulate of special relativity in any sense?
 
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What do you mean by "divide the speed of light into components"? Are you referring to vector components?
 
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Yes, the velocity of light has components (x,y,z or whatever basis). The invariance of the speed of light applies to the magnitude of the velocity. The components adjust themselves accordingly.
 
Ibix said:
What do you mean by "divide the speed of light into components"? Are you referring to vector components?
Yeah, I referred to vector components.
 
jtbell said:
Yes, the velocity of light has components (x,y,z or whatever basis). The invariance of the speed of light applies to the magnitude of the velocity. The components adjust themselves accordingly.
Thanks. But a detailed work on this topic would be appreciated (from books or notes).
 
phymath7 said:
Thanks. But a detailed work on this topic would be appreciated (from books or notes).
It's easy enough - it follows from the invariance of the interval. If you have two events on the same light pulse's worldline separated by ##\Delta t## in time and ##\Delta x##, ##\Delta y## and ##\Delta z## in space, then ##c^2\Delta t^2=\Delta x^2+\Delta y^2+\Delta z^2##. You can rearrange this to get ##0=c^2\Delta t^2-\Delta x^2-\Delta y^2-\Delta z^2## and recognise the right hand side as the interval, ##\Delta s^2##, which is invariant - hence ##0=c^2\Delta t'^2-\Delta x'^2-\Delta y'^2-\Delta z'^2##, which says that the speed of light is the same in the other frame. Or if you aren't familiar with the interval, use the Lorentz transforms to eliminate the unprimed quantities from the first equation to get the last. You can also use the Lorentz transforms to transform the ##\Delta## quantities explicitly if you want to see how the light's velocity vector transforms. The x component of its three velocity is just ##\Delta x/\Delta t## and similarly for the y and z components. Likewise in the primed frame - just remember to use the primed spatial and time deltas.
 
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Ibix said:
It's easy enough - it follows from the invariance of the interval. If you have two events on the same light pulse's worldline separated by ##\Delta t## in time and ##\Delta x##, ##\Delta y## and ##\Delta z## in space, then ##c^2\Delta t^2=\Delta x^2+\Delta y^2+\Delta z^2##. You can rearrange this to get ##0=c^2\Delta t^2-\Delta x^2-\Delta y^2-\Delta z^2## and recognise the right hand side as the interval, ##\Delta s^2##, which is invariant - hence ##0=c^2\Delta t'^2-\Delta x'^2-\Delta y'^2-\Delta z'^2##, which says that the speed of light is the same in the other frame. Or if you aren't familiar with the interval, use the Lorentz transforms to eliminate the unprimed quantities from the first equation to get the last. You can also use the Lorentz transforms to transform the ##\Delta## quantities explicitly if you want to see how the light's velocity vector transforms. The x component of its three velocity is just ##\Delta x/\Delta t## and similarly for the y and z components. Likewise in the primed frame - just remember to use the primed spatial and time deltas.
Does the 2nd postulate of special relativity imply that if I shift the origin of a co-ordinate system to make another(without rotation),only then the speed of light is constant in both reference frame but so is not true when I do the shifting with rotation?
 
phymath7 said:
Does the 2nd postulate of special relativity imply that if I shift the origin of a co-ordinate system to make another(without rotation),only then the speed of light is constant in both reference frame but so is not true when I do the shifting with rotation?
No. The speed of light is the same in all inertial reference frames. You can see that easily enough in the maths above. The components of the 3-velocity vector change under rotation or Lorentz boost, but not its magnitude.
 
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Ibix said:
No. The speed of light is the same in all inertial reference frames. You can see that easily enough in the maths above. The components of the 3-velocity vector change under rotation or Lorentz boost, but not its magnitude.
Another way of saying this is that although all inertial frames agree on the speed of a beam of light, they don't all agree on the beam's direction (relative to the frame axes). This is due to aberration.
 
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  • #10
I don't know, what you define as a "velocity vector of light". The speed of light in Maxwell's equations (or in the somewhat hidden form of ##\mu_0 \epsilon_0=1/c^2## in the SI) is the phase velocity of plane-wave solutions.

The closest related vector quantity to it is the wave-fourvector, ##k=(\omega/c,\vec{k})## of an em. wave in vacuum, which is necessarily a null-vector, ##\omega^2/c^2-\vec{k}^2=0## or ##\omega=c |\vec{k}|##. It transforms as a four-vector, and of course ##\omega## and ##\vec{k}## both change under boosts, describing the Doppler effect (change of ##\omega##) and aberration (change of direction of ##\vec{k}##). The speed of light is the same, because a null vector stays a null vector, i.e., you also have ##\omega'=c|\vec{k}'|## in the new frame.
 
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phymath7 said:
Does the 2nd postulate of special relativity imply that if I shift the origin of a co-ordinate system to make another(without rotation),only then the speed of light is constant in both reference frame but so is not true when I do the shifting with rotation?
The spacetime interval is invariant under rotations, translations, time translations, and Lorentz boosts.
 
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