Can motion affect spectral signatures in a hydrogen-filled cube?

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Discussion Overview

The discussion centers on whether the motion of a cube containing a glob of excited hydrogen affects the spectral signatures detected by spectrometers positioned on its faces. Participants explore the implications of motion, particularly in the context of special relativity and the Doppler effect, considering both inertial and accelerated frames of reference.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that during inertial motion, the spectral signature remains unchanged across all spectrometers, as nothing is moving relative to anything else.
  • Others propose that during acceleration, the Doppler effect applies, leading to blue shifts and red shifts depending on the direction of motion relative to the emission point of the photons.
  • There is a discussion about the implications of constant linear motion on the properties of light, with some arguing that it has no measurable effect, while others reference the relativistic Doppler shift as a counterpoint.
  • Some participants express skepticism about the completeness of special relativity, suggesting that the concept of an ether could be detectable under certain conditions, despite mainstream views dismissing it.
  • There are claims that the vacuum of space is not empty, with references to radiation emitted during acceleration in a vacuum, which raises questions about the nature of space and its properties.

Areas of Agreement / Disagreement

Participants generally disagree on the effects of motion on spectral signatures, with competing views on the implications of special relativity and the existence of an ether. The discussion remains unresolved regarding the detectability of the ether and the completeness of current physical theories.

Contextual Notes

Limitations include the dependence on definitions of motion and the unresolved nature of the ether concept in relation to special relativity. The discussion also highlights the complexity of interpreting light's behavior under different frames of reference.

Chrisc
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I have a cube with a spectrometer at the center of each face. In the center of the cube is an exited glob of hydrogen. The spectral lines (signature) of the hydrogen are registered at the same frequency on all six spectrometers.
I now set the cube in motion.
Does the signature move up or down the spectrum on any of the spectrometers?
 
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During acceleration, yes.

During inertial motion, no.
 
DaleSpam said:
During inertial motion, no.

What if the cube is traveling at a constant [non-zero] velocity relative to the "glob"?

Regards,

Bill
 
Then, yes, but that is not how I interpreted the OP.
 
The cube is at rest with respect to the source (hydrogen) at the center.

So the frequency of light detected will be the same for all spectrometers?
And an identical construct in any other inertial frame will show the same results?
 
Chrisc said:
I have a cube with a spectrometer at the center of each face. In the center of the cube is an excited glob of hydrogen. The spectral lines (signature) of the hydrogen are registered at the same frequency on all six spectrometers.
I now set the cube in motion.
Does the signature move up or down the spectrum on any of the spectrometers?

DaleSpam is correct. For inertial motion, nothing is moving relative to anything else, so all 6 spectrometers record the same frequency.

During acceleration, analyse this from the inertial frame in which the cube was at rest when some photons were emitted from the glob in all directions. By the time these photons reach the sides of the cube, the cube is no longer stationary in that frame. So the doppler shift formula applies. Blue shift for the rear face (moving towards the emission point). Red shift for the front face. And transverse doppler for the other four sides.
 
Chrisc said:
The cube is at rest with respect to the source (hydrogen) at the center.

So the frequency of light detected will be the same for all spectrometers?
And an identical construct in any other inertial frame will show the same results?
Yes.
 
Then constant linear motion has no measurable effect on the properties of light?
This seems to indicate light (EM) is nothing more than a propagating modulation of spacetime.
A modulation that is held constant between all inertial frames via time dilation and length contraction.
 
Chrisc said:
Then constant linear motion has no measurable effect on the properties of light?
There is the relativistic Doppler shift which is measurable. Your set up seemed expressly designed to avoid that.

Chrisc said:
This seems to indicate light (EM) is nothing more than a propagating modulation of spacetime.
A modulation that is held constant between all inertial frames via time dilation and length contraction.
I don't know what you mean by that, but if you mean something different than Maxwell's equations or a QM description of light then it probably belongs on a different forum.
 
  • #10
Chrisc said:
Then constant linear motion has no measurable effect on the properties of light?
Yep. That is the point of Special Relativity. Moving with constant motion results in no measurable effects that any different to be stationary.

Chrisc said:
This seems to indicate light (EM) is nothing more than a propagating modulation of spacetime.
A modulation that is held constant between all inertial frames via time dilation and length contraction.

That is one way of looking at it, but it is not the view of Special Relativity. It is the view of Lorentz Ether theory which produces identical results to Special Relativity but unfortunately it makes the ether undectable. If the ether is undetectable then "there is no need of it" as Einstein said.
 
  • #11
DaleSpam said:
I don't know what you mean by that, but if you mean something different than Maxwell's equations or a QM description of light then it probably belongs on a different forum.

I mean it in the sense of Maxwell's equations, QFT and GR. All of which express dynamics of space-time in their own "separate" way.
Is there a forum here that permits one to question the mainstream metaphysical modeling of GR, QT and the Standard Model?

kev, there is another way. The ether is not it.
A very careful (first principled) study of time in all of physics makes it clear. I cannot get into it here as mentioned above.
But if you're interested, consider this: there are only three dimensions in physics (in the universe) - space, time and mass.
The first continuum was modeled by Einstein as space-time.
The next includes mass in "exactly" the same relativistic structure.
 
  • #12
kev said:
If the ether is undetectable then "there is no need of it" as Einstein said.

Aether is undetectable and "there is no need of it" only if Special Relativity have unlimited domain of applicability and that is clearly not the case as for any theory of physics.
And as that is not the case aether could be detectable.
 
  • #13
zonde said:
Aether is undetectable and "there is no need of it" only if Special Relativity have unlimited domain of applicability and that is clearly not the case as for any theory of physics.
And as that is not the case aether could be detectable.

Well, it can be shown that the vacuum of space is not empty. Put a rocket in an otherwise empty universe and start to accelerate hard. Accelerate relative to what? Don't worry about that. Just look behind you and notice all the radiation that is popping out of the vacuum. Clearly the vacuum of space is not empty.
 
  • #14
kev said:
Well, it can be shown that the vacuum of space is not empty. Put a rocket in an otherwise empty universe and start to accelerate hard. Accelerate relative to what? Don't worry about that. Just look behind you and notice all the radiation that is popping out of the vacuum. Clearly the vacuum of space is not empty.
Right, probably detectable is not the right word because it all the same is only concept of physics. Probably better would be to say that it could be competitive approach to use less abstract concepts with more realistic descriptions.
 

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