SR vs GR Simultaneity: Comparing Moving & Static Observers

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Discussion Overview

The discussion revolves around the concept of simultaneity in Special Relativity (SR) and General Relativity (GR), particularly how different observers—both moving and static—perceive simultaneity in flat and curved spacetime. Participants explore the implications of these theories on the understanding of time and simultaneity, addressing both theoretical and conceptual aspects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that in SR, observers at rest and moving observers slice spacetime differently, raising the question of how this translates to GR and curved spacetime.
  • Another participant emphasizes that the definition of simultaneity in GR is not straightforward and suggests that simultaneity is a convention in SR without a clear counterpart in GR.
  • A participant questions the specific versions of SR and GR being referenced, asking for clarity on the theoretical frameworks being discussed.
  • In response to the previous question, another participant clarifies that Minkowski spacetime is used in SR and that GR involves solutions to the Einstein Field Equations.
  • One participant agrees with a previous point that certain cases in GR may have a more natural notion of simultaneity, such as in cosmological spacetimes where a preferred time coordinate exists.
  • There is a challenge regarding the relevance of discussing Maxwell's equations and their relation to the topic, with a suggestion to separate those discussions from the current thread.

Areas of Agreement / Disagreement

Participants express differing views on the nature of simultaneity in GR compared to SR, with some agreeing that simultaneity is a convention in SR while others propose specific cases in GR where simultaneity can be more clearly defined. The discussion remains unresolved regarding the implications of these differences.

Contextual Notes

Participants highlight the dependence of simultaneity on the choice of coordinate systems in GR, and the discussion reflects varying interpretations of the foundational theories of SR and GR, including historical context and theoretical structures.

smoothoperator
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In SR, we may choose any inertial observer and his reference frame at which he is at rest, and other observers are movin wrt to him. All the moving observers 'slice' spacetime in a different way than the observer at rest, at different angles relative to his simultaneity surfaces. This is all flat space time nature.

My question is, how does this translate to GR and curved space time? How do different observers slice curved space time and what does it look like compared to SR. I know that we have hovering observers and relative to them clocks far away form gravity run faster etc. What about moving observers (free falling observers) and the simultaneity slicing while gravitational time dilation is present? And please don't say that any coordinate system is acceptable, I know that, and my question is basically the comparision in simultaneity differences between moving and static observers in SR and GR.

Thanks in advance.
 
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This depends completely on how you wish to define simultaneity in GR. In SR there is a natural choice, but this is no longer true in GR. You might think of creating the spacelike hypersurface created by taking the union of all geodesics orthogonal to an observer's world line, or simply take a spacelike coordinate surface. However, my preeference is to simply acknowledge that simultaneity is a convention in SR that does not necessarily have a unambiguous counterpart in a general spacetime. This is why your question will normally be met with the "any coordinate system goes" reply.
 
When you say GR, what do you mean, 1916 or 1917? Also, when you say SR what do you mean, 1905 or 1917? Be specific, please. Also, when you say time space, what structure are you using, Maxwell's equations (cannot use timespace [a coordinate system] without a structure, can you)? But is not Maxwell's equations derived using Faraday's induction law that is not optical, and isn't Hertz's spark gap emitting electrons? Is an induction current the same as an ionization current?
 
Last edited:
seaocean1234 said:
When you say GR, what do you mean, 1916 or 1917? Also, when you say SR what do you mean, 1905 or 1917?

He means SR and GR, the current scientific theories. If there were different versions of those theories in prior years (I'm not sure why you are picking the particular years you are picking), that's a matter of history, not physics.

seaocean1234 said:
when you say time space, what structure are you using

In SR, Minkowski spacetime. In GR, whatever solution of the Einstein Field Equation is being discussed.

seaocean1234 said:
Maxwell's equations

Are not a "time space structure".

seaocean1234 said:
is not Maxwell's equations derived using Faraday's induction law that is not optical, and isn't Hertz's spark gap emitting electrons? Is an induction current the same as an ionization current?

This is irrelevant to the topic of this thread. Please start a separate thread in the appropriate forum if you have questions about Maxwell's Equations or electrodynamics.
 
Basically Orodruin's #2 is the answer to the question. However, there are certain specific cases in GR where one notion of simultaneity is more natural than another. For example, in a cosmological spacetime we have a preferred time coordinate, which is the time on a clock that is at rest with respect to the Hubble flow. In an asymptotically flat spacetime, you can essentially use SR's notion of simultaneity for distant regions.
 

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