Special relativity effects in general relativity

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Discussion Overview

The discussion centers on the compatibility of Special Relativity (SR) with General Relativity (GR), particularly how SR effects such as time dilation, length contraction, and relative simultaneity manifest in the context of curved space-time. Participants explore theoretical implications, analogies, and specific scenarios involving both frameworks.

Discussion Character

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

Main Points Raised

  • Some participants propose that SR is an approximation applicable in regions where curvature effects are negligible, while GR accounts for curvature in space-time.
  • One analogy compares the difference between SR and GR to living on a flat plane versus a curved surface, suggesting that curvature effects become significant over larger distances.
  • Participants discuss the concept of tangent spaces in GR, where local flatness allows SR effects to be observed, but additional curvature effects arise in larger regions.
  • There is a question about whether a curve in space would experience length contraction relative to a moving frame, and how flat space-time effects transmit to curved space-time.
  • Some participants clarify that length contraction and time dilation in GR are defined at specific events and can include both SR kinematic effects and GR gravitational effects.
  • Questions arise regarding the nature of paths in GR, with some asserting that paths are straight lines in curved space-time, while others suggest that extended objects may be subject to tidal forces.
  • Participants express uncertainty about how to reconcile the concepts of straight and curved paths in the context of GR and SR.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the nature of paths in GR and the implications of curvature on physical objects. The discussion remains unresolved on several points, with multiple competing views presented.

Contextual Notes

Limitations include the dependence on definitions of curvature and straightness in space-time, as well as the unresolved nature of how SR effects apply globally in GR. The discussion also highlights the complexity of relating local observations to global geometrical structures.

  • #31
analyst5 said:
Ok, I guess I'm wrong, but kinematical time dilation and gravitational time dilation do add up?

Sort of, at least in simple circumstances. For example if we have an observer in circular free fall orbit in Schwarzschild space-time then the observer's "gamma factor" in Schwarzschild coordinates will be ##\gamma = (1 - 2M/R - R^2 \omega^2)^{-1/2}## where the ##2M/R## accounts for the gravitational part and the ##R^2 \omega^2## accounts for the kinematical part. Then ##\gamma^{-1}## represents the rate at which the circularly orbiting observer's clock ticks relative to a clock at spatial infinity.
 

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