Expressing Locality in Vector Space for GR

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Discussion Overview

The discussion revolves around expressing the concept of locality within vector spaces in the context of general relativity (GR). Participants explore the boundaries and implications of using vector spaces to describe physical phenomena, particularly the motion of particles in gravitational fields and the transition between different reference frames.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question how to define the boundaries of a vector space in GR, suggesting that one could theoretically use the entirety of ##\mathbb{R}^4## for local calculations.
  • There is a proposal that calculations become inaccurate when moving away from a specific point of consideration, but the extent of this inaccuracy is debated.
  • One participant mentions that Newtonian physics is sufficient until precision measurements (like those with atomic clocks) are required, implying a threshold for when GR becomes necessary.
  • Another participant emphasizes that the local tangent space can be transported along curves in the manifold, but raises the question of how parallel transport differs along different curves.
  • A participant corrects the original poster by stating that space-time is a manifold rather than a vector space.
  • Historical context is introduced with a reference to Gauss's early ideas on non-Euclidean geometry and its observational implications, linking it to modern concepts like the Hubble constant.

Areas of Agreement / Disagreement

Participants express differing views on the definition of locality in vector spaces and the implications of using GR. There is no consensus on the accuracy of calculations or the necessity of splitting reference frames, indicating an unresolved discussion.

Contextual Notes

Participants note the importance of singularities and different connection components in the discussion of tangent spaces. There are also references to specific calculations and historical ideas that may not be fully substantiated within the current context.

kent davidge
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How do we express the locality of a vector space in general relativity?

I mean, it's not clear what the boundaries of a given vector space are.

To put in another way, we could, in principle, blindly consider that we have the entire of ##\mathbb{R}^4## at our disposal to describe, say, the motion of a particle near Earth. The question which comes in is to what extent our calculations become wrong, at which point we should sort of split our reference frame in two, three.. etc reference frames as required by general relativity.
 
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kent davidge said:
How do we express the locality of a vector space in general relativity?

I mean, it's not clear what the boundaries of a given vector space are.

To put in another way, we could, in principle, blindly consider that we have the entire of ##\mathbb{R}^4## at our disposal to describe, say, the motion of a particle near Earth. The question which comes in is to what extent our calculations become wrong, at which point we should sort of split our reference frame in two, three.. etc reference frames as required by general relativity.
The calculations become wrong the moment you leave the point of consideration. The question is how wrong? E.g. Newton works perfectly well, until you decide to measure with atomic clocks. Or as @PeterDonis has recently put it: As long as you don't want to establish a GPS for Mars, general relativity isn't needed. I think the crucial point is, that the local tangent space can be transported along curves in the manifold and it is still a tangent space at some new point. Of course this only works well as long as no singularities or different connection components come into play. An interesting example are fast myons in cosmic radiation. For an average lifetime of ##2\cdot 10^{-6}## seconds, how come we can detect them on the ground? So when calculations are wrong is what calculations are performed.
 
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fresh_42 said:
that the local tangent space can be transported along curves in the manifold and it is still a tangent space at some new point
This remains true also globally. The question is how much the parallel transports along different curves differ.

It should also be pointed out to the OP that space-time itself is a manifold, not a vector space.
 
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kent davidge said:
at which point we should sort of split our reference frame in two, three.. etc reference frames as required by general relativity.

I don't understand what you're referring to here.
 
If I am not mistaken, though I can not find its proof on internet now, in early 1800s, Friedlich Gauss proposed an idea that non-Eucledian geometry may be found by observation of stars in space far away. Discovery by Hubble might have been on this line. Evaluation of Hubble constant might give some numerical estimation to your problem, deviation from flat spacetime.

Hubble constant
67.15 km/s /Mpc=67.15 km/s / 3.086 E22 m = 2.18E-18 (m/s) /m
1m distance of two "still" bodies increases 2 attometer every second.
 
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