Levi-Civita connection and pseudoRiemannian metric

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Discussion Overview

The discussion revolves around the properties of the Levi-Civita connection in the context of pseudo-Riemannian metrics and their implications for the structure of manifolds. Participants explore the relationship between metric spaces and pseudo-Riemannian manifolds, particularly focusing on distance functions, invariant intervals, and the compatibility of these concepts in the framework of general relativity.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the Levi-Civita connection preserves the metric tensor, allowing for the definition of invariant intervals in a manifold.
  • Others argue that invariant intervals are a property of the metric tensor itself, independent of the Levi-Civita connection.
  • A participant questions how distance functions in spacetime relate to the metric space structure, particularly regarding lightlike intervals and null curves.
  • There is a discussion about the differences between "metric space" and "metric tensor," with some participants emphasizing that they are separate concepts.
  • One participant proposes a specific definition of a distance function based on the infimum of lengths of smooth curves connecting points in the manifold.
  • Another participant seeks clarification on how the pseudo-Riemannian metric defines distance functions in a pseudo-Riemannian manifold.
  • There is a suggestion to avoid using the term "metric space" in favor of more precise terminology to reduce confusion.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between the Levi-Civita connection and invariant intervals, as well as the implications of pseudo-Riemannian metrics for distance functions. The discussion remains unresolved, with multiple competing perspectives on these topics.

Contextual Notes

Participants highlight the need for clarity regarding the definitions of distance functions and the implications of pseudo-Riemannian metrics on the structure of manifolds. There is an acknowledgment of the complexity introduced by the terminology used in the discussion.

  • #91
Just out of curiosity, what is the point of this thread?
 
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  • #92
TrickyDicky said:
In the text it is literally stated "we need to calculate the null geodesic from G1 to us".

Which, taken in context, means "find an expression for ##\int ds = 0## along the null geodesic, and then split it up into pieces that have different physical interpretations". What the text does *not* say is anything along the lines of "these separate pieces, even though they have obvious physical interpretations as integrals along timelike or spacelike geodesics, are actually integrals of some function other than ##ds = 0## along the null geodesic the light follows".

TrickyDicky said:
Calculations based on the integration of the null geodesic equations

I'm not sure what you mean by "integration of the null geodesic equations". Finding an expression for ##\int ds = 0## is not the same as integrating the geodesic equation; the ##\int ds = 0## expression can be written down purely from the FRW line element. The geodesic equation itself doesn't appear anywhere in the integrand.

TrickyDicky said:
Hairsplitting whether thy are about "how far" or "how long" or whether each integral by itself is the integral of a null geodesic is a purely terminologic discussion that is of not much utility in practice.

If you mean you don't need to go into all these details in order to get a numerical answer, of course you're right. But the same can be said of hairsplitting about whether what we are doing can be interpreted as calculating a "distance" along the null geodesic that's different from the physical ##ds = 0## distance (i.e., whether we can interpret what we're doing as calculating ##D_T## instead of ##D_M##), as opposed to splitting up the ##\int ds = 0## expression into pieces with obvious physical interpretations as integrals along timelike or spacelike geodesics. None of these interpretations matter if all you're concerned with is getting a numerical answer for ##D_p##. They only matter if you have particular preferences for how to justify interpreting ##D_p## as a "distance".
 
  • #93
PeterDonis said:
Which, taken in context, means "find an expression for ##\int ds = 0## along the null geodesic, and then split it up into pieces that have different physical interpretations". What the text does *not* say is anything along the lines of "these separate pieces, even though they have obvious physical interpretations as integrals along timelike or spacelike geodesics, are actually integrals of some function other than ##ds = 0## along the null geodesic the light follows".
I am saying(like you I think) that they are integrals of ##ds = 0## along the null geodesic the light follows.


I'm not sure what you mean by "integration of the null geodesic equations". Finding an expression for ##\int ds = 0## is not the same as integrating the geodesic equation; the ##\int ds = 0## expression can be written down purely from the FRW line element. The geodesic equation itself doesn't appear anywhere in the integrand.
Right, the sentence is read:integration of the "null geodesic" equations (ds=0), not integration of the null "geodesic equations".


If you mean you don't need to go into all these details in order to get a numerical answer, of course you're right. But the same can be said of hairsplitting about whether what we are doing can be interpreted as calculating a "distance" along the null geodesic that's different from the physical ##ds = 0## distance (i.e., whether we can interpret what we're doing as calculating ##D_T## instead of ##D_M##), as opposed to splitting up the ##\int ds = 0## expression into pieces with obvious physical interpretations as integrals along timelike or spacelike geodesics. None of these interpretations matter if all you're concerned with is getting a numerical answer for ##D_p##. They only matter if you have particular preferences for how to justify interpreting ##D_p## as a "distance".
Fair enough.
Since there is some curiosity about the point of this thread and just in case you are interested in what goes on beyond the purely computational side of it, the chapter "On the structure of space-time" page 178(in google books preview) in the book "Space, time and geometry" is what inspired my OP.
 
  • #94
Do you mean the book by P. Suppes? I must say that I have absolutely no idea how that page of the book led you to this question!
 
  • #95
martinbn said:
Do you mean the book by P. Suppes? I must say that I have absolutely no idea how that page of the book led you to this question!

Yes, that book. But that is just the first page in the essay, he mentions metric spaces and how this definition applies to relativity and classical space-times in pge 180.
 

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