Notion of parallel worldlines in curved geometry

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SUMMARY

The discussion centers on the concept of parallel worldlines in curved geometry, specifically in the context of spacetime curvature and geodesic deviation. It establishes that two worldlines can only be considered parallel when they start close enough to each other in a flat spacetime, allowing for an unambiguous definition. The Levi-Civita connection derived from the metric tensor is identified as the standard method for determining parallelism in curved spacetime. Furthermore, the conversation explores whether the definition of parallelism can extend to non-geodesic worldlines, concluding that no widely accepted definition exists for such cases.

PREREQUISITES
  • Understanding of spacetime curvature and geodesic deviation
  • Familiarity with the Levi-Civita connection and metric tensors
  • Knowledge of geodesics and their properties in differential geometry
  • Basic concepts of non-Euclidean geometry
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  • Research the properties of the Levi-Civita connection in curved spacetime
  • Explore geodesic deviation and its implications in general relativity
  • Investigate the concept of Clifford parallelism in non-Euclidean geometry
  • Examine the differences between geodesic and non-geodesic worldlines
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The discussion is beneficial for physicists, mathematicians, and students of general relativity who are interested in the geometric interpretation of spacetime and the behavior of worldlines in curved geometries.

cianfa72
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TL;DR
About the notion "to be parallel" in the context of curved geometry
The notion of spacetime curvature is just the same as geodesic deviation. Therefore take for instance two bodies at different altitudes from Earth surface. In order to evaluate their geodesic deviation the two worldlines must start parallel in spacetime (actually in tangent spaces at both initial points/events).

We know in curved spacetime the notion of "to be parallel" is path dependent and it is given by the affine connection assigned to the spacetime as metric manifold (i.e. the Levi-Civita connection derivated from the metric tensor ##g## is normally used).

That said, which is the relevant/implied path to say that the two worldlines start parallel ? I believe it is the geodesic path one gets exponentiating the (spacelike) vector orthogonal to the first worldline's 4-velocity at its starting point that intersect the other worldline at its starting point.
 
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cianfa72 said:
TL;DR Summary: About the notion "to be parallel" in the context of curved geometry

That said, which is the relevant/implied path to say that the two worldlines start parallel ?
Usually you can only make such a statement when those two worldlines are initially close enough that you can treat them as being in a flat spacetime. Then it is unambiguous.
 
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Dale said:
Usually you can only make such a statement when those two worldlines are initially close enough that you can treat them as being in a flat spacetime. Then it is unambiguous.
Ok. Does the above definition of parallelism apply also to non geodesic worldlines as well?

Take for instance two concentric circles on the euclidean plane. From any point on the bigger one, draw the orthogonal straight line to the other circle getting a point.The tangents to circles on both points stay always parallel.
 
cianfa72 said:
Does the above definition of parallelism apply also to non geodesic worldlines as well?
I have never seen a definition of parallel that would apply to non-geodesics. There might be one, but I don't know of it.
 
Does the definition of "to be parallel" for geodesics also demand that the distance/lenght along the orthogonal geodesics between them at any point stays the same?

See also Clifford parallel.
 
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I believe the definition of "to be parallel" for geodesics in the context of non-euclidean geometry actually doesn't demand that the (minimum) distance between them must stay constant.
 
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