Physical meaning of a spacelike geodesic

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SUMMARY

The discussion centers on the physical meaning of spacelike geodesics in the context of general relativity. Participants clarify that while spacelike geodesics represent the longest path between two events in curved spacetime, their physical interpretation is less straightforward than that of timelike geodesics, which correspond to proper time. The conversation highlights the importance of geometry in physics, arguing that geometric relationships are integral to understanding physical interactions, despite some participants questioning the physical significance of spacelike geodesics without specific conventions.

PREREQUISITES
  • Understanding of general relativity concepts, particularly geodesics.
  • Familiarity with spacetime geometry and its implications in physics.
  • Knowledge of proper time and proper length in the context of timelike and spacelike paths.
  • Basic grasp of foliation in spacetime and its relevance to physical measurements.
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  • Explore the implications of spacelike geodesics in curved spacetime.
  • Study the concept of proper length and its measurement in general relativity.
  • Investigate the role of foliation in spacetime and its impact on physical interpretations.
  • Learn about the relationship between geometry and physical laws in theoretical physics.
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Physicists, mathematicians, and students of general relativity seeking to deepen their understanding of the interplay between geometry and physical phenomena, particularly in the context of spacelike and timelike geodesics.

  • #61
That's also true, if you interpret the tangent space at the point under consideration as an affine point space. This affine space then indeed has the full Poincare symmetry, but for general GR spacetimes you usually don't have a translation symmetry.
 
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  • #62
vanhees71 said:
That's also true, if you interpret the tangent space at the point under consideration as an affine point space.
As discussed in a recent thread, to endow the underlying set (i.e. the set of spacetime points) of an affine structure the set of tangent spaces at each point must met let me say a 'consistency condition'. Basically vectors belonging to different tangent spaces have to be understood/treated as elements of the same vector space (i.e. the translation vector space) in a such way that axioms of affine space are fullfilled.
 
  • #63
We were talking about one tangent space at one fixed point in spacetime. An affine space is flat, but general-relativistic spacetime at presence of gravitational fields is not.
 
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