I Physical meaning of a spacelike geodesic

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The discussion centers on the physical meaning of spacelike geodesics, contrasting them with timelike geodesics, which represent proper time for objects in free fall. Participants debate whether the geometric interpretation of spacelike geodesics can be considered physical, with some arguing that geometry is integral to physics and others asserting that it lacks intrinsic physical meaning. The conversation highlights the complexities of measuring lengths along spacelike geodesics, especially in non-static spacetimes, and the necessity of conventions for defining physical quantities. Ultimately, the ambiguity of "physical meaning" in this context is acknowledged, indicating that further specification is often required. The dialogue underscores the intricate relationship between geometry and physical interpretation in the realm of spacetime.
  • #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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