Simultaneity in General Relativity

In summary, William Lane Craig discusses a specific coordinate system that is well-suited to describe the universe's large-scale behavior, based on the Friedmann metric as a solution to Einstein's field equations. While there are multiple ways to slice the spacetime into hypersurfaces, there is only one that has desirable properties and can be considered the "preferred" coordinate system. This is similar to the case of the Levi-Cevita connection, where elegance and niceness do not necessarily mean absoluteness.
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syra
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I had a much longer post typed with quotes and everything but I was auto-logged out, couldn't recover the text, and don't feel like typing it all in full. >:[

William Lane Craig, in "Einstein, Relativity, and Absolute Simultaneity" says that the Friedman metric as solution to Einstein's field equations (standard in cosmology) produces a unique hypersurface of simultaneity. Is this true, or is more than one hypersurface of simultaneity possible?
 
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Short answer: Each coordinate system defines simultaneity differently, but there's one particular coordinate system that's particularly well suited to describe the large-scale behavior of the universe. That's the coordinate system he's talking about. (I doubt that he fully understands that though).

Longer answer: The Friedmann(-Lemaitre-Robertson-Walker) class of solutions of Einstein's equation describe those spacetimes that can be sliced into a one-parameter family of spacelike hypersurfaces that are homogeneous and isotropic in a specific technical sense. It's convenient to choose the parameter that labels the hypersurfaces to be the proper time (from the big bang to the event where it intersects the hypersurface) of a geodesic that's orthogonal to the hypersurfaces. This convention enables us to think of the hypersurface labeled by parameter value t as "space, at time t". The "preferred" coordinate system is defined by choosing the coordinate time of any event to be equal to the parameter that labels the hypersurface, and by choosing the coordinate distance between any two points in the same hypersurface to be the proper distance in that hypersurface.

There are many ways to slice one of these spacetimes into hypersurfaces that we can think of as "space" at different "times", but there's only one slicing with the nice properties mentioned above. That's why the "nicest" coordinate system we can associate with that slicing can be considered "preferred".

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Ah man, thanks Fredrik. When I first read this from Craig, I instantly thought it was something like the case with the Levi-Cevita connection: it's the unique torsion-free one, but this doesn't mean that which tangent vectors are parallel or not on a manifold is uniquely determined (i.e. absolute), as there are many connections possible. Elegance and niceness isn't the same as absoluteness.
 

FAQ: Simultaneity in General Relativity

What is simultaneity in general relativity?

Simultaneity in general relativity refers to the concept of events occurring at the same time from the perspective of an observer. In classical physics, simultaneity is absolute and independent of an observer's frame of reference. However, in general relativity, simultaneity is relative and depends on an observer's relative motion and gravitational field.

How does general relativity explain simultaneity?

General relativity explains simultaneity by incorporating the effects of gravity into the concept of time. According to general relativity, time is not absolute and can be affected by gravitational fields. This means that two events that appear simultaneous to one observer may not be simultaneous to another observer in a different gravitational field.

What is the "relativity of simultaneity" in general relativity?

The relativity of simultaneity in general relativity is the idea that simultaneity is relative and can differ between different observers. This is in contrast to classical physics, where simultaneity is absolute and independent of an observer's frame of reference.

How does the theory of special relativity relate to simultaneity in general relativity?

The theory of special relativity is a special case of general relativity in which gravitational effects are not taken into account. In this theory, simultaneity is also relative and depends on an observer's frame of reference. However, general relativity expands on this concept by including the effects of gravity, which can further alter the perception of simultaneity between observers.

Can simultaneity be measured in general relativity?

In general relativity, simultaneity is a subjective concept and cannot be measured precisely. This is because it depends on an observer's frame of reference and the gravitational field they are in. However, in practical applications, scientists can use mathematical equations and observations to estimate and predict the relative simultaneity between different events in space and time.

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