Why do people care about vacuum solutions in GR?

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SUMMARY

Vacuum solutions in general relativity (GR) are essential for understanding regions of the universe that are well-approximated by vacuum, such as interstellar space. These solutions, including the Schwarzschild vacuum, are mathematically tractable and provide insights into more complex astrophysical models. Birkhoff’s theorem confirms that the exterior solution to a spherically symmetric mass distribution is a vacuum solution, reinforcing the relevance of vacuum solutions in practical applications. Consequently, vacuum solutions are not ignored as non-physical; they are critical for modeling and understanding gravitational phenomena.

PREREQUISITES
  • Understanding of general relativity (GR) principles
  • Familiarity with Birkhoff’s theorem
  • Knowledge of Schwarzschild solutions
  • Basic concepts of mathematical modeling in physics
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  • Study the implications of Birkhoff’s theorem in GR
  • Explore the mathematical properties of the Schwarzschild vacuum solution
  • Investigate the role of vacuum solutions in gravitational wave propagation
  • Learn about the Oppenheimer-Snyder model of stellar collapse
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Physicists, astrophysicists, and students of general relativity seeking to deepen their understanding of vacuum solutions and their applications in modeling the universe.

ohwilleke
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TL;DR
People study vacuum solutions in general relativity, but I don't really understand why.
I understand that there are vacuum solutions of the equations of general relativity (GR) (i.e. equations with no mass-energy content contributing to the stress-energy tensor), that are studied by physicists interested in GR.

I don't understand why these are studied or what purpose they serve. Why aren't these solutions simply ignored as non-physical?

Could someone explain this at a very basic level?
 
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They're often mathematically tractable.

You don't need to write down an equation of state for matter that you may not entirely believe under extreme circumstances anyway. (Contributes to the previous paragraph.)

Most of space on interstellar scales is vacuum to a very good approximation, so you need vacuum solutions. Because of this, realistic and semi-realistic astrophysical models are often vacuum solutions around non-vacuum regions. And things like gravitational waves are effectively propagating in vacuum.

Analysing mathematically tractable models can give you insight into how to approach numerical simulations of more general cases. And elephant traps to be aware of.
 
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ohwilleke said:
TL;DR Summary: People study vacuum solutions in general relativity, but I don't really understand why.

Could someone explain this at a very basic level?
Vacuum does not mean uninteresting. Most of the universe is very well approximated by vacuum - making Minkowski space a pretty good approximation locally. In addition you have things like Birkhoff’s theorem ensuring that the solution outside a spherically symmetric streas-energy distribution is the exterior Schwarzschild solution - which is a vacuum solution.
 
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Ibix said:
And elephant traps to be aware of.
Who knew that there were elephants in space? :cool: Life always brings surprises I guess.
 
Orodruin said:
Vacuum does not mean uninteresting. Most of the universe is very well approximated by vacuum - making Minkowski space a pretty good approximation locally. In addition you have things like Birkhoff’s theorem ensuring that the solution outside a spherically symmetric streas-energy distribution is the exterior Schwarzschild solution - which is a vacuum solution.
Does this mean that a vacuum solution requires boundary conditions, or for that matter, just boundaries?
 
ohwilleke said:
Could someone explain this at a very basic level?
Consider the analogous situation in electrostatics. The field equation in vacuum for the electrostatic potential ##\varphi## is ##\nabla^{2}\varphi\left(r\right)=0##. The spherically-symmetric solution to this is ##\varphi\left(r\right)=\frac{k}{r}+\varphi\left(\infty\right)##, i.e., it's the potential outside of an isolated charge. This is a physical result. The gravitational analog is the vacuum Schwarzschild solution of general relativity, i.e., it's the metric tensor outside of an isolated mass. This is also a physical result.
 
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ohwilleke said:
Does this mean that a vacuum solution requires boundary conditions, or for that matter, just boundaries?
No, but the universe has matter in it, so you will often be interested in solutions that join a matter-filled solution to a vacuum solution. For example, the Oppenheimer-Snyder black hole is a toy model of stellar collapse that consists of a small part of a closed FLRW solution started from the instantaneous rest point (this is the star) stitched to a Schwarzschild vacuum (the space around the star).

Separately, there is the notion of "domain of applicability". Minkowski spacetime is a fine model for studying even something like Fizeau's experiments with light in water - clearly not a vacuum, but the failure to be vacuum is a tiny tiny correction to the result. SR is applicable in domains where the curvature is negligible.
 
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ohwilleke said:
Why aren't these solutions simply ignored as non-physical?
Um, because they're not?

Our universe has plenty of significant regions which are, to a very good approximation, vacuum. Vacuum solutions describe these regions to a very good approximation, certainly good enough for practical use. A specific solution in GR does not have to describe an entire spacetime. It can perfectly well describe a region of spacetime that is joined to another non-vacuum region.
 
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ohwilleke said:
Does this mean that a vacuum solution requires boundary conditions, or for that matter, just boundaries?
Generally speaking, a vacuum region will have a boundary with a non-vacuum region, yes.
 
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PeterDonis said:
A specific solution in GR does not have to describe an entire spacetime.
This is what I hadn't realized about these solutions.
 
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