This is an old revision of this page, as edited by Hillman (talk | contribs) at 19:51, 29 May 2005 (Moved one sentence to the end and corrected external link). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
Revision as of 19:51, 29 May 2005 by Hillman (talk | contribs) (Moved one sentence to the end and corrected external link)(diff) ← Previous revision | Latest revision (diff) | Newer revision → (diff)In general relativity, Birkhoff's theorem states that any spherically symmetric solution of the vacuum field equations must be static and asymptotically flat. This means that the exterior metric must be given by the Schwarzschild solution.
The intuitive idea of Birkhoff's theorem is that a spherically symmetric gravitational field should be produced by some massive object at the origin; if there were another concentration of mass-energy somewhere else, this would disturb the spherical symmetry, so we can expect the solution to represent an isolated object. That is, the field should vanish at large distances, which is what we mean by saying the solution is asymptotically flat. Thus, this part of the theorem is just what we would expect from the fact that general relativity reduces to Newtonian gravitation in the Newtonian limit.
The conclusion that the exterior field must also be static is more surprising, and has an interesting consequence. Suppose we have a spherically symmetric star of fixed mass which is experiencing spherical pulsations. Then Birkhoff's theorem says that the exterior geometry must be Schwarzschild; the only effect of the pulsation is to change the location of the stellar surface. This means that a spherically pulsating star cannot emit gravitational waves.
Birkhoff's theorem can be generalized: any spherically symmetric solution of the Einstein/Maxwell field equations must be static and asympotically flat, so the exterior geometry of a spherically symmetric charged star must be given by the Reissner/Nordstrom electrovacuum.
The theorem was proven in 1927 by G. D. Birkhoff (author of an even more famous Birkhoff theorem, the pointwise ergodic theorem which lies at the foundation of ergodic theory).
Reference
- . ISBN 0-19-859686-3.
{{cite book}}
: Missing or empty|title=
(help); Unknown parameter|Author=
ignored (|author=
suggested) (help); Unknown parameter|Publisher=
ignored (|publisher=
suggested) (help); Unknown parameter|Title=
ignored (|title=
suggested) (help); Unknown parameter|Year=
ignored (|year=
suggested) (help) See section 14.6 for a proof of the Birkhoff theorem, and see section 18.1 for the generalized Birkhoff theorem.
External link
- ScienceWorld page on Birkhoff's Theorem