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 solution (i.e. the spacetime outside of a spherical, nonrotating, gravitating body) must be given by the Schwarzschild metric.

The theorem was proven in 1923 by G. D. Birkhoff (author of another famous *Birkhoff theorem*, the *pointwise ergodic theorem* which lies at the foundation of ergodic theory). However, Stanley Deser recently pointed out that it was published two years earlier by a little-known Norwegian physicist, Jørg Tofte Jebsen.

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## Intuitive rationale

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 (partly) 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.

## Implications

The conclusion that the exterior field must also be *stationary* 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.

Another interesting consequence of Birkhoff's theorem is that for a spherically symmetric thin shell, the interior solution must be given by the Minkowski metric; in other words, the gravitational field must vanish inside a spherically symmetric shell. This agrees with what happens in Newtonian gravitation.

## Generalizations

Birkhoff's theorem can be generalized: any spherically symmetric solution of the Einstein/Maxwell field equations, without Λ, must be stationary and asymptotically flat, so the exterior geometry of a spherically symmetric charged star must be given by the Reissner–Nordström electrovacuum.

## See also

- Shell theorem in Newton's gravity
- Special Relativity

## References

- Deser, S & Franklin, J (2005). "Schwarzschild and Birkhoff a la Weyl".
*American Journal of Physics*.**73**(3): 261–264. arXiv:gr-qc/0408067. Bibcode:2005AmJPh..73..261D. doi:10.1119/1.1830505. - Johansen, Nils Voje; and Ravndal, Finn On the discovery of Birkhoff's theorem version of September 6, 2005.
- D'Inverno, Ray (1992).
*Introducing Einstein's Relativity*. Oxford: Clarendon Press. ISBN 0-19-859686-3. See*section 14.6*for a proof of the Birkhoff theorem, and see*section 18.1*for the generalized Birkhoff theorem. - Birkhoff, G. D. (1923).
*Relativity and Modern Physics*. Cambridge, Massachusetts: Harvard University Press. LCCN 23008297. - Jebsen, J. T. (1921). "Über die allgemeinen kugelsymmetrischen Lösungen der Einsteinschen Gravitationsgleichungen im Vakuum (On the General Spherically Symmetric Solutions of Einstein's Gravitational Equations in Vacuo)".
*Arkiv för Matematik, Astronomi och Fysik*.**15**: 1–9.