Birkhoff's theorem states that the gravitational field outside a spherically symmetric mass is static and described by the Schwarzschild metric.In 1915, Karl Schwarzschild found the first exact solution to Einstein's equations — a metric describing spacetime around a stationary spherical mass. But what if the mass is not stationary, but pulsating or collapsing? Early 20th-century astronomers were at a loss. The answer came from American mathematician George David Birkhoff in 1923: the external solution always remains Schwarzschild if the system stays spherically symmetric. In other words, pulsations don't escape outward, just as sound doesn't leave a tightly sealed room. Birkhoff proved his theorem by analyzing the field equations, and the result was surprisingly simple: spherical symmetry 'locks in' any internal changes.
In 1916, Karl Schwarzschild found a solution for a point mass. Almost immediately the question arose: is the external field necessarily static if the source pulsates? In 1923, George David Birkhoff proved the uniqueness of the Schwarzschild solution in vacuum under spherical symmetry. Interestingly, two years earlier, in 1921, a little-known Dutch student Johannes Droste obtained a similar result, but his work went unnoticed. Birkhoff's theorem became a cornerstone of relativistic astrophysics and a rigorous foundation for why black holes have no 'hair'.
The theorem is widely used in numerical and analytical general relativity. It simplifies modeling of stellar collapse: as long as the system retains spherical symmetry, the external solution is known in advance. In quantum gravity, its consequence is the absence of 'breathing' modes for black holes. However, the slightest deviation from symmetry (rotation, tidal forces) breaks the theorem's conclusions: then the external field becomes dynamic and gravitational waves arise. Therefore, real astrophysical black holes generally rotate and are described by the Kerr metric.
Birkhoff's theorem explains why the spherical collapse of a star into a black hole does not radiate gravitational waves, and why the external field of a black hole is always described by the Schwarzschild solution.
If the Sun suddenly started to alternately expand and contract once a day, our instruments on Earth would detect not the slightest change in gravity — clocks and scales would continue as if nothing happened. The only way to know about the pulsations would be to observe radiation from the surface, but gravitationally, the Sun would remain absolutely 'silent'.
| G | variable | gravitational constant — gravitational constant cubic metre per kilogram per second squared |
| M | variable | mass of the object — mass kilogram |
| R | variable | radius of the object — radius metre |
| c | variable | speed of light in vacuum — speed of light metre per second |
| ds^2 | variable | spacetime interval — spacetime interval metre squared |
| dt | variable | coordinate time differential — time differential second |
| dr | variable | radial coordinate differential — radial coordinate differential metre |
| dΩ^2 | variable | solid angle element squared — solid angle element squared |
| r | variable | radial coordinate — radial coordinate metre |
| t | variable | coordinate time — coordinate time second |
| G | constant | Newton's constant of universal gravitation — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared |
| c | constant | speed of light in vacuum — speed of light = 299792458 metre per second |
| M | constant | mass of the central object — mass kilogram |
| d | operator | infinitesimal change — differential |







