Schwarzschild metric
In Einstein's theory of general relativity, the Schwarzschild solution (or the Schwarzschild vacuum) describes the gravitational field outside a spherical, non-rotating mass such as a (non-rotating) star, planet, or black hole. It is also a good approximation to the gravitational field of a slowly rotating body like the Earth or Sun. According to Birkhoff's theorem, the Schwarzchild solution is the most general static, spherically symmetric, vacuum solution of Einstein's field equations. A Schwarzschild black hole or static black hole is a black hole that has no charge or angular momentum. A Schwarzschild black hole has a Schwarzschild metric, and cannot be distinguished from any other Schwarzschild black hole except by its mass.
See also
- black hole, a general review
- Reissner-Nordström black hole
- Kerr metric (rotating solution)
~ Table of Content ~
| ► | Introduction |
| ► | The Schwarzschild metric |
| ► | Singularities and black holes |
| ► | Embedding Schwarzschild space in Euclidean space |
| ► | Orbital motion |
| ► | Quotes |
| ► | References |
| ► | See also |
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