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Part of the book series: Undergraduate Lecture Notes in Physics ((ULNP))

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Abstract

A derivation of the Schwarzschild metric and a discussion of its main properties (including a detailed computation of the precession of the planetary orbits). The Schwarzschild solution is also used as a simple example of “black hole” geometry, in order to illustrate the physical effects of the event horizon and the need for introducing the so-called “maximal analytical extension” of the coordinate system.

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Notes

  1. 1.

    Actually, radiation can be emitted thanks to quantum effects, as first shown by [24].

  2. 2.

    There is a curious coincidence concerning the name of the physicist who discovered this metric: Schwarzschild, in German language, means indeed “black shield”.

  3. 3.

    If the metric is not Ricci-flat, i.e. if \(R_{\mu\nu }\not=0\) and R≠0, the number of such scalar objects raises from 4 to 14.

References

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  2. Hawking, S.W.: Commun. Math. Phys. 43, 199 (1975)

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  3. Hawking, S.W., Ellis, G.R.F.: The Large Scale Structure of Spacetime. University Press, Cambridge (1973)

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  4. Ohanian, H.C., Ruffini, R.: Gravitation and Spacetime. Norton, New York (1994)

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  5. Wald, R.: General Relativity. University of Chicago Press, Chicago (1984)

    MATH  Google Scholar 

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Gasperini, M. (2013). The Schwarzschild Solution. In: Theory of Gravitational Interactions. Undergraduate Lecture Notes in Physics. Springer, Milano. https://doi.org/10.1007/978-88-470-2691-9_10

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