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[[Category:General relativity]]
[[Category:Mathematical methods in general relativity]]

Revision as of 17:31, 6 February 2006

The weak-field approximation in general relativity is used to describe the gravitational field very far from the source of gravity.

In this approximation, we assume the metric for spacetime () be written in coordinates as:

where is the Minkowski metric, is the deviation from the Minkowski metric and is taken to be a non-zero real constant.

A relation between the Newtonian gravitational potential and the deviation term above can be obtained by calculating the Christoffel symbols (upon ignoring terms of order higher than ):

from which follows:

()

The geodesic equation becomes

where is the Newtonian gravitational potential and is the speed of light. Thus:

As we know that

where is the gravitational constant, is the mass of the gravitating body and is the radial distance from the centre of this body, we find that:

The weak-field approximation is useful in finding the values of certain constants, for example in the Einstein field equations and in the Schwarzschild metric.

See also

References

  • . ISBN 0-521-37941-5. {{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)CS1 maint: extra punctuation (link)
  • . ISBN 0-070-00423-4. {{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)