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Non-exact solutions in general relativity : ウィキペディア英語版 | Non-exact solutions in general relativity Non-exact solutions in general relativity are solutions of Albert Einstein's field equations of general relativity which hold only approximately. These solutions are typically found by treating the gravitational field, , as a background space-time, , (which is usually an exact solution) plus some small perturbation, . Then one is able to solve the Einstein field equations as a series in , dropping higher order terms for simplicity. A common example of this method results in the linearised Einstein field equations. In this case we expand the full space-time metric about the flat Minkowski metric, : ::, and dropping all terms which are of second or higher order in . ==See also==
* Exact solutions in general relativity * Linearized gravity * Post-Newtonian expansion * Parameterized post-Newtonian formalism * Numerical relativity
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