Solving Einstein's Equations for Binary Black Hole Spacetimes
Solving Einstein's Equations for Binary Black Hole Spacetimes
Solving Einstein's Equations for Binary Black Hole Spacetimes
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General Relativity Theory<br />
Einstein’s theory of gravitation, general relativity theory, is a<br />
geometrical theory in which gravitational effects are described as<br />
geometrical structures on spacetime.<br />
The fundamental “gravitational” field is the spacetime metric ψ ab<br />
— a non-degenerate symmetric tensor field.<br />
Coordinates x a are used to label points in spacetime.<br />
The spacetime metric determines the physical lengths of curves<br />
x a (λ) in spacetime, L 2 = ± ∫ dx<br />
ψ a dx b<br />
ab dλ dλ dλ.<br />
Coordinates x a can be chosen in any convenient way.<br />
For example x a can be chosen at any point in spacetime so that<br />
ds 2 = ψ ab dx a dx b = −dt 2 + dx 2 + dy 2 + dz 2 at that point.<br />
In these special coordinates the second-order differential operator<br />
ψ ab ∂ a ∂ b reduces to the standard wave operator:<br />
.<br />
ψ ab ∂ a ∂ b = −∂ 2 t + ∂ 2 x + ∂ 2 y + ∂ 2 z<br />
Lee Lindblom (Caltech) <strong>Binary</strong> <strong>Black</strong> <strong>Hole</strong>s UW Milwaukee 10/14/2011 4 / 32