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Kerr-Newman metric

The Kerr-Newman metric is a solution of Einstein's field equations that describes the spacetime geometry around a charged (Q\neq0), rotating (J\neq0) black hole of mass m. The Kerr-Newman metric is:

ds^{2}=-\frac{\Delta}{\rho^{2}}\left(dt-a\sin^{2}\theta d\phi\right)^{2}+\frac{\sin^{2}\theta}{\rho^{2}}\left[\left(r^{2}+a^{2}\right)d\phi-{a}dt\right]^{2} +\frac{\rho^{2}}{\Delta}dr^{2}+\rho^{2}d\theta^{2}

\frac{\Delta}{\rho^{2}}\equiv \frac{r^{2}-{2}{M}{r}+a^{2}+Q^{2}}{r^{2}+a^{2}\cos^{2}\theta}

\rho^{2}\equiv r^{2}+a^{2}\cos^{2}\theta

a\equiv\frac{J}{M}

Source(s)

01-04-2007 01:16:19
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