General Relativity: An Introduction for Physicists · Problem 9.3

The Schwarzschild geometry — Hobson, Efstathiou & Lasenby

Physics · schwarzschild-geodesic-connection-coefficients

Problem

The Schwarzschild line element is ds2=c2(1−2μr)dt2−(1−2μr)−1dr2−r2 dθ2−r2sin⁡2θ dϕ2.ds^2 = c^2\left(1-\frac{2\mu}{r}\right)dt^2 - \left(1-\frac{2\mu}{r}\right)^{-1}dr^2 - r^2\,d\theta^2 - r^2\sin^2\theta\,d\phi^2. By considering the 'Lagrangian' L=gμνx˙μx˙νL = g_{\mu\nu}\dot{x}^\mu\dot{x}^\nu, where the dots denote differentiation with respect to an affine parameter λ\lambda, calculate the connection coefficients Γνσμ\Gamma^\mu_{\nu\sigma}. Hence verify that the geodesic equations are given by (9.17--9.20).

Browse the problem library