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Schwarzschild Metric

This metric is fundamental for calculating gravitational effects near a point mass.
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The statement of the theorem

For a static, spherically symmetric mass MM in vacuum, the Schwarzschild metric gμνg_{\mu\nu} in coordinates (t,r,θ,ϕ)(t, r, \theta, \phi) is given by:\n\nds2=gμνdxμdxν=(12GMc2r)c2dt2+1(12GMc2r)dr2+r2(dθ2+sin2θdϕ2)ds^2 = g_{\mu\nu} dx^\mu dx^\nu = -\left(1 - \frac{2GM}{c^2 r}\right) c^2 dt^2 + \frac{1}{\left(1 - \frac{2GM}{c^2 r}\right)} dr^2 + r^2 (d\theta^2 + \sin^2 \theta d\phi^2)\n\nWhere GG is the gravitational constant, MM is the mass, and cc is the speed of light. The components are gtt=(12GMc2r)g_{tt} = -\left(1 - \frac{2GM}{c^2 r}\right), grr=(12GMc2r)1g_{rr} = \left(1 - \frac{2GM}{c^2 r}\right)^{-1}, and gθθ=r2g_{\theta\theta} = r^2.
Source: Wikipedia