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General Relativity — Foundations

Manual: General · Subject: General Relativity

Spacetime curvature, geodesics, and Einstein's field equations

Gravity as Curved Spacetime

The Equivalence Principle and Curved Spacetime

Einstein's equivalence principle: a uniform gravitational field is locally indistinguishable from acceleration. This leads to the conclusion that gravity is spacetime curvature.

The metric tensor gμνg_{\mu\nu} encodes distances: ds2=gμνdxμdxνds^2 = g_{\mu\nu}dx^\mu dx^\nu. Flat spacetime (Minkowski): ds2=−c2dt2+dx2+dy2+dz2ds^2 = -c^2dt^2 + dx^2 + dy^2 + dz^2.

Einstein's Field Equations

Gμν+Λgμν=8πGc4TμνG_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4}T_{\mu\nu} where Gμν=Rμν−12RgμνG_{\mu\nu} = R_{\mu\nu} - \frac{1}{2}Rg_{\mu\nu} is the Einstein tensor, RμνR_{\mu\nu} the Ricci tensor, Λ\Lambda the cosmological constant, and TμνT_{\mu\nu} the stress-energy tensor.

Free particles in curved spacetime follow geodesics (locally straight paths): d2xμdτ2+Γαβμdxαdτdxβdτ=0\frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu_{\alpha\beta}\frac{dx^\alpha}{d\tau}\frac{dx^\beta}{d\tau} = 0.

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Schwarzschild Metric

For a spherically symmetric mass MM in vacuum:<br>ds2=−(1−rsr)c2dt2+(1−rsr)−1dr2+r2dΩ2ds^2 = -\left(1-\frac{r_s}{r}\right)c^2dt^2 + \left(1-\frac{r_s}{r}\right)^{-1}dr^2 + r^2d\Omega^2<br>where rs=2GM/c2r_s = 2GM/c^2 is the Schwarzschild radius (event horizon).

Einstein's field equations relate:

The Schwarzschild radius of Earth (M⊕=6×1024M_\oplus = 6\times10^{24} kg) is approximately:

What observational evidence supports general relativity? Name at least three.