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Einstein’s Field Equations and Black Hole Spacetime

Manual: General · Subject: Physics

Covers the field equations, canonical solutions, and core strong-gravity predictions.

The Geometry of Gravity

Einstein Field Equations

Einstein’s field equations are Gμν+Λgμν=8πGc4Tμν.G_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4}T_{\mu\nu}. They relate spacetime curvature, encoded in the Einstein tensor GμνG_{\mu\nu}, to the stress-energy tensor TμνT_{\mu\nu}.

Schwarzschild Solution

The vacuum solution outside a spherically symmetric non-rotating mass is the Schwarzschild metric. It predicts gravitational time dilation, light bending, perihelion precession, and an event horizon at the Schwarzschild radius rs=2GMc2.r_s = \frac{2GM}{c^2}.

Physical Interpretation

Black holes are regions from which causal signals cannot escape to infinity once inside the event horizon. Their existence is a robust consequence of classical GR under broad conditions, not merely a coordinate artifact.

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Coordinate vs Physical Singularity

The Schwarzschild radius is a horizon, not a true curvature singularity; the central singularity at r=0r=0 is where curvature invariants diverge.

What does TμνT_{\mu\nu} represent in Einstein’s equations?

Write the Schwarzschild radius formula.

Canonical GR Predictions

EffectFormula/FeaturePhysical Meaning
Gravitational redshiftClock rates vary with potentialClocks deeper in gravity run slower
Light bendingNull geodesics curvePhotons follow spacetime geometry
Perihelion precessionOrbital advance beyond Newtonian theoryMercury’s orbit shifts
Event horizonr=rsr = r_sCausal boundary of a black hole

Which statement about a black hole horizon is correct?

Reading the Field Equations

  1. 1

    Step 1: Identify the spacetime symmetry and choose an ansatz for the metric.

  2. 2

    Step 2: Compute curvature tensors from the metric.

  3. 3

    Step 3: Set the Einstein tensor equal to the stress-energy source.

  4. 4

    Step 4: Interpret horizons, redshifts, and geodesics physically.