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๐ŸŒ€Riemannian Geometry Unit 13 Review

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13.3 Schwarzschild solution and black holes

๐ŸŒ€Riemannian Geometry
Unit 13 Review

13.3 Schwarzschild solution and black holes

Written by the Fiveable Content Team โ€ข Last updated September 2025
Written by the Fiveable Content Team โ€ข Last updated September 2025
๐ŸŒ€Riemannian Geometry
Unit & Topic Study Guides

The Schwarzschild solution is a key concept in general relativity, describing the spacetime around non-rotating, spherically symmetric masses. It introduces the idea of event horizons and black holes, where gravity becomes so strong that even light can't escape.

This solution reveals fascinating phenomena like gravitational time dilation and geodesic motion in curved spacetime. It also provides a framework for understanding black hole structure, including the event horizon and singularity, which challenge our understanding of physics.

Schwarzschild Solution

Metric and Radius

  • Schwarzschild metric describes spacetime geometry around a non-rotating, spherically symmetric mass
  • Expressed in spherical coordinates $(t, r, \theta, \phi)$ as: ds2=โˆ’(1โˆ’2GMrc2)c2dt2+(1โˆ’2GMrc2)โˆ’1dr2+r2(dฮธ2+sinโก2ฮธdฯ•2)ds^2 = -(1-\frac{2GM}{rc^2})c^2dt^2 + (1-\frac{2GM}{rc^2})^{-1}dr^2 + r^2(d\theta^2 + \sin^2\theta d\phi^2)
  • Schwarzschild radius $r_s = \frac{2GM}{c^2}$ defines the event horizon boundary
  • Represents distance from center where escape velocity equals speed of light
  • Depends on mass of the object (larger mass results in larger Schwarzschild radius)

Time Dilation and Geodesic Motion

  • Gravitational time dilation occurs near massive objects due to spacetime curvature
  • Time passes more slowly for observers closer to the gravitational source
  • Calculated using the formula: ฮ”tโˆž=ฮ”t0/1โˆ’2GMrc2\Delta t_\infty = \Delta t_0 / \sqrt{1-\frac{2GM}{rc^2}} Where $\Delta t_\infty$ is time measured by distant observer, $\Delta t_0$ is proper time
  • Geodesic motion describes path of freely falling objects in curved spacetime
  • Follows principle of least action, maximizing proper time between two events
  • Geodesic equation in general relativity: d2xฮผdฯ„2+ฮ“ฮฑฮฒฮผdxฮฑdฯ„dxฮฒdฯ„=0\frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu_{\alpha\beta}\frac{dx^\alpha}{d\tau}\frac{dx^\beta}{d\tau} = 0 Where $\Gamma^\mu_{\alpha\beta}$ are Christoffel symbols, $\tau$ is proper time

Black Hole Structure

Event Horizon and Singularity

  • Event horizon marks boundary beyond which light cannot escape
  • Acts as one-way membrane, allowing matter and light to enter but not exit
  • Located at Schwarzschild radius for non-rotating black holes
  • Singularity resides at center of black hole where spacetime curvature becomes infinite
  • Classical general relativity breaks down at singularity, requiring quantum gravity
  • Cosmic censorship hypothesis suggests singularities always hidden behind event horizons

Coordinate Systems and Diagrams

  • Kruskal-Szekeres coordinates provide complete description of Schwarzschild spacetime
  • Removes coordinate singularity at event horizon present in Schwarzschild coordinates
  • Allows visualization of both exterior and interior regions of black hole
  • Metric in Kruskal-Szekeres coordinates: ds2=32G3M3reโˆ’r/2GM(โˆ’dT2+dX2)+r2(dฮธ2+sinโก2ฮธdฯ•2)ds^2 = \frac{32G^3M^3}{r}e^{-r/2GM}(-dT^2 + dX^2) + r^2(d\theta^2 + \sin^2\theta d\phi^2)
  • Penrose diagram offers compact representation of causal structure of spacetime
  • Uses conformal transformations to bring infinity to finite distance
  • Illustrates light cones, event horizons, and singularities in single diagram
  • Helps visualize global structure of spacetime, including multiple universes and white holes