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Black holes and the Schwarzschild radius

PHYS 501 · Compact Objects

Black holes are regions where gravity is so strong that not even light can escape. This lesson introduces event horizons, Schwarzschild radius, accretion, and observational evidence.

Key equations

v_{esc}=sqrt{ rac{2GM}{r}}v_{esc}=cR_s= rac{2GM}{c^2}r=R_s

Learning objectives

  • Define a black hole and event horizon.
  • Derive the Schwarzschild radius scale.
  • Explain why the event horizon is not a material surface.
  • Distinguish stellar-mass and supermassive black holes.
  • Describe observational evidence for black holes.

What is a black hole?

A black hole is a region of spacetime with an event horizon: a boundary beyond which future-directed paths cannot escape to distant observers. The event horizon is not a material surface. It is a causal boundary.

Black holes are predicted by general relativity, not Newtonian gravity. However, a useful scale can be motivated by setting Newtonian escape speed equal to light speed.

Schwarzschild radius

The Newtonian escape speed from mass MM at radius rr is

v_{esc}=sqrt{ rac{2GM}{r}}

Set vesc=cv_{esc}=c and solve for rr:

R_s= rac{2GM}{c^2}

This is the Schwarzschild radius for a nonrotating, uncharged black hole.

For the Sun's mass, RsR_s is about 3 km. The actual Sun is much larger than this, so it is not a black hole.

Event horizon

At the event horizon of a Schwarzschild black hole, r=Rsr=R_s. Light emitted outward exactly at the horizon cannot increase its distance from the black hole. Inside the horizon, all future paths lead inward toward smaller rr.

This is not because light locally slows down. Locally, light still travels at cc. The global geometry of spacetime determines what paths can escape.

Singularity and limits of theory

Classical general relativity predicts a singularity inside a black hole, where curvature becomes infinite. Most physicists expect this indicates the breakdown of classical theory and the need for quantum gravity.

The event horizon is well described by classical relativity for large black holes, but the singularity is a sign of incomplete physics.

Stellar and supermassive black holes

Stellar-mass black holes form from the collapse of massive stars. Supermassive black holes, with millions to billions of solar masses, reside in the centers of many galaxies, including the Milky Way.

Their formation may involve early seed black holes, accretion, mergers, and galaxy evolution.

Accretion disks

Black holes themselves emit no classical light from inside the horizon, but material falling toward them can shine intensely. Gas with angular momentum forms an accretion disk. Friction, turbulence, and magnetic fields heat the disk, producing radiation.

Some accreting black holes launch powerful jets. The energy source is gravitational potential energy and, in some cases, black hole spin.

Observational evidence

Black holes are detected through their gravitational influence and accretion emission. Evidence includes stellar orbits around the Milky Way's central black hole, X-ray binaries, gravitational waves from black hole mergers, and horizon-scale imaging of supermassive black holes.

No single observation is the whole story, but together they strongly support black holes as real astrophysical objects.

The big idea

A black hole has an event horizon, a causal boundary from which light cannot escape. The Schwarzschild radius Rs=2GM/c2R_s=2GM/c^2 gives the horizon size for a nonrotating black hole. Black holes reveal gravity at its most extreme and connect stellar death, galaxy evolution, gravitational waves, and quantum questions.

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