Black Hole Spacetime
Event Horizons, Ergospheres & Frame Dragging
Schwarzschild rₛ
2M
Photon sphere
1.5 rₛ
Schw. ISCO
3 rₛ = 6M
Kerr r₊
M + √(M²−a²)
Static limit
2M (equator)
Extremal Kerr
a = M
Schwarzschild describes a non-rotating, uncharged black hole — a single event horizon at rₛ, a photon sphere where light orbits, and a fixed ISCO at 6M.
Kerr adds rotation. The horizon shrinks and is wrapped by an ergosphere — a region where spacetime is dragged faster than any observer can resist, so no rest frame exists. Inside, you must corotate.
Kerr also reveals an inner Cauchy horizon r₋, prograde and retrograde ISCOs at very different radii (2.32M vs 8.7M for a/M=0.9), and the ability to extract energy from the spin.
M87* (EHT 2019)
First imageThe first directly imaged supermassive black hole. The bright ring is the photon sphere, gravitationally lensed into a circle; the dark central shadow is ~2.6 × the event horizon, broadened by lensing. Mass: ~6.5 × 10⁹ M☉.
Sagittarius A* (EHT 2022)
4 × 10⁶ M☉Our galaxy's central SMBH, imaged after years of effort. Variability complicates reconstruction, but the ring structure matches Kerr predictions for ~4 × 10⁶ M☉, with a spin parameter constrained to a/M ≳ 0.5 — moderately rapidly rotating.
GW150914 ringdown (2015)
First GW + Kerr testThe first detected gravitational wave. After two black holes merged, the remnant 'rang down' through Kerr quasi-normal modes. The frequencies recovered a single Kerr black hole of ~62 M☉ with a/M ≈ 0.67 — direct confirmation of Kerr geometry from a real merger.
Penrose process
Ergosphere physicsInside the ergosphere, an object can carry negative energy as measured at infinity. Splitting an object so the negative-energy fragment falls in extracts rotational energy from the black hole. Believed to power the relativistic jets of active galactic nuclei.
