
A rotating black hole solution to Einstein's field equations, described by the Kerr metric.A Kerr black hole is a rotating black hole solution to Einstein's field equations of general relativity, discovered by Roy Kerr in 1963. Unlike the non-rotating Schwarzschild black hole, a Kerr black hole is described by its mass and angular momentum, and it possesses two event horizons and an ergosphere—a region outside the outer horizon where spacetime is dragged along by the rotation. The Kerr metric is considered the most physically realistic description of black holes in the universe, as most black holes are expected to spin.
Roy Kerr derived the solution in 1963 while at the University of Texas at Austin, solving a problem that had stumped physicists for decades. His work was a breakthrough in general relativity and remains one of the most important exact solutions in the field.
The rotation of the black hole drags spacetime around it, an effect known as frame-dragging. The outer event horizon is the point of no return for infalling matter, while the inner horizon is a Cauchy horizon where causality may break down. The ergosphere allows energy extraction through the Penrose process, where particles can enter the ergosphere and leave with more energy than they entered. The geometry also supports quasinormal modes—characteristic 'ringing' frequencies that encode the black hole's mass and spin, which are now routinely measured by gravitational wave observatories.
Kerr black holes are used to model astrophysical black holes in X-ray binaries and galactic centers, and to interpret gravitational wave signals from mergers detected by LIGO and Virgo.
The inner horizon of a Kerr black hole is a region where time and space swap roles again, and it may act as a gateway to other universes—though any traveler would first encounter a singularity of infinite density.














