concept

kerr metric

The Kerr metric describes the spacetime geometry around a rotating black hole.
161 related articles

Description

The Kerr metric is the exact solution to Einstein's field equations of general relativity that describes the spacetime geometry around a rotating, uncharged black hole. It was derived by Roy Kerr in 1963 and is considered one of the most important exact solutions in physics. The metric is characterized by two parameters: mass and angular momentum, and it predicts several fascinating phenomena, including frame-dragging (the dragging of spacetime around the rotating black hole) and the existence of an ergosphere, a region outside the event horizon where objects cannot remain stationary.

History

Roy Kerr, a New Zealand mathematician, derived the solution in 1963 while working at the University of Texas at Austin. His work was a breakthrough, as it provided a realistic description of black holes that form from collapsing rotating stars.

How it works

The Kerr metric is a stationary, axisymmetric solution, meaning it does not change with time and is symmetric around the rotation axis. It reduces to the Schwarzschild metric (for non-rotating black holes) when the angular momentum is zero. The metric's mathematical form involves a complex interplay of mass, spin, and the radial distance from the black hole, leading to a horizon structure that includes an outer event horizon and an inner Cauchy horizon. The ergosphere is a region where spacetime itself is dragged along with the black hole's rotation, allowing energy extraction via the Penrose process.

In practice

The Kerr metric is essential for modeling astrophysical black holes, interpreting observations of their accretion disks and jets, and analyzing gravitational wave signals from black hole mergers, as detected by LIGO and Virgo.

Fun fact

The Kerr metric predicts that a rotating black hole can have up to two horizons, and at maximum spin, the event horizon and the ergosphere merge, a state known as an extremal black hole.

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Related articles · 161

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General Relativity2026-08-201 minarXiv:2608.19774express
A Black Hole Rings Like a Bell, and a Neural Network Listens
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The Milky Way's Rotation Curve: The Dark Halo Puzzle
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General Relativity2026-08-072 minarXiv:2608.06798express
A Black Hole Under the Microscope of Ripples
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A Black Hole as a Fussy Thermometer
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Black hole in a dark matter cocoon
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General Relativity2026-08-051 minarXiv:2608.05268express
Black Holes on the Brink: When Theory Breaks Down
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The Black Hole and Its Secret Twin
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General Relativity2026-08-032 minarXiv:2608.02481express
The Heart of a Black Hole: Why a Smooth Center Isn't Everything
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General Relativity2026-08-021 minarXiv:2608.00934express
Black Hole Collisions: What Remains After the Merger
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General Relativity2026-08-021 minarXiv:2608.01152express
The Hidden Twin of a Black Hole's Spin
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Flat Bands: Magnetism Without Motion
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General Relativity2026-08-011 minarXiv:2608.00519express
Black Hole Shadow: How Fluffy Dark Matter Reshapes the Horizon
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General Relativity2026-07-312 minarXiv:2607.28930express
Where a Black Hole's Ringing Begins
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General Relativity2026-07-312 minarXiv:2607.29350express
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General Relativity2026-07-311 minarXiv:2608.00305express
A Black Hole with Bristles and Its Shadow
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General Relativity2026-07-311 minarXiv:2608.00307express
Black Hole on a Dark Matter Diet
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General Relativity2026-07-302 minarXiv:2607.28249express
Mosaic on the Surface of a Black Hole
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General Relativity2026-07-291 minarXiv:2607.27129express
Chaos in the Shadow of a Black Hole
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General Relativity2026-07-281 minarXiv:2607.25311express
How Black Holes Ring After a Strike
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Light Fires Up the Valley Compass
A potter tries to measure the thickness of a jug's wall, but every time the gauge also reports the curvature of the vessel.
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Gravitational Waves Without the Mathematical Jungle
A taut trampoline sheet dips under a heavy ball. If the ball spins quickly, the sheet begins to twist around it. Spacetime near a rotating black hole behaves similarly: it is not just curved, but also dragged along by the rotation, like water swirling around a whirlpool.
General Relativity2026-07-181 minarXiv:2607.16842express
How a Spinning Black Hole Bends Light in a New Way
A light ray passing by a massive body gets deflected: this is the effect of gravitational lensing, familiar from images of distant galaxies. The astrophysicists started with a rotating black hole (Kerr spacetime) and added a tiny correction to how light itself propagates.
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General Relativity2026-07-121 minarXiv:2607.10533express
Spindle Black Hole: The Shadow Changes Shape
At the center of attention is a black hole of unusual shape. Its geometry resembles a spindle: a slight elongation is added to the usual rotation. The parameter B measures this deformation. The spindle deformation is not just a mathematical toy.
General Relativity2026-07-121 minarXiv:2607.10603express
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General Relativity2026-07-112 minarXiv:2607.10199express
A Black Hole Without a Breaking Point
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General Relativity2026-07-101 minarXiv:2607.09840express
General Relativity2026-07-091 minarXiv:2607.08570express
Gravitational Waves and the Black Hole Horizon
The LIGO detectors caught the signal GW250114—a gravitational wave from the merger of two black holes. After the main burst, a decaying 'tail' remained — direct waves from the newborn hole's horizon. It was expected that their damping would reveal the gravitational strength at the horizon's surface. But the measured value came out smaller.