law

First law of black hole mechanics

The first law of black hole mechanics relates changes in mass, angular momentum, and horizon area to energy conservation in black hole thermodynamics.
17 related articles · 3 formulas · 2 who worked here

Description

In the 1970s, James Bardeen, Brandon Carter, and Stephen Hawking, pondering the analogy between thermodynamics and black holes, formulated four laws of black hole mechanics. The first law reads: dM = (κ/8π) dA + Ω dJ + Φ dQ. Here mass M is analogous to energy, surface gravity κ to temperature, horizon area A to entropy, and Ω and Φ are angular velocity and electric potential. Initially, this was considered a mathematical game, but after Hawking's discovery of black hole radiation, it turned out the analogy is exact. Black holes truly have temperature and entropy – for instance, their horizon area never decreases, just like entropy in an isolated system.

History

In 1972, James Bardeen, Brandon Carter, and Stephen Hawking published a paper presenting four laws of black hole mechanics in analogy with thermodynamics. The first law linked the differentials of the main parameters. In 1975, Stephen Hawking, using quantum effects near the horizon, showed that black holes emit thermal radiation with a temperature proportional to κ. This turned the formal analogy into a physically meaningful theory. Earlier, Jacob Bekenstein had suggested that horizon area is proportional to entropy, and with Hawking's work, the coefficient was refined to 1/4. Thus was born black hole thermodynamics, uniting gravity, quantum mechanics, and statistical physics.

How it works

The law is actively applied to calculate matter accretion onto black holes, mergers, and Hawking radiation. It holds for stationary black holes in classical general relativity. At the quantum level, accounting for radiation corrections, the law continues to hold if entropy is defined as A/4 plus quantum additions. The limits of applicability arise at Planck scales, where a theory of quantum gravity is needed.

In practice

The law is used by gravitational observatories LIGO and Virgo: by measuring the change in mass and rotation before and after black hole mergers, they calculate how much energy was carried away by gravitational waves.

Fun fact

If you throw a star into a black hole, its entropy (hidden in the horizon area) jumps by a gigantic amount. For example, the supermassive black hole at the center of the Milky Way, upon swallowing one Sun, would increase its entropy by a number with 80 zeros.

Concept graph →

Formulas

$$\delta M = \frac{\kappa}{8\pi} \delta A + \Omega_H \delta J$$
Changes in black hole mass relate to area and angular momentum.
What is in the formula
δMvariableInfinitesimal change in black hole mass — mass kilogram
κvariableSurface gravity of the black hole — surface gravity metre per second squared
δAvariableInfinitesimal change in horizon area — area square metre
Ω_HvariableAngular velocity of the horizon — angular velocity radian per second
δJvariableInfinitesimal change in angular momentum — angular momentum kilogram square metre per second
δoperatorInfinitesimal variation of a quantity — variation
δa=\frac{8π}{\kappa}(δe-ω_hδj) · 2606.06592v1
$$dU = \delta Q - \delta W$$
Change in internal energy equals heat added minus work done.
What is in the formula
dUvariableInfinitesimal change in internal energy — internal energy joule
δQvariableInfinitesimal heat added to the system — heat joule
δWvariableInfinitesimal work done by the system — work joule
doperatorExact differential of a state function — exact differential
δoperatorInexact differential for path-dependent quantities — inexact differential
de=tds-pdv · 2607.03749
$$\Delta(r) = r^2 - 2Mr + a^2$$
Horizon function for Kerr black holes with mass M and spin a.
What is in the formula
\Delta(r)variableHorizon function of the Kerr metric — horizon function square metre
rvariableRadial coordinate (Boyer-Lindquist) — radial coordinate metre
MvariableBlack hole mass — mass kilogram
avariableSpecific angular momentum (spin parameter) — specific angular momentum metre
δ_{{dm}}(r)=r^2-2m[1+\frac{\varepsilon}{m}μ_{{dm}}(r)]r+a^2 · 2607.13992

Related articles · 309

Quantum Dance Without a Shared Stage
Two dancers on the same stage mirror each other's moves even when a curtain separates them. In the quantum world, such pairs are called entangled, and physicists have spent half a century probing how far this connection reaches. Until now, all tests with massive particles concerned their internal properties, such as spin, but not their motion itself.
Black hole on a chip: how a quantum processor played the role of an information maze
A black hole is a maze with no way out. But what happens to the information inside? To test this, physicists didn't fly to the nearest hole; instead, they built a tiny replica on a quantum processor. The maze was played by a chain of 32 superconducting qubits, where each step leads only forward, like a one-way corridor.
General Relativity2026-08-162 minarXiv:2608.15723express
A Date of Two Black Holes: How to Calculate Their Dance More Precisely
Two black holes, caught in a dance, spiral closer and closer until they merge into one. This dance is not silent: it shakes spacetime itself, sending gravitational waves rippling across the Universe. To understand what we hear in these waves, we need a precise mathematical model of the dance.
HEP Theory2026-08-102 minarXiv:2608.09797express
Black Hole Rings Like a Hot Bell
Drop a pebble into a pond, and ripples spread across the water. Something similar happens when a black hole merges with another: it emits gravitational waves that resemble the fading ring of a bell.
Galaxies2026-08-091 minarXiv:2608.08945express
General Relativity2026-08-082 minarXiv:2608.08302express
The Universe's Horizon as a Heat Engine
Stare long enough into the night sky, and sooner or later your gaze hits a blackness beyond which nothing is visible. This is not just a distant fence: it is the edge of the universe accessible to us, the cosmic horizon. Light from more distant stars simply hasn't had time to reach us.
HEP Phenomenology2026-08-082 minarXiv:2608.08144express
Black Holes That Didn't Evaporate
A campfire that doesn't go out all at once but smolders for hours because the wood inside still holds the heat of the past flame. That's roughly how the memory effect works for black holes. Normally, a tiny black hole with the mass of a mountain should evaporate in fractions of a second, scattering particles like sparks.
General Relativity2026-08-072 minarXiv:2608.06798express
A Black Hole Under the Microscope of Ripples
When two heavy balls merge into one, ripples spread across the water's surface for a long time. A black hole behaves similarly: after a merger, it 'rings' for a while, emitting special gravitational oscillations — quasinormal modes. Usually, this ring fades quickly, like an echo dying out in an empty hall.
General Relativity2026-08-072 minarXiv:2608.07046express
How Entropy Builds a Black Hole
A black hole is not just a dark spot in space. It has a temperature, and it radiates. It has entropy — a measure of hidden information encoded on its horizon's surface, like a pattern on a soap bubble.
General Relativity2026-08-071 minarXiv:2608.07182express
Black Hole Cools Down and Freezes
A boiling kettle on the stove eventually boils dry — and so, according to the classical picture, a black hole should gradually vanish in a hiss of radiation. But what if you add a special ingredient to the kettle?
Cosmology2026-08-071 minarXiv:2608.07264express
How the Jitters of Space Can Stifle the Birth of Black Holes
When you blow up a balloon too quickly, its surface starts to quiver. Something similar happened to space in the first moments after the Big Bang: the universe expanded rapidly, and the very fabric of space began to ripple.
HEP Theory2026-08-062 minarXiv:2608.05795express
The Third Law for a Black Hole
A black hole has three laws, just like an ideal gas. The first: energy is conserved. The second: the horizon area never decreases. And the third, the most finicky, demands that at zero temperature the entropy (a measure of disorder) tend to zero or a universal constant.
HEP Theory2026-08-062 minarXiv:2608.05801express
A Black Hole as a Fussy Thermometer
A fussy thermometer shows different temperatures depending on who is looking at it. A black hole behaves much the same way: its thermal properties, entropy and temperature, depend on how we describe the information hidden inside.
General Relativity2026-08-062 minarXiv:2608.05861express
Black hole in a dark matter cocoon
Somewhere in the center of a galaxy, a black hole is spinning. It doesn't hang in a void — around it swirls an invisible swarm of dark matter particles. Until now, this swarm was described for non-rotating holes, but in reality, holes always rotate.
Black Holes Sound Different in a Curved World
A black hole rings like a bell after being struck. This ring is the gravitational waves that detectors pick up. But what changes if the space around the hole is curved not only by its mass but also by an additional quantum correction?
HEP Phenomenology2026-08-052 minarXiv:2608.05282express
Hunting the Invisible: The Sensitivity Limit of Detectors
A hunter sets snares in the woods. They know the animal's habits but not whether it will ever show up. In much the same way, physicists set up detectors in hopes of catching particles of dark matter — the invisible substance thought to make up most of the Universe's mass. A new study offers hunters an unusual tool: not a trap, but a measuring tape.
General Relativity2026-08-051 minarXiv:2608.04346express
Tiny Black Holes and Their Charge Jitter
A black hole is not an eternal vacuum cleaner. It slowly loses mass by emitting particles, much like a heated stone cooling as it radiates heat. This process, discovered by Stephen Hawking, is barely noticeable for large holes, but for tiny ones, with masses comparable to a mountain, it becomes a violent evaporation.
General Relativity2026-08-052 minarXiv:2608.04461express
The Black Hole Trampoline: A Jump Through the Horizon
The idea was elegant: take a BTZ black hole (the three-dimensional analog of a regular black hole) and smooth its horizon with a special function. The hope was that inside, the spacetime signature might change — time becoming space, and space becoming time. But the calculations showed otherwise.
General Relativity2026-08-051 minarXiv:2608.04470express
How Dark Matter Reshapes Black Holes
An invisible scaffold holds galaxies together, keeping them from flying apart. This is dark matter — matter that doesn't shine and barely interacts with ordinary stuff. Astrophysicists have long debated what it's made of.
General Relativity2026-08-052 minarXiv:2608.05061express
Black Holes Don't Like Being Squeezed
Drop a stone into a calm lake, and ripples spread in even circles. Spacetime around a massive body behaves similarly: if the body is perfectly round, the disturbances it causes are symmetric. A black hole in general relativity resembles a perfectly smooth mirror of water.
General Relativity2026-08-051 minarXiv:2608.05268express
Black Holes on the Brink: When Theory Breaks Down
A black hole spun up almost to its limit is like an athlete balancing on the edge of a record. The most interesting action isn't inside the hole itself, but in the thinnest film of spacetime at its horizon. It's there that tiny corrections to Einstein's gravity can suddenly swell to gigantic proportions.
General Relativity2026-08-042 minarXiv:2608.03538express
Black Hole Turns Inside Out into a White Fountain
A black hole that swallows matter might not just evaporate over billions of years: it could pop like a soap bubble and turn into its opposite: a white hole. This scenario emerged from numerical experiments in semiclassical gravity.
General Relativity2026-08-031 minarXiv:2608.02051express
Dark Matter Around a Black Hole: A Torus-Shaped Cloud
A black hole isn't just a cosmic vacuum cleaner. If it rotates, it can amplify waves around it, much like a mountain echo repeats sound. For ultralight dark matter (particles billions of times lighter than an electron), this effect, called superradiance, can create a huge cloud.
General Relativity2026-08-031 minarXiv:2608.02259express
The Black Hole and Its Secret Twin
A rotating black hole is no calm whirlpool. Space around it shudders and rings at the slightest disturbance, like a guitar string after a pluck. These oscillations are described by the Teukolsky equation — a complex mathematical construct that physicists have studied for half a century. Recently, a strange symmetry was noticed in this equation.
General Relativity2026-08-032 minarXiv:2608.02481express
The Heart of a Black Hole: Why a Smooth Center Isn't Everything
An old house. The facade is freshly painted, the stairs don't creak. A pretty picture. But try to move in heavy furniture, and the floorboards give way. The beauty of the facade says nothing about the strength of the floors. It's much the same with black holes without singularities.
General Relativity2026-08-021 minarXiv:2608.00934express
Black Hole Collisions: What Remains After the Merger
Two black holes circle in a cosmic dance, spiraling closer together. In the end, they merge into one, and that moment unleashes a powerful burst of gravitational waves, ripples in spacetime itself. But what remains after the merger?
General Relativity2026-08-021 minarXiv:2608.01061express
Listening to the Echo of a Black Hole
You could send a short radio pulse toward a black hole and wait for the reflected echo. Intuitively, the shorter the signal, the better it would probe the finest details of spacetime right at the horizon: that region from which even light cannot return.
General Relativity2026-08-021 minarXiv:2608.01152express
The Hidden Twin of a Black Hole's Spin
The Kerr-NUT black hole is not just a cosmic vacuum cleaner. It's a solution to Einstein's equations where the hole has mass, rotation, and a strange NUT parameter. This parameter behaves like a magnetic charge for gravity: seemingly invisible, yet it alters the properties of surrounding space.
General Relativity2026-08-022 minarXiv:2608.01200express
A Black Hole in a Dark Fur Coat
A black hole is not silent. When perturbed, it rings like a bell, and that ring is its quasinormal modes — damped oscillations. Physicists delved into the world of charged black holes in anti-de Sitter space (a universe with negative curvature, like a saddle).
General Relativity2026-08-011 minarXiv:2608.00519express
Black Hole Shadow: How Fluffy Dark Matter Reshapes the Horizon
A black hole is not an empty funnel. Invisible matter can accumulate around it, and then the familiar boundaries shift. A group of theorists found a simple condition: if the mass of this surrounding material grows smoothly and satisfies the inequality 1 − 2m' − rm'' > 0, then the event horizon remains well-defined and the hole stays stable.
HEP Theory2026-08-011 minarXiv:2608.00590express
Black Holes as Bridges to the Dawn of the Universe
A black hole is not just an abyss. It is a seething cauldron whose temperature rises as it evaporates. The authors of the study found that when the heat reaches a critical threshold, the hole seems to boil. It emits superheavy particles — the very ones that exist on a scale where any theory of gravity collapses.
High Energy2026-07-311 minarXiv:2607.28919express
How Black Holes Spit Out Energy
A whirlpool gulps down water, but splashes most of it back out. That's roughly how a black hole behaves when too much matter falls onto it. In a new study, astrophysicists ran 32 computer simulations to understand how a black hole's parameters — mass, spin, and "appetite"—control these cosmic fountains.
HEP Theory2026-07-311 minarXiv:2607.29028express
The Thermal Breath of a Black Hole
A black hole is not an absolutely black bag. In 1974, Stephen Hawking showed that it glows — faintly, but continuously. This radiation is born not inside, but outside, right at the boundary from which even light cannot escape. A new study sharpens the picture.
High Energy2026-07-312 minarXiv:2607.29121express
A Black Hole's Shadow with a Secret from Other Dimensions
A cosmic object spins, but its shadow isn't round. Astrophysicists examined a black hole in an unusual version of gravity — the so-called brane world (where our universe is a three-dimensional surface in a space of higher dimensions).
High Energy2026-07-312 minarXiv:2607.29273express
Black Hole Echo: What the Horizon Sounds Like
When two black holes merge, ripples spread across the fabric of spacetime — gravitational waves. But what if one of them isn't a run-of-the-mill black hole but something else — an exotic compact object?
General Relativity2026-07-311 minarXiv:2608.00305express
A Black Hole with Bristles and Its Shadow
A black hole doesn't just spin: it's surrounded by bristles of an extra field (the Kalb–Ramond field). This paper explores how a massive field (waves with mass) behaves near such a black hole when it's almost spinning at its maximum rate. The Klein–Gordon–Fock equation for this field was separated into two independent parts — radial and angular.
General Relativity2026-07-311 minarXiv:2608.00307express
Black Hole on a Dark Matter Diet
A black hole is not a perfect vacuum cleaner. It is surrounded by a swarm of particles and fields, and this swarm alters its fate. In a new study, astrophysicists examined how a massive vector field, a hypothetical form of dark matter, behaves near a rotating black hole.
General Relativity2026-07-301 minarXiv:2607.28044express
Invisible clouds around spinning black holes
A black hole is a gargantuan cosmic whirlpool that drags in everything nearby. But beyond visible matter, an invisible mist can hover in its vicinity — dark matter. Physicists have studied its behavior. Unlike ordinary matter, the field doesn’t necessarily fall through the horizon.
General Relativity2026-07-291 minarXiv:2607.27129express
Chaos in the Shadow of a Black Hole
A star circles a rotating black hole like a figure skater at the center of a rink. While it is far away and can be treated as a point, the dance remains predictable: the orbit follows clear laws, like music that is easy to glide to. But as it approaches, gravity begins to act unevenly.
General Relativity2026-07-281 minarXiv:2607.25311express
How Black Holes Ring After a Strike
A stone falls into still water — ripples spread across the surface. A black hole behaves similarly when something falls into it or when it merges with another black hole. The hole begins to oscillate, and these oscillations propagate through space as gravitational waves.