The first law of black hole mechanics relates changes in mass, angular momentum, and horizon area to energy conservation in black hole thermodynamics.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.
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.
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.
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.
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.
| δM | variable | Infinitesimal change in black hole mass — mass kilogram |
| κ | variable | Surface gravity of the black hole — surface gravity metre per second squared |
| δA | variable | Infinitesimal change in horizon area — area square metre |
| Ω_H | variable | Angular velocity of the horizon — angular velocity radian per second |
| δJ | variable | Infinitesimal change in angular momentum — angular momentum kilogram square metre per second |
| δ | operator | Infinitesimal variation of a quantity — variation |
| dU | variable | Infinitesimal change in internal energy — internal energy joule |
| δQ | variable | Infinitesimal heat added to the system — heat joule |
| δW | variable | Infinitesimal work done by the system — work joule |
| d | operator | Exact differential of a state function — exact differential |
| δ | operator | Inexact differential for path-dependent quantities — inexact differential |
| \Delta(r) | variable | Horizon function of the Kerr metric — horizon function square metre |
| r | variable | Radial coordinate (Boyer-Lindquist) — radial coordinate metre |
| M | variable | Black hole mass — mass kilogram |
| a | variable | Specific angular momentum (spin parameter) — specific angular momentum metre |









