
A gravitational singularity is a point in spacetime where gravitational forces become infinite and general relativity breaks down.A gravitational singularity is a region predicted by general relativity (Einstein's theory of gravity) where the density of matter and the curvature of spacetime become infinitely large. Such singularities hide at the centers of black holes and probably existed at the moment of the Big Bang. Under these conditions, normal physical laws break down, so scientists seek a more complete theory—quantum gravity, which will unite gravity and quantum mechanics.
In 1916, Karl Schwarzschild found an exact solution to Einstein's equations for a spherically symmetric mass distribution, which contained a singularity at the center (at r=0). For a long time this was considered a mathematical curiosity. In the 1960s, John Wheeler and his colleagues developed the concept of a black hole as a real astrophysical object. Singularity theorems proved by Roger Penrose (1965) and Stephen Hawking showed that during gravitational collapse a singularity inevitably forms. Later, Hawking applied quantum theory to black holes and predicted radiation that should lead to their evaporation; in doing so, the singularity may be smeared out by quantum fluctuations.
When a star with mass above the Oppenheimer–Volkoff limit (about 3 solar masses) exhausts its nuclear fuel, the pressure of degenerate neutrons is unable to resist gravity. The core collapses, matter is squeezed, and spacetime curves so strongly that the metric of the Schwarzschild equation becomes singular. Inside the event horizon, the radial coordinate becomes timelike, so any motion is directed toward the singularity. Quantum corrections change the scenario: Hawking radiation can carry away mass and, possibly, information; in a full theory of quantum gravity, the singularity is likely smoothed out or disappears.
The study of singularities stimulates the development of quantum gravity theory, which could describe the birth of the Universe in the Big Bang and possibly explain whether wormholes—hypothetical shortcuts through spacetime—could exist.
Although the singularity is hidden by the event horizon, its powerful gravity holds stars in rapid orbits around the center of the Milky Way, betraying the presence of a supermassive black hole.
| v | variable | terminal velocity — velocity metre per second |
| m | variable | mass of the falling object — mass kilogram |
| g | variable | gravitational acceleration — gravitational acceleration metre per square second |
| ρ | variable | density of the fluid — density kilogram per cubic metre |
| A | variable | cross-sectional area — area square metre |
| C_D | variable | drag coefficient — drag coefficient |
| t_{\text{rip}} - t_0 | variable | Time remaining until Big Rip — time interval second |
| w | variable | Equation of state parameter — equation of state parameter |
| \rho_0 | variable | Current dark energy density — energy density joule per cubic metre |
| G | constant | Constant of gravitation in Newton's law — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared |
| \pi | constant | Ratio of circle circumference to diameter — pi = 3.14159 |






