quantity

radius

The distance from the center of a spherical object to its surface or boundary.
6 related articles · 6 formulas

Description

Radius is the distance from the center of a spherical object to its surface or boundary. In physics, the concept of radius appears in countless contexts: from the radius of an atom (about 0.1 nanometers) to the radius of a black hole's event horizon (the Schwarzschild radius). It is a fundamental geometric parameter that determines properties like volume, surface area, and gravitational pull. In the given titles, no specific use is mentioned, but the concept is ubiquitous in describing the size of particles, orbits, lenses, and detectors.

History

The concept of radius dates back to ancient geometry, with Euclid defining the circle by its radius around 300 BCE. The Bohr radius was introduced by Niels Bohr in 1913 in his model of the hydrogen atom. The Schwarzschild radius was derived by Karl Schwarzschild in 1916 from Einstein's field equations.

How it works

The radius is defined as half the diameter of a sphere or circle. In physics, it often enters formulas through geometric relationships: for a sphere, volume = (4/3)πr³ and surface area = 4πr². In dynamics, the radius of curvature describes how sharply a path bends. In quantum mechanics, the Bohr radius (about 0.053 nm) sets the scale for hydrogen-like atoms. In relativity, the Schwarzschild radius r_s = 2GM/c² defines the size of a black hole for a given mass M.

In practice

Radius is used in designing optical lenses, particle accelerators (bending radius of magnets), and in medical imaging to characterize tumors or blood vessels.

Fun fact

The Earth's radius is not constant: it is about 22 kilometers larger at the equator than at the poles due to the planet's rotation, making it an oblate spheroid rather than a perfect sphere.

Concept graph →

Formulas

$$\frac{2GM}{c^2 R} \leq \frac{8}{9}$$
Maximum compactness for a stable spherical object.
What is in the formula
Gvariablegravitational constant — gravitational constant cubic metre per kilogram per second squared
Mvariablemass of the object — mass kilogram
Rvariableradius of the object — radius metre
cvariablespeed of light in vacuum — speed of light metre per second
$$v^2 = \frac{G M}{r}$$
Orbital speed squared equals gravitational constant times mass over radius.
What is in the formula
vvariableorbital speed — velocity metre per second
Mvariablecentral mass — mass kilogram
rvariableorbital radius — radius metre
GconstantUniversal constant of gravitation, determining the strength of gravitational force. — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
$$r_H \propto \frac{\dot{M}}{\rho c_s}$$
Horizon radius scales with accretion rate over density and sound speed.
What is in the formula
r_HvariableAccretion horizon radius — radius metre
\dot{M}variableMass accretion rate — mass flow rate kilogram per second
\rhovariableMass density of accreting material — mass density kilogram per cubic metre
c_svariableSound speed in accreting material — speed metre per second
$$\dot{r}^2 = \frac{2GM(r)}{r} - k$$
Describes radial motion with density-dependent critical factor.
What is in the formula
rvariableradial coordinate (distance from center) — radius metre
M(r)variableenclosed mass within radius r — mass kilogram
kvariableconstant of motion (related to energy per unit mass) — specific energy metre squared per second squared
GconstantNewtonian constant of gravitation, fundamental strength of gravity — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
˙operatorderivative with respect to time — time derivative
$$r_s = \frac{2GM}{c^2}$$
Radius of event horizon for non-rotating black hole.
What is in the formula
r_svariableSchwarzschild radius — radius metre
MvariableMass of the black hole — mass kilogram
GconstantConstant of gravitation in Newton's law — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
cconstantSpeed of light in vacuum — speed of light = 299792458 metre per second
$$\Gamma_1 > \frac{4}{3} + k\frac{GM}{Rc^2}$$
Stellar stability requires adiabatic index above 4/3 plus GR correction.
What is in the formula
\Gamma_1variableFirst adiabatic index — adiabatic index
MvariableMass of the star — mass kilogram
RvariableRadius of the star — radius metre
cvariableSpeed of light — speed metre per second
GconstantNewtonian gravitational constant — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
kconstantNumerical constant of order unity depending on stellar structure — structure constant = 1

Related articles · 6

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.
Horizon Equalizer: How the Whisper of the Abyss Was Heard in Gravitational Noise
The merger of two black holes is not just a silent dance, but a grand act after which spacetime itself vibrates for a long time. These damped oscillations — quasi-normal modes — are like the ringing of a gigantic bell. But there is another echo: barely perceptible, almost ghostly.
HEP Theory2026-06-291 minarXiv:2606.30794express
A Black Hole in a Fluffy Fur Coat
An ordinary black hole is surrounded by a thin photon sphere — a place where light can loop around before falling in or escaping. In the new work, this region has puffed up into a whole layer packed with massless particles that zip around at nearly the speed of light and don't press against the walls.
General Relativity2026-06-281 minarXiv:2606.29307express
Quantum Ripples Around a Black Hole
A textbook black hole resembles a perfectly smooth sphere: everything outside it calmly flies off to infinity. However, quantum gravity paints a different picture. Recently, within loop quantum gravity, a solution was found — a 'Kruskal' black hole where spacetime beyond the horizon behaves differently.
Long-Throat Wormholes: How Doppler Notes Give Them Away
When a black hole steps into the lens, it leaves a perfect darkness in the image — a gravitational well where light falls forever.
General Relativity2026-03-031 minarXiv:2603.03421express
Minimal Shadow Size of a Black Hole
A black hole is like a dark ball in space onto which luminous matter falls. A black hole has a shadow — a region from which rays cannot escape. But due to light bending, the shadow appears larger than the hole itself: just like a ball's shadow on a wall grows bigger when the lamp is far away.