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Schwarzschild Radius Calculator

Calculator

Results

Enter values to see results

Schwarzschild Radius

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m

Schwarzschild Radius

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km

Ratio: Rs / Actual Radius

—

Density Required for Collapse

—

kg/m³

Results

Enter values to see results

Schwarzschild Radius

—

m

Schwarzschild Radius

—

km

Ratio: Rs / Actual Radius

—

Density Required for Collapse

—

kg/m³

The Schwarzschild Radius Calculator computes the critical radius at which any object, if compressed to that size, would become a black hole. Named after Karl Schwarzschild who derived it in 1916, the Schwarzschild radius is the radius of the event horizon — the point of no return for a non-rotating black hole — and is one of the most fundamental quantities in general relativity.

The Schwarzschild radius is derived from Einstein's field equations: Rs = 2GM/c², where G is the gravitational constant (6.674x10-11 N m² kg-2), M is the mass in kilograms, and c is the speed of light (2.998x10^8 m/s). The factor of 2 reflects the full general relativistic treatment — the Newtonian escape velocity formula v = sqrt(2GM/r) gives the same numerical result when set equal to c, but this is a coincidence; the physics is fundamentally different in GR.

The Schwarzschild radius scales linearly with mass: double the mass, double the Schwarzschild radius. For the Sun, Rs = 2 x 6.674e-11 x 1.989e30 / (2.998e8)^2 ≈ 2,953 m ≈ 2.95 km. The Sun is currently about 696,000 km in radius — about 236,000 times larger than its Schwarzschild radius. To become a black hole, it would need to be compressed to a sphere with a 3 km radius.

For Earth, Rs ≈ 8.87 mm — so Earth would need to be compressed to a marble-sized sphere to become a black hole. For a human body of 70 kg, Rs ≈ 1.04x10-25 m — far smaller than an atomic nucleus.

The density required to collapse an object into a black hole decreases dramatically with increasing mass (density scales as 1/M^2). This is why supermassive black holes can have average densities less than water, yet stellar remnants require nuclear densities to become stellar-mass black holes.

How It Works

Schwarzschild radius: Rs = 2GM/c², where G = 6.674x10-11 N m² kg-2, c = 2.998x10^8 m/s. For solar masses: Rs(km) = 2.953 x M_solar. For Earth masses: Rs(mm) = 8.87 x M_earth. The ratio Rs/R_object shows how far an object is from being a black hole. Required collapse density: rho = M / (4/3 pi Rs^3), treating the black hole as a uniform sphere of radius Rs.

Understanding Your Results

Rs/R_object ratio: Sun = 0.000004 (needs 236,000x compression). Earth = 0.0000014 (needs 718,000x compression). Neutron star = 0.3 to 0.5 (close to collapse). Typical stellar-mass black hole has Rs = 3-100 km. Supermassive black holes have Rs = millions to billions of km.

Worked Examples

The Sun

Inputs

mass value1
mass unitsolar

Results

rs m2953
rs km2.953
rs vs object0.00000424
density required18400000000000000000

The Sun's Schwarzschild radius is about 2.95 km. The Sun would need to be compressed by a factor of ~236,000 in radius (or ~10^16 in volume) to become a black hole.

Earth

Inputs

mass value1
mass unitearth

Results

rs m0.008872
rs km0.000008872
rs vs object0.00000139
density required2.04e+30

Earth's Schwarzschild radius is about 8.87 mm. Compressing Earth to the size of a marble would create a black hole with mass equal to that of Earth.

Frequently Asked Questions

The Schwarzschild radius is the radius of the event horizon of a non-rotating (Schwarzschild) black hole. It is the critical size an object must be compressed to in order for its escape velocity to equal the speed of light: Rs = 2GM/c². Any mass compressed below its Schwarzschild radius collapses into a black hole.

Yes. Every object with mass has a Schwarzschild radius, calculated as Rs = 2GM/c². However, for ordinary matter, this radius is far below the actual size of the object. It represents a hypothetical limit: if you compressed all of Earth into a sphere less than 8.87 mm in radius, it would become a black hole.

Theoretically yes, if compressed to below their Schwarzschild radius. For a 70 kg person, this is about 1x10-25 m — about 10 orders of magnitude smaller than a proton. In practice, no known physical process could create such compression outside of the extreme environments near already-existing black holes.

From Rs = 2GM/c², increasing mass M proportionally increases Rs. Doubling the mass doubles the Schwarzschild radius. This contrasts with the density needed for collapse: since density goes as M/Rs^3 = M/(2GM/c^2)^3 = c^6/(8G^3 M^2), more massive objects require LOWER density to become black holes.

A Schwarzschild black hole is non-rotating — a perfectly spherical solution to Einstein's equations with only a single parameter (mass). A Kerr black hole is rotating and has two parameters (mass and angular momentum). Real astrophysical black holes are expected to be Kerr black holes since they form from rotating stellar cores. Kerr black holes have two horizons and an ergosphere — a region outside the event horizon where rotation of spacetime cannot be avoided.

No. The event horizon is a mathematical boundary — a surface of no return — not a physical surface. An observer falling through the event horizon would not feel anything special locally at the moment of crossing. The event horizon is defined globally: it is the boundary from within which no signal can ever escape to infinity. Its location can only be determined in retrospect, given the entire future evolution of the spacetime.

Neutron stars are the densest known stable objects, with masses of 1.4-2.5 solar masses and radii of only 10-12 km. For a 1.4 solar mass neutron star, the Schwarzschild radius is about 4.1 km — roughly one-third the actual radius. Neutron stars are close to but still outside their Schwarzschild radii. Adding mass pushes them toward the limit, and above about 2-3 solar masses, nothing known can halt collapse to a black hole.

Inside the Schwarzschild radius, the time and space coordinates of general relativity interchange roles — the singularity at r=0 is in the future, not in space, so all trajectories (causal paths through spacetime) inevitably reach the singularity. There is no known mechanism to escape or halt this progression. General relativity predicts a singularity at r=0 (infinite density), but quantum gravity is expected to modify this at Planck scales.

Gravitational waves carry energy but in ordinary astrophysical settings their amplitude is far too small to cause significant compression. Near the merger of two compact objects (neutron stars or black holes), the gravitational wave amplitudes are enormous and the dynamics are governed by full numerical general relativity, with material inevitably crossing the Schwarzschild radius during the final plunge.

The photon sphere is a spherical region at radius 1.5 Rs = 3GM/c^2 around a Schwarzschild black hole where gravity is strong enough that photons orbit in circles. It is unstable — photons slightly inside will spiral in, and slightly outside will spiral out. The photon sphere plays a role in the appearance of black hole shadows observed by the Event Horizon Telescope.

Sources & Methodology

Schwarzschild, K. (1916) — Uber das Gravitationsfeld eines Massenpunktes nach der Einsteinschen Theorie. Misner, Thorne, Wheeler — Gravitation. Hartle, J.B. — Gravity: An Introduction to Einstein's General Relativity.
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