Virtual laboratory/Physics/Astrophysics/Black hole — the Schwarzschild radius

Black hole — the Schwarzschild radius

Compress a mass into a small enough region and you get a black hole. Its event horizon has radius R_s=2GM/c² and grows linearly with mass. Nothing escapes from beneath the horizon — not even light (the escape velocity exceeds c). As a black hole, Earth would be ~9 mm across, the Sun ~3 km. Change the mass of the object.

Black hole — the Schwarzschild radius
Physics · Astrophysics · Schwarzschild radius (FIZ.ASTR)
Mass of the object MM (log scale)1.00 M☉
The greater the mass of the object, the event horizon (Schwarzschild radius) will be:
mass M
1.99e+30 kg
in solar masses
1.00 M☉
radius Rₛ
2.95 km
Rₛ in metres
2.95e+3 m
🎯 Challenge: how much mass for the event horizon to reach a given size?

What just happened?

You doubled the mass, and the event horizon grew exactly twofold. The Schwarzschild radius is directly (linearly) proportional to mass — there is no power or root involved.

Schwarzschild radius:

Rs=2GMc2R_s = \dfrac{2GM}{c^2}

— where MM is the mass of the object, GG — the gravitational constant, cc — the speed of light. It is the radius of the ball into which the mass MM must be compressed for it to become a black hole.

What is the event horizon?

It is the boundary around a black hole with radius RsR_s. Nothing escapes from beneath it — neither matter nor light. It is not a physical surface but a “point of no return”: every path outward leads back inside.

Why does even light not escape?

The escape velocity grows with mass and falls with distance. At the event horizon it reaches the value cc — the speed of light. Closer to the centre it would have to exceed cc, and nothing moves faster than light. That is why a photon aimed “outward” falls inward anyway.

How small would Earth or the Sun be?

If you compressed the entire Earth into a black hole, its horizon would have a radius of ≈ 9 mm — smaller than a walnut. The Sun would fit into a ball of radius ≈ 3 km. Black holes are not “large” — they are extremely dense.

Why this matters for your exam:

The formula Rs=2GM/c2R_s = 2GM/c^2 is a classic astrophysics problem: plug in the mass, compute the radius, compare it with the size of the object. The trick: RsR_s grows linearly with mass — 10× more mass means a 10× larger horizon, no more, no less.

Remember: the event horizon is the boundary from beneath which nothing escapes, and its radius Rs=2GM/c2R_s = 2GM/c^2 grows linearly with mass: Rs∝MR_s \propto M.

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Theory & formulas

The Schwarzschild radius

The event horizon has radius: Rs=2GMc2R_s = \dfrac{2GM}{c^2} It grows linearly with mass. Nothing escapes from beneath the horizon — the escape velocity exceeds cc.

Where it comes from

Set the escape velocity equal to cc: 2GM/R=c\sqrt{2GM/R}=c gives R=2GM/c2R=2GM/c^2. The same result follows from general relativity.

Scale

Earth as a black hole: Rs≈9 mmR_s\approx9\ \mathrm{mm}; the Sun: Rs≈3 kmR_s\approx3\ \mathrm{km}.

Notation: RsR_s — Schwarzschild radius, GG — gravitational constant, MM — mass, cc — speed of light.

Frequently asked questions

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What is the Schwarzschild radius?

The radius of a black hole's event horizon: R_s=2GM/c². It marks the boundary from beneath which nothing can escape.

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Why does light not escape from a black hole?

Because beneath the horizon the escape velocity exceeds the speed of light c — even a photon lacks enough "speed" to get out.

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How small would Earth be as a black hole?

You would have to compress its entire mass down to a radius of ~9 mm — then R_s=2GM/c² creates an event horizon.

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