Schwarzschild Radius Calculator

Calculate the event horizon radius of a black hole from its mass. Includes photon sphere, ISCO, Hawking temperature, and famous black hole comparisons.

Schwarzschild Radius Calculator

Schwarzschild Radius
2.9540 km
R_s = 2GM/c² = 2.9540e+3 m
Radius (Solar Radii)
0.000004
1 R☉ = 695,700 km
Radius (AU)
1.9746e-8
In astronomical units
Photon Sphere
4.4310 km
= 1.5 × R_s — light orbits the black hole here
ISCO
8.8619 km
= 3 × R_s — innermost stable circular orbit
Hawking Temperature
6.1689e-8 K
Extremely cold for stellar-mass BHs; hotter for tiny BHs
Evaporation Time
2.10e+67 years
Time for complete Hawking evaporation
Event Horizon Area
1.0965e+8 m²
4π R_s² — proportional to entropy
Key Radii Comparison
Event Horizon
2.95 km
Photon Sphere
4.43 km
ISCO
8.86 km

Famous Black Holes

NameMass (M☉)R_s (km)R_s (AU)Distance (ly)Type
Cygnus X-121.262.64.186e-76,070.00Stellar
V404 Cygni9.026.61.777e-77,800.00Stellar
Sagittarius A*4.0e+61.182e+77.898e-226,000.00Supermassive
M87*6.5e+91.920e+101.283e+25.40e+7Supermassive
TON 6186.6e+101.950e+111.303e+31.04e+10Ultramassive
Phoenix A1.0e+112.954e+111.975e+35.70e+9Ultramassive
Planning notes, formulas, and examples

About the Schwarzschild Radius Calculator

The Schwarzschild radius defines the event horizon of a non-rotating black hole — the boundary beyond which nothing, not even light, can escape. First derived by Karl Schwarzschild in 1916 from Einstein's general relativity field equations, this radius is directly proportional to the black hole's mass: Rs = 2GM/c².

Black holes span an enormous range of sizes: stellar-mass black holes from collapsed stars have radii of a few kilometers, supermassive black holes at galaxy centers can be larger than our solar system, and hypothetical primordial micro black holes might be smaller than an atom.

This calculator computes the Schwarzschild radius along with related properties — the photon sphere, the innermost stable circular orbit (ISCO), Hawking radiation temperature, and estimated evaporation time. A comparison mode lets you check whether any given object compressed to its mass would form a black hole, and a reference table of famous black holes provides real-world context.

When This Page Helps

This calculator helps you move from a black-hole mass to the key scales that matter near the horizon. It is useful when comparing stellar-mass and supermassive black holes, checking whether an object would collapse into a black hole at a given radius, or building intuition for how quickly black-hole size grows with mass.

How to Use the Inputs

  1. Enter the mass of the object in kilograms, solar masses, Earth masses, or Jupiter masses.
  2. Use preset buttons for the Sun, Earth, or famous black holes like Sagittarius A*.
  3. Switch to "Compare to Object Size" mode to check if an object would become a black hole at its current mass.
  4. Enter the object's actual radius in meters for the comparison.
  5. Review all outputs: Schwarzschild radius, photon sphere, ISCO, Hawking temperature.
  6. Explore the famous black holes table for real-world comparisons.
Formula used
Schwarzschild radius: R_s = 2GM/c², where G = 6.674 × 10⁻¹¹ m³/(kg·s²), M is mass (kg), c = 2.998 × 10⁸ m/s. Photon sphere: r_ph = 1.5 R_s. ISCO: r_isco = 3 R_s. Hawking temperature: T = ℏc³/(8πGMk_B).

Example Calculation

Result: R_s ≈ 2.953 km

If the Sun were compressed into a black hole, its event horizon would have a radius of about 2.95 km. Its photon sphere would be at 4.43 km and the ISCO at 8.86 km.

Tips & Best Practices

  • The Schwarzschild radius scales linearly with mass — 10× the mass gives 10× the radius.
  • Sagittarius A* (4 million M☉) has R_s ≈ 12 million km — about 17 solar radii.
  • Hawking evaporation time for stellar-mass BHs far exceeds the age of the universe.
  • An object is a black hole if its actual radius is smaller than its Schwarzschild radius.
  • The density required for a BH decreases as mass increases — supermassive BHs can be less dense than water.

Event Horizon Scale

The Schwarzschild radius grows linearly with mass. That makes it a clean way to compare compact objects, from stellar remnants to galaxy-center black holes, without needing a more complex rotating solution.

Nearby Radii

The photon sphere and ISCO show where light and matter can still orbit before becoming unstable. Those values are useful for thinking about accretion disks, lensing, and the appearance of the shadow around a non-rotating black hole.

Physical Limits

Hawking temperature and evaporation time are included for context, not for everyday engineering use. For stellar and supermassive black holes, the evaporation time is far longer than the age of the universe, so the practical takeaway is usually the horizon scale and orbital distances.

Sources & Methodology

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Frequently Asked Questions

  • The radius of the event horizon of a non-rotating (Schwarzschild) black hole. Any object compressed within its Schwarzschild radius would become a black hole.