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Black Hole Calculator

Last updated: April 5, 2026

The Black Hole Calculator computes Schwarzschild radius, Hawking temperature, event horizon area, and gravitational time dilation for any black hole mass. A single tool covering all key black hole physics parameters — from stellar-mass to supermassive black holes at galactic centers.

Calculator

Results

Mass

1.9885e+31

kg

Mass

10

M☉

Schwarzschild Radius

29.533394

km

Photon Sphere Radius

44.300091

km

Surface Gravity at Event Horizon

1,521,591,430,016.805

m/s²

Hawking Temperature

0.00000000617

K

Average Density Inside Schwarzschild Radius

1.842852e+17

kg/m³

Light Crossing Time Across Radius

98.512798

µs

Results

Mass

1.9885e+31

kg

Mass

10

M☉

Schwarzschild Radius

29.533394

km

Photon Sphere Radius

44.300091

km

Surface Gravity at Event Horizon

1,521,591,430,016.805

m/s²

Hawking Temperature

0.00000000617

K

Average Density Inside Schwarzschild Radius

1.842852e+17

kg/m³

Light Crossing Time Across Radius

98.512798

µs

In This Guide

  1. 01The Schwarzschild Radius: Event Horizon Size
  2. 02Hawking Radiation Temperature
  3. 03Event Horizon Surface Area and the Bekenstein-Hawking Entropy
  4. 04Gravitational Time Dilation at the Event Horizon

A black hole is defined entirely by three quantities: mass, spin, and charge. From mass alone (for non-rotating, uncharged Schwarzschild black holes), all fundamental properties — the size of the event horizon, the temperature at which it radiates, the degree to which time is distorted near it — are calculable from exact formulas derived from general relativity. The black hole calculator computes all these properties simultaneously for any mass input.

The Schwarzschild Radius: Event Horizon Size

The Schwarzschild radius is the radius at which the escape velocity equals the speed of light — the boundary of the event horizon:

r_s = 2GM / c²

where G = 6.674 × 10⁻¹¹ N·m²/kg² (gravitational constant), c = 2.998 × 10⁸ m/s (speed of light), M = mass in kg.

Simplified for solar masses (M_☉ = 1.989 × 10³⁰ kg): r_s ≈ 2.95 × M/M_☉ km

Examples:

  • Sun (if it became a black hole): r_s = 2.95 km (radius 2.95 km; the Sun's actual radius is 696,000 km)
  • 10 solar mass black hole: r_s = 29.5 km — typical stellar-mass black hole
  • Sagittarius A* (4.15 million M_☉, Milky Way center): r_s ≈ 12.2 million km — about 17× the Sun's radius

Use this online calculator for any mass in solar masses, Earth masses, or kilograms. The black hole temperature calculator focuses specifically on Hawking radiation.

Hawking Radiation Temperature

Stephen Hawking's 1974 discovery that black holes emit thermal radiation due to quantum effects near the event horizon:

T_H = ℏc³ / (8πGMk_B)

where ℏ = 1.055 × 10⁻³⁴ J·s (reduced Planck constant), k_B = 1.381 × 10⁻²³ J/K (Boltzmann constant).

Simplified: T_H ≈ 6.17 × 10⁻⁸ K × (M_☉/M)

Practical values: a 10 M_☉ black hole has T_H ≈ 6 × 10⁻⁹ K — immeasurably colder than the cosmic microwave background (2.73 K); Hawking radiation is completely undetectable for any astrophysically realistic black hole. Only hypothetical primordial micro-black holes with masses below about 10¹² kg would have high enough temperatures to radiate detectably.

Event Horizon Surface Area and the Bekenstein-Hawking Entropy

The event horizon area: A = 4πr_s² = 16πG²M²/c⁴

Bekenstein-Hawking entropy: S = k_B × A / (4l_P²) where l_P = √(ℏG/c³) is the Planck length.

For a 10 solar mass black hole: A = 4π × (29,500 m)² ≈ 1.1 × 10¹⁰ m² (11 billion m² ≈ the area of Morocco); entropy ≈ 10⁷⁹ k_B — the immense entropy of black holes underpins the holographic principle and the black hole information paradox. The astronomical calculators and astrophysics calculators provide complementary space science tools.

Gravitational Time Dilation at the Event Horizon

General relativity predicts that time runs slower in stronger gravitational fields. At a distance r from a Schwarzschild black hole: time dilation factor = √(1 − r_s/r). As r approaches r_s, this factor approaches 0 — time appears to freeze at the event horizon from a distant observer's perspective. An infalling observer experiences no frozen time and crosses the event horizon in finite proper time; but a distant observer sees the infalling object asymptotically approach the horizon, redshifting to invisibility, never quite crossing — an illustration of the observer-dependent nature of event horizons in general relativity.

Visual Analysis

How It Works

Enter the black hole mass in solar masses, Earth masses, or kilograms. Schwarzschild radius = 2GM/c². Hawking temperature = ℏc³/(8πGMkB). Event horizon surface area = 4π × rs². Gravitational time dilation at any specified distance r is √(1 − rs/r). All fundamental constants (G, c, ℏ, kB) are applied with their 2018 CODATA values.

Understanding Your Results

Stellar-mass black holes (3-100 solar masses) form from collapsing massive stars. Intermediate-mass black holes range from 100 to 100,000 solar masses. Supermassive black holes at galactic centers range from millions to billions of solar masses. A Hawking temperature above 2.7 K (the CMB temperature) means the black hole is theoretically evaporating — only micro black holes well below 10^11 kg could achieve this.

Worked Examples

Stellar Black Hole

Inputs

mass solar10
mass typesolar

Results

schwarzschild radius m29.53
hawking temp6.17e-9
density18400000000000000
surface gravity bh15200000000000

A typical stellar black hole of 10 solar masses has a Schwarzschild radius of about 29.5 km and an incredibly small Hawking temperature, far below the CMB.

Sagittarius A* (Galactic Center)

Inputs

mass solar4000000
mass typesolar

Results

schwarzschild radius m11803440
hawking temp1.54e-17
density2550
surface gravity bh38000000

The Milky Way's central black hole has a Schwarzschild radius of about 11.8 million km. Its average density is surprisingly low — less than water — because it is so massive.

Frequently Asked Questions

The Schwarzschild radius of the Sun is approximately 2.95 km — if the Sun's entire mass (1.989 × 10³⁰ kg) were compressed into a sphere with radius less than 2.95 km, it would form a black hole. The Sun's actual radius is 696,000 km — about 236,000 times larger than its Schwarzschild radius. The Sun will never become a black hole; it lacks the mass. After its red giant phase (in approximately 5 billion years), the Sun will become a white dwarf. Stellar black holes form from stars with masses above approximately 20 solar masses that end their lives in supernova collapse.
The Schwarzschild radius (r_s = 2GM/c²) is the critical radius at which the escape velocity equals the speed of light. At exactly this radius, not even light can escape — it defines the boundary of the event horizon for a non-rotating (Schwarzschild) black hole. An object compressed below its Schwarzschild radius becomes a black hole. The concept predates general relativity: John Michell (1783) and Pierre-Simon Laplace (1796) independently proposed 'dark stars' using Newtonian mechanics where escape velocity equals c, arriving at the same radius formula. Karl Schwarzschild derived the exact relativistic solution in 1916, published just months before his death while serving on the Eastern Front in World War I.
Hawking radiation arises from quantum field theory effects near the event horizon. In quantum mechanics, the vacuum is not empty — virtual particle-antiparticle pairs constantly appear and annihilate. Near the event horizon, such a pair can appear with one particle inside the horizon and one outside. The outside particle can escape to infinity (appearing as real radiation), while the inside particle falls into the black hole. Energy conservation requires the black hole to lose mass equal to the escaped particle's energy — a net mass decrease. The radiation has a thermal (blackbody) spectrum with temperature inversely proportional to mass: T = ℏc³/(8πGMkB). Hawking radiation is purely a theoretical prediction; no direct observation has been confirmed for astrophysical black holes, which have temperatures far below the CMB background.
TON 618 is currently one of the largest known black holes, with a mass of approximately 66 billion solar masses, giving it a Schwarzschild radius of approximately 194 billion km — about 1,300 AU (Astronomical Units) or 0.006 light-years across. The event horizon of TON 618 is larger than our entire solar system out to the Oort Cloud. For context: Sagittarius A*, the supermassive black hole at the Milky Way's center, has a mass of 4.15 million solar masses and a Schwarzschild radius of 12.2 million km (about 17 solar radii). TON 618 is a hyperluminous quasar located approximately 10.4 billion light-years away, observed as it appeared when the universe was only 3.3 billion years old.
From a distant observer's perspective, an infalling object asymptotically approaches the event horizon, becoming increasingly redshifted and appearing to slow down — never quite crossing the horizon in the observer's time frame. The infalling observer has a completely different experience: they cross the event horizon in finite proper (personal) time and do not experience any local singularity at the boundary. This difference is not a paradox but a feature of general relativity: simultaneity and time flow are observer-dependent. Practically: the redshifting object becomes unobservably faint before the observable time asymptote is reached — an observer watching someone fall into a stellar-mass black hole would see them fade to invisibility within fractions of a second as the redshift exponentially increases.
The Hawking evaporation time scales as M³: T_evap ≈ 5,120 × π × G² × M³ / (ℏ × c⁴). For a stellar mass black hole (10 M_☉): T_evap ≈ 2 × 10⁷⁴ years — incomprehensibly longer than the current age of the universe (1.4 × 10¹⁰ years). For the Hawking evaporation of any astrophysically relevant black hole to complete, the universe would need to be 10⁶⁴ times older than it currently is. A black hole evaporating within the observable universe's lifetime would need a mass below approximately 10¹² kg (smaller than an asteroid) — hypothetical 'primordial' micro-black holes potentially formed in the early universe. The final evaporation stage is an explosive burst of gamma radiation as the mass drops to near-Planck scale.

Sources & Methodology

Schwarzschild, K. (1916). On the Gravitational Field of a Mass Point. Sitzungsberichte der Königlich Preußischen Akademie der Wissenschaften. Hawking, S.W. (1974). Black hole explosions? Nature, 248, 30–31. Bekenstein, J.D. (1973). Black holes and entropy. Physical Review D, 7(8), 2333.

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