Escape Velocity Calculator
Calculate the minimum speed needed to escape the gravity of a planet, moon, star, or other spherical celestial body.
About escape velocity
Escape velocity examples
These ideal surface values use mean mass and radius data.
| Celestial body | Escape velocity | Interpretation |
|---|---|---|
| Earth: 5.972e24 kg, 6,371 km | 11.186 km/s | Ideal speed from mean sea-level radius. |
| Moon: 7.342e22 kg, 1,737.4 km | 2.376 km/s | Low gravity makes lunar escape much easier. |
| Mars: 6.4171e23 kg, 3,389.5 km | 5.027 km/s | Uses Mars's mean planetary radius. |
How to calculate escape velocity
- Enter the celestial body's mass in kilograms, using scientific notation for very large values if convenient.
- Enter the distance from the body's center in meters; for a surface launch, use its mean radius.
- Select Calculate Escape Velocity to evaluate the classical gravitational equation.
- Read the result in meters per second and kilometers per second, then account separately for real mission losses.
Escape velocity FAQ
Does the escaping object's mass affect escape velocity?
No, its mass cancels when kinetic and gravitational potential energy are equated. A heavier object needs more total energy, but the ideal threshold speed is unchanged.
Why do rockets not launch instantly at 11.2 km/s?
Rockets add speed progressively while climbing and can follow an orbital trajectory before departing Earth. Atmospheric drag, gravity losses, and propulsion efficiency also make the practical maneuver different from the ideal calculation.
Is escape velocity the same at every altitude?
No, it decreases as distance from the body's center increases. Add altitude to the mean radius when calculating from a point above the surface.
How is escape velocity related to orbital velocity?
At a given radius, ideal escape velocity is sqrt(2) times the circular orbital velocity. Both relationships assume a spherical body and a two-body Newtonian model.
Can this equation be used for black holes?
Not reliably near a black hole or another extremely compact object. General relativity is required when spacetime curvature is strong and the classical result approaches the speed of light.