Earth gives you a push
Launch eastward near the equator and Earth’s spin hands you ~0.46 km/s of sideways speed—almost 4% of the surface escape velocity for free.
The concept of escape velocity is central to spaceflight and planetary science. It is the minimum speed required for an object to break free from the gravitational attraction of a planet, moon, or star without any further propulsion. Mathematically, the escape velocity at a distance r from the center of a body with gravitational parameter μ (the product of the gravitational constant G and the body’s mass M) is given by:
vesc = √(2μ / r) with r = R + h
Here R is the mean radius of the body and h is the altitude above that surface. For comparison, the circular orbital speed at the same altitude is vcirc = √(μ / r). This leads to the elegant relation vesc = √2 · vcirc. In other words, escape velocity is about 41% higher than the speed needed to maintain a stable circular orbit at the same radius.
The values of escape velocity vary widely depending on the body. On Earth’s surface, the required speed is about 11.2 km/s (roughly 25,000 mph). At a 400 km altitude, such as the orbit of the International Space Station, the value is slightly reduced because the spacecraft is farther from Earth’s center of mass. The Moon, being much smaller, requires only about 2.38 km/s, which explains why Apollo lunar ascent modules could reach orbit with modest engines. Mars, larger than the Moon but smaller than Earth, has a surface escape velocity of about 5.0 km/s. Gas giants such as Jupiter or Saturn have escape velocities exceeding 50 km/s at their visible clouds, making them far more difficult to leave.
Escape velocity does not mean a spacecraft must instantly accelerate to that speed. Rockets work gradually, continually adding energy through thrust until the spacecraft’s total mechanical energy becomes positive. However, the concept provides an important benchmark for mission design, energy requirements, and comparisons between different worlds. Launch vehicles such as the Saturn V or SpaceX Falcon Heavy do not “jump” to 11 km/s but steadily build up orbital velocity, followed by additional burns to exceed escape conditions on interplanetary missions.
This calculator assumes an idealized spherical body, no atmosphere, and no planetary rotation. In reality, factors such as atmospheric drag, launch site latitude, Earth’s rotation, and gravitational perturbations significantly influence the velocity needed to actually escape. Nevertheless, the simple formula remains a cornerstone of introductory physics, astronomy education, and quick back-of-the-envelope engineering calculations.
Disclaimer: This tool is for educational purposes only. It ignores atmosphere, drag, oblateness, and operational constraints. Use professional mission analysis software for real spacecraft design.
Launch eastward near the equator and Earth’s spin hands you ~0.46 km/s of sideways speed—almost 4% of the surface escape velocity for free.
Small asteroids like Bennu have escape speeds under 0.2 m/s. A gentle hop could launch you into space unless you’re tethered down.
No matter the planet, escape speed is always √2 times faster than a circular orbit at the same altitude—so a 3 km/s circular orbit means a 4.24 km/s escape burn.
Kinetic energy scales with v², so doubling escape velocity would need four times the energy per kilogram—one reason super-heavy worlds are so unforgiving.
The “black” in black hole means the escape velocity at the event horizon exceeds the speed of light, so not even photons can reach infinity.