How it works
Konstantin Tsiolkovsky showed in 1903 that a rocket's velocity change depends only on its exhaust velocity and the logarithm of its mass ratio. Because of the logarithm, adding more propellant gives diminishing returns, which is why large rockets use stages.
Reaching low Earth orbit takes about 9.3–10 km/s of Δv in practice: about 7.8 km/s orbital speed plus gravity and drag losses.
Variables
Δv— change in velocity the stage can deliverIsp— specific impulse (seconds)g₀— standard gravity, 9.80665 m/s²m₀, m_f— initial (wet) and final (dry) mass
Assumptions and limits
- Single stage, constant specific impulse
- No gravity losses, drag or steering losses (ideal Δv)
- Thrust acts along the direction of motion
For education only. These models are simplified and are not suitable for spacecraft navigation or safety-critical engineering. See our scientific accuracy policy.