Speed gained by rocket. u = exhaust speed relative to rocket, m₀ = initial mass, m = current mass.
The situation
A rocket in free space (no gravity, no air resistance) ejects exhaust gas at speed u relative to the rocket. The rocket starts with mass m0 and velocity v0. After burning fuel until mass reduces to m, what is the rocket's velocity v?
v−v0=ulnmm0
Derivation
At time t: rocket has mass M and velocity v.
In a small time dt: rocket ejects mass ∣dM∣ (so rocket mass decreases: dM<0).
The exhaust moves at velocity v−u (rocket velocity minus exhaust speed relative to rocket).
Conservation of momentum:
Before: total momentum =Mv
After: rocket has mass M+dM and velocity v+dv. Exhaust has mass −dM and velocity v−u.
Mv=(M+dM)(v+dv)+(−dM)(v−u)
Mv=Mv+Mdv+vdM+dMdv−vdM+udM
Drop the second-order term dMdv:
0=Mdv+udM
Mdv=−udM
dv=−uMdM
Integrate from m0 to m (mass) and v0 to v (velocity):
∫v0vdv=−u∫m0mMdM
v−v0=−u[lnM]m0m=−u(lnm−lnm0)=ulnmm0
v−v0=ulnmm0
Understanding the result
Since m0>m (mass decreases as fuel burns), lnmm0>0 — the rocket speeds up.
Δv=ulnmm0
- Larger exhaust speed u → more Δv per kg of fuel
- Larger mass ratio m0/m → more Δv (but diminishing returns due to the logarithm)
The mass ratio problem
To achieve Δv=u (speed equal to exhaust speed):
mm0=e≈2.718
About 63% of the initial mass must be fuel.
To achieve Δv=2u:
mm0=e2≈7.39
About 86% must be fuel.
To achieve Δv=3u:
mm0=e3≈20
About 95% must be fuel. The diminishing returns of the logarithm make very high velocities extremely costly in fuel mass. This is the fundamental challenge of rocket propulsion.
With gravity
In a gravitational field g (rocket launching vertically):
v−v0=ulnmm0−gt
The gravity term −gt reduces the velocity gain. This is why multi-stage rockets are used — discarding empty fuel tanks reduces the mass being accelerated.
Note
This equation was derived by Konstantin Tsiolkovsky in 1903 — before any rocket had ever flown. It is the fundamental equation that governs all rocket propulsion, from fireworks to the Saturn V.