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Rocket Equation (Tsiolkovsky)

Speed gained by rocket. u = exhaust speed relative to rocket, m₀ = initial mass, m = current mass.
Class 11Class JEE
Derivation

The situation

A rocket in free space (no gravity, no air resistance) ejects exhaust gas at speed uu relative to the rocket. The rocket starts with mass m0m_0 and velocity v0v_0. After burning fuel until mass reduces to mm, what is the rocket's velocity vv?

vv0=ulnm0mv - v_0 = u\ln\frac{m_0}{m}

Derivation

At time tt: rocket has mass MM and velocity vv.

In a small time dtdt: rocket ejects mass dM|dM| (so rocket mass decreases: dM<0dM < 0).

The exhaust moves at velocity vuv - u (rocket velocity minus exhaust speed relative to rocket).

Conservation of momentum:

Before: total momentum =Mv= Mv

After: rocket has mass M+dMM + dM and velocity v+dvv + dv. Exhaust has mass dM-dM and velocity vuv - u.

Mv=(M+dM)(v+dv)+(dM)(vu)Mv = (M + dM)(v + dv) + (-dM)(v - u)

Mv=Mv+Mdv+vdM+dMdvvdM+udMMv = Mv + M \, dv + v \, dM + dM \, dv - v \, dM + u \, dM

Drop the second-order term dMdvdM \, dv:

0=Mdv+udM0 = M \, dv + u \, dM

Mdv=udMM \, dv = -u \, dM

dv=udMMdv = -u \frac{dM}{M}

Integrate from m0m_0 to mm (mass) and v0v_0 to vv (velocity):

v0vdv=um0mdMM\int_{v_0}^v dv = -u\int_{m_0}^m \frac{dM}{M}

vv0=u[lnM]m0m=u(lnmlnm0)=ulnm0mv - v_0 = -u[\ln M]_{m_0}^m = -u(\ln m - \ln m_0) = u\ln\frac{m_0}{m}

vv0=ulnm0m\boxed{v - v_0 = u\ln\frac{m_0}{m}}

Understanding the result

Since m0>mm_0 > m (mass decreases as fuel burns), lnm0m>0\ln\frac{m_0}{m} > 0 — the rocket speeds up.

Δv=ulnm0m\Delta v = u\ln\frac{m_0}{m}

  • Larger exhaust speed uu → more Δv\Delta v per kg of fuel
  • Larger mass ratio m0/mm_0/m → more Δv\Delta v (but diminishing returns due to the logarithm)

The mass ratio problem

To achieve Δv=u\Delta v = u (speed equal to exhaust speed):

m0m=e2.718\frac{m_0}{m} = e \approx 2.718

About 63% of the initial mass must be fuel.

To achieve Δv=2u\Delta v = 2u:

m0m=e27.39\frac{m_0}{m} = e^2 \approx 7.39

About 86% must be fuel.

To achieve Δv=3u\Delta v = 3u:

m0m=e320\frac{m_0}{m} = e^3 \approx 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 gg (rocket launching vertically):

vv0=ulnm0mgtv - v_0 = u\ln\frac{m_0}{m} - gt

The gravity term gt-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.