Paper 4, Section II, A

Dynamics and Relativity
Part IA, 2017

(a) A rocket moves in a straight line with speed v(t)v(t) and is subject to no external forces. The rocket is composed of a body of mass MM and fuel of mass m(t)m(t), which is burnt at constant rate α\alpha and the exhaust is ejected with constant speed uu relative to the rocket. Show that

(M+m)dvdtαu=0.(M+m) \frac{d v}{d t}-\alpha u=0 .

Show that the speed of the rocket when all its fuel is burnt is

v0+ulog(1+m0M)v_{0}+u \log \left(1+\frac{m_{0}}{M}\right)

where v0v_{0} and m0m_{0} are the speed of the rocket and the mass of the fuel at t=0t=0.

(b) A two-stage rocket moves in a straight line and is subject to no external forces. The rocket is initially at rest. The masses of the bodies of the two stages are kMk M and (1k)M(1-k) M, with 0k10 \leqslant k \leqslant 1, and they initially carry masses km0k m_{0} and (1k)m0(1-k) m_{0} of fuel. Both stages burn fuel at a constant rate α\alpha when operating and the exhaust is ejected with constant speed uu relative to the rocket. The first stage operates first, until all its fuel is burnt. The body of the first stage is then detached with negligible force and the second stage ignites.

Find the speed of the second stage when all its fuel is burnt. For 0k<10 \leqslant k<1 compare it with the speed of the rocket in part (a) in the case v0=0v_{0}=0. Comment on the case k=1k=1.