Paper 2, Section I, D

Classical Dynamics
Part II, 2021

Show that, in a uniform gravitational field, the net gravitational torque on a system of particles, about its centre of mass, is zero.

Let SS be an inertial frame of reference, and let SS^{\prime} be the frame of reference with the same origin and rotating with angular velocity ω(t)\boldsymbol{\omega}(t) with respect to SS. You may assume that the rates of change of a vector vv observed in the two frames are related by

(dvdt)S=(dvdt)S+ω×v.\left(\frac{d \mathbf{v}}{d t}\right)_{S}=\left(\frac{d \mathbf{v}}{d t}\right)_{S^{\prime}}+\omega \times \mathbf{v} .

Derive Euler's equations for the torque-free motion of a rigid body.

Show that the general torque-free motion of a symmetric top involves precession of the angular-velocity vector about the symmetry axis of the body. Determine how the direction and rate of precession depend on the moments of inertia of the body and its angular velocity.