A3.2

Principles of Dynamics | Part II, 2003

(i) An axisymmetric bowling ball of mass MM has the shape of a sphere of radius aa. However, it is biased so that the centre of mass is located a distance a/2a / 2 away from the centre, along the symmetry axis.

The three principal moments of inertia about the centre of mass are (A,A,C)(A, A, C). The ball starts out in a stable equilibrium at rest on a perfectly frictionless flat surface with the symmetry axis vertical. The symmetry axis is then tilted through θ0\theta_{0}, the ball is spun about this axis with an angular velocity nn, and the ball is released.

Explain why the centre of mass of the ball moves only in the vertical direction during the subsequent motion. Write down the Lagrangian for the ball in terms of the usual Euler angles θ,ϕ\theta, \phi and ψ\psi.

(ii) Show that there are three independent constants of the motion. Eliminate two of the angles from the Lagrangian and find the effective Lagrangian for the coordinate θ\theta.

Find the maximum and minimum values of θ\theta in the motion of the ball when the quantity C2n2AMga\frac{C^{2} n^{2}}{A M g a} is (a) very small and (b) very large.

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