Classical Mechanics (Kibble & Berkshire) · Problem 14.6

The general theory of small oscillations — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · hamiltonian-shortening-string-pendulum

Problem

Pendulum with a shortening string A particle is suspended from a support by a light inextensible string which passes through a small fixed ring vertically below the support. The particle moves in a vertical plane with the string taut. At the same time, the support is made to move vertically having an upward displacement Z(t)Z(t) at time tt. The effect is that the particle oscillates like a simple pendulum whose string length at time tt is a−Z(t)a - Z(t), where aa is a positive constant. Show that the Lagrangian is L=12m((a−Z)2θ˙2+Z˙2)+mg(a−Z)cos⁡θ,L = \tfrac{1}{2}m\left((a-Z)^2\dot{\theta}^2 + \dot{Z}^2\right) + mg(a-Z)\cos\theta, where θ\theta is the angle between the string and the downward vertical. Find the Hamiltonian and obtain Hamilton's equations. Is HH conserved?

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