Paper 2, Section II, B

Classical Dynamics
Part II, 2013

(i) The action for a system with a generalized coordinate qq is given by

S=t1t2L(q,q˙,t)dtS=\int_{t_{1}}^{t_{2}} L(q, \dot{q}, t) d t

(a) State the Principle of Least Action and derive the Euler-Lagrange equation.

(b) Consider an arbitrary function f(q,t)f(q, t). Show that L=L+df/dtL^{\prime}=L+d f / d t leads to the same equation of motion.

(ii) A wire frame ABCA B C in a shape of an equilateral triangle with side aa rotates in a horizontal plane with constant angular frequency ω\omega about a vertical axis through AA. A bead of mass mm is threaded on BCB C and moves without friction. The bead is connected to BB and CC by two identical light springs of force constant kk and equilibrium length a/2a / 2.

(a) Introducing the displacement η\eta of the particle from the mid point of BCB C, determine the Lagrangian L(η,η˙)L(\eta, \dot{\eta}).

(b) Derive the equation of motion. Identify the integral of the motion.

(c) Describe the motion of the bead. Find the condition for there to be a stable equilibrium and find the frequency of small oscillations about it when it exists.