3.I.9C

Classical Dynamics | Part II, 2006

A pendulum of length \ell oscillates in the xyx y plane, making an angle θ(t)\theta(t) with the vertical yy axis. The pivot is attached to a moving lift that descends with constant acceleration aa, so that the position of the bob is

x=sinθ,y=12at2+cosθ.x=\ell \sin \theta, \quad y=\frac{1}{2} a t^{2}+\ell \cos \theta .

Given that the Lagrangian for an unconstrained particle is

L=12m(x˙2+y˙2)+mgy,L=\frac{1}{2} m\left(\dot{x}^{2}+\dot{y}^{2}\right)+m g y,

determine the Lagrangian for the pendulum in terms of the generalized coordinate θ\theta. Derive the equation of motion in terms of θ\theta. What is the motion when a=ga=g ?

Find the equilibrium configurations for arbitrary aa. Determine which configuration is stable when

 (i) a<g\text { (i) } a<g

and when

 (ii) a>g\text { (ii) } a>g \text {. }

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