A bead starts from rest at a point and slides without friction along a wire

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Mechanics & Dynamical Systems · Lagrangian mechanics

Action and Symmetry, Ch The action, the first variation and the boundary term

Problem

A bead starts from rest at a point OO and slides without friction along a wire, under uniform gravity g=9.8 m s−2g=9.8\,\mathrm{m\,s^{-2}}, to a vertical wall a horizontal distance D=1.2 mD=1.2\,\mathrm{m} from OO. The wire is shaped to make the travel time stationary, and the height at which it meets the wall is left free. Measure xx horizontally and yy downward from OO, so that the travel time is 12g∫0D1+y′2y dx\dfrac{1}{\sqrt{2g}}\displaystyle\int_0^D\sqrt{\dfrac{1+y'^2}{y}}\,\mathrm{d}x. ((a)) State the condition that the free end imposes where the wire meets the wall, and say why. ((b)) Show that the curve x=R(ϕ−sin⁡ϕ)x=R(\phi-\sin\phi), y=R(1−cos⁡ϕ)y=R(1-\cos\phi), with RR a constant length and ϕ\phi a parameter, satisfies the Beltrami first integral y(1+y′2)=constanty(1+y'^2)=\text{constant} of this integrand, and find the constant. Then use part (a) to find RR and the depth y2y_2 at which the wire meets the wall. ((c)) Using energy conservation for the bead's speed, show that the travel time along this curve is πR/g\pi\sqrt{R/g}, and evaluate it. ((d)) Find the shortest time for the bead to reach the wall along any straight ramp from OO, and compare it with part (c).

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