Classical Mechanics (Kibble & Berkshire) · Problem 3.9

Problems in particle dynamics — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · gravitation-continuous-distributions

Problem

A uniform wire of mass MM has the form of a circle of radius aa and a particle of mass mm lies in the plane of the wire at a distance bb (b<ab < a) from the centre OO. Show that the gravitational force exerted by the wire on the particle (in the direction OPOP) is given by F=mMG2πa2∫02π(cos⁡θ−ξ) dθ{1+ξ2−2ξcos⁡θ}3/2,F = \frac{mMG}{2\pi a^2} \int_0^{2\pi} \frac{(\cos\theta - \xi)\,d\theta}{\{1 + \xi^2 - 2\xi\cos\theta\}^{3/2}}, where the dimensionless distance ξ=b/a\xi = b/a. Use computer assistance to plot the graph of (dimensionless) FF against ξ\xi for 0≤ξ≤0.80 \leq \xi \leq 0.8 and confirm that FF is positive for ξ>0\xi > 0. Is the position of equilibrium at the centre of the circle stable? Could the rings of Saturn be solid?

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