A particle of mass moving under an attractive inverse-square force with fixed angular…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Mechanics & Dynamical Systems · Calculus of change and accumulation

Mathematical Methods for Physics, Ch The derivative as a physical instrument

Problem

A particle of mass mm moving under an attractive inverse-square force with fixed angular momentum LL has an effective potential energyUeff(r)=L22mr2−kr,r>0,U_{\text{eff}}(r) = \frac{L^2}{2mr^2} - \frac{k}{r}, \qquad r > 0,where k>0k > 0 is the force constant. The distance rr from the centre then changes as if the particle moved in one dimension with energy E=12mr˙2+Ueff(r)E = \tfrac12 m\dot r^2 + U_{\text{eff}}(r), and EE stays constant. Take L=4.0 kg m2 s−1L = 4.0\,\mathrm{kg\,m^2\,s^{-1}}, m=2.0 kgm = 2.0\,\mathrm{kg} and k=8.0 J mk = 8.0\,\mathrm{J\,m}. ((a)) Find the stationary point r0r_0 of Ueff(r)U_{\text{eff}}(r). ((b)) Evaluate Ueff′′(r0)U_{\text{eff}}''(r_0) and state whether r0r_0 is a minimum or a maximum. ((c)) Given that Ueff→+∞U_{\text{eff}}\to+\infty as r→0+r\to0^+ and Ueff→0−U_{\text{eff}}\to0^- as r→∞r\to\infty, sketch in words the shape of the curve. A particle placed at r0r_0 with r˙=0\dot r = 0 keeps a constant rr, so it moves in a circle. Use your result from (b) to say whether a small change in rr from r0r_0 meets a force back towards r0r_0 or away from it.

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