Classical Mechanics (Kibble & Berkshire) · Problem 7.10

Non-linear oscillations and phase space — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · nearly-circular-orbits

Problem

A particle of mass mm moves under the central field F=−m(γ e−ϵr/ar2)r^,\boldsymbol{F} = -m\left(\frac{\gamma\, e^{-\epsilon r/a}}{r^2}\right)\hat{\boldsymbol{r}}, where γ\gamma, aa and ϵ\epsilon are positive constants. Find the apsidal angle for a nearly circular orbit of radius aa. When ϵ\epsilon is small, show that the perihelion of the orbit advances by approximately πϵ\pi\epsilon on each revolution.

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