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Homework Statement
A particle moves around the surface of an upside-down cone, in a horizontal circular path, in equilibrium. The particle is given a small radial kick. Use the Lagrangian equation for motion (found in a previous section of this problem):
m\ddot{r} = (ml_{z}^{2})/(r^{3}cos^{2}(\alpha)sin^{2}(\alpha)) - cos(\alpha)mg
to decide whether the circular path is stable. If so, with what frequency does r oscillate about the equilibrium?
Homework Equations
The Attempt at a Solution
If I can put in r_{o} ± \epsilon for r in that equation and show that the right side is positive when epsilon is negative and negative when epsilon is positive, then I will have shown that it is stable.
But I don't know how to do that. Also, when I can show that it is stable, how should I go about knowing the frequency of oscillation?