A Mechanics Problem Involving Equilibrium Rotational Motion

The following is a useful Mechanics 3 level problem involving a particle in equilibrium whilst undergoing rotational motion. I give my suggested solution below.

The Problem

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Suggested solution

I sketch the relevant forces in the following diagram:

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Since the particle is in equilibrium, the centripetal and centrifugal forces must be equal so resolving towards the central axis of the cone we must have

R(\leftarrow), \frac{mv^2}{\frac{1}{3}a} - F_C = 0                      (1)

Since there is no motion up or down the inner surface of the cone we must also have (resolving downwards along the inner surface)

R(\swarrow), mg\cos(90^{\circ} - \theta) - F_C\cos\theta = 0        (2)

But

\cos(90^{\circ} - \theta) = \sin\theta                  (3)

Using (1) and (3) in (2) we get

mg\sin\theta = \frac{mv^2}{\frac{1}{3}a}\cos\theta

and therefore

g\tan\theta = \frac{v^2}{\frac{1}{3}a}                     (4)

But

\tan\theta = \frac{\frac{1}{3}h}{\frac{1}{3}a}             (5)

Using (5) in (4) gives

g\frac{\frac{1}{3}h}{\frac{1}{3}a} = \frac{v^2}{\frac{1}{3}a} \Longleftrightarrow v = \sqrt{\frac{1}{3}hg} as required.