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Question: A long horizontal rod has a bead which can slide along its length, and initially placed at a distanc...

A long horizontal rod has a bead which can slide along its length, and initially placed at a distance LL from one end AA of the rod. The rod is set in angular motion about A with constant angular accelerationα\alpha. If the coefficient of friction between the rod and the bead is μ\mu, and gravity is neglected, then the time after which the bead starts slipping is

A

μα\sqrt{\frac{\mu}{\alpha}}

B

μα\frac{\mu}{\sqrt{\alpha}}

C

1μα\frac{1}{\sqrt{\mu\alpha}}

D

Infinitesimal

Answer

μα\sqrt{\frac{\mu}{\alpha}}

Explanation

Solution

Let the bead starts slipping after time t

For critical condition

Frictional force provides the centripetal force mω2L=μR=μm×at=μmLαm\omega^{2}L = \mu R = \mu m \times a_{t} = ⥂ \mu mL\alpha

m (αt)2L = μmLαt=μαt = \sqrt{\frac{\mu}{\alpha}} (As ω = αt)