2011: Problem 25

Topic: Rigid Bodies
Concepts: Inclined plane, Rolling down inclined plane


Solution:

Recall the acceleration of an object rolling without slipping down an inclined plane is given by

a=gsinθ1+βa=\frac{g\sin\theta}{1+\beta}

where the moment of inertia of the object is I=βmr2I=\beta mr^2. Recall the acceleration of a block sliding down an inclined plane is given by

a=g(sinθμcosθ)a=g(\sin\theta-\mu\cos\theta)

Since the hollow cylinder and block reach the bottom at the same time, they both have the same acceleration:

gsinθ1+β=g(sinθμcosθ)\frac{g\sin\theta}{1+\beta}=g(\sin\theta-\mu\cos\theta)
μcosθ=sinθ(111+β)\mu\cos\theta=\sin\theta\left(1-\frac{1}{1+\beta}\right)

For a hollow cylinder, β=1\beta=1:

μcosθ=sinθ2\mu\cos\theta=\frac{\sin\theta}{2}
μ=tanθ2\mu=\frac{\tan\theta}{2}

so the answer is C.

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