Rotational Motion: Numerical Problems Set (3)

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Question

A solid cylinder of mass M=4 kgM = 4 \text{ kg} and radius R=0.2 mR = 0.2 \text{ m} rolls without slipping down a 30°30° incline of length L=5 mL = 5 \text{ m}, starting from rest. Find (a) its acceleration, (b) speed at the bottom, and (c) the minimum coefficient of friction needed for pure rolling. Take g=10 m/s2g = 10 \text{ m/s}^2.

Solution — Step by Step

Three forces act: gravity MgMg (down), normal NN (perpendicular to incline), and friction ff (up the incline, since the cylinder tends to slip down).

Along the incline: Mgsinθf=MaMg\sin\theta - f = Ma.

Perpendicular: N=MgcosθN = Mg\cos\theta.

Friction is the only torque-producing force about the center. Moment of inertia of a solid cylinder is I=12MR2I = \tfrac{1}{2}MR^2.

τ=fR=Iα=12MR2α\tau = fR = I\alpha = \tfrac{1}{2}MR^2 \alpha.

Pure rolling means a=Rαa = R\alpha, so α=a/R\alpha = a/R. Substituting: f=12Maf = \tfrac{1}{2}Ma.

Putting this back into the linear equation: Mgsinθ12Ma=MaMg\sin\theta - \tfrac{1}{2}Ma = Ma, giving

a=2gsinθ3=2×10×0.53=1033.33 m/s2a = \frac{2g\sin\theta}{3} = \frac{2 \times 10 \times 0.5}{3} = \frac{10}{3} \approx 3.33 \text{ m/s}^2

Using v2=2aLv^2 = 2aL: v=2×3.33×5=33.35.77 m/sv = \sqrt{2 \times 3.33 \times 5} = \sqrt{33.3} \approx 5.77 \text{ m/s}.

Friction needed: f=12Ma=12(4)(3.33)=6.67 Nf = \tfrac{1}{2}Ma = \tfrac{1}{2}(4)(3.33) = 6.67 \text{ N}.

For pure rolling, fμsNf \le \mu_s N, so μmin=f/N=6.67/(4×10×cos30°)=6.67/34.640.192\mu_{min} = f/N = 6.67/(4 \times 10 \times \cos 30°) = 6.67/34.64 \approx 0.192.

Final answers: a3.33 m/s2a \approx \mathbf{3.33 \text{ m/s}^2}, v5.77 m/sv \approx \mathbf{5.77 \text{ m/s}}, μmin0.192\mu_{min} \approx \mathbf{0.192}.

Why This Works

In rolling without slipping, friction does no work on the cylinder (the contact point is momentarily at rest). All of MgsinθLMg\sin\theta \cdot L converts to translational + rotational KE in ratio 1:I/(MR2)=1:0.51 : I/(MR^2) = 1 : 0.5. That’s why the cylinder accelerates at 23gsinθ\tfrac{2}{3}g\sin\theta, not gsinθg\sin\theta.

The minimum-friction condition matters: if the slope is too steep or surface too smooth, the cylinder slips and the analysis changes completely.

Alternative Method

Energy conservation gives vv directly: Mgh=12Mv2+12Iω2=34Mv2Mgh = \tfrac{1}{2}Mv^2 + \tfrac{1}{2}I\omega^2 = \tfrac{3}{4}Mv^2.

So v=4gh/3=4×10×2.5/3=33.35.77 m/sv = \sqrt{4gh/3} = \sqrt{4 \times 10 \times 2.5/3} = \sqrt{33.3} \approx 5.77 \text{ m/s}. Faster, but doesn’t give us aa or ff — kinematics is still needed for those.

Common Mistake

Many students treat f=μNf = \mu N as if friction is always at its maximum during pure rolling. It’s not — static friction adjusts to whatever value is needed (up to μsN\mu_s N) to maintain a=Rαa = R\alpha. Using f=μNf = \mu N in the equations gives wrong aa and tags pure rolling as “kinetic friction” problem.

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