A solid cylinder of mass M=4 kg and radius R=0.2 m rolls without slipping down a 30° incline of length L=5 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/s2.
Solution — Step by Step
Three forces act: gravity Mg (down), normal N (perpendicular to incline), and friction f (up the incline, since the cylinder tends to slip down).
Along the incline: Mgsinθ−f=Ma.
Perpendicular: N=Mgcosθ.
Friction is the only torque-producing force about the center. Moment of inertia of a solid cylinder is I=21MR2.
τ=fR=Iα=21MR2α.
Pure rolling means a=Rα, so α=a/R. Substituting: f=21Ma.
Putting this back into the linear equation: Mgsinθ−21Ma=Ma, giving
a=32gsinθ=32×10×0.5=310≈3.33 m/s2
Using v2=2aL: v=2×3.33×5=33.3≈5.77 m/s.
Friction needed: f=21Ma=21(4)(3.33)=6.67 N.
For pure rolling, f≤μsN, so μmin=f/N=6.67/(4×10×cos30°)=6.67/34.64≈0.192.
Final answers:a≈3.33 m/s2, v≈5.77 m/s, μmin≈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 Mgsinθ⋅L converts to translational + rotational KE in ratio 1:I/(MR2)=1:0.5. That’s why the cylinder accelerates at 32gsinθ, not gsinθ.
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 v directly: Mgh=21Mv2+21Iω2=43Mv2.
So v=4gh/3=4×10×2.5/3=33.3≈5.77 m/s. Faster, but doesn’t give us a or f — kinematics is still needed for those.
Common Mistake
Many students treat f=μN 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) to maintain a=Rα. Using f=μN in the equations gives wrong a and tags pure rolling as “kinetic friction” problem.
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