The Forces of Rolling — Question 2

Section 11-3 · Physics pages 1594–1595

Question 2 A center pull needs backward friction to establish rolling A horizontal force F = 12 N acts at the center of a 3 kg disk on level ground. The disk rolls without slip and has I = MR2/2. C vC F Side view; arrows and labels specify the directions. (a) Find center acceleration and static friction. (b) Explain why friction points opposite the applied force.
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Question 2 - Solution A center pull needs backward friction to establish rolling C vC F (a) Derivation and calculation Choose rightward translation and counterclockwise rotation positive. Then F + f = Ma, Rf = Iα, α = −a/R. Elimination gives a = F M + I/R2 = 12 3 + 1.5 = 8 3 m/s2 , f = Ma −F = 3(8/3) −12 = −4 N . (b) Result and interpretation The central applied force has zero moment about C. Friction supplies τC = Rf = −4R, α = −4R MR2/2 = −8 3R. Without friction, a = F/M but α = 0, so the bottom would accelerate right relative to the ground. Leftward friction opposes that incipient slip. Physical check The resulting clockwise angular acceleration satisfies a + Rα = 0.

Question 2

A center pull needs backward friction to establish rolling

A horizontal force F=12NF=12\,\mathrm N acts at the center of a 3kg3\,\mathrm{kg} disk on level ground. The disk rolls without slip and has I=MR2/2I=MR^2/2.

Diagram shown in the original SVG worksheet.

  1. Find center acceleration and static friction.

  2. Explain why friction points opposite the applied force.

Question 2 - Solution

A center pull needs backward friction to establish rolling

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Choose rightward translation and counterclockwise rotation positive. Then F+f=Ma,Rf=Iα,α=−a/R.F+f=Ma,\qquad Rf=I\alpha,\qquad\alpha=-a/R. Elimination gives a=FM+I/R2=123+1.5=83m/s2,\boxed{a=\frac{F}{M+I/R^2}=\frac{12}{3+1.5}=\frac83\ \mathrm{m/s^2}}, f=Ma−F=3(8/3)−12=−4N.\boxed{f=Ma-F=3(8/3)-12=-4\ \mathrm N}.

(b) Result and interpretation

The central applied force has zero moment about CC. Friction supplies τC=Rf=−4R,α=−4RMR2/2=−83R.\tau_C=Rf=-4R,\qquad\alpha=\frac{-4R}{MR^2/2}=-\frac8{3R}. Without friction, a=F/Ma=F/M but α=0\alpha=0, so the bottom would accelerate right relative to the ground. Leftward friction opposes that incipient slip.

Physical check

The resulting clockwise angular acceleration satisfies a+Rα=0a+R\alpha=0.