The Forces of Rolling — Question 4

Section 11-3 · Physics pages 1598–1599

Question 4 A particular pull height eliminates friction entirely A wheel has inertia I = βMR2. A horizontal rightward force F acts at height y above its center, with −R ≤y ≤R. Assume rolling without slip on a level surface. C vC F y Side view; arrows and labels specify the directions. (a) Derive acceleration and signed friction. (b) At what height does friction vanish, and when is that height accessible?
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Question 4 - Solution A particular pull height eliminates friction entirely C vC F y (a) Derivation and calculation With rightward f positive, F + f = Ma, −Fy + fR = −βMRa. Insert f = Ma −F into the moment equation: M(1 + β)a = F(1 + y/R). Thus a = F(1 + y/R) M(1 + β) , f = F(y/R −β) 1 + β . (b) Result and interpretation The zero-friction height follows from f = 0 ⇒y = βR . This lies in the allowed interval [−R, R] when 0 ≤β ≤1, as for mass confined within R. For F > 0, f > 0 above this height and f < 0 below it. Physical check For a disk, y = 0 gives backward friction and y = R gives forward friction, matching the preceding two cases.

Question 4

A particular pull height eliminates friction entirely

A wheel has inertia I=βMR2I=\beta MR^2. A horizontal rightward force FF acts at height yy above its center, with −R≤y≤R-R\le y\le R. Assume rolling without slip on a level surface.

Diagram shown in the original SVG worksheet.

  1. Derive acceleration and signed friction.

  2. At what height does friction vanish, and when is that height accessible?

Question 4 - Solution

A particular pull height eliminates friction entirely

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

With rightward ff positive, F+f=Ma,−Fy+fR=−βMRa.F+f=Ma,\qquad-Fy+fR=-\beta MRa. Insert f=Ma−Ff=Ma-F into the moment equation: M(1+β)a=F(1+y/R).M(1+\beta)a=F(1+y/R). Thus a=F(1+y/R)M(1+β),f=F(y/R−β)1+β.\boxed{a=\frac{F(1+y/R)}{M(1+\beta)}},\qquad \boxed{f=\frac{F(y/R-\beta)}{1+\beta}}.

(b) Result and interpretation

The zero-friction height follows from f=0⇒y=βR.f=0\Rightarrow\boxed{y=\beta R}. This lies in the allowed interval [−R,R][-R,R] when 0≤β≤10\le\beta\le1, as for mass confined within RR. For F>0F>0, f>0f>0 above this height and f<0f<0 below it.

Physical check

For a disk, y=0y=0 gives backward friction and y=Ry=R gives forward friction, matching the preceding two cases.