The Forces of Rolling — Question 1

Section 11-3 · Physics pages 1592–1593

Question 1 Static friction accelerates spin on a downhill ramp A solid disk rolls from rest down a 30◦incline without slip. Let its mass be M, radius R, and I = MR2/2; use g = 9.8. vC Schematic inclined surface; slope and dimensions are specified in the text. (a) Derive its acceleration and friction force. (b) Find the minimum static friction coefficient.
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Question 1 - Solution Static friction accelerates spin on a downhill ramp vC (a) Derivation and calculation Take downhill translation positive and let f denote uphill friction. The equations are Mg sin θ −f = Ma, fR = I a R. For I = MR2/2, f = Ma/2, hence a = 2g sin θ 3 = 2(9.8)(.5) 3 = 3.267 m/s2 , f = Mg sin θ 3 = Mg/6 uphill . (b) Result and interpretation Normal balance gives N = Mg cos θ. The no-slip solution is admissible only if f ≤µsN ⇒µs ≥f N = 1 3 tan θ. Thus µs,min = 1 3 √ 3 = .1925 . Static friction takes the value required by the dynamics and reaches µsN only at its limiting case. Physical check The uphill friction both reduces translational acceleration and supplies the torque needed for rolling.

Question 1

Static friction accelerates spin on a downhill ramp

A solid disk rolls from rest down a 30∘30^\circ incline without slip. Let its mass be MM, radius RR, and I=MR2/2I=MR^2/2; use g=9.8g=9.8.

Diagram shown in the original SVG worksheet.

  1. Derive its acceleration and friction force.

  2. Find the minimum static friction coefficient.

Question 1 - Solution

Static friction accelerates spin on a downhill ramp

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Take downhill translation positive and let ff denote uphill friction. The equations are Mgsin⁡θ−f=Ma,fR=IaR.Mg\sin\theta-f=Ma,\qquad fR=I\frac aR. For I=MR2/2I=MR^2/2, f=Ma/2f=Ma/2, hence a=2gsin⁡θ3=2(9.8)(.5)3=3.267m/s2,\boxed{a=\frac{2g\sin\theta}{3}=\frac{2(9.8)(.5)}3=3.267\ \mathrm{m/s^2}}, f=Mgsin⁡θ3=Mg/6uphill.\boxed{f=\frac{Mg\sin\theta}{3}=Mg/6\quad\text{uphill}}.

(b) Result and interpretation

Normal balance gives N=Mgcos⁡θN=Mg\cos\theta. The no-slip solution is admissible only if f≤μsN⇒μs≥fN=13tan⁡θ.f\le\mu_sN\Rightarrow\mu_s\ge\frac{f}{N}=\frac13\tan\theta. Thus μs,min=133=.1925.\boxed{\mu_{s,\min}=\frac1{3\sqrt3}=.1925}. Static friction takes the value required by the dynamics and reaches μsN\mu_sN only at its limiting case.

Physical check

The uphill friction both reduces translational acceleration and supplies the torque needed for rolling.