The Yo-Yo — Question 1

Section 11-4 · Physics pages 1612–1613

Question 1 An unwinding yo-yo falls more slowly than a dropped particle A yo-yo of mass 0.20 kg has axle radius r = 0.010 m and inertia I = 4.0 × 10−5 kg m2. It descends from rest on a vertical fixed light cord without slipping. Use g = 9.8. T Mg Yo-yo side view; the light cord is tangent to the inner axle. (a) Find acceleration and cord tension. (b) Find angular acceleration and the zero-inertia limit.
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Question 1 - Solution An unwinding yo-yo falls more slowly than a dropped particle T Mg (a) Derivation and calculation Choose downward translation and unwinding spin positive. Then Mg −T = Ma, Tr = Iα, a = rα. Eliminating T, α gives a = Mg M + I/r2 = .20(9.8) .20 + .40 = 49 15 = 3.267 m/s2 , T = M(g −a) = 98 75 = 1.307 N . (b) Result and interpretation The angular acceleration is α = a/r = 3.267/.010 = 326.7 rad/s2 . For fixed M, r, the zero-inertia limit is I →0 : a →g, T →0. The tension is below the weight because the center accelerates downward; rotational dynamics do not require the tension to balance gravity. Physical check The effective rotational mass I/r2 = .40 kg is twice the actual mass, making a = g/3.

Question 1

An unwinding yo-yo falls more slowly than a dropped particle

A yo-yo of mass 0.20kg0.20\,\mathrm{kg} has axle radius r=0.010mr=0.010\,\mathrm m and inertia I=4.0×10−5kgm2I=4.0\times10^{-5}\,\mathrm{kg\,m^2}. It descends from rest on a vertical fixed light cord without slipping. Use g=9.8g=9.8.

Diagram shown in the original SVG worksheet.

  1. Find acceleration and cord tension.

  2. Find angular acceleration and the zero-inertia limit.

Question 1 - Solution

An unwinding yo-yo falls more slowly than a dropped particle

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Choose downward translation and unwinding spin positive. Then Mg−T=Ma,Tr=Iα,a=rα.Mg-T=Ma,\qquad Tr=I\alpha,\qquad a=r\alpha. Eliminating T,αT,\alpha gives a=MgM+I/r2=.20(9.8).20+.40=4915=3.267m/s2,\boxed{a=\frac{Mg}{M+I/r^2}=\frac{.20(9.8)}{.20+.40}=\frac{49}{15}=3.267\ \mathrm{m/s^2}}, T=M(g−a)=9875=1.307N.\boxed{T=M(g-a)=\frac{98}{75}=1.307\ \mathrm N}.

(b) Result and interpretation

The angular acceleration is α=a/r=3.267/.010=326.7rad/s2.\boxed{\alpha=a/r=3.267/.010=326.7\ \mathrm{rad/s^2}}. For fixed M,rM,r, the zero-inertia limit is I→0:a→g,T→0.I\to0:\qquad a\to g,\qquad T\to0. The tension is below the weight because the center accelerates downward; rotational dynamics do not require the tension to balance gravity.

Physical check

The effective rotational mass I/r2=.40I/r^2=.40 kg is twice the actual mass, making a=g/3a=g/3.