The Yo-Yo — Question 10

Section 11-4 · Physics pages 1630–1631

Question 10 An opposing axle torque can halt unwinding before free fall A descending yo-yo has M = 0.20 kg, r = 0.010 m, I = 4 × 10−5 kg m2 and constant opposing axle torque b = 0.006 N m. Use g = 10 and a fixed no-slip cord. T Mg Yo-yo side view; the light cord is tangent to the inner axle. (a) Find downward acceleration and tension while unwinding. (b) Find the torque magnitude that would maintain constant descending speed.
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Question 10 - Solution An opposing axle torque can halt unwinding before free fall T Mg (a) Derivation and calculation During unwinding, the opposing axle torque reduces the net moment: Mg −T = Ma, Tr −b = Iα = Ia/r. Eliminating T, a = Mg −b/r M + I/r2 = 2 −.600 .20 + .40 = 7 3 m/s2 , T = M(g −a) = .20(10 −7/3) = 23 15 = 1.533 N . (b) Result and interpretation At constant descending speed, a = α = 0: T = Mg, Tr −b = 0. Therefore bconstant = Mgr = .20(10)(.010) = .0200 N m . A larger opposing torque decelerates existing descent; the behavior once rest is reached requires a static-torque model. Physical check At constant speed the resisting power bω = Mgr(v/r) = Mgv removes the released gravitational power.

Question 10

An opposing axle torque can halt unwinding before free fall

A descending yo-yo has M=0.20kgM=0.20\,\mathrm{kg}, r=0.010mr=0.010\,\mathrm m, I=4×10−5kgm2I=4\times10^{-5}\,\mathrm{kg\,m^2} and constant opposing axle torque b=0.006Nmb=0.006\,\mathrm{N\,m}. Use g=10g=10 and a fixed no-slip cord.

Diagram shown in the original SVG worksheet.

  1. Find downward acceleration and tension while unwinding.

  2. Find the torque magnitude that would maintain constant descending speed.

Question 10 - Solution

An opposing axle torque can halt unwinding before free fall

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

During unwinding, the opposing axle torque reduces the net moment: Mg−T=Ma,Tr−b=Iα=Ia/r.Mg-T=Ma,\qquad Tr-b=I\alpha=Ia/r. Eliminating TT, a=Mg−b/rM+I/r2=2−.600.20+.40=73m/s2,\boxed{a=\frac{Mg-b/r}{M+I/r^2}=\frac{2-.600}{.20+.40}=\frac73\ \mathrm{m/s^2}}, T=M(g−a)=.20(10−7/3)=2315=1.533N.\boxed{T=M(g-a)=.20(10-7/3)=\frac{23}{15}=1.533\ \mathrm N}.

(b) Result and interpretation

At constant descending speed, a=α=0a=\alpha=0: T=Mg,Tr−b=0.T=Mg,\qquad Tr-b=0. Therefore bconstant=Mgr=.20(10)(.010)=.0200Nm.\boxed{b_{\mathrm{constant}}=Mgr=.20(10)(.010)=.0200\ \mathrm{N\,m}}. A larger opposing torque decelerates existing descent; the behavior once rest is reached requires a static-torque model.

Physical check

At constant speed the resisting power bω=Mgr(v/r)=Mgvb\omega=Mgr(v/r)=Mgv removes the released gravitational power.