The Yo-Yo — Question 6

Section 11-4 · Physics pages 1622–1623

Question 6 An ascending yo-yo can accelerate downward before reversing A yo-yo with I = 3Mr2 moves upward at 1.0 m/s while winding onto a fixed cord. Ignore losses and use g = 10. The no-slip constraint remains valid through the turning point. T Mg Yo-yo side view; the light cord is tangent to the inner axle. (a) Find its acceleration, time to the highest point and rise. (b) Find tension at the highest point; does zero speed imply zero torque?
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Question 6 - Solution An ascending yo-yo can accelerate downward before reversing T Mg (a) Derivation and calculation The downward acceleration does not depend on the instantaneous direction of motion: a = g 1 + I/(Mr2) = 10/4 = 2.50 m/s2 . With initial downward velocity v0 = −1.0 m/s, 0 = v0 + at ⇒ttop = .400 s , 0 = v2 0 + 2a∆y ⇒rise = −∆y = .200 m . (b) Result and interpretation At the highest point, T = M(g −a) = M(7.50 m/s2) , τ = Tr̸ = 0, α = a/r = 2.50/r̸ = 0. Although v = ω = 0 at that instant, the tension and accelerations remain finite and reverse the winding motion into unwinding descent. Physical check The turning point changes the velocity signs, not the constant downward acceleration.

Question 6

An ascending yo-yo can accelerate downward before reversing

A yo-yo with I=3Mr2I=3Mr^2 moves upward at 1.0m/s1.0\,\mathrm{m/s} while winding onto a fixed cord. Ignore losses and use g=10g=10. The no-slip constraint remains valid through the turning point.

Diagram shown in the original SVG worksheet.

  1. Find its acceleration, time to the highest point and rise.

  2. Find tension at the highest point; does zero speed imply zero torque?

Question 6 - Solution

An ascending yo-yo can accelerate downward before reversing

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The downward acceleration does not depend on the instantaneous direction of motion: a=g1+I/(Mr2)=10/4=2.50m/s2.\boxed{a=\frac{g}{1+I/(Mr^2)}=10/4=2.50\ \mathrm{m/s^2}}. With initial downward velocity v0=−1.0v_0=-1.0 m/s, 0=v0+at⇒ttop=.400s,0=v_0+at\Rightarrow\boxed{t_{\mathrm{top}}=.400\ \mathrm s}, 0=v02+2aΔy⇒rise=−Δy=.200m.0=v_0^2+2a\Delta y\Rightarrow\boxed{\text{rise}=-\Delta y=.200\ \mathrm m}.

(b) Result and interpretation

At the highest point, T=M(g−a)=M(7.50m/s2),\boxed{T=M(g-a)=M(7.50\ \mathrm{m/s^2})}, τ=Tr≠0,α=a/r=2.50/r≠0.\tau=Tr\ne0,\qquad\alpha=a/r=2.50/r\ne0. Although v=ω=0v=\omega=0 at that instant, the tension and accelerations remain finite and reverse the winding motion into unwinding descent.

Physical check

The turning point changes the velocity signs, not the constant downward acceleration.