The Yo-Yo — Question 9

Section 11-4 · Physics pages 1628–1629

Question 9 A finite cord ends the validity of the smooth descent model A yo-yo with I = 4Mr2 starts from rest and unwinds 1.0 m of usable cord on a fixed support. Use g = 10 and r = 0.020 m. No losses occur before the cord end is reached. T Mg Yo-yo side view; the light cord is tangent to the inner axle. (a) Find the time, speed and angular speed just before full extension. (b) Can the rebound speed be determined from these assumptions alone?
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Question 9 - Solution A finite cord ends the validity of the smooth descent model T Mg (a) Derivation and calculation Before the end event, fixed-cord unwinding gives a = g 1 + 4 = 2.00 m/s2. For a descent h = 1.0 m from rest, t = √ 2h/a = 1.00 s , v = √ 2ah = 2.00 m/s , |ω| = v/r = 2/.020 = 100 rad/s . (b) Result and interpretation These are the state variables just before full extension. Across the end event, impulses may change them: M(v+ −v−) = Jy, I(ω+ −ω−) = Jτ. Neither the impulse relation nor energy recovery is specified for that event. A restitution, cord-elasticity, or contact-transition model is required to determine the rebound speed. Physical check The lossless-descent assumption applies before full extension and does not prescribe the physics of the end transition.

Question 9

A finite cord ends the validity of the smooth descent model

A yo-yo with I=4Mr2I=4Mr^2 starts from rest and unwinds 1.0m1.0\,\mathrm m of usable cord on a fixed support. Use g=10g=10 and r=0.020mr=0.020\,\mathrm m. No losses occur before the cord end is reached.

Diagram shown in the original SVG worksheet.

  1. Find the time, speed and angular speed just before full extension.

  2. Can the rebound speed be determined from these assumptions alone?

Question 9 - Solution

A finite cord ends the validity of the smooth descent model

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Before the end event, fixed-cord unwinding gives a=g1+4=2.00m/s2.a=\frac{g}{1+4}=2.00\ \mathrm{m/s^2}. For a descent h=1.0h=1.0 m from rest, t=2h/a=1.00s,v=2ah=2.00m/s,\boxed{t=\sqrt{2h/a}=1.00\ \mathrm s},\qquad \boxed{v=\sqrt{2ah}=2.00\ \mathrm{m/s}}, |ω|=v/r=2/.020=100rad/s.\boxed{|\omega|=v/r=2/.020=100\ \mathrm{rad/s}}.

(b) Result and interpretation

These are the state variables just before full extension. Across the end event, impulses may change them: M(v+−v−)=Jy,I(ω+−ω−)=Jτ.M(v_+-v_-)=J_y,\qquad I(\omega_+-\omega_-)=J_\tau. Neither the impulse relation nor energy recovery is specified for that event. A restitution, cord-elasticity, or contact-transition model is required to determine the rebound speed.

Physical check

The lossless-descent assumption applies before full extension and does not prescribe the physics of the end transition.