The Yo-Yo — Question 8

Section 11-4 · Physics pages 1626–1627

Question 8 Cutting the cord changes acceleration but not instantaneous velocity A yo-yo descends on a fixed cord with center speed 2 m/s and clockwise spin 100 rad/s. The cord is cut without an impulse. Take g = 10 and ignore air resistance. T Mg Configuration immediately before cutting; after the cut the tension is zero. (a) Find center speed and angular speed 0.30 s later. (b) For axle radius 0.020 m, test the old no-slip relation after the cut.
Show solutionHide solution
Question 8 - Solution Cutting the cord changes acceleration but not instantaneous velocity T Mg (a) Derivation and calculation No cutting impulse means that center velocity and angular velocity remain continuous. After cutting, a = g, τC = 0 ⇒α = 0. At t = .30 s, v = 2 + 10(.30) = 5.00 m/s down , |ω| = 100 rad/s clockwise . (b) Result and interpretation The previous contact condition would require v = r|ω| = .020(100) = 2.00 m/s. Instead, v −r|ω| = 5 −2 = 3.00 m/s . The relation no longer applies because the cord contact has been removed; gravity changes translation but supplies no torque about the center. Physical check The old constraint holds immediately before and at the cut, then ceases to govern subsequent motion.

Question 8

Cutting the cord changes acceleration but not instantaneous velocity

A yo-yo descends on a fixed cord with center speed 2m/s2\,\mathrm{m/s} and clockwise spin 100rad/s100\,\mathrm{rad/s}. The cord is cut without an impulse. Take g=10g=10 and ignore air resistance.

Diagram shown in the original SVG worksheet.

  1. Find center speed and angular speed 0.30s0.30\,\mathrm s later.

  2. For axle radius 0.020m0.020\,\mathrm m, test the old no-slip relation after the cut.

Question 8 - Solution

Cutting the cord changes acceleration but not instantaneous velocity

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

No cutting impulse means that center velocity and angular velocity remain continuous. After cutting, a=g,τC=0⇒α=0.a=g,\qquad\tau_C=0\Rightarrow\alpha=0. At t=.30t=.30 s, v=2+10(.30)=5.00m/sdown,|ω|=100rad/sclockwise.\boxed{v=2+10(.30)=5.00\ \mathrm{m/s}\quad\text{down}},\qquad \boxed{|\omega|=100\ \mathrm{rad/s}\quad\text{clockwise}}.

(b) Result and interpretation

The previous contact condition would require v=r|ω|=.020(100)=2.00m/s.v=r|\omega|=.020(100)=2.00\ \mathrm{m/s}. Instead, v−r|ω|=5−2=3.00m/s.\boxed{v-r|\omega|=5-2=3.00\ \mathrm{m/s}}. The relation no longer applies because the cord contact has been removed; gravity changes translation but supplies no torque about the center.

Physical check

The old constraint holds immediately before and at the cut, then ceases to govern subsequent motion.