Conservation of Angular Momentum — Question 6

Section 11-10 · Physics pages 1742–1743

Question 6 A radial pull changes tangential speed without supplying torque A 1 kg bead slides on a frictionless horizontal table, attached to a cord through a small central hole. Initially it moves tangentially at radius 2 m and speed 3 m/s. The cord is pulled until the radius is 1 m; radial speed is zero at both endpoints. vi Cord acts radially through the hole; dashed circles mark endpoint radii. (a) Find final tangential speed. (b) Find work done by the pull and explain why zero torque does not imply zero work.
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Question 6 - Solution A radial pull changes tangential speed without supplying torque vi (a) Derivation and calculation The cord force is radial, so its torque about the hole vanishes:⃗ τ =⃗r × (−T ˆer) = 0 ⇒mrivi = mrfvf. Thus vf = ri rf vi = 2 1(3) = 6.00 m/s . (b) Result and interpretation Radial speed is zero at both endpoints, so the work is the change in tangential kinetic energy: W = ∆K = 1 2(1)(62 −32) = 13.5 J . During inward motion, PT =⃗T ·⃗v = −T ˙r > 0 ( ˙r < 0). Zero torque does not imply zero work: radial tension has a zero moment but can act along the radial displacement. Physical check The final angular speed is vf/rf = 6 rad/s, while mrv stays at 6 kg m2/s.

Question 6

A radial pull changes tangential speed without supplying torque

A 1kg1\,\mathrm{kg} bead slides on a frictionless horizontal table, attached to a cord through a small central hole. Initially it moves tangentially at radius 2m2\,\mathrm m and speed 3m/s3\,\mathrm{m/s}. The cord is pulled until the radius is 1m1\,\mathrm m; radial speed is zero at both endpoints.

Diagram shown in the original SVG worksheet.

  1. Find final tangential speed.

  2. Find work done by the pull and explain why zero torque does not imply zero work.

Question 6 - Solution

A radial pull changes tangential speed without supplying torque

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The cord force is radial, so its torque about the hole vanishes: τ→=r→×(−Têr)=0⇒mrivi=mrfvf.\vec\tau=\vec r\times(-T\hat e_r)=0\Rightarrow mr_iv_i=mr_fv_f. Thus vf=rirfvi=21(3)=6.00m/s.\boxed{v_f=\frac{r_i}{r_f}v_i=\frac21(3)=6.00\ \mathrm{m/s}}.

(b) Result and interpretation

Radial speed is zero at both endpoints, so the work is the change in tangential kinetic energy: W=ΔK=12(1)(62−32)=13.5J.\boxed{W=\Delta K=\tfrac12(1)(6^2-3^2)=13.5\ \mathrm J}. During inward motion, 𝒫T=T→⋅v→=−Tṙ>0(ṙ<0).\mathcal P_T=\vec T\cdot\vec v=-T\dot r>0\quad(\dot r<0). Zero torque does not imply zero work: radial tension has a zero moment but can act along the radial displacement.

Physical check

The final angular speed is vf/rf=6v_f/r_f=6 rad/s, while mrvmr v stays at 6 kg m2^2/s.