Angular Momentum — Question 4

Section 11-6 · Physics pages 1658–1659

Question 4 Angular momentum fixes tangential speed but leaves radial motion open A 2 kg particle is at radius 3 m in a plane and has angular momentum 12ˆz kg m2/s about the plane origin. x y⃗ r vθ Schematic; labels, not drawing lengths, specify the data. (a) Find tangential velocity and the minimum possible kinetic energy. (b) If its actual kinetic energy is 13 J, determine the possible radial velocities.
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Question 4 - Solution Angular momentum fixes tangential speed but leaves radial motion open x y⃗ r vθ (a) Derivation and calculation Only tangential velocity contributes to angular momentum: Lz = mrvθ ⇒vθ = 12 2(3) = 2.00 m/s . The energy is K = 1 2m(v2 r + v2 θ) ≥1 2mv2 θ, so Kmin = 4.00 J , attained at vr = 0. (b) Result and interpretation For K = 13 J, 13 = 1 2(2)(v2 r + 22) ⇒v2 r = 9, vr = +3.00 m/s or −3.00 m/s . Energy fixes the magnitude of radial motion; angular momentum fixes the tangential component. Neither measurement distinguishes outward from inward radial motion at this instant. Physical check The extra 9 J above the minimum is precisely the radial kinetic energy.

Question 4

Angular momentum fixes tangential speed but leaves radial motion open

A 2kg2\,\mathrm{kg} particle is at radius 3m3\,\mathrm m in a plane and has angular momentum 12ẑkgm2/s12\hat z\,\mathrm{kg\,m^2/s} about the plane origin.

Diagram shown in the original SVG worksheet.

  1. Find tangential velocity and the minimum possible kinetic energy.

  2. If its actual kinetic energy is 13J13\,\mathrm J, determine the possible radial velocities.

Question 4 - Solution

Angular momentum fixes tangential speed but leaves radial motion open

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Only tangential velocity contributes to angular momentum: Lz=mrvθ⇒vθ=122(3)=2.00m/s.L_z=mr v_\theta\Rightarrow\boxed{v_\theta=\frac{12}{2(3)}=2.00\ \mathrm{m/s}}. The energy is K=12m(vr2+vθ2)≥12mvθ2,K=\tfrac12m(v_r^2+v_\theta^2)\ge\tfrac12mv_\theta^2, so Kmin=4.00J\boxed{K_{\min}=4.00\ \mathrm J}, attained at vr=0v_r=0.

(b) Result and interpretation

For K=13K=13 J, 13=12(2)(vr2+22)⇒vr2=9,13=\tfrac12(2)(v_r^2+2^2)\Rightarrow v_r^2=9, vr=+3.00m/sor−3.00m/s.\boxed{v_r=+3.00\ \mathrm{m/s}\quad\text{or}\quad-3.00\ \mathrm{m/s}}. Energy fixes the magnitude of radial motion; angular momentum fixes the tangential component. Neither measurement distinguishes outward from inward radial motion at this instant.

Physical check

The extra 9 J above the minimum is precisely the radial kinetic energy.