The Angular Momentum of a System of Particles — Question 9

Section 11-8 · Physics pages 1708–1709

Question 9 Opposite angular momenta can coexist with substantial kinetic energy Two 1 kg particles are at (1, 0, 0) and (−1, 0, 0) m and both move at 2ˆy m/s.⃗ v1 =⃗v2 Schematic; labels, not drawing lengths, specify the data. (a) Find total angular momentum about the origin and total kinetic energy. (b) Describe their center-frame motion and explain the cancellation.
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Question 9 - Solution Opposite angular momenta can coexist with substantial kinetic energy⃗ v1 =⃗v2 (a) Derivation and calculation The two angular momenta cancel:⃗ L1 = ˆx × 2ˆy = 2ˆz,⃗ L2 = (−ˆx) × 2ˆy = −2ˆz,⃗ LO =⃗0 . Their positive kinetic energies add: K = 2 [ 1 2(1)(2)2] = 4.00 J . (b) Result and interpretation The center is at the origin and has velocity⃗VC = 2ˆy. Each relative velocity is⃗ ui =⃗vi −⃗VC = 0. Thus the motion is instantaneously pure translation, with LC = 0 and⃗RC × M⃗VC = 0. Signed angular momenta can cancel while scalar kinetic energies remain positive. Physical check The center translational energy MV 2 C/2 = 2(4)/2 = 4 J accounts for the entire energy.

Question 9

Opposite angular momenta can coexist with substantial kinetic energy

Two 1kg1\,\mathrm{kg} particles are at (1,0,0)(1,0,0) and (−1,0,0)m(-1,0,0)\,\mathrm m and both move at 2ŷm/s2\hat y\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find total angular momentum about the origin and total kinetic energy.

  2. Describe their center-frame motion and explain the cancellation.

Question 9 - Solution

Opposite angular momenta can coexist with substantial kinetic energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The two angular momenta cancel: L→1=x̂×2ŷ=2ẑ,L→2=(−x̂)×2ŷ=−2ẑ,\vec L_1=\hat x\times2\hat y=2\hat z,\qquad \vec L_2=(-\hat x)\times2\hat y=-2\hat z, L→O=0→.\boxed{\vec L_O=\vec0}. Their positive kinetic energies add: K=2[12(1)(2)2]=4.00J.\boxed{K=2\left[\tfrac12(1)(2)^2\right]=4.00\ \mathrm J}.

(b) Result and interpretation

The center is at the origin and has velocity V→C=2ŷ\vec V_C=2\hat y. Each relative velocity is u→i=v→i−V→C=0.\vec u_i=\vec v_i-\vec V_C=0. Thus the motion is instantaneously pure translation, with LC=0L_C=0 and R→C×MV→C=0\vec R_C\times M\vec V_C=0. Signed angular momenta can cancel while scalar kinetic energies remain positive.

Physical check

The center translational energy MVC2/2=2(4)/2=4MV_C^2/2=2(4)/2=4 J accounts for the entire energy.