The Angular Momentum of a System of Particles — Question 1

Section 11-8 · Physics pages 1692–1693

Question 1 Zero total momentum does not imply zero total angular momentum Two 1 kg particles are at (0, 1, 0) and (0, −1, 0) m. Their velocities are respectively (2, 0, 0) and (−2, 0, 0) m/s.⃗ p1⃗ p2 O Schematic; labels, not drawing lengths, specify the data. (a) Find total linear and angular momentum about the origin. (b) Would translating the origin change total angular momentum at this instant?
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Question 1 - Solution Zero total momentum does not imply zero total angular momentum⃗ p1⃗ p2 O (a) Derivation and calculation The two momenta are⃗p1 = 2ˆx and⃗p2 = −2ˆx kg m/s, so⃗ P =⃗p1 +⃗p2 =⃗0 . Their angular momenta add:⃗ L1 = ˆy × 2ˆx = −2ˆz,⃗ L2 = (−ˆy) × (−2ˆx) = −2ˆz,⃗ LO = −4ˆz kg m2/s . (b) Result and interpretation For a translated origin A at⃗a,⃗ LA = ∑ (⃗ri −⃗a) ×⃗pi =⃗LO −⃗a ×⃗P. Since⃗P = 0,⃗ LA =⃗LO for every⃗a. This comparison keeps the same velocity frame. Physical check Equal opposite momenta cancel their resultant but can add angular momentum through opposite lever arms.

Question 1

Zero total momentum does not imply zero total angular momentum

Two 1kg1\,\mathrm{kg} particles are at (0,1,0)(0,1,0) and (0,−1,0)m(0,-1,0)\,\mathrm m. Their velocities are respectively (2,0,0)(2,0,0) and (−2,0,0)m/s(-2,0,0)\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find total linear and angular momentum about the origin.

  2. Would translating the origin change total angular momentum at this instant?

Question 1 - Solution

Zero total momentum does not imply zero total angular momentum

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The two momenta are p→1=2x̂\vec p_1=2\hat x and p→2=−2x̂\vec p_2=-2\hat x kg m/s, so P→=p→1+p→2=0→.\boxed{\vec P=\vec p_1+\vec p_2=\vec0}. Their angular momenta add: L→1=ŷ×2x̂=−2ẑ,L→2=(−ŷ)×(−2x̂)=−2ẑ,\vec L_1=\hat y\times2\hat x=-2\hat z,\qquad \vec L_2=(-\hat y)\times(-2\hat x)=-2\hat z, L→O=−4ẑkgm2/s.\boxed{\vec L_O=-4\hat z\ \mathrm{kg\,m^2/s}}.

(b) Result and interpretation

For a translated origin AA at a→\vec a, L→A=∑(r→i−a→)×p→i=L→O−a→×P→.\vec L_A=\sum(\vec r_i-\vec a)\times\vec p_i =\vec L_O-\vec a\times\vec P. Since P→=0\vec P=0, L→A=L→Ofor every a→.\boxed{\vec L_A=\vec L_O}\quad\text{for every }\vec a. This comparison keeps the same velocity frame.

Physical check

Equal opposite momenta cancel their resultant but can add angular momentum through opposite lever arms.