The Angular Momentum of a System of Particles — Question 5

Section 11-8 · Physics pages 1700–1701

Question 5 An impulsive couple changes internal motion without center recoil Two particles at⃗r1 = (1, 0, 0) and⃗r2 = (−1, 0, 0) m receive simultaneous impulses⃗J1 = (0, 2, 0) and⃗J2 = (0, −2, 0) N s. Positions do not change appreciably during the impulses.⃗ J1⃗ J2 Schematic; labels, not drawing lengths, specify the data. (a) Find changes in total linear and angular momentum. (b) Explain why the center velocity remains unchanged for any positive particle masses.
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Question 5 - Solution An impulsive couple changes internal motion without center recoil⃗ J1⃗ J2 (a) Derivation and calculation The total impulse is ∆⃗P =⃗J1 +⃗J2 = 2ˆy −2ˆy =⃗0 . The angular impulse is ∆⃗L = (ˆx) × (2ˆy) + (−ˆx) × (−2ˆy) = 4ˆz kg m2/s . (b) Result and interpretation For any positive total mass, M∆⃗VC = ∆⃗P = 0 ⇒∆⃗VC = 0 . Positions do not appreciably change during the pulse, so the center orbital contribution remains fixed. The angular impulse changes internal angular momentum while leaving the center velocity unchanged. Physical check The two impulses have opposite linear effects but the same signed angular effect.

Question 5

An impulsive couple changes internal motion without center recoil

Two particles at r→1=(1,0,0)\vec r_1=(1,0,0) and r→2=(−1,0,0)m\vec r_2=(-1,0,0)\,\mathrm m receive simultaneous impulses J→1=(0,2,0)\vec J_1=(0,2,0) and J→2=(0,−2,0)Ns\vec J_2=(0,-2,0)\,\mathrm{N\,s}. Positions do not change appreciably during the impulses.

Diagram shown in the original SVG worksheet.

  1. Find changes in total linear and angular momentum.

  2. Explain why the center velocity remains unchanged for any positive particle masses.

Question 5 - Solution

An impulsive couple changes internal motion without center recoil

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The total impulse is ΔP→=J→1+J→2=2ŷ−2ŷ=0→.\boxed{\Delta\vec P=\vec J_1+\vec J_2=2\hat y-2\hat y=\vec0}. The angular impulse is ΔL→=(x̂)×(2ŷ)+(−x̂)×(−2ŷ)=4ẑkgm2/s.\Delta\vec L=(\hat x)\times(2\hat y)+(-\hat x)\times(-2\hat y) =\boxed{4\hat z\ \mathrm{kg\,m^2/s}}.

(b) Result and interpretation

For any positive total mass, MΔV→C=ΔP→=0⇒ΔV→C=0.M\Delta\vec V_C=\Delta\vec P=0\Rightarrow\boxed{\Delta\vec V_C=0}. Positions do not appreciably change during the pulse, so the center orbital contribution remains fixed. The angular impulse changes internal angular momentum while leaving the center velocity unchanged.

Physical check

The two impulses have opposite linear effects but the same signed angular effect.