The Angular Momentum of a System of Particles — Question 7

Section 11-8 · Physics pages 1704–1705

Question 7 Relative motion can be represented with reduced mass Two particles have masses m1 = 2 and m2 = 3 kg. Their relative position is⃗ r =⃗r1 −⃗r2 = (4, 0, 0) m and relative velocity is⃗v =⃗v1 −⃗v2 = (0, 5, 0) m/s. m2 = 3 m1 = 2 C⃗ u2⃗ u1⃗ r = 4ˆx Relative positions and velocities in the mass-center frame give the same angular-momentum direction for both particles. (a) Derive and evaluate angular momentum about the center of mass. (b) Find the same value using each particle separately in the center frame.
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Question 7 - Solution Relative motion can be represented with reduced mass m2 = 3 m1 = 2 C⃗ u2⃗ u1⃗ r = 4ˆx (a) Derivation and calculation With M = m1 + m2,⃗ ρ1 = m2 M⃗r,⃗ ρ2 = −m1 M⃗r,⃗ u1 = m2 M⃗v,⃗ u2 = −m1 M⃗v. Substitution into the particle sum gives⃗ LC = m1m2(m1 + m2) M2⃗ r ×⃗v = µ⃗r ×⃗v, µ = 2(3) 5 = 1.20 kg. Thus⃗LC = 1.2(4)(5)ˆz = 24ˆz kg m2/s . (b) Result and interpretation The individual center-frame variables are⃗ ρ1 = 2.4ˆx,⃗ ρ2 = −1.6ˆx,⃗ u1 = 3ˆy,⃗ u2 = −2ˆy. Their angular momenta are L1,z = 2.4(2)(3) = 14.4, L2,z = (−1.6)(3)(−2) = 9.6, LC,z = 14.4 + 9.6 = 24 kg m2/s . Physical check The relative velocity is 3 −(−2) = 5 m/s and the center-frame momenta sum to zero.

Question 7

Relative motion can be represented with reduced mass

Two particles have masses m1=2m_1=2 and m2=3kgm_2=3\,\mathrm{kg}. Their relative position is r→=r→1−r→2=(4,0,0)m\vec r=\vec r_1-\vec r_2=(4,0,0)\,\mathrm m and relative velocity is v→=v→1−v→2=(0,5,0)m/s\vec v=\vec v_1-\vec v_2=(0,5,0)\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Derive and evaluate angular momentum about the center of mass.

  2. Find the same value using each particle separately in the center frame.

Question 7 - Solution

Relative motion can be represented with reduced mass

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

With M=m1+m2M=m_1+m_2, ρ→1=m2Mr→,ρ→2=−m1Mr→,u→1=m2Mv→,u→2=−m1Mv→.\vec\rho_1=\frac{m_2}{M}\vec r,\quad\vec\rho_2=-\frac{m_1}{M}\vec r,\quad \vec u_1=\frac{m_2}{M}\vec v,\quad\vec u_2=-\frac{m_1}{M}\vec v. Substitution into the particle sum gives L→C=m1m2(m1+m2)M2r→×v→=μr→×v→,μ=2(3)5=1.20kg.\vec L_C=\frac{m_1m_2(m_1+m_2)}{M^2}\vec r\times\vec v =\mu\vec r\times\vec v,\quad\mu=\frac{2(3)}5=1.20\ \mathrm{kg}. Thus L→C=1.2(4)(5)ẑ=24ẑkgm2/s\boxed{\vec L_C=1.2(4)(5)\hat z=24\hat z\ \mathrm{kg\,m^2/s}}.

(b) Result and interpretation

The individual center-frame variables are ρ→1=2.4x̂,ρ→2=−1.6x̂,u→1=3ŷ,u→2=−2ŷ.\vec\rho_1=2.4\hat x,\quad\vec\rho_2=-1.6\hat x,\qquad \vec u_1=3\hat y,\quad\vec u_2=-2\hat y. Their angular momenta are L1,z=2.4(2)(3)=14.4,L2,z=(−1.6)(3)(−2)=9.6,L_{1,z}=2.4(2)(3)=14.4,\qquad L_{2,z}=(-1.6)(3)(-2)=9.6, LC,z=14.4+9.6=24kgm2/s.\boxed{L_{C,z}=14.4+9.6=24\ \mathrm{kg\,m^2/s}}.

Physical check

The relative velocity is 3−(−2)=53-(-2)=5 m/s and the center-frame momenta sum to zero.