The Linear Momentum of a System of Particles — Question 10

Section 9-4 · Physics pages 1230–1231

Question 10 The same momentum can conceal different internal motion Two 1 kg particles move along a line. In state A their velocities are 1 and 3 m/s; in state B they are −2 and 6 m/s. A B 1 1 1 1 1 3 −2 6 Both pairs have the same total momentum, but their separation speeds differ; masses are in kg and velocities in m/s. (a) Compare total momentum and center velocity in the two states. (b) Compare kinetic energies in the lab and in the common center frame. What information does total momentum omit?
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Question 10 - Solution The same momentum can conceal different internal motion A B 1 1 1 1 1 3 −2 6 (a) Derivation and calculation Compute the two momentum sums: PA = 1(1) + 1(3) = 4, PB = 1(−2) + 1(6) = 4 kg m/s. PA = PB = 4 kg m/s , VC,A = VC,B = 2 m/s . (b) Result and interpretation The laboratory energies are KA = (1 + 9)/2 = 5 J and KB = (4 + 36)/2 = 20 J. Subtract the common frame speed from each velocity: K′ A = 1 2[(−1)2 + 12] = 1 J , K′ B = 1 2[(−4)2 + 42] = 16 J . K = 1 2MV 2 C + K′ = 4 J + K′. Total momentum omits the relative-motion energy. Physical check The common translational contribution is identical while the center-frame energy differs by 15 J.

Question 10

The same momentum can conceal different internal motion

Two 1kg1\,\mathrm{kg} particles move along a line. In state A their velocities are 11 and 3m/s3\,\mathrm{m/s}; in state B they are −2-2 and 6m/s6\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Compare total momentum and center velocity in the two states.

  2. Compare kinetic energies in the lab and in the common center frame. What information does total momentum omit?

Question 10 - Solution

The same momentum can conceal different internal motion

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Compute the two momentum sums: PA=1(1)+1(3)=4,PB=1(−2)+1(6)=4kgm/s.P_A=1(1)+1(3)=4,\qquad P_B=1(-2)+1(6)=4\quad\mathrm{kg\,m/s}. PA=PB=4kgm/s,VC,A=VC,B=2m/s.\boxed{P_A=P_B=4\ \mathrm{kg\,m/s}},\qquad\boxed{V_{C,A}=V_{C,B}=2\ \mathrm{m/s}}.

(b) Result and interpretation

The laboratory energies are KA=(1+9)/2=5K_A=(1+9)/2=5 J and KB=(4+36)/2=20K_B=(4+36)/2=20 J. Subtract the common frame speed from each velocity: KA′=12[(−1)2+12]=1J,KB′=12[(−4)2+42]=16J.K_A^{\prime}=\tfrac12[(-1)^2+1^2]=\boxed{1\ \mathrm J},\qquad K_B^{\prime}=\tfrac12[(-4)^2+4^2]=\boxed{16\ \mathrm J}. K=12MVC2+K′=4J+K′.K=\tfrac12MV_C^2+K^{\prime}=4\ \mathrm J+K^{\prime}. Total momentum omits the relative-motion energy.

Physical check

The common translational contribution is identical while the center-frame energy differs by 15 J.