The Linear Momentum of a System of Particles — Question 1

Section 9-4 · Physics pages 1212–1213

Question 1 A vector inventory reveals the center velocity Three particles have masses 1, 2, 3 kg and velocities (4, 0), (−1, 2), (0, −1) m/s. x y⃗ p1⃗ p2⃗ p3⃗ P Head-to-tail addition of the three particle momenta gives the system momentum. (a) Find total momentum and center velocity. (b) Can replacing the particles by a 6 kg point at the center reproduce their total kinetic energy?
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Question 1 - Solution A vector inventory reveals the center velocity x y⃗ p1⃗ p2⃗ p3⃗ P (a) Derivation and calculation Sum the vector momenta, then divide by total mass:⃗ P = 1(4, 0) + 2(−1, 2) + 3(0, −1) = (2, 1) kg m/s . M = 6 kg,⃗ VC =⃗P/M = (1/3, 1/6) m/s . (b) Result and interpretation The actual and center-translation energies differ: K = 1 2(1)(16) + 1 2(2)(5) + 1 2(3)(1) = 14.5 J. KC = P 2 2M = 5 12 J, Krelative = K −KC = 169 12 J . A single center point reproduces momentum but omits relative-motion energy. Physical check The nonnegative relative energy explains why zero or small center speed need not mean little kinetic energy.

Question 1

A vector inventory reveals the center velocity

Three particles have masses 11, 22, 3kg3\,\mathrm{kg} and velocities (4,0)(4,0), (−1,2)(-1,2), (0,−1)m/s(0,-1)\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find total momentum and center velocity.

  2. Can replacing the particles by a 6kg6\,\mathrm{kg} point at the center reproduce their total kinetic energy?

Question 1 - Solution

A vector inventory reveals the center velocity

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Sum the vector momenta, then divide by total mass: P→=1(4,0)+2(−1,2)+3(0,−1)=(2,1)kgm/s.\boxed{\vec P=1(4,0)+2(-1,2)+3(0,-1)=(2,1)\ \mathrm{kg\,m/s}}. M=6kg,V→C=P→/M=(1/3,1/6)m/s.M=6\ \mathrm{kg},\qquad\boxed{\vec V_C=\vec P/M=(1/3,1/6)\ \mathrm{m/s}}.

(b) Result and interpretation

The actual and center-translation energies differ: K=12(1)(16)+12(2)(5)+12(3)(1)=14.5J.K=\tfrac12(1)(16)+\tfrac12(2)(5)+\tfrac12(3)(1)=14.5\ \mathrm J. KC=P22M=512J,Krelative=K−KC=16912J.K_C=\frac{P^2}{2M}=\frac5{12}\ \mathrm J,\qquad \boxed{K_{\mathrm{relative}}=K-K_C=\frac{169}{12}\ \mathrm J}. A single center point reproduces momentum but omits relative-motion energy.

Physical check

The nonnegative relative energy explains why zero or small center speed need not mean little kinetic energy.