A New Look at Energy — Question 6

Section 37-11 · Physics pages 6242–6243

Question 6 An asymmetric inelastic collision separates bulk motion from internal energy A particle of mass m moving at 0.60c strikes an identical stationary particle and sticks to it. The system is isolated and radiates no energy. Use E2 = p2c2 + m2c4, E = γmc2, K = E −mc2, and v = c2p/E. .6c rest isolated inelastic collision Schematic; labels, not drawing lengths, specify the data. (a) Find the composite velocity and invariant mass from total energy and momentum. (b) Find the composite laboratory kinetic energy and the increase of its rest energy above 2mc2.
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Question 6 - Solution An asymmetric inelastic collision separates bulk motion from internal energy .6c rest isolated inelastic collision (a) Method and calculation Ei = (1.25 + 1)mc2 = 9 4mc2, Pi = 3 4mc ⇒ Vf = c/3 . M2c4 = E2 i −P 2 i c2 = 9 2m2c4 ⇒ M = 3m/ √ 2 . (b) Interpretation and further calculation Kf = (9 4 −3 √ 2 ) mc2 ≃0.128680mc2 . ∆Einternal = ( 3 √ 2 −2 ) mc2 ≃0.121320mc2 . Physical check The initial 0.250mc-squared kinetic energy is divided between final bulk motion and retained internal energy.

Question 6

An asymmetric inelastic collision separates bulk motion from internal energy

A particle of mass m moving at 0.60c0.60c strikes an identical stationary particle and sticks to it. The system is isolated and radiates no energy. Use E2=p2c2+m2c4E^2=p^2c^2+m^2c^4, E=γmc2E=\gamma mc^2, K=E−mc2K=E-mc^2, and 𝒗=c2𝒑/E\mathbf v=c^2\mathbf p/E.

Diagram shown in the original SVG worksheet.

  1. Find the composite velocity and invariant mass from total energy and momentum.

  2. Find the composite laboratory kinetic energy and the increase of its rest energy above 2mc22mc^2.

Question 6 - Solution

An asymmetric inelastic collision separates bulk motion from internal energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ei=(1.25+1)mc2=94mc2,Pi=34mc⇒Vf=c/3.E_i=(1.25+1)mc^2=\tfrac94mc^2,\quad P_i=\tfrac34mc\quad\Rightarrow\quad\boxed{V_f=c/3}.M2c4=Ei2−Pi2c2=92m2c4⇒M=3m/2.M^2c^4=E_i^2-P_i^2c^2=\tfrac92m^2c^4\quad\Rightarrow\quad\boxed{M=3m/\sqrt2}.

(b) Interpretation and further calculation

Kf=(94−32)mc2≃0.128680mc2.\boxed{K_f=\left(\frac94-\frac3{\sqrt2}\right)mc^2\simeq0.128680mc^2}.ΔEinternal=(32−2)mc2≃0.121320mc2.\boxed{\Delta E_{\mathrm{internal}}=\left(\frac3{\sqrt2}-2\right)mc^2\simeq0.121320mc^2}.

Physical check

The initial 0.250mc-squared kinetic energy is divided between final bulk motion and retained internal energy.