A New Look at Energy — Question 7

Section 37-11 · Physics pages 6244–6245

Question 7 Fixed-target and collider thresholds differ because of center-of-mass motion Two incident particles each have mass m. A reaction requires total final rest mass 3m; ignore any additional selection rules. At threshold there is no final relative kinetic energy in the center-of-momentum frame. p1 p2 compare fixed target and equal beams Schematic; labels, not drawing lengths, specify the data. (a) For one target initially at rest, use total energy and momentum to find the projectile threshold kinetic energy. (b) For equal and opposite incident beams, find the total incident kinetic energy needed and compare.
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Question 7 - Solution Fixed-target and collider thresholds differ because of center-of-mass motion p1 p2 compare fixed target and equal beams (a) Method and calculation S = (E + mc2)2 −(pc)2 = 2m2c4 + 2mc2E. Sth = 9m2c4 ⇒ Eth = 7 2mc2, Kth = 5 2mc2 . (b) Interpretation and further calculation Pcollider = 0 : Etotal = 3mc2, Ktotal = mc2 . Kfixed/Kcollider,total = 5/2 . Physical check The fixed-target laboratory retains unavoidable bulk motion at threshold, so less of its input energy is available as final rest energy.

Question 7

Fixed-target and collider thresholds differ because of center-of-mass motion

Two incident particles each have mass m. A reaction requires total final rest mass 3m3m; ignore any additional selection rules. At threshold there is no final relative kinetic energy in the center-of-momentum frame.

Diagram shown in the original SVG worksheet.

  1. For one target initially at rest, use total energy and momentum to find the projectile threshold kinetic energy.

  2. For equal and opposite incident beams, find the total incident kinetic energy needed and compare.

Question 7 - Solution

Fixed-target and collider thresholds differ because of center-of-mass motion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝒮=(E+mc2)2−(pc)2=2m2c4+2mc2E.\mathcal S=(E+mc^2)^2-(pc)^2=2m^2c^4+2mc^2E.𝒮th=9m2c4⇒Eth=72mc2,Kth=52mc2.\mathcal S_{\mathrm{th}}=9m^2c^4\quad\Rightarrow\quad E_{\mathrm{th}}=\tfrac72mc^2,\quad\boxed{K_{\mathrm{th}}=\tfrac52mc^2}.

(b) Interpretation and further calculation

Pcollider=0:Etotal=3mc2,Ktotal=mc2.P_{\mathrm{collider}}=0:\quad E_{\mathrm{total}}=3mc^2,\quad\boxed{K_{\mathrm{total}}=mc^2}.Kfixed/Kcollider,total=5/2.\boxed{K_{\mathrm{fixed}}/K_{\mathrm{collider,total}}=5/2}.

Physical check

The fixed-target laboratory retains unavoidable bulk motion at threshold, so less of its input energy is available as final rest energy.