Some Nuclear Properties — Question 7

Section 42-2 · Physics pages 7024–7025

Question 7 A negative reaction Q value implies more than a simple energy deficit A projectile of mass m strikes a stationary target of mass M = 4m. A reaction has Q = −2.00 MeV. Work to leading nonrelativistic order in |Q|/(Mc2). The available center-of-mass kinetic energy is Ecm = EM/(m + M). m, E 4m Schematic; labels, not drawing lengths, specify the data. (a) Find the laboratory threshold energy. (b) At incident energy 3.00 MeV, find the final kinetic energy available in the center-of-mass frame.
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Question 7 - Solution A negative reaction Q value implies more than a simple energy deficit m, E 4m (a) Method and calculation Ecm,th + Q = 0 ⇒Eth = −Q(1 + m/M) . Eth = 2.00(1 + 1/4) = 2.50 MeV . (b) Interpretation and further calculation Ecm = 3.00(4/5) = 2.40 MeV. Kf,cm = Ecm + Q = .400 MeV . Physical check Some laboratory energy must remain as translational motion of the center of mass. That momentum constraint raises the threshold above the magnitude of Q.

Question 7

A negative reaction Q value implies more than a simple energy deficit

A projectile of mass m strikes a stationary target of mass M=4mM=4m. A reaction has Q=−2.00MeVQ=-2.00\,\mathrm{MeV}. Work to leading nonrelativistic order in |Q|/(Mc2)|Q|/(Mc^2). The available center-of-mass kinetic energy is Ecm=EM/(m+M)E_{\mathrm{cm}}=EM/(m+M).

Diagram shown in the original SVG worksheet.

  1. Find the laboratory threshold energy.

  2. At incident energy 3.00 MeV, find the final kinetic energy available in the center-of-mass frame.

Question 7 - Solution

A negative reaction Q value implies more than a simple energy deficit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ecm,th+Q=0⇒Eth=−Q(1+m/M).E_{{\mathrm{cm}},\mathrm{th}}+Q=0\Rightarrow\boxed{E_{\mathrm{th}}=-Q(1+m/M)}.Eth=2.00(1+1/4)=2.50MeV.\boxed{E_{\mathrm{th}}=2.00(1+1/4)=2.50\,\mathrm{MeV}}.

(b) Interpretation and further calculation

Ecm=3.00(4/5)=2.40MeV.E_{\mathrm{cm}}=3.00(4/5)=2.40\,\mathrm{MeV}.Kf,cm=Ecm+Q=.400MeV.\boxed{K_{f,\mathrm{cm}}=E_{\mathrm{cm}}+Q=.400\,\mathrm{MeV}}.

Physical check

Some laboratory energy must remain as translational motion of the center of mass. That momentum constraint raises the threshold above the magnitude of Q.