A Model for Nuclear Fission — Question 6

Section 43-2 · Physics pages 7182–7183

Question 6 Neutron capture supplies excitation through separation energy A heavy target absorbs a neutron. Neglect target recoil, so compound-nucleus excitation is E∗= Sn + Kn. Two hypothetical nuclei have (Sn, Bf) = (6.4, 6.0) MeV and (4.8, 6.0) MeV. Here Bf is the fission barrier above the compound ground state. compound ground state barrier Bf Schematic; labels, not drawing lengths, specify the data. (a) For negligible neutron kinetic energy, decide which compound excitation lies above its barrier. (b) Find the minimum neutron kinetic energy needed to reach the barrier in each idealized case.
Show solutionHide solution
Question 6 - Solution Neutron capture supplies excitation through separation energy compound ground state barrier Bf (a) Method and calculation Kn ≃0 : E∗ A −BA = +.4 MeV, E∗ B −BB = −1.2 MeV . A : above barrier; B : below barrier . (b) Interpretation and further calculation Sn + Kn ≥Bf ⇒Kn,min = max(0, Bf −Sn) . Kn,min,A = 0, Kn,min,B = 1.2 MeV . Physical check Above-barrier excitation does not guarantee fission: neutron emission and photon emission may compete. Quantum tunneling can permit below-barrier decay.

Question 6

Neutron capture supplies excitation through separation energy

A heavy target absorbs a neutron. Neglect target recoil, so compound-nucleus excitation is E*=Sn+KnE^*=S_n+K_n. Two hypothetical nuclei have (Sn,Bf)=(6.4,6.0)(S_n,B_f)=(6.4,6.0) MeV and (4.8,6.0)(4.8,6.0) MeV. Here BfB_f is the fission barrier above the compound ground state.

Diagram shown in the original SVG worksheet.

  1. For negligible neutron kinetic energy, decide which compound excitation lies above its barrier.

  2. Find the minimum neutron kinetic energy needed to reach the barrier in each idealized case.

Question 6 - Solution

Neutron capture supplies excitation through separation energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Kn≃0:EA*−BA=+.4MeV,EB*−BB=−1.2MeV.K_n\simeq0:\quad\boxed{E_A^*-B_A=+.4\,\mathrm{MeV},\quad E_B^*-B_B=-1.2\,\mathrm{MeV}}.A: above barrier;B: below barrier.\boxed{A:\text{ above barrier};\qquad B:\text{ below barrier}}.

(b) Interpretation and further calculation

Sn+Kn≥Bf⇒Kn,min=max⁡(0,Bf−Sn).S_n+K_n\ge B_f\Rightarrow\boxed{K_{n,\min}=\max(0,B_f-S_n)}.Kn,min⁡,A=0,Kn,min⁡,B=1.2MeV.\boxed{K_{n,\min,A}=0,\quad K_{n,\min,B}=1.2\,\mathrm{MeV}}.

Physical check

Above-barrier excitation does not guarantee fission: neutron emission and photon emission may compete. Quantum tunneling can permit below-barrier decay.