A Model for Nuclear Fission — Question 2

Section 43-2 · Physics pages 7174–7175

Question 2 Charge separation reduces the self energy of two distant drops A uniformly charged drop has Coulomb self energy UC = 3Q2/(20πε0R). It divides equally in charge and volume. Treat the two daughter drops as infinitely separated; initial self energy is 900 MeV. R r Schematic; labels, not drawing lengths, specify the data. (a) Find the sum of daughter self energies relative to the parent value. (b) Compute the energy decrease and identify the extra Coulomb term needed at a finite center separation d.
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Question 2 - Solution Charge separation reduces the self energy of two distant drops R r (a) Method and calculation Qd = Q/2, r = R2−1/3 ⇒UC,f UC,i = 2(Q/2)2 Q2 R r . UC,f/UC,i = 2−2/3 = .629961 . (b) Interpretation and further calculation ∆UC = 900(2−2/3 −1) = −333.036 MeV . Umutual(d) = (Q/2)2 4πε0d > 0 (d ≥2r). Physical check The mutual term vanishes only at infinite separation. Adding it at contact prevents confusing self-energy relief with the full deformation path.

Question 2

Charge separation reduces the self energy of two distant drops

A uniformly charged drop has Coulomb self energy UC=3Q2/(20πε0R)U_C=3Q^2/(20\pi\varepsilon_0R). It divides equally in charge and volume. Treat the two daughter drops as infinitely separated; initial self energy is 900 MeV.

Diagram shown in the original SVG worksheet.

  1. Find the sum of daughter self energies relative to the parent value.

  2. Compute the energy decrease and identify the extra Coulomb term needed at a finite center separation d.

Question 2 - Solution

Charge separation reduces the self energy of two distant drops

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qd=Q/2,r=R2−1/3⇒UC,fUC,i=2(Q/2)2Q2Rr.Q_d=Q/2,\quad r=R2^{-1/3}\Rightarrow\frac{U_{C,f}}{U_{C,i}}=2\frac{(Q/2)^2}{Q^2}\frac Rr.UC,f/UC,i=2−2/3=.629961.\boxed{U_{C,f}/U_{C,i}=2^{-2/3}=.629961}.

(b) Interpretation and further calculation

ΔUC=900(2−2/3−1)=−333.036MeV.\boxed{\Delta U_C=900(2^{-2/3}-1)=-333.036\,\mathrm{MeV}}.Umutual(d)=(Q/2)24πε0d>0(d≥2r).\boxed{U_{\mathrm{mutual}}(d)=\frac{(Q/2)^2}{4\pi\varepsilon_0d}>0}\quad(d\ge2r).

Physical check

The mutual term vanishes only at infinite separation. Adding it at contact prevents confusing self-energy relief with the full deformation path.