A Model for Nuclear Fission — Question 3

Section 43-2 · Physics pages 7176–7177

Question 3 Competing surface and Coulomb changes can favor separated fragments A two-drop model has parent surface energy 600 MeV and Coulomb self energy 900 MeV. For an equal split at infinite separation use Us,f = 21/3Us,i and UC,f = 2−2/3UC,i. Other contributions cancel. q U Schematic; labels, not drawing lengths, specify the data. (a) Compute the potential-energy change and resulting Q value. (b) Find the minimum parent Coulomb-to-surface ratio that makes the separated final state energetically favorable.
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Question 3 - Solution Competing surface and Coulomb changes can favor separated fragments q U (a) Method and calculation ∆U = 600(21/3 −1) + 900(2−2/3 −1). ∆U = −177.083 MeV, Q = −∆U = 177.083 MeV . (b) Interpretation and further calculation ∆U < 0 ⇒UC,i Us,i > 21/3 −1 1 −2−2/3 = .702414 . 900/600 = 1.50 > .702414 so the separated state is lower. Physical check This comparison of endpoints says nothing about the highest energy along the path; it is not a criterion for barrier-free fission.

Question 3

Competing surface and Coulomb changes can favor separated fragments

A two-drop model has parent surface energy 600 MeV and Coulomb self energy 900 MeV. For an equal split at infinite separation use Us,f=21/3Us,iU_{s,f}=2^{1/3}U_{s,i} and UC,f=2−2/3UC,iU_{C,f}=2^{-2/3}U_{C,i}. Other contributions cancel.

Diagram shown in the original SVG worksheet.

  1. Compute the potential-energy change and resulting Q value.

  2. Find the minimum parent Coulomb-to-surface ratio that makes the separated final state energetically favorable.

Question 3 - Solution

Competing surface and Coulomb changes can favor separated fragments

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔU=600(21/3−1)+900(2−2/3−1).\Delta U=600(2^{1/3}-1)+900(2^{-2/3}-1).ΔU=−177.083MeV,Q=−ΔU=177.083MeV.\boxed{\Delta U=-177.083\,\mathrm{MeV},\quad Q=-\Delta U=177.083\,\mathrm{MeV}}.

(b) Interpretation and further calculation

ΔU<0⇒UC,iUs,i>21/3−11−2−2/3=.702414.\Delta U<0\Rightarrow\boxed{\frac{U_{C,i}}{U_{s,i}}>\frac{2^{1/3}-1}{1-2^{-2/3}}=.702414}.900/600=1.50>.702414so the separated state is lower.\boxed{900/600=1.50>.702414}\quad\text{so the separated state is lower}.

Physical check

This comparison of endpoints says nothing about the highest energy along the path; it is not a criterion for barrier-free fission.