A Model for Nuclear Fission — Question 10

Section 43-2 · Physics pages 7190–7191

Question 10 Shell corrections can reverse a smooth-model preference for a split A smooth liquid-drop model predicts final potential energies 0 MeV for symmetric channel S and +4 MeV for asymmetric channel A, relative to a common reference. Shell corrections are -1 MeV for S and -8 MeV for A. S A shell corrections lower both energies Schematic; labels, not drawing lengths, specify the data. (a) Calculate the corrected channel energies and identify which is lower. (b) For a supplied statistical weight model wi ∝e−Ui/Θ with Θ = 1.50 MeV, find wA/wS before and after the corrections.
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Question 10 - Solution Shell corrections can reverse a smooth-model preference for a split S A shell corrections lower both energies (a) Method and calculation US = −1 MeV, UA = 4 −8 = −4 MeV . UA −US = −3 MeV so A is lower. (b) Interpretation and further calculation (wA/wS)smooth = e−4/1.5 = .069483 . (wA/wS)corrected = e−(−3)/1.5 = e2 = 7.38906 . Physical check This supplied weight law illustrates sensitivity to structure. Real fission yields also depend on dynamical paths and cannot be predicted from endpoint energy alone.

Question 10

Shell corrections can reverse a smooth-model preference for a split

A smooth liquid-drop model predicts final potential energies 0 MeV for symmetric channel S and +4 MeV for asymmetric channel A, relative to a common reference. Shell corrections are -1 MeV for S and -8 MeV for A.

Diagram shown in the original SVG worksheet.

  1. Calculate the corrected channel energies and identify which is lower.

  2. For a supplied statistical weight model wi∝e−Ui/Θw_i\propto e^{-U_i/\Theta} with Θ=1.50\Theta=1.50 MeV, find wA/wSw_A/w_S before and after the corrections.

Question 10 - Solution

Shell corrections can reverse a smooth-model preference for a split

Diagram shown in the original SVG worksheet.

(a) Method and calculation

US=−1MeV,UA=4−8=−4MeV.\boxed{U_S=-1\,\mathrm{MeV},\quad U_A=4-8=-4\,\mathrm{MeV}}.UA−US=−3MeVso A is lower.\boxed{U_A-U_S=-3\,\mathrm{MeV}}\quad\text{so A is lower}.

(b) Interpretation and further calculation

(wA/wS)smooth=e−4/1.5=.069483.\boxed{(w_A/w_S)_{\mathrm{smooth}}=e^{-4/1.5}=.069483}.(wA/wS)corrected=e−(−3)/1.5=e2=7.38906.\boxed{(w_A/w_S)_{\mathrm{corrected}}=e^{-(-3)/1.5}=e^2=7.38906}.

Physical check

This supplied weight law illustrates sensitivity to structure. Real fission yields also depend on dynamical paths and cannot be predicted from endpoint energy alone.