A Model for Nuclear Fission — Question 4

Section 43-2 · Physics pages 7178–7179

Question 4 Small deformations test local stability of a nuclear drop For a dimensionless quadrupole deformation q, a supplied model gives U(q) −U(0) = (2Us −UC)q2/5 + O(q3). Compare drop A with Us = 500 MeV, UC = 800 MeV and drop B with Us = 500 MeV, UC = 1100 MeV. q U −U(0) A B Schematic; labels, not drawing lengths, specify the data. (a) Calculate the curvature at the spherical state and classify each drop locally. (b) Estimate the energy change at q=.100 for each and state the limit of this expansion.
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Question 4 - Solution Small deformations test local stability of a nuclear drop q U −U(0) A B (a) Method and calculation U′′(0) = 2 5(2Us −UC) . U′′ A = 80 MeV > 0, U′′ B = −40 MeV < 0 . (b) Interpretation and further calculation ∆UA ≃+.400 MeV, ∆UB ≃−.200 MeV . |q| ≪1 : O(q3) ≪O(q2) away from vanishing quadratic coefficient. Physical check Positive curvature implies a local minimum, not global stability. If the quadratic term vanishes, higher-order terms decide the behavior.

Question 4

Small deformations test local stability of a nuclear drop

For a dimensionless quadrupole deformation q, a supplied model gives U(q)−U(0)=(2Us−UC)q2/5+O(q3)U(q)-U(0)=(2U_s-U_C)q^2/5+O(q^3). Compare drop A with Us=500U_s=500 MeV, UC=800U_C=800 MeV and drop B with Us=500U_s=500 MeV, UC=1100U_C=1100 MeV.

Diagram shown in the original SVG worksheet.

  1. Calculate the curvature at the spherical state and classify each drop locally.

  2. Estimate the energy change at q=.100 for each and state the limit of this expansion.

Question 4 - Solution

Small deformations test local stability of a nuclear drop

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U′′(0)=25(2Us−UC).\boxed{U^{\prime\prime}(0)=\frac25(2U_s-U_C)}.UA′′=80MeV>0,UB′′=−40MeV<0.\boxed{U_A^{\prime\prime}=80\,\mathrm{MeV}>0,\quad U_B^{\prime\prime}=-40\,\mathrm{MeV}<0}.

(b) Interpretation and further calculation

ΔUA≃+.400MeV,ΔUB≃−.200MeV.\boxed{\Delta U_A\simeq+.400\,\mathrm{MeV},\quad\Delta U_B\simeq-.200\,\mathrm{MeV}}.|q|≪1:O(q3)≪O(q2)away from vanishing quadratic coefficient.|q|\ll1:\quad O(q^3)\ll O(q^2)\quad\text{away from vanishing quadratic coefficient}.

Physical check

Positive curvature implies a local minimum, not global stability. If the quadratic term vanishes, higher-order terms decide the behavior.