Alpha Decay — Question 6

Section 42-4 · Physics pages 7062–7063

Question 6 A rectangular-barrier model quantifies tunneling sensitivity For a simplified barrier, use P = e−2κL, where κ = √ 2µc2(V0 −Q)/(ℏc). Let µc2 = 3600 MeV, V0 −Q = 10.0 MeV, L = 10.0 fm, and ℏc = 197.3 MeV fm. x V Q V0 0 L Schematic; labels, not drawing lengths, specify the data. (a) Evaluate kappa and the penetration probability. (b) Find the ratio of probabilities if the barrier width increases by 1.00 fm while all other quantities remain fixed.
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Question 6 - Solution A rectangular-barrier model quantifies tunneling sensitivity x V Q V0 0 L (a) Method and calculation κ = √ 2(3600)(10.0)/197.3 = 1.360 fm−1 . P = e−2κL = 1.54 × 10−12 . (b) Interpretation and further calculation P(L + ∆L)/P(L) = e−2κ∆L. P(11.0)/P(10.0) = e−2(1.360)(1.00) ≃.0659 . Physical check The rectangular barrier is a supplied approximation, not the true Coulomb shape. It demonstrates how a small geometric change can strongly alter the decay rate.

Question 6

A rectangular-barrier model quantifies tunneling sensitivity

For a simplified barrier, use P=e−2κLP=e^{-2\kappa L}, where κ=2μc2(V0−Q)/(ℏc)\kappa=\sqrt{2\mu c^2(V_0-Q)}/(\hbar c). Let μc2=3600MeV\mu c^2=3600\,\mathrm{MeV}, V0−Q=10.0MeVV_0-Q=10.0\,\mathrm{MeV}, L=10.0fmL=10.0\,\mathrm{fm}, and ℏc=197.3MeVfm\hbar c=197.3\,\mathrm{MeV\,fm}.

Diagram shown in the original SVG worksheet.

  1. Evaluate kappa and the penetration probability.

  2. Find the ratio of probabilities if the barrier width increases by 1.00 fm while all other quantities remain fixed.

Question 6 - Solution

A rectangular-barrier model quantifies tunneling sensitivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

κ=2(3600)(10.0)/197.3=1.360fm−1.\boxed{\kappa=\sqrt{2(3600)(10.0)}/197.3=1.360\,\mathrm{fm^{-1}}}.P=e−2κL=1.54×10−12.\boxed{P=e^{-2\kappa L}=1.54\times10^{-12}}.

(b) Interpretation and further calculation

P(L+ΔL)/P(L)=e−2κΔL.P(L+\Delta L)/P(L)=e^{-2\kappa\Delta L}.P(11.0)/P(10.0)=e−2(1.360)(1.00)≃.0659.\boxed{P(11.0)/P(10.0)=e^{-2(1.360)(1.00)}\simeq.0659}.

Physical check

The rectangular barrier is a supplied approximation, not the true Coulomb shape. It demonstrates how a small geometric change can strongly alter the decay rate.