Alpha Decay — Question 5

Section 42-4 · Physics pages 7060–7061

Question 5 The Coulomb barrier extends beyond the nuclear surface Outside a daughter nucleus of charge ZD = 82, an alpha particle sees V (r) = K/r with K = 2ZD(1.44) MeV fm. Take nuclear matching radius R = 9.00 fm and relative alpha-daughter energy Q=5.00 MeV. r V Q R b Schematic; labels, not drawing lengths, specify the data. (a) Find the Coulomb energy at R and the outer classical turning radius b. (b) Find the classically forbidden interval width and explain why an escaping alpha is classically forbidden there.
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Question 5 - Solution The Coulomb barrier extends beyond the nuclear surface r V Q R b (a) Method and calculation K = 236.16 MeV fm, V (R) = K/R = 26.24 MeV . V (b) = Q ⇒b = K/Q = 47.232 fm . (b) Interpretation and further calculation b −R = 38.232 fm . R < r < b : p2 r/(2µ) = Q −V (r) < 0 classically forbidden. Physical check Quantum tunneling permits a finite transmission probability through this region. The relative-motion energy Q and reduced mass belong in the two-body barrier model.

Question 5

The Coulomb barrier extends beyond the nuclear surface

Outside a daughter nucleus of charge ZD=82Z_D=82, an alpha particle sees V(r)=K/rV(r)=K/r with K=2ZD(1.44)MeVfmK=2Z_D(1.44)\,\mathrm{MeV\,fm}. Take nuclear matching radius R=9.00fmR=9.00\,\mathrm{fm} and relative alpha-daughter energy Q=5.00 MeV.

Diagram shown in the original SVG worksheet.

  1. Find the Coulomb energy at R and the outer classical turning radius b.

  2. Find the classically forbidden interval width and explain why an escaping alpha is classically forbidden there.

Question 5 - Solution

The Coulomb barrier extends beyond the nuclear surface

Diagram shown in the original SVG worksheet.

(a) Method and calculation

K=236.16MeVfm,V(R)=K/R=26.24MeV.\boxed{K=236.16\,\mathrm{MeV\,fm},\quad V(R)=K/R=26.24\,\mathrm{MeV}}.V(b)=Q⇒b=K/Q=47.232fm.V(b)=Q\Rightarrow\boxed{b=K/Q=47.232\,\mathrm{fm}}.

(b) Interpretation and further calculation

b−R=38.232fm.\boxed{b-R=38.232\,\mathrm{fm}}.R<r<b:pr2/(2μ)=Q−V(r)<0classically forbidden.R<r<b:\quad\boxed{p_r^2/(2\mu)=Q-V(r)<0}\quad\text{classically forbidden}.

Physical check

Quantum tunneling permits a finite transmission probability through this region. The relative-motion energy Q and reduced mass belong in the two-body barrier model.