Discovering the Nucleus — Question 9

Section 42-1 · Physics pages 7008–7009

Question 9 Matter-wave resolution tests whether a nucleus can be resolved For a nonrelativistic alpha particle use pc = √ 2mc2E, mc2 = 3727 MeV and ℏc = 197.3 MeV fm. Define a reduced-wavelength resolution scale ℓ= ℏ/p. R p Schematic; labels, not drawing lengths, specify the data. (a) Calculate ell for E=5.00 MeV. (b) Find the kinetic energy for ℓ= 2.00 fm, and check whether the nonrelativistic approximation remains reasonable.
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Question 9 - Solution Matter-wave resolution tests whether a nucleus can be resolved R p (a) Method and calculation pc = √ 2(3727)(5.00) = 193.1 MeV. ℓ= ℏc/(pc) = 1.022 fm . (b) Interpretation and further calculation E = (ℏc)2/[2mc2ℓ2] = 1.306 MeV . E/(mc2) = 3.503 × 10−4 ≪1 . Physical check The full de Broglie wavelength is 2 pi times ell. Short wavelength alone does not ensure close approach; the Coulomb barrier also restricts which radii are sampled.

Question 9

Matter-wave resolution tests whether a nucleus can be resolved

For a nonrelativistic alpha particle use pc=2mc2Epc=\sqrt{2mc^2E}, mc2=3727MeVmc^2=3727\,\mathrm{MeV} and ℏc=197.3MeVfm\hbar c=197.3\,\mathrm{MeV\,fm}. Define a reduced-wavelength resolution scale ℓ=ℏ/p\ell=\hbar/p.

Diagram shown in the original SVG worksheet.

  1. Calculate ell for E=5.00 MeV.

  2. Find the kinetic energy for ℓ=2.00fm\ell=2.00\,\mathrm{fm}, and check whether the nonrelativistic approximation remains reasonable.

Question 9 - Solution

Matter-wave resolution tests whether a nucleus can be resolved

Diagram shown in the original SVG worksheet.

(a) Method and calculation

pc=2(3727)(5.00)=193.1MeV.pc=\sqrt{2(3727)(5.00)}=193.1\,\mathrm{MeV}.ℓ=ℏc/(pc)=1.022fm.\boxed{\ell=\hbar c/(pc)=1.022\,\mathrm{fm}}.

(b) Interpretation and further calculation

E=(ℏc)2/[2mc2ℓ2]=1.306MeV.\boxed{E=(\hbar c)^2/[2mc^2\ell^2]=1.306\,\mathrm{MeV}}.E/(mc2)=3.503×10−4≪1.\boxed{E/(mc^2)=3.503\times10^{-4}\ll1}.

Physical check

The full de Broglie wavelength is 2 pi times ell. Short wavelength alone does not ensure close approach; the Coulomb barrier also restricts which radii are sampled.