Some Nuclear Properties — Question 5

Section 42-2 · Physics pages 7020–7021

Question 5 Atomic masses give binding energy when the electron counts cancel Use neutral-atom masses mH = 1.007825 u, mn = 1.008665 u, and M(4He) = 4.002603 u. Take 1 u c2 = 931.5 MeV and neglect electronic binding corrections. 2H + 2n B released 4He Schematic; labels, not drawing lengths, specify the data. (a) Find the mass defect and total binding energy of the helium nucleus. (b) Find binding energy per nucleon and explain the choice of hydrogen-atom mass rather than bare proton mass.
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Question 5 - Solution Atomic masses give binding energy when the electron counts cancel 2H + 2n B released 4He (a) Method and calculation ∆m = 2mH + 2mn −M = .030377 u . B = ∆mc2 = .030377(931.5) = 28.296 MeV . (b) Interpretation and further calculation B/A = 28.296/4 = 7.074 MeV . 2mH ≃2mp + 2me, M ≃mnucleus + 2me ⇒2me cancels . Physical check Using atomic masses consistently avoids an electron-rest-mass error. The small difference in electronic binding energies is outside the precision of this exercise.

Question 5

Atomic masses give binding energy when the electron counts cancel

Use neutral-atom masses mH=1.007825um_H=1.007825\,\mathrm u, mn=1.008665um_n=1.008665\,\mathrm u, and M(4He)=4.002603uM({}^{4}\mathrm{He})=4.002603\,\mathrm u. Take 1uc2=931.5MeV1\,\mathrm u\,c^2=931.5\,\mathrm{MeV} and neglect electronic binding corrections.

Diagram shown in the original SVG worksheet.

  1. Find the mass defect and total binding energy of the helium nucleus.

  2. Find binding energy per nucleon and explain the choice of hydrogen-atom mass rather than bare proton mass.

Question 5 - Solution

Atomic masses give binding energy when the electron counts cancel

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δm=2mH+2mn−M=.030377u.\boxed{\Delta m=2m_H+2m_n-M= .030377\,\mathrm u}.B=Δmc2=.030377(931.5)=28.296MeV.\boxed{B=\Delta mc^2=.030377(931.5)=28.296\,\mathrm{MeV}}.

(b) Interpretation and further calculation

B/A=28.296/4=7.074MeV.\boxed{B/A=28.296/4=7.074\,\mathrm{MeV}}.2mH≃2mp+2me,M≃mnucleus+2me⇒2me cancels.2m_H\simeq2m_p+2m_e,\quad M\simeq m_{\mathrm{nucleus}}+2m_e\Rightarrow\boxed{2m_e\text{ cancels}}.

Physical check

Using atomic masses consistently avoids an electron-rest-mass error. The small difference in electronic binding energies is outside the precision of this exercise.