Some Nuclear Properties — Question 2

Section 42-2 · Physics pages 7014–7015

Question 2 Isotopic abundance determines the mean atomic mass An idealized element contains isotopes of masses 62.0 u and 65.0 u. Its mean atomic mass is 63.2 u. Let f be the number fraction of the heavier isotope. m .6 .4 62 65 Schematic; labels, not drawing lengths, specify the data. (a) Find the abundance fractions. (b) Find the standard deviation of the mass of a randomly selected atom and distinguish it from the uncertainty in the mean of 106 independent atoms.
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Question 2 - Solution Isotopic abundance determines the mean atomic mass m .6 .4 62 65 (a) Method and calculation ¯m = (1 −f)(62.0) + f(65.0) = 62.0 + 3f. f = (63.2 −62.0)/3 = .400, 1 −f = .600 . (b) Interpretation and further calculation σ2 m = .6(62 −63.2)2 + .4(65 −63.2)2 = 2.16 u2, σm = 1.470 u . σ ¯m = σm/ √ 106 = .001470 u . Physical check The isotope spread is a real variation among atoms. Averaging many independent atoms reduces uncertainty in the mean without narrowing that underlying distribution.

Question 2

Isotopic abundance determines the mean atomic mass

An idealized element contains isotopes of masses 62.0 u and 65.0 u. Its mean atomic mass is 63.2 u. Let f be the number fraction of the heavier isotope.

Diagram shown in the original SVG worksheet.

  1. Find the abundance fractions.

  2. Find the standard deviation of the mass of a randomly selected atom and distinguish it from the uncertainty in the mean of 10610^6 independent atoms.

Question 2 - Solution

Isotopic abundance determines the mean atomic mass

Diagram shown in the original SVG worksheet.

(a) Method and calculation

m‾=(1−f)(62.0)+f(65.0)=62.0+3f.\bar m=(1-f)(62.0)+f(65.0)=62.0+3f.f=(63.2−62.0)/3=.400,1−f=.600.\boxed{f=(63.2-62.0)/3=.400,\quad1-f=.600}.

(b) Interpretation and further calculation

σm2=.6(62−63.2)2+.4(65−63.2)2=2.16u2,σm=1.470u.\boxed{\sigma_m^2=.6(62-63.2)^2+.4(65-63.2)^2=2.16\,\mathrm{u^2},\quad\sigma_m=1.470\,\mathrm u}.σm‾=σm/106=.001470u.\boxed{\sigma_{\bar m}=\sigma_m/\sqrt{10^6}=.001470\,\mathrm u}.

Physical check

The isotope spread is a real variation among atoms. Averaging many independent atoms reduces uncertainty in the mean without narrowing that underlying distribution.