Discovering the Nucleus — Question 5

Section 42-1 · Physics pages 7000–7001

Question 5 A thin-foil count rate measures differential cross section A foil has areal nuclear density nt = 2.00 × 1022 m−2. The beam rate is F = 106 s−1. A small detector subtends ∆Ω= 10−3 sr and has efficiency .800. At its angle, dσ/dΩ= 5.00 × 10−28 m2/sr. Assume single scattering. source detector r Schematic; labels, not drawing lengths, specify the data. (a) Derive and evaluate detected rate. (b) How long is needed for a 5 percent relative Poisson uncertainty in the signal if background is negligible?
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Question 5 - Solution A thin-foil count rate measures differential cross section source detector r (a) Method and calculation P = nt dσ dΩ∆Ω, R = εFP. R = .800(106)(2 × 1022)(5 × 10−28)(10−3) = .00800 s−1 . (b) Interpretation and further calculation σN/N = 1/ √ N = .0500 ⇒N = 400 . t = N/R = 5.00 × 104 s = 13.89 h . Physical check The small scattering probability justifies neglecting repeated scattering into the detector. Counting uncertainty depends on detected counts, not on incident beam particles.

Question 5

A thin-foil count rate measures differential cross section

A foil has areal nuclear density nt=2.00×1022m−2n_t=2.00\times10^{22}\,\mathrm{m^{-2}}. The beam rate is F=106s−1F=10^6\,\mathrm{s^{-1}}. A small detector subtends ΔΩ=10−3sr\Delta\Omega=10^{-3}\,\mathrm{sr} and has efficiency .800. At its angle, dσ/dΩ=5.00×10−28m2/srd\sigma/d\Omega=5.00\times10^{-28}\,\mathrm{m^2/sr}. Assume single scattering.

Diagram shown in the original SVG worksheet.

  1. Derive and evaluate detected rate.

  2. How long is needed for a 5 percent relative Poisson uncertainty in the signal if background is negligible?

Question 5 - Solution

A thin-foil count rate measures differential cross section

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P=ntdσdΩΔΩ,R=εFP.P=n_t\frac{d\sigma}{d\Omega}\Delta\Omega,\qquad R=\varepsilon FP.R=.800(106)(2×1022)(5×10−28)(10−3)=.00800s−1.\boxed{R=.800(10^6)(2\times10^{22})(5\times10^{-28})(10^{-3})=.00800\,\mathrm{s^{-1}}}.

(b) Interpretation and further calculation

σN/N=1/N=.0500⇒N=400.\sigma_N/N=1/\sqrt N=.0500\Rightarrow\boxed{N=400}.t=N/R=5.00×104s=13.89h.\boxed{t=N/R=5.00\times10^4\,\mathrm s=13.89\,\mathrm h}.

Physical check

The small scattering probability justifies neglecting repeated scattering into the detector. Counting uncertainty depends on detected counts, not on incident beam particles.