Measuring Radiation Dosage — Question 4

Section 42-7 · Physics pages 7118–7119

Question 4 Activity becomes dose only after emission and absorption are specified A source has constant activity A = 106 Bq during a 600 s interval. Each decay emits on average .500 photons of energy 1.00 MeV. A specified absorber of mass .100 kg retains .0100 of the total photon energy emitted. Use 1 MeV = 1.60 × 10−13 J. source absorber r Schematic; labels, not drawing lengths, specify the data. (a) Find the emitted photon number and absorbed energy. (b) Find absorbed dose and identify the factors that prevent activity alone from determining dose.
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Question 4 - Solution Activity becomes dose only after emission and absorption are specified source absorber r (a) Method and calculation Nγ = Aty = (106)(600)(.500) = 3.00 × 108 . Eabs = fNγEγ = .0100(3.00 × 108)(1.60 × 10−13) = 4.80 × 10−7 J . (b) Interpretation and further calculation D = Eabs/m = 4.80 × 10−6 Gy = 4.80 µGy . D = At yEγf/m requires yield, energy, deposition fraction and mass. Physical check The deposition fraction already includes geometry and energy escape for the stated absorber. It must not be counted a second time as another efficiency.

Question 4

Activity becomes dose only after emission and absorption are specified

A source has constant activity 𝒜=106Bq\mathcal A=10^6\,\mathrm{Bq} during a 600 s interval. Each decay emits on average .500 photons of energy 1.00 MeV. A specified absorber of mass .100 kg retains .0100 of the total photon energy emitted. Use 1MeV=1.60×10−13J1\,\mathrm{MeV}=1.60\times10^{-13}\,\mathrm J.

Diagram shown in the original SVG worksheet.

  1. Find the emitted photon number and absorbed energy.

  2. Find absorbed dose and identify the factors that prevent activity alone from determining dose.

Question 4 - Solution

Activity becomes dose only after emission and absorption are specified

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Nγ=𝒜ty=(106)(600)(.500)=3.00×108.\boxed{N_\gamma=\mathcal A t y=(10^6)(600)(.500)=3.00\times10^8}.Eabs=fNγEγ=.0100(3.00×108)(1.60×10−13)=4.80×10−7J.\boxed{E_{\mathrm{abs}}=fN_\gamma E_\gamma=.0100(3.00\times10^8)(1.60\times10^{-13})=4.80\times10^{-7}\,\mathrm J}.

(b) Interpretation and further calculation

D=Eabs/m=4.80×10−6Gy=4.80μGy.\boxed{D=E_{\mathrm{abs}}/m=4.80\times10^{-6}\,\mathrm{Gy}=4.80\,\mu\mathrm{Gy}}.D=𝒜tyEγf/mrequires yield, energy, deposition fraction and mass.\boxed{D=\mathcal A t\,yE_\gamma f/m}\quad\text{requires yield, energy, deposition fraction and mass}.

Physical check

The deposition fraction already includes geometry and energy escape for the stated absorber. It must not be counted a second time as another efficiency.