Measuring Radiation Dosage — Question 7

Section 42-7 · Physics pages 7124–7125

Question 7 Source decay limits the integrated dose in a fixed geometry In a fixed source-detector arrangement, dose rate initially is ˙D0 = .800 mGy/h and follows the source decay with half-life 2.00 h. Geometry and absorption remain fixed. t ˙D Schematic; labels, not drawing lengths, specify the data. (a) Derive dose accumulated in time T and its infinite-time limit. (b) Calculate the dose over 6.00 h and the overestimate from assuming constant initial dose rate.
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Question 7 - Solution Source decay limits the integrated dose in a fixed geometry t ˙D (a) Method and calculation D(T) = ∫T 0 ˙D0e−λtdt = ˙D0 λ (1 −e−λT ) . D(∞) = ˙D0/λ = .800(2.00)/ ln 2 = 2.308 mGy . (b) Interpretation and further calculation D(6) = D(∞)(1 −1/8) = 2.020 mGy . Dconstant = .800(6) = 4.800 mGy, Dconstant/D(6) = 2.377 . Physical check The infinite-time total is finite because the integrated number of parent decays is finite. Time units for the rate and decay constant must agree.

Question 7

Source decay limits the integrated dose in a fixed geometry

In a fixed source-detector arrangement, dose rate initially is Ḋ0=.800mGy/h\dot D_0=.800\,\mathrm{mGy/h} and follows the source decay with half-life 2.00 h. Geometry and absorption remain fixed.

Diagram shown in the original SVG worksheet.

  1. Derive dose accumulated in time T and its infinite-time limit.

  2. Calculate the dose over 6.00 h and the overestimate from assuming constant initial dose rate.

Question 7 - Solution

Source decay limits the integrated dose in a fixed geometry

Diagram shown in the original SVG worksheet.

(a) Method and calculation

D(T)=∫0TḊ0e−λtdt=Ḋ0λ(1−e−λT).D(T)=\int_0^T\dot D_0e^{-\lambda t}dt=\boxed{\frac{\dot D_0}{\lambda}(1-e^{-\lambda T})}.D(∞)=Ḋ0/λ=.800(2.00)/ln⁡2=2.308mGy.\boxed{D(\infty)=\dot D_0/\lambda=.800(2.00)/\ln2=2.308\,\mathrm{mGy}}.

(b) Interpretation and further calculation

D(6)=D(∞)(1−1/8)=2.020mGy.\boxed{D(6)=D(\infty)(1-1/8)=2.020\,\mathrm{mGy}}.Dconstant=.800(6)=4.800mGy,Dconstant/D(6)=2.377.\boxed{D_{\mathrm{constant}}=.800(6)=4.800\,\mathrm{mGy},\quad D_{\mathrm{constant}}/D(6)=2.377}.

Physical check

The infinite-time total is finite because the integrated number of parent decays is finite. Time units for the rate and decay constant must agree.