Measuring Radiation Dosage — Question 5

Section 42-7 · Physics pages 7120–7121

Question 5 A moving detector accumulates an integral of the inverse-square dose rate An ideal point source gives dose rate ˙D(r) = ˙D0(r0/r)2 in a small detector. It moves radially outward with r(t) = r0 + vt, with r0 = 1.00 m, v = .100 m/min and ˙D0 = 12.0 µGy/min. Ignore attenuation and source decay. source detector r v Schematic; labels, not drawing lengths, specify the data. (a) Integrate dose over a travel time T. (b) Evaluate dose for T=10.0 min and compare it with remaining at r0 for that interval.
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Question 5 - Solution A moving detector accumulates an integral of the inverse-square dose rate source detector r v (a) Method and calculation D(T) = ˙D0r2 0 ∫T 0 dt (r0 + vt)2 . D(T) = ˙D0r0 v ( 1 − r0 r0 + vT ) . (b) Interpretation and further calculation D(10) = 12.0(1.00) .100 (1 −1/2) = 60.0 µGy . Dfixed = ˙D0T = 120 µGy, D/Dfixed = .500 . Physical check The point-source model applies when detector and source dimensions are small relative to their separation. The time average of an inverse-square rate is not generally its value at the mean distance.

Question 5

A moving detector accumulates an integral of the inverse-square dose rate

An ideal point source gives dose rate Ḋ(r)=Ḋ0(r0/r)2\dot D(r)=\dot D_0(r_0/r)^2 in a small detector. It moves radially outward with r(t)=r0+vtr(t)=r_0+vt, with r0=1.00mr_0=1.00\,\mathrm m, v=.100m/minv=.100\,\mathrm{m/min} and Ḋ0=12.0μGy/min\dot D_0=12.0\,\mu\mathrm{Gy/min}. Ignore attenuation and source decay.

Diagram shown in the original SVG worksheet.

  1. Integrate dose over a travel time T.

  2. Evaluate dose for T=10.0 min and compare it with remaining at r0r_0 for that interval.

Question 5 - Solution

A moving detector accumulates an integral of the inverse-square dose rate

Diagram shown in the original SVG worksheet.

(a) Method and calculation

D(T)=Ḋ0r02∫0Tdt(r0+vt)2.D(T)=\dot D_0r_0^2\int_0^T\frac{dt}{(r_0+vt)^2}.D(T)=Ḋ0r0v(1−r0r0+vT).\boxed{D(T)=\frac{\dot D_0r_0}{v}\left(1-\frac{r_0}{r_0+vT}\right)}.

(b) Interpretation and further calculation

D(10)=12.0(1.00).100(1−1/2)=60.0μGy.\boxed{D(10)=\frac{12.0(1.00)}{.100}(1-1/2)=60.0\,\mu\mathrm{Gy}}.Dfixed=Ḋ0T=120μGy,D/Dfixed=.500.\boxed{D_{\mathrm{fixed}}=\dot D_0T=120\,\mu\mathrm{Gy},\quad D/D_{\mathrm{fixed}}=.500}.

Physical check

The point-source model applies when detector and source dimensions are small relative to their separation. The time average of an inverse-square rate is not generally its value at the mean distance.