Measuring Radiation Dosage — Question 10

Section 42-7 · Physics pages 7130–7131

Question 10 Calorimetry measures dose through a very small temperature rise An insulated absorber has specific heat c = 4000 J/(kg K) and undergoes radiation-induced temperature rise ∆T = .250 µK. Assume all deposited energy becomes heat, with no heat loss. Independent relative standard uncertainties are 1.00 percent in c and 4.00 percent in temperature rise. c, ∆T insulated absorber Schematic; labels, not drawing lengths, specify the data. (a) Derive and calculate absorbed dose without needing the absorber mass. (b) Find the relative and absolute standard uncertainties in dose.
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Question 10 - Solution Calorimetry measures dose through a very small temperature rise c, ∆T insulated absorber (a) Method and calculation E = mc∆T, D = E/m ⇒D = c∆T . D = 4000(.250 × 10−6) = .00100 Gy = 1.00 mGy . (b) Interpretation and further calculation σD D = √ (.0100)2 + (.0400)2 = .04123 . σD = .04123 mGy . Physical check The mass cancels because heat capacity and absorbed dose use the same material mass. Heat losses or chemical energy storage would require additional corrections.

Question 10

Calorimetry measures dose through a very small temperature rise

An insulated absorber has specific heat c=4000J/(kgK)c=4000\,\mathrm{J/(kg\,K)} and undergoes radiation-induced temperature rise ΔT=.250μK\Delta T=.250\,\mu\mathrm K. Assume all deposited energy becomes heat, with no heat loss. Independent relative standard uncertainties are 1.00 percent in c and 4.00 percent in temperature rise.

Diagram shown in the original SVG worksheet.

  1. Derive and calculate absorbed dose without needing the absorber mass.

  2. Find the relative and absolute standard uncertainties in dose.

Question 10 - Solution

Calorimetry measures dose through a very small temperature rise

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E=mcΔT,D=E/m⇒D=cΔT.E=mc\Delta T,\quad D=E/m\Rightarrow\boxed{D=c\Delta T}.D=4000(.250×10−6)=.00100Gy=1.00mGy.\boxed{D=4000(.250\times10^{-6})=.00100\,\mathrm{Gy}=1.00\,\mathrm{mGy}}.

(b) Interpretation and further calculation

σDD=(.0100)2+(.0400)2=.04123.\boxed{\frac{\sigma_D}{D}=\sqrt{(.0100)^2+(.0400)^2}=.04123}.σD=.04123mGy.\boxed{\sigma_D=.04123\,\mathrm{mGy}}.

Physical check

The mass cancels because heat capacity and absorbed dose use the same material mass. Heat losses or chemical energy storage would require additional corrections.