Measuring Radiation Dosage — Question 8

Section 42-7 · Physics pages 7126–7127

Question 8 Physical decay and biological removal combine into an effective half-life In a one-compartment teaching model, a retained radionuclide is removed independently by physical decay and biological clearance. Its physical half-life is 8.00 d and clearance half-life is 4.00 d. The dose rate in a fixed target is proportional to retained activity and starts at .300 mGy/d. retained N physical decay clearance Schematic; labels, not drawing lengths, specify the data. (a) Derive and calculate the effective half-life. (b) Find the integrated dose from t=0 to infinity under the stated constant-deposition model.
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Question 8 - Solution Physical decay and biological removal combine into an effective half-life retained N physical decay clearance (a) Method and calculation ˙N = −(λp + λb)N ⇒λeff= λp + λb . T −1 eff= T −1 p + T −1 b , Teff= 8/3 = 2.667 d . (b) Interpretation and further calculation D∞= ∫∞ 0 ˙D0e−λefftdt = ˙D0/λeff. D∞= .300(8/3)/ ln 2 = 1.154 mGy . Physical check Clearance removes undecayed nuclei from the modeled compartment; it is not itself radioactive decay. Real internal dosimetry may require multiple compartments and time-dependent deposition.

Question 8

Physical decay and biological removal combine into an effective half-life

In a one-compartment teaching model, a retained radionuclide is removed independently by physical decay and biological clearance. Its physical half-life is 8.00 d and clearance half-life is 4.00 d. The dose rate in a fixed target is proportional to retained activity and starts at .300 mGy/d.

Diagram shown in the original SVG worksheet.

  1. Derive and calculate the effective half-life.

  2. Find the integrated dose from t=0 to infinity under the stated constant-deposition model.

Question 8 - Solution

Physical decay and biological removal combine into an effective half-life

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ṅ=−(λp+λb)N⇒λeff=λp+λb.\dot N=-(\lambda_p+\lambda_b)N\Rightarrow\boxed{\lambda_{\mathrm{eff}}=\lambda_p+\lambda_b}.Teff−1=Tp−1+Tb−1,Teff=8/3=2.667d.\boxed{T_{\mathrm{eff}}^{-1}=T_p^{-1}+T_b^{-1},\quad T_{\mathrm{eff}}=8/3=2.667\,\mathrm d}.

(b) Interpretation and further calculation

D∞=∫0∞Ḋ0e−λefftdt=Ḋ0/λeff.D_{\infty}=\int_0^\infty\dot D_0e^{-\lambda_{\mathrm{eff}}t}dt=\dot D_0/\lambda_{\mathrm{eff}}.D∞=.300(8/3)/ln⁡2=1.154mGy.\boxed{D_{\infty}=.300(8/3)/\ln2=1.154\,\mathrm{mGy}}.

Physical check

Clearance removes undecayed nuclei from the modeled compartment; it is not itself radioactive decay. Real internal dosimetry may require multiple compartments and time-dependent deposition.