Measuring Radiation Dosage — Question 6

Section 42-7 · Physics pages 7122–7123

Question 6 Layered attenuation multiplies transmissions and adds optical thicknesses For an ideal narrow photon beam use transmission I/I0 = e−µx. It passes through 2.00 cm of material 1 with µ1 = .500 cm−1, then 5.00 cm of material 2 with µ2 = .200 cm−1. Treat the downstream detector dose rate as proportional to transmitted intensity. µ1, x1 µ2, x2 Schematic; labels, not drawing lengths, specify the data. (a) Find total transmission and dose rate if the unattenuated value is 10.0 µGy/min. (b) Find additional thickness of material 2 that would halve the transmitted intensity again.
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Question 6 - Solution Layered attenuation multiplies transmissions and adds optical thicknesses µ1, x1 µ2, x2 (a) Method and calculation I I0 = e−µ1x1e−µ2x2 = e−(µ1x1+µ2x2). I/I0 = e−2 = .1353, ˙D = 1.353 µGy/min . (b) Interpretation and further calculation e−µ2∆x = 1/2 ⇒∆x = ln 2/µ2. ∆x = .693147/.200 = 3.466 cm . Physical check This is a narrow-beam model without scattered-photon buildup or changes in spectrum. It is a calculation exercise, not a complete shielding design.

Question 6

Layered attenuation multiplies transmissions and adds optical thicknesses

For an ideal narrow photon beam use transmission I/I0=e−μxI/I_0=e^{-\mu x}. It passes through 2.00 cm of material 1 with μ1=.500cm−1\mu_1=.500\,\mathrm{cm^{-1}}, then 5.00 cm of material 2 with μ2=.200cm−1\mu_2=.200\,\mathrm{cm^{-1}}. Treat the downstream detector dose rate as proportional to transmitted intensity.

Diagram shown in the original SVG worksheet.

  1. Find total transmission and dose rate if the unattenuated value is 10.0μGy/min10.0\,\mu\mathrm{Gy/min}.

  2. Find additional thickness of material 2 that would halve the transmitted intensity again.

Question 6 - Solution

Layered attenuation multiplies transmissions and adds optical thicknesses

Diagram shown in the original SVG worksheet.

(a) Method and calculation

II0=e−μ1x1e−μ2x2=e−(μ1x1+μ2x2).\frac I{I_0}=e^{-\mu_1x_1}e^{-\mu_2x_2}=e^{-(\mu_1x_1+\mu_2x_2)}.I/I0=e−2=.1353,Ḋ=1.353μGy/min.\boxed{I/I_0=e^{-2}=.1353,\quad\dot D=1.353\,\mu\mathrm{Gy/min}}.

(b) Interpretation and further calculation

e−μ2Δx=1/2⇒Δx=ln⁡2/μ2.e^{-\mu_2\Delta x}=1/2\Rightarrow\Delta x=\ln2/\mu_2.Δx=.693147/.200=3.466cm.\boxed{\Delta x=.693147/.200=3.466\,\mathrm{cm}}.

Physical check

This is a narrow-beam model without scattered-photon buildup or changes in spectrum. It is a calculation exercise, not a complete shielding design.