A narrow, monoenergetic photon beam of intensity travels along the -direction through…

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Radiation interactions, detection and dosimetry · Radiation interactions, detection and dosimetry

Life at Thermal Energy, Ch Radiation in tissue: interaction, dose and risk

Problem

A narrow, monoenergetic photon beam of intensity II travels along the xx-direction through a uniform absorbing medium. In each thin layer of thickness dx\mathrm{d}x, a photon already in the beam has a constant probability μ dx\mu\,\mathrm{d}x of being removed from the beam (by absorption or by scattering out of it), independent of how far it has already travelled; μ\mu is the linear attenuation coefficient of the medium, in cm−1\mathrm{cm^{-1}}. ((a)) Starting from the removal probability per layer, write down the differential equation obeyed by I(x)I(x) and solve it for I(x)I(x) in terms of I0=I(0)I_0=I(0), μ\mu and xx. ((b)) Define the half-value layer HVL\mathrm{HVL} as the thickness that halves the beam and express it in terms of μ\mu. ((c)) Water at 60 keV60\,\mathrm{keV} has μ/ρ=0.206 cm2 g−1\mu/\rho = 0.206\,\mathrm{cm^2\,g^{-1}} and density ρ=1.00 g cm−3\rho = 1.00\,\mathrm{g\,cm^{-3}}. Compute HVL\mathrm{HVL} for water at this energy.

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