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  1. As shown in the discussion of the attenuation of beta and alpha particles, the mass attenuation coefficient is used to partially remove the dependence on different atomic compositions and densities, and provides in an unified measure of photon attenuation amongst various materials. Linear Attenuation Coefficients.

  2. Linear Attenuation Coefficients. Monochromatic photons are attenuated exponentially in a uniform target. The number of photons in a pencil beam interact within a small distance dx is. dN = -μ Ndx. where μ is the linear attenuation coefficient and the solution to the above differential equation is.

  3. Attenuation Coefficients Linear attenuation coefficient µ: The probability of an interaction per unit distance traveled. µ has the dimensions of inverse length (eg. cm-1). N =N e−µx 0 The coefficient µ depends on photon energy and on the material being traversed. Radiation Interactions: photons Page 9 of 13

  4. Linear Attenuation Coefficients. Table of Linear Attenuation Coefficients (in cm-1) for different materials at photon energies of 100, 200, and 500 keV.

  5. The Linear Attenuation Coefficient for Air is the product of the Mass-Attentuation Coefficient of Air and the density of Air. The density of air is 0.001293 g/cm 3

  6. Linear Attenuation CoefficientsTables. Table of Linear Attenuation Coefficients (in cm-1) for different materials at gamma-ray energies of 100, 200, and 500 keV.

  7. The linear attenuation coefficient, attenuation coefficient, or narrow-beam attenuation coefficient characterizes how easily a volume of material can be penetrated by a beam of light, sound, particles, or other energy or matter. [1]

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