In gamma shielding, attenuation with thickness is described by which relation?

Study for the ISPH Nuclear Energy Test. Boost your knowledge with flashcards and multiple-choice questions that include hints and explanations. Prepare efficiently for your examination!

Multiple Choice

In gamma shielding, attenuation with thickness is described by which relation?

Explanation:
Attenuation of gamma rays through shielding is exponential with thickness, governed by the linear attenuation coefficient μ. The transmitted intensity is I = I0 exp(-μ x). Here μ depends on the material (through its density and composition) and on the photon energy. A denser, high‑Z material increases μ and thus strengthens shielding, while higher photon energy generally reduces μ, making attenuation less for the same thickness. So the best description is an exponential decrease with thickness that depends on material properties and energy. The other statements are not correct: attenuation is not linear with thickness, it does depend on energy, and it does not simply increase with photon energy.

Attenuation of gamma rays through shielding is exponential with thickness, governed by the linear attenuation coefficient μ. The transmitted intensity is I = I0 exp(-μ x). Here μ depends on the material (through its density and composition) and on the photon energy. A denser, high‑Z material increases μ and thus strengthens shielding, while higher photon energy generally reduces μ, making attenuation less for the same thickness. So the best description is an exponential decrease with thickness that depends on material properties and energy. The other statements are not correct: attenuation is not linear with thickness, it does depend on energy, and it does not simply increase with photon energy.

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