Feasibility of clay-shielding material for low-energy photons (Gamma/X)

While considering the photon attenuation coefficient (μ) and its related parameters for photons shielding, it is necessary to account for its transmitted and reflected photons energy spectra and dose contribution. Monte Carlo simulation was used to study the efficiency of clay (1.99 g cm−3) as a shi...

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Bibliographic Details
Main Authors: S.M. Tajudin, A.H.A. Sabri, M.Z. Abdul Aziz, S.F. Olukotun, B.M. Ojo, M.K. Fasasi
Format: Article
Language:English
Published: Elsevier 2019-09-01
Series:Nuclear Engineering and Technology
Online Access:http://www.sciencedirect.com/science/article/pii/S1738573319301809
Description
Summary:While considering the photon attenuation coefficient (μ) and its related parameters for photons shielding, it is necessary to account for its transmitted and reflected photons energy spectra and dose contribution. Monte Carlo simulation was used to study the efficiency of clay (1.99 g cm−3) as a shielding material below 150 keV photon. Am-241 gamma source and an X-ray of 150 kVp were calculated. The calculated value of μ for Am-241 is higher within 5.61% compared to theoretical value for a single-energy photon. The calculated half-value layer (HVL) is 0.9335 cm, which is lower than that of ordinary concrete for X-ray of 150 kVp. A thickness of 2 cm clay was adequate to attenuate 90% and 85% of the incident photons from Am-241 and X-ray of 150 kVp, respectively. The same thickness of 2 cm could shield the gamma source dose rate of Am-241 (1 MBq) down to 0.0528 μSv/hr. For X-ray of 150 kVp, photons below 60 keV were significantly decreased with 2 cm clay and a dose rate reduction by ∼80%. The contribution of reflected photons and dose from the clay is negligible for both sources. Keywords: Monte Carlo, Attenuation, Gamma source, X-ray, Photon spectra, Dose rate
ISSN:1738-5733