2020
DOI: 10.1088/1361-6498/ab6aaf
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Gamma radiation shielding properties of some Bi-Sn-Zn alloys

Abstract: We investigate the gamma radiation shielding properties of some Bi-Sn-Zn alloys. For this study, we synthesised five bismuth-based lead-free alloy samples using the melt quench technique with the composition Bi50Sn Zn where Apart from physical parameters such as the weight, density, and thickness of the alloy samples, we estimated their optimum thickness range at photon energies of 122, 511, 662, and 1250 keV. The mass attenuation coefficients and effective atomic number, measured experimentally, were found… Show more

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Cited by 33 publications
(7 citation statements)
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“…Researchers have investigated various radiation shielding materials to protect life and its surroundings from debasing consequences that occurred from radiation exposure under attenuation or absorption of unwanted radiations (Singh et al 2014a, b;Al-Buriahi et al 2020;Levet et al 2020;More et al 2020a, b;Rani et al 2020). Weight, space, cost, and attenuation or absorption capabilities of the materials used for radiological protection are key points that defy researchers to synthesize and develop appropriate shielding materials.…”
Section: Introductionmentioning
confidence: 99%
“…Researchers have investigated various radiation shielding materials to protect life and its surroundings from debasing consequences that occurred from radiation exposure under attenuation or absorption of unwanted radiations (Singh et al 2014a, b;Al-Buriahi et al 2020;Levet et al 2020;More et al 2020a, b;Rani et al 2020). Weight, space, cost, and attenuation or absorption capabilities of the materials used for radiological protection are key points that defy researchers to synthesize and develop appropriate shielding materials.…”
Section: Introductionmentioning
confidence: 99%
“…For gamma ray attenuation experiment, a fine beam geometry setup has been established to perform a gamma transmission experiment. Considerations regarding material thickness and beam width during the preparation of the experiment setup can be found in [12][13][14][15]. Figure 1 shows the experiment setup including the source house, prepared sample, shielded detector, and electronic equipment.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…At a fixed photon energy, Z eff of the prepared samples with the atomic numbers of Z 1 and Z 2 , provided by ANS data sheet [30], were inserted into equation (9) to calculate the GP fitting parameters (b, c, a, X k , and d) of samples P1, P2, and P3, as shown in tables (4-6), respectively. The GP fitting parameters of prepared samples were inserted into equation (12) to calculate the photon dose multiplicative factor K. The K values were introduced into equation (10) to calculate EBF of prepared samples in the energy range of 0.03-15.0 MeV and up to penetration depth of 40 MFP.…”
Section: Exposure Build Up Factormentioning
confidence: 99%
“…The melting point is relatively low and processing is easier. Second, in the case of shielding materials, the higher the atomic density, the better the shielding ability, but in the case of blended filament, the atomic density is high [ 18 ] Third, the price of pure metal 3D printer and the pure metal filament is high, and the price competitiveness of products is reduced. For this reason, metal-blended filament is used in various industries.…”
Section: Introductionmentioning
confidence: 99%