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Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems

The gamma-ray shielding features of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) glass systems were experimentally reported. The mass attenuation coefficient (MAC) for the fabricated glasses was experimentally measured at seven energy values (between 0.0595 and 1.33 MeV). The compatibility between the practi...

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Autores principales: Aloraini, Dalal Abdullah, Almuqrin, Aljawhara H., Sayyed, M. I., Al-Ghamdi, Hanan, Kumar, Ashok, Elsafi, M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8433772/
https://www.ncbi.nlm.nih.gov/pubmed/34501151
http://dx.doi.org/10.3390/ma14175061
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author Aloraini, Dalal Abdullah
Almuqrin, Aljawhara H.
Sayyed, M. I.
Al-Ghamdi, Hanan
Kumar, Ashok
Elsafi, M.
author_facet Aloraini, Dalal Abdullah
Almuqrin, Aljawhara H.
Sayyed, M. I.
Al-Ghamdi, Hanan
Kumar, Ashok
Elsafi, M.
author_sort Aloraini, Dalal Abdullah
collection PubMed
description The gamma-ray shielding features of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) glass systems were experimentally reported. The mass attenuation coefficient (MAC) for the fabricated glasses was experimentally measured at seven energy values (between 0.0595 and 1.33 MeV). The compatibility between the practical and theoretical results shows the accuracy of the results obtained in the laboratory for determining the MAC of the prepared samples. The mass and linear attenuation coefficients (MACs) increase with the addition of Bi(2)O(3) and A4 glass possesses the highest MAC and LAC. A downward trend in the linear attenuation coefficient (LAC) with increasing the energy from 0.0595 to 1.33 MeV is found. The highest LAC is found at 1.33 MeV (in the range of 0.092–0.143 cm(−1)). The effective atomic number (Z(eff)) follows the order B1 > A1 > A2 > A3 > A4. This order emphasizes that increasing the content of Bi(2)O(3) has a positive effect on the photon shielding proficiencies owing to the higher density of Bi(2)O(3) compared with Na(2)O. The half value layer (HVL) is also determined and the HVL for the tested glasses is computed between 0.106 and 0.958 cm at 0.0595 MeV. The glass with 10 mol% of Bi(2)O(3) has lower HVL than the glasses with 0, 2.5, 5, and 7.5 mol% of Bi(2)O(3). So, the A4 glass needs a smaller thickness than the other glasses to shield the same radiation. As a result of the reported shielding parameters, inserting B(2)O(3) provides lower values of these three parameters, which in turn leads to the development of superior photons shields.
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spelling pubmed-84337722021-09-12 Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems Aloraini, Dalal Abdullah Almuqrin, Aljawhara H. Sayyed, M. I. Al-Ghamdi, Hanan Kumar, Ashok Elsafi, M. Materials (Basel) Article The gamma-ray shielding features of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) glass systems were experimentally reported. The mass attenuation coefficient (MAC) for the fabricated glasses was experimentally measured at seven energy values (between 0.0595 and 1.33 MeV). The compatibility between the practical and theoretical results shows the accuracy of the results obtained in the laboratory for determining the MAC of the prepared samples. The mass and linear attenuation coefficients (MACs) increase with the addition of Bi(2)O(3) and A4 glass possesses the highest MAC and LAC. A downward trend in the linear attenuation coefficient (LAC) with increasing the energy from 0.0595 to 1.33 MeV is found. The highest LAC is found at 1.33 MeV (in the range of 0.092–0.143 cm(−1)). The effective atomic number (Z(eff)) follows the order B1 > A1 > A2 > A3 > A4. This order emphasizes that increasing the content of Bi(2)O(3) has a positive effect on the photon shielding proficiencies owing to the higher density of Bi(2)O(3) compared with Na(2)O. The half value layer (HVL) is also determined and the HVL for the tested glasses is computed between 0.106 and 0.958 cm at 0.0595 MeV. The glass with 10 mol% of Bi(2)O(3) has lower HVL than the glasses with 0, 2.5, 5, and 7.5 mol% of Bi(2)O(3). So, the A4 glass needs a smaller thickness than the other glasses to shield the same radiation. As a result of the reported shielding parameters, inserting B(2)O(3) provides lower values of these three parameters, which in turn leads to the development of superior photons shields. MDPI 2021-09-03 /pmc/articles/PMC8433772/ /pubmed/34501151 http://dx.doi.org/10.3390/ma14175061 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Aloraini, Dalal Abdullah
Almuqrin, Aljawhara H.
Sayyed, M. I.
Al-Ghamdi, Hanan
Kumar, Ashok
Elsafi, M.
Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title_full Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title_fullStr Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title_full_unstemmed Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title_short Experimental Investigation of Radiation Shielding Competence of Bi(2)O(3)-CaO-K(2)O-Na(2)O-P(2)O(5) Glass Systems
title_sort experimental investigation of radiation shielding competence of bi(2)o(3)-cao-k(2)o-na(2)o-p(2)o(5) glass systems
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8433772/
https://www.ncbi.nlm.nih.gov/pubmed/34501151
http://dx.doi.org/10.3390/ma14175061
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