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Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System
According to the Makishema–Mackenzie model assumption, the dissociation energy and packing density for a quaternary TeO(2)-As(2)O(3)-B(2)O(3)-Li(2)O glass system were evaluated. The dissociation energy rose from 67.07 to 71.85 kJ/cm(3), whereas the packing factor decreased from 16.55 to 15.21 cm(3)/...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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MDPI
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8303416/ https://www.ncbi.nlm.nih.gov/pubmed/34300979 http://dx.doi.org/10.3390/ma14144060 |
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author | Almuqrin, Aljawhara H. Hanfi, Mohamed Y. Sayyed, M. I. Mahmoud, K. G. Al-Ghamdi, Hanan Aloraini, Dalal Abdullah |
author_facet | Almuqrin, Aljawhara H. Hanfi, Mohamed Y. Sayyed, M. I. Mahmoud, K. G. Al-Ghamdi, Hanan Aloraini, Dalal Abdullah |
author_sort | Almuqrin, Aljawhara H. |
collection | PubMed |
description | According to the Makishema–Mackenzie model assumption, the dissociation energy and packing density for a quaternary TeO(2)-As(2)O(3)-B(2)O(3)-Li(2)O glass system were evaluated. The dissociation energy rose from 67.07 to 71.85 kJ/cm(3), whereas the packing factor decreased from 16.55 to 15.21 cm(3)/mol associated with the replacement of TeO(2) by LiO(2) compounds. Thus, as a result, the elastic moduli (longitudinal, shear, Young, and bulk) were enhanced by increasing the LiO(2) insertion. Based on the estimated elastic moduli, mechanical properties such as the Poisson ratio, microhardness, longitudinal velocity, shear velocity, and softening temperature were evaluated for the investigated glass samples. In order to evaluate the studied glasses’ gamma-ray shield capacity, the MCNP-5 code, as well as a theoretical Phy-X/PSD program, were applied. The best shielding capacity was achieved for the glass system containing 25 mol% of TeO(2,) while the lowest ability was obtained for the glass sample with a TeO(2) concentration of 5 mol%. Furthermore, a correlation between the studied glasses’ microhardness and linear attenuation coefficient was performed versus the LiO(2) concentration to select the glass sample which possesses a suitable mechanical and shielding capacity. |
format | Online Article Text |
id | pubmed-8303416 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-83034162021-07-25 Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System Almuqrin, Aljawhara H. Hanfi, Mohamed Y. Sayyed, M. I. Mahmoud, K. G. Al-Ghamdi, Hanan Aloraini, Dalal Abdullah Materials (Basel) Article According to the Makishema–Mackenzie model assumption, the dissociation energy and packing density for a quaternary TeO(2)-As(2)O(3)-B(2)O(3)-Li(2)O glass system were evaluated. The dissociation energy rose from 67.07 to 71.85 kJ/cm(3), whereas the packing factor decreased from 16.55 to 15.21 cm(3)/mol associated with the replacement of TeO(2) by LiO(2) compounds. Thus, as a result, the elastic moduli (longitudinal, shear, Young, and bulk) were enhanced by increasing the LiO(2) insertion. Based on the estimated elastic moduli, mechanical properties such as the Poisson ratio, microhardness, longitudinal velocity, shear velocity, and softening temperature were evaluated for the investigated glass samples. In order to evaluate the studied glasses’ gamma-ray shield capacity, the MCNP-5 code, as well as a theoretical Phy-X/PSD program, were applied. The best shielding capacity was achieved for the glass system containing 25 mol% of TeO(2,) while the lowest ability was obtained for the glass sample with a TeO(2) concentration of 5 mol%. Furthermore, a correlation between the studied glasses’ microhardness and linear attenuation coefficient was performed versus the LiO(2) concentration to select the glass sample which possesses a suitable mechanical and shielding capacity. MDPI 2021-07-20 /pmc/articles/PMC8303416/ /pubmed/34300979 http://dx.doi.org/10.3390/ma14144060 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 Almuqrin, Aljawhara H. Hanfi, Mohamed Y. Sayyed, M. I. Mahmoud, K. G. Al-Ghamdi, Hanan Aloraini, Dalal Abdullah Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title | Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title_full | Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title_fullStr | Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title_full_unstemmed | Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title_short | Influence of Li(2)O Incrementation on Mechanical and Gamma-Ray Shielding Characteristics of a TeO(2)-As(2)O(3)-B(2)O(3) Glass System |
title_sort | influence of li(2)o incrementation on mechanical and gamma-ray shielding characteristics of a teo(2)-as(2)o(3)-b(2)o(3) glass system |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8303416/ https://www.ncbi.nlm.nih.gov/pubmed/34300979 http://dx.doi.org/10.3390/ma14144060 |
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