Cargando…

The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources

The role La(2)O(3) on the radiation shielding properties of La(2)O(3)-CaO-B(2)O(3)-SiO(2) glass systems was investigated. The energies were selected between 0.284 and 1.275 MeV and Phy-X software was used for the calculations. BLa10 glass had the least linear attenuation coefficient (LAC) at all the...

Descripción completa

Detalles Bibliográficos
Autores principales: Al-Ghamdi, Hanan, Dong, Mengge, Sayyed, M. I., Wang, Chao, Almuqrin, Aljawhara H., Almasoud, Fahad I.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8432568/
https://www.ncbi.nlm.nih.gov/pubmed/34500865
http://dx.doi.org/10.3390/ma14174776
_version_ 1783751193778978816
author Al-Ghamdi, Hanan
Dong, Mengge
Sayyed, M. I.
Wang, Chao
Almuqrin, Aljawhara H.
Almasoud, Fahad I.
author_facet Al-Ghamdi, Hanan
Dong, Mengge
Sayyed, M. I.
Wang, Chao
Almuqrin, Aljawhara H.
Almasoud, Fahad I.
author_sort Al-Ghamdi, Hanan
collection PubMed
description The role La(2)O(3) on the radiation shielding properties of La(2)O(3)-CaO-B(2)O(3)-SiO(2) glass systems was investigated. The energies were selected between 0.284 and 1.275 MeV and Phy-X software was used for the calculations. BLa10 glass had the least linear attenuation coefficient (LAC) at all the tested energies, while BLa30 had the greatest, which indicated that increasing the content of La(2)O(3) in the BLa-X glasses enhances the shielding performance of these glasses. The mass attenuation coefficient (MAC) of BLa15 decreases from 0.150 cm(2)/g to 0.054 cm(2)/g at energies of 0.284 MeV and 1.275 MeV, respectively, while the MAC of BLa25 decreases from 0.164 cm(2)/g to 0.053 cm(2)/g for the same energies, respectively. At all energies, the effective atomic number (Z(eff)) values follow the trend BLa10 < BLa15 < BLa20 < BLa25 < BLa30. The half value thickness (HVL) of the BLa-X glass shields were also investigated. The minimum HVL values are found at 0.284 MeV. The HVL results demonstrated that BLa30 is the most space-efficient shield. The tenth value layer (TVL) results demonstrated that the glasses are more effective attenuators at lower energies, while decreasing in ability at greater energies. These mean free path results proved that increasing the density of the glasses, by increasing the amount of La(2)O(3) content, lowers MFP, and increases attenuation, which means that BLa30, the glass with the greatest density, absorbs the most amount of radiation.
format Online
Article
Text
id pubmed-8432568
institution National Center for Biotechnology Information
language English
publishDate 2021
publisher MDPI
record_format MEDLINE/PubMed
spelling pubmed-84325682021-09-11 The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources Al-Ghamdi, Hanan Dong, Mengge Sayyed, M. I. Wang, Chao Almuqrin, Aljawhara H. Almasoud, Fahad I. Materials (Basel) Article The role La(2)O(3) on the radiation shielding properties of La(2)O(3)-CaO-B(2)O(3)-SiO(2) glass systems was investigated. The energies were selected between 0.284 and 1.275 MeV and Phy-X software was used for the calculations. BLa10 glass had the least linear attenuation coefficient (LAC) at all the tested energies, while BLa30 had the greatest, which indicated that increasing the content of La(2)O(3) in the BLa-X glasses enhances the shielding performance of these glasses. The mass attenuation coefficient (MAC) of BLa15 decreases from 0.150 cm(2)/g to 0.054 cm(2)/g at energies of 0.284 MeV and 1.275 MeV, respectively, while the MAC of BLa25 decreases from 0.164 cm(2)/g to 0.053 cm(2)/g for the same energies, respectively. At all energies, the effective atomic number (Z(eff)) values follow the trend BLa10 < BLa15 < BLa20 < BLa25 < BLa30. The half value thickness (HVL) of the BLa-X glass shields were also investigated. The minimum HVL values are found at 0.284 MeV. The HVL results demonstrated that BLa30 is the most space-efficient shield. The tenth value layer (TVL) results demonstrated that the glasses are more effective attenuators at lower energies, while decreasing in ability at greater energies. These mean free path results proved that increasing the density of the glasses, by increasing the amount of La(2)O(3) content, lowers MFP, and increases attenuation, which means that BLa30, the glass with the greatest density, absorbs the most amount of radiation. MDPI 2021-08-24 /pmc/articles/PMC8432568/ /pubmed/34500865 http://dx.doi.org/10.3390/ma14174776 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
Al-Ghamdi, Hanan
Dong, Mengge
Sayyed, M. I.
Wang, Chao
Almuqrin, Aljawhara H.
Almasoud, Fahad I.
The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title_full The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title_fullStr The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title_full_unstemmed The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title_short The Vital Role of La(2)O(3) on the La(2)O(3)-CaO-B(2)O(3)-SiO(2) Glass System for Shielding Some Common Gamma Ray Radioactive Sources
title_sort vital role of la(2)o(3) on the la(2)o(3)-cao-b(2)o(3)-sio(2) glass system for shielding some common gamma ray radioactive sources
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8432568/
https://www.ncbi.nlm.nih.gov/pubmed/34500865
http://dx.doi.org/10.3390/ma14174776
work_keys_str_mv AT alghamdihanan thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT dongmengge thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT sayyedmi thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT wangchao thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT almuqrinaljawharah thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT almasoudfahadi thevitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT alghamdihanan vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT dongmengge vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT sayyedmi vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT wangchao vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT almuqrinaljawharah vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources
AT almasoudfahadi vitalroleofla2o3onthela2o3caob2o3sio2glasssystemforshieldingsomecommongammarayradioactivesources