Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach

The mechanical and radiation shielding properties for the PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> glass system were theoretically investigated in this paper. The PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<su...

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Main Authors: Aljawhara H. Almuqrin, M. I. Sayyed, Badriah Albarzan, Abigaile Mia V. Javier-Hila, Norah Alwadai, Ashok Kumar
Format: Article
Language:English
Published: MDPI AG 2021-06-01
Series:Applied Sciences
Subjects:
keV
Online Access:https://www.mdpi.com/2076-3417/11/12/5538
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spelling doaj-4925d94d11cb42f1828ae07f915652122021-07-01T00:15:28ZengMDPI AGApplied Sciences2076-34172021-06-01115538553810.3390/app11125538Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical ApproachAljawhara H. Almuqrin0M. I. Sayyed1Badriah Albarzan2Abigaile Mia V. Javier-Hila3Norah Alwadai4Ashok Kumar5Department of Physics, College of Science, Princess Nourah bint Abdulrahman University, Riyadh 11671, Saudi ArabiaDepartment of Nuclear Medicine Research, Institute for Research and Medical Consultations (IRMC), Imam Abdulrahman bin Faisal University (IAU), P.O. Box 1982, Dammam 31441, Saudi ArabiaDepartment of Physics, College of Science, Princess Nourah bint Abdulrahman University, Riyadh 11671, Saudi ArabiaDepartment of Science and Technology, Philippine Nuclear Research Institute (DOST-PNRI), Commonwealth Avenue, Diliman, Quezon City 1101, PhilippinesDepartment of Physics, College of Science, Princess Nourah bint Abdulrahman University, Riyadh 11671, Saudi ArabiaDepartment of Physics, University College, Benra-Dhuri 148024, IndiaThe mechanical and radiation shielding properties for the PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> glass system were theoretically investigated in this paper. The PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> glass system (coded as investigated glasses) was fabricated using the melt quenching mechanism. The optical packing density (OPD) increases from 75.563 to 84.366, and oxygen molar volume (OMV) decreases from 13.234 to 11.853 cm<sup>3</sup>/mol when increasing the PbO concentration. The values of elastic moduli decreased from 47.06 to 39.67 GPa for Young, from 33.51 to 32.41 GPa for bulk, from 19.82 to 16.29 GPa for shear and from 59.94 to 54.14 GPa for longitudinal moduli as the PbO is increased. The radiation attenuation characteristics were reported at the photon energies used in diagnostic radiology. The mass attenuation coefficient (MAC) was evaluated using the three photoatomic data libraries EPICS2017, EPDL97, and XCOM, available in the EpiXS and Phy-X programs. The MAC for the five investigated glasses at 20 keV was much higher than the MAC at 40, 60 and 80 keV. The MAC for investigated glasses increased with the addition of PbO, with Pb-S1 demonstrating the lowest MAC, and Pb-S5 demonstrating the highest MAC. Additionally, the rate of the increment of MAC at 20 keV as the concentration of PbO increased was higher than that at 40, 60 and 80 keV. The effective atomic number (EAN) was determined using Phy-X program. The EAN follows the trend: Pb-S5 > Pb-S4 > Pb-S3 > Pb-S2 > Pb-S1. The EAN results proved that the glass with low amounts of B<sub>2</sub>O<sub>3</sub> and higher amounts of PbO had good attenuation features. The EAN had the maximum values of 73.55–76.67 at 20 keV, whereas the lowest values occurred at 80 keV and varied between 53.63 and 63.39. The half-value layer (HVL) results showed that the Pb-S1 glass had the greatest HVL, while Pb-S5 had the least. There is a higher discrepancy between the tenth-value layer values at 80 keV than at 20 keV. At 20 keV, the difference between the highest and lowest TVL values (Pb-S1 and Pb-S5) was only 0.004 cm, while the difference at 80 keV was 0.152 cm. Pb-S5 is the most space-efficient radiation shield.https://www.mdpi.com/2076-3417/11/12/5538diagnostic radiologykeVglassesradiation attenuation propertiesmechanical properties
collection DOAJ
language English
format Article
sources DOAJ
author Aljawhara H. Almuqrin
M. I. Sayyed
Badriah Albarzan
Abigaile Mia V. Javier-Hila
Norah Alwadai
Ashok Kumar
spellingShingle Aljawhara H. Almuqrin
M. I. Sayyed
Badriah Albarzan
Abigaile Mia V. Javier-Hila
Norah Alwadai
Ashok Kumar
Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
Applied Sciences
diagnostic radiology
keV
glasses
radiation attenuation properties
mechanical properties
author_facet Aljawhara H. Almuqrin
M. I. Sayyed
Badriah Albarzan
Abigaile Mia V. Javier-Hila
Norah Alwadai
Ashok Kumar
author_sort Aljawhara H. Almuqrin
title Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
title_short Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
title_full Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
title_fullStr Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
title_full_unstemmed Mechanical and Gamma-Ray Interaction Studies of PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> Glass System for Shielding Applications in The Low Energy Region: A Theoretical Approach
title_sort mechanical and gamma-ray interaction studies of pbo–moo<sub>3</sub>–li<sub>2</sub>o–b<sub>2</sub>o<sub>3</sub> glass system for shielding applications in the low energy region: a theoretical approach
publisher MDPI AG
series Applied Sciences
issn 2076-3417
publishDate 2021-06-01
description The mechanical and radiation shielding properties for the PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> glass system were theoretically investigated in this paper. The PbO–MoO<sub>3</sub>–Li<sub>2</sub>O–B<sub>2</sub>O<sub>3</sub> glass system (coded as investigated glasses) was fabricated using the melt quenching mechanism. The optical packing density (OPD) increases from 75.563 to 84.366, and oxygen molar volume (OMV) decreases from 13.234 to 11.853 cm<sup>3</sup>/mol when increasing the PbO concentration. The values of elastic moduli decreased from 47.06 to 39.67 GPa for Young, from 33.51 to 32.41 GPa for bulk, from 19.82 to 16.29 GPa for shear and from 59.94 to 54.14 GPa for longitudinal moduli as the PbO is increased. The radiation attenuation characteristics were reported at the photon energies used in diagnostic radiology. The mass attenuation coefficient (MAC) was evaluated using the three photoatomic data libraries EPICS2017, EPDL97, and XCOM, available in the EpiXS and Phy-X programs. The MAC for the five investigated glasses at 20 keV was much higher than the MAC at 40, 60 and 80 keV. The MAC for investigated glasses increased with the addition of PbO, with Pb-S1 demonstrating the lowest MAC, and Pb-S5 demonstrating the highest MAC. Additionally, the rate of the increment of MAC at 20 keV as the concentration of PbO increased was higher than that at 40, 60 and 80 keV. The effective atomic number (EAN) was determined using Phy-X program. The EAN follows the trend: Pb-S5 > Pb-S4 > Pb-S3 > Pb-S2 > Pb-S1. The EAN results proved that the glass with low amounts of B<sub>2</sub>O<sub>3</sub> and higher amounts of PbO had good attenuation features. The EAN had the maximum values of 73.55–76.67 at 20 keV, whereas the lowest values occurred at 80 keV and varied between 53.63 and 63.39. The half-value layer (HVL) results showed that the Pb-S1 glass had the greatest HVL, while Pb-S5 had the least. There is a higher discrepancy between the tenth-value layer values at 80 keV than at 20 keV. At 20 keV, the difference between the highest and lowest TVL values (Pb-S1 and Pb-S5) was only 0.004 cm, while the difference at 80 keV was 0.152 cm. Pb-S5 is the most space-efficient radiation shield.
topic diagnostic radiology
keV
glasses
radiation attenuation properties
mechanical properties
url https://www.mdpi.com/2076-3417/11/12/5538
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