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. 2021 Jul 13;14(14):3897.
doi: 10.3390/ma14143897.

Newly Developed Vanadium-Based Glasses and Their Potential for Nuclear Radiation Shielding Aims: A Monte Carlo Study on Gamma Ray Attenuation Parameters

Affiliations

Newly Developed Vanadium-Based Glasses and Their Potential for Nuclear Radiation Shielding Aims: A Monte Carlo Study on Gamma Ray Attenuation Parameters

Huseyin Ozan Tekin et al. Materials (Basel). .

Abstract

This study aimed to investigate different types of glasses based on the 46V2O5-46P2O5-(8-x) B2O3-xCuO system in terms of their nuclear radiation shielding properties. Accordingly, five different CuO-doped vanadate glasses were investigated extensively to determine the necessary gamma shielding parameters along with effective conductivity at 300,000 and buildup factors. Phy-x PSD software was used for determination of these vital parameters. Furthermore, these parameters, such as half value layer, tenth value layer, and mean free path were investigated in a broad energy range between 0.015 and 15 MeV. The results revealed that the amount of CuO reinforced in each sample plays an essential role in determination of the shielding abilities of the samples. The sample with the highest CuO content had the highest linear attenuation coefficient and mass attenuation coefficient values. Additionally, the lowest mean free path, half value layer, and tenth value layer values were recorded for glass sample VPCu8. There was an inverse relation between the effective conductivity and effective atomic number and photon energy; that is, as energy increases, the effective conductivity and effective atomic number decreased rapidly, especially in the regions of low energy. Glass sample VPCu8 reported the highest values for both parameters. Moreover, glass sample VPCu8 had the lowest exposure buildup factor and energy absorption buildup factor values. Our findings showed that CuO-reinforced vanadate glass composition, namely 46V2O5-46P2O5-8CuO, with a glass density of 2.9235 g/cm3, was reported to have superior gamma ray attenuation properties. These results would be helpful for scientists in determining the most appropriate additive rare earth type, as well as the most appropriate glass composition, to offer shielding characteristics similar to those described above, taking into consideration the criteria for usage and the needs of the community. The results of this research will be useful to the scientific community in evaluating the prospective characteristics of CuO-doped glass systems and related glass compositions. CuO-doped glass systems and associated glass compositions have a wide range of properties.

Keywords: CuO-doped; Phy-x PSD; radiation shielding; vanadate glasses.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
Physical appearances of Cu-doped VPBxCuy glasses along with their codes.
Figure 2
Figure 2
2-D view and dimensions of designed MCNPX simulation setup for gamma ray transmission competencies of VPBxCuy glasses (obtained from MCNPX Visual Editor VE VisedX22S).
Figure 3
Figure 3
3-D view of designed MCNPX simulation setup for gamma ray transmission competencies of VPBxCuy glasses (obtained from MCNPX Visual Editor VE VisedX22S).
Figure 4
Figure 4
Variation of linear attenuation coefficient (μ) against photon energy for VPBxCuy glass samples.
Figure 5
Figure 5
Variation of mass attenuation coefficient (μm) against photon energy for VPBxCuy glass samples.
Figure 6
Figure 6
Variation of mass attenuation coefficients as a function of increasing CuO reinforcement.
Figure 7
Figure 7
Variation of half value layer (T1/2) against photon energy for VPBxCuy glass samples.
Figure 8
Figure 8
Variation of tenth value layer (T1/10) against photon energy for VPBxCuy glass samples.
Figure 9
Figure 9
Variation of mean free path (λ) against photon energy for VPBxCuy glass samples.
Figure 10
Figure 10
Variation of effective atomic number (Zeff) against photon energy for VPBxCuy glass samples.
Figure 11
Figure 11
Variation of (a) EBF and (b) EABF against photon energy for sample VPB8.
Figure 12
Figure 12
Variation of (a) EBF and (b) EABF against photon energy for sample VPB6Cu2.
Figure 13
Figure 13
Variation of (a) EBF and (b) EABF against photon energy for sample VPB4Cu4.
Figure 14
Figure 14
Variation of (a) EBF and (b) EABF against photon energy for sample VPB2Cu6.
Figure 15
Figure 15
Variation of (a) EBF and (b) EABF against photon energy for sample VPCu8.
Figure 16
Figure 16
Variation of effective conductivity (Ceff) at 300K (s/m) for VPBxCuy glass samples.

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