Synthesis of barium-doped PVC/Bi2WO6 composites for X-ray radiation shielding
0
조회
0
다운로드
0
인용
0
참고문헌
키워드
초록
In this study, composites containing undoped and barium-doped Bi2WO6:Ba2þwere investigated for theirshielding against diagnostic X-ray. At first, Bi2WO6 and barium-doped Bi2WO6 were synthesized withdifferent weight percentages of barium oxide through a hydrothermal process. The as-synthesizednanostructures were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM),energy-dispersive X-ray spectroscopy (EDS) and Raman spectroscopy (RS). After that, some shields weregenerated with undoped and barium-doped Bi2WO6:Ba2þ nanostructure particles incorporated intopolyvinyl chloride (PVC) polymer with different thicknesses and 15% weight of the nanostructure. Finally,the prepared samples were exposed to an X-ray tube at 40, 80, and 120 kV voltages, 10 mAs and, 44.5 cmSID (i.e. the distance from the X-ray beam source to the specimen). Linear and mass attenuation coefficientswere also calculated for different samples. The results indicated that, among the samples, theone with 7.5 mmol barium-doped Bi2WO6 had the most attenuation at the voltage of 40kV, and theattenuation coefficients would increase with an increase in the amount of barium. The samples with 15and 17.5 mmol barium-doped Bi2WO6 had higher attenuation than the others at 80 and 120 kV. Moreover, the half-value layer (HVL), tenth-value layer (TVL) and 0.25 mm lead equivalent thicknesswere calculated for all the samples. The lowest HVL value was for the sample with 7.5 mmol bariumdopedBi2WO6. As the result clearly show, an increment in the barium-doping content leads to adecrease in both HVL and TVL. In every three voltages, 0.25 mm lead equivalent thickness of the barium-doped composites (7.5 mmoland 15 mmol) had less than the other composites. The lowest value of 0.25 mm lead equivalent thicknesswas 7.5 barium-doped in 40 kV voltage and 15 mmol barium-doped in 80 kV and 120 kV voltages. Theseresults were obtained only for 15% weight of the nanostructure.
Abstract
In this study, composites containing undoped and barium-doped Bi2WO6:Ba2þwere investigated for theirshielding against diagnostic X-ray. At first, Bi2WO6 and barium-doped Bi2WO6 were synthesized withdifferent weight percentages of barium oxide through a hydrothermal process. The as-synthesizednanostructures were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM),energy-dispersive X-ray spectroscopy (EDS) and Raman spectroscopy (RS). After that, some shields weregenerated with undoped and barium-doped Bi2WO6:Ba2þ nanostructure particles incorporated intopolyvinyl chloride (PVC) polymer with different thicknesses and 15% weight of the nanostructure. Finally,the prepared samples were exposed to an X-ray tube at 40, 80, and 120 kV voltages, 10 mAs and, 44.5 cmSID (i.e. the distance from the X-ray beam source to the specimen). Linear and mass attenuation coefficientswere also calculated for different samples. The results indicated that, among the samples, theone with 7.5 mmol barium-doped Bi2WO6 had the most attenuation at the voltage of 40kV, and theattenuation coefficients would increase with an increase in the amount of barium. The samples with 15and 17.5 mmol barium-doped Bi2WO6 had higher attenuation than the others at 80 and 120 kV. Moreover, the half-value layer (HVL), tenth-value layer (TVL) and 0.25 mm lead equivalent thicknesswere calculated for all the samples. The lowest HVL value was for the sample with 7.5 mmol bariumdopedBi2WO6. As the result clearly show, an increment in the barium-doping content leads to adecrease in both HVL and TVL. In every three voltages, 0.25 mm lead equivalent thickness of the barium-doped composites (7.5 mmoland 15 mmol) had less than the other composites. The lowest value of 0.25 mm lead equivalent thicknesswas 7.5 barium-doped in 40 kV voltage and 15 mmol barium-doped in 80 kV and 120 kV voltages. Theseresults were obtained only for 15% weight of the nanostructure.
참고문헌 (26)
- M. Mahesh, "The essential physics of medical imaging", Med. Phys, 40 (2013)[DOI]
- H. M. Soylu, "Gamma radiation shielding efficiency of a new lead-free composite material", J. Radioanal. Nucl. Chem, 305, pp.529~534 (2015)[DOI]
- J. Kim, "Nano-W dispersed gamma radiation shielding materials", Adv. Eng. Mater, 16, pp.1083~1089 (2014)[DOI]
- J. H. Liu, "Elevated gamma-rays shielding property in lead-free bismuth tungstate by nanofabricating structures", J. Phys. Chem. Solid, 112, pp.185~189 (2018)[DOI]
- H. Chai, "lead-free X-ray-shielding materials containing tungsten and bismuth(III)oxide", J. Appl. Polym. Sci, 133, pp.43012~ (2016)[DOI]
- H. Alavian, "Study on gamma shielding polymer composites reinforced with different sizes and proportions of tungsten particles using MCNP code", Prog. Nucl. Energy, 115, pp.91~98 (2019)[DOI]
- N. Asari Shik, "X-ray shielding performance of the EPVC composites with micro- or nanoparticles of WO3, PbO or Bi2O3", Appl. Radiat. Isot, 139, pp.61~65 (2018)[DOI]
- L. Gholamzadeh, "A study of the shielding performance of fibers coated with high-Z oxides against ionizing radiations", Detect. Assoc. Equip, 973, pp.164174~ (2020)[DOI]
- J. W. Hong, "Effectiveness evaluation of self-produced micro-and nanosized tungsten materials for radiation shielding with diagnostic X-ray imaging system", Optik, 172, pp.760~765 (2018)[DOI]
- H. A. Maghrabi, "Bismuth oxide-coated fabrics for Xray shielding", Textil. Res. J, 86, pp.649~658 (2016)[DOI]
- A. Erol, "Radiation shielding of polymer composite materials with wolfram carbide and boron carbide", Radiat. Protect. Environ, 39, pp.3~6 (2016)[DOI]
- S. C. Kim, "Physical analysis of the shielding capacity for a lightweight apron designed for shielding low intensity scattering X-rays", Sci. Rep, 6, pp.27721~ (2016)[DOI]
- J. Kim, "Nano-W dispersed gamma radiation shielding materials", Adv. Eng. Mater, 16, pp.1083~1089 (2014)[DOI]
- A. Barabash, "Polymer-composite materials for radiation protection", Adv. Intell. Syst. Comput, 983, pp.352~360 (2019)[DOI]
- N. Z. N. Azman, "Microstructural design of lead oxide-epoxy composites for radiation shielding purposes", J. Appl. Polym. Sci, 128, pp.3213~3219 (2013)[DOI]
- W. Poltabtim, "Properties of lead-free gamma-ray shielding materials from metal oxide", EPDM rubber composites, 2018, pp.153, 1~9
- S. Jayakumar, "Polymer nanocomposites containing b-Bi2O3 and silica nanoparticles : thermal stability, surface topography and Xray attenuation properties", J. Appl. Polym. Sci, 137, pp.49048~ (2020)[DOI]
- S. Jayakumar, "characterization and X-ray attenuation property of Gd2O3 based nanocomposites", Appl. Nanosci, 7, pp.919~931 (2017)[DOI]
- C. Zhang, "Synthesis of square Bi2WO6 nanoplates as high-Activity visible-light-driven photocatalysts", Chem. Mater, 17, pp.3537~3545 (2005)[DOI]
- Y. C. Xu, "Tailoring lattices of Bi2WO6 crystals via Ce doping to improve the shielding properties against low-energy gamma rays", J. Phys. Chem. Solid, 127, pp.76~80 (2019)[DOI]
- N. Damla, "Radiation dose estimation and mass attenuation coefficients of cement samples used in Turkey", J. Hazard Mater, 176, pp.644~649 (2010)[DOI]
- S. Atef, "Effect of gamma irradiation and lead content on the physical and shielding properties of PVC", NBR polymer blends, 2020, pp.77, 5423~5438
- R. Bagheri, "Gamma-ray shielding studies on borate glasses containing BaO, Bi2O3, and PbO in different concentrations", Radiat. Phys. Chem, 184, pp.109434~ (2021)[DOI]
- J. Kenneth Shultis, "Radiation Shielding and Radiological Protection", Handbook of Nuclear Engineering, pp.1313~1448 (2010), Springer US[DOI]
- J. K. Shultis, "Fundamentals of Nuclear Science and Engineering" (2002), CRC Press
- J. P. McCaffrey, "Optimizing non-Pb radiation shielding materials using bilayers", Med. Phys, 36, pp.5586~5594 (2009)[DOI]
