Investigation of gamma radiation shielding properties of polyethylene glycol in the energy range from 8.67 to 23.19 keV
| Autor: | M.W. Marashdeh, M. AlAqeel, H. Akhdar |
|---|---|
| Rok vydání: | 2022 |
| Předmět: |
Range (particle radiation)
Low energy Materials science Photon Attenuation TK9001-9401 Analytical chemistry Geant4 Polyethylene glycol Radiation Photon energy Half value layer Effective atomic numbers chemistry.chemical_compound Nuclear Energy and Engineering chemistry PEG ratio Nuclear engineering. Atomic power Mass attenuation coefficient Atomic number Polyethylene glycol (PEG) |
| Zdroj: | Nuclear Engineering and Technology, Vol 54, Iss 2, Pp 701-708 (2022) |
| ISSN: | 1738-5733 |
| DOI: | 10.1016/j.net.2021.08.028 |
| Popis: | The mass attenuation coefficients (μm) of polyethylene glycol (PEG) of different molecular weights (1000–200,000) were measured using single-beam photon transmission. The X-ray fluorescent (XRF) photons from Zinc (Zn), Zirconium (Zr), Molybdenum (Mo), Silver (Ag) and Cadmium (Cd) targets were used to determine the attenuation of gamma radiation of energy range between 8.67 and 23.19 keV in PEG samples. The results were compared to theoretical values using XCOM and Monte Carlo simulation using Geant4 toolkit which was developed to validate the experiment at those certain energies. The mass attenuation coefficients were then used to compute the effective atomic numbers, electron density and half value layers for the studied samples. The outcomes showed good agreement between experimental and simulated results with those calculated theoretically by XCOM within 5% deviation. The PEG 1000 sample showed slightly higher μm value compared with the other samples. The dependence of the photon energy and PEG composition on the values of μm and HVL were investigated and discussed. In addition, the values of Zeff and Neff for all PEG samples behaved similarly in the given photon energy range, and they decreased as the photon energy increased. |
| Databáze: | OpenAIRE |
| Externí odkaz: |
|