Neutron and optical properties of wood and fiber reinforced polymer composites γ Radiation shielding attenuation characteristics
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https://www.eduzhai.net American Journal of Materials Science 2019, 9(1): 8-14 DOI: 10.5923/j.materials.20190901.02 Attenuation Property of Wood and Fiber Reinforced Polymer Composite Materials for Neutron and Gamma Radiation Shielding M. Shamsuzzaman1,*, M. A. M. Khan2, M. M. H. Bhuiyan1, M. S. Rahman1, M. J. H. Khan1, D. Paul1, D. R. Sarkar2 1Institute of Nuclear Science and Technology, Atomic Energy Research Establishment, Savar, Dhaka, Bangladesh 2Department of Physics, Jagannath University, Dhaka, Bangladesh Abstract The radiation shielding capacity of some locally available wood and composite materials were explored. The attenuation capacity was investigated in terms of relative attenuation factor (RAF), linear attenuation coefficient (µ) and mass attenuation coefficient (µm) which determined for both low and high gamma photons, and neutron radiation. The determined attenuation coefficients of some wood samples of Mehagany (Swietenia macrophylla), Rain tree (Albizia saman) and Mango (Mangifera indica) wood were compared with the fiber reinforced polymer composite samples of Glass fiber and Jute composite. The µm profile implied a better attenuation capacity of wood samples than that of the glass fiber composite and jute composite samples for low energy gamma photons. In the case of high energy photons, wood samples revealed the uppermost attenuation capacity in comparison to the glass fiber composite, jute composite samples and concrete slab in terms of µm. For neutron beam, both the glass fiber composite and jute composite samples indicated higher attenuation capacity than that of the wood samples in terms of µ; although, µm showed a similar attenuating performance with a steepened fashion. Hence, Glass fiber and Jute composites possessed a good shielding worth in the case of neutron beam, and Rain tree wood exhibited a satisfactory attenuation capacity for low and high energy gamma photon beams. Keywords Shielding, Radiation, Composite materials, Linear attenuation coefficient, Mass attenuation coefficient 1. Introduction Ionization radiation is an indispensable part of nuclear technology which is currently being used in various fields of industry, medicine, agriculture and scientific research . In reality, although nuclear technology is advantageous but ionizing radiation enacts harmful effects on human health and environment that documented quite well . Thus, radiation protection emphasizes on the emplacement of shielding materials between the ionizing radiation source and the worker or the environment . Shielding material is a prerequisite to attenuate the photon beam. When photon beam passes into a shielding medium in a form of radiation, some of the energies of the beam are transferred to that medium . If the energy of the beam is stronger than the required absorbing capacity of the medium, the energy of the beam comes out and affects the other medium as well as * Corresponding author: firstname.lastname@example.org (M. Shamsuzzaman) Published online at https://www.eduzhai.net Copyright © 2019 The Author(s). Published by Scientific & Academic Publishing This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/ person near to it. Radiation passing through body tissues may produce biological damage, so medical, scientific and technical personnel who are working with radiation source should maintain the proper distance. However, in practical there is limitation on keeping larger distance in a workplace. Therefore, the most effective method of radiation protection is the use of shielding materials to curtail radiation . This radiation can be reduced by maintaining proper thickness with appropriate composition of the shielding materials. The thickness of different material composition chosen for the principal shielding material depends on the required attenuation of neutron and gamma rays of a specific energy. The possible interaction probability between gamma rays and atomic nuclei depends on the attenuation coefficient of a particular material . Many researchers determined the attenuation coefficients using various techniques [7-12], but those measurements did not incorporate the similar wood and composite materials as available in Bangladesh. Further, the attenuation coefficient of several foreign wood materials published in various studies by different countries cannot be directly used on performing shielding calculations [13-15]. Further, all foreign studied materials are not locally available in everywhere, and some study materials are very costly as well. In this situation, the study of attenuation capacity of American Journal of Materials Science 2019, 9(1): 8-14 9 some locally available wood and composite materials is essential to verify whether these materials could be a good option for radiation shielding design. The purpose of present study is to determine the attenuation coefficient and the attenuation factor of some locally available, cost effective and environmental friendly potential shielding materials to be used for radiation protection at various radiation facilities in Bangladesh. 2. Method and Materials Collimated radiation beam of gamma and neutron radiation sources were used to estimate the shielding properties of some composite and wooden materials. In this perspective, locally available wood samples, jute composite material, and glass fiber composite materials were taken to evaluate their radiation attenuation capacity in relatively low and high energy gamma radiation, neutron radiation. The Gamma radiation attenuation capacity was investigated with these wood samples to check their potential usage as shielding material within the photon energy rangy range of 59.5 – 1332 keV. In this perspective, 241Am source was used for the low energy gamma photon of 59.5 keV, and 60Co source was used for relatively high energy gamma photon of 1332 keV. 241Am-Be source was used to determine the neutron radiation attenuation capacity. The aforesaid three types of sample materials and radiation sources were used with necessary radiation measuring detector. The low energetic photon beam outputs were found to be attenuated significantly while using the sample materials, in comparison to the direct readings, due to absorption of the photon beam in the sample matrix. The attenuation of the high energy photon beam was observed as well with the same studied materials. When gamma-ray beam traverses an absorber, the intensity of the beam will be attenuated according to the Beer-Lambert's law [6, 7]. In present experiment, the attenuation of the transmitted gamma photon and neutron intensity through the absorbing materials is described by this law: I = I0e−µt (1) Where I0 and I are the unattenuated and attenuated gamma ray beam intensities, µ (cm-1) is the linear attenuation coefficient and t is the thickness of the material (cm). In this study, I0 indicates the initial radiation dose rate (D) for neutron, low energy gamma photon (Eγ = 59.5 KeV), and high energy gamma photon (Eγ = 1332 KeV). The linear attenuation coefficient could be useful to determine the mass attenuation coefficients µ ρ (cm2/g) by applying the bulk densities of the respective samples as follows: µ = 1 ρt ln I0 I (2) The linear attenuation coefficient reflects the removal of photons from a radiation beam by interaction with electrons of the sample material. The higher the electron density, the more interaction of gamma photons with the sample material occurs. These interactions can cause the absorption of the photons (i.e., removal from the beam) or scattering (i.e., change of direction with reduction in energy). Therefore, it seems appropriate to scale the linear attenuation coefficient with the sample density. The linear attenuation coefficient can also be rewritten as: µ = µ ρ ρ (3) Where µ ρ is the mass attenuation coefficient (cm2/g) and ρ is the density (g/cm3). The mass attenuation coefficient is approximately constant for different materials in a specified energy range, and therefore the linear attenuation coefficient is strongly determined by the density. The linear attenuation coefficient is also strongly energy dependent. In general, lower energetic gamma photons have a higher interaction probability, and hence cause relatively high attenuation. In this study, photon beam transmission was considered in a relatively broad energy range (i.e. 59.5 – 1332 keV) to verify the shielding applicability of the studied samples in a wide energy range. 3. Experimental Details 3.1. Sample Preparation In the present study four types of locally available wood samples were collected to investigate their shielding potential. The chemical composition of wood varies from species to species, however the conventional composition of the composite  and wood  samples is presented in Table 1. Wood samples were collected from the local timber market locates at various places in Dhaka city. After collection, wood samples were dried to make it moisture free. Then, it was polished properly to make both surfaces smooth enough. Jute composite samples were prepared with jute fiber, sandwiched with synthetic resins. The properties of synthetic resins are similar to natural plant resins. The glass fiber composite samples were prepared with fine fibers of glass materials. The reference concrete sample for gamma radiation was prepared from the ordinary Portland cement with water-cement ratio of 0.50 and cement-sand ratio of 1:1.5 was maintained. As a reference shielding material for neutron radiation, wax sample was prepared with Beeswax (cera alba) which is a natural wax. The size of all samples was organized based on the aperture of the collimator. Figure 1 shows the physical view of different types of studied samples. Prior to perform the experimental analysis, the physical appearance of the sample materials were checked to ensure the good shape and appearance, and then these samples were used. After getting the required physical condition, these samples were deployed to determine their attenuations coefficient and relative attenuation factor. 10 M. Shamsuzzaman et al.: Attenuation Property of Wood and Fiber Reinforced Polymer Composite Materials for Neutron and Gamma Radiation Shielding (a) Jute composite (b) Glass fiber composite (c) Rain tree wood (d) Mango wood (e) Mehagany (f) Concrete slab (g) Wax slab Figure 1. Locally available potential shielding materials used for experimental study The elemental description of the glass fiber, jute fiber, and conventional wood materials are presented in Table 1. Table 1. Elemental composition of the composite and wood samples Name of Element Jute fiber polypropylene composite (0.9049 g/cc)  E-glass fiber polypropylene Composite (1.1 g/cc)  Conventional indigenous wood (%)  H 0.103 0.072 6 B 0.016 C 0.629 0.428 50 O 0.268 0.239 43 Na 2.226E-3 Mg 0.014 Al 0.040 Si 0.127 Ca 0.062 Other elements (mainly calcium, potassium, sodium, magnesium, iron, and manganese) 1 3.2. Experimental Arrangement In the present experiments samples were paced in front of the source collimator to investigate the radiation shielding property for high energy gamma photons, and fast neutron of energy 4.4 MeV. In the case of low energy gamma photons samples were placed at 30 cm distance from the 241Am source. The photographic views of the experimental arrangements are shown in Figure 2(a), (b), and (c). In this figure, (a) represents the setup of high energy gamma photon with 60Co source, (b) represents the setup of low energy gamma photon with 241Am source, and (c) represents the setup of neutron radiation with 241Am-Be source. In the first step of experiment, radiation dose rate was recorded without any samples in the radiation beam. Then, in the second step, respective samples were placed in the radiation beam to estimate their attenuation capacity. Consequently, attenuation coefficients of all the studied samples were determined based on the Beer-Lambert's law. American Journal of Materials Science 2019, 9(1): 8-14 11 (a) (b) (c) Figure 2. Experimental setup for attenuation assessment of various samples with (a) 60Co gamma source (b) 241Am low energy gamma source (c) 241Am-Be neutron source 4. Results and Discussion This study presents the attenuation capacity of some wood samples and fiber reinforced polymer composite samples against gamma radiation and neutron. The analyzed composite materials were based on Glass fiber and Jute composite. Also three types of wood samples such as Mehagany, Rain tree and Mango wood were used in the experiments. Relative attenuation factors (RAF), linear attenuation coefficients (µ), and mass-attenuation coefficients (µm) of these potential shielding materials (i.e., Glass fibers, Jute composite, Mehagany, Rain tree and Mango wood) were determined in the present experiments. The experimental observation of RAF for the low and high gamma photon is presented in Table 2 and Table 3. A descending trend of the RAF is observed from these two tables for the respective studied materials with gamma photons. The experimental breakthrough of µ and µm are presented in Figure 3(a) and (b) for low gamma photons. In these figures, an ascending trend of µ and µm is observed with sample thickness. In the case of high energy gamma photons, µ and µm are presented in Figure 4 (a) and (b). The neutron shielding capacity in terms of µ and µm of the studied materials is presented in Figure 5 (a) and (b). From these figures, a similar ascending trend of µ and µm is observed as well. In this study concrete and wax were used as the reference shielding material for neutron radiation and gamma radiation respectively. The calculated attenuation coefficients of the composite and wooden materials indicate a reasonable shielding potential for the gamma and neutron radiation attenuation. In the case of neutron radiation, experimentally determined values of RAF are presented in Table 4. From this table a descending trend of the RAF is evident in a similar fashion of the gamma photons. Table 2. Relative Attenuation Factors (RAF) of the studied samples in terms of concrete slab for low energy gamma radiation Thickness (cm) 0.50 1.00 1.50 2.00 2.50 Dconcrete Dglass fiber 0.802 0.736 0.543 0.576 0.492 Relative Attenuation Factor (RAF) Dconcrete Djute composite Dconcrete Dmehagany wood Dconcrete Drain tree wood 0.754 0.781 0.749 0.715 0.662 0.637 0.479 0.466 0.460 0.451 0.444 0.439 0.372 0.364 0.351 Dconcrete Dmango wood 0.741 0.630 0.442 0.424 0.337 Table 3. Relative Attenuation Factors (RAF) of the studied samples in terms of concrete slab for the high energy gamma radiation Thickness (cm) 0.50 1.00 1.50 2.00 2.50 Dconcrete Dglass fiber 0.967 0.956 0.945 0.933 0.897 Relative Attenuation Factor (RAF) Dconcrete Djute composite Dconcrete Dmehagany wood Dconcrete Drain tree wood 0.958 0.957 0.956 0.936 0.920 0.915 0.920 0.891 0.892 0.894 0.864 0.854 0.853 0.812 0.802 Dconcrete Dmango wood 0.947 0.904 0.866 0.837 0.789 12 M. Shamsuzzaman et al.: Attenuation Property of Wood and Fiber Reinforced Polymer Composite Materials for Neutron and Gamma Radiation Shielding Table 4. Calculated Relative Attenuation Factors (RAF) of the studied samples in terms of wax for neutron radiation Thickness (cm) 0.50 1.00 1.50 Dwax Dglass fiber 0.866 0.861 0.848 Relative Attenuation Factor (RAF) Dwax Djute composite Dwax Drain tree wood 0.854 0.826 0.850 0.793 0.817 0.713 Dwax Dmango wood 0.815 0.769 0.699 exhibit better attenuation capacity than that of the glass fiber composite and jute composite samples. Figure 3. Variation of (a) linear attenuation coefficient and (b) mass attenuation coefficient of six analyzed shielding materials for the low energy gamma photon of 241Am source A comparative assessment of the linear attenuation (µ), and mass-attenuation coefficients (µm) for the six studied samples with low energy gamma photon are expressed in a graphical view, and presented in Figure 3 (a) and (b). Figure 3(a) indicates that in the case of µ, highest liner attenuation capacity is evident for the concrete slab, and both the glass fiber composite and jute composite samples indicated higher attenuation capacity than that of the wood samples. On the other hand, based on µm profile from Figure 3 (b), although concrete indicates the highest attenuation capacity in a similar fashion of µ variation, however wood samples Figure 4. Variation of (a) linear attenuation coefficient and (b) mass attenuation coefficient of six analyzed shielding materials for the high energy gamma photon of 60Co source In the case of high energy photon beams, a comparative assessment of µ and µm is shown in Figure 4 (a) and (b). From these figures, concrete slab indicates the highest attenuation tend in terms of µ, whereas based on µm, concrete indicates the lowest attenuation capacity in comparison to the studied samples. From Figure 4 (a) it is seen that, both the glass fiber composite and jute composite samples indicated higher attenuation capacity than that of the wood samples based on µ. However, in terms of µm, wood samples exhibit American Journal of Materials Science 2019, 9(1): 8-14 13 the highest attenuation capacity in comparison to the glass fiber composite, jute composite samples and concrete slab, as shown in Figure 4 (b). For the neutron radiation, the comparison of µ and µm for five studied samples are verified in a graphical observation, as presented in Figure 5 (a) and (b). Figure 5 (a) indicates that in the case of µ, highest liner attenuation capacity is apparent for the wax sample, and both the glass fiber composite and jute composite samples indicated higher attenuation capacity than that of the wood samples. In the case of µm variation from Figure 5 (b), although wax indicates the highest attenuation capacity in a similar manner of µ, however attenuation capacity of the glass fiber composite, jute composite and the wood samples are relatively reduced with the similar trend in comparison of µ. descending trend of RAF was observed for all the studied samples for both gamma photon and neutron beams. For low energy gamma photons wood samples exhibit better attenuation capacity than that of the glass fiber composite and jute composite samples based on µm profile. In the case of high energy photons, wood samples exhibited the highest attenuation capacity in comparison to the glass fiber composite, jute composite samples and concrete slab in terms of µm. For neutron beam, both the glass fiber composite and jute composite samples indicated higher attenuation capacity in comparison to wood samples in terms of µ. Therefore, Glass fiber and Jute composites possessed a good shielding worth in the case of neutron beam. On the other hand, some wood materials exhibited an attenuation capacity for low and high energy gamma photon beams. Thus, the studied materials have good scope for the potential shielding applications in scientific laboratory, medical, industrial shielding purposes. REFERENCES  Merril Eisenbud, Industrial uses of Ionizing radiation, American Journal of Public Health, Vol. 55, No. 5, 1965.  Gabriele Mraz, Oda Becker, Health effects of ionizing radiation and their consideration in radiation protection, Vienna Ombuds-Office for Environmental Protection, Vienna, 2017, http://www.ecology.at/files/pr887_2.pdf.  Y. Elmahroug, B. Tellili, C. Souga, Calculation of Gamma and Neutron Shielding Parameters for Some materials Polyethelene-based, International Journal of Physics and Research (IJPR), Vol.3, Issue 1, 33-40, 2013.  Aurther Beiser, “Concepts of Modern Physics”, Fifth edition TATA McGRAW-Hill, 81.  Ero F.A and Adebo B.A., Determination of γ - Radiation Shielding Characteristics of some Woods in Western Nigeria, International Archive of Applied Sciences and Technology, Volume 3, 14 – 20, 2012.  M. N. Alam, M.M.H. Miah, M.I. Chowdhury, M. Kamal, S, Ghose, Runi Rahman, “Attenuation coefficients of soils and some building materials of Bangladesh in the energy range 276 – 1332 keV” Applied Radiation & Isotopes, 54, 973 (2001). Figure 5. Variation of (a) linear attenuation coefficient and mass attenuation coefficient of studied shielding materials for neutron radiation of 241Am-Be source  Y. Elmahroug, B. Tellili & C. Souga, “Calculation of gamma and neutron shielding parameters for some materials polyethylene-based”. International Journal of Physics and Research, 3, 33 – 40 (2013). 5. Conclusions  M. J. H. Khan, Mubarak A. Khan, R. A. Khan, M. M. Sarker and M. Rahman, A computational analysis on attenuation The attenuation capacities of some locally available wood property of fiber reinforced polymer based composit using and fiber reinforced polymer composite samples were evaluated in terms of relative attenuation factor (RAF), linear attenuation (µ), and mass-attenuation coefficients (µm). Monte Carlo Technique, Proceedings of the International Conference on magnetism and Advanced Materials (ICMAM-2010), 03 – 07 March 2010, Dhaka, Bangladesh. Apparently, all the studied materials indicated a potential  Arthur B. Anderson, “The composition and structure of wood” shielding property for both gamma and neutron radiation. A J. Chem. Educ., 1958, 35 (10), p 487 (1958). 14 M. Shamsuzzaman et al.: Attenuation Property of Wood and Fiber Reinforced Polymer Composite Materials for Neutron and Gamma Radiation Shielding  B. H. Damla, A. Celik, E. Kiris, U. Cevik, “Calculation of radiation attenuation coefficient affective atomic number and electronic densities for some building materials” Radiation Protection Dosimetry, 150, 541 – 549 (2012).  E. Storm, H. I. Israel, “Photon cross sections from 1 KEV to 100 MEV for elements Z=1 to Z=100” Nuclear data Table A7, 565-681 (1970).  J. H. Hubbel, “Photon mass attenuation and energy absorption coefficients from 1 keV to 20 MeV” Applied Radiation & Isotopes, 33, 1269 (1982).  I. C. P Salinas, C.C. Conti and R.T. Lopes, “Effective density and mass attenuation coefficient for building material in Brazil” Applied Radiation & Isotopes, 64 (1), 13 (2006).  C. R. Appoloni, E. A. Rios, “Mass attenuation coefficients of brazilian soils in the range 10–1450 keV” Applied Radiation & Isotopes, 45 (3), 287, (1994).  R. Cesareo, J. T. De Assis, S. Crestana, “Attenuation coefficients and tomographic measurements for soil in the energy range 10—300 keV” Applied Radiation & Isotopes, 45 (5), 613, (1994).
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