The glasses studied here have been prepared by the melt quenching technique from Egyptian rice husk silica.The obtained solid glasses exhibit amorphous nature and transparency. These glasses were selected to obey the following composition, (75-x) mol % RH silica. 25mol % Na2O. x mol % Bi2O3, where x takes the values, 0, 5, 10, 15 and 20. It was found that, as Bi2O3 was gradually increased both the density and molar volume values increased. The comparison between the experimental and empirical density and molar volume values confirm that all the studied glasses are in amorphous glassy phase. Moreover, all samples showed also good shielding properties against gamma ray radiation and neutrons. The mass attenuation coefficient of gamma ray radiation increased gradually as Bi2O3 was gradually increased while the HVL values exhibit gradual decrease, and the sample that contains 20 mol % Bi2O3 appeared the efficient one at low gamma ray energy (especially at 356 KeV). On the other hand "for shielding neutrons" the sample that contains 5 mol% Bi2O3 appeared the best one since it exhibits the highest neutron removal cross section.
Published in | American Journal of Modern Physics (Volume 4, Issue 4) |
DOI | 10.11648/j.ajmp.20150404.11 |
Page(s) | 149-157 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2015. Published by Science Publishing Group |
Bismuth Oxide, Agricultural Wastes, Egyptian RH- Silica, Shielding Properties, Radioactive Sources, Fast Neutron
[1] | M. Jalali and A. Mohammadi, J. Radiat. Phys. Chem., 77 (2008) 523. |
[2] | N. Chanthima, J. Kaewkhao and P. Limsuwan, J. Ann. Nucl. Energy, 41 (2012) 119. |
[3] | N. Chanthima, P. Prongsamrong, J. Kaewkhao and P. Limsuwan, J. Procedia Eng., 32 (2012) 976. |
[4] | J. Kaewkhao and P. Limsuwan, J. Nucl. Instrum. Method Phys. Res. A, 619 (2010) 295. |
[5] | K. Kirdsiri, J. Kaewkhao, N. Chanthima and P. Limsuwan, J. Ann. Nucl. Energy, 38 (2011) 1438. |
[6] | M. Kurudirek, Y. Ozdemir, O. Simsek and R. Durak, J. Nucl. Mater., 407 (2010) 110. |
[7] | S.R. Manohara, S.M. Hanagodimath and L. Gerward, J. Nucl. Mater., 393 (2009) 465. |
[8] | H. Singh, K. Singh, L. Gerward, K. Singh, H.S. Sahota and R. Nathuram, J. Nucl. Instrum. Method Phys. Res. B, 207 (2003) 257. |
[9] | K. Singh, H. Singh, V. Sharma, R. Nathuram, A. Khanna, R. Kumar, S.S. Bhatti and H.S. Sahota, J. Nucl. Instrum. Method Phys. Res. B, 194 (2002) 1. |
[10] | K. Singh, H. Singh, G. Sharma, L. Gerward, A. Khanna, R. Kumar, R. Nathuram and H.S. Singh, J. Radiat. Phys. Chem., 72 (2005) 225. |
[11] | K.J. Singh, N. Singh, R.S. Kuandal and K. Singh, J. Nucl. Instrum. Methods. B, 266 (6) (2008) 944. |
[12] | S. Singh, A. Kumar, D. Singh, K. Singh, K.S. Thind and G.S. Mudahar, J. Nucl. Instrum. Meth. B, 266 (1) (2008) 140. |
[13] | N. Singh, K.J. Singh, K. Singh and H. Singh, J. Nucl. Instrum. Method Phys. Res. B, 225 (2004) 305. |
[14] | N. Singh, K.J. Singh, K. Singh and H. Singh, J. Radiat. Meas., 41 (2006) 84. |
[15] | L. Gerward, N. Guilbert, K.B. Jensen and H. Levring, J. Radiat. Phys. Chem., 60 (2001) 23. |
[16] | L. Gerward, N. Guilbert, K.B. Jensen and H. Levring, J. Radiat. Phys. Chem., 71 (2004) 653. |
[17] | Japan Cement Association, 2008. Report: Cement Demand and Supply in Japan, 1. |
[18] | S. Chandrasekhar, PN. Pramada and J. Majeed, J. Materials Science, 41 (2006) 7926. |
[19] | S. Chandrasekhar, PN. Pramada and L. Praveen, J. Materials Science, 40 (2005) 6535. |
[20] | H. A. Saudi, S. M. Salem, S. S. Mohammad, A. G. Mostafa and M. Y. Hassaan, to be published in the American Journal of physics and applications, (2015). |
[21] | A.K. Varshneya, “Fundamentals of Inorganic Glasses,” Society of Glass Technology, Sheffield, UK, 2006. |
[22] | N. Singh, K. J. Singh, K. Singh and H. Singh, J. Nucl. Instr. Meth. (B), 225 (2004) 305. |
[23] | N. Singh, K. J. Singh, K. Singh and H. Singh, J. Radiat. Meas., 41 (2006) 84. |
[24] | K. J. Singh, N. Singh, R. S. Kaundal and K. Singh, J. Nucl. Instr. Meth. (B), 266 (2008) 944. |
[25] | N. Singh, R. Singh and K. J. Singh, Glass Technol., 46 (4) (2005) 311. |
[26] | M. E. Medhat, J. Ann. Nucl. Energy, 36 (2009) 849. |
[27] | U. Cevik, N. Damla, A. I. Kobya, N. Celik, A. Celik and A. A. Van, J. Radiol. Prot., 29 (2009) 61. |
[28] | A. G. Mostafa, M. Y. Hassaan, A. A. Ramadan, A. Z. Hussein and A. Y. Abdel-Hassib, J. Nature and Science, 11 (5) (2014) 148. |
[29] | J.E. Shelby, the Royal Society of Chemistry, UK, (1997) 137. |
[30] | H. A. Saudy, S. El Mosallamy, S. U. El Kameesy, N. Sheta, A. G. Mostafa, and H. A. Sallam, World J. Condens. Matter Phys., 03 (2013) 9. |
[31] | R. El-Mallawany, N. El-Khoshkhany and H. Afifi, J. Materials Chemistry and Physics, 95 (2006) 321. |
[32] | C. Narayana Reddy, V. C. Veeranna Gowda and R. P. Sreekanth Chakradhar, Journal of Non- Crystalline Solids, 354 (2008) 32. |
[33] | Yasser B. Saddeek, M. S. Gaafar and Safaa A. Bashier, J. Journal of Non-Crystalline Solids, 356 (2010) 1089. |
[34] | J. Qi, D. Xue, H. Ratajczak and G. Ning, Physica B, 349 (2004) 265. |
[35] | H. Doweidar and Yasser B. Saddeek, J. Non-Crystalline Solids, 355 (2009) 348. |
[36] | S. S. Mohammad, M. Sc. Thesis, Al-Azhar Univ., (2012). |
[37] | D. A. Magdas, A, Cosar, V. Chis, I. Ardelean and N. Vedeanu, Vib. Spectrosc., 48 (2008) 251. |
[38] | L. Gerward, N. Guilbert, K.B. Jensen and H. Levring, J. Radiat. Phys.Chem., 71 (2004) 653. |
[39] | J. H. Hubbell, Int. J. Appl. Radiat. Isot., 33 (1982) 1269. |
[40] | J. H. Hubbell, J. Phys .Med. Biol., 44 (1999) 1. |
[41] | I. I. Bashter, J. Ann. Nucl. Energy, 24 (1997) 1389. |
[42] | A. B. Chilton, J. K. Shultis and R. E. Faw, principles of Radiation Shielding, Prentice Hall, New York., (1984) |
[43] | M.F. Kaplan, Wiley, New York (1989). |
[44] | H. A. Saudi, J. Applied Mathematics and Physics, 4 (2013) 143. |
APA Style
A. G. Mostafa, H. A. Saudi, M. Y. Hassaan, S. M. Salem, S. S. Mohammad. (2015). Studies on the Shielding Properties of Transparent Glasses Prepared from Rice Husk Silica. American Journal of Modern Physics, 4(4), 149-157. https://doi.org/10.11648/j.ajmp.20150404.11
ACS Style
A. G. Mostafa; H. A. Saudi; M. Y. Hassaan; S. M. Salem; S. S. Mohammad. Studies on the Shielding Properties of Transparent Glasses Prepared from Rice Husk Silica. Am. J. Mod. Phys. 2015, 4(4), 149-157. doi: 10.11648/j.ajmp.20150404.11
AMA Style
A. G. Mostafa, H. A. Saudi, M. Y. Hassaan, S. M. Salem, S. S. Mohammad. Studies on the Shielding Properties of Transparent Glasses Prepared from Rice Husk Silica. Am J Mod Phys. 2015;4(4):149-157. doi: 10.11648/j.ajmp.20150404.11
@article{10.11648/j.ajmp.20150404.11, author = {A. G. Mostafa and H. A. Saudi and M. Y. Hassaan and S. M. Salem and S. S. Mohammad}, title = {Studies on the Shielding Properties of Transparent Glasses Prepared from Rice Husk Silica}, journal = {American Journal of Modern Physics}, volume = {4}, number = {4}, pages = {149-157}, doi = {10.11648/j.ajmp.20150404.11}, url = {https://doi.org/10.11648/j.ajmp.20150404.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20150404.11}, abstract = {The glasses studied here have been prepared by the melt quenching technique from Egyptian rice husk silica.The obtained solid glasses exhibit amorphous nature and transparency. These glasses were selected to obey the following composition, (75-x) mol % RH silica. 25mol % Na2O. x mol % Bi2O3, where x takes the values, 0, 5, 10, 15 and 20. It was found that, as Bi2O3 was gradually increased both the density and molar volume values increased. The comparison between the experimental and empirical density and molar volume values confirm that all the studied glasses are in amorphous glassy phase. Moreover, all samples showed also good shielding properties against gamma ray radiation and neutrons. The mass attenuation coefficient of gamma ray radiation increased gradually as Bi2O3 was gradually increased while the HVL values exhibit gradual decrease, and the sample that contains 20 mol % Bi2O3 appeared the efficient one at low gamma ray energy (especially at 356 KeV). On the other hand "for shielding neutrons" the sample that contains 5 mol% Bi2O3 appeared the best one since it exhibits the highest neutron removal cross section.}, year = {2015} }
TY - JOUR T1 - Studies on the Shielding Properties of Transparent Glasses Prepared from Rice Husk Silica AU - A. G. Mostafa AU - H. A. Saudi AU - M. Y. Hassaan AU - S. M. Salem AU - S. S. Mohammad Y1 - 2015/06/09 PY - 2015 N1 - https://doi.org/10.11648/j.ajmp.20150404.11 DO - 10.11648/j.ajmp.20150404.11 T2 - American Journal of Modern Physics JF - American Journal of Modern Physics JO - American Journal of Modern Physics SP - 149 EP - 157 PB - Science Publishing Group SN - 2326-8891 UR - https://doi.org/10.11648/j.ajmp.20150404.11 AB - The glasses studied here have been prepared by the melt quenching technique from Egyptian rice husk silica.The obtained solid glasses exhibit amorphous nature and transparency. These glasses were selected to obey the following composition, (75-x) mol % RH silica. 25mol % Na2O. x mol % Bi2O3, where x takes the values, 0, 5, 10, 15 and 20. It was found that, as Bi2O3 was gradually increased both the density and molar volume values increased. The comparison between the experimental and empirical density and molar volume values confirm that all the studied glasses are in amorphous glassy phase. Moreover, all samples showed also good shielding properties against gamma ray radiation and neutrons. The mass attenuation coefficient of gamma ray radiation increased gradually as Bi2O3 was gradually increased while the HVL values exhibit gradual decrease, and the sample that contains 20 mol % Bi2O3 appeared the efficient one at low gamma ray energy (especially at 356 KeV). On the other hand "for shielding neutrons" the sample that contains 5 mol% Bi2O3 appeared the best one since it exhibits the highest neutron removal cross section. VL - 4 IS - 4 ER -