Borosilicate Glass Containing Bismuth and Zinc Oxides as a Hot Cell Material for Gamma-Ray Shielding

H. A. Saudi, H. A. Sallam, K. Abdullah

  Open Access OPEN ACCESS  Peer Reviewed PEER-REVIEWED

Borosilicate Glass Containing Bismuth and Zinc Oxides as a Hot Cell Material for Gamma-Ray Shielding

H. A. Saudi1,, H. A. Sallam1, K. Abdullah2

1Physics Department, Faculty of Science, Al-Azhar University, Girls Branch, Nasr City, Cairo, Egypt

22Physics Department, Faculty of Science, Al-Azhar University, boys Branch, Nasr City, Cairo, Egypt

Abstract

Gamma-ray attenuation coefficients (the half value layer parameters, gamma – ray shielding properties) for the x ZnO - (5−x) Bi2O3 -10 B2O3 -40 SiO2 (x = 0, 5, 10, 15 and 20) at 662, 1173 and 1332 keV photon energies have been determined experimentally, using a narrow beam transmission method, as well as theoretically using the ‘mixture rule’ and the ‘XCOM’ computer software. The molar volume and FTIR investigations have been used to study the structural properties of the glass system. Optical, UV-visible, absorption measurements were performed also to investigate the transmittance aimed to investigate the performance of the glass system for using as hot cells for shielding windows in nuclear technology.

At a glance: Figures

Cite this article:

  • Saudi, H. A., H. A. Sallam, and K. Abdullah. "Borosilicate Glass Containing Bismuth and Zinc Oxides as a Hot Cell Material for Gamma-Ray Shielding." Physics and Materials Chemistry 2.1 (2014): 20-24.
  • Saudi, H. A. , Sallam, H. A. , & Abdullah, K. (2014). Borosilicate Glass Containing Bismuth and Zinc Oxides as a Hot Cell Material for Gamma-Ray Shielding. Physics and Materials Chemistry, 2(1), 20-24.
  • Saudi, H. A., H. A. Sallam, and K. Abdullah. "Borosilicate Glass Containing Bismuth and Zinc Oxides as a Hot Cell Material for Gamma-Ray Shielding." Physics and Materials Chemistry 2, no. 1 (2014): 20-24.

Import into BibTeX Import into EndNote Import into RefMan Import into RefWorks

1. Introduction

Today, the use of nuclear energy and radiation is indispensable in modern society. Handling with radiation sources with safe is essential. The knowledge of gamma-ray interaction parameters such as mass attenuation coefficient, half value layer, mean free path, etc. is very important in the field of radiation shielding materials[1, 2]. The most radiation shielding materials commonly used is concrete because it is inexpensive and adaptable for any construction design. There are however many drawbacks associated with the usage of concrete, such as considerable variability in its composition and water content. This variation results in uncertainty in calculations for shield design predictions of the radiation distribution and attenuation in the shield. Water contents have the disadvantages of decreasing both density and structural strength of concrete. However, its drawback is the loss of water when concrete becomes hot by absorption of energy from radiation [2, 3]. Recently glass materials are one of the possible alternatives to concrete because they can be transparent to visible light and their properties can be modified by composition and preparation techniques. Silicate glasses are the most commonly available commercial glasses due to ease of fabrication and excellent transmission to visible light. Borosilicate glasses are known for having very low coefficients of thermal expansion making them resistant to thermal shock and these glasses have also the ability for an excellent transmission to visible light. Bismuth is expected to enhance the gamma-ray attenuation due to its higher atomic number. Addition of bismuth to glasses has improved also there chemical durability [4]; therefore, bismuth contributes to the stabilization of the glass structure [4]. ZnO containing optical materials have been drawing a good attention of the scientific community over world due to their very interesting optical properties in combination with their non-toxicity, non-hygroscopic nature and lower cost [5].

With these considerations in mind, we have selected this glass system for exploring the possibility of using them as hot cell material for gamma-ray shielding.

2. Theory

For photons in an attenuating medium, HVL (half value layer) is the thickness of a material required to reduce the intensity of the emergent radiation to half [6]. I = Ioemt where Io denotes the photons with energy E, intensity without attenuation; I the photons with energy E, intensity after attenuation; μm = μ/ρ (cm2/g) is the mass attenuation coefficient and t (g/cm2) is sample mass thickness (the mass per unit area). The total μm values for materials composed of multi elements is the sum of the (μm)i values of each constituent element [6] by the following mixture rule μm =∑I wi (μm)i, HVL=0.693/μ(cm).

3. Experimental Work

Analytically, pure grade chemicals were used to prepare the following glass samples according to the formula :(x ZnO - (5−x) Bi2O3 -10 B2O3 -40 SiO2 mol% where x = 0, 5, 10, 15 and 20. The batch mixtures were melted in porcelain crucibles at 1100 ° for two hours until homogeneous glasses were obtained and then annealed in a separate annealing furnace at 250 °C and then slowly cooled to the room temperature to remove any internal stresses. Samples have been obtained in circular shape of 2 cm. Glass density measurements were measured at room temperature using the standard Archimedes method, with toluene as the immersion fluid of stable density (0.866 g/cm3).

Attenuation coefficients of the proposed glass system were measured in a narrow beam transmission geometry by using a 2 × 2 NaI(TI) crystal detector with energy resolution of 12.5% at 662 keV in conjunction with multi-channel analyzer (MCA). Samples were placed on specimen holder at a distance of 10 cm from source. The distance between source and detector was 20 cm. Radioactive sources 60Co and 137Cs having activities (10 μCi) each were used for different photon energies. Incident and transmitted intensities of photons were measured on MCA for fixed preset time for each sample by selecting a narrow region symmetrical with respect to the centroid of the photo peak. Counting time was chosen such that 103-105 counts, which were recorded under each photo peak.

The infrared absorption spectra of the glass system were measured at room temperature in the range 2000–400 cm−1 by a Fourier Transform infrared spectrometer (type Perken Elmer spectrometer, model RTX, FTIR) using the KBr disc technique.

Optical ultraviolet (UV) –visible absorption measurements, transmission spectra of the prepared glasses in the range 190 to 1100 nm were measured by Genway 6405 -UV-VIS spectrophotometer.

4. Results and Discussion

4.1. Structural Properties
4.1.1. Density (ρ) and Molar Volume

The density is a powerful tool capable of exploring the changes in the structure of glasses. The density is affected by the structural softening/compactness[7], change in geometrical configuration, coordination number, cross-link density and dimension of interstitial spaces of the glass. In the studied glasses, it is noted that Figure 1, the density decreases with increasing ZnO content in the glass due to the replacement of the heavy metal oxide (Bi2O3) by lighter oxide (ZnO). So addition of ZnO to network causes some type of structural rearrangement of the atoms. There is a possibility for the alteration of the geometrical configuration upon substitution of ZnO into the glass network. The density value of glass agrees well with that resulted from the present IR. Accordingly, the structure of the studied glasses will not be expanded, but with more compactness and low number of covalent bonds with decrease in the number of bridging oxygens. The more compactness is evident from the decreasing of the packing density as shown in Figure 1 and the decrease in covalent bonds and bridging oxygens are evident from our IR analysis as the Bi2O3 content decreases. This is congruent with decrease in the molar volume as the ZnO content increases. So Molar volume is also an important physical property.

Figure 1. Dependence of the density and the molar volume of on the percentage of ZnO content

4.1.2. FT-IR Absorption Spectra Analysis

Infrared spectroscopy is a valuable tool for studying the glass network structure [8]. In the IR spectra, 2, there are two broad bands that appear around 450 and 1008 cm−1. The broad bands as shown in 2 and Table 1 are an overlapping of some individual bands with each other. Each individual band is related to some type of vibration of a specific structural group. Therefore, it was necessary to use a deconvolution process [9] for separating these individual bands. Each individual band has its characteristic parameters such as its center (C), which is related to some type of vibration of a specific structural group, and its relative area (A), which is proportional to the concentration of this structural group. The deconvolution parameters of the bands for the investigated glasses are given in Table 1 and Figure 2.

Figure 2. IR spectra of :(5- x) Bi2O3x ZnO–1 0B2O340 SiO2 glasses and their deconvolution, which show the difference between the experimental and simulated curves

Table 1. Deconvolution parameters of the IR spectra of the glass system :( 0.5- x) Bi2O3x ZnO–0.1 B2O3–0.4 SiO2. C is the component band center and A is the relative area (%) of the component band

The IR analysis of the glass system indicates that the band around 450 cm−1, which appears in all glasses, is due to overlapping of Bi–O bending vibrations in BiO6 octahedral units and Si-O-Si bending in SiO4 tetrahedra [4, 10]. The Intensity of this band is decreasing with increasing the contents of ZnO because of decrease in BiO6 group. At the same time, a new band has been observed at 576cm-1 in sample with 5 ZnO which is due to the presence of Zn+2 ions which act as modifier in ZnO4 units overlapping with the vibrations of the BiO6 octahedral unit [4] in a location with the ring structure of SiO2 [10, 11]. The absorption band in the region 610–623 cm−1 may be due to Bi- O- stretching vibrations (non-bridging oxygen in BiO6 units. The band at 699–712 cm−1 is assigned to the bending vibrations of B–O linkages in the borate network [4, 12]. A weak band has been observed at 885 cm-1 which is due to non bridging oxygens of BO4 groups overlapping with the symmetrical stretching vibrations of the Bi–O bond in the BiO3, ZnO bond stretching of the tetrahedral ZnO4 units and Si- O- stretching with non-bridging oxygen [4, 11, 12]. So increasing the contents of ZnO, help for conversion of BO3 to BO4 groups and extra oxygen’s from Bi2O3 helps to form ZnO4 units in glass. This reveals the decrease of BiO3 units and the formation of more tetrahedral BO4 and ZnO4 groups. The band in the region 1006–1028 cm−1 is overlapping the symmetric stretching vibration of SiO4, BO4 tetrahedral units [4, 11]. The band in the region 1060–1075 cm−1 is attributed to the the Si- O- Si anti symmetric stretching vibrations of bridging oxygen in tetrahedra and BO4 units [13]. Upon increasing the zinc content the band at about 1060 cm-1 shifts to higher wave number 1075cm-1. The increasing of intensity of this band indicates an increase of BO4 groups. The band present around 1370cm-1 is due to stretching and bending vibration BO3 groups [14]. The Spectra reveal that the intensity of the band around 1370 cm-1 decreases and corresponding to it, the intensity of the band between 800 and 1200 cm-1 increases. This reveals that an addition of zinc modifies the glass network.

4.2. Gamma-ray Shielding Properties

The experimental values of mass attenuation coefficients along with theoretical values are shown in Figure 3. A good agreement has been observed between experimental and theoretical values and the discrepancies are within the experimental errors. The results of mass attenuation coefficients decrease with the mol% of ZnO which may be due to the decrease in the weight fraction of higher atomic number constituent (Bi) as compared to other elements. The mass attenuation coefficients for 5 to 15 ZnO content is nearly linear, This is due to the presence of Zn+2 ions in glass structure which modifies the borosilicate glass network by converting more BO3 to BO4 where extra oxygen’s from Bi2O3 helps to form ZnO4 units in glass. This reveals the decrease of BiO3 units and the formation of more tetrahedral BO4 and ZnO4 groups.

HVL is used to describe the effectiveness of γ-ray shielding [4]. Figure 4 show the behavior of the HVL for glasses with different amounts of ZnO and different γ-energies. This figure indicates that the half value layer (HVL) increases with decreasing weight fractions of Bi2O3 in this glass system. This is due to the lower values of mass attenuation coefficients and densities for glass samples. For all glass system higher γ-ray energies need more HVL of glasses.

Figure 3. Experimental and theoretical values of mass attenuation coefficients (μm) as function of mol% of ZnO in the glass system at 662, 1173 and 1332 keV
Figure 4. HVL function of mol% of ZnO in the glass system at 662, 1173 and 1332 keV
4.3. UV–Visible Transmission Spectra

Spectra of all prepared samples follow one common pattern, where an edge extended over wide wavelength range is observed Figure 5. This is in consistence with the non-crystalline nature of the glasses. The cut-off wavelength (λc) exhibit red shift with increasing ZnO content. Such behavior can be accounted for by increasing the number of non-bridging oxygen. The same behavior was observed by increasing ZnO content in bismuth borate glass [15]. A shoulder at 663 nm was observed and broadened with increasing ZnO content. It is evident from the figure that, the percentage of transmission decreases with increasing ZnO content except the sample with x = 5 ZnO which shows high percentage of transmittance in the visible region of the spectra (656 nm to 998 nm) Furthermore, sample with 20 ZnO content show a strong absorption in the UV region up to 530 nm. From IR results it can explain the transmission by the overlapping of the vibrations of the Bi–O bonds in the BiO6 octahedral unit with deformation modes of network structure and vibration of chemical bond Zn2+ - O2- in a location of with the ring structure of SiO2 at 575 cm−1. So x=0.05 make this concentration is more transparent than others.

Figure 5. The optical Transmission as a function of wavelength in the UV region of the prepared glasses

5. Conclusion

The results of ZnO doped in bismuth borosilicate glass samples with chemical composition :(5- x) Bi2O3x ZnO–10 B2O3–40 SiO2 proved that the density, molar volume and mass attenuation coefficient of glass samples were decreased along with increasing the concentration of ZnO, due to high molecular weight of Bi2O3 compared with ZnO. The FTIR spectra supported also the structural changes with composition. The UV–VIS transmission spectra of these glasses show that the system is transparent especially at concentration with ZnO =5 due to the formation of Zn2+ - O2-. So small amount of ZnO (~5%) is necessary to make the above glass system is transparent and good attenuating to γ-rays at the same time.

References

[1]  Sukhpal Prehar, Min Zi, Delvac Oceandy, Adam Pickard, Elizabeth Cartwright, Ludwig Neyses, Journal of Molecular and Cellular Cardiology, Volume 44, Issue 4, April 2008, Page 755.
In article      CrossRef
 
[2]  Murat Kurudirek, Yüksel Özdemir, Önder Şimşek, Rıdvan Durak, Journal of Nuclear Materials, Volume 407, Issue 2, 15 December 2010, Pages 110-115.
In article      CrossRef
 
[3]  S.R. Manohara, S.M. Hanagodimath, L. Gerward, Journal of Nuclear Materials, Volume 393, Issue 3, 15 September 2009, Pages 465-472.
In article      CrossRef
 
[4]  H.A. Saudi, A.G. Mostafa, N. Sheta, S.U. El Kameesy, H.A. Sallam, Physica B: Condensed Matter, Volume 406, Issue 21, 1 November 2011, Pages 4001-4006.
In article      CrossRef
 
[5]  Y.I. Alivov, D.C. Look, B.M. Ataev, M.V. Chukichev, V.V. Mamedov, V.I. Zinenko, Y.A. Agafonov, A.N. Pustovit, Solid State Electron., 48 (12) (2004), p. 2343.
In article      CrossRef
 
[6]  J.H. Hubbell, S.M. Seltzer. Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, Volume 213, January 2004, Pages 1-9.
In article      CrossRef
 
[7]  Pawan P. Singh, John H. Cushman, Dirk E. Maier, Chemical Engineering Science, Volume 58, Issue 11, June 2003, Pages 2409-2419.
In article      
 
[8]  F.G. Bianchini, L.D. Riu, G. Gagliardi, M. Gulielmi, C.G. Pantano, Glastech. Ber., 64 (8) (1991), pp. 205–217.
In article      
 
[9]  Tom O'Haver, Intro to Signal Processing-Deconvolution, University of Maryland at College Park, Retrieved, 2008.
In article      
 
[10]  Domingos De Sousa Meneses, Myriam Eckes, Leire del Campo, Cristiane N. Santos, Yann Vaills, Patrick Echegut, Vibrational Spectroscopy, Volume 65, March 2013, Pages 50-57.
In article      
 
[11]  Yufeng Chen, Gensheng Yu, Fei Li, Junchao Wei, Journal of Non-Crystalline Solids, Volume 358, Issue 15, 1 August 2012, Pages 1772-1777.
In article      CrossRef
 
[12]  G. Chryssikos, L. Liu, C. Varsamis, E. Kamitsos, J. Non-Cryst. Solids, 235 (1998), p. 761.
In article      CrossRef
 
[13]  Degang Deng, Hongping Ma, Shiqing Xu, Qian Wang, Lihui Huang, Shilong Zhao, Huanping Wang, Chenxia Li, Journal of Non-Crystalline Solids, Volume 357, Issue 5, 1 March 2011, Pages 1426-1429.
In article      CrossRef
 
[14]  M. Subhadra, P. Kistaiah, Vibrational Spectroscopy, Volume 62, September 2012, Pages 23-27.
In article      CrossRef
 
[15]  Nam Jin Kim, Young Hoon La, Sang Hyeok Im, Won-Tack Han, and Bong Ki Ryu, Electronic Materials Letters, Vol. 5, No. 4 (2009), pp. 209-212.
In article      
 
comments powered by Disqus
  • CiteULikeCiteULike
  • MendeleyMendeley
  • StumbleUponStumbleUpon
  • Add to DeliciousDelicious
  • FacebookFacebook
  • TwitterTwitter
  • LinkedInLinkedIn