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| Influence of Fe2O3 on the physical, structural and electrical properties of sodium lead borate glasses |
| Safeya IBRAHIMa,Mohamed Mahmoud GOMAAb*,Hussein DARWISHa |
aGlass Research Department, National Research Centre, Dokki, Cairo, Egypt bGeophysical Sciences Department, National Research Centre, Dokki, Cairo, Egypt |
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Abstract The influence of adding Fe2O3 at the expense of Na2O in sodium lead borate glasses on the structural, physical and electrical properties have been investigated. Results obtained from Fourier transform infrared (FTIR) spectra indicated that Fe2O3 plays an important role in converting three coordinated boron atoms [BO3] to four coordinated boron atoms [BO4]. The physical properties such as density and molar volume helped to evaluate the compact structure of the prepared glass samples due to presence of [BO4] groups. The increase of Fe2O3/Na2O replacements led to increasing the microhardness values and decreasing the thermal expansion coefficients of the studied glasses. The increase of Fe2O3/Na2O replacements generally decreased the AC conductivity. That decrease might be due to converting of the three coordinated boron atoms [BO3] to four coordinated boron atoms [BO4]. Dielectric constants of the samples might be an indication of the distortion in the coordinated boron atoms. The obtained experimental data indicated the internal structure of glass network and the change of the structure of the samples from three [BO3] to four coordinated boron atoms [BO4].
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Received: 19 March 2014
Published: 12 June 2015
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Corresponding Authors:
Mohamed Mahmoud GOMAA
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A schematic representation of the sample holder.
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| Glass No. | Glass composition (mol%) | Density (g/cm3) | Molar volume (cm3/mol) | 〈dB–B〉 nm | Microhardness (kg/mm2) | | Fe2O3 | Na2O | PbO | B2O3 | | G1 | 0 | 25 | 25 | 50 | 3.6200 | 29.3106 | 0.3651 | 374 | | G2 | 5 | 20 | 25 | 50 | 4.0257 | 27.5703 | 0.3578 | 380 | | G3 | 10 | 15 | 25 | 50 | 4.2884 | 27.0207 | 0.3553 | 429 | | G4 | 15 | 10 | 25 | 50 | 4.4865 | 26.9166 | 0.3549 | 528 |
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Chemical composition, density, molar volume, average boron–boron separation and microhardness of the investigated glasses
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Composition dependence of density and molar volume for the studied glasses.
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Infrared transmission spectra of Fe2O3–Na2O–PbO–B2O3 glasses.
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| Glass No. | Tg (℃) | Ts (℃) | α at 25–300 ℃ (10-7℃-1) | Average coordination number (m) | Number of bonds per unit volume nb (1029m-3) | | G1 | 352 | 374 | 121 | 3.25 | 0.6677 | | G2 | 365 | 386 | 111 | 3.50 | 0.7645 | | G3 | 375 | 395 | 104 | 3.75 | 0.8357 | | G4 | 400 | 418 | 95 | 4.00 | 0.8949 |
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Glass transition temperature, dilatometric softening temperature, thermal expansion coefficient, average coordination number and number of bonds per unit volume of the glass samples
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Variation of thermal expansion coefficient of the glasses as a function of Fe2O3 content.
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Conductivity variation with frequency for samples G1 (◆),G2 (●), G3 (▲) and G4 (★).
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Dielectric constant variation with frequency for samples G1 (◆),G2 (●), G3 (▲) and G4 (★).
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Imaginary impedance variation with real impedance for samples G1 (◆), G2 (●), G3 (▲) and G4 (★).
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Cg and R∞ are the capacitance and resistance of the sample at high frequency, respectively; Ci is the interfacial capacitance and Ri is the interfacial resistance).">
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Equivalent circuit that represents the sample (Cg and R∞ are the capacitance and resistance of the sample at high frequency, respectively; Ci is the interfacial capacitance and Ri is the interfacial resistance).
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