Table of Contents
Indian Journal of Materials Science
Volume 2015 (2015), Article ID 638341, 8 pages
Research Article

Effects of M2+ (M = Ca, Sr, and Ba) Addition on Crystallization and Microstructure of SiO2-MgO-Al2O3-B2O3-K2O-F Glass

Glass Science & Technology Section, Glass Division, CSIR-Central Glass & Ceramic Research Institute, 196 Raja S. C. Mullick Road, Kolkata 700032, India

Received 27 May 2015; Revised 23 July 2015; Accepted 26 July 2015

Academic Editor: Maximina Romero Pérez

Copyright © 2015 Mrinmoy Garai et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


In understanding the effect of K+ substitution by M2+ (M = Ca, Sr, and Ba) on crystallization and microstructural properties of boroaluminosilicate glass system, the SiO2-MgO-Al2O3-B2O3-MgF2-K2O-Li2O-AlPO4 glasses were prepared by single-step melt-quenching at 1500°C. Density of base glass (2.64 g·cm−3) is found to be decreased in presence of CaO and SrO. is increased by 5–10°C and decreased by 13–20°C on addition of M2+. The variation of , and decrease of thermal expansion (CTE) from 7.55 to 6.67–6.97 (×10−6/K, at 50–500°C) in substituting K+ by M2+ are attributed to the higher field-strength of Ca2+, Sr2+, and Ba2+. Opaque mica glass-ceramics were derived from the transparent boroaluminosilicate glasses by controlled heat treatment at 1050°C (duration = 4 h); and the predominant crystalline phase was identified as fluorophlogopite (KMg3AlSi3O10F2) by XRD and FTIR study. Glass-ceramic microstructure reveals that the platelike mica flake crystals predominate in presence of K2O and CaO but restructured to smaller droplet like spherical shaped mica on addition of SrO and BaO. Wide range of CTE values (9.54–13.38 × 10−6/K at 50–800°C) are obtained for such glass-ceramics. Having higher CTE value after crystallization, the CaO containing SiO2-MgO-Al2O3-B2O3-MgF2-K2O-Li2O-AlPO4 glass can be useful as SOFC sealing material.

1. Introduction

The development of high temperature sustainable material is an archetypal challenge to materials science researchers since the last decade. Higher thermal expansion (CTE) value and good thermal shock resistivity are two foremost criterions for this purpose. Amongst various types of high temperature materials, mica, a kind of aluminosilicate based glass-ceramic with typical layer microstructure having component system Si-Mg-Al-K-O-F, proved its effectiveness. And, thus, the increase of CTE and shock resisting capability is of great interest for mica based glass and the corresponding glass-ceramics. Over controlled heat treatment, the glass based on SiO2-MgO-Al2O3-K2O-F system is converted to glass-ceramic containing fluorophlogopite mica (KMg3AlSi3O10F2) through the process of heterogeneous phase separation, precipitation of primary crystalline nuclei, and then the formation of metastable and stable phases from these nuclei [13]. Different nucleating agents like ZrO2, P2O5, ZnO, MnO, Fe2O3, Ta2O5, WO3, F, and so forth are used to facilitate this crystallization mechanism [2, 3]. Due to the replacement of ions by means of similar sizes and different properties, mica phase becomes the solid solution having uncertain chemical formula. The mica crystals possess excellent cleavage planes because of the weak attraction of alkali layers. Since the progression of crystallization in silicate based glass (predominated by Si-O-Si network) considerably depends upon the nature and composition of precursor material as well as thermal treatment, the addition of different alkaline earth metal ions can affect the crystallization characteristics and microstructural properties [412]. In addition, the alkaline earth ion plays significant role in controlling the glass transition temperature, softening point, thermal expansion, and density of aluminosilicate glass. Of particular interest is the proportion of nonbridging oxygen (NBO), which impacts significantly on the thermal and mechanical properties. In the study of binary, ternary, and quaternary silicates of CaO, BaO, and ZnO for applying as high temperature SOFC seals, Kerstan et al. [4] established that CTE of sealing glass is affected not only by the CTE of the crystalline phases but also by that of the residual glassy phase and sealing glass’s and glass-ceramic’s elastic properties. Tarlakov and his coworkers [5] investigated the effects of CaO addition on the glass structure and crystallization mechanism of Li2O-CaO-SiO2 system. They [5] argued that the increase of CaO content in glass matrix results in increasing the temperature interval of crystallization. Hamzawy and Darwish [6] established that the substitution of Ca for Mg in stoichiometric Na-fluorophlogopite decreases the glass transformation temperature and increases the crystallization range () and thermal expansion values. They [6] furthermore accomplished that the crystallization at CaO/MgO molar ratio = 0.25 in the base glass did not enhance the formation of Na-fluorophlogopite phase but catalysed the development of fluororichterite with cristobalite crystals. In ZnO-Al2O3-SiO2 based glass-ceramics, the addition of Ba2+ caused a structural change which renders the Si-O-Si network of the residual glassy phase in ceramic matrix more open than Ca2+ and Sr2+ [6, 7]. And the decrease in strength of glass phase network is attributed to dielectric loss. Additionally, the increase of nonbridging oxygen () and network strength (Si-O-Si) play significant role in controlling the physical and thermal properties. Yazawa and his coworkers [10] successfully prepared the alkali-resistant porous glass in SiO2-B2O3-ZrO2-RO system to ascertain the effects of MgO, CaO, SrO, BaO, and ZnO (RO). They [10] explored the effects of RO constituent to promote the phase separation in silicate based glass as CaO > SrO > BaO.

The present work is concerned to demonstrate the effect of MO (M = Ca, Sr, and Ba) addition substituting K2O on the crystallization characteristics, microstructure, and thermal properties of Li2O and AlPO4 containing SiO2-MgO-Al2O3-K2O-B2O3-F (SMAKBF) glass. We report the comparative study of MO addition in SMAKBF glasses by characterizing the techniques of dilatometry, XRD, FESEM, EDX, and FTIR spectroscopy.

2. Experimental

The SMAKBF glasses were prepared from the powders of SiO2 (Quartz Powder), Mg (OH)2 (97%, Loba Chemie, Mumbai, India), Al (OH)3 (97%, Loba Chemie, Mumbai, India), K2CO3 (98%, Loba Chemie, Mumbai, India), H3BO3 (99.5%, Loba Chemie, Mumbai, India), MgF2 (99.9%, Loba Chemie, Mumbai, India), LiCO3 (99.9%, Loba Chemie, Mumbai, India), AlPO4 (99%, Merck, Mumbai, India), CaCO3 (98%, Loba Chemie, Mumbai, India), SrCO3 (98%, Loba Chemie, Mumbai, India), and BaCO3 (99%, Merck, Mumbai, India) of high pure quality. The chemical compositions of the prepared glass samples are given in Table 1. Accurately weighed and homogeneously mixed (by ball milling for 1 h) batches were melted in a platinum crucible at 1500°C for 2 h. The melts were then cast into preheated graphite molds of the required dimensions. Resultant glass melts were immediately transferred into a furnace regulated at 620°C for annealing (to remove the internal stress generated during sudden cooling). Small piece of each annealed glass was then heat-treated at 1050°C (duration = 4 h) for controlled crystallization. Thermal properties such as coefficient of thermal expansion (CTE), glass transition temperature (), and dilatometer softening point () were evaluated by cylinder shaped sample with length ~25 mm and diameter ~6 mm using a horizontal dilatometer, NETZSCH DIL 402 PC (NETZSCH-Gerätebau GmbH, Germany), at a heating rate of 5°C/min under ±1% accuracy after calibration with a standard Al2O3 cylinder. Density () of different glass and glass-ceramic bulk samples was determined by the Archimedes principle using distilled water as immersion liquid. The crystallization characteristics and microstructural morphology of SMAKBF glass-ceramics (heat-treated at 1050°C/4 h) were examined using field emission scanning electron microscopy (FESEM model S430i, LEO, CEA, USA) using finely polished glass-ceramic specimens (chemically etched by immersion in 2 vol% aqueous HF solution for 5 min). The crystalline phases generated in SMAKBF glass-ceramics after heat treatment (1050°C for 4 h) were identified by X-ray diffraction (XRD) analyses as recorded using a XPERTPRO MPD diffractometer (PANalytical, Almelo, Netherlands) operating with Ni-filtered CuKα = 1.5406 Å radiation as the X-ray source at voltage ~40 kV and current ~40 mA. Crystalline phases were analysed in the 2θ range 5–90° with a step size of 0.05°at room temperature (~25°C). Heat-treated SMAKBF glass-ceramics were subjected to Fourier transformed infrared (FTIR) transmission spectroscopy recorded by a FTIR spectrometer (model 1615, Perkin-Elmer Corporation, Norwalk, CT) at a resolution of ±2 cm−1 after 16 scans in the wave number range 400–2000 cm−1. The FTIR analyses were done using the transparent thin pellet (prepared by uniaxial hydraulic press providing hand pressure ~10 tons) made by the mixture of KBr and SMAKBF glass-ceramic powder in an approximate volume proportion ~300 : 1.

Table 1: Composition (wt%) and dilatometric thermal properties of different precursor glasses.

3. Results and Discussion

Thermal properties, , , and CTE of SMAKBF glasses were evaluated by dilatometric study and represented in Figure 1. Thermal expansion (CTE) is calculated from the elongation data and the formula is written aswhere is the initial length and and are the difference in length and temperature of sample, respectively. For glassy material, thermal expansion value is increased with temperature and at glass transition point it increases very much due to considerable decrease in viscosity. As evident from Figure 1, the linear increase in CTE up to followed by sudden jump and then decrease after is displayed by all the SMAKBF glasses. For M-1 glass, the CTE value is evaluated as 7.11 and 7.55 × 10−6/K at 50–300 and 50–500°C, respectively. As seen from Table 1, CTE value decreased to 6.67–6.97 × 10−6/K at 50–500°C on addition of MO (M is Ca, Sr, and Ba) in place of K2O (5 wt%). The decrease in CTE can be attributed to the cationic field strength [/()2, where , , and are the charge of cation, radius of cation, and radius of anion, resp.] of the additive alkaline earth metals. When M2+ (M = Ca/Sr/Ba) having larger field strength (Ca2+ = 0.35, Sr2+ = 0.32, and Ba2+ = 0.27) than K+ (0.13) is added in the SiO2-MgO-Al2O3-K2O-B2O3-Li2O-AlPO4-F glass system, the strength of glass structure (controlled by Si-O-Si network) is increased, and, hence, thermal expansion value decreased. Density of M-1 glass is calculated as 2.64 g·cm−3. As seen from Table 1, and value of the SMAKBF glass are varied considerably on substituting K+ by Ca2+, Sr2+, and Ba2+. M-1 glass, containing 12 wt% MgO and 9 wt% K2O, possesses value 598°C. It is increased to 609, 603, and 609°C on addition of CaO, SrO, and BaO, respectively. In M-1 system, total glass modifier oxide content is 22 wt% (12 MgO + 9 K2O + 1 Li2O), where the alumina content is 16 wt% (16 Al2O3) and B2O3 = 10 wt%. When the total of Al2O3 and B2O3 content is almost balanced by modifier oxide, the all O atoms are in bridging approach, that is, Al-O-Al and B-O-B along with Si-O-Si. The addition of modifier oxide results in increase of nonbridging oxygen (NBO), which affects the stabilization of glass matrix to increase the glass transition range. After point, the structural relaxation occurring in Si-O-Si glass matrix caused the increase of CTE value exceedingly up to temperature. For M-1 glass, CTE value obtained at 50–700°C is 9.66 × 10−6/K and decreased on addition of MO. value obtained for M-1 glass is 677°C and decreased to 658, 662, and 664°C for M-2, M-3, and M-4 glasses, respectively, due to the decrease of electrostatic attraction. Potassium (K+), being the network modifier ion, binds together with silicate anions () by electrostatic force of attraction and hence effectively acts as ionic bridges between two kinds of nonbridging oxygen (NBO). The addition of CaO, SrO, and BaO replacing K2O results in reducing the electrostatic forces between the kinds of nonbridging oxygen (NBO) considerably and hence decreases the value of glasses [12]. Likewise , density of M-2 (CaO content) and M-3 (SrO content) glass is reduced and evaluated as 2.61 and 2.55 g·cm−3, respectively. It is somewhat increased on addition of BaO because of large atomic mass compared to CaO and SrO, because the cation size of Ba2+ is 33% larger than Ca2+, but mass of BaO (molecular weight = 153 g) is almost 3.4 times larger than CaO (molecular weight = 56 g).

Figure 1: Thermal expansion behavior of precursor SiO2-MgO-Al2O3-B2O3-K2O-Li2O-AlPO4–F glasses.

The crystallization characteristics of SMAKBF glasses have been intended by XRD technique in the 2θ range of 5–90°. The hump that appeared at around (2θ) 20−35° in Figure 2 confirms the amorphous nature of the present SiO2-MgO-Al2O3-B2O3-MgF2-K2O-Li2O-AlPO4 glasses. The transparent SMAKBF glasses were crystallized at 1050°C (for 4 h duration) to convert into opaque glass-ceramic (GC). The crystalline nature of four synthesized glasses is represented in Figure 3. As is evident from Figure 3, the two higher intense crystalline planes (001) and (003) are formed at 2θ = 8.82 and 26.72° for all the glass-ceramics. In addition, three low intense crystalline planes (200), (005), and (331) are developed due to phase reflections at 2θ = 34.14, 45.50, and 60.34°. All these crystalline planes appeared due to the formation of crystalline phase fluorophlogopite mica, KMg3AlSi3O10F2 (monoclinic end centered system, JCPDS file number 10-0494, molecular weight = 421.24, lattice parameter a = 5.299, b = 9.188, and c = 10.13), where the tightly bonded aluminosilicate sheets are weakly bonded together by large 12-coordinated K+ ions [12]. In presence of CaO, SrO, and BaO, crystalline peak intensity is increased (as seen from Figure 3) due to favorable crystallization owing to the large cationic field strength (cluster forming tendency). Two additional phase reflections at 28.25 and 30.87 (2θ) corresponding to (112) and (113) planes are observed for M-3 and M-4 glass-ceramics (Figure 3(c) and (d)). Development of this fluorophlogopite mica is composed of some crucial stages like amorphous phase separation, precipitation of primary crystalline nuclei, and the formation of metastable and stable phases from these nuclei [1, 2]. The primary nucleation phenomenon of SiO2-MgO-Al2O3-B2O3-MgF2-K2O-Li2O-AlPO4 glass is supposed to be the precipitation of F- and Mg-rich phase MgF2 on heating above annealing temperature (620°C). Ca2+, Sr2+, and Ba2+ having larger cationic field strength can form “cluster” to initiate heterogeneous phase separation. During the primary stage of crystallization event, very fine grained crystals of norbergite (Mg2SiO4·MgF2), MgF2, and mullite (3Al2O3·2SiO2) are developed [1, 2, 12, 13]. Further heating results in increasing the crystallization of mullite phase. And then a typical solid phase reaction of norbergite and mullite crystals with K2O-SiO2 glass takes place which finally results in producing two-dimensional fluorophlogopite mica crystalline phase. Increase in the quantity of mica crystals occurs on further heating and, at 1050°C, the randomly distributed mica crystal predominates in the ceramic matrix [12].

Figure 2: X-ray diffractogram of precursor (a) M-1, (b) M-2, (c) M-3, and (d) M-4 glasses (inset shows the photograph of transparent SiO2-MgO-Al2O3-B2O3-K2O-Li2O-AlPO4–F glasses synthesized by melt quenching).
Figure 3: XRD analysis of M-1 (a), M-2 (b), M-3 (c), and M-4 (d) glass-ceramics heat-treated at 1050°C for 4 h (inset shows the photograph of opaque glass-ceramics developed from SiO2-MgO-Al2O3-B2O3-K2O-Li2O-AlPO4–F glasses).

Thermal, optical, and mechanical properties are significantly changed when silicate based glass materials are converted into glass-ceramics. Amount, variety, shape, and packing of the crystalline phases developed in glass-ceramic matrix contribute significantly on the variation of these properties. In order to ascertain the change in microstructural morphology on substituting K+ by Ca2+, Sr2+, and Ba2+, the field emission scanning electron microscopy (FESEM) was done for SMAKBF glass-ceramics heat-treated at 1050°C. SMAKBF glasses are converted to glass-ceramics containing fluorophlogopite mica, KMg3(AlSi3O10)F2 crystalline phases predominately, which are mainly responsible for varying the thermal properties of present glass-ceramics. In Figure 4, the FESEM morphology of glass-ceramics (GC) heat-treated at 1050°C for 4 h is represented. Microstructure of the M-1 GC is exhibited in Figure 4(a), whereas Figures 4(b)4(d) depict the microstructure of CaO, SrO, and BaO (5 wt%) containing GCs, respectively. As is evident from Figure 4(a), M-1 GC is composed of some rodlike cylindrical shaped and some platelike fluorophlogopite mica [KMg3(AlSi3O10)F2] flake crystals randomly dispersed throughout the crystallized matrix. It possesses density value 2.66 g·cm−3 and thermal expansion (CTE) 8.69 and 13.38 × 10−6/K at 50–500 and 50–800°C, respectively. Alkali quantity (K2O) in M-1 glass is 9 wt%. As seen from Figure 4(b), 5 wt% CaO/K2O substitution results in the crystalline aggregation of smaller mica crystals, to develop longer platelike microstructure and, hence, homogeneous compactness. This compactness of microstructure caused its thermal expansion values to be reduced into 7.20 and 12.68 × 10−6/K at 50–500 and 50–800°C, respectively. Density of M-2 GC is calculated as 2.63 g-cm−3. The CaO has a bit tendency to substitute some K2O in the chemical formula of mica, K(Mg,Ca)3AlSi3O10F2. Mica belongs to the end centered cubic lattice and monoclinic system where several kinds of atoms can coexist. Thus, uniform nucleation is difficult to occur in the glass phase on heat treatment. In Figure 4(c), the microstructure of M-3 GC where 5 wt% K2O has been substituted by SrO is represented. There, the platelike mica crystals are broken into smaller droplet like micas and the droplet like mica crystals are agglomerated for endowing a compact microstructure. A large number of spherical particles, which are almost uniform in size (average particle diameter is about 200–400 nm), coexist there. Therefore, the thermal expansion value is reduced to 7.56 and 9.54 × 10−6/K at 50–500 and 50–800°C, respectively. Figure 4(d) depicts the microstructure of M-4 GC, where 5 wt% K2O is substituted by BaO. This microstructure is exceedingly different from others; 2–6 μm sized cylindrical shaped fluorophlogopite mica crystals are predominating in the matrix. Better fitted arrangement with mica crystals in this GC is responsible for higher density (2.68 g-cm−3) and lower thermal expansion value. At 50–500 and 50–800°C, CTE of M-4 GC is 7.23 and 10.91 × 10−6/K, respectively. Higher thermal expansion value (10.91–13.38 × 10−6/K) of M-1, M-2, and M-4 glass-ceramic makes them useful for high temperature vacuum sealing application with metal having higher thermal expansion coefficient.

Figure 4: FESEM photomicrograph of (a) M-1, (b) M-2, (c) M-3, and (d) M-4 glass-ceramic specimens (chemically etched by immersion in 2 vol% aqueous HF solution for 5 minutes) heat-treated at 1050°C for 4 h.

In Figure 5, the FTIR transmission spectra of SMAKBF glass-ceramics (GCs) are depicted in the wave number range of 400–2000 cm−1. The different bands appeared in Figure 5 and respective wave numbers are almost the same for all the SMAKBF GCs. Table 2 provides the different transmission bands and their respective band assignments. The transmission band centered at 477 cm−1 for all the GCs corresponds to Si-O-Si bending vibration for tetrahedral [SiO4] unit [1420]. Initial substitution of CaO in place of K2O strengthens the Si-O-Si network and hence glass structure. The addition of modifier oxide results in increase of nonbridging oxygen (NBO), which affects the stabilization of glass matrix controlled by Si-O-Si network. Higher ionic radius of Sr2+ and Ba2+ further decreased their cationic field strength, and so higher intense band appeared at 477 cm−1 for M-3 and M-4 GCs compared to M-1 and M-2. The transmission band at 612 cm−1 for M-2 GC is assigned to Al-O-Al stretching vibration of octahedral [AlO6] units [20, 21]. And the band peak position at 686 cm−1 is ascribed to Al-O-Al symmetric stretching vibration of 4-coordinated [AlO4] unit [1618]. Here, an interesting observation is the disappearance of the band at 612 cm−1 in M-3 and M-4 GCs. When 5 wt% K2O (of M-1 system) is substituted by CaO, octahedral [AlO6] units are developed. But the substitution by SrO and BaO results in converting the 6-coordinated [AlO6] units into 4-coordinated [AlO4] units due to higher atomic volume of Sr and Ba. The FTIR spectrum for all four GCs illustrates a characteristic band region at 990–1010 cm−1 which corresponds to Si-O-Si asymmetric stretching vibration of SiO4 unit [1418]. The band region is broadened due to the B-O stretching vibration of 4-coordinated [BO4] units which has also characteristic band at this region of 990–1010 cm−1. The sharp band at this wave number (990–1010 cm−1) for all the systems suggests that the glass structure is predominately controlled by silicate (SiO4) network and the addition of larger alkaline earth ion does not affect the network vibration considerably. In all the four SMAKBF GCs, the lower intense transmission band at 1280 cm−1 is attributed to Si-O-Si antisymmetric stretching vibration of [SiO4] unit. Another low intense band region at 1440 cm−1 is assigned to B-O symmetric stretching vibration of tetrahedral [BO4] units. In the spectrum of all investigated SMAKBF GCs, the characteristic band at 1630 cm−1 is due to H-O-H bending vibration of H2O molecule [21, 22].

Table 2: FTIR band position and assignment of different glass-ceramics heat-treated at 1050°C/4 h.
Figure 5: FTIR transmission spectra of glass-ceramics heat-treated at 1050°C for 4 h (see Table 2 for IR band assignments).

In Figure 6, the CTE trend of all SMAKBF GCs (heat-treated at 1050°C) is represented. The linear increase of CTE is seen for each SMAKBF GC although its value is decreased on addition of CaO, SrO, and BaO. Table 3 provides the CTE values in the temperature range of 50–300, 50–500, 50–700, 50–800, and 50–900°C. For mica based glass-ceramic materials, the thermal expansion is significantly dependent on nature and amount of crystalline phases and also microstructural arrangement. M-1 as prepared glass possesses thermal expansion value 7.11 × 10−6/K at 50–300°C. After heating at 1050°C, it is converted to glass-ceramic containing fluorophlogopite mica and so the CTE is increased to 8.35 × 10−6/K. With increasing the alkaline earth metal content (in place of K2O) in M-1 glass-ceramic, CTE value decreased due to the higher cationic field strength of M2+ ions. In SMAKBF system, the accumulation of glass modifier oxide results in increase of nonbridging oxygen (NBO), which affects the stabilization of glass-ceramic matrix to increase the thermal expansion value. CTEs obtained for M-2, M-3, and M-4 GCs are 6.71, 7.16, and 6.89 (×10−6/K), respectively, at 50–300°C (Table 3). In the temperature range 50–800°C, CTEs of M-1, M-2, M-3, and M-4 GCs are 13.38, 12.66, 9.54, and 10.91 × 10−6/K, respectively, which are higher due to the presence of fluorophlogopite mica. In the temperature range 50–900°C, CTE values are 9.47–13.57 × 10−6/K, and this wide variation can be attributed to the change in microstructural morphology. As seen from Figure 4(c), the compact interlocked type microstructure is developed in SrO containing GC and this is the reason of its lower CTE value. Higher thermal expansion (12.42–13.57 × 10−6/K at 50–900°C) of these (M-1 and M-2) GCs makes them efficiently useful for high temperature vacuum sealing application with metal. And the linear increase of CTE, obtained up to 900°C for SMAKBF GCs, indicates that these glasses are not liable for crack generation in a thermal recycling operation for high temperature application purpose (like SOFC). Figure 7 confirms the effectiveness of M-2 glass (CaO content = 5 wt%) as a good sealing material for solid oxide fuel cell (SOFC), as it has not fashioned any chemical reaction with SOFC interconnect material, Crofer 22 APU. The glass seal was not liable to any considerable chemical reaction with SOFC electrolyte, yttria stabilized zirconia (YSZ).

Table 3: Variation of CTE of different glass-ceramics heat-treated at 1050°C for 4 h.
Figure 6: Comparison of thermal expansion trend as a function of temperature of GCs heat-treated at 1050°C for 4 h (see Table 3 for detailed CTE values and inset shows the variation of density of glass-ceramics).
Figure 7: (a) FESEM photograph of glass to SOFC interconnect interface (with 10-micron scale bar) showing good bonding without any chemical reaction and (b) coupon cells prepared using YSZ electrolyte and M-2 glass seal.

4. Conclusions

In this study, 5 wt% K2O of 39SiO2-12MgO-16Al2O3-10B2O3-12MgF2-9K2O-1Li2O-1AlPO4 (wt%) glass is substituted by CaO, SrO, and BaO and the relevant alteration of thermal properties, crystallization pattern, and microstructure have been inspected to draw the following conclusions:(i)The glass transition temperature () is increased and dilatometric softening point () decreased on addition of CaO, SrO, and BaO substituting K2O (5 wt%).(ii)Transparent boroaluminosilicate glasses are converted into opaque glass-ceramics on controlled heat treatment at 1050°C and the predominant crystalline phase is identified as fluorophlogopite mica, KMg3AlSi3O10F2. The platelike fluorophlogopite mica flake crystals predominate in presence of K2O and CaO but changed to smaller droplet like spherical shaped mica on addition of SrO and BaO. CaO containing boroaluminosilicate glass seal provides good bonding with solid oxide fuel cell materials without any considerable reaction.(iii)Density trend of glasses and glass-ceramics increases in direction of BaO addition > base glass > CaO addition > SrO addition.(iv)Thermal expansion coefficients of precursor boroaluminosilicate glass samples in temperature range 50–500°C changed from 7.55 × 10−6/K to 6.67–6.97 × 10−6/K in presence of CaO, SrO, and BaO. For glass-ceramics, a wide range of thermal expansion values (9.54–13.38 × 10−6/K at 50–800°C) are obtained. The higher value of thermal expansion coefficients of CaO and BaO containing glass-ceramics makes them appropriate for high temperature vacuum sealing application with metal possessing large thermal expansion.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.


The authors thank Mr. Kamal Dasgupta, Acting Director, Dr. R. Sen, Head, Glass Division, and Dr. R. N. Basu, Head, Fuel Cell and Battery Division, for their encouragement and support to carry out this work. They thankfully acknowledge the CSIR-NMITLI funded project TLP 0005 for financial support. They are thankful to Dr. K. Annapurna for FTIR study, XRD and Electron Microscope Sections of this institute.


  1. D. G. Grossman, “Machinable glass-ceramics based on tetrasilicic mica,” Journal of the American Ceramic Society, vol. 55, no. 9, pp. 446–449, 1972. View at Publisher · View at Google Scholar
  2. W. Höland and G. H. Beall, Glass-Ceramic Technology, The American Ceramic Society, Westerville, Ohio, USA, 2002.
  3. H.-I. Hsiang, S. W. Yung, and C. C. Wang, “Crystallization, densification and dielectric properties of CaO-MgO-Al2O3-SiO2 glass with ZrO2 as nucleating agent,” Materials Research Bulletin, vol. 60, pp. 730–737, 2014. View at Publisher · View at Google Scholar
  4. M. Kerstan, M. Müller, and C. Rüssel, “Binary, ternary and quaternary silicates of CaO, BaO and ZnO in high thermal expansion seals for solid oxide fuel cells studied by high-temperature X-ray diffraction (HT-XRD),” Materials Research Bulletin, vol. 46, no. 12, pp. 2456–2463, 2011. View at Publisher · View at Google Scholar
  5. Y. P. Tarlakov, I. F. Es'kova, and A. M. Shevyakov, “Spectroscopic study of high silica glasses of the lithium oxide-sodium oxide-calcium oxide-silicon dioxide system,” Issled. Strukt. Sostyaniya Neorg. Veshchestu, vol. 1, pp. 7–10, 1974. View at Google Scholar
  6. E. M. A. Hamzawy and H. Darwish, “Crystallization of sodium fluormica Na(Mg, Zn, Ca)2.5Si4O10F2 glasses,” Materials Chemistry and Physics, vol. 71, no. 1, pp. 70–75, 2001. View at Publisher · View at Google Scholar
  7. S. N. Hoda and G. H. Beall, “Advances in ceramics,” Journal of the American Ceramic Society, vol. 54, p. 287, 1982. View at Google Scholar
  8. C. B. da Silveira, S. D. de Campos, S. C. de Castro, and Y. Kawano, “Preparation and characterization of glass-ceramic materials in the BaO-Li2O-ZrO2-SiO2 system and their dependence on treatment temperatures,” Materials Research Bulletin, vol. 34, no. 10, pp. 1661–1671, 1999. View at Publisher · View at Google Scholar
  9. P. W. McMillan and G. Partridge, “The dielectric properties of certain ZnO-Al2O3-SiO2 glass-ceramics,” Journal of Materials Science, vol. 7, no. 8, pp. 847–855, 1972. View at Publisher · View at Google Scholar
  10. T. Yazawa, H. Tanaka, K. Eguchi, and S. Yokoyama, “Novel alkali-resistant porous glass prepared from a mother glass based on the SiO2-B2O3-RO-ZrO2 (R = Mg, Ca, Sr, Ba and Zn) system,” Journal of Materials Science, vol. 29, no. 13, pp. 3433–3440, 1994. View at Publisher · View at Google Scholar · View at Scopus
  11. X.-M. Qin, X.-Y. Sun, Z.-M. Xiu, and L. Zuo, “Effects of ZrO2 on the microstructure of a mica glass-ceramic,” Chinese Journal of Structural Chemistry, vol. 23, no. 10, pp. 1111–1116, 2004. View at Google Scholar
  12. M. Garai, N. Sasmal, A. R. Molla, S. P. Singh, A. Tarafder, and B. Karmakar, “Effects of nucleating agents on crystallization and microstructure of fluorophlogopite mica-containing glass-ceramics,” Journal of Materials Science, vol. 49, no. 4, pp. 1612–1623, 2014. View at Publisher · View at Google Scholar · View at Scopus
  13. E. Ercenk and S. Yilmaz, “Crystallization kinetics of mica glass-ceramic in the SiO2-Al2O3-MgO-K2O-B2O3-F2 system,” Journal of Ceramic Processing Research, vol. 16, pp. 169–175, 2015. View at Google Scholar
  14. G. Kaur, M. Kumar, A. Arora, O. P. Pandey, and K. Singh, “Influence of Y2O3 on structural and optical properties of SiO2–BaO–ZnO–xB2O3–(10−x) Y2O3 glasses and glass ceramics,” Journal of Non-Crystalline Solids, vol. 357, no. 3, pp. 858–863, 2011. View at Publisher · View at Google Scholar · View at Scopus
  15. M. Garai, N. Sasmal, A. R. Molla, and B. Karmakar, “Structural effects of Zn+2/Mg+2 ratios on crystallization characteristics and microstructure of fluorophlogopite mica-containing glass-ceramics,” Solid State Sciences, vol. 44, pp. 10–21, 2015. View at Publisher · View at Google Scholar
  16. G. Fuxi, Optical and Spectroscopic Properties of Glass, Springer, Berlin, Germany, 1992.
  17. S. G. Motke, S. P. Yawale, and S. S. Yawale, “Infrared spectra of zinc doped lead borate glasses,” Bulletin of Materials Science, vol. 25, no. 1, pp. 75–78, 2002. View at Publisher · View at Google Scholar · View at Scopus
  18. S. P. Singh, K. Pal, A. Tarafder, M. Das, K. Annapurna, and B. Karmakar, “Effects of SiO2 and TiO2 fillers on thermal and dielectric properties of eco-friendly bismuth glass microcomposites of plasma display panels,” Bulletin of Materials Science, vol. 33, no. 1, pp. 33–41, 2010. View at Publisher · View at Google Scholar · View at Scopus
  19. J. Yu, X. Zhao, J. C. Yu, G. Zhong, J. Han, and Q. Zhao, “The grain size and surface hydroxyl content of super-hydrophilic TiO2/SiO2 composite nanometer thin films,” Journal of Materials Science Letters, vol. 20, no. 18, pp. 1745–1748, 2001. View at Publisher · View at Google Scholar
  20. P. Tarte, “Infra-red spectra of inorganic aluminates and characteristic vibrational frequencies of AlO4 tetrahedra and AlO6 octahedra,” Spectrochimica Acta Part A: Molecular Spectroscopy, vol. 23, no. 7, pp. 2127–2143, 1967. View at Publisher · View at Google Scholar
  21. M. Garai, N. Sasmal, A. R. Molla, A. Tarafder, and B. Karmakar, “Effects of in-situ generated coinage nanometals on crystallization and microstructure of fluorophlogopite mica containing glass-ceramics,” Journal of Materials Science & Technology, vol. 31, no. 1, pp. 110–119, 2015. View at Publisher · View at Google Scholar · View at Scopus
  22. N. Abd El-Shafi and M. M. Morsi, “Optical absorption and infrared studies of some silicate glasses containing titanium,” Journal of Materials Science, vol. 32, no. 19, pp. 5185–5189, 1997. View at Publisher · View at Google Scholar · View at Scopus