characterization and phase evolution of cordierite based glass
Transcription
characterization and phase evolution of cordierite based glass
JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 30 CHARACTERIZATION AND PHASE EVOLUTION OF CORDIERITE BASED GLASS SYNTHESIS FROM PURE OXIDE AND MINERALS Banjuraizah Johar1, Hasmaliza Mohamad2, Zainal Arifin Ahmad2. 1 2 School of Materials Engineering, Universiti Malaysia Perlis School of Materials and Mineral Resources Engineering, Universiti Sains Malaysia Engineering Campus, 14300 Nibong Tebal [email protected] ABSTRACT α Cordierite is very important phase in MgO-Al2O3-SiO2 system because of their very outstanding thermal, chemical and electrical properties. In this presents study nonstoichiometry cordierite (MgO:Al2O3:SiO2 = 3:1.5:5) using 2 different initial raw materials ( (i)mixture of pure oxide, and ii) mainly mixture of minerals) were fabricated and compared in terms of phase transformation and physical properties. Cordierite was prepared by glass method at low melting temperature (1350oC). Low melting temperature has resulted in partly crystalline glass which has possesses higher hardness, required longer milling time and result in contamination from grinding media. However, α-cordierite has successfully crystallized and fully densified at 850oC/2h. Activation energy for densification was investigated from thermal expansion coefficient (TCE) results. Other properties that were discussed included thermal properties using DTA/TGA. ABSTRAK α Cordierite amat peringkat penting dalam sistem MgO-Al2O3-SiO2 disebabkan oleh mereka sangat terma cemerlang, kimia dan sifat-sifat elektrik. Dalam hadiah-hadiah ini mengkaji tidak stoikiometri kordierit (MgO:Al2O3:SiO2 = 3:1.5:5) menggunakan 2 bahan-bahan mentah permulaan berbeza ( (i) campuran oksida tulen, dan (ii) terutamanya campuran mineral) telah dibuat dan dibandingkan dalam syarat-syarat penjelmaan fasa dan sifat fizikal. Kordierit telah bersedia dengan kaca kaedah pada suhu lebur rendah (1350oC). Suhu lebur rendah telah menghasilkan dalam sebahagiannya kaca habluran yang telah memiliki kekerasan lebih tinggi, dikehendaki lebih panjang masa pengilangan dan mengakibatkan pencemaran daripada media pengisaran. Bagaimanapun, α-cordierite telah dengan jayanya mengkristalkan dan sepenuhnya densified di 850oC/2h. Tenaga pengaktifan untuk penumpatan telah disiasat daripada pekali pengembangan terma (TCE) keputusan-keputusan. Sifat-sifat lainnya yang telah dibincangkan termasuk sifat terma menggunakan DTA / TGA. Keywords: Nonstoichiometric cordierite glass ceramic, characterization, kaolin, talc, INTRODUCTION Indialite or α cordierite materials are extensively used in broad range of applications, including automobile exhaust systems, as substrate material for integrated circuit boards and as kiln furniture, carriers for purifying exhaust emission, filter for liquid at high temperature (Gonzalez-Velasco, Ferret, Lopez-Fonseca, & Gutierrez-Ortiz, 2005; Goren, Gocmez, & Ozgur, 2006; Shi, Liang, & Gu, 2001; Yalamac & Akkurt, 2006). There are several methods use to 237 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 syntheses α cordierite such as solid state reaction, sol-gel and crystallization from glass (Goren et al., 2006). Although many researchers was conducted to lower the sintering temperature of α cordierite either by mechanical activation before solid state reaction, combination of mechanical activation and sintering aids, or even by sol-gel methods using various precursor and various sintering aids, however only a few of them successful in decreasing the sintering temperature of α cordierite and the value of crystallization temperature is still above 1000°C. It is widely cited in the literature on the difficulty to produce dense α cordierite ceramic by solid state reaction because of its sintering temperature is near the incongruent melting point of α cordierite (1350oC). Recently, dense cordierite ceramics that were fired at <1000oC have been produced via glass crystallization method or via sol-gel method using alkoxide (Katsuhiro Sumi, Yuichi Kobayashi, & Kato, 1999). Lower sintering temperature (less than 1000°C) is necessary for electronic application packaging in order to be co-fired with copper (1083°C), silver (961°C), or gold (1061°C). Among these methods, crystallization of glass powders had much higher potential to decrease the sintering temperature of α cordierite to lower than 1000oC. Since there has been no report on synthesis cordierite from talc and kaolinite via glass method using non stoichiometric ratio (3:1.5:5) to produced α cordierite, therefore in the present investigation, α cordierite was synthesized from mainly talc and kaolin using glass crystallization method. As a comparison, α cordierite was also prepared using high purity metal oxide using the same stoichimetric and processing technique. Above stoichiometric have been proved by Chen et. al (Chen, 2008) can obtained single phase α cordierite at 950oC/2h and give better result in dielectric properties. Beside to compare the properties of cordierite glass ceramic from high purity oxide grade and mixture of minerals, the purpose of this work is to get general idea to setup experimental parameter in order to achieve low sintering temperature and high purity of α cordierite phase using mainly minerals talc and kaolin. METHODOLOGY The starting raw materials for oxides samples (Sample A) were MgO, Al2O3, SiO2, CaO, whereas, for second sample (Sample B), compositions were mainly from minerals talc and kaolin which has higher MgO, Al2O3 and SiO2 content. CaO, MgO, Al2O3, SiO2 were added in this second composition to compensate the chemical formulation. Composition of oxides for both samples was taken from Chen et. al (Chen, 2008). The stoichiometric composition used in this present work is 3MgO. 1.5 Al2O3. 5SiO2. The weight percent of minerals powder (Sample B) used was calculate base on chemical formulation of talc and kaolin. The homogenized mixture of raw ingredients was melted in alumina crucibles at 1500oC for 4 hours. The molten glass was quenched in distilled water to form frit. The frits were then crushed and dry milled for 6h using zirconia ball mill to obtain particle size with the average 1-3 μm. The glass powder than were sieved to less than 45 μm, followed by uniaxially pressing at 400 MPa to form a pellet with 10 mm diameter. Dimension and initial weight were recorded. The green pellets were then sintered at 850oC with heating rate of 5oC/min for 2 hours soaking time. The FSEM/EDX analyses were carried out in a VP FESEM-Supra 35VP microscope. The X-ray diffractometer diffraction (XRD) patterns of the milled products were obtained using a Bruker D8 Advanced operated in Bragg–Brentano geometry, with Cu Kα radiation, in the 10° ≤ 2θ ≤to 90° range. A differential thermal analyzer (DTA/TG) (Model Linseis) was used to record the themograms of codierite glass powder. During DTA/TG runs, the samples were heated from 25oC to 1000oC at heating rate of 5oC/min with α Alumina as reference. Thermal expansion coefficient were performed using Linseis dilatometer at heating rate 5oC/min in the temperature range room to 1000oC on sample 20 mm x 8 mm x 8mm pressed at 150 MPa. The 238 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 average linear expansion coefficient from 2 different ranges was calculated following usual method. RESULTS AND DISCUSSION Physical observation of glasses Sample from mineral precursor was green in color and appeared in opaque. Both samples seem to be partly crystalline and hard. However, sample from pure oxide is less glassy than sample from minerals. Based on the observation, it seems sample from pure oxide required high temperature for melting compared to sample from minerals. XRD pattern of glass sample as shown in Figure 1, clearly indicate that both samples are partly crystalline and sample A has higher crystalline phase compared to sample B. Figure 1: XRD pattern of glass powder. Diffraction pattern of sample A is a curve with black in color while sample B is a curve with red in color. Q-Quartz, O-olivine, C-α-cordierite Table 1: Phases present in heat treated samples Sample A Sample Phase present after sintering Amorphous, α cordierite, forsterite, zircornia-cubic, zircornia- monoclinic, zircornia-cubic Amorphous,α cordierite, forsterite, zircornia-cubic, 239 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 B zircornia- monoclinic, zircornia-cubic Crystallization behavior The XRD pattern of a crushed pellet sintered at various temperatures was properly indexed using standard JCPDS files. Figure 1 show XRD pattern for both glass samples after quenching and underwent intensive grinding for 6 hours. Figure 2 shows diffraction pattern of both type of cordierite glass heat treated at 900oC, and the results is summarized in Table 1. The X-ray diffraction measurements on the sintered samples clearly indicate that α cordierite (PDF#48-1600) as the prevailing phase along with a significant amount of forsterite (PDF#88-1000), zirconia-cubic (PDF#89-9069), zircornia tetragonal(PDF#89-9068),, and zircornia-monoclinic (PDF#89-9066). α cordierite has successfully crystallize at 850oC for both sample and glass crystallization method has been proved to be a method to synthesized α cordierite at such lower temperature. The intensity of diffraction peak for α cordierite is higher for sample A as compared to sample B. This indicates that the concentration of α cordierite is higher in sample A, compared to sample B. Forsterite phase was presence and not anorthite phase as what has been obtained by Chen et. al (Chen, 2008) using the same composition. The possibility of forsterite to crystallized is higher using this formulation (3MgO.1.5Al2O3.5SiO2), since excess MgO and less alumina from exact stoichiometric of cordierite (2MgO.2Al2O3.5SiO2) will cause excess MgO and SiO2 to react and form forsterite (MgSiO4). XRD pattern for both samples also indicate the presence of all three type of zircornia polymorph at 850oC. Zirconia that was presence in both samples coming from milling media. This contamination may come from wear mechanism which caused by collision between the powder and the ball. Due to partly crystalline the samples tend to be very hard. Hardness test was carried out to investigate the hardness of samples and zircornia ball. The results are tabulated in Table 2 indicates that the hardness of quenched sample is just slightly lower than the hardness of zircornia ball. Therefore, from this observation, we can decide that the sample should be melting at much higher temperature until fully glass phase is obtained. This is because the glass will exists in meta-stable state and has free energy higher than that corresponding crystalline phase of the same composition. In addition, during melting, the bonding between the atoms was disturbed and it may exist in a single atom or disordered form. Therefore it will be easy to break the sample. Secondly, milling media should be choose from hard and high wear resistance to avoid the presence of other phases from grinding media. 240 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 Figure 2: Comparison on XRD pattern between sample from pure oxide and minerals after heat treated at 900oC/ 2h. a-α cordierite, Fforsterite, M-zirconia monoclinic, t-zirconia tetragonal, c-zirconia cubic Table 2: The hardness of milling media and as-quenched sample. Zircornia glass from sample B Average Hardness, Hv (GPa) 9.725 8.665 DTA & TGA Figure 3 demonstrates DTA/TG results for both samples. Thermogravimetric analysis of all cordierite glass powders show three distinct temperature ranges of weight loss. The first weight loss occurred in the temperature range 30-200oC is due to removal of physically adsorbed water. The second weight loss appears in the temperature range 400-450oC is probably associated with the removal of chemical bonded water (Pal, 1996). It is clear from these results that sample B materials undergo greater weight loss on heating compared to sample A. Total percent weight loss for sample A when heated up 1000oC is about 2.4% while 4% for sample B. DTA scan of both samples show only single exothermic peak present in each sample. An endothermic peak signifying the glass transition temperature, Tg is not present in all thermograms under the condition of this experiment. The absence of an endothermic peak may result from the high activity of the fine glass powder (Kim, 1994). The exothermic peak indicates the crystallization of certain phase. The exothermal peak can be assigned to the 241 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 crystallization α cordierite. An intense and sharp peak corresponding to α cordierite has been observed in the diffragtogram of the powders obtained by heat treated the cordierite glass within that temperature. DTA results indicate that crystallization began between 865.3 and 886.9oC for sample A and between 842.9 and 879.8oC for sample B. This shows that the crystallization of α cordierite can be obtained at lower temperature when using mineral precursors compared to high purity of metal oxides. A B Figure 3: DTA/TG curves of glass powder (a) sample A and (b) sample B Microstructural characterization Figure 4 shows microstructure of both glasses. Sample B has low porosity than sample A, and likely more compact. This explain why sample B posses higher hardness compared to sample A, and as a result it tends to worn out at much higher degree. This indicates that why sample B has higher contamination from grinding media compared to sample A. EDX analysis that was done on glass sample as show in Figure 5, indicated that sample A is highly pure, whereas sample B contain carbon as impurities. Elemental composition of metal oxide on both samples also differed. Although chemical has been received as pure, detail characterization of kaolin and talc is necessary. Compositions design based on chemical equation between stoichiometric kaolin and talc has resulted in difference metal oxide contents in the sample. Figure 6 clearly shows that sample B has lower grain size as compared to sample A. 242 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 A B Figure 4: Micrograph of cordierite glass before milling showing dense structure a) sample A glass b) sample B A B Figure 5: EDX analysis of glass sample a) sample A b) sample B. 243 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 B A Figure 6: SEM micrograph etched sample a) sample A and b) sample B Coefficient of thermal expansion Dilatometry was performed to track the linear shrinkage of cordierite samples as a function of temperature with a heating rate 5oC/min. Table 3 present the results of the dilatometric test. Sample B shows negative TCE, while sample A gives TCE value equal to 5x10-8 oC-1 which is much lower from what commonly report for high purity α- cordierite (2x10-6 oC-1). This is may be due to existing of micro crack in the microstructure of sample. From dilatometry curve, large densification rate occurred at 735oC for sample B and 803oC for sample A. This is related to the formation of a glassy phase. The starting materials (kaolinite and talc) that were used to synthesized cordierite glass contains many impurities in which may contribute in decreasing the sintering temperature and increased the densification rate of cordierite. Densification occurs before the formation of α cordierite phase, as expected for reaction sintering process. This can be seen from DTA graphs where crystallization occurs at slightly larger than the densification temperature. Densification has occurred before the crystallization of cordierite, as expected for a reaction sintering process. This statement was confirmed through DTA and dilatometry analysis. The activation energy for densification, Q can be calculated from the shrinkage data on Figure 7a and 7b (in the temperature range 735-889oC for sample B and 803 to 907oC for sample A). A linear relationship of ln (ΔL/Lo T2) and T-1 was plot in Figure 7 to calculate activation energy. Results of linear thermal expansion coefficient and activation energy for densifications are shown in Table 3. From activation energy data, it can be concluded that sample B is more effective in enhancing the densification of the cordierite glass during the initial period of densification. Table 3: Result of CTE and activation energy for densifications. Activation energy for densification Sample Sample A (oxide) CTE o -1 (kJ/mol) -8 354 -1 oC-1x 10-7 269 5 C x 10 Sample B (minerals) 244 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 Figure 7: Dilatometric curve and plot of ln (dl/lo.T2 vs 1/T) 245 JOURNAL Of NUCLEAR And Related TECHNOLOGIES, Volume 6, No. 1, Special Edition, 2009 CONCLUSION α cordierite has been successfully synthesized using mainly minerals talc, kaolin with small amount of MgO, Al2O3 , CaO and SiO2 to compensate the formulation, and P2O5 and B2O3 as nucleating agent below 900oC. Therefore this sample has an ability to be co-fired with electrode such as Cu. It also has relative density higher than 90%, better hardness and negative cte. Microstructure reveal that micro cracks were physically observed in several samples, load for compaction of pellet should be decrease during compaction. Contaminations which come from grinding media exist due to the higher hardness of quenched glass. The glass is partly crystalline and therefore high melting temperature is needed to obtain fully glass so as to decrease the hardness of glass powder and consequently decrease the contamination from grinding media. Furthermore hardened milling media should be used to avoid this contamination. Further characterization of minerals talc and kaolin is necessary since EDX has demonstrated different metal oxide contents in both samples. ACKNOWLEDGEMENTS The authors gratefully acknowledge the financial supports from Islamic Development Bank (IDB) and Fundamental Research Grant Scheme (FRGS 9003-00171) Universiti Malaysia Perlis and technical assistants from Universiti Sains Malaysia (USM). REFERENCE B. H. Kim, K. H. L. (1994). Crystallization and sinterability of cordierite-based glass powders containing CeO2. J. Mater. Sci., 29, 6592-6598. Chen, G.-h. (2008). 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