Slag formation during high temperature interactions between refractories containing SiO 2 and iron melts with oxygen

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Slag formation during high temperature interactions between refractories containing SiO 2 and iron melts with oxygen E. Kapilashrami* 1, V. Sahajwalla 2 and S. Seetharaman 1 Refractory metal interactions and associated reactions are important during casting as they can lead to the formation of inclusions. High temperature interactions between aluminosilicate refractories and molten steel were studied in the present investigation using the sessile drop method. Changes in the contact angles between molten iron with well defined oxygen levels and substrates of silica, mullite (3Al 2 O 3.2SiO 2 ) as well as commercial refractories, were measured in the dynamic mode. In all cases, the reaction led to slag formation. The experiments were performed under isothermal conditions at 1823 and 1873 K. A known and constant oxygen partial pressure was imposed above the iron drop, through appropriate CO CO 2 Ar mixtures. For all substrates, the contact angles started decreasing due to lowering of the surface tension of iron, as oxygen was imposed onto the system. When a critical level of oxygen was reached, slag started forming at the drop/substrate interface and at this stage, the contact angle dropped suddenly. Subsequent behaviour of silica and mullite was observed to be different, with SiO 2 showing a non-wetting behaviour. In the case of SiO 2 substrate, there were also deep erosions along the periphery of the drops and there was slag accumulation at the sides of the metal drop, probably due to Marangoni flow and/or SiO (g) formation. SEM and EDS analysis of the substrates revealed that the formed slag was fayalite. The thermodynamic criteria for slag formation and possible mechanisms of the reaction are discussed in the light of the experiments. Keywords: Silica, Mullite, Fayalite, Corundum, Slag formation, Sessile drop I&S/1906 Introduction The present work was initiated aiming at an understanding of the reactions between refractories containing silica and liquid iron containing well defined amounts of oxygen. The work is of relevance to clean steel production, as refractory erosion products can be sources of non-metallic inclusions in the steel. Erosion of refractories by steel with slightly higher amounts of oxygen during the tapping of LD furnaces and erosion of refractory runners during ingot casting are process steps for which the present study is of relevance. As the refractories commonly in use are aluminosilicates, studies were undertaken of the reactions between molten iron containing oxygen, and SiO 2 as well as mullite. The reactions between the above mentioned refractories and iron containing oxygen are characterised by the formation of molten slag at the interface. Slag formation seriously affects the mechanism of refractory 1 Department of Material Science and Engineering, Royal Institute of Technology, 100 44 Stockholm, Sweden 2 School of Materials Science and Engineering, The University of New South Wales, Sydney, NSW 2052, Australia *Corresponding author, e-mail era@mse.kth.se reactions and thereby has serious implications for the performance and life of refractories. Thus, the present paper aims at an understanding of the implications of slag formation for refractory life from a fundamental viewpoint. The studies were carried out at microscale by a sessile drop technique, whereby the reaction was followed by visual observation of the drop images dynamically. Thermodynamic background To understand the nature of the reactions of slag formation, it is crucial to have an understanding of the thermodynamics of the reactions occurring between the refractory oxides and iron containing oxygen as well as with pure iron. As part of the present work, a thermodynamic study was carried out in which the stabilities of the various phases in the system Fe O Si were calculated using thermodynamic data from the literature. From this input data, a phase stability diagram, presented in Fig. 1, was constructed. Calculations showed that the two silicates likely to be formed in this system are orthosilicate and metasilicate. However, at steelmaking temperatures, only the orthosilicate or fayalite in liquid form will be stable. On the ß 2004 Institute of Materials, Minerals and Mining Published by Maney on behalf of the Institute Accepted 24 September 2004 DOI 10.1179/030192304225019379 Ironmaking and Steelmaking 2004 VOL 31 NO 6 509

1 Phase stability diagram for system Fe O Si other hand, as the system is cooled down, metasilicate can precipitate. The constructed phase stability diagram shows that Fe 2 SiO 4 would be formed if the oxygen content in the molten iron exceeded 0?1 wt-%. This is likely to happen during certain steelmaking steps where the oxygen potential in the slag is high. In the case of aluminosilicates, the reactions are a bit more complex. An examination of the phase diagram 1 of the system Al 2 O 3 SiO 2 reveals the formation of a very stable compound, mullite, with the formula 3Al 2 O 3.2SiO 2 as well as 2Al 2 O 3.SiO 2. The reaction and its Gibbs energy of formation 2 for the former compound are as follows 3Al 2 O 3 z2sio 2 ~3Al 2 O 3 :2SiO 2 DG1 0 ~18,779{26: 953 : (1) T J mole {1 As seen, the Gibbs energy of formation is very low and it is therefore reasonable to assume that this could be a predominant phase in the runner refractory. The reaction between molten iron containing oxygen and mullite could result in the formation of fayalite slag and hercynite (FeAl 2 O 4 ) particles. The reaction and the Gibbs energy of the formation 2 of fayalite are 2 : FezO 2 zsio 2 ~Fe 2 SiO 4 DG 0 2 ~{518,959z116: 82 : T J mole {1 (T range 1000{1400 K) At temperatures above the melting point of iron, the silica part of mullite will react with the metal and form fayalite. As mentioned previously, the ironmetasilicate being stable at lower temperatures would not be present in the system. The Gibbs energy of formation of solid hercynite, FeAl 2 O 4, is given by the equation 2 FezAl 2 O 3 z1=2 : O 2 ~FeAl 2 O 4 DG3 0 ~{328,349z82: 044 : (3) T J mole {1 The phase stability diagram of the Fe Al O system at steelmaking temperature was presented in earlier work. 3 When solid hercynite and liquid fayelite are formed, there is likely to be a reaction between these two and they will form a ternary slag that will have a composition that changes with temperature, according to the phase diagram FeO Al 2 O 3 SiO 4 2 presented in Fig. 2. The formation and composition of this slag will not just (2) 2 Phase diagram of system FeO Al 2 O 3 SiO 2 be dependent on the thermodynamics of the reactions but also on the kinetics of the reaction. Dynamic investigation experimental work In the present work, the reactions between substrate containing silica and iron drops containing oxygen were investigated at microlevel by means of the Sessile drop technique. The contact angle between substrates and iron containing varying amounts of oxygen were investigated in static and dynamic modes. Experiments were carried out in purified argon as well as with varying oxygen partial pressures imposed on the system by means of suitable mixtures of CO, CO 2 and Ar into the system. Details regarding the furnace, the gas cleaning system and the image recording device have been presented elsewhere. 5,6 The change in contact angle was followed as a function of time at different temperatures. The samples were heated in purified argon gas and the appropriate Ar CO CO 2 gas mixture was then introduced into the system after attainment of the experimental temperature. X-ray images of the drop along with the substrate were taken in the video mode, following the changes in contact angle over time. The experimental details, temperatures, gas ratios and the corresponding values of dissolved oxygen in molten iron, are presented in Table 1. At the end of the measurements, the Ar CO CO 2 gas mixture was replaced by purified argon gas and the sample was then quenched. The substrate was taken out and the crosssection examined by scanning electron microscopy (SEM) and also through energy dispersive spectroscopy (EDS). Some selected experiments were then repeated in order to confirm the reproducibility of the results. The contact angle between substrate and iron drop was evaluated using the video film and software developed at the Department of Material Science and Engineering, Carnegie Mellon University, USA complemented by an image analysis system developed at the Division of Metallurgy, Department of Material Science and Engineering, Royal Institute of Technology, Sweden. 510 Ironmaking and Steelmaking 2004 VOL 31 NO 6

3 X-ray images of sessile-drop at 1833 K at different time intervals after oxygen partial pressure of 1.5610 22 Pa imposed at zero time Results and discussion The experiments were carried out in pure argon gas as well as with different partial pressures of oxygen, the highest partial pressure corresponding to 0?19 wt-%o at 1823 K and 0?29 wt-%o as oxygen dissolved in molten iron at 1833 K, i.e. more than required to form fayelite slag according to the thermodynamic analysis. Results with silica substrate Images of the drops from the experimental series with the highest oxygen partial pressure and at 1833 K are presented in Fig. 3. It is seen that the drop flattens as the atmosphere is changed to gas mixtures with higher oxygen partial pressure, confirming thereby that the contact angle decreases due to the introduction of oxygen, which is surface active. An interesting observation in the present series is that the contact angle exhibits a tendency to increase after reaching a minimum point. A reasonable explanation for the initial decrease in contact angle would be the increase in surface oxygen concentration due to oxygen picked up from the gas phase. The oxygen from the surface has to diffuse into the bulk, which perhaps would account for the plateau region. Further decrease in the contact angle is indicative of the attainment of the equilibrium oxygen concentration at the metal/substrate interface and the progress of the reaction. At this point, the drop would also have reached the equilibrium oxygen content with respect to the gas phase and enough oxygen will be present in the system for fayalite slag to form. There is a likelihood of a thin fayalite layer formation between the substrate and the drop, which would arrest the reaction. At this stage, the contact angle measured would most probably be between the iron drop with oxygen potential equal to that of the gas phase and the thin 4 Photomicrograph of section of reacted drop and silica substrate after sessile drop experiments at 1833 and oxygen partial pressure, P O2 51.5610 22 Pa slag film on the silica substrate. This evidently is the fayalite slag formed by the following reaction: 2 : Fe (l) z2 : O (Fe,l) zsio 2(s) ~Fe 2 SiO 4(l) (4) Beyond this point, the iron drop showed a tendency to move from its original position. This behaviour is likely to be due to the imbalance in the forces acting on the drop. A similar phenomenon was observed by the present authors in the case of the dynamic contact angle measurements between liquid iron and alumina substrate. 3 A SEM micrograph of the reacted drop with the substrate after the experiment at 1833 K is presented in Fig. 4. The insert in the figure shows the location of the field of vision vis-à-vis the iron drop. The low contact angle between the drop and the substrate is quite evident in this figure. It is also seen that a thick product layer is formed by the side of the drop as mentioned earlier. The atomic ratio of iron to silicon in this layer, obtained by EDS was close to 2, confirming that this phase was indeed the fayalite slag. The figure, on higher magnification, showed clearly the formation of dendrites in the slag. These were found to be pure SiO 2 by EDS analysis. The SEM micrographs of the drops at other oxygen partial pressures and temperatures were found to be quite similar, the amount of slag decreasing with decreasing oxygen partial pressure. In some of the experiments, there was preferential corrosion observed along the periphery of the drop. This may be caused by the formation and evaporation of SiO, either due to direct decomposition of SiO 2 substrate at the low oxygen potentials prevailing in the gas phase or Table 1 Experimental sequences and their conditions Experimental series CO/CO 2 ratio Targeted P O2 Pa Corresponding ppm O Temperature, K A,10 214 1823, 1873 B 0.28/0.42 1.5610 22 2900 1873 B 0.28/0.42 1.5610 22 1960 1823 C 0. 42/0. 28 3. 0610 23 871 1823 D 0. 56/0. 14 9. 9610 24 327 1823 Ironmaking and Steelmaking 2004 VOL 31 NO 6 511

5 Photomicrograph of section of reacted drop and mullite substrate after sessile drop experiments at 1823 K and oxygen partial pressure, P O2 51.5610 22 Pa the reaction between silicon dissolved in the liquid metal and SiO 2 substrate, both reactions leading to the formation of SiO gas. These reactions would become dampened as the slag layer was formed around the bottom of the metal drop. Another plausible explanation is that the erosion is caused by Marangoni flow in the melt induced by differential surface tension due to concentration gradients. Results with mullite substrate The results observed in the case of mullite, namely the immediate decrease in contact angle with the introduction of gas mixture with high oxygen potentials, the somewhat steady state when oxygen diffuses from the surface of the drop to the bulk, and then the final slow drop in contact angle were similar to those of silica substrate. However, the slag formed during the reaction between mullite and molten iron would be different from that formed in the silica system. Thermodynamic analysis shows that when mullite and iron containing oxygen starts reacting, fayalite and hercynite will be formed. According to the ternary phase diagram presented in Fig. 2, the mullite, fayalite and hercynite will start to dissolve into each other and form a slag. The composition path of the slag will go towards mullite and an intermediate phase, iron cordierite, could be formed. At the experimental temperature, the ternary slag would consist of FeO Al 2 O 3 SiO 2, the final composition being marked as x in Fig. 2. If the reactions are allowed to continue, this slag will be in equilibrium with mullite and corundum. This is in agreement with the results of SEM- EDS analyses. However, due to the kinetics of the reactions, there could still be particles of iron cordierite and hercynite, as the reactions may not reach equilibrium. The composition of the slag would also change during cooling, and low temperature phases could precipitate, making the EDS analysis of the slag very complicated and difficult. An SEM micrograph of the reacted drop with the substrate after the experiment at 1823 K and the highest partial pressure of oxygen is presented in Fig. 5. Once again, the insert in the figure shows the location of the field of vision vis-à-vis the iron drop. It is seen that the drop has reacted with the substrate and has also sunk into it. It is also seen that a molten phase has been formed and that there are free particles in this phase. The slag phase, in the figure entrapped by the molten iron, was magnified and examined through EDS mapping and the result is presented in Fig. 6. It is seen that the slag mainly consist of alumina, silica and iron oxide. The particles are found to be alumina particles and at the periphery of these particles there is a layer containing aluminium, oxygen, and iron. This layer was found to be hercynite. The EDS mapping also shows that the composition of the slag varies. The present experimental work also showed that other factors, besides the composition of the substrate, have an impact on the reaction mechanism. Factors like inhomogeneity, surface roughness, and amount of pores are also of importance. Analysis of the porous mullite substrate revealed that, along with the surface reaction with the substrate, reactions were taking place downwards into the substrate, which could escalate slag formation and corrosion of refractories. The present work is of great importance for the steel industry, especially for steel plants targeting the production of clean steel. The results show that the composition of the refractory plays a significant role in corrosion of the furnace linings, resulting in slag formation, which, in turn, can result in the formation of non-metallic inclusions in the steel matrix. The 6 EDS mapping of slag formed during reaction between mullite substrate and molten iron containing oxygen 512 Ironmaking and Steelmaking 2004 VOL 31 NO 6

present work shows that silica, even though chemically bonded strongly in mullite, reacts with molten iron that contains some amounts of oxygen and forms a slag. The formation of a thin, dense, non-wetting hercynite layer between molten iron containing oxygen and alumina substrates shows the protective influence of the presence of higher alumina contents in the lining material, leading to less reaction with steel and thereby resulting in fewer nonmetallic inclusions. A distinct possibility to increase the life of furnace linings is to coat them with a non-wetting layer, for example, hercynite. This layer would act as a barrier between the refractory and the metal and it would prevent further reactions with the refractory. Of course, the economic gain in clean steel with these changes should be compared to the higher cost of refractory production. Summary The present work was focused on studying the slag formation phenomenon during reactions between molten iron containing oxygen and aluminosilicate lining materials by means of an X-ray sessile drop method. In the case of silica or mullite refractories, the reactions resulted in the formation of a slag. With silica substrate, the slag was found to be fayalite (2FeO.SiO 2 ). In the case of mullite, the slag phase formed contained alumina. The slag formation led to non-wetting conditions and the movement of the iron drop. Preferential corrosion of the silica refractory due to possible SiO evaporation or Marangoni convection was also observed in the present study. The factors that influence the corrosion of lining materials, apart from the chemical reactions, were oxygen content in the metal, porosity and surface roughness of the refractories. The present studies are expected to lead to the development of new generation refractories that are resistant to chemical attack by molten steel, thereby leading to less contamination of the steel produced by non-metallic inclusions. Acknowledgements Part of the work was carried out at in the University of New South Wales, Australia. Financial supports for travel to Australia from Brinell Centre, KTH and Axel Hultgrens Trust are gratefully acknowledged. This paper is based on a presentation at the 7th International Conference on Molten slags, fluxes and salts held in Cape Town on 25 28 January 2004. Reference 1. N. L. Bowen and J. W. Greig: J. Am. Soc., 1924, 7, 242. 2. I. Barin: Thermodynamical data of pure substances, Part I and II, 1993, VCH. 3. E. Kapilashrami, A. Jakobson, A. K. Lahiri and S. Seetharaman: Metall. Mater. Trans. B, 2003, 34B, 193 199. 4. E. M. Levin, C. R. Robbins and H. F. McMurdie: Phase diagrams for ceramists, (ed. M. K. Reser), 696; 1964, Ohio, The American Ceramic Society. 5. E. Kapilashrami, A. K. Lahiri, A. W. Cramb and S. Seetharaman: Metall. Mater. Trans. B, 2003, 34B, 647 652. 6. E. Kapilashrami, V. Sahajwalla and S. Seetharaman: ISIJ Int., 2004, 44, 653 659. Ironmaking and Steelmaking 2004 VOL 31 NO 6 513