JMRTEC-1037; No. of Pages 8
ARTICLE IN PRESS j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Available online at www.sciencedirect.com
www.jmrt.com.br
Original Article
Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag Jiaqi Song a , Yongjie Liu a , Xueming Lv a , Zhixiong You a,b,∗ a
College of Materials Science and Engineering, Chongqing University, Chongqing 400044, China Chongqing Key Laboratory of Vanadium–Titanium Metallurgy and Advanced Materials, Chongqing University, Chongqing 400044, China
b
a r t i c l e
i n f o
a b s t r a c t
Article history:
Alumina–based refractory is widely used as lining material of rotary hearth furnace (RHF)
Received 15 September 2019
in the direct reduction process. However, corrosion of refractory by the burden is a cru-
Accepted 25 October 2019
cial problem which affects the RHF production. In this study, a sessile drop technique
Available online xxx
was used to investigate the wetting and corrosion behavior of Al2 O3 substrate against SiO2 –MgO–FeO–CaO–Al2 O3 slag, whose composition was determined according to the slag
Keywords:
obtained from smelting nickel laterite in the RHF process. The experimental results showed
Corrosion behavior
that the slags with basicity ((MgO + CaO)/SiO2 ) of 0.43 and 0.63 had a low apparent contact
Wetting
angle of approximately 25◦ and 30◦ , respectively. It indicated the slag samples could wet
Al2 O3 substrate
well on the Al2 O3 substrate. The spreading of slag on the substrate was mainly ascribed to
Apparent contact angle
the decrease of surface tension at the initial stage. As the wetting process proceeded, Al2 O3 dissolved into the slag forming an interfacial layer which gradually covered the substrate
Slag.
surface under the droplet and inhibited further dissolution of Al2 O3 . Good wettability and the dissolution of Al2 O3 are two main factors that caused the corrosion of substrate. Separating the burden from the Al2 O3 substrate was restrained after cooling, which would possibly bring severe sticking problems between the burden and alumina refractories. © 2019 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
1.
Introduction
Nickel plays an important role in modern manufactures. It is one of the essential elements for stainless steel production, which accounts for 65 wt% of the nickel consumption [1,2]. In recent years, the world annual demand for nickel has increased tremendously due to soaring stainless steel production [3,4]. Nickel sulfide and laterite ores are two main
resources for extracting nickel. With continuous consumption of high–grade sulfide resource, the use of nickel laterite has drawn increasing attention [5,6]. China is short of nickel resource, and has depended on importation for a long period. Utilizing low–grade nickel laterite is regarded as a main solution of the increasing demand for ferronickel alloy production. However, the extraction of nickel from laterite ore is relatively difficult because of the low Ni content and nickel mainly exists as isomorphic substitution in serpentine.
∗ Corresponding author at: College of Materials Science and Engineering, Chongqing University, No. 174 Shazhengjie, Shapingba District, Chongqing 400044, China. E-mail:
[email protected] (Z. You). https://doi.org/10.1016/j.jmrt.2019.10.060 2238-7854/© 2019 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license (http:// creativecommons.org/licenses/by-nc-nd/4.0/).
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
2
ARTICLE IN PRESS j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Rotary kiln–electric furnace (RKEF) process is one of the main pyrometallurgical technologies to deal with nickel laterite ore [7–9]. An alternative route of direct reduction–physical separation has also been widely studied [10,11]. The ferronickel alloy obtained from physical separation is considered as superior material for manufacturing stainless steels. For example, Nippon Yakin Kogyo Co., Ltd. has employed the above route by reduction in a rotary kiln and then followed by magnetic/gravity separation [12]. However, this process still requires a relatively high temperature and long reduction time for partially melting of the matrix. The formation of ring inside the kiln is still an intractable problem during the reduction process. Besides, lots of additives, such as sodium sulfate, calcium sulfate, etc., were added to enhance the reduction of laterite ore as well as the aggregation of ferronickel particles [13]. Recently, non–electric process with simple technological flow and low energy consumption becomes great potential in the production of ferronickel from laterite ore. In the last decades, non–blast furnace ironmaking processes applying rotary hearth furnace (RHF) technology have made huge progress. Representative processes included ITmk3, DryIron, Inmetco, FASTMET, and Redsmelt [14]. In particular, ITmk3 process is regarded as the most promising technology in which the RHF was used to produce iron nugget directly from iron ore [14–16]. The RHF process was also alternative to directly produce ferronickel nugget from nickel laterite ore. In the RHF process, nickel laterite ore pellets containing reductant were placed on the bed of alumina–based refractory lining, and heated from room temperature to 1400 ◦ C for about 30 min. During the reduction process, nickel and iron oxides were reduced to metallic state while the gangue minerals entered into the slag. As the slag melted, it would wet on the lining and even corrode the refractory. Alumina–based refractory is widely used as lining material due to its good corrosion and dissolution resistance. The corrosion behavior of high–alumina refractories has been intensively investigated [17]. Various slags, such as synthetic CaO–Al2 O3 , CaO–Al2 O3 –SiO2 systems and industrial slags, etc., have been employed to study the corrosion behavior [17–19]. The corrosion process generally included the dissolution of alumina and the precipitation of phases with high melting point. In contrast, the properties of alumina–based refractories on the corrosion resistance has also attracted increased attention. The study by Fu et al. indicated that the apparent porosity and pore size have pivotal impact on slag resistance [20]. The slag penetration and corrosion would also relieve after incorporating reinforced phases (such as magnesiaalumina spinel, nano-silica, and so on) into the refractories or castables [21–24]. With respect to the corrosion mechanism, the corrosion of refractories was mainly resulted from a reactive transport mechanism in many cases. The corrosive species (slag or gas) firstly impregnate the open porous space preferentially within the matrix and react with the material. The reactions usually proceed via a dissolution–precipitation mechanism [25,26]. Actually, no matter reducing in the RHF process or rotary kiln, the corrosion and sticking phenomena between molten slag and furnace refractory lining are the crucial problems.
The life of refractories and the stability during discharging would be affected severely if the refractories were eroded by the slag. However, few studies have been carried out to investigate the corrosion behavior of refractory lining by the slag from smelting nickel laterite ore. In order to simulate the RHF process, in this study, the wetting and corrosion behaviors of SiO2 –MgO–FeO–CaO–Al2 O3 quinary slag on Al2 O3 substrate were investigated by the sessile drop method. The pre–melted slag was placed on Al2 O3 substrate and heated from room temperature to the desired temperature. The microstructure of interface between the slag and Al2 O3 substrate was analyzed. Then the corrosion mechanism of slag samples with different basicity were also discussed.
2.
Experimental
2.1.
Preparation
Pure grade reagents (Kenong Chemical Co., Inc.) were used and pre–melted to prepare the slag samples for the wetting experiments. In order to improve the grade of Ni in ferronickel nugget, the reduction of iron oxides was restricted and part of iron remained as wustite (FeO) in the slag during reduction roasting. The chemical composition of the slag samples, which simulate the components of laterite ore after smelting in RHF process, is shown in Table 1. The content of FeO was fixed as 10 wt%, and the basicity ((MgO + CaO)/SiO2 ) given by weight ratio was set at 0.43 and 0.63, respectively. According to the quinary phase diagram of CaO-MgO-SiO2 - Al2 O3 -FeO [27], it can be observed that the basicity located at the low-melting ˜ field is in the range of 0.430.83. Higher basicity means greater amount of CaO should be added in the melting process. Thus the slags with basicity of 0.43 and 0.63 were compared in this study. Before the wetting experiment, pure reagents were weighed according to the above proportion and mixed manually, 10 g of the mixture was pressed into a cylindrical briquette (20 mm) using a uniaxial hydraulic presser with 10 MPa pressure. The briquettes were then loaded in platinum crucible and pre–melted in an electric resistance furnace by roasting at 1500 ◦ C for 2 h. The slag samples were totally melted into liquid state under Ar atmosphere. After melting, the slags were naturally cooled to room temperature in the furnace under Ar atmosphere. Cubic slag samples with 3 mm × 3 mm × 3 mm in dimension and approximately 60 mg in weight were then incised from the cooled slag and used for wetting experiment. The Al2 O3 substrate used in this experiment was 20 mm × 20 mm × 5 mm in dimension, and 99 wt% in purity. The porosity of substrate is 2.7% [28]. A smooth surface is important to achieve an accurate measurement of wettability behavior [29]. To obtain a smooth surface, the Al2 O3 substrate was smoothed with abrasive paper (400, 600, 800 and 1200 CW successively) and polished with diamond paste. The average surface roughness of the polished substrate was approximately 300–500 nm measured by a microscope (Boyue Instruments Co. Ltd., Dektak 150). The slag samples and Al2 O3 substrate were cleaned with acetone (≥99.5 wt%) using an ultrasonic wave cleaner and prepared for wetting experiment.
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
ARTICLE IN PRESS
JMRTEC-1037; No. of Pages 8
3
j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Table 1 – Chemical composition of the slag samples (mass% and mole%). Slag A
Basicity
Proportion, %
SiO2
CaO
MgO
Al2 O3
FeO
0.43
mass mole mass mole
57.47 54.02 50.96 48.82
2.53 2.55 12.43 12.76
22.19 31.28 19.67 28.26
7.81 4.32 6.94 3.91
10.00 7.83 10.00 6.25
0.63
B
Specimen
Fexible connector Thermo-couple
Stainless-steel tube Molten droplet
Alumina tube
Mo reflector He-Ne laser
High-resolution digital cameras
Tantalum heater
Evacuating pump system Substrate Lifting system
Band-pass filter
3.
Results and discussion
Ar gas
3.1.
Change in contact angle
Computer
Fig. 1 – Schematic diagram of the apparatus for wetting experiment.
2.2.
K␣, tube current and voltage: 250 mA, 40 kV, scanning range: 10◦ –90◦ (2), step size: 0.02◦ (2) and scanning speed: 8◦ /min. The microstructure of the cross–section between the slag and substrate was examined by scanning electron microscopy (SEM, Evo18, Carl Zeiss, Germany). The solubility of Al2 O3 in the specified slag samples was calculated by the software of FactSage 6.2 under the conditions of 1400 ◦ C and 1 atm. The quinary phase diagram was also calculated by FactSage 6.2 under 1 atm.
Methods
In order to simulate the RHF process, in this study, the wetting behavior of quinary slag on Al2 O3 substrate was investigated by the sessile drop method. The slag sample was firstly placed on the Al2 O3 substrate at room temperature. High temperature–vacuum furnace was used in the wetting experiment. The schematic diagram of apparatus is shown in Fig. 1. The furnace chamber was evacuated to 7 × 10–4 Pa by molecular pump to expel the air. High pure argon gas (99.999%) was charged and the furnace chamber was controlled at approximately 1.05 atm during the experiment. All the experiments were carried out under high purity argon to prevent the oxidation of FeO. In the RHF process, the duration of pellets in high temperature reduction zone is about 10 min, and hence in this study, the furnace was then heated to 1200 ◦ C at 60 ◦ C/min and to 1400 ◦ C at 20 ◦ C/min. The changes in drop profiles were recorded continuously by high–resolution (2000 × 1312 pixels) digital camera to reflect the change in contact angle. Laser was used to irradiate the sample for obtaining clear and distinct images of the slag. Surftens43 software with an accuracy of ±1◦ was used to facilitate the calculation of appearance contact angle [28,30]. Each experiment was repeated at least once, and the results were regarded as credible if the relative error was less than 5%. The average of two reproducible runs was regarded as the final results. The slag samples together with the substrate after wetting were cooled down naturally and then prepared for subsequent analyses. The slag samples were separated manually and analyzed by X–ray diffraction using a diffractometer (XRD, RIGAKU D/Max 2500PC, Japan) under the conditions as follows: Cu
The profile of SiO2 –MgO–FeO–CaO–Al2 O3 slag droplets on Al2 O3 substrate at different temperatures is shown in Fig. 2. The apparent contact angle () was measured from these images. For each droplet in view, the contact angle on both edges was measured and the average value was defined as the instant apparent contact angle. Fig. 3 shows the change of apparent contact angle as a function of temperature. When the slag samples started to melt, the contact angle decreased distinctly with increasing temperature. Both of the slags quickly spread along the Al2 O3 substrate and gradually approached to equilibrium where the contact angles were almost unchanged at temperatures above 1360 ◦ C. The equilibration apparent contact angles were determined as approximately 25◦ and 30◦ for the slags with basicity of 0.43 and 0.63, respectively. The results in Figs. 2 and 3 indicate that the slag samples wet well on Al2 O3 substrate at 1400 ◦ C. Good wettability would possibly bring sticking problems between pellet and alumina refractory in RHF process. The slag formed during reduction roasting process would wet and even erode the alumina refractory materials, which will bring adverse impact on the RHF process.
3.2.
Mineralogical composition of slags
The XRD patterns in Fig. 4 show the phase composition of slags A and B, which were separated from the substrate after cooling to room temperature. The obvious amorphous diffraction was mainly attributed to the fast cooling rate (60 ◦ C/min) after wetting experiment. The results reveal that various silicates including Mg2 SiO4 , MgSiO3 , Fe2 SiO4 and FeSiO3 were formed in both slags A and B. More calcium–containing phases (ie. CaAl2 Si2 O8 ) were observed in slag B due to its higher amount of CaO. Besides, a small amount of forsterite (Mg2 SiO4 , MgSiO3 ) was transformed into monticellite (MgCaSiO4 ). The phase composition will be further discussed according to the phase diagram in Sec. 3.4.3.
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
4
ARTICLE IN PRESS j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Fig. 2 – The change of the slag sample profile as a function of temperature.
Fig. 3 – The relationship between apparent contact angle and temperature.
3.3. Microstructure and elemental distribution analyses The microstructure of the slag–substrate interface after wetting experiment was investigated by SEM–EDS analysis. Figs. 5 and 6 show the morphology of different regions for slags A and B, respectively. The slag–substrate sample after corrosion was incised vertically and the microscopic morphology is shown in Fig. 5(a). A schematic diagram of the sample after wetting is shown in Fig. 5(a ). It can be seen from Fig. 5 that the microstructure can be divided into three layers, layer I is the slag, layer II is interfacial layer and layer III represents the original Al2 O3 substrate. The thickness of the interfacial layer is about 10 m. The results of line scanning in Fig. 5(b) reveal the distribution of the main elements. It indicates that the contents of Mg gradually decrease from layer I to III, while the Al content exhibits an opposite change. It is evident that the phases of Mg would diffuse from the slag towards the interfacial layer, while Al2 O3 was dissolved and Al ion diffused from the substrate to the interfacial layer. Regarding the slag with basicity of 0.63, the distribution of main elements was observed to be similar with that of slag A, as shown in Fig. 6. The chemical composition of EDS results (mole%) is plotted in Table 2. The EDS analysis indicates that the chemical com-
Fig. 4 – X–ray diffraction patterns of slags A and B after wetting experiment.
position of spot 1 (layer I) in either Figs. 5 or 6 is closed to the original components of slag samples. According to the XRD results in Sec. 3.2, the slags may consist of calcium silicates, forsterite (Mg2 SiO4 ) as well as fayalite (Fe2 SiO4 ) after crystallization. The comparison of Ca atom percentage of spot 1 in Figs. 5 and 6 is also in accordance with original components. The EDS results of spots 2 and 3 which were located at the interface layer II revealed Al and Mg were the main components. The contents of Si was far less than that of spot 1 while Al was obviously higher. It can be predicted that magnesium aluminate spinel may be formed in the interface layer. By comparing the Al atom proportion in layer II, it is found that the Al content of slag basicity 0.63 is a little higher than that of basicity 0.43. It can be deduced that higher basicity would result in heavier corrosion on the substrate.
3.4.
Discussion on the corrosion mechanism
3.4.1.
The change of surface tension of the slag
Surface tension, an important parameter of surface property, is directly related to the wetting phenomenon. Zisman et al. [31] reported that the degree of wetting improves with decreasing surface tension. T. Young [32] has studied the theories of surface tension and capillarity. On the basis of those theories, he asserted that a tension equilibrium exists at the inter-
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
ARTICLE IN PRESS 5
j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Fig. 5 – SEM–EDS results of the sample from slag A–Al2 O3 substrate.
Fig. 6 – SEM–EDS results of the sample from slag B–Al2 O3 substrate.
Table 2 – Chemical composition of the EDS results (mole%). Slag
A
B
Spot
SiO2
CaO
MgO
Al2 O3
FeO
1 2 3 1 2 3
55.00 8.44 8.78 47.81 8.51 9.13
2.58 4.48 4.80 18.86 7.20 6.98
31.88 34.62 33.31 22.21 29.60 29.67
2.56 45.82 46.69 2.20 48.77 48.75
7.98 6.63 6.42 8.93 5.92 5.47
face of solid/liquid/gas during wetting equilibrium, namely s/g = s/l + l/g ·cos (Fig. 5(a’)). In the present wetting experiment, the interfacial tension of solid/gas phase ( s/g ) was kept constant, s/l can be neglected as it was much less than l/g , and l/g was very close to the surface tension of the liquid ( l ) measured in vacuum [32]. Thus, l could be considered as
the major factor that affected the value of (apparent contact angle). A model developed by Mills et al. was widely used to estimate the surface tension of the molten slag system [33]. Surface tension in the model is a function of temperature and chemical composition of the slag. The surface tension as
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
6
ARTICLE IN PRESS j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
be also attributed to the formation of high melting phases in the interfacial layer.
3.4.3.
Fig. 7 – Surface tension of slags A and B as a function of temperature.
a function of temperature is calculated based on the above model and presented in Fig. 7. The value below 1360 ◦ C was not calculated because solid particles were still existed in the briquette. As shown in Fig. 7, the surface tension of both slags A and B decreased slightly with increasing temperature. According to the results in Fig. 3 and Fig. 7, it can be observed that the surface tension of slag A is smaller than that of slag B regardless of temperature, which was in consistent with the results that the equilibration contact angle of slag A was smaller than that of slag B.
3.4.2.
The dissolution of Al2 O3 into the slag
As can be seen from Figs. 5 and 6, the amount of Mg, Al and Si was quite different between layers I and II. It is probably attributed to two reasons. The first one is the diffusion of Mg and Si towards the Al2 O3 substrate, and the other one is the dissolution of Al2 O3 into the slag. The solubility of Al2 O3 in the specified slag samples calculated (1400 ◦ C, 1 atm) by FactSage 6.2. It is found that the content of Al2 O3 was as high as 23.8 wt% and 21.8 wt% when Al2 O3 was saturated in slags A and B, respectively. Compared to the original Al2 O3 contents of slag samples, it indicated that the content of Al2 O3 in slags A and B was far from saturating, which means Al2 O3 in the substrate will dissolve into the molten slag. In the study of Choi et al [34], the authors discussed the dissolution rate of Al2 O3 into molten CaO–SiO2 –Al2 O3 slag. It was found that the dissolution rate was dependent on the temperature, CaO content as well as the viscosity and diffusivity of slag [20,35]. Meanwhile, the diffusion of Mg, Si as well as the dissolution of Al2 O3 may be inhibited due to the formation of layer II. The Al2 O3 substrate would not be further corroded by the slags as high melting point phases was formed in layer II. Yu et al. [28] have studied the wetting behavior of Al2 O3 substrate by calcium ferrite (CF) series melts, and they found that the interface structure and products of the CF–2 M (calcium ferrite melt with 2 wt% MgO) differed from those of the other slag systems (CF–2S (2 wt% SiO2 ), CF–2A (2 wt% Al2 O3 )). No obvious corrosion phenomenon was observed by CF–2 M slag, which may
The crystallization process after wetting
In the RHF process, the reduced pellets will be discharged at about 1000 ◦ C after reduction. That is to say, as the wetting was finished, the semi–molten slag will crystallize, which can be analyzed according to the quinary phase diagram in Fig. 8. The diagram was calculated by fixing the contents of CaO and FeO. The sum of other three phases (SiO2 , MgO, Al2 O3 ) were 100%. Point O represents the original composition according to that in Table 1 (slag A). Assuming that the dissolution of Al2 O3 only affected the composition of interfacial layer, it can be deduced that the main body of slag crystallized along the direction of O→A→B. Thus, MgSiO3 , SiO2 and Mg2 Al4 Si5 O18 were expected to be formed in the final product. However, other phases, such as fayalite and calcium alumino–silicate, were observed in the XRD patterns. This may be attributed to the reason that the cooling process was in non–equilibrium condition and the slag was not uniform after crystallization. With respect to the interfacial layer after Al2 O3 was dissolved, the composition of the molten slag will transfer in the direction of O→C (towards the position of Al2 O3 ) depending on the dissolution rate of Al2 O3 . If the composition was transferred into the preliminary crystallization region of Mg2 SiO4 or Mg2 Al4 Si5 O18 , the phases of MgSiO3 , Mg2 SiO4 and Mg2 Al4 Si5 O18 will be formed in the interfacial layer after cooling. From the atom percentage of EDS results in Figs. 5 and 6, it was observed that Al and Mg were the main components at spots 2 and 3 while the content of Si was far less than the original percentage. As a result, it can be predicted that the diffusion of Mg as well as the dissolution of Al2 O3 were promoted after the slag wetted on the substrate. From the above discussion, the corrosion mechanism of Al2 O3 substrate by the specified slags can be explained in Fig. 9. Upon heating, the solid slag melted gradually into liquid state accompanied by a decrease in the contact angle. Initially, the slag was not completely melted, and the surface tension of the slag was relatively high because of the existence of solid phase. Surface tension was the main resistance of wetting and the dissolution of Al2 O3 was restrained at this stage. With increase in the temperature, the surface tension of slag decreased obviously, thus the contact angle decreased correspondingly and then remained stable. Wetting was the first step that caused the corrosion of Al2 O3 substrate. As the slags melted into liquid state, the dissolution of Al2 O3 from the substrate was accelerated. However, the heating rate was relatively fast which lead to a short dissolution time. Meanwhile, Mg and Ca ions in the slag would diffuse towards the substrate to react with Al2 O3 . The dissolution of Al2 O3 was another important reason that caused the corrosion of substrate. Line scanning results in Figs. 5 and 6 also proved the distribution of Mg and Al from layer I to layer III. With the dissolution of Al2 O3 as well as the proceeding of reaction among MgO, SiO2 and Al2 O3 , high melting point phases were deduced to be precipitated in the interfacial layer. The generated products gradually covered the substrate surface under the droplet which would inhibit further dissolution of Al2 O3 . Therefore, no obvious corrosion was observed on the Al2 O3 substrate after the wetting experiment. The difference between the exper-
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
ARTICLE IN PRESS j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
7
Fig. 8 – SiO2 –2.53 wt% CaO–MgO–Al2 O3 –10 wt% FeO quinary phase diagram.
Fig. 9 – The corrosion mechanism of Al2 O3 substrate by the slag.
imental slags was not distinct which may be accounted for similar solubility of Al2 O3 in the slags. However, the experimental slags will be tightly bonded with the substrate after cooling. Good wettability and the dissolution of Al2 O3 into slag would result in severe sticking problems between burden and alumina refractory which was adverse to the discharge stage of RHF process.
4.
Conclusions
(1) The corrosion process was summarized as three stages: melting & wetting, dissolution & diffusion and crystallization. Good wettability and the dissolution of Al2 O3 into slag are two main factors that caused the corrosion of substrate. (2) The specified slags with basicity of 0.43 and 0.63 had a relatively low apparent contact angle of approximately 25◦ and 30◦ , respectively. The wetting and corrosion phenomenon between these two slags was not distinct which may be accounted for similar solubility of Al2 O3 in the slags.
(3) These two slag samples could wet well on the Al2 O3 substrate under the experimental conditions. The spreading of slag on Al2 O3 substrate was mainly ascribed to the decrease of surface tension at the initial stage. (4) As the wetting process went on, Al2 O3 dissolved into the slag and Mg,Al–bearing compound was expected to be formed in interface between slag and substrate. Superior wettability would possibly bring sticking problems between pellet and alumina refractory and even erode the alumina-based refractories, which will bring negative impact on the RHF process.
Conflict of interest statement We declare that we have no financial and personal relationships with other people or organizations that can inappropriately influence our work, there is no professional or other personal interest of any nature or kind in any product, service or company that could be construed as influencing the position presented in, or the review of, the manuscript entitled.
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060
JMRTEC-1037; No. of Pages 8
ARTICLE IN PRESS
8
j m a t e r r e s t e c h n o l . 2 0 1 9;x x x(x x):xxx–xxx
Zhixiong You, on behalf of the others.
Declarations of interest None.
Acknowledgements The authors are especially grateful to the National Key R&D Program of China (2018YFC1900500) and the Fundamental Research Funds for the Central Universities (2018CDQYCL0026) for the financial support of this research.
references
[1] King MG. Nickel laterite technology−Finally a new dawn. JOM 2005;57(7):35–9. [2] Warner AEM, Diaz CM, Dalvi AD, Mackey PJ, Tarasov AV. JOM world nonferrous smelter survey, part III: nickel: laterite. JOM 2006;58(4):11–20. [3] Lv XM, Lv W, You ZX, Lv XW, Bai CG. Non–isothermal kinetics study on carbothermic reduction of nickel laterite ore. Powder Technol 2018;340:495–501. [4] Lv XM, Lv W, Liu M, You ZX, Lv XW, Bai CG. Effect of sodium sulfate on preparation of ferronickel from nickel laterite by carbothermal reduction. ISIJ Int 2018;58(5):799–807. [5] Li YJ, Sun YS, Han YX, Gao P. Coal–based reduction mechanism of low–grade laterite ore. Trans Nonferrous Met Soc China 2013;23(11):3428–33. [6] Chang YF, Zhai XJ, Fu Y, Ma LZ, Li BC, Zhang TA. Phase transformation in reductive roasting of laterite ore with microwave heating. Trans Nonferrous Met Soc China 2008;18(4):969–73. [7] Zevgolis EN, Zografidis C, Perraki T, Devlin E. Phase tranformations of nickliferous laterites during preheating and reduction with carbon monoxide. J Therm Anal Calorim 2010;100(1):133–9. [8] Lv XW, Bai CG, He SP, Huang QY. Mineral change of Philippine and Indonesia nickel lateritic ore during sintering and mineralogy of their sinter. ISIJ Int 2010;50(3):380–5. [9] Liu P, Li BK, Cheung SCP, Wu WY. Material and energy flows in rotary kiln–electric furnace smelting of ferronickel alloy with energy saving. Appl Therm Eng 2016;109:542–59. [10] Kim J, Dodbiba G, Tanno H, Okaya K, Matsuo S, Fujita T. Calcination of low–grade laterite for concentration of Ni by magnetic separation. Miner Eng 2010;23(4):282–8. [11] Chen S, Guo SQ, Jiang L, Xu YL, Ding WZ. Thermodynamic of selective reduction of laterite ore by reducing gases. Trans Nonferrous Met Soc China 2015;25(9):3133–8. [12] Kobayashi Y, Todoroki H, Tsuji H. Melting behavior of siliceous nickel ore in a rotary kiln to produce ferronickel alloys. ISIJ Int 2011;51(1):35–40. [13] Rao MJ, Li GH, Jiang T, Luo J, Zhang YB, Fan XH. Carbothermic reduction of nickeliferous laterite ores for nickel pig iron production in China: a Review. JOM 2013;65(11):1573–83. [14] Murakami T, Nagata K. New ironmaking process from the viewpoint of carburization and iron melting at low temperature. Miner Process Extr M 2013;24(3–4):253–67. [15] Eissa M, El-Farmawy H. Carbothermic smelting of high carbon ferrochromium alloy from low and high grade chromite ores. Ironmak Steelmak 2012;39(1):31–7.
[16] Kapure GU, Rao CB, Tathavadkar VD, Sen R. Direct reduction of low grade chromite overburden for recovery of metals. Ironmak Steelmak 2011;38(8):590–6. [17] Eriksson G, Pelton A. Critical evaluation and optimization of the thermodynamic properties and phase diagrams of the CaO-Al2 O3 , Al2 O3 -SiO2 , and CaO-Al2 O3 -SiO2 systems. Metall Trans B 1993;24(5):807–16. [18] Mao H, Hillert M, Selleby M, Sundman B. Thermodynamic assessment of the CaO–Al2 O3 –SiO2 system. J Am Ceram Soc 2006;89(1):298–308. [19] Diaz LA, Torrecillas R, de Aza AH, Pena P. Effect of spinel content on slag attack resistance of high alumina refractory castables. J Eur Ceram Soc 2007;27:4623–31. [20] Fu LP, Huang A, Lian PF, Gu HZ. Isolation or corrosion of microporous alumina in contact with various CaO–Al2 O3 –SiO2 slags. Corros Sci 2017;120:211–8. [21] Ramezani A, Mohebi MM, Souri A. Incorporating nano-silica as a binder to improve corrosion resistance of high alumina refractory castables. J Mater Eng Perform 2013;22(4):1010–7. [22] Sako EY, Braulio MAL, Brant PO, Pandolfelli VC. The impact of pre-formed and in situ spinel formation on the physical properties of cement-bonded high alumina refractory castables. Ceram Int 2010;36:2079–85. [23] Fu LP, Huang A, Gu HZ, Lu DH, Lian PF. Effect of nano-alumina sol on thesintering properties and microstructure of microporous alumina. Mater Des 2016;89:21–6. [24] Fu LP, Gu HZ, Huang A, Bai C. Effect of MgO micropowder on sinteringproperties and microstructures of microporous alumina aggregates. Ceram Int 2015;41(4):5857–62. [25] Sako EY, Braulio MAL, Luz AP, Zinngrebe E, Pandolfelli VC. Slag resistance of Al2 O3 –MgO refractory castables in different environmental conditions. J Am Ceram Soc 2013;96(10):3252–7. [26] Blond E, Schmitt N, Hild F, Blumenfeld P, Poirier J. Effect of slag impregnation on thermal degradations in refractories. J Am Ceram Soc 2007;90(1):154–62. [27] Luo J, Li GH, Peng ZW, Rao MJ, Zhang YB, Jiang T. Phase evolution and Ni-Fe granular growth of saprolitic laterite ore–CaO mixtures during reductive roasting. JOM 2016;68(12):3015–21. [28] Yu B, Lv XW, Bai CG, Yin JQ. Wetting behavior of Al2 O3 substrate by calcium ferrite series melts. ISIJ Int 2015;55(3):483–90. [29] Amondarain Z, Kolbeinsen L, Luis AJ. Wetting behavior of sintered nanocrystalline powders by armco Fe and 22CrNiMoV5–3 steel grade using sessile drop wettability technique. ISIJ Int 2011;51(5):733–42. [30] Shen P, Fujii H, Matsumoto T, Nogi K. The influence of surface structure on wetting of ␣–Al2 O3 by aluminum in a reduced atmosphere. Acta Mater 2003;51:4897–906. [31] Fox H, Zisman WA. The spreading of liquids on low energy surfaces. I. Polytetrafluoroethylene. J Colloid Interf Sci 1950;5(6):514–31. [32] Young T. An essay on the cohesion of fluids. Proc R Soc London 1805;95:65–87. [33] Mills KC, Keene BJ. Physical properties of bos slags. Int Mater Rev 1987;41(6):209–42. [34] Choi JY, Lee HG, Kim JS. Dissolution rate of Al2 O3 into molten CaO–SiO2 –Al2 O3 slags. ISIJ Int 2002;42(8):852–60. [35] Bilbao ED, Dombrowski M, Pilliere H, Poirier J. Time–resolved high–temperature X–ray diffraction for studying the kinetics of corrosion of high–alumina refractory by molten oxides. Corros Sci 2018;139:346–54.
Please cite this article in press as: Song J, et al. Corrosion behavior of Al2 O3 substrate by SiO2 –MgO–FeO–CaO–Al2 O3 slag. J Mater Res Technol. 2019. https://doi.org/10.1016/j.jmrt.2019.10.060