Abstract
CaO–MgO–Al2O3–SiO2 glass-ceramics with diopside as the main crystalline phase were prepared by melting blast furnace slag obtained from Baotou Iron and Steel Company. The effect of heat treatment on the crystallization behavior of glass-ceramics, containing a large proportion of melted blast furnace slag, was studied by means of differential thermal analysis and scanning electron microscopy. The optimum heat-treatment regime was obtained by orthogonal experimental results for glass-ceramics in which blast furnace slag comprised 70% of the composition and 1% Cr2O3 and 4% TiO2 were used as nucleating agents. The nucleation temperature was 750°C for 2.5 h and the crystallization temperature was 930°C for 1 h. Under this regime, the performance of the glass-ceramic was better than that of other groups in the orthogonal experiment.
1 Introduction
The water-quenched slag of Baotou Iron and Steel Company (Inner Mongolia, China) is mainly used to produce cement and slag powder. This utilization has disadvantages of high capital cost, low added value of products, and inefficient utilization of slag heat. The main chemical components of the blast furnace slag are CaO, SiO2, MgO, and Al2O3, which account for about 90% of the total slag and contain less harmful impurities [1,2]. This is an ideal raw material for decorative glass-ceramics of the CaO–SiO2–MgO–Al2O3 system, and also an effective economic way to increase value added to the blast furnace slag.
Glass-ceramics prepared with large-scale molten blast furnace slag can not only greatly improve utilization of the slag but also make full use of its heat energy [3]. Diopside and melilite are the main crystalline phases of glass-ceramics developed by the Turkish steel producer, Erdemir, using their blast furnace slag [4], with up to 50% of slag in the formulation. In research on glass-ceramics carried out by Weifeng [5,6], the proportion of blast furnace slag was up to 60%, but higher proportions are not reported in the literature. In this study, the proportion of blast furnace slag was 70%, which makes full use of the slag and its heat energy. Owing to the higher addition of blast furnace slag, the crystallization behavior of the glass-ceramics is strongly affected, and their physicochemical properties deteriorate. Defects caused by the high addition of blast furnace slag can be remedied by optimizing the heat-treatment parameters.
Baowei et al. [7] and Xueli [8] studied the effect of nucleation and crystallization temperature and time on the bending strength of slag glass-ceramics through orthogonal experiments and then determined an appropriate heat-treatment system that enabled their flexural strength to exceed 100 MPa and achieve excellent physical and chemical properties. Bochen [9] studied the heat treatment system of glass-ceramics from blast furnace slag of Baotou Iron and Steel Company by orthogonal test. The influence of selected factors on the properties of glass-ceramics was found out. The flexural strength of glass-ceramics under the optimum heat treatment system was determined to be 221.7 MP. Yang and Hanning [10] optimized the heat treatment system of glass-ceramics by means of orthogonal experiment and determined the optimum technological parameters as follows: the nucleation temperature is 840°C, holding for 1 h; the crystallization temperature is 910°C, holding for 1 h. Under the same experimental method, Xin [11] optimized the heat treatment system by orthogonal design and obtained the best technological parameters and glass-ceramics samples with good properties. Therefore, proper heat treatment is an important condition to ensure good microstructure and properties of glass-ceramics [11]. In this study, flexural strength was considered as the main examination index of glass-ceramics, and the heat-treatment system was optimized using an orthogonal experimental method to determine the best heat-treatment parameters.
2 Materials and methods
2.1 Raw materials
Blast furnace water-quenched slag from Baotou Iron and Steel Company, which is shown in Figure 1, was used as the main raw material. Its proportion in the ceramic formulation was up to 70%. The chemical composition of the slag is shown in Table 1. The other raw materials were quartz sand and purification reagents, CaO, MgO, and Al2O3. The nucleating agents were Cr2O3 and TiO2. The purities of the raw materials are shown in Table 2.

Blast furnace water-quenched slag used in this study.
Chemical composition of blast furnace slag from Baotou Iron and Steel Company (mass%)
Chemical components | SiO2 | CaO | MgO | Al2O3 | FeO | Na2O | K2O | F | TiO2 | Loss on ignition |
---|---|---|---|---|---|---|---|---|---|---|
Mass percentage | 34.06 | 37.79 | 9.67 | 13.08 | 1.65 | 0.34 | 0.31 | 0.27 | 0.93 | 1.90 |
Purity of raw materials (mass%)
Raw material | Quartz sand | CaO | MgO | Al2O3 | Cr2O3 | TiO2 |
---|---|---|---|---|---|---|
Purity | 96.87 | 98.00 | 98.00 | 93.93 | 99.00 | 99.00 |
2.2 Procedures
2.2.1 Preparation of glass-ceramics
Glass-ceramics were prepared by melting the blast furnace slag. The slag was ground in a ball mill and passed through a screen with a diameter of 0.074 mm. The slag and other raw materials were accurately weighed, mixed evenly, placed in a corundum crucible, and melted in a high-temperature furnace using a Si–Mo rod as the heater. The mixture was held at 1,500°C for 3 h to obtain a uniform glass liquid. The molten glass liquid was then poured into steel molds for natural cooling and annealed at 600°C for 2 h to eliminate internal stress. Samples of glass-ceramics were obtained after nucleating and crystallizing heat treatment.
The steps of the operation were as follows: batching → mixing → melting → molten glass casting → annealing → nucleating and crystallizing heat treatment → glass-ceramic.
2.2.2 Detection and analysis methods
Differential thermal analysis (DTA) of glass powders was carried out using a STA + PT1600 pressurized simultaneous thermal analyzer (Linseis, Germany) to determine the heat-treatment temperature [12]. The glass sample was ground to below 0.074 mm diameter, and α-Al2O3 was used as the reference sample. The heating rate was 10°C/min. Argon was used as protective gas. The microstructure was determined using a JSM-6510 scanning electron microscope (SEM; Jeol, Japan).
The measured physical and chemical properties of the glass-ceramics included flexural strength, density, and acid and alkaline corrosion resistance. Flexural strength was measured using a three-point bending method on a universal testing machine, the standard of the test sample is 40 mm long, 3 mm wide, and 4 mm high. Three or four samples were calculated according to formula (1), and the average flexural strength was obtained; the volume density of the samples was measured by Archimedes’ method; the acid and alkaline corrosion resistance tests were carried out by immersing samples for 15 days in 3% H2SO4 and 3% NaOH solution, respectively, and measuring their mass change.
In formula (1), σ – flexural strength of specimens (MPa), F – the maximum load beared by a specimen at fracture (N), b – fracture width (mm), h – fracture height (mm).
2.3 Determination of heat-treatment temperature
Glass-ceramics were prepared by introducing 70% blast furnace slag and 1% Cr2O3 and 4% TiO2 as nucleating agents to the composition. The differential scanning calorimetry (DSC) curve of the glass sample was carried out by DTA, as shown in Figure 2, and used to determine the nucleation and crystallization temperatures.

DTA curve of the glass sample.
According to the crystallography theory [13], the precipitation of crystal nuclei needs some energy from the environment, which is an endothermic process; in contrast, crystallization is a phase transformation from unsteady state to steady-state, which is an exothermic process. The endo- and exothermic peaks in the DSC curve, therefore, respectively, represent the nucleation and crystallization processes of the glass. An exiguous endothermic peak occurred at about 710°C, and there were two obvious exothermic peaks at 944.7°C and 988.8°C [14].
To further determine the crystallization temperature, the glass sample was heat-treated at the temperatures of the two exothermic peaks. The microstructures of the samples after heat treatment are shown in Figure 3(a) and (b), and their flexural strengths were measured, as shown in Table 3.

Microstructures of glass samples after heat treatment at crystallization peak temperatures: (a) 945°C and (b) 989°C.
Flexural strength at different crystallization temperatures
No. | Tn (°C) | tn (h) | Tc (°C) | tc (h) | Average flexural strength (MPa) |
---|---|---|---|---|---|
1 | 770 | 1.5 | 945 | 1.5 | 96.14 |
2 | 770 | 1.5 | 989 | 1.5 | 57.43 |
SEM micrographs showed that the overall crystallization degree is relatively high in Figure 3(a), the grain distribution is uniform and compact, the grain growth degree is reasonable, the grain size is distributed in 10–30 microns, and the shape is mostly long columnar and massive crystals, as shown in point A; the crystallization temperature in Figure 3(b) is 989°C, and the grain size increases at higher temperatures. The grain size is distributed in 30–45 microns, as shown in point B. Most of them are massive crystals, some of them are even connected into flakes. The overall microstructure of grain distribution is sparse, and the residual glass phase is obvious.
The grain size, quantity, and distribution determine the physical and chemical properties of glass-ceramics [15,16]. The selection of an appropriate heat-treatment regime is a prerequisite for ensuring the good microstructure and properties of these materials. The average flexural strengths of the samples after heat treatment and the heat-treatment parameters used are shown in Table 3, in which Tn and Tc are nucleation and crystallization temperatures, respectively, and tn and tc are nucleation and crystallization times, respectively.
The average flexural strength of the glass-ceramic was 96.14 MPa when the crystallization temperature was 945°C, and it was 57.43 MPa when the crystallization temperature was 989°C. Therefore, the exothermic peak temperature at 945°C was determined to be the optimum crystallization temperature.
2.4 Optimization of heat-treatment parameters
Heat treatment is a key step in the preparation of glass-ceramics from blast furnace slag [17,18]. Its main purpose is to transform the glass into a polycrystalline solid material containing a large number of crystalline phases. The main technical parameters include nucleation and crystallization temperature and time. In this study, the flexural strength was taken as the comparative index, and an orthogonal experiment designed to determine the optimum parameters. The ranges of nucleation and crystallization temperatures were determined from the DSC curve.
The endothermic peak at 710°C on the DSC curve represents the glass transition temperature (Tg). According to the literature, the nucleation temperature is generally higher than the glass transition temperature by about 40–80°C [19,20] and the crystallization temperature is generally the peak exothermic temperature – of 945°C, in this case. In this study, an orthogonal experimental design using four factors and four levels of k (44) was carried out for the main heat-treatment parameters of nucleation temperature, nucleation time, crystallization temperature, and crystallization time. The nucleation temperature range was 750–810°C, and the crystallization temperature ranged from 930 to 975°C. The time intervals for nucleation and crystallization were 0.5 h, ranging from 1.0 h to 2.5 h. The levels and factors of the orthogonal test are listed in Table 4; the flexural strength and orthogonal experimental design are listed in Table 5; the results are listed in Table 6.
Levels and factors of orthogonal test
Factors | Tn (°C) | Tc (°C) | tn (h) | tc (h) |
---|---|---|---|---|
Levels | ||||
1 | 750 | 930 | 1.0 | 1.0 |
2 | 770 | 945 | 1.5 | 1.5 |
3 | 790 | 960 | 2.0 | 2.0 |
4 | 810 | 975 | 2.5 | 2.5 |
Flexural strength and orthogonal experimental design for different heat-treatment systems
No. | Tn (°C) | Tc (°C) | tn (h) | tc (h) | Flexural strength (MPa) |
---|---|---|---|---|---|
1 | 750 | 930 | 1.0 | 1.0 | 84.15 |
2 | 750 | 945 | 1.5 | 1.5 | 96.14 |
3 | 750 | 960 | 2.0 | 2.0 | 79.51 |
4 | 750 | 975 | 2.5 | 2.5 | 61.46 |
5 | 770 | 930 | 1.5 | 2.0 | 88.62 |
6 | 770 | 945 | 1.0 | 2.5 | 54.52 |
7 | 770 | 960 | 2.5 | 1.0 | 82.31 |
8 | 770 | 975 | 2.0 | 1.5 | 48.06 |
9 | 790 | 930 | 2.0 | 2.5 | 89.06 |
10 | 790 | 945 | 2.5 | 2.0 | 92.36 |
11 | 790 | 960 | 1.0 | 1.5 | 46.38 |
12 | 790 | 975 | 1.5 | 1.0 | 68.82 |
13 | 810 | 930 | 2.5 | 1.5 | 89.58 |
14 | 810 | 945 | 2.0 | 1.0 | 87.84 |
15 | 810 | 960 | 1.5 | 2.5 | 69.44 |
16 | 810 | 975 | 1.0 | 2.0 | 44.61 |
Range analysis of orthogonal experimental results for different heat-treatment systems
No. | Tn (°C) | Tc (°C) | tn (h) | tc (h) |
---|---|---|---|---|
∑(1) | 321.26 | 352.01 | 229.66 | 323.12 |
∑(2) | 273.51 | 330.86 | 298.19 | 280.16 |
∑(3) | 297.22 | 277.64 | 305.07 | 305.10 |
∑(4) | 292.47 | 222.95 | 325.71 | 275.08 |
∑(1)/4 | 80.32 | 88.00 | 57.42 | 80.78 |
∑(2)/4 | 68.38 | 82.72 | 74.55 | 70.04 |
∑(3)/4 | 74.31 | 69.41 | 76.27 | 76.28 |
∑(4)/4 | 73.12 | 55.74 | 81.43 | 68.77 |
R | 11.94 | 32.27 | 24.01 | 12.01 |
Notes: ∑(1): sum of flexural strength of level 1; ∑(2): sum of flexural strength of level 2; ∑(3): sum of flexural strength of level 3; ∑(4): sum of flexural strength of level 4; ∑(1)/4: average flexural strength of level 1; ∑(2)/4: average flexural strength of level 2; ∑(3)/4: average flexural strength of level 3; ∑(4)/4: average flexural strength of level 4; R: range of flexural strength.
Tables 5 and 6 indicate that the range of crystallization temperature Tc was largest (R = 32.27), the range of nucleation time tn was second-largest (R = 24.01), and those of nucleation temperature Tn and crystallization time tc were almost the same (11.94 and 12.01, respectively). Therefore, crystallization temperature had the greatest influence on the flexural strength, followed by nucleation time. The nucleation temperature and crystallization time had the least influence on the flexural strength of the blast furnace slag glass-ceramic.
2.5 Determination of optimal heat-treatment system and properties of glass-ceramic
The optimum heat-treatment parameters to prepare these glass-ceramics were determined by orthogonal experiment using a nucleation temperature of 750°C for 2.5 h and crystallization temperature of 930°C for 1 h. The heating rate was 5°C/min before nucleation and 3°C/min before crystallization. After heat treatment, the samples were cooled in the furnace. The optimum heat-treatment system is shown in Figure 4. Properties of this glass-ceramic prepared under the optimum heat-treatment system, such as flexural strength, density, porosity, acid resistance, alkali resistance, and water absorption, are compared with those reported for marble, granite, and similar materials in Table 7. The flexural strength of the blast furnace slag glass-ceramic under the optimum heat-treatment regime reached 102.2 MPa, which is superior to that of 16 points in the orthogonal experiment. Compared with other studies, the other physical and chemical properties of the glass-ceramic were also reasonably superior, ranking in the upper-middle level [21,22,23].

Optimal heat-treatment system.
Comparison of main properties of glass-ceramics prepared under an optimized heat-treatment system with those of marble, granite, and other materials
Products | Flexural strength (MPa) | Density (g/cm3) | Porosity (%) | Acid resistance (%) | Alkali resistance (%) | Water absorption rate (%) |
---|---|---|---|---|---|---|
Glass ceramics | 102.20 | 2.72 | 0.08 | 0.28 | 0.33 | 0.06 |
Marble | 5.70–15.00 | 2.70 | 0.10 | 10.00 | 0.30 | 0.30 |
Granite | 8.00–15.00 | 2.00 | 0.10 | 0.10 | 0.10 | 0.35 |
Other studies [21,22,23] | 65.00–147.00 | 2.68–3.15 | 0.01–0.15 | 0.02–0.52 | 0.15–0.80 | 0.08–0.10 |
3 Conclusions
Using a 70% blast furnace slag from Baotou Iron and Steel Company as the main raw material and 1% Cr2O3 and 4% TiO2 as nucleating agents, an orthogonal experiment was carried out to optimize the heat-treatment process for preparing CaO–SiO2–MgO–Al2O3 glass-ceramics. The results showed that the crystallization temperature had the greatest influence on the flexural strength of the glass-ceramics, followed by nucleation time; nucleation temperature and crystallization time had the least influence.
The optimum heat-treatment system for preparing glass-ceramics from this large-scale blast furnace slag comprised a nucleation temperature of 750°C for 2.5 h and a crystallization temperature of 930°C for 1 h. Under these conditions, the flexural strength of the glass-ceramics reached 102.2 MPa.
Acknowledgments
This work was financially supported by the National Natural Science Foundation of China (Grant No. 51664044 and No. 51664045), Inner Mongolia Natural Science Foundation (Grant No. 2018LH05026), the Special Fund of Scientific and Technological Achievements Transformation of Inner Mongolia Autonomous Region (Grant No. 2019CG073), and Research Fund of State Key Laboratory of Advanced Metallurgy (Grant No. KF19-01).
References
[1] Yongliang, G., X. Chunshuai, S. Chunyan, and H. Binsheng. Research progress and prospects of blast furnace slag glass-ceramics. Chinese Ceramics, Vol. 52, No. 3, 2016, pp. 1–5.Search in Google Scholar
[2] Ye, L. Preparation of glass-ceramics from steel slag and its performance evaluation. World Metal Herald, No. B12, 2018, pp. 9–11.Search in Google Scholar
[3] Yanmei, G., S. Daosheng, L. Kaiwei, W. Aiguo, and Z. Yan. Research progress in component design and preparation process of industrial waste glass-ceramics. Materials Report, Vol. 30, No. 03, 2016, pp. 105–108.Search in Google Scholar
[4] Erkmen, Z. E., E. Catakli, and M. Lutfi Ovecoglu. Characterisation and crystallization kinetics of glass ceramics developed from Erdemir blast furnace slags containing Cr2O3 and TiO2 nucleants. Advances in Applid Ceramics, Vol. 108, No. 1, 2009, pp. 57–66.10.1179/174367608X364294Search in Google Scholar
[5] Weifeng, J. Comprehensive utilization of blast furnace slag – manufacturing glass-ceramics with high proportion of blast furnace slag. Comprehensive Utilization of China Resources, No. 3, 2003, pp. 28–29.Search in Google Scholar
[6] Jiakuan, Y., X. Bo, Y. Dingwen, and W. Xiuping. Preparation and microstructure analysis of yellow phosphorus slag glass-ceramics. Comprehensive Utilization of Minerals, No. 2, 2003, pp. 40–43, 1550–1553.Search in Google Scholar
[7] Baowei, L., D. Leibo, Z. Xuefeng, J. Xiaolin, Z. Ming, and Z. Mingxing. Optimization design of heat treatment system for slag glassceramics. Bulletin of the Chinese Ceramic Society, Vol. 31, No. 6, 2012, pp. 1550–1553.Search in Google Scholar
[8] Xueli, N. Development of glass-ceramics. M.Eng, Lanzhou University of Technology, Lanzhou, 2006.Search in Google Scholar
[9] Bochen, L. Study on heat treatment system of glass-ceramics from blast furnace slag of Baotou Iron and Steel Company. M.Sc, Inner Mongolia University of Science and Technology, Baotou, 2015.Search in Google Scholar
[10] Yang, L., and X. Hanning. The effect of blast furnace slag content and heat treatment system on the performance of slag glass-ceramics. Ceramics, Vol. 37, No. 6, 2003, pp. 17–20.Search in Google Scholar
[11] Xin, J. Discussion on the production of glass-ceramics from metallurgical slag. China’s New Technology and New Products, No. 1, 2017, pp. 84–85.Search in Google Scholar
[12] Guohua, C. Application of differential thermal analysis in glass-ceramics. Journal of Luoyang Institute of Technology: Natural Science Edition, Vol. 5, No. 4, 1995, pp. 5–9.Search in Google Scholar
[13] Endo, H., and Y. Nagayoshi. Production of Glass-Ceramics from Sewage Sludge. Water Science & Technology, Vol. 36, No. 11, 1997, pp. 235–241.10.2166/wst.1997.0416Search in Google Scholar
[14] Barbieri, L., A. Corradi, and I. Lancelotti. Thermal and chemical behavior of different glasses containing steelfiy ash and their transformation into glass-ceramics. Journal of the European Ceramic Society, Vol. 22, No. 11, 2002, pp. 1759–1765.10.1016/S0955-2219(01)00492-7Search in Google Scholar
[15] Wenming, H., and C. Chao. Effect of crystallization temperature on microstructure and acid corrosion resistance of blast furnace slag glass-ceramics. Materials Review, Vol. 29, No. S1, 2015, pp. 333–336.Search in Google Scholar
[16] Chongchong, B., L. Xuefei, W. Zixiang, P. Pengfei, and W. Yubo. Crystallization behavior in blast furnace slag glass-ceramic system. Journal of Materials and Metallurgy, Vol. 17, No. 1, 2018, pp. 20–25+31.Search in Google Scholar
[17] Barbieri, L., A. Corradi, and I. Lancelotti. Thermal and chemical behav-ior of different glasses containing steelfiy ash and their transforma-tion into glass-ceramics. Journal of the European Ceramic Society, Vol. 22, No. 11, 2002, pp. 1759–1765.10.1016/S0955-2219(01)00492-7Search in Google Scholar
[18] Ponsot, I, E. Bernardo, E. Bontempi, L. Depero, R. Detsch, and R. Krishnachinnam. Recycling of pre-stabilized municipal waste incinerator fly ash and soda-lime glass into sintered glass-ceramics. Journal of Cleaner Production, Vol. 89, 2015, pp. 224–230.10.1016/j.jclepro.2014.10.091Search in Google Scholar
[19] Yawen, W., G. Yongliang, S. Chunyan, X. Chunshuai, and Z. Jinlong. Research progress in preparation of glass-ceramics from blast furnace slag. Comprehensive Utilization of Minerals, No. 2, 2018, pp. 1–6.Search in Google Scholar
[20] Baoqing, L., G. Yanping, F. Hongsheng, H. Danghaifeng, L. Zhenxing, and W. Wenxiang. Effect of crystallization temperature on crystallization and properties of CaO–Al2O3–MgO–SiO2 glass-ceramics synergistically prepared from fly ash/waste screen glass. Journal of Ceramics, Vol. 39, No. 04, 2018, pp. 443–448.Search in Google Scholar
[21] Jingjing, L. Effect of crystal nucleating agent on the structure and properties of blast furnace slag glass-ceramics. M.Eng, Hunan University, Changsha, 2016.Search in Google Scholar
[22] Bochen, L. Study on the heat treatment system of blast furnace slag glass-ceramics at Baotou Steel. M.Sc, Inner Mongolia University of Science and Technology, Baotou, 2015.Search in Google Scholar
[23] Fuzhi, S., X. Yongli, L. Yongqian, L. Yin, and X. Mengqin. Preparation and characterization of blast furnace slag glass-ceramics with Cr2O3, Fe2O3 and TiO2 composite nucleating agents. Baosteel Technology, No. 5, 2015, pp. 13–17.Search in Google Scholar
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- Effects of metallurgical factors on reticular crack formations in Nb-bearing pipeline steel
- Investigation on microstructure and its transformation mechanisms of B2O3-SiO2-Al2O3-CaO brazing flux system
- Energy Conservation and CO2 Abatement Potential of a Gas-injection Blast Furnace
- Experimental validation of the reaction mechanism models of dechlorination and [Zn] reclaiming in the roasting steelmaking zinc-rich dust process
- Effect of substituting fine rutile of the flux with nano TiO2 on the improvement of mass transfer efficiency and the reduction of welding fumes in the stainless steel SMAW electrode
- Microstructure evolution and mechanical properties of Hastelloy X alloy produced by Selective Laser Melting
- Study on the structure activity relationship of the crystal MOF-5 synthesis, thermal stability and N2 adsorption property
- Laser pressure welding of Al-Li alloy 2198: effect of welding parameters on fusion zone characteristics associated with mechanical properties
- Microstructural evolution during high-temperature tensile creep at 1,500°C of a MoSiBTiC alloy
- Effects of different deoxidization methods on high-temperature physical properties of high-strength low-alloy steels
- Solidification pathways and phase equilibria in the Mo–Ti–C ternary system
- Influence of normalizing and tempering temperatures on the creep properties of P92 steel
- Effect of temperature on matrix multicracking evolution of C/SiC fiber-reinforced ceramic-matrix composites
- Improving mechanical properties of ZK60 magnesium alloy by cryogenic treatment before hot extrusion
- Temperature-dependent proportional limit stress of SiC/SiC fiber-reinforced ceramic-matrix composites
- Effect of 2CaO·SiO2 particles addition on dephosphorization behavior
- Influence of processing parameters on slab stickers during continuous casting
- Influence of Al deoxidation on the formation of acicular ferrite in steel containing La
- The effects of β-Si3N4 on the formation and oxidation of β-SiAlON
- Sulphur and vanadium-induced high-temperature corrosion behaviour of different regions of SMAW weldment in ASTM SA 210 GrA1 boiler tube steel
- Structural evidence of complex formation in liquid Pb–Te alloys
- Microstructure evolution of roll core during the preparation of composite roll by electroslag remelting cladding technology
- Improvement of toughness and hardness in BR1500HS steel by ultrafine martensite
- Influence mechanism of pulse frequency on the corrosion resistance of Cu–Zn binary alloy
- An interpretation on the thermodynamic properties of liquid Pb–Te alloys
- Dynamic continuous cooling transformation, microstructure and mechanical properties of medium-carbon carbide-free bainitic steel
- Influence of electrode tip diameter on metallurgical and mechanical aspects of spot welded duplex stainless steel
- Effect of multi-pass deformation on microstructure evolution of spark plasma sintered TC4 titanium alloy
- Corrosion behaviors of 316 stainless steel and Inconel 625 alloy in chloride molten salts for solar energy storage
- Determination of chromium valence state in the CaO–SiO2–FeO–MgO–CrOx system by X-ray photoelectron spectroscopy
- Electric discharge method of synthesis of carbon and metal–carbon nanomaterials
- Effect of high-frequency electromagnetic field on microstructure of mold flux
- Effect of hydrothermal coupling on energy evolution, damage, and microscopic characteristics of sandstone
- Effect of radiative heat loss on thermal diffusivity evaluated using normalized logarithmic method in laser flash technique
- Kinetics of iron removal from quartz under ultrasound-assisted leaching
- Oxidizability characterization of slag system on the thermodynamic model of superalloy desulfurization
- Influence of polyvinyl alcohol–glutaraldehyde on properties of thermal insulation pipe from blast furnace slag fiber
- Evolution of nonmetallic inclusions in pipeline steel during LF and VD refining process
- Development and experimental research of a low-thermal asphalt material for grouting leakage blocking
- A downscaling cold model for solid flow behaviour in a top gas recycling-oxygen blast furnace
- Microstructure evolution of TC4 powder by spark plasma sintering after hot deformation
- The effect of M (M = Ce, Zr, Ce–Zr) on rolling microstructure and mechanical properties of FH40
- Phase evolution and oxidation characteristics of the Nd–Fe–B and Ce–Fe–B magnet scrap powder during the roasting process
- Assessment of impact mechanical behaviors of rock-like materials heated at 1,000°C
- Effects of solution and aging treatment parameters on the microstructure evolution of Ti–10V–2Fe–3Al alloy
- Effect of adding yttrium on precipitation behaviors of inclusions in E690 ultra high strength offshore platform steel
- Dephosphorization of hot metal using rare earth oxide-containing slags
- Kinetic analysis of CO2 gasification of biochar and anthracite based on integral isoconversional nonlinear method
- Optimization of heat treatment of glass-ceramics made from blast furnace slag
- Study on microstructure and mechanical properties of P92 steel after high-temperature long-term aging at 650°C
- Effects of rotational speed on the Al0.3CoCrCu0.3FeNi high-entropy alloy by friction stir welding
- The investigation on the middle period dephosphorization in 70t converter
- Effect of cerium on the initiation of pitting corrosion of 444-type heat-resistant ferritic stainless steel
- Effects of quenching and partitioning (Q&P) technology on microstructure and mechanical properties of VC particulate reinforced wear-resistant alloy
- Study on the erosion of Mo/ZrO2 alloys in glass melting process
- Effect of Nb addition on the solidification structure of Fe–Mn–C–Al twin-induced plasticity steel
- Damage accumulation and lifetime prediction of fiber-reinforced ceramic-matrix composites under thermomechanical fatigue loading
- Morphology evolution and quantitative analysis of β-MoO3 and α-MoO3
- Microstructure of metatitanic acid and its transformation to rutile titanium dioxide
- Numerical simulation of nickel-based alloys’ welding transient stress using various cooling techniques
- The local structure around Ge atoms in Ge-doped magnetite thin films
- Friction stir lap welding thin aluminum alloy sheets
- Review Article
- A review of end-point carbon prediction for BOF steelmaking process