1. Introduction
High temperature, high pressure pipe material is one of the most important materials found in thermal power plants; it not only plays an important role in the safety of the power plant operation, but also affects the construction investment of the power plant [
1,
2]. The P22 heat-resistant pipe steel used in early stages is a low-alloy heat-resistant steel with Cr and Mo as the main elements and structure of perlite, and its composition is the same as 12Cr1MoV Steel in China. Although it has good processing and welding properties, the working condition of this kind steel is harsh due to the low strength and poor heat resistance. In the follow-up project construction, 10CrMo910 steel was first used in the main steam pipeline of ultra-high pressure 125 MW and 200 MW units, but this pearlitic heat-resistant steel cannot meet the service conditions under high temperatures of 600–650 °C. Meanwhile, martensitic heat-resistant steel can be used at higher temperatures and high strength, and the typical representative is 9Cr-1Mo steel. P91 steel is a new type of steel by adding V, Nb, N, and other strengthening elements to the original 9Cr-1Mo steel [
3]. P91 steel is a typical martensitic heat-resistant steel, and its maximum service temperature can reach 650 °C, which fills the vacancy of pipeline steel under high temperature conditions. The supercritical and ultra-supercritical units developed in recent years regarded P91 steel as an important steel for the mainstream pipe: the hot section of reheated main steam pipe and its corresponding high-temperature header [
4,
5,
6,
7].
The inclusion of P91 steel is an important factor affecting its properties. Its internal inclusions mainly exist in the form of non-metallic compounds, such as oxides, sulfides, nitrides, etc. Non-metallic inclusions are often the cause of surface and internal defects of steel, especially coarse inclusions, which not only worsen the cold and hot workability, but also have a negative impact on the mechanical properties, especially the fatigue properties of steel [
8,
9,
10,
11]. Due to the difference of thermal expansion coefficients between the inclusion and matrix, radial tensile force would be generated in the steel matrix around the inclusion. This stress, together with the external cyclic stress, promotes the formation of fatigue cracks in the steel matrix close to the inclusion, and worsens the fatigue performance of the steel [
12]. However, inclusions with a small size and spherical contour have little deteriorated effect on steel properties [
13,
14,
15]. In 1991, Murakami et al. [
16] proposed the concept of the “critical size” of inclusions affecting the fatigue performance of steel. If the inclusion size was smaller than the “critical size”, it would not have a deteriorated effect on the fatigue life of steel. Sun et al. [
17] found that when the inclusion size was doubled, the fatigue life of the material decreased by two orders of magnitude. Therefore, the inclusion size had a significant impact on the mechanical properties of steel. The influence of non-metallic inclusions on the fatigue properties of steel was also related to the shape of inclusions. The smaller the radius of curvature of inclusions (the sharper the contour), the more serious the stress concentrated in the steel matrix. Under the alternating stress, fatigue cracks first initiated at the sharp corners of inclusions perpendicular to the direction of tensile stress, and the crack growth rate was much faster than that of spherical inclusions. Therefore, the inclusion with the irregular shape and multiple edges and corners was more harmful to the fatigue performance than the spherical inclusion [
18,
19,
20]. The refinement and spheroidization of inclusions in P91 martensitic heat resistant steel could effectively improve its properties.
In general, the inclusion grade of P91 steel is required to be below grade 2.5 (including A, B, C, D, and DS) [
21]. Traditional ideas for removing inclusions mainly include gas stirring to improve molten steel flow, setting flow control devices in tundish to obtain reasonable flow field, and using filters to forcibly separate inclusions in tundish [
22,
23]. In this paper, a new method for optimizing the inclusion morphology in P91 steel is proposed, and the inclusion refinement mechanism is discussed. The results showed that multi-point regional micro-supply of Al elements was achieved by feeding twisted Al wire into the melt during the smelting process of P91 steel, and Al
2O
3 oxide particles are obtained with fine size and dispersive distribution. Al
2O
3 oxide particles playing the role of heterogeneous nucleation and refined SiO
2, MgO, (Ca, Mg) (O), and other inclusions in steel. This study provided a new idea for the optimization of inclusions in steel.
3. Results
As shown in
Figure 2, in all samples the sum of inclusion grades less than grade 1 in P91 steel prepared by traditional smelting method was less than 15% [
24], while the sum of inclusion grades of experimental P91 steel obtained by multi-point regional micro-supply alloying method could all be controlled at or below grade 1.
The high-grade DS inclusions in experimental P91 steel were characterized. In general, there are four types of inclusions.
Firstly, as shown in
Figure 3, Al
2O
3 inclusions are angular and spherical, which are independently distributed in the steel matrix, and their sizes are 6.8 μm and 7.7 μm, respectively (
Figure 3a). EDS results showed that Al
2O
3 inclusion was composed of Al, O, and Fe elements (
Figure 3b–d), in which the presence of Fe was mainly caused by interference of the matrix.
Secondly, there are Al
2O
3-SiO
2 composite inclusions in new experimental P91 steel. As shown in
Figure 4, these DS inclusions contained Al, O, and Si elements, with a size of about 10 μm. SiO
2 in traditional P91 steel was mostly sharp single-phase inclusions with edges and corners. When being stressed, the tip of such inclusions could easily produce stress concentrations, which resulted in microcracks and became the source of cracking failure. Meanwhile, the Al
2O
3-SiO
2 composite inclusions in experimental P91 steel samples prepared by multi-point regional micro-supply method had a spherical shape, which was conducive to maintaining the material properties.
Thirdly, there are few MgO-A1
2O
3 composite inclusions, with a small size and a circular shape.
Figure 5 showed the results of EDS mapping of one inclusion. The size of the inclusion was 10 μm, the shape was approximately spherical, and the main components were C, Al, Mg, and O. According to the point scan in
Figure 5e, the contents of Al, Mg, and O elements were 42.85 wt.%, 3.48 wt.%, and 45.10 wt.%, respectively. The remaining elements were C, Fe, Cr, and other elements.
Fourthly, there are also (Ca, Mg, Al) (O) compound inclusions in experimental P91 steel. The structure was nearly spherical and the size was about 5–27 μm. As shown in
Figure 6, the matrix of the whole inclusion was Al
2O
3. The size of inclusion was 26.60 μm. It can be seen that most of the spherical inclusion was composed of Al
2O
3, and the elements from the outside to the inside were S, Ca, and Mg, respectively. Sulfide was attached to the periphery of the compound inclusion, forming a “core-shell” structure. The inclusion “core” was mainly the composite oxide inclusion formed by CaO, MgO, and Al
2O
3, et al.
Figure 7 showed the EDS mapping for Al
2O
3 inclusion at micron scale. Inclusion was analyzed by TEM, as shown in
Figure 8a,b. According to the analysis of TEM and diffraction pattern calibration, the central prat was Al
2O
3, which was surrounded with Cr
7C
3. Al
2O
3 was uniformly and densely distributed, and carbides grew on the periphery of Al
2O
3. It was found that the micron-magnitude precipitates were precipitated by adopting nano Al
2O
3 oxide as nucleation particle. Therefore, it could be deduced that nano alumina particles might exist as the nucleation core during the formation of a shell structure.
4. Discussion
The thermodynamic and dynamics conditions of oxide growth in molten steel were discussed. Based on the thermodynamic analysis of oxide nucleation and growth in steel, the nucleation size, nucleation rate, and inclusion nano-crystallization process of alumina in high-strength steel were analyzed qualitatively and quantitatively. The following Equation (1) [
25] was used to calculate the critical nucleation radius of oxide particles in melts.
The critical nucleation radius:
where
is specific surface energy;
is theoretical melting point of Al
2O
3;
is the melting heat of Al
2O
3;
is the difference between
(2051 °C) [
26] and actual solidification temperature. The parameters in the above equations are as follows:
= 2.6 J/m
2 [
27],
= 94.14 kJ/mol [
28].
When the aluminum wire was fed into the molten steel, it reacted with the oxygen in the molten steel. The critical nucleation radius was related to the temperature of the molten steel, which was generally 1500–1680 °C. According to Equation (1), the critical nucleation radius of Al2O3 was in the range of 6.79–10.08 nm.
The change of oxide particle size with interface concentration is described as [
29]:
where
is the diameter of the crystal nucleus;
is the solute diffusion coefficient in liquid metal;
is the density of oxide;
is the density of alloy element;
is the molecular weight of oxide;
is the molecular weight of alloy element;
is the solute concentration in the front of the interface;
is the equilibrium solute concentration of the crystal nucleus. The growth driving force of the nano oxide particle was the solute segregation of the solute atom in the front of the oxide interface and the equilibrium concentration of the oxide (
(t)) −
(t)), and its growth speed was influenced by the size of the oxide and the solute micro area concentration fluctuations in the front of the interface between oxide and melt. As
Figure 9 showed, the growth speed of nano oxide particle was slower with the increase of its radius; meanwhile, its growth speed was reduced sharply, even reduced to zero with the decrease of the [Al] content in the front of the interface. According to
Figure 9 and Equation (2), we can conclude that the growth speed of nano oxide particle was proportional to the difference value (
(t) −
(t)), and under a certain temperature, it was only influenced by the [Al] content in the micro area. The growth speed of nano oxide particles in molten steel could be controlled by adjusting these two parameters.
The formation process of oxide inclusions in molten steel could be divided into two stages. In the first stage, when the oxygen concentration in the initial steel was as high as 800–1000 ppm, the growth rate of particles was positively related to the concentration of alloy elements. At this stage, because of the high concentration, the growth rate of oxides was accelerated, and large particle inclusions were formed. It was feasible to remove inclusions floating in the liquid steel. In the second stage, when the oxygen concentration was low (30 ppm, or even a dozen ppm), the oxide particles formed in the molten steel were smaller (under 10 μm) with the decrease of the oxygen concentration, which cannot be removed in the molten steel. Then, due to the redistribution of solute, the oxygen concentration at the solid-liquid interface increased sharply, and the inclusion particles would further grow up, resulting in a higher final inclusion grade. Therefore, technology of multi-point regional micro-supply in-situ nano particle formation technology was adopted, which schematic diagram was shown in
Figure 10. When the oxygen concentration was low (30 ppm), in order to make the inclusions smaller, the twisted Al wire composed of multiple Al wires with small diameter instead of ordinary single Al wire with large diameter were fed in the molten steel. For the same volume of Al, the larger the specific surface area, the smaller the regional concentration of Al in the molten steel. Since the specific surface area of Al wire with small diameter was larger than that of the single Al wire with large diameter, by using multi-point regional micro-supply method the regional concentration of Al generated by contact with the oxygen in the molten steel was lower and the possibility of growing up for oxide particles was smaller. Fine oxide particles would form in the molten steel. At the same concentration, the number of oxide particles increased, which were dispersed in the molten steel. Using the heterogeneous nucleation of fine oxides, the inclusion-forming elements were attached to the fine oxides to refine the inclusions and optimize their shape, as shown in
Figure 8, with Al
2O
3 at the core position of the inclusions. The remaining elements were distributed at the core shell, forming a “core-shell” structure.
Author Contributions
Conceptualization: X.C. and Z.W.; methodology: S.L. and Y.W.; software: S.L.; validation: X.C. and Z.W.; formal analysis: Y.W. and W.F.; investigation: W.F. and X.Y.; resources: S.L. and W.F.; data curation: Y.W. and X.Y.; writing—original draft preparation: X.C., S.L. and W.F.; writing—review and editing: X.C. and Z.W.; visualization: W.F.; supervision: X.C., Z.W. and J.Y. All authors have read and agreed to the published version of the manuscript.
Funding
This work was supported by the National Natural Science Foundation of China (52071012, 51971031), the Academic and Technical Leaders of Major Disciplines in Jiangxi Province (20182BCB22020) and the Central Funds Guiding the Local Science and Technology Development-Fundamental Research (YDZX2021005).
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
The data presented in this study are available upon request from the corresponding author.
Conflicts of Interest
The authors declare no conflict of interest.
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