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Article

Microstructure and Wear Resistance of Ti5Si3/Ti3Al Composite Coatings Prepared by Laser Cladding on TA2 Titanium Alloy

1
State Key Laboratory of Materials Processing and Die & Mould Technology, Huazhong University of Science and Technology, Wuhan 430074, China
2
State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology, Wuhan 430070, China
*
Author to whom correspondence should be addressed.
Lubricants 2023, 11(5), 213; https://doi.org/10.3390/lubricants11050213
Submission received: 11 April 2023 / Revised: 3 May 2023 / Accepted: 5 May 2023 / Published: 9 May 2023
(This article belongs to the Special Issue Laser Surface Engineering for Tribology)

Abstract

:
In order to improve the wear resistance of titanium alloy, a Ti5Si3/Ti3Al composite coating with improved wear resistance was successfully prepared by laser cladding TA2 titanium alloy using the double-layer presetting method of Ti-63 wt.% Al mixed powder layer/Si powder layer. The microstructure, phase composition and wear resistance of the coating were studied using X-ray diffraction (XRD), scanning electron microscopy (SEM) and pin-disk friction and wear method. The results show that the coating is mainly composed of the Ti5Si3 primary phase and Ti5Si3/Ti3Al eutectic structure. The microhardness of the coating is higher than that of the matrix. The average microhardness of the coating is about 668 HV0.1, which is 3.34 times that of the matrix. The coating significantly improves the wear resistance of the TA2 matrix, and the mass wear rate is 1/5.79 of that of the TA2 matrix. The main wear mechanisms of the coating are abrasive wear, adhesive wear and oxidative wear, whereas the main wear mechanisms of the TA2 matrix are adhesive wear and oxidative wear.

1. Introduction

Titanium alloy has the advantages of low density, high specific strength and strong corrosion resistance, and has broad application prospects in aerospace, ocean engineering, medical devices and other fields. However, the low hardness and poor wear resistance of titanium alloy significantly restrict its service life under frictional conditions. In order to overcome the weakness of low hardness and poor wear resistance of titanium alloy, surface modification technology is widely used to prepare the coating on titanium alloy to improve the wear resistance of titanium alloy. At present, the commonly used surface modification technologies include ion implantation [1], plasma spraying [2,3], vapor deposition [4,5], micro-arc oxidation [6], laser alloying [7], laser cladding [8,9], etc. Among them, laser cladding is of high significance because of its advantages of metallurgical bonding with the matrix and adjustable coating thickness.
Based on the literature, it is known that two methods, namely, the powder presetting method [10,11,12,13,14,15,16,17,18,19,20] and the powder feeding method [7,9,21,22,23,24], are mainly used in the laser surface modification of titanium alloy. Among them, powder presetting methods reported in the literature all used single pure powder or mixed powder for one-time presetting, and there are no reports in the literature on the layered presetting method adopted in this paper. For users who cannot afford a laser cladding powder delivery system but need a laser cladding multi-component powder system, using the layered preset powder layer method can reduce the time of pre-mixing powder and improve work efficiency. Therefore, it is necessary to carry out the feasibility of the layered preset powder layer method. This is the purpose and significance of this paper. The hardness and wear resistance of the coating are greatly improved [8,9,10,11,12,13,15,17,18,19,20,21,22,23]. Ti-Al intermetallic compounds [19] and Ti5Si3 silicide [25,26] formed by laser surface modification of Al and Si elements have excellent wear resistance. The wear mechanisms of the coating and substrate are mainly abrasive wear and adhesive wear, respectively [27]. In addition, Ti5Si3 has a high melting point, low density, high hardness and good chemical inertness, whereas Ti3Al and TA2 titanium alloy have similar thermal expansion coefficients and melting points. Therefore, as long as the ratio of Ti5Si3/Ti3Al is appropriate, it is possible to obtain composite coatings with higher temperature resistance, wear resistance and corrosion resistance than the TA2 titanium alloy.
In this paper, a Ti5Si3/Ti3Al composite coating (which refers to the composite coating mainly composed of Ti5Si3 and Ti3Al phases with high hardness) was prepared on TA2 titanium alloy by laser cladding based on the layered presetting powder method, and the microstructure, phase composition and wear resistance of the coating were studied.

2. Materials and Methods

TA2 titanium alloy was selected as the matrix material, and its specific chemical composition is shown in Table 1. The TA2 titanium alloy with dimensions of 100 mm × 50 mm × 10 mm was selected as the substrate for laser cladding. The substrate was sanded and ultrasonically cleaned with ethanol before the powder was preset.
Al powder, Si powder and Ti powder with purity of 99.0 wt.% were selected as laser cladding powder materials in this paper. The powder layer was preset as shown in Figure 1. The thickness of each layer was about 0.4 mm, and the total thickness was about 0.8 mm. The binder used was 4 wt.% polyvinyl alcohol (PVA) aqueous solution. In order to ensure the homogeneity of Ti-63 wt.% Al mixed powder, the process of pre-ball milling was adopted in this paper. The specific parameters of the ball milling were as follows. The XQM-1.2L planetary ball milling produced by Xi’an Liyou Mechanical Equipment Co., Ltd., (Xi’an, China) was used; the weight ratio of the agate ball to powder was 6:1; the rotation speed of the ball milling was 180 r/min; and the ball milling time was 2 h.
Laser cladding was carried out using a Rofin 4 KW fiber laser produced by Rofin Laser Technology Co., Ltd. (Hamburg, Germany). During the laser cladding, argon gas with a purity of 99.999% was used as a protective gas to prevent oxygen in the air from entering the laser molten pool. After several laser cladding parameters were explored, the following optimized laser cladding parameters were finally adopted: laser power P = 1 KW; laser scanning speed V = 10 mm/s; laser spot diameter D = 2 mm; the overlapping rate of the laser spot f = 35%; Ar gas flow rate Vg = 16 L/min.
After laser cladding, the coating and TA2 substrate were cut into 9 mm × 9 mm × 10 mm samples using the wire cutting method, which were mainly used for the XRD phase composition test, SEM microstructure observation, coating microhardness test and wear resistance test. After wire cutting, all samples were cleaned ultrasonically, dried in a drying oven and then placed in a drying dish for later use. An HVS-1000A microhardness tester produced by Laizhou Huayin Test Instrument Co., Ltd., (Laizhou, China) was used to test the microhardness of the cross-section of the coating. The test parameters were as follows: a load of 100 g and a loading time of 15 s. Finally, the relationship curve between the microhardness HV and surface depth h was drawn according to the microhardness values at different depths.
The wear resistance of the coating and TA2 matrix was tested based on the principle of pin-disk friction and wear tests. The size of the wear sample was 9 mm × 9 mm × 10 mm. The wear device model was Ecomet300/Automet300. The parameters of the dry sliding friction and wear (Figure 2) were as follows: the rotary speed was 200 r/min, the applied load was 45 N, the dry sliding speed was 0.921 m/s, the dry sliding wear time was 5 min, the total wear distance was 276.32 m, and the grinding material was 200# SiC sandpaper. The mass of the samples before and after wear was measured using an SOP Quintix124-1CN electronic analysis balance, and the morphology of the wear was observed using SEM to study the wear mechanism of the coating and substrate.
Phase analysis was performed on the X ‘Pert PRO type X-ray diffractometer produced by PANalytical B.V. in the Netherlands (Almelo, The Netherlands). The test conditions were as follows: Cu target, wavelength λ = 0.15406 nm, tube pressure 40 kV, tube flow 40 mA, and 2θ scanning range of 10°~90°. The microstructure of the coating was observed using a ZEISS ΣIGMA HD scanning electron microscope made by Carl Zeiss (Jena, Germany). The micromorphology of the worn coating and TA2 matrix was observed using a JSM-7600F scanning electron microscope produced by JEOL (Akishima, Tokyo). The cross-section of the laser cladding coating should be inlaid, ground, polished and etched before the morphology analysis. The composition and proportion of the etching liquid used were HF:HNO3:H2O = 7:43:50 (volume ratio), and the etching time was 5~10 s.

3. Results

3.1. Microstructure of the Laser Cladding Coating

Figure 3 shows the XRD pattern of the laser cladding coating. It can be seen from the figure that the laser cladding coating is mainly composed of Ti3Al (JCPDS 00-052-0859) and Ti5Si3 (JCPDS 03-065-3597). The formation of these two phases is undoubtedly very favorable for improving the wear resistance of laser cladding coating because the hardness of Ti3Al and Ti5Si3 is 5.2 GPa and 11.3 GPa, respectively, both of which are higher than that of Ti (2 GPa). In the laser cladding process, the preset Si powder layer and Ti-63 wt.% Al mixed powder layer melts under the laser and reacts in situ with the partially melted matrix Ti to form Ti5Si3 (5Ti + 3Si = Ti5Si3) and Ti3Al (3Ti + Al = Ti3Al). According to the calculation results of Zhang [28], the above two reactions in the temperature range of 300~1500 K, ΔG and ΔH are negative. In terms of thermodynamics, a negative ΔH indicates that these two reactions are exothermic and a negative ΔG indicates that these two reactions can occur spontaneously.
Figure 4a shows the overall morphology of the cross-section coating. It can be seen from the figure that the thickness of the laser cladding layer is about 1 mm. There is a metallurgical bonding between the laser cladding layer and matrix, and no obvious porosity or cracks appear in the coating. Figure 4b–d show the amplified SEM morphologies of the different parts in Figure 4a. According to EDS results (Table 2) and XRD calibration results (Figure 3), it can be determined that the large black block in the coating is the primary Ti5Si3 phase, and the rest microstructure is a typical Ti3Al-Ti5Si3 eutectic structure. There are more primary Ti5Si3 near the top and middle of the coating (point 1 in Figure 4b and point 3 in Figure 4c), whereas the primary Ti5Si3 near the bottom of the coating is less and even completely becomes Ti3Al-Ti5Si3 eutectic structure (point 5 in Figure 4d). This type of microstructure is consistent with those reported by Vojtěch et al. [29] and Wu et al. [30]. Moreover, the components of Al, Si and Ti (see Table 1) also fall within the range of hypereutectic components of Ti3Al-Ti5Si3 reported in the literature [30,31,32].
The solidification process is as follows. After a high-power laser is applied to Ti-63 wt.% Al mixed powder layer and Si powder layer, Ti-63 wt.% Al mixed powder, Si powder and part of the Ti matrix melt after absorbing the laser energy. The three kinds of melts are mixed under the action of the stirring force of a molten pool. When the high-power laser leaves, the molten melt in the molten pool begins to solidify. First, the Ti5Si3 phase with a high melting point crystallizes, forming the primary Ti5Si3 phase. With a decrease in temperature, a high-temperature eutectic reaction occurs in the remaining liquid phase [29]:
L → β-Ti(Al,Si) + ε-Ti5(Si,Al)3
As the temperature continues to decrease, an isomeric transformation occurs in phase β-Ti(Al,Si) [29]:
β-Ti(Al,Si) → α-Ti(Al,Si)
When the temperature continues to decrease, an ordered reaction occurs in phase α-Ti(Al,Si) [29]:
α-Ti(Al,Si) → α2-Ti3(Al,Si)
Thus, when the temperature is lowered to room temperature, the resulting structure is the primary Ti5Si3 phase and α2-Ti3(Al,Si) + ε-Ti5(Si,Al)3 is the eutectic structure.
It should be pointed out that in the literature [28], a single-layer presetting method was adopted to laser cladding Ti, Al and Si mixed powders on Ti-6Al-4V titanium alloy, where the thickness of the presetting powder was 0.6~0.8mm. The prepared coating was mainly composed of Ti5Si3, Ti7Al5Si12, Ti3AlC2, Ti3Al, TiAl, TiAl3 and α-Ti, which is much more complex than the coating prepared by the double-layer presetting method in this paper. This may be related to the flow regularity of Ti, Si and Al powders during the laser action. During the process of laser action, there is a large temperature gradient on the upper and lower surfaces of the molten pool, thus forming a very steep surface tension. The surface tension causes a strong convection in the molten pool, and the convection in the molten pool can produce a strong stirring force so that the liquid metal in the molten pool is mixed evenly. Convection in the molten pool mainly comes from three aspects. First, convection in the molten pool comes from the energy distribution of the laser beam. The Gaussian laser beam used in this experiment can cause severe convection in the molten pool [33]. The second factor is the protective gas blown out in order to prevent the oxidation of the liquid metal at high temperatures. This high-pressure protective gas can produce a certain stirring effect and promote the diffusion of the liquid metal. Third, at high temperatures, the thermal expansion of liquid metal causes a certain density difference in the molten pool, so buoyancy is generated in the molten pool, and the existence of buoyancy causes natural convection of the melt [34]. These three factors that make the layer preset powder can also form a single-layer preset powder structure to reduce the powder mixing time and improve production efficiency.

3.2. Wear Properties of the Laser Cladding Coating

Figure 5 shows the microhardness distribution of the laser cladding coating. As can be seen from the figure, the average microhardness of the coating is about 668 HV0.1, which is 3.34 times that of the TA2 matrix (200 HV0.1). Since the microhardness of Ti5Si3 and Ti3Al is 1500 HV [28] and 530 HV0.2 [35], respectively, the microhardness of the laser cladding coating is mainly due to the existence of these harder intermetallic compounds (Figure 3) and fine-grain strengthening due to rapid solidification during laser cladding. Obviously, an increase in the microhardness of the coating is beneficial to the improvement of the wear resistance of the coating.
Figure 6 shows a comparison of the mass wear rates of laser cladding coating and TA2 matrix under dry friction and wear conditions at room temperature. As can be seen from the figure, under the conditions of dry friction loading of 45 N and wear distance of 276.32 m, the mass wear rate of the TA2 matrix is 16.22 mg/min, and that of laser cladding coating is 2.8 mg/min, about 1/5.79 of TA2 matrix. Therefore, the wear resistance of the laser cladding coating is 5.79 times that of the TA2 matrix; that is, the wear resistance of the laser cladding coating is obviously better than that of the TA2 matrix. It is known that the higher the hardness of a material, the better the wear resistance [36]. The average microhardness of the laser cladding coating is 3.34 times that of the TA2 matrix (Figure 5), so the wear resistance of the laser cladding coating is better than that of the TA2 matrix.
It should be pointed out that the improvement factor of wear resistance of the laser cladding coating relative to TA2 matrix is significantly higher than that reported in the literature [37]. In the literature [37], Ti2SC/TiS composite coating was prepared on TA2 matrix by laser cladding, and the wear rate of TA2 matrix was 3 times that of the composite coating, which was less than 5.79 times that of the coating in this paper.
Figure 7 shows the SEM morphology of TA2 matrix and laser cladding coating after dry friction and wear. Table 3 shows the EDS results of the worn TA2 matrix and laser cladding coating. According to the SEM morphology of the TA2 matrix after wear in Figure 7a,b, it can be seen that the TA2 matrix after dry friction and wear presents adhesive wear characteristics of being pressed. At the same time, there are deep and wide pear grooves, and there are a large number of fine particles in the grooves. The EDS results in Table 3 show that during dry friction and wear of TA2 matrix, a large number of fine TiO or TiOx particles are generated due to surface friction heat generation and oxidation. As the abrasive material is SiC with a microhardness of 3200 HV [28], its microhardness is much higher than that of the TA2 matrix. Therefore, under the condition of dry friction and wear, the hard abrasive SiC continuously presses TA2 matrix, causing the surface of the matrix to be scratched and flattened. At the same time, due to the heat generated by dry friction, the Ti in TA2 matrix is oxidized into an incomplete valence TiOx [38]. Therefore, the main wear mechanisms of TA2 matrix are adhesive wear and oxidative wear.
Figure 7c,d show the SEM morphologies of the laser cladding coating after dry friction and wear. Combined with the EDS results in Table 3, it can be seen that after dry friction and wear, furrows of different depths and widths and wear particles of different sizes appear on the surface of the coating. Due to the heat generated by dry friction, most oxidation reactions occur and different oxides are generated, but the furrows of all the coatings are shallow and narrow. The different groove depths and widths of the coating should be closely related to the surface microhardness of the coating, and the different sizes of the coating wear particles should be related to the type and volume fraction of the intermetallic compounds in the coating. In general, the larger the volume fraction of Ti5Si3 phase with higher microhardness in the coating, the smaller the particles, the more severe the abrasive wear of the coating, the more spalling wear particles, the shallower the groove, the lighter the adhesive wear, and the more severe the oxidation wear. However, because the microhardness of the coating is lower than that of the hard anti-abrasive material SiC, abrasive wear, adhesive wear and oxidation wear coexist.
In summary, the wear mechanisms of TA2 matrix are mainly adhesive wear and oxidative wear, whereas the wear mechanisms of coating are abrasive wear, adhesive wear and oxidative wear that co-exist, which is similar to the results reported in the literature [27,39,40].

4. Discussion

4.1. Formation and Flow Characteristics of the Laser Cladding Molten Pool with Double-Layer Preset Powder Layer

As a relatively economical and new surface modification technology, laser cladding can significantly improve the surface properties of substrate materials such as wear resistance, corrosion resistance and oxidation resistance. The laser cladding process is a non-equilibrium, instantaneous and non-uniform physicochemical metallurgical process. The heat conduction and melt flow in the molten pool determine the microstructure, grain morphology and defect types of the cladding layer, thus affecting the properties of the materials and the service life of the parts.
In the case of laser cladding of the double-layer preset powder layer (Figure 1), under the action of the laser beam, the double-layer preset powder layer absorbs the laser energy and melts quickly to form a molten pool. When the laser beam leaves the molten pool, it solidifies quickly. There are three heat transfer modes in this preset laser cladding: heat radiation from the laser to the powder layer, heat convection between the protective gas and powder layer, and heat conduction between the powder layers [41]. These three heat transfer modes lead to complex physical phenomena, such as melting, solidification and phase transformation during laser cladding. Figure 8 shows a schematic diagram of the flow behavior of the cross-section molten pool during laser cladding with a double-layer preset powder layer.
During the laser action, the double-layer preset powder layer and part of the substrate melt rapidly due to the absorption of laser energy, forming a large and uneven temperature gradient, resulting in a tension gradient on the surface of the molten pool. Generally, a symmetrical surface tension gradient is generated on the left and right sides of the symmetrical line at the center of the molten pool. Due to the influence of surface tension, the high-temperature melt in the center of the molten pool flows to the surface of the molten pool. At the same time, under the comprehensive action of buoyancy, gravity and other factors, the high-temperature melt flows to both sides along the surface near the center point of the interface. The closer the area is to the edge, the more intense the melt flow and the higher the velocity. Due to the continuity of movement, the low-temperature melt reaching the edge of the molten pool flows along the solid–liquid boundary towards the bottom of the molten pool, and then converges and rises in the middle area of the molten pool, forming the left and right circulating flows of the molten pool (see blue arrows in Figure 8), respectively.
In particular, the change in the surface temperature of the laser molten pool causes a change in the surface tension gradient of the fluid and induces the flow of the surface fluid from the region of low surface tension to the region of high surface tension. This Marangoni flow is the main driving force for mass transmission in the molten pool [42]:
γ = γ0 + σ(T − T0)
where: γ0 is the surface tension at the reference temperature T0; σ is the surface tension coefficient.
Moreover, in the process of laser cladding, in addition to the influence of laser cladding process parameters on the temperature field and velocity field of the molten pool, the surface tension coefficient of the material also has an impact on the temperature field and velocity field of the molten pool [43]. When the surface tension coefficient of the material is less than 0, the melt in the molten pool flows from the laser center to the edge of the molten pool. When the material surface tension coefficient is greater than 0, the melt in the molten pool flows from the edge of the molten pool to the laser center, but the peak velocity of both fluid flows appears at the edge of the molten pool surface. The surface tension coefficients of Ti, Si and Al powders used in this paper are −0.16 mN/m, −0.25 mN/m and −0.25 mN/m [44], respectively, which are all negative values, so the flow of the molten pool belongs to the former.
In particular, in the stable zone of the laser cladding layer, the molten pool tends to be stable as the heat input reaches a dynamic equilibrium with the heat lost due to heat transfer. Moreover, under the action of Marangoni flow, the molten double-layer preset powder layer and part of the substrate are mixed and stirred in the molten pool to promote the homogenization of the alloying elements in the molten pool.
In conclusion, under the action of Marangoni flow, Al, Si and Ti alloying elements in the molten pool can be evenly mixed to obtain the effect of laser cladding of a single preset powder layer, and then obtain the laser cladding layer microstructure with basically a uniform composition to ensure the performance and service life of the coating.

4.2. Formation Mechanism of Different Phases in the Coating

In the laser cladding double-layer preset powder layer, once the molten pool is formed, the melted Ti-63 wt.% Al powder layer, the melted Si powder layer and the partially melted TA2 matrix mix with each other under the action of Marongoni flow stirring force. According to the isothermal section diagram of the Ti-Al-Si ternary system at 1000 °C [45], Ti-Al intermetallic compounds and Ti-Si ceramic reinforced phases can be formed by different in situ reactions of Ti, Al and Si powders in different proportions. In addition, according to the Ti-Al binary phase diagram [46], there are mainly TiAl3, TiAl2, TiAl and Ti3Al among Ti-Al intermetallic compounds. The melting point of Ti3Al is 1600 °C, which is higher than that of TiAl2 (1425 °C), TiAl (1465 °C) and TiAl3 (1340 °C). According to the Ti-Si binary phase diagram [46], TiSi2, TiSi, Ti5Si4, Ti5Si3, Ti3Si and other compounds can be generated when Ti reacts with Si. The melting point of Ti5Si3 is 2130 °C, which is the highest melting point of Ti-Si compounds. In addition, according to the calculation results of Zhu [47], the enthalpy changes in ΔH and Gibbs free energy ΔG of Ti5Si3 are the lowest among Ti-Si compounds, so Ti5Si3 is the easiest to obtain by solidification first when the composition is appropriate. Si has a low solubility in the Ti-Al phase, and Ti5Si3 has a high melting point, so Ti5Si3 is the easiest to form in the laser cladding process [48]. Therefore, in this paper, a preset powder scheme was designed according to the location range of the Ti5Si3 + Ti3Al phase generated in the literature [45], which was finally verified; that is, only the Ti5Si3 and Ti3Al phases were generated in the coating.

4.3. Wear Mechanism of the Coating and TA2 Matrix

As we all know, friction and wear is an extremely complex process. Compared with lubricating friction, dry friction without lubricating medium results in a more intense friction process, more severe wear, and shorter effective working life of friction pairs. The wear amount is a basic parameter that reflects the wear resistance of the material. The smaller the wear amount per unit time, the better the wear resistance. Wear resistance refers to the ability of the material itself to resist wear damage, and it is usually expressed by the amount of wear. There is a negative correlation between the wear amount and wear resistance; that is, the smaller the wear amount, the better the wear resistance.
The mathematical model of material wear can quantitatively describe the wear process and calculate the normal working life of the friction pairs to better grasp the essence of the wear problem, reduce and control the wear degree, and improve the reliability of the friction pair. In 1953, Archard [49], a professor at the University of Leicester, proposed a computational model for adhesive wear. Archard’s wear calculation formula is as follows:
Q = k × (NL)/H
where, Q is the amount of adhesive wear on the contact surface; K is the coefficient of adhesive wear, representing the probability of an abrasive particle generated by mutual friction between a pair of micro-convex bodies; N is the normal pressure; H is the hardness of the soft surface materials; L is the relative sliding distance.
Archard’s adhesive wear theory describes the general rules of material wear. The wear amount is proportional to the displacement and positive pressure and inversely proportional to the hardness of the softer materials. It connects the wear with the material properties, which makes it convenient to calculate the wear amount. It can be seen that hardness is an important index to evaluate material properties. In general, the higher the hardness, the better the wear resistance of the material.
Specifically in this paper, on the one hand, it can be seen from Figure 5 that the microhardness of the laser cladding coating is higher than that of the TA2 matrix. Therefore, under the same conditions, the wear resistance of the laser cladding coating is better than that of the TA2 matrix (Figure 6).
On the other hand, the wear resistance of materials depends not only on the hardness of the materials but also on the hardness of the abrasives. The microhardness of Ti5Si3, Ti3Al, TA2 and SiC are 1500HV [28], 530HV0.2 [35], 200HV0.1 (Figure 5) and 3700HV [28], respectively. Therefore, when the applied load is 45N, it is inevitable that the wear mechanism of the TA2/SiC friction pairs is different from the coating (Ti5Si3 + Ti3Al)/SiC friction pairs. That is, although the two groups of friction pairs cause oxidative wear due to the heat generated by dry friction and wear (as evidenced by the appearance of the O element in Table 3) and the hardness difference of the TA2/SiC friction pairs is larger, TA2 is prone to plastic deformation and adhesive wear, whereas the hardness difference of the coating (Ti5Si3 + Ti3Al)/SiC friction pairs is relatively small. Ti5Si3 (Ti3Al) is prone to brittle fracture and abrasive wear; however because the hardness of Ti5Si3 (Ti3Al) is lower than that of SiC, adhesive wear also occurs. In conclusion, the TA2/SiC friction pairs mainly exhibit adhesive wear and oxidative wear, whereas the coating(Ti5Si3 + Ti3Al)/SiC friction pairs mainly exhibit abrasive wear, adhesive wear and oxidative wear.

5. Conclusions

(1)
The wear-resistant Ti5Si3/Ti3Al composite coatings were successfully prepared on TA2 titanium alloy by laser cladding using the double layer preset method of Ti-63 wt.% Al mixed powder layer/Si powder layer.
(2)
The coating is mainly composed of coarse primary Ti5Si3 phase and fine Ti5Si3/Ti3Al eutectic structure, with more Ti5Si3 on the top layer and in the middle of the coating and more Ti5Si3/Ti3Al eutectic on the bottom.
(3)
The mass wear rate of the laser cladding coating is 1/5.79 of that of the TA2 matrix. The wear mechanisms of the coatings are mainly abrasive wear, adhesive wear and oxidative wear, whereas the wear mechanisms of the TA2 matrix are adhesive wear and oxidative wear.
(4)
The effect of laser cladding of the double preset powder layer is similar to that of the single preset powder layer because of the strong stirring effect of the Marongoni flow in the molten pool.

Author Contributions

Investigation—K.H. and W.H.; writing—original draft preparation, W.H.; writing—review and editing, K.H. All authors have read and agreed to the published version of the manuscript.

Funding

This work was supported by the Open Project Program (No. 2022-KF-19) of the State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, Wuhan University of Technology.

Data Availability Statement

The data of this study are available from the corresponding author upon reasonable request.

Acknowledgments

The authors are grateful to the Analytical and Testing Center of Huazhong University of Science and Technology.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Schematic diagram of presetting powder layer.
Figure 1. Schematic diagram of presetting powder layer.
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Figure 2. Schematic diagram of dry friction and wear experiment of laser cladding coating.
Figure 2. Schematic diagram of dry friction and wear experiment of laser cladding coating.
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Figure 3. XRD pattern of the laser cladding coating.
Figure 3. XRD pattern of the laser cladding coating.
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Figure 4. SEM morphology of the cross-section coating: (a) whole; (b) locally amplified at position A in (a); (c) locally amplified at position B in (a); (d) locally amplified at position C in (a).1, 2, 3, 4 and 5 in figure represent the location points of the EDS test, respectively.
Figure 4. SEM morphology of the cross-section coating: (a) whole; (b) locally amplified at position A in (a); (c) locally amplified at position B in (a); (d) locally amplified at position C in (a).1, 2, 3, 4 and 5 in figure represent the location points of the EDS test, respectively.
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Figure 5. Microhardness distribution of the laser cladding coating.
Figure 5. Microhardness distribution of the laser cladding coating.
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Figure 6. Comparison of mass wear rate between laser cladding coating and TA2 matrix.
Figure 6. Comparison of mass wear rate between laser cladding coating and TA2 matrix.
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Figure 7. SEM morphology of the worn TA2 matrix and laser cladding coating. (a) Whole SEM morphology of the worn TA2 matrix; (b) local amplified SEM morphology of the worn TA2 matrix in area A in Figure 6a; (c) whole SEM morphology of the worn coating; (d) local amplified SEM morphology of the worn coating in area B in Figure 6c. 1, 2, 3, 4, 5, 6, 7, 8, 9, 10 and 11 in figure represent the location points of the EDS test, respectively.
Figure 7. SEM morphology of the worn TA2 matrix and laser cladding coating. (a) Whole SEM morphology of the worn TA2 matrix; (b) local amplified SEM morphology of the worn TA2 matrix in area A in Figure 6a; (c) whole SEM morphology of the worn coating; (d) local amplified SEM morphology of the worn coating in area B in Figure 6c. 1, 2, 3, 4, 5, 6, 7, 8, 9, 10 and 11 in figure represent the location points of the EDS test, respectively.
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Figure 8. Schematic diagram of flow behavior of cross-section molten pool during laser cladding with double-layer preset powder layer.
Figure 8. Schematic diagram of flow behavior of cross-section molten pool during laser cladding with double-layer preset powder layer.
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Table 1. Chemical composition of TA2 (wt.%).
Table 1. Chemical composition of TA2 (wt.%).
ElementFeSiCNHOTi
Content0.20.10.10.050.0150.1Bal.
Table 2. EDS results of the cross-section coating at different points.
Table 2. EDS results of the cross-section coating at different points.
Different PointsTi (at.%)Al (at.%)Si (at.%)Possible Phases
160.794.8334.38Ti5Si3
270.0019.8210.18Ti5Si3/Ti3Al
361.234.7034.07Ti5Si3
478.8312.188.99Ti5Si3/Ti3Al
575.0619.725.22Ti5Si3/Ti3Al
Table 3. EDS results of worn TA2 matrix and coating.
Table 3. EDS results of worn TA2 matrix and coating.
Different PointsTi (at.%)Al (at.%)Si (at.%)O (at.%)Possible Phases
191.80--8.20Ti + TiOx
251.11--48.89TiO
3100.00---Ti
492.11--7.89Ti + TiOx
587.00--13.00Ti + TiOx
643.342.5224.7829.36Ti5Si3 + Al2O3 + TiO2
764.695.2730.03-Ti5Si3 + Ti3Al
845.002.9622.9929.08Ti5Si3 + Al2O3 + TiO2
945.542.1729.4022.88Ti5Si3 + Al2O3 + TiO2
1040.922.3124.3732.39Ti5Si3 + Al2O3 + TiO2
1158.5814.184.8022.43Ti3Al + TiO2 + SiO2
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Huang, K.; Huang, W. Microstructure and Wear Resistance of Ti5Si3/Ti3Al Composite Coatings Prepared by Laser Cladding on TA2 Titanium Alloy. Lubricants 2023, 11, 213. https://doi.org/10.3390/lubricants11050213

AMA Style

Huang K, Huang W. Microstructure and Wear Resistance of Ti5Si3/Ti3Al Composite Coatings Prepared by Laser Cladding on TA2 Titanium Alloy. Lubricants. 2023; 11(5):213. https://doi.org/10.3390/lubricants11050213

Chicago/Turabian Style

Huang, Kaijin, and Wanxia Huang. 2023. "Microstructure and Wear Resistance of Ti5Si3/Ti3Al Composite Coatings Prepared by Laser Cladding on TA2 Titanium Alloy" Lubricants 11, no. 5: 213. https://doi.org/10.3390/lubricants11050213

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