# Effects of Process Parameters on Geometrical Characteristics and Microstructure of TiC Particle-Reinforced Co50 Alloy by Laser Cladding

Authors: Nga Pham Thi-Hong
Journal: Advances in Materials Science and Engineering
 (2021)

---

## Abstract

Laser cladding of Co50 alloy coating and Co50 composite coatings doped with 10, 20, and 30 wt.% TiC particles was performed on the H13 steel surface. The effects of TiC concentration on the phase composition, microstructure, and microhardness of the coatings were studied. The results indicated that, in 10% TiC coating, the “bright band” is a quite flat-growth tissue, while with 20% TiC, the “white bright band” contains a large amount of black TiC particles. The composite coating Co50, 10% TiC, and 20% TiC samples can clearly distinguish the cladding zone, bonding zone, and heat-affected zone, and a good metallurgical bond is formed between the coating and the substrate. The 30% TiC coating and the substrate are not well bonded, which is attributed to the high TiC content in the coating; however, it has the best surface morphology, and there is no porosity on the surface. 10% TiC coatings have poor surface quality, show a spraying material phenomenon on two side edges which is quite serious, and a lot of porosity on the surface of the coating. In addition, 10% TiC coating includes the original TiC particles and primary TiC particles that are precipitated in situ from the liquid phase during solidification; 20% TiC coating indicates a large amount of TiC in the form of cross petals and twigs, and the figure points out that TiC exists like a large number of diffusely distributed spherical structures in the 30% TiC coating. The coatings of TiC/Co composite with less than 20% TiC showed good metallurgical bonding characteristics with the H13 steel surface.


---

## Body

## 1. Introduction

H13 hot work molds are constantly subjected to physical and chemical wear and tear, thermal fatigue, erosion, stress corrosion, surface thermal welding, and other physical and chemical effects, as well as the effects of cold and hot alternating and impact loads during mechanical production and use. In this harsh environment, the mold is prone to failure in the form of thermal fatigue, thermal wear, and cracking, which leads to a significant reduction in the life of the mold. As one of the important parts of automobile engines, connecting rods have high requirements on their weight and appearance quality. The shape and size of the connecting rod are guaranteed by forging. The workpiece in the final forging process of the connecting rod is a preform after preforging of the bar material, the big end is the round bar material, and the small end has been flattened (as shown in Figure1). The large-end projection of the forging die first comes into contact with the workpiece, and the plastic deformation of the workpiece begins to enter the forging model groove; when the two ends of the workpiece are plastically deformed, they contact the bridge, then the flow is blocked, and the workpiece gradually fills the groove. Therefore, this requires that the connecting rod forging die must have a very high precision, which also puts forward higher requirements on the die material.Figure 1
Hot die forging of the connecting rod and detail of the surface of the used H13 forging die showing severe plastic deformation.Machining after forging has been a traditional manufacturing method widely used in hot forging dies [1, 2]. How to improve the life of hot forging dies has always been one of the main tasks of forging die researchers. The traditional method of welding repair is used to repair the mold at the root of the groove, so that the mold can continue to be used without being scrapped. In response to this problem, existing studies have shown that laser repair of the H13 steel surface is a very effective method, and many researchers have also achieved some results in their laser surface modification [3, 4]. Due to the rapid development of processing technology in the world, 1–20 kW lasers have been mass produced and used in many engineering fields; 100 kW high-power lasers and 3D five-axis CO2 lasers have been successfully developed and started to be popularized. Now, it has begun to develop high-power CO2 lasers, and the most widely used lasers are 1–5 kW.In recent years, China and other countries in the world have conducted more research on laser cladding (LC) technology, and it has reached the stage of industrial application. From LC powder materials, one of influencing factors of LC layer, many research studies have been conducted. According to previous studies, the hardness, wear resistance, and corrosion resistance of H13 steel can be improved to a certain extent after LC. Cao et al. [5] used a 5 kW cross-flow CO2 laser to prepare a Ni60A coating on the surface of H13 steel. The analysis showed that the coating and the substrate formed a good metallurgical bond, and the coating microhardness, which was 800–900 HV, was significantly higher than that of H13 steel. He used a 5 kW cross-flow CO2 laser to prepare Ni-based and Co-based coatings on the surface of H13 steel through multipass lap large-area cladding. Research shows that a good metallurgical bond is achieved between the coating and the substrate, and the microhardness of the multilayer lap coating is Ni60A ⟶ Co50 ⟶ Co42 ⟶ H13 from high to low. Through a long-term high-temperature oxidation test, the hardness of Co-based alloy at high-temperature oxidation is studied. There is no decline; that is, Co-based alloy is better than Ni-based alloys [6]. In addition, in order to further improve the performance of the coating, researchers added various particle reinforcement phases to the cladding powder. Zhang et al. [7] conducted laser cladding WC particle-reinforced Ni-based powder experiments on the surface of H13 steel. The experiment showed that the coating has a dense structure, no cracks, pores, and other defects; the grain is refined, and it is firmly bonded to the substrate. A similar result was reported by Shao-yi et al. [8]; they used a 7 kW cross-flow CO2 laser to prepare a WC-Ni/TiC coating on the surface of H13 steel by LC. The results show that nano-TiC improves the hardness and toughness of the coating through dispersion strengthening and fine-grain strengthening.Although LC technology has been widely used in parts repair and other fields, there are still many problems in the technology. Cracks and pore defects in the cladding layer are the main problems to be solved by material workers. The cracks of the LC layer are mainly related to four aspects: laser process parameters, process conditions, coating materials, and substrate conditions. In other words, the way to control the generation of cracks in the LC layer can be achieved by optimizing the laser process parameters, optimizing the process conditions, rationally designing the composition of the cladding layer, and improving the substrate condition. These measures are beneficial to reduce the source of cracks and pores and reduce the occurrence of cracks and pores. For the cracking of the coating, the researchers proposed the following solutions or mitigations:(1)
From the technical means, we optimize the process parameters and perform preheating and postheating treatment. In the actual preparation process, in order to further enhance the overall performance of the metal-ceramic composite coating, most of the current research focuses on various treatment methods after LC. Liu [9] used Co-based/WC mixed powder for powder feeding LC. The results showed that the cladding layer reheating treatment at 850 °C can achieve the purpose of stress relief annealing; the cladding layer is suitable for working under the environment of repeated heating and cooling in this temperature range. Studies of Chen et al. [10] have shown that, after laser remelting of the WC/Co plasma sprayed layer on the surface of 45 steel, an LC layer with a metallurgical interface is obtained, which eliminates the pores and cracks in the plasma-sprayed layer, and its structure and performance are obviously improved. Li et al. [11] also sprayed a layer of WC-12Co coating on a 45 steel surface and then performed laser remelting treatment. It was found that its wear resistance was nearly 3 times higher than that of the matrix structure.From the existing literature, it can be seen that double-layer coating and multilayer coating cannot eliminate the problem of performance mismatch between the substrate and the coating and between the internal layers of the coating. In this regard, researchers began to explore the use of gradient coating, laminated cladding, or the introduction of a transition layer between the coating and the substrate. The purpose of the laminated cladding method is that, along the thickness direction of the coating, the content of the ceramic phase component gradually increases, and the content of the metal phase component decreases accordingly. The distribution law of ceramic particles in the coating shows a step change, the metal phase and the ceramic phase. There is no obvious interface between the coatings, so that the stress in the coating is weakened or eliminated to the greatest extent, and the bonding strength between the coating and the substrate is improved. The work of Xu et al. [12] adopted the layered cladding method to change the content and particle size of ceramic particles in the mixed powder layer by layer. After multiple layers of cladding, the distribution of ceramic particles in the coating showed a step change. However, there is no substantial difference between the layered gradient coating and the method of introducing a transition layer between the coating and the substrate, but the number of transition layers is increased. Some authors [13, 14] prepared a gradient-structure TiC/Ni-based composite coating by a one-step laser coating method and proposed to use the flow and solidification behavior of the laser melt pool, relying on the continuous growth and regular movement of TiC particles in the melt pool, which can automatically achieve the coating continuous gradient structure.(2)
From the aspect of alloying element toughening, toughness phases such as Ni and Co are added. From the aspect of grain refinement, rare earth oxides, some nanopowders, or a small amount of other metal elements are added to the cladding layer. Bisides, ultrasonic vibration or electromagnetic vibration is also applied [15]. Qiang, Fu [16] added an appropriate amount of In2O3 to the WC/Ni-based alloy powder to obtain a high-quality cladding layer without pores on A3 steel. Studies have shown that the addition of In2O3 inhibits the decomposition of WC, thereby reducing the content of C in the molten pool, reducing the possibility of forming CO and CO2 in the molten pool. Chen et al. [17] added a certain amount of metal reducing agent Ti during the cladding of WC/Co cemented carbide with laser powder feeding, which effectively suppressed the porosity. However, Ti powder and In2O3 are expensive, and their use will increase the cladding cost to some extent. On the other hand, Al and C can better combine with oxygen to form Al2O3 with high chemical stability, which reduces the oxygen content in the molten pool, thereby effectively inhibiting the generation of stomata. Because the density of Al2O3 is very small, Al2O3 will float on the surface of the cladding layer to form slag during the cladding process, which further protects the cladding layer [18]. A similar result was reported by Xiao-Wei [19, 20]; the results showed that the addition of Al2O3 has the effect of changing the microstructure and performance of the LC layer. The microstructure is refined, and wear resistant has been significantly improved. Several authors prepared nano-Al2O3/Co-based coatings on the surface of Ni-based superalloys. The results showed that the addition of nano-Al2O3 changed the growth morphology of the interface from elongated columnar dendrites to shorter dendrites; when the content of nano-Al2O3 is more than 1%, an equiaxed dendrite structure is obtained on the entire section; nano-Al2O3 serves as the core of heterogeneous nucleation, which refines the structure; nano-Al2O3 is unevenly distributed in the cladding layer, which promotes the transformation of γ-Co to ε-Co [21, 22].In general, using optimized process parameters, preheating, postheat treatment, adding tough phase, adding rare earth oxides, adding a small amount of other metal elements, or performing ultrasonic vibration or electromagnetic vibration on the cladding layer have achieved good results, but did not fundamentally solve this problem. The reason is mainly because LC uses thermal spray alloy powder for a long time, but there is no series of alloy powder specially used for the LC process. In addition, because there is a significant difference between the thermal expansion coefficient and the elastic modulus between the metal-based alloy and the strengthened ceramic phase, this will cause a temperature gradient in each phase in the molten pool, thereby causing thermal stress and the formation of holes and cracks. In the abovementioned research, alloying elements such as B and Si, which are relatively high in self-fusible alloy powder, are prone to form low-melting liquid films such as borosilicate in the laser melt pool, and the liquid film breaks during the rapid solidification of the laser melt pool. It is easy to become a source of cracks later [23]. From this perspective, trying to reduce the content of B and Si elements in the traditional self-fusible alloy powder should reduce the tendency of crack formation. Wang et al. used self-designed alloy powder to reduce the content of B and Si elements. The results show that by controlling the content of B and Si elements, crystal cracks can be prevented and performance requirements can be met [24]. However, the content of B and Si elements should not be too small because the reduction of these two elements in the powder will inevitably cause a decrease in the surface finish of the cladding layer [25, 26].From the results of the abovementioned research, during the LC process, on the one hand, the difference in the temperature gradient and thermal expansion coefficient between the cladding layer and the base material often causes the mold surface to be uneven, and the composition of the cladding layer is not uniformly controlled. On the other hand, due to moisture and oxidation during cladding of the coating powder before cladding, pores are easily generated in the cladding layer; in addition, due to the extremely fast laser heating and cooling speed, the mold surface is prone to burn damage, deformation, cracks, and other phenomena. In order to solve this problem, several authors used LC technology to prepare H13-TiC composite coatings with different TiC content on the surface of H13 steel. The analysis believed that the combined effect of dispersion and fine-grain strengthening in the cladding layer and the hardness and strength of the coating after LC are significantly higher than those of the substrate, but with the increase in TiC content, the presence of too much second phase increases the chance of crack nucleation and propagation, resulting in a decrease in the tensile strength and fracture toughness of the composite material [27]. Xiaodan et al. [28] showed that the scanning speed has a greater influence on the morphology and size of the particles; the TiC content has a great influence on the morphology and particle size of the fine precipitated TiC; and with the increase of TiC, the corrosion resistance decreases.Beside the LC parameters, the cladding material plays a critical role in the formation of a high-quality coating. The cladding material system varies from single alloy to multiple ceramics or alloys. In this, the melting alloy layers of the metal platform technology have developed rapidly, intending to enhance the corrosion resistance of a material such as Co-based alloys, Ti-based alloys, Fe-based alloys, and Ti-based alloys. From the perspective of the repair layer material, Co-based alloy coating can obtain high oxidation resistance, high temperature strength, high temperature hardness, and thermal fatigue resistance, which is very suitable for hot work of die steel. In a recent paper, Zhang et al. [29] performed LC on the surface of 2Cr13 stainless steel. The test results show that, by selecting appropriate laser irradiation process parameters, a Co-based alloy coating with an excellent performance can be obtained. In addition, Li et al. [30] used laser-clad Hoganas Co-based alloy on a Ni-based cast superalloy/45# steel substrate with a broadband and narrow-band laser to prepare a defect-free coating; the result showed that a new type of fine dendrites with a crystalline direction parallel to the laser scanning speed was found. From the current research status, the addition of WC, B4C, SiC, Cr2C3, TiN, and other ceramic particles to the Co-based alloy can significantly improve the performance of the coating. Songhua et al. [31] prepared Co55 alloy coating, Co-based/20% ​​SiCp (CoSiC) coating, and Co-based/20% ​​B4Cp (CoB4C) on a 16 Mn steel surface. It is found that CoSiC coating and CoB4C coating have higher hardness and better wear resistance than Co55 coating, in which CoSiC coating has the highest hardness and wear resistance. Among carbide ceramic particles, TiC has high hardness, good thermal stability, high melting point, and good resistance to high-temperature oxidation. Studies of Emamian et al. [32, 33] showed that compared with WC, TiC has a lighter weight and higher hardness and has a better effect than WC as a reinforcement and can obtain higher wear resistance. Although the ceramic phase can improve the hardness, its thermal and physical properties differ greatly with the metal matrix. For example, the melting point of the ceramic phase is much higher than that of the metal matrix, and the thermal expansion coefficient, elastic modulus, and thermal conductivity are very different. The temperature gradient of the molten pool area formed after laser irradiation is very large, resulting in large thermal stress, so the coating often has holes and microcracks [34–37]. This requires materials workers to further study the behavior of carbides in the LC layer, as well as the basic theory and production process of laser surface strengthening, which lays a foundation for the successful application of LC carbide/metal-based composite coatings in actual production.


## 2. Materials and Methods

H13 steel was selected for the experiment, and its chemical composition is shown in Table1; a steel sample of 30 mm × 10 mm x 100 mm was used. Before testing, the samples are cleaned, rinsed with alcohol and acetone, and then, dried by using an oven. Self-melting Co50 alloy powders have the chemical components listed in Table 1, with particle size ∼ 53 μm; TiC powders have 1 ∼ 10 μm particle size (Figure 2).Table 1
Chemical composition of H13 steel and Co50 alloy powder used in experiments (% by weight).
ElementCSiCrMoVMnFeWBNiCoH13 steel0.431.174.791.380.940.48Bal.————Co50 alloy0.63.520.05.1——5.03.02.2514.0Bal.Figure 2
Topography of TiC powder used for laser cladding.The process is coating the test sample by a preplaced powder layer using a homemade binder and then applying LC to melt it. Preplaced powder layers include a Co50 alloy powder layer and a Co50 + 10%, Co50 + 20%, and Co50 + 30% TiC composite powder layer (% by weight), with ∼ 1 mm thickness. n electronic balance is used to weigh the cladding powder according to the abovementioned composition ratio. Before the experiment, those preplaced powder layers were added with a 3 wt.% homemade binder polyvinyl alcohol organic adhesive on the surface of H13 steel. After preplacing, the thickness is about 1 mm. The preplacing coating sample was dried by using the oven for 8 hours before being melted away by LC.Laser cladding of Co50 and Co50/TiC coatings is made on the type of GS-6000 TFL transverse-flow CO2 with the remaining technology parameters given in Table 2, the distance from the laser head to H13 steel surface is 55 mm, and flow of Ar protecting the coating is 8 L/min.Table 2
The experimental parameters applied in the laser cladding.
SampleComponent ratio (TiC : Co50) (% by weight)Laser powerP (kW)Scanning speed,Vs (mm/min)Laser energy density,Pw (kW.s./cm2)A11 : 03.335014.37A21 : 03.340012.57A31 : 03.345011.18A41 : 03.350010.06B19 : 13.635015.68B29 : 13.640013.72B39 : 13.645012.19B49 : 13.650010.97C14 : 13.935016.98C24 : 13.940014.86C34 : 13.945013.21C44 : 13.950011.89D17 : 34.235018.29D27 : 34.240016.00D37 : 34.245014.22D47 : 34.250012.80After the LC experiment, first, the surface formation is observed to see whether the surface of the cladding layer is smooth, whether there are ripples and unevenness, and whether there are pores, slag inclusions, and preliminary observation of the surface cracks with a magnifying glass. The experiment used aqua regia (HCl + 3HNO3) to corrode the metallographic sample of Co-based coating for 15 s, and the TiC/Co-based coating was saturated with FeCl3 and HCl saturated solution The microstructure was observed after 2 minutes of corrosion.The microstructure morphology of the coating was observed using a LEICA DFC280 optical image analysis system and Philips XL30ESEM-TMP scanning electron microscope with a resolution of 3.5 nm. The EDAX-Phoenix integrated energy spectrometer included in the scanning electron microscope was used to analyze the EDS spectrum of the coating section.The experimental samples were processed by wire cutting into blocks with a size of 20 mm × 6 mm × 4 mm, and then, the coating surface was mechanically polished by 400#, 600#, and 800# metallographic sandpaper in turn, the polished test. The sample was washed in absolute ethanol, then dried with a blower to make a metallographic sample, and placed in a dry box for use.


## 3. Results and Discussion

### 3.1. Analysis of the Overlay Shape

The technology parameters have a decisive influence on the shape of the coating and the microstructure of the coating. The main technological parameters include laser power (P), laser spot size (diameter D or area S), laser beam scanning speed (vs), the method of adding materials to the coating, and methods of protecting molten lakes. Normally, the selection of the technological parameters is mainly based on the experimental data planning method.Table3 illustrates the surface morphology and macrograph of the A group sample. Co50 coatings have the characteristic bright white color. Looking at the detail, group A coatings have a relatively smooth surface, the surface is relatively smooth, and the two side edges are also quite smooth.Table 3
The surface morphology and macrograph of the A group.
CoatingSurface morphologyMacrographA1A2A3A4Table4 presents the surface morphology and macrograph of the B group sample. Overall, it can be seen that when adding TiC in the coating, its appearance changes from bright white to black color. Unlike Co50 coatings with bright white color, group B coatings have a poor surface quality, show a spraying material phenomenon on 2 side edges which is quite serious, and a lot of porosity on the surface of the coating.Table 4
The surface morphology and macrograph of the B group.
CoatingSurface morphologyMacrographB1B2B3B4Table5 shows the surface morphology and macrograph of the C group sample. It can be seen that group C has better quality than group B, with no cracks; however, the height of the coating is not uniform. Besides, there are a few particles of the material being shot during the LC process and the surface of the coatings still has porosities, especially C3 and C4 are peeled in some part of the coatings.Table 5
The surface morphology and macrograph of the C group.
CoatingSurface morphologyMacrographC1C2C3C4Lastly, groupD has the best surface morphology (Table 6). When adding TiC, with the increasing of TiC ratio, the quality of the coating surface also increases. There is no air pitting on the surface, but the surface presents cracks. In addition, group D coatings also have a peeling phenomenon and its height is not steady.Table 6
The surface morphology and macrograph of theD group.
CoatingSurface morphologyMacrographD1D2D3D4(1)Pw=P⋅tS.The experiment used the laser beam wattage density parameters as the general parameters of all other technical parameters such as laser beam power and scanning speed and surveyed the influence of power density with the coating formation. In the LC process, the laser energy density is a very important parameter, which characterizes the wattage magnitude of an area unit containing laser points. Different power densities on the material's surface will have different effects, thereby affecting the laser's absorption of the material [38].In the abovementioned equation,Pw is the laser energy density (kW.s/cm2); P is the laser beam power (kW); t is the duration of the laser action within a laser point (s); and S is the laser spot area (cm2). It is possible to treat laser points as circles; thus,(2)t=Dvs,(3)S=πD22.Here,D is the laser point diameter (mm) and vs is the laser scanning speed (mm/s); substituting formula (2) and (3) into (1), we get(4)Pw=kPD⋅vswith k=1.27.The specific laser energy density is shown in Table2. The laser energy density is determined by the laser power and the size of a laser spot. Typically, the higher the laser power, the harder it is to clad. Scanning speed and laser energy density will determine the temperature and heating time of laser energy. The laser energy density is determined by the degree of evaporation of the material:(1)
Under the irradiation of a laser beam which has a sufficient energy density, the surface of the powder material is heated to the melting point, so the material is melted, even evaporated.(2)
If the laser energy density is low and the scanning speed is fast enough, the metal will absorb the energy and only cause an increase in the temperature of the material surface. At this time, the depth of the molten lake at the swept point will be small, and the precoated powder layer cannot melt.(3)
If the laser energy density is too high and the scanning speed is low, the surface of the material will evaporate, instead of melting in the molten lake. Therefore, inconsistent laser energy density and scanning speed may cause uneven microstructure and affect the coating quality. Therefore, the choice of laser power plays a main role in the LC process. Generally, with small laser power and high scanning speed, the cladding will have low shot temperature, short cladding time, and small cladding thickness.With the appropriate combination of laser power and scanning speed, the thickness of the coating can be optimized. However, increasing the thickness of the cladding, its dilution rate decreases rapidly, and defects such as pitting, cracking, and peeling will appear in the coating.Coating with high thermal stress and cracking are the two major shortcomings of the LC method; especially, cracks occur at the contiguous areas of the coating and the background material, leading to peeling of the coating. In fact, the crack is caused due to technical parameters, processing technology conditions, coating, substrate status, and other factors. Because the metal substrate and carbides are quite different in thermal parameters, in the crystallization process, the coating will shrink at a different level compared to the substrate, generating tensile stress. When the tensile stress is greater than the critical stress, the coating will show cracks.Table7 gives information about material properties of TiC, Co50, and H13 tool steel. It can be seen that the material properties of the base alloy Co and the H13 steel are quite similar, whereas the opposite is true for TiC. Looking at the detail, the coefficient of thermal expansion of base alloy Co and H13 steel are quite similar, which is very beneficial for minimizing thermal stress and cracking formation. Similarly, the melting point of these two materials is approximately the same, so it can reduce the thinness, preserve metal bonding, and help prevent the coating surface from being rough, porous, and contaminated. In terms of TiC, it has a very small coefficient of thermal expansion (7.4 × 10−6/°C), but the elastic module is high and the melting point is also higher than Co. When projecting a laser beam, the area of the molten material has a very high temperature gradient, thus creating large thermal stress, facilitating the crack formation and peeling. Because the substrate and the coating have different mechanical properties, in addition to the very fast heating and cooling speed of the laser beam, the thermal stress generating in the coating is large.Table 7
Material properties of TiC, Co, and H13 steel.
MaterialDensity (g/cm3)Melting point (oC)Coefficient of thermal expansion (×10−6/oC)Modulus of elasticity (GPa)TiC4.9331477.4460Co8.83149212.5219H13 steel7.80142712.4210Because the surface of the melting zone has a high temperature gradient, the surface tension is enormous. This surface tension causes the inner melting zone to have a strong convection phenomenon. The convection phenomenon of the liquid state metal in the melting zone will determine the uniformity of chemical composition in the coating, whose laser beam energy distribution characteristic has a great influence on the convection phenomenon. Therefore, the characteristic distribution of laser beam energy is an important factor determining the uniformity of chemical composition in the coating (Figure3).Figure 3
The diagrammatic sketch of the melt pool when the substrate slightly fuses.


### 3.2. Microstructure of the Heat-Affected Zone and Bonding Characteristics of the Cladding

Figure4 illustrates the shape of the overlays A1 and B1 cladding. From top to bottom, the structure of the coating includes the coating (CZ), bonding layer (BZ), heat-affected area (HAZ), and steel substrate (SUB). It can be seen that the HAZ is very narrow. This is the outstanding advantage of the LC method. The reason is during the melting process, the laser accumulation is low, so the energy penetrating the substrate is very small. Figure 4(b) shows the heat-affected zone of B1 coating. The organized steel is martensite (H13steel), and after LC, it is found that the matrix does not undergo phase transformation due to the high-energy laser heating. The reason is that the substrate steel is affected by heat from the large energy source of the laser beam which causes the particle boundaries’ moving and lead to large particles “swallowing” small particles. This process happens in a very short time. The result also shows that if the adjustment of technological parameters is not appropriate, it is easy for the thermal stresses to appear, thereby generating cracks and affecting product quality. Therefore, in the LC method, the determination of technology parameters is very important. The width of the heat-affected zone of the laser sample was measured with a metallographic microscope, and it was found that the width of the heat-affected zone decreased as the laser scanning speed increased. The size of the substrate heat-affected zone is related to the energy of the laser input substrate and the thermal deposition depth density. When the laser input power is increased or the scanning speed is reduced, the specific energy of the laser is increased, and the specific energy required to melt the powder is constant. The increased specific energy is absorbed by the matrix, and therefore, the width of the heat-affected zone is increased. During LC, if the process parameters are not properly matched, cracks are likely to occur due to thermal stress and tissue stress, which affects the quality of the parts, such as the A1-coated substrate (Figure 4(a)). The residual stress of the LC layer is the main reason for its cracking. This residual stress mainly comes from three aspects: thermal stress, phase transformation stress, and restraint stress. Because there is not enough liquid metal to supplement the LC and solidification process, it is bound by the surrounding colder substrate during the subsequent solid cooling shrinkage process, which causes these stresses to be difficult to be released. Once released, it will cause cracks. Among these three kinds of stress, due to the characteristics of LC quenching and heating, the influence of thermal stress is the most obvious.Figure 4
SEM of the A1 and B1 coating from the transverse cross section and heat-affected zone: (a) and (b) A1 coating; (c) and (d) B1 coating.
(a)(b)(c)(d)Figure5 shows the elements line scanning spectra of A2 coating and B4 coating. It can be seen that, with the constant capacity, the further away from the link, the higher the concentration of the elements Co, Cr, Ni, and W, while the content of Fe decreases significantly. This means that, during the melting process, there was quite a strong diffusion of Fe from the base steel to the coating, or in other words, it formed a stable metal-type bond between the coating and the steel substrate.Figure 5
Elements line scanning spectra: (a) A2 coating; (b) B4 coating.
(a)(b)In addition, in the B1 coating, the energy spectrum analysis was also carried out at 35μm, 70 μm, and 140 μm from the “white bright band.” Table 8 shows the distribution of the main components of Co, Cr, Ni, W, and Fe in the B coating. It can be seen that, under the constant power refractive index, the farther away from the “white bright band”, the content of alloying elements Co, Cr, Ni, and W in the coating increases, while the Fe content decreases. It shows that, during the LC process, the elements on the surface of the coating and the substrate diffused together, so that a good crystalline bond is formed between the coating and the H13 steel substrate. This is extremely beneficial to improve the bonding characteristics of the coating and the substrate and improve the mechanical properties of H13 steel.Table 8
EDS analysis for Co, Cr, Ni, W, and Fe of B1 coating.
Distance from the interface (μm)Element contents (wt.%)CrCoNiWFe3518.5225.753.326.0838.347024.0334.964.926.7022.1314024.6936.675.268.3814.88


### 3.3. The Cross-Section Geometry of the Cladding

Based on the analysis results of the macroscopic morphology, the samples with the same composition are selected from each group for analysis. The corresponding sample numbers are shown in Table9.Table 9
Preparation parameters and the corresponding sample numbers.
CoatingsComposition ratios,rm (Co50 : TiC)Laser power, P/kWScanning speed,vs (mm/min)Laser energy density,Pw/(kW.s/cm2)A (A2)1 : 03.340012.57B (B4)9 : 13.650010.97C (C1)4 : 13.935016.98D (D1)7 : 34.235018.29Figure6 demonstrates the microstructure of A, B, C, and D coatings. It can be seen that the coating and the substrate interface show a clear “white bright band,” showing that the coating and the H13 steel substrate can achieve a good metallurgical bond. In A coating, the “bright band” is a quite flat-growth tissue. In C coating with 20% TiC, the “white bright band” contains a large amount of black TiC particles. When the TiC content in the preset layer was increased to 30%, the D coating did not achieve a good combination with the substrate. The reason is the thermal expansion coefficients of TiC powders and Co-based alloy powders are quite dissimilar. Consequently, when the temperature gradient increases, the thermal stress and the formation of cracks generated by expansion increase. In addition, the required laser energy density is related to the melting point, when the absorption rate is high, and the required laser energy density is greater. Studies by Si [39, 40] found that if the content of added carbide reinforcing phase is too high, the brittleness of the coating will experience a significantly increased. This is because of the formation of a large amount of carbides, leading to the coating being prone to cracks and spalling during working operation.Figure 6
Microstructure of coatings: (a) A coating, (b) B coating, (c) C coating, and (d) D coating.It can also be seen that the microstructure density of the A sample is good, and a good metallurgical bond is achieved between the coating and the substrate. The composite coating A, B, and C samples can clearly distinguish the cladding zone, bonding zone, and heat-affected zone. A good metallurgical bond is formed between the coating and the substrate. The microstructure density of the C sample is better than that of the B sample. The D coating and the substrate are not well bonded, which is attributed to the high TiC content in the coating. According to the geometry of the composite coating, it can be analyzed that increasing the number of carbides is beneficial to enhance the strengthening effect, but excessive TiC content is often beneficial to the formation of bulk carbides (eutectic and secondary precipitation), which makes the coating brittle increase. Generally, the total amount of carbides cannot be too large, so the degree of strengthening is limited. The research by Chen et al. [41] has shown that the content of carbides has an important effect and usually has an optimal value (about 30 vol.%). When the content increases or decreases, the wear resistance will decrease.Figure7 illustrates the microstructure of the cross section of B, C, and D coating samples. In A coating, the dendrite structure of the coating gradually disappeared from the bottom to the surface, and it turned into a large number of dense fine structures near the coating surface. The A coating has obvious growth characteristics of columnar dendrites and equiaxed crystals and solidifies and develops towards the coating surface perpendicular to the bonding zone. Compared with the microstructure of the A coating, the structure of the B coating is no longer composed of neat columnar dendrites, and there is no obvious direction of dendrite growth. Many interdendritic eutectic structures exist. In addition, it can be seen that the structure of the B coating is composed of bright white dendrites, eutectics between the dendrites, and black TiC particles, and the TiC particles are diffusely distributed, which can play a good hardening role. In C coating with 20% TiC, with the increase in the amount of TiC in the preset layer, the content of the TiC reinforcing phase and the phase structure of the coating evolve accordingly. The coating is also composed of bright white dendrites, eutectics between the dendrites, and black TiC particles. While the size of the TiC particles in the structure increases, the number decreases slightly. The resulting TiC is evenly distributed in the coating. When the TiC content in the preset layer was increased to 30%, the D coating did not achieve a good combination with the substrate. The figure points out that TiC exists like a large number of diffusely distributed spherical structures.Figure 7
Microstructure of the cross section of the coatings after the laser cladding process. (a) A coating, (b) B coating, (c) C coating, and (d) D coating.Figure8 shows the microstructure from the bottom zone to the upper zone of B, C, and D cladding. It can be seen that the morphology of TiC is mainly spherical. The morphology of TiC in the B coating structure is different due to its different parts in the molten pool, and its composition, temperature distribution, and cooling rate are different. TiC in the middle and the surface of the coating is a large block structure, while the bottom of the coating has a low temperature and insufficient melting, and due to the rapid heat transfer effect of the cold matrix, the cooling rate is large, and the TiC grains are too late. It has stopped growing when it is large, so a fine granular structure is formed. C cladding demonstrates that TiC has the form of “cross flower” and “twigs” in the bottom zone [42–44]. In the middle zone and upper zone, TiC mostly exists in a spherical shape. In particular, the size of the TiC rises steadily from the bottom zone to the surface of the cladding. In the D cladding, TiC exhibits like a large number of diffusely distributed spherical structures. Unlike C coating, TiC particle size in D coating has no clear gradient change.Figure 8
Microstructure of the Co50/TiC claddings: (a) B cladding, (b) C cladding, and (c) D cladding.
(a)(b)(c)Pei [14] studied the gradient change law of TiC particle size and the gradient change law of TiC volume content. The results of statistical analysis showed that the average diameter of TiC particles gradually increased about 0.8 μm to 4.5 μm from the bottom to the upper zone of the cladding. The change of the particle size is significant and continuous; the average diameter of TiC particles (Sp) and the distance (d) from the bonding zone are in a quadratic function relationship Sp = 0.8 + 1.22 × 10−2d −10−5d2. The study also found that although the spacing between TiC particles in the cladding increases slowly with its distribution position upwards, the volume content of TiC still shows a certain gradient growth law along the thickness direction, about 4% at the bottom to 33% at the upper zone. According to Stokes’ law, in Co alloy melting, the floating speed of TiC particles with different sizes is different. Because the larger TiC particles rise faster than the smaller ones, it results in selective capture of TiC particles. That is, small particles with a slower moving speed are always captured first. On the other hand, the melt shear caused by strong convection in the laser molten pool also promotes collisions between particles. After the TiC particles collide together, their growth and bonding characteristics will be mainly controlled by the time they exist in the melt (Figure 9). In the rapid solidification process of the laser molten pool, the melting and bonding of the particles are usually difficult to complete. Li and Chen et al. [45] have shown that the TiC morphology in the coating structure is different due to its different parts of the molten pool (the composition, temperature gradient, and cooling rate are different). The different morphologies of TiC in different regions are caused by different cooling rates.Figure 9
Schematic illustration of TiC collision and sintering within Co alloy melt: (a) a stuck TiC moving at faster speed v2 catching up a single TiC; (b) collision with each other; (c) partial sintering among TiC particles and growth of the whole cluster.
(a)(b)(c)


## 3.1. Analysis of the Overlay Shape

The technology parameters have a decisive influence on the shape of the coating and the microstructure of the coating. The main technological parameters include laser power (P), laser spot size (diameter D or area S), laser beam scanning speed (vs), the method of adding materials to the coating, and methods of protecting molten lakes. Normally, the selection of the technological parameters is mainly based on the experimental data planning method.Table3 illustrates the surface morphology and macrograph of the A group sample. Co50 coatings have the characteristic bright white color. Looking at the detail, group A coatings have a relatively smooth surface, the surface is relatively smooth, and the two side edges are also quite smooth.Table 3
The surface morphology and macrograph of the A group.
CoatingSurface morphologyMacrographA1A2A3A4Table4 presents the surface morphology and macrograph of the B group sample. Overall, it can be seen that when adding TiC in the coating, its appearance changes from bright white to black color. Unlike Co50 coatings with bright white color, group B coatings have a poor surface quality, show a spraying material phenomenon on 2 side edges which is quite serious, and a lot of porosity on the surface of the coating.Table 4
The surface morphology and macrograph of the B group.
CoatingSurface morphologyMacrographB1B2B3B4Table5 shows the surface morphology and macrograph of the C group sample. It can be seen that group C has better quality than group B, with no cracks; however, the height of the coating is not uniform. Besides, there are a few particles of the material being shot during the LC process and the surface of the coatings still has porosities, especially C3 and C4 are peeled in some part of the coatings.Table 5
The surface morphology and macrograph of the C group.
CoatingSurface morphologyMacrographC1C2C3C4Lastly, groupD has the best surface morphology (Table 6). When adding TiC, with the increasing of TiC ratio, the quality of the coating surface also increases. There is no air pitting on the surface, but the surface presents cracks. In addition, group D coatings also have a peeling phenomenon and its height is not steady.Table 6
The surface morphology and macrograph of theD group.
CoatingSurface morphologyMacrographD1D2D3D4(1)Pw=P⋅tS.The experiment used the laser beam wattage density parameters as the general parameters of all other technical parameters such as laser beam power and scanning speed and surveyed the influence of power density with the coating formation. In the LC process, the laser energy density is a very important parameter, which characterizes the wattage magnitude of an area unit containing laser points. Different power densities on the material's surface will have different effects, thereby affecting the laser's absorption of the material [38].In the abovementioned equation,Pw is the laser energy density (kW.s/cm2); P is the laser beam power (kW); t is the duration of the laser action within a laser point (s); and S is the laser spot area (cm2). It is possible to treat laser points as circles; thus,(2)t=Dvs,(3)S=πD22.Here,D is the laser point diameter (mm) and vs is the laser scanning speed (mm/s); substituting formula (2) and (3) into (1), we get(4)Pw=kPD⋅vswith k=1.27.The specific laser energy density is shown in Table2. The laser energy density is determined by the laser power and the size of a laser spot. Typically, the higher the laser power, the harder it is to clad. Scanning speed and laser energy density will determine the temperature and heating time of laser energy. The laser energy density is determined by the degree of evaporation of the material:(1)
Under the irradiation of a laser beam which has a sufficient energy density, the surface of the powder material is heated to the melting point, so the material is melted, even evaporated.(2)
If the laser energy density is low and the scanning speed is fast enough, the metal will absorb the energy and only cause an increase in the temperature of the material surface. At this time, the depth of the molten lake at the swept point will be small, and the precoated powder layer cannot melt.(3)
If the laser energy density is too high and the scanning speed is low, the surface of the material will evaporate, instead of melting in the molten lake. Therefore, inconsistent laser energy density and scanning speed may cause uneven microstructure and affect the coating quality. Therefore, the choice of laser power plays a main role in the LC process. Generally, with small laser power and high scanning speed, the cladding will have low shot temperature, short cladding time, and small cladding thickness.With the appropriate combination of laser power and scanning speed, the thickness of the coating can be optimized. However, increasing the thickness of the cladding, its dilution rate decreases rapidly, and defects such as pitting, cracking, and peeling will appear in the coating.Coating with high thermal stress and cracking are the two major shortcomings of the LC method; especially, cracks occur at the contiguous areas of the coating and the background material, leading to peeling of the coating. In fact, the crack is caused due to technical parameters, processing technology conditions, coating, substrate status, and other factors. Because the metal substrate and carbides are quite different in thermal parameters, in the crystallization process, the coating will shrink at a different level compared to the substrate, generating tensile stress. When the tensile stress is greater than the critical stress, the coating will show cracks.Table7 gives information about material properties of TiC, Co50, and H13 tool steel. It can be seen that the material properties of the base alloy Co and the H13 steel are quite similar, whereas the opposite is true for TiC. Looking at the detail, the coefficient of thermal expansion of base alloy Co and H13 steel are quite similar, which is very beneficial for minimizing thermal stress and cracking formation. Similarly, the melting point of these two materials is approximately the same, so it can reduce the thinness, preserve metal bonding, and help prevent the coating surface from being rough, porous, and contaminated. In terms of TiC, it has a very small coefficient of thermal expansion (7.4 × 10−6/°C), but the elastic module is high and the melting point is also higher than Co. When projecting a laser beam, the area of the molten material has a very high temperature gradient, thus creating large thermal stress, facilitating the crack formation and peeling. Because the substrate and the coating have different mechanical properties, in addition to the very fast heating and cooling speed of the laser beam, the thermal stress generating in the coating is large.Table 7
Material properties of TiC, Co, and H13 steel.
MaterialDensity (g/cm3)Melting point (oC)Coefficient of thermal expansion (×10−6/oC)Modulus of elasticity (GPa)TiC4.9331477.4460Co8.83149212.5219H13 steel7.80142712.4210Because the surface of the melting zone has a high temperature gradient, the surface tension is enormous. This surface tension causes the inner melting zone to have a strong convection phenomenon. The convection phenomenon of the liquid state metal in the melting zone will determine the uniformity of chemical composition in the coating, whose laser beam energy distribution characteristic has a great influence on the convection phenomenon. Therefore, the characteristic distribution of laser beam energy is an important factor determining the uniformity of chemical composition in the coating (Figure3).Figure 3
The diagrammatic sketch of the melt pool when the substrate slightly fuses.


## 3.2. Microstructure of the Heat-Affected Zone and Bonding Characteristics of the Cladding

Figure4 illustrates the shape of the overlays A1 and B1 cladding. From top to bottom, the structure of the coating includes the coating (CZ), bonding layer (BZ), heat-affected area (HAZ), and steel substrate (SUB). It can be seen that the HAZ is very narrow. This is the outstanding advantage of the LC method. The reason is during the melting process, the laser accumulation is low, so the energy penetrating the substrate is very small. Figure 4(b) shows the heat-affected zone of B1 coating. The organized steel is martensite (H13steel), and after LC, it is found that the matrix does not undergo phase transformation due to the high-energy laser heating. The reason is that the substrate steel is affected by heat from the large energy source of the laser beam which causes the particle boundaries’ moving and lead to large particles “swallowing” small particles. This process happens in a very short time. The result also shows that if the adjustment of technological parameters is not appropriate, it is easy for the thermal stresses to appear, thereby generating cracks and affecting product quality. Therefore, in the LC method, the determination of technology parameters is very important. The width of the heat-affected zone of the laser sample was measured with a metallographic microscope, and it was found that the width of the heat-affected zone decreased as the laser scanning speed increased. The size of the substrate heat-affected zone is related to the energy of the laser input substrate and the thermal deposition depth density. When the laser input power is increased or the scanning speed is reduced, the specific energy of the laser is increased, and the specific energy required to melt the powder is constant. The increased specific energy is absorbed by the matrix, and therefore, the width of the heat-affected zone is increased. During LC, if the process parameters are not properly matched, cracks are likely to occur due to thermal stress and tissue stress, which affects the quality of the parts, such as the A1-coated substrate (Figure 4(a)). The residual stress of the LC layer is the main reason for its cracking. This residual stress mainly comes from three aspects: thermal stress, phase transformation stress, and restraint stress. Because there is not enough liquid metal to supplement the LC and solidification process, it is bound by the surrounding colder substrate during the subsequent solid cooling shrinkage process, which causes these stresses to be difficult to be released. Once released, it will cause cracks. Among these three kinds of stress, due to the characteristics of LC quenching and heating, the influence of thermal stress is the most obvious.Figure 4
SEM of the A1 and B1 coating from the transverse cross section and heat-affected zone: (a) and (b) A1 coating; (c) and (d) B1 coating.
(a)(b)(c)(d)Figure5 shows the elements line scanning spectra of A2 coating and B4 coating. It can be seen that, with the constant capacity, the further away from the link, the higher the concentration of the elements Co, Cr, Ni, and W, while the content of Fe decreases significantly. This means that, during the melting process, there was quite a strong diffusion of Fe from the base steel to the coating, or in other words, it formed a stable metal-type bond between the coating and the steel substrate.Figure 5
Elements line scanning spectra: (a) A2 coating; (b) B4 coating.
(a)(b)In addition, in the B1 coating, the energy spectrum analysis was also carried out at 35μm, 70 μm, and 140 μm from the “white bright band.” Table 8 shows the distribution of the main components of Co, Cr, Ni, W, and Fe in the B coating. It can be seen that, under the constant power refractive index, the farther away from the “white bright band”, the content of alloying elements Co, Cr, Ni, and W in the coating increases, while the Fe content decreases. It shows that, during the LC process, the elements on the surface of the coating and the substrate diffused together, so that a good crystalline bond is formed between the coating and the H13 steel substrate. This is extremely beneficial to improve the bonding characteristics of the coating and the substrate and improve the mechanical properties of H13 steel.Table 8
EDS analysis for Co, Cr, Ni, W, and Fe of B1 coating.
Distance from the interface (μm)Element contents (wt.%)CrCoNiWFe3518.5225.753.326.0838.347024.0334.964.926.7022.1314024.6936.675.268.3814.88


## 3.3. The Cross-Section Geometry of the Cladding

Based on the analysis results of the macroscopic morphology, the samples with the same composition are selected from each group for analysis. The corresponding sample numbers are shown in Table9.Table 9
Preparation parameters and the corresponding sample numbers.
CoatingsComposition ratios,rm (Co50 : TiC)Laser power, P/kWScanning speed,vs (mm/min)Laser energy density,Pw/(kW.s/cm2)A (A2)1 : 03.340012.57B (B4)9 : 13.650010.97C (C1)4 : 13.935016.98D (D1)7 : 34.235018.29Figure6 demonstrates the microstructure of A, B, C, and D coatings. It can be seen that the coating and the substrate interface show a clear “white bright band,” showing that the coating and the H13 steel substrate can achieve a good metallurgical bond. In A coating, the “bright band” is a quite flat-growth tissue. In C coating with 20% TiC, the “white bright band” contains a large amount of black TiC particles. When the TiC content in the preset layer was increased to 30%, the D coating did not achieve a good combination with the substrate. The reason is the thermal expansion coefficients of TiC powders and Co-based alloy powders are quite dissimilar. Consequently, when the temperature gradient increases, the thermal stress and the formation of cracks generated by expansion increase. In addition, the required laser energy density is related to the melting point, when the absorption rate is high, and the required laser energy density is greater. Studies by Si [39, 40] found that if the content of added carbide reinforcing phase is too high, the brittleness of the coating will experience a significantly increased. This is because of the formation of a large amount of carbides, leading to the coating being prone to cracks and spalling during working operation.Figure 6
Microstructure of coatings: (a) A coating, (b) B coating, (c) C coating, and (d) D coating.It can also be seen that the microstructure density of the A sample is good, and a good metallurgical bond is achieved between the coating and the substrate. The composite coating A, B, and C samples can clearly distinguish the cladding zone, bonding zone, and heat-affected zone. A good metallurgical bond is formed between the coating and the substrate. The microstructure density of the C sample is better than that of the B sample. The D coating and the substrate are not well bonded, which is attributed to the high TiC content in the coating. According to the geometry of the composite coating, it can be analyzed that increasing the number of carbides is beneficial to enhance the strengthening effect, but excessive TiC content is often beneficial to the formation of bulk carbides (eutectic and secondary precipitation), which makes the coating brittle increase. Generally, the total amount of carbides cannot be too large, so the degree of strengthening is limited. The research by Chen et al. [41] has shown that the content of carbides has an important effect and usually has an optimal value (about 30 vol.%). When the content increases or decreases, the wear resistance will decrease.Figure7 illustrates the microstructure of the cross section of B, C, and D coating samples. In A coating, the dendrite structure of the coating gradually disappeared from the bottom to the surface, and it turned into a large number of dense fine structures near the coating surface. The A coating has obvious growth characteristics of columnar dendrites and equiaxed crystals and solidifies and develops towards the coating surface perpendicular to the bonding zone. Compared with the microstructure of the A coating, the structure of the B coating is no longer composed of neat columnar dendrites, and there is no obvious direction of dendrite growth. Many interdendritic eutectic structures exist. In addition, it can be seen that the structure of the B coating is composed of bright white dendrites, eutectics between the dendrites, and black TiC particles, and the TiC particles are diffusely distributed, which can play a good hardening role. In C coating with 20% TiC, with the increase in the amount of TiC in the preset layer, the content of the TiC reinforcing phase and the phase structure of the coating evolve accordingly. The coating is also composed of bright white dendrites, eutectics between the dendrites, and black TiC particles. While the size of the TiC particles in the structure increases, the number decreases slightly. The resulting TiC is evenly distributed in the coating. When the TiC content in the preset layer was increased to 30%, the D coating did not achieve a good combination with the substrate. The figure points out that TiC exists like a large number of diffusely distributed spherical structures.Figure 7
Microstructure of the cross section of the coatings after the laser cladding process. (a) A coating, (b) B coating, (c) C coating, and (d) D coating.Figure8 shows the microstructure from the bottom zone to the upper zone of B, C, and D cladding. It can be seen that the morphology of TiC is mainly spherical. The morphology of TiC in the B coating structure is different due to its different parts in the molten pool, and its composition, temperature distribution, and cooling rate are different. TiC in the middle and the surface of the coating is a large block structure, while the bottom of the coating has a low temperature and insufficient melting, and due to the rapid heat transfer effect of the cold matrix, the cooling rate is large, and the TiC grains are too late. It has stopped growing when it is large, so a fine granular structure is formed. C cladding demonstrates that TiC has the form of “cross flower” and “twigs” in the bottom zone [42–44]. In the middle zone and upper zone, TiC mostly exists in a spherical shape. In particular, the size of the TiC rises steadily from the bottom zone to the surface of the cladding. In the D cladding, TiC exhibits like a large number of diffusely distributed spherical structures. Unlike C coating, TiC particle size in D coating has no clear gradient change.Figure 8
Microstructure of the Co50/TiC claddings: (a) B cladding, (b) C cladding, and (c) D cladding.
(a)(b)(c)Pei [14] studied the gradient change law of TiC particle size and the gradient change law of TiC volume content. The results of statistical analysis showed that the average diameter of TiC particles gradually increased about 0.8 μm to 4.5 μm from the bottom to the upper zone of the cladding. The change of the particle size is significant and continuous; the average diameter of TiC particles (Sp) and the distance (d) from the bonding zone are in a quadratic function relationship Sp = 0.8 + 1.22 × 10−2d −10−5d2. The study also found that although the spacing between TiC particles in the cladding increases slowly with its distribution position upwards, the volume content of TiC still shows a certain gradient growth law along the thickness direction, about 4% at the bottom to 33% at the upper zone. According to Stokes’ law, in Co alloy melting, the floating speed of TiC particles with different sizes is different. Because the larger TiC particles rise faster than the smaller ones, it results in selective capture of TiC particles. That is, small particles with a slower moving speed are always captured first. On the other hand, the melt shear caused by strong convection in the laser molten pool also promotes collisions between particles. After the TiC particles collide together, their growth and bonding characteristics will be mainly controlled by the time they exist in the melt (Figure 9). In the rapid solidification process of the laser molten pool, the melting and bonding of the particles are usually difficult to complete. Li and Chen et al. [45] have shown that the TiC morphology in the coating structure is different due to its different parts of the molten pool (the composition, temperature gradient, and cooling rate are different). The different morphologies of TiC in different regions are caused by different cooling rates.Figure 9
Schematic illustration of TiC collision and sintering within Co alloy melt: (a) a stuck TiC moving at faster speed v2 catching up a single TiC; (b) collision with each other; (c) partial sintering among TiC particles and growth of the whole cluster.
(a)(b)(c)


## 4. Conclusions

In 10% TiC coating, the “bright band” is a quite flat-growth tissue. In the coating with 20% TiC, the “white bright band” contains a large amount of black TiC particles. When the TiC content in the preset layer was increased to 30%, the coating did not achieve a good combination with the substrate. The microstructure density of the Co50 sample is good, and a good metallurgical bond is achieved between the coating and the substrate. The composite coating Co50, 10% TiC, and 20% TiC samples can clearly distinguish the cladding zone, bonding zone, and heat-affected zone. The microstructure density of the 20% TiC sample is better than the 10% TiC sample. The 30% TiC coating and the substrate are not well bonded, which is attributed to the high TiC content in the coating.Co50 coatings have the characteristic bright white color, when adding TiC, and with the increase in TiC ratio, the quality of coating surface also increases. Co50 coatings have a relatively smooth surface, the surface is relatively smooth, and the two side edges are also quite smooth. 10% TiC coatings have a poor surface quality, a spraying material phenomenon on 2 side edges which is quite serious, and a lot of porosity on the surface of the coating. 20% TiC has better quality than 10% TiC, with no cracks, but the coatings have a large undulating level and the flatness of the coatings is quite low. 30% TiC has the best surface morphology, but the surface exhibits cracks.10% TiC coating includes the original TiC particles that are not fully melted, and there are also primary TiC particles that are precipitated in situ from the liquid phase during solidification. 20% TiC coating indicates a large amount of TiC in the form of cross petals and twigs. In the middle part and upper part, TiC mostly exists in a spherical shape. In the 30% TiC sample coating, the figure points out that TiC exists like a large number of diffusely distributed spherical structures.The coatings of TiC/Co composite with less than 20% TiC showed good metallurgical bonding characteristics with the H13 steel surface.The coatings of Co-based composite with 20% TiC represent good comprehensive properties, satisfying the requirements of production.



---

*Source: 8898693-2021-03-05.xml*