3.1. Phase and Morphology Characteristics
Figure 3 reveals the XRD results of the friction-assisted electrodeposition of Cu-SiC composite deposition and Cu substrate. Cu and SiC phases appear in all samples. The friction speed does not change the phase composition of the deposition layer samples. The formation of Cu is mainly because the Cu
2+ in the electrolyte obtains electrons on the cathode plate under the action of the electric field and is reduced to atoms and finally deposited [
16]. The flow of the electrodeposition liquid under friction stirring conditions causes the SiC solid particles to suspend and move to the vicinity of the cathode. After the particles are charged, they are electrophoresed to the cathode surface under the action of the electric field force and finally deposited on the substrate. However, during the friction electrodeposition process, the distance between the cathode and the anode is very small, and the electrolyte filled between the electrodes is turbulent, making the formation of the deposited layer in a nonlinear state. The formation of the friction-assisted electrodeposition layer mainly involves three steps (see
Figure 4). Firstly, the SiC in the electrolyte is positively charged under the action of the electric field, and the SiC particles move toward the cathode surface during electrodeposition. Secondly, the positively charged SiC particles are captured by the cathode and adhere to the substrate surface. Thirdly, the SiC particles adhering to the cathode surface are squeezed with the friction ball and embedded into the substrate surface to form the deposited layer.
Figure 5a reveals the morphological characteristics of the friction-assisted electrodeposition. There is an obvious deposition layer in the friction direction. It is noteworthy that the deposited layer only appears in the friction area. The length and width of the deposition layer are shown in
Figure 5b. The friction speed has an important influence on the deposition size of the electrodeposited layer. As the deposition speed increases, the width and length of the deposited layer increase. The average lengths of the S1–S4 deposition layers are 7.16, 7.23, 7.26, and 7.31 mm, respectively. The average widths of the S1–S4 deposition layers are 1.57, 2.21, 2.61, and 2.65 mm, respectively. With the increase of friction speed, the width and length of the deposition layer increase. The width of the S4 sample increased by 68.7% compared to the S1 sample, while the length increased by 2.1%.
3.2. Microstructure Properties
The morphology of the electrodeposited composite layer is shown in
Figure 6a–d. In all samples, there is a clear boundary between the deposition and the substrate. No obvious cracks or other defects are found at the interface, which indicates that the deposition is well-deposited. To further analyze the effect of friction speed on the interface of electrodeposition, EDS was used to analyze the element distribution at the interface of deposited layer S1 and S4 samples, as shown in
Figure 7. There is a more obvious void structure at the S1 interface. As the friction speed increases, the void phenomenon at the interface is alleviated. The occurrence of voids in
Figure 7 is inextricably linked to the distribution of oxygen. The interfacial EDS analysis results at S1 and S4 show that oxygen is mainly enriched in the electrodeposited layer, and the distribution is not obvious in the Cu substrate. This indicates that the oxygen elements in the electrolyte diffuse differently to the deposition and the substrate during the deposition process, which produces the Kirkendall effect, resulting in the formation of voids [
17]. With the increase of friction velocity, the Kirkendall effect was weakened, thus suppressing the generation of voids.
At the S1 interface, the distribution of SiC is not obvious. As the friction speed increases, an obvious SiC distribution is detected at the interface of the deposited layer. This shows that as the friction speed increases, SiC is more easily deposited at the interface. The reason for this phenomenon may be that the increase in friction speed accelerates the aggregation of SiC on the Cu substrate, resulting in more SiC deposition at the interface. In addition, the deposition of SiC is also related to the void phenomenon at the interface of the deposited layer. The presence of voids affects the bonding between particles, making it difficult for SiC to be deposited on the substrate. The increase in friction speed alleviates this phenomenon.
The current density at the cathode under forced convection can be expressed as [
18]:
where
is Levich current (
A),
n is the number of electrons transferred,
F is Faraday’s Constant,
A is the surface area of the working electrode,
D is diffusion coefficient of the analyte,
is the angular rotation rate of the electrode,
is the kinematic viscosity,
C is the concentration of the analyte.
From Formula (1), it can be seen that the cathode current density can be increased by increasing the stirring speed, which has an important influence on the formation of the electrodeposition layer. Related studies have shown that the higher the cathodic limit current density, the higher the deposition rate of the electrodeposited layer [
19,
20]. This means that the deposition rate of the electrodeposited layer is higher as the friction velocity increases. In this study,
Figure 7 shows the deposition condition at the interface between the electrodeposited layer and the substrate with different friction rates. The increase in the electrodeposition rate caused more SiC to be deposited on the substrate. At the same time, the increase in deposition rate makes it easier for metal ions in the solution to deposit and mold, reducing the voids at the interface. This has an important influence on the mechanical properties of the deposited layer.
In addition, the pH values of S1–S4 electrolytes become 9.3, 11.6, 12.1, and 13.8, respectively, during the deposition process. This means that with the increase of friction speed, the pH value of the electrode liquid increases. The H+ in the plating solution decreases under the action of friction, increasing the pH value. The higher the pH value, the stronger the conductivity of the electrolyte, which can improve the efficiency of the electrolysis process. This also reveals that with the increase of friction speed, the macroscopic size of the deposited layer also increases.
The microstructure evolution of the deposited layer is shown in
Figure 8a–d. There are obvious dendrites in the microstructure [
21]. The results show the presence of larger-sized iron oxides in S1.
Figure 9 and
Figure 10 reveal that the S4 deposited layer has finer dendrite morphology in the microstructure. In addition, the iron oxides in S4 are finer than those in S1. This phenomenon indicates that the increase in friction velocity refines the microstructure size of Cu-SiC deposited layer. In addition, there is Fe in the EDS results of the deposition. This phenomenon occurs because stainless steel is used as an anode. During the deposition process, Fe enters the deposition layer and turns into iron oxide. The presence of iron oxide was obvious in S1 and S2 deposited layers (see
Figure 6). As the friction speed increased, the larger area of oxides disappeared. The reason for this phenomenon may be that as the friction speed increases, the friction force on the metal oxide with a larger area increases, thereby crushing the iron oxide with a larger area into small fragments. In addition, the elemental content of the microstructure of the deposited layer was tested by EDS, as shown in
Table 3. As the friction speed increases, the content of Fe in the deposited layer gradually decreases. This phenomenon occurs because the Fe in the stainless steel rod enters the deposited layer during the friction process. However, friction and extrusion lead to the refinement of the microstructure, making it difficult for Fe elements to aggregate, resulting in a decrease in the Fe content in the deposited layer.
Therefore, it can be said that the friction speed has an important influence on the formation and microstructural characteristics of the deposited layer during the electrodeposition process. During the deposition process, Fe in the stainless steel anode dissolves and is deposited on the Cu substrate. Theoretically, the amount of anode dissolution and metal deposition directly depends on the amount of current passing through. According to Faraday’s law, it can be calculated using the following formula [
22]:
where
N is the deposition layer factor,
I is the current between the electrode and the solution, and
t is the deposition time.
In this study, the deposition layer factor and deposition time are constant values. According to Formula (2), the change in the morphology of the deposition layer is closely related to the current density. In other words, the friction speed changes the current between the electrode and the solution, thereby changing the morphology and microstructural characteristics of the electrodeposited layer. Related studies have also shown that the greater the current density, the finer the microstructure of the electrodeposited layer [
23]. In the previous discussion, it was found that increasing the stirring speed during the electrodeposition process can increase the limiting current density of the cathode. Therefore, the reasons for the refinement of the S4 sample in this study come from two aspects. Firstly, under the action of friction, the increase in the current density of the deposition layer leads to an increase in the amount of stainless steel electrode dissolved in the deposition layer, which accelerates the dissolution of Fe into the deposition layer. Secondly, under the action of friction, the anode squeezes the SiC particles in the solution, making it easier for them to deposit on the Cu substrate. The embedding of the SiC particles disrupts the growth pattern of the deposition layer, causing areas where coarse grains might have formed to be refined into smaller grains. The SiC particles attached to the Cu matrix are squeezed against each other under the action of friction and are more easily broken into fine particles, which has an important influence on improving the mechanical properties of the deposited layer. In addition, the mechanical process and fluid dynamic factors in the friction-assisted electrodeposition process cannot be ignored. Specifically, SiC particles are transferred to the cathode surface by the moving fluid, and once they contact the cathode, they stay on it by external force. During the residence time, they are captured by the growing metal and embedded in the deposited layer. In this process, fluid dynamic factors have an important influence on the transfer and residence time of particles.
In addition, the dissolution of Fe in the electrolyte has an important influence on the performance of the deposited layer. In the previous discussion, it was found that the increase in friction speed will accelerate the entry of Fe into the deposited layer, which will lead to solid solution strengthening, thereby enhancing the mechanical properties of the deposited layer.
3.3. Microhardness
Figure 11 reveals the microhardness of the layers. The average microhardness of the S1–S4 deposited layers are 142.4, 154.0, 165.4, and 177.6 HV, respectively. The microhardness of the deposition is greater than that of the substrate. With the increase of friction speed, the microhardness of the deposition increases. The microhardness of the S4 sample increased by 24.7% compared with the S1 sample. This study found that the closer the deposited layer is to the substrate, the higher the microhardness.
This is consistent with the study of M. Shourgeshty et al. [
24]. During the friction-assisted electrodeposition process, as the friction speed increases, more SiC particles at the interface participate in the deposition process and enter the Cu lattice, causing a greater degree of lattice distortion; the grains of different forms are more tightly combined; the number of holes in the composite deposition layer decreases; and the density gradually increases. Therefore, the composite deposition layer has an enhanced ability to withstand external load indentation and resist local plastic deformation, which is manifested as increased microhardness. Furthermore, the increase in microhardness of the deposited layer is inextricably linked to the refinement of the microstructure. It has been demonstrated that finer microstructure size has higher grain boundary density, which improves the strength and hardness of the deposited layer. According to the Hall–Petch criterion, the microhardness of the deposited layer can be improved as the grain size decreases [
25]. Under the effect of friction, the microstructure of the deposited layer is more refined, which leads to an increase in the hardness of the deposited layer.
In other words, the improvement of the microhardness of the deposited layer by the friction effect is related to grain refinement and the interface characteristics of the deposited layer and the substrate. As analyzed in
Figure 7, the increase in friction speed reduces the generation of voids in the deposited layer, which is beneficial for improving the microhardness of the deposited layer. Under the action of friction, more SiC particles are embedded in the deposited layer, which improves the hardness of the deposited layer to a certain extent. Therefore, under the action of friction, the improvement of the hardness of the deposited layer comes from many aspects, which are the refinement of the microstructure, the reduction of voids, and the increase in the amount of SiC embedded.
3.5. Wear Properties
The friction coefficient (COF) curve and the average friction coefficient of the electrodeposited layer are shown in
Figure 14. By observing the friction curve of the electrodeposited layer, it is found that with the increase of friction time, the friction coefficient of the electrodeposited layer increases with fluctuation and then tends to be stable. The reason for this phenomenon is that the resistance in the initial stage of friction is small. With the increase of friction time, the deposited layer undergoes plastic deformation under the action of cyclic load, and the wear debris gradually increases, which plays an obstructive role and increases the friction coefficient [
28]. When the Si
3N
4 ball reaches a stable contact state with the friction surface, the friction coefficient region is stable. The average friction coefficients of the S1–S4 electrodeposited layers are 0.74, 0.69, 0.63, and 0.55, respectively. During the electrodeposition process, as the anode friction speed increases, the friction coefficient of the electrodeposited layer decreases. Compared with the S1 deposited layer, the COF of the S4 deposited layer decreases by 25.6%.
Figure 13.
Surface morphology of anode ball after electrodeposition: (a) S1 electrodeposition layer; (b) S2 electrodeposition layer; (c) S3 electrodeposition layer; (d) S4 electrodeposition layer.
Figure 13.
Surface morphology of anode ball after electrodeposition: (a) S1 electrodeposition layer; (b) S2 electrodeposition layer; (c) S3 electrodeposition layer; (d) S4 electrodeposition layer.
Figure 14.
COF of the electrodeposited layer: (a) COF curve; (b) Average COF values.
Figure 14.
COF of the electrodeposited layer: (a) COF curve; (b) Average COF values.
To further reveal the wear mechanism of the electrodeposited layer, the microscopic morphology of the worn samples was tested, as shown in
Figure 15. The wear morphology reveals that the electrodeposited layer has different degrees of wear during the friction experiment. There are obvious spalling pits and plowing grooves in the wear morphology of the deposited layer. The spalling pits in the S1 and S2 deposited layers are more obvious. The presence of spalling pits can increase the friction coefficient during the friction process [
29]. During the friction process, under the combined action of extrusion and plowing, the SiC particles in the deposited layer participate in the transfer of wear debris to the contact surface of the friction pair and delaminate and fracture under the action of mechanical shear force, and disperse on the contact surface to form a solid lubricating film, which can play a friction-reducing role, thereby reducing the friction coefficient of the composite deposition. The material transfer phenomenon appeared in the wear morphology of the deposited layer. EDS analysis was performed on different parts of the wear morphology (see
Table 4). More Si elements were found in the EDS test of the material stacking part. This means that this part has a large distribution of SiC. The higher the SiC content in the composite electrodeposition layer, the more particles will naturally transfer and delaminate during the friction process, which will cause a larger area of solid lubrication film to form on the contact surface of the friction pair, which will effectively reduce friction and reduce the friction coefficient [
30]. In addition, the density of the material in the composite electrodeposition layer also affects the friction coefficient. Since the material at the interface of the S4 deposition layer is smoother and denser, its ability to resist plastic deformation is enhanced, which also reduces the friction coefficient. Due to the low content of SiC particles at the interface of the S1 deposition layer, there are very few particles that are delaminated and fractured and transferred to the contact surface of the friction pair under the combined action of extrusion and plowing during the friction process, and the self-lubricating and friction-reducing effect is limited. In addition, the composite deposition formed when the SiC particle content is low has many crystal defects and a poor ability to resist local plastic deformation, which together lead to an increase in the friction coefficient of the S1 sample.
The wear scar morphology of the laser-deposited layer was tested by optical microscopy, as shown in
Figure 16. It can be seen from the figure that the wear scar width of the S1 deposited layer is the highest. Combined with the wear characteristics such as furrows and local peeling observed in
Figure 15a, this shows that the surface wear of the S1 sample is more serious. The wear scar width of the S4 deposit layer is reduced by about 21.2% compared with that of the S1 deposit layer.
As shown in
Figure 15, wear features such as furrows and local peeling can be observed on the wear surface of the S1 and S2 deposit layers, and the edge is accompanied by wear debris accumulation. This shows that the wear degree of the deposit layer surface is serious. The reason is that the deposited layer has low microhardness and poor wear resistance. It is easy to cause adhesive wear and abrasive wear during the friction process. At the same time, furrows are formed under the action of extrusion and plowing, accompanied by local peeling [
31]. As shown in
Figure 15c,d, as the friction speed increases during the electrodeposition process, the peeling pit phenomenon formed on the surface of the composite deposit layer gradually disappears. This is related to the different content of SiC particles in the composite deposit layer and the difference in the self-lubricating and friction-reducing effect of the particles during the friction process. During the friction process, hardness also has an important influence on the friction coefficient of the electrodeposited layer. The increase in hardness, the resistance to local plastic deformation, and wear resistance are enhanced, thereby reducing the friction coefficient and wear width of the composite electrodeposited layers.