3.2. Analysis of the Variation Law of Residual Stress and Deformation
For precision machining, between-centers turning was employed to investigate the deformation of the workpiece following the removal of the top constraints at both ends after turning, as well as the deformation following stress relief annealing, through runout measurements. To minimize measurement errors, nine workpieces were selected for processing and subsequent testing.
The runout of the workpiece after precision machining and annealing is shown in
Figure 6. After precision machining, the radial runouts of the workpiece are predominantly greater than 0.05 mm, with the maximum runout reaching 0.4045 mm. This phenomenon can be attributed to the reduced stiffness and the rebalancing of internal stresses of the workpiece after the turning process, which leads to increased deformation. After the annealing treatment, the workpiece deformation is further exacerbated, with the maximum radial runout reaching 0.6682 mm, resulting in the scrapping of some workpieces and the inability to complete subsequent processing. The reason is that, during turning, the radial allowance of the workpiece is removed unevenly, leading to significant and non-uniformly distributed internal stresses. However, during annealing, the residual stresses on the surface and within the workpiece are released under high temperature, causing a redistribution of internal stresses and further altering the deformation characteristics of the workpiece.
To verify that the workpiece deformation originates from uneven stress distribution along the axial direction, residual stress measurements were conducted on the mid-sections of the first, second, and third axial segments, designated as P1, P2, and P3, respectively, as shown in
Figure 1. Four equally spaced measurement points were selected along the circumferential direction of each cross-section for axial residual stress evaluation. The averaged values for each cross-section were calculated for comparative analysis, as shown in
Figure 7.
From
Figure 7, it can be seen that after precision machining, the surface residual stresses of the workpiece exhibit negative values, indicating compressive stresses. The compressive stress distribution ranges from −78.5 to −493.7 MPa, with considerable variability. Significant difference in residual-stress values are observed across different cross-sections of the same workpiece. For instance, in workpiece 2, P1 = −200 MPa, whereas P3 = −475 MPa, demonstrating non-uniform axial distribution of residual stresses on the workpiece surface, which may induce workpiece deformation. Although each workpiece is processed using identical machining parameters, significant differences in residual stresses are present. The observed phenomenon arises from significant axial heterogeneity in initial residual stress distribution during material fabrication, coupled with post-machining stress redistribution, ultimately leading to pronounced surface stress variations.
In order to compare the residual stress values on the same section, the third group of workpieces was randomly selected, with the section at the middle of each axial segment chosen for residual stress measurement. On each cross-section, four measurement points are uniformly distributed along the circumferential direction, designated as σ
1, σ
2, σ
3, and σ
4, as shown in
Figure 8, and the measurement results are shown in
Figure 9.
The results demonstrate that the residual-stress values exhibit significant variations across different measurement points within the same section. For instance, at section P1, the maximum residual stress reaches −367 MPa, while the minimum is −142 MPa. Such severe circumferential non-uniformity in residual-stress distribution leads to warping and substantial deformation in long-axis workpieces with low stiffness.
3.3. The Influence of Turning Scheme on Deformation and Optimization Improvement
Based on the above experimental findings, it was concluded that TC18 titanium alloy demonstrates high sensitivity to stress and strain during turning operations, particularly when machining slender forged shafts. After annealing treatment, the maximum runout of the precision-machined workpiece reached 0.6682 mm. To address this, a semi-precision machining step with a 0.8 mm allowance was introduced prior to the annealing and final precision machining processes to ensure dimensional accuracy.
In order to investigate the effects of different precision machining schemes on the deformation and surface quality of the workpieces, the between-centers turning scheme was adopted to conduct a single-factor cutting experiment, where the feed rates were 0.05 mm/r, 0.1 mm/r, 0.15 mm/r, and 0.3 mm/r; the cutting speed values were 640 r/min, 800 r/min, 1000 r/min, and 1500 r/min; and the cutting depth values were 0.05 mm, 0.1 mm, 0.2 mm, and 0.4 mm. Due to the high sensitivity of the deformation degree during between-centers turning of slender shaft workpieces with eccentric structures to the thrust force of the center, instability frequently occurs. Therefore, the thrust force was varied as a variable, with the percentage of the rated thrust force of the machine tool as the variable factor, 6%, 10%, 15%, and 40%.
Furthermore, in order to determine the optimal turning parameters, workpiece vibration during machining must be taken into account. Specifically when inappropriate parameters are selected, workpiece vibration intensifies due to the combined effects of the thrust force of the center and centrifugal force. Consequently, surface roughness Ra was incorporated as an additional evaluation criterion, with measurement results presented in
Table 3.
The experimental results from groups 1, 2, 3, and 4 in
Table 3 demonstrate that when the thrust force of the center exceeds 15% of rated thrust force, the radial runout of the workpiece exhibits a significant increase, resulting in dimensional deviations and elevated surface roughness. The reason is that the low stiffness of the slender shaft workpiece intensifies its vibration under excessive thrust force, leading to increased runout and roughness. However, when the thrust force is reduced to 6%, the workpiece roughness still increases due to inadequate clamping, which fails to sufficiently dampen the vibrations. Additionally, the data from groups 2, 8, 9, and 10 reveal that when the cutting speed is elevated to 1500 r/min, the peak workpiece runout reaches 0.345 mm. This phenomenon is attributed to an eccentric geometry in the mid-section of the workpiece. At higher rotational speeds, the augmented centrifugal force intensifies machining vibrations, consequently increasing both workpiece deformation and surface roughness.
The experimental results from groups 2, 5, 6, and 7 demonstrate that when the cutting depth increases to 0.4 mm, the runout of the workpiece exhibits an increasing trend. The reason is that as the cutting depth increases, the workpiece is subjected to increased radial cutting force, and the radial compression of the workpiece increases, resulting in increased deformation. Compared with the surface roughness in groups 2 and 5, when the cutting depth reaches 0.2 mm in group 6, the roughness value exhibits a decreasing trend. The reason is that when the titanium alloy is cut, the depth of the hardened layer is about 0.2 mm [
17]. When the cutting depth exceeds the depth of the hardened layer of the workpiece, the vibration decreases. From the data of groups 2, 11, 12 and 13, it can be seen that when the feed rate increases to 0.3 mm/r, the runout of the workpiece increases and the roughness increases significantly, and the reason is that as the feed rate increases, the cutting force increases, causing an increase in workpiece vibration.
In summary, to minimize workpiece deformation and ensure surface quality during turning, between-centers turning should be employed, with strict control of the turning parameters. Optimal results for long-axis workpieces, characterized by minimal deformation and good surface quality, are achieved when the rotational speed is set to 640–800 rpm, the feed rate to 0.05–0.1 mm/r, the cutting depth to 0.1 mm, and the thrust force of the center to 10% of the rated value. Additionally, given the significant deformation that workpieces undergo after annealing, when utilizing the between-centers turning method, to ensure the positional and dimensional accuracy of the center holes, center holes should be refined or remachined if the billet length permits, guaranteeing concentricity between the center holes on both ends.
Based on the experimental results, exponential models for roughness
Ra and runout Rt are independently established, with their expressions formulated as follows:
The correction coefficient of
C depends on the processing material and cutting conditions;
ν,
ap,
f, and
F represent the rotational speed, cutting depth, feed rate, and the thrust force of the center, respectively. Items
k,
m,
n, and
q are constants associated with the cutting parameters. Equation (1) is subjected to linear transformation and linear regression analysis to calculate the linear regression correlation coefficient. The fitted parameter values are then substituted into the formula to obtain the exponential model (2) of surface roughness Ra, and the model is subjected to the F-test.
Based on the variance analysis of the empirical formula in
Table 4, the calculated F-statistic is 12.30944 at a significance level of α = 0.05. With F (p, n − p – 1) = F
0.05 (4, 8) = 3.84, with the model’s F-value exceeding this critical value, it is concluded that the model is statistically significant.
Furthermore, the exponential model for runout
Rt is formulated as follows:
Based on the variance analysis of the empirical formula in
Table 5, the calculated F-statistic is 4.488708 at a significance level of α = 0.05. With F (p, n − p – 1) = F
0.05 (4, 8) = 3.84, and the model’s F-value exceeding this critical value, it is concluded that the model is statistically significant.
3.5. Analysis of Grinding Effect Verification
After processing, the workpiece undergoes a sequence of processes comprising grinding, annealing, sandblasting, milky white chromium (MWC) coating, vacuum diffusion annealing, hard chromium (WHC) coating, and final precision grinding. To validate the efficacy of the optimized processing and heat treatment scheme in achieving final grinding compatibility and surface integrity, three workpieces with initial maximum runouts of 0.02 mm, 0.02 mm, and 0.06 mm were strategically selected for full-scale process validation. And the residual stress and deformation were measured, as shown in
Figure 15 and
Figure 16.
As shown in
Figure 15, the surface residual stress exhibits substantial fluctuations during the manufacturing process, with repeated alternations between compressive and tensile states. After turning, the surface residual compressive stress reaches −400 MPa, which is subsequently reduced to −200 MPa following the initial grinding stage. This stress evolution arises primarily from the higher material removal rate from turning compared to that from grinding, where the more severe plastic deformation induces greater compressive residual stresses.
Sandblasting can significantly increase the value of surface roughness and improve the adhesion of coatings, but also increase the residual compressive stress on the surface to approximately −600 MPa. Furthermore, as shown in
Figure 15, after grinding, the workpiece still needs to undergo two annealing processes, which effectively adjust its residual stress value to near 0 MPa, thereby eliminating the stress. During manufacturing processes, residual stress on the workpiece surface experiences dynamic transitions between compressive and tensile states, accompanied by substantial variations in stress magnitudes. Taking sample 3 as an example, during sandblasting and chrome plating, the residual stress value increases from −525 MPa to +566 MPa, which is not conducive to deformation control. Therefore, to mitigate workpiece deformation, beyond controlling the turning and heat treatment parameters, each process step requires stringent control. For instance, automated sandblasting equipment is recommended to ensure uniform stress distribution on the workpiece surface.
As shown in
Figure 16, multiple annealing and electroplating processes will progressively exacerbate workpiece deformation. Specifically, the runout of sample 1 and sample 2 measures 0.045 mm and 0.048 mm, respectively, whereas sample 3 exhibits a significantly higher runout of 0.083 mm. This trend arises from cyclic residual stress generation and redistribution during manufacturing, with localized stress inhomogeneity inducing radial runout accumulation. Notably, the initial runout of workpiece 1 and workpiece 2 is relatively small, so they can ultimately meet the requirement of 0.05 mm runout. These findings suggest that strict control of machining-induced runout is critical to reserve adequate dimensional tolerance for subsequent processes, such as sandblasting.
Following chromium electroplating and subsequent grinding processes, samples 1 and 2 met specifications, whereas sample 3 failed due to localized coating detachment at its point of maximum radial runout. As shown in
Figure 17, localized coating detachment occurred exclusively at the workpiece end. This phenomenon was attributed to warping deformation at this location, resulting in reduced coating thickness and inadequate interfacial bonding strength after grinding. Furthermore, as shown in
Figure 15, the residual tensile stress on the surface of the workpiece after chrome plating was relatively high, which can promote microcrack initiation and propagation toward the coating–substrate interface, degrading interfacial adhesion, then coating detachment may occur when interfacial adhesion strength falls below the applied grinding forces.
To further investigate the chromium layer microstructure after grinding and analyze the reasons for localized detachment of the chromium layer, samples 3 and 2 underwent wire electrical discharge machining, followed by mechanical polishing, electrolytic etching, and then were subjected to metallographic structure comparison observation, as shown in
Figure 18.
From
Figure 18, it is evident that the chromium layer surface is flat and smooth after grinding. In contrast, sample 3 exhibits localized detachment of the chromium layer, specifically at the interface between the hard chromium and milky chromium layers. The residual thickness of the hard chromium layer after grinding is approximately 10 μm, with localized detachment observed. Conversely, sample 2, featuring an initial radial runout of 0.02 mm, retained a coating thickness of about 30 μm after grinding, exhibiting uniform thickness distribution. When there was no detachment of the coating, and the appearance inspection showed no cracks, the product was qualified. Localized thinning of the coating or detachment occurs because the initial electroplating thickness is comparable, but significant workpiece runout leads to localized runout variations, causing thinning of the coating after grinding. When the thickness is less than 10 μm, the interfacial bonding strength between the hard chromium and milky chromium layers is insufficient to withstand the grinding shear forces, resulting in the detachment of the hard chromium layer. For workpieces with minimal radial runout, the grinding removal rate is uniform, ensuring uniform residual coating thickness. Therefore, it is essential to rigorously control workpiece deformation during processing to prevent the coating from becoming excessively thin or detaching.
To further analyze the microstructure and morphology of the substrate and coating and investigate the mechanisms underlying localized coating detachment, backscattered electron imaging and electron probe microanalyzer elemental mapping were conducted on the sample, with the corresponding results presented in
Figure 19.
As shown in
Figure 19, longitudinal microcracks are distributed within both the milky white chromium layer and the hard chromium layer, with transverse microcracks predominantly observed at their interface. Per the acceptance criteria, when the bonding force is guaranteed, the presence of non-penetrating microcracks in the coating is permissible. The formation of these microcracks may be attributed to substantial residual tensile stresses developed on the surface during electroplating. Surface microdefects in the coating, particularly pores, may serve as stress concentration sites, initiating cracking under tensile stress. During vacuum diffusion annealing, hydrogen desorption from the chromium layer induces localized volumetric contraction, which amplifies stress concentration and consequently promotes crack propagation. To characterize the compositional variations adjacent to microcracks, elemental composition analysis was conducted using an electron probe at selected locations and along defined trajectories, as shown in
Figure 20.
Scanning path 1 in
Figure 20a traverses the longitudinal crack within the coating, while scanning path 2 spans the continuous interface between the milky white chromium layer and the hard chromium layer. Scanning path 3 crosses the transverse crack located at the coating connection. As shown in
Figure 19 and
Figure 20, paths 1 and 3 intersect longitudinal and transverse cracks, respectively, where significant enrichment of O and S elements is observed. In contrast, path 2 passes through a crack-free interface without detectable enrichment of O and S elements. Given the elevated concentrations of O and S in the electrolyte, it can be inferred that microcracks develop during the electroplating process.
In summary, improper control of electroplating parameters, such as current density and solution ratio, can result in the formation of longitudinal cracks and transverse detachment within the coating. Additionally, during workpiece manufacturing, excessive runout leads to thinning of the coating after grinding, reducing the interfacial bonding strength, and directly causing localized coating detachment. Therefore, in the manufacturing process, the runout of the workpiece must be strictly controlled to <0.05 mm to ensure coating integrity.