1. Introduction
Medical-grade stainless steel 316L (SS 316L) is widely employed in numerous biomedical applications owing to its exceptional mechanical strength and cost-effectiveness [
1,
2]. Traditional machining of this material suffers from inadequate surface integrity due to elevated cutting pressures and temperatures at tool–work contact, resulting in significant tool wear [
3,
4]. This frequently leads to elevated machining expenses and subpar surface quality [
5]. Non-conventional machining methods are regarded as superior for machining SS 316L [
6].
A range of unconventional methods has been established, including electrochemical machining, electrical discharge machining and chemical machining [
7,
8]. Among them, electropolishing is particularly suitable for the fabrication of metallic materials, especially stainless steel 316L [
9]. Electropolishing, as a novel machining technique, provides exceptional opportunities for the treatment and shaping of robust industrial materials such as SS 316L [
10]. The lack of physical contact between the tool and the workpiece material results in negligible or absent mechanical and thermal stresses [
11]. In the electropolishing process, any hard conductive material can be machined using a softer tool material [
12]. Furthermore, it offers numerous advantages over alternative machining methods, including smooth and crack-free surfaces, burr-free finishes, little tool wear, an elevated material removal rate, and the capability to fabricate complex geometric shapes [
13]. The material removal method is predicated on Faraday’s law of electrolysis, wherein anodic dissolution of the workpiece occurs within the electrolyte [
14]. In electropolishing, a voltage of 5–30 V is delivered across the minimal cutting gap between the tool (cathode) and the workpiece (anode) [
15].
Electropolishing is often performed in concentrated acid electrolytes, including phosphoric acid, sulphuric acid, perchloric acid, and their combinations, depending on the materials of the workpiece [
16]. Lu [
17] conducted electropolishing and magnetoelectropolishing surface treatments on SS 316L in a solution of 20% HClO
4 and 80% CH
3COOH (vol%). A magnetic field with a flux density of 0.3 T was applied to the surface of the electropolishing workpiece. An elevated chromium content and a more protective passive coating can be attained with MEP treatment, which accelerates the selective dissolution of magnetic components like iron and nickel during electropolishing under a magnetic field. Using synchrotron X-ray imaging and multiphysics modelling, Mi et al. [
18] studied how electromagnetic pulses (which affect the solidification dynamics of intermetallic phases) improve phase distribution, fluid flow, and microstructures. This refers to magnetoelectropolishing, whereby an applied magnetic field improves ion transport and surface homogeneity during electropolishing. Magnetic fields in electropolishing increase surface smoothing by influencing electrolyte flow and ion removal, whereas EMPs maximize metal solidification by managing phase transitions, hence producing more homogeneous and defect-free surfaces. Both systems improve material qualities and performance by using electromagnetic forces.
Hryniewicz examined the corrosion characteristics of SS 316L following magnetoelectropolishing at 0.35 T in a sulphuric/orthophosphoric acids electrolyte mixture, and found out that magnetoelectropolishing elevated the chromium content of the surface and enhanced corrosion resistance [
19]. Given the environmental and safety concerns associated with prevalent acid-based electrolytes for electropolishing, there is a significant demand for the development of new eco-friendly and safe polishing electrolytes that yield high surface quality [
20].
An eco-friendly electrolyte is provided and filled in the machining gap to facilitate current flow and to transport heat and dissolved metal [
21]. The rate of anodic dissolution is influenced by electrical characteristics, electrolyte attributes, the distance of the machining gap and material qualities [
22]. Researchers have conducted extensive studies to determine the various degrees of process parameters for enhanced electropolishing performance. Kim employed the Taguchi method to ascertain the optimal parameters for the electropolishing process of titanium [
23]. They found that the voltage exerted the most substantial impact on surface roughness, directly affecting the thickness and microstructure of the oxide layer; however, excessive voltage resulted in surface damage. In addition, according to the Taguchi robust design, the ideal parameters for titanium electropolishing are a voltage of 16 V, a process period of 25 min, a temperature of 35 °C, an ethylene glycol ratio of 2, and a concentration of 30% additional distilled water.
Likewise, environmentally sustainable electrolytes are being explored for titanium; similar to stainless steel studies, elevated temperatures were utilized without altering the flux density, and the previous research was not optimized. Consequently, due to these deficiencies, the current study determined the optimal conditions for the electropolishing of SS 316L using NaCl-based solutions enhanced with ethanol, applying the Taguchi robust design approach. This method involved conducting an analysis of variance (ANOVA) and enhancing the signal-to-noise ratio through Taguchi’s “the-larger-the-better” criterion. The Pareto ANOVA technique was employed to assess the influence of four machining factors (applied voltage, ethanol concentration in the electrolyte, machining gap, and magnetic field) and their levels on achieving a high material removal rate. In addition, surface analysis was performed utilizing a surface roughness tester, and the outcomes of each treatment were compared.
3. Results and Discussion
Table 5 encapsulates the findings of the material removal rate from three iterations and the S/N ratio for each L
9 orthogonal array subsequent to the completion of the nine experimental matrixes. The mean S/N ratio for each factor, as presented in
Table 6, can be derived from the numerical data in
Table 5.
Figure 2 illustrates the average signal-to-noise ratio for each level, together with the individual effects of each factor, referred to as major effects.
3.1. Optimal Level Combination for Each Factor
This study aims to enhance the material removal rate by identifying the ideal amount for each element. The best level for each factor can be identified by the level that exhibits the maximum signal-to-noise ratio value.
Figure 3 and
Table 7 indicate that the optimal combination of each factor includes an applied voltage of 10 V, an ethanol concentration of 20 vol.%, a magnetic field of 0.4 T, and a machining gap of 0.5 cm, all of which significantly enhance the material removal rate.
Table 8 presents the Pareto ANOVA for the material removal rate during the electropolishing of SS 316L. The critical elements selected from the left side of the aforementioned Pareto diagram, presented in
Table 8 and
Figure 4, collectively represent approximately 90% of the total. The flux density’s contribution to this experiment exceeds 90%, as indicated in
Table 8, demonstrating that the magnetic field is not pivotal in attaining a high material removal rate. Hence, it is necessary to set the machining conditions as: applied voltage of 10 V, a machining gap of 5 mm, and an ethanol concentration of 20 vol.%.
Three verification experiments were conducted to assess the repeatability of the optimal combination of machining parameters outlined in
Table 9. The highest average material removal rate, 6.07 mg/min, is derived from the validation test results presented in
Table 5. The combination of the levels for each factor can be confirmed as accurate and designated as the best parameters for SS 316L electropolishing.
3.2. Effect of Applied Voltage on the Electropolishing Process
The critical factors in Pareto ANOVA analysis are selected from the left-hand side, collectively accounting for approximately 90% of the total contribution. According to the Pareto analysis presented in
Table 8, the applied voltage has been identified as a critical parameter in the electropolishing process, demonstrating a significance of 53.42% in achieving substantial material removal.
In the process of electropolishing, the current density–voltage curve is typically employed to analyze the dissolution mechanism of the anodic material [
24].
Figure 5 illustrates the current density–voltage curve of the electropolishing process for several materials, incorporating the etching, passivating, polishing, and gas evolution zones. In the etching zones, the workpiece is directly dissolved. The mechanically polished surface leads to the development of pitting on the metal surface in this area. In the passivating zone, the current density gradually declines with higher voltage due to the formation of a passive oxide layer on the anodic surface. In the gas evolution zone, the passive oxide layer deteriorates as the voltage increases, and anodic dissolution occurs with the generation of oxygen. The presence of oxygen bubbles trapped on the workpiece surface facilitates the occurrence of pitting in this area, which is consequently referred to as the pitting zone. This process induces rapid anodic dissolution, therefore, as the applied voltage rises, the machining current in the inter-electrode gap escalates, resulting in an improved material removal rate [
25]. The applied voltage accounts for 53.42% of the significance level, and the statistical analysis confirmed the density–voltage correlation to achieve a high clearance rate.
3.3. Effect of Machining Gap on the Electropolishing Process
Table 8 indicates that the machining gap is a substantial impact (21.84%) in enhancing the material removal rate. A narrower machining gap width (5 mm) between the anode and cathode results in an increased material removal rate, as illustrated in
Figure 6. The gap width between the electrode and the workpiece directly affects the current conditions and the discharge residues of the electrolyte. A narrow interelectrode gap generates a strong electric field, leading to elevated current density and thus, significant material removal. However, a reduced interelectrode distance has some drawbacks. Firstly, it is likely to induce a short circuit [
26], and secondly, the flushing of the electrolyte becomes progressively more difficult due to the prolonged duration of electropolishing, which negatively affects the precision of the process.
3.4. Effect of Ethanol Concentration on the Electropolishing Process
This study utilizes ionic liquids, a mixture of ethylene glycol and salt, along with ethanol as an addition, with concentration being one of the variables examined for its impact on enhancing material removal.
Table 8 presents the Pareto ANOVA analysis, indicating that the concentration of ethanol in the electrolyte solution (ethylene glycol-NaCl) significantly influences the material removal rate by 16.57%. This component is regarded as a crucial parameter in material removal, as it cumulatively surpasses 90% following the application of voltage and the machining gap. As the concentration of ethanol rises, the material removal rate of 316L samples escalates, suggesting that ethanol exerts a facilitative influence on dissolution. This is due to the fact that ethanol lowers the solubility of ferrous ions in comparison to water; it increases the dissolving rate and is therefore essential for the electropolishing of SS 316L [
27,
28]. Higher acidity of ethanolic solutions promotes the SS 316L deterioration during electropolishing. Moreover, ethanol affects important electrolyte characteristics including viscosity, conductivity, and mass transfer, therefore optimizing the metal removal mechanism. Ethanol reduces surface tension, thereby facilitating gas bubble dissociation and increasing ion mobility at the metal–electrolyte interface, so promoting a more homogeneous dissolving process [
29].
Moreover, ethanol changes the anodic dissolution mechanism, therefore preventing overly strong localized etching and producing a surface finish with the best possible material removal rate [
30]. It also diminishes the creation and dimensions of oxygen bubbles produced during anodic reactions, enhancing electrolyte–metal contact and polishing uniformity [
31]. The physicochemical effects collectively reveal the moderate yet significant impact of ethanol concentration identified in the Taguchi-ANOVA analysis, confirming its mechanistic function in enhancing electropolishing efficacy.
3.5. Effect of Magnetic Field on the Electropolishing Process
Numerous attempts have been made to explore the magnetoelectropolishing technology by examining the impact of incorporating a magnetic field into the electropolishing process. Electropolishing and magnetoelectropolishing were conducted on commercially available titanium during the experiment. The experimental results demonstrated that electropolishing alters the surface chemistry and morphology by creating a porous structure, whereas magnetoelectropolishing yields a microgranular structure. By affecting mass transfer, gas bubble dynamics, and electrolyte flow, a magnetic field applied in electropolishing improves the material removal rate. Lorentz forces produced by the interaction of the magnetic field with the electric current in the electrolyte cause magnetohydrodynamic convection, hence lowering the diffusion layer thickness and accelerating the movement of dissolved metal ions away from the surface. This increases the efficiency of anodic dissolution, hence raising the MRR. Furthermore, the magnetic field enhances gas bubble detachment, therefore avoiding their obstruction of active polishing sites and guaranteeing a consistent material removal procedure. Furthermore, the field changes electrolyte conductivity and ion mobility, so optimizing the electrochemical interactions engaged in metal dissolution. The best magnetic field intensity found in this work was 0.4 T. On the other hand, increasing the magnetic field strength over 0.4 T produces a Lorentz force so strong that it disturbs the electrolyte’s convective flow and causes turbulence [
29,
32,
33]. This outcome is consistent with other studies in which, mostly due to better mass transfer and bubble removal efficiency, introducing a magnetic field boosts the material removal rate compared to traditional electropolishing [
30].
In this work, while the magnetic field contributes to an increased material removal rate, it is not as significant a parameter as the applied voltage, machining gap, and ethanol concentration in the electrolyte, as shown in
Table 8. The Pareto ANOVA figure demonstrates that the contribution ratio of the magnetic field to the increase in material removal rate is merely 8.17%, suggesting that this parameter is not relevant for achieving a greater material removal rate.
3.6. Effect of Electropolishing Process on Water Contact Angle
One of the most important characteristics of a metal surface in a biomedical device application is its hydrophilicity. The surface hydrophilicity of the manufactured electropolished surface can be examined using the water contact angle of the surface. In general, a hydrophilic surface denotes a smaller contact angle—one that is less than 90⁰.
Figure 6 displays the electropolished membrane’s contact angles. The electropolished membranes with the best machining parameters are the most hydrophobic, as seen in
Figure 7. The most hydrophilic surface was achieved with an applied voltage of 8 V, a 0% ethanol content, a 0.41 T magnetic field, and a 15 mm machining gap.
3.7. Effect of Electropolishing Process on Surface Finish
Table 10 presents the surface roughness outcomes derived from the instrumental parameters shown in
Table 4, together with the identified optimal parameter (
Table 10). The optimal electropolishing parameters established by material removal rate were an applied voltage of 10 V, a machining gap of 5 mm, an ethanol concentration of 20 vol.%, and a magnetic field strength of 0.4 T. Under these conditions, the average surface roughness was 0.7
, which is substantially greater than the minimum value of 0.56
derived from the experimental parameters. In electropolishing, an increased material removal rate typically results in greater surface roughness, indicating that while rapid material removal can expedite the process, it frequently yields a less smooth surface finish; thus, the quicker the material is removed, the more irregular the surface may become [
34].
Figure 8 shows the surface morphology of the electropolished SS 316L. As presented in
Figure 8, the choice of machining parameters in electropolishing significantly influences the final surface topography and the material removal distribution within the electropolished region. Consequently, the choice of optimal electropolishing parameters is essential, as shown in this study, resulting in a notable decrease in surface roughness when compared to other surfaces processed at a low material removal rate.
According to
Table 10, experiment no. 1 exhibited the lowest surface roughness at 0.56
, coinciding with the lowest material removal rate observed.
Table 10 indicates that the minimum surface roughness of the electropolished SS 316L (0.56
) was observed in trial no. 1, which also showed the lowest material removal rate. Additionally, the morphology exhibited some inconsistencies, attributed to the lack of applied voltage and the absence of ethanol in the electrolyte.
Improving the material removal rate in electropolishing directly addresses key manufacturing constraints such as production efficiency, cost reduction, and surface quality. A higher MRR reduces processing time, allowing manufacturers to increase throughput while maintaining high-quality surface coatings. This is critical in industries like medical devices, where precision and fluidity are essential. Additionally, an enhanced MRR lowers energy consumption and electrolyte usage, reducing overall production costs while ensuring conformance with industry standards for corrosion resistance and biocompatibility.