1. Introduction
Tungsten alloys, due to their advantages of high density, hardness, high melting point, and corrosion resistance, are widely used in integrated circuits; medical devices; and aerospace, atomic energy, and other fields [
1,
2]. The surface smoothness of alloys is crucial for precision components that require ultra-high surface quality. The surface roughness of tungsten and its alloys is usually subject to strict demands [
1,
3,
4] in industrial applications.
Hard tungsten alloys have low machinability due to their high hardness and superior mechanical properties [
5]. Grinding and cutting are two of the most commonly used surface processing techniques [
6,
7]. However, materials processed by grinding are prone to elastic–plastic deformation. Moreover, obvious grinding marks on the surface reduce the surface quality of the alloys [
8]. The use of cutting methods can cause problems, such as brittle fracture of the alloys, subsurface cracking, and tool wear [
9,
10,
11]. A high degree of non-uniformity at far depths along the jet alignment direction is observed with abrasive machining. Neither of the abovementioned methods can perform ultra-precision machining on complex parts.
Electrochemical polishing is a processing technique in which a metal workpiece is used as the anode and the surface of the workpiece is selectively dissolved to obtain a smooth surface. The electrolytic process conforms to Faraday’s [
12,
13] law and is widely [
14,
15] used in the processing industry due to its high efficiency, low workpiece loss [
13], simple operation, and easy processing. At present, the electrolytic polishing solutions commonly used for tungsten alloys are acidic solutions, mainly sulfuric acid–methanol acidic electrolyte [
16]. Wang et al. [
17] observed that an appropriate concentration of sulfuric acid can form a dense tungstic acid colloid layer on the surface of Ni-W alloy, which affects the polishing effect of the alloy surface. Electropolishing in the H
2SO
4-CH
3OH electrolyte results in the anodic dissolution of tungsten, where anisotropic and isotropic etchings occur in two stages. The rate-controlling stages include charge transfer and mass transport, respectively [
18,
19]. However, the high sulfuric acid concentration leads to a high post-treatment cost.
In an alkaline environment, the surface quality of the tungsten alloys can be efficiently improved, and the alkaline electrolyte of NaOH [
20] can be used for tungsten alloys. Under this condition, tungsten is oxidized to form WO
3, and the resulting WO
3 interacts with the electrolyte and dissolves. The reaction equations are shown in Equations (1)–(3).
Due to the high hardness and corrosion resistance of tungsten alloys, alkaline polishing can avoid the excessive corrosion or grain boundary erosion that may be caused by acidic electrolytes. However, sodium hydroxide electrolyte may cause tungsten in the alloy to dissolve quickly, while other metals—such as Ni and Fe—dissolve slowly, resulting in uneven dissolution and poor surface quality. In addition, high concentrations of NaOH are highly corrosive, which presents an issue in ensuring the safety of equipment and operators. Moreover, high concentrations of NaOH lead to continuous etching, causing damage to the W surface. This has prompted the selection of an aqueous electrolyte with an optimized concentration [
21]. Recently, Deng et al. [
22] analyzed the effects of current- and potential-driven electrochemical polishing techniques, and proposed a two-step polishing process that resulted in a smoother and flatter tungsten surface.
Therefore, the polishing effect of tungsten alloys is greatly [
23,
24,
25,
26] influenced by the process conditions. Exploring a more environmentally friendly electrolyte and investigating the mechanism of electrochemical polishing of tungsten alloys can provide theoretical and technical guidance for the surface treatment of other high-hardness alloys. In-depth research on electrochemical polishing in tungsten alloys has both important engineering practical value and scientific significance. In this work, a novel trisodium phosphate–sodium hydroxide–glycerol electrolyte was explored for electrochemical polishing of tungsten–nickel–iron alloy. The rationality of using glycerol as an additive in the electrolyte was investigated through theoretical calculation, and the probable polishing mechanism was proposed.
2. Materials and Methods
The experimental setup is shown in
Figure 1. Tungsten alloy from Ganzhou Jiangwu Ferrotungsten Co., Ltd., Nachang, China (Composition: W 95 wt%, Ni 2.8–4.3 wt%, Fe 0.7–2.2 wt%) was cut into 1 cm × 1 cm × 0.2 cm pieces. Before electropolishing, the samples were polished with 400 mesh, 800 mesh, and 1200 mesh sandpaper for 30 min, respectively. To ensure the uniformity of polishing, the sandpaper was replaced after each test, and the direction of sandpaper movement was adjusted by 90°.
The samples were rinsed continuously with deionized water for 30 s, then ultrasonically oscillated in anhydrous ethanol to remove possible residual impurities on the surface. The ultrasonic-treated samples were washed again with deionized water to remove the anhydrous ethanol and then dried in air for 12 h. The electrolytic polishing solutions were prepared with sodium trisodium phosphate, sodium hydroxide, and glycerol in different volumes. During the electrochemical polishing process, DC power was supplied by HSPY-20-5 from Beijing han sheng PuYuan technology Co., Ltd., Beijing, China. The rotating speed magnetic stir bar was adjusted to 400 rpm. A titanium plate with a size of 5 cm × 5 cm × 0.02 cm was used as the cathode. The effects of the solution composition, temperature, and voltage on the tungsten–nickel–iron alloy surface were systematically explored.
The molecular structure of the additive was calculated using Materials Studio, and the frontier molecular orbitals and electrostatic potential distribution of the additive molecules were obtained using the Forcite and DMol3 modules, respectively. The molecular dynamics simulation method was used to study the adsorption behavior of additives on the tungsten (110) crystal surface. Firstly, the tungsten atomic crystal plane was constructed. The tungsten crystal was imported, the crystal plane index was input, the tungsten (110) was cut, and a vacuum layer was added to expand into a supercell. Then, a solution model was constructed, and the optimized additive molecules were placed into a solution box. Finally, the tungsten (110) crystal plane was combined with the solution box containing additives, and a 5 nm thick vacuum layer was added above the box to form an adsorption model. Molecular dynamics simulations were conducted using a Forcite module.
The roughness and 3D profile were measured with an Olympus BSX510 (San Diego, CA, USA), and the average of five roughness test points was taken. The “Confocal Mode” was selected and the pinhole was automatically enabled, switching the three-dimensional measurement mode. The sample surface was securely fixed on the stage. After selecting an appropriate magnification objective lens, the lateral and longitudinal parameters were adjusted to select a clear scanning plane. A software was used to rotate, zoom, and adjust the viewing angle to observe the three-dimensional morphology. The “Pseudo-colour Mode” was selected to provide a more intuitive display of surface undulations. The samples were scanned, and a three-dimensional morphology map was generated using a selected area of 499 × 499 μm. Each point was measured five times and the average was taken. The roughness of each sample was measured at five points to obtain the average roughness value. Microscopic topography analysis was conducted using a scanning electron microscope (HITACHI SU8010, Tokyo, Japan) with an acceleration voltage of 10.0 kV and a current of 10.0 μA.
3. Results and Discussion
The process parameters of the electrochemical polishing tungsten–nickel–iron alloy include voltage, temperature, and electrolyte composition.
Figure 2 and
Figure 3 show the effect of the trisodium phosphate concentration at 6 g/L of sodium hydroxide at 30 °C on electrochemical polishing tungsten–nickel–iron alloy. The alloy surface was the smoothest when the roughness of Sa was 0.582 μm and the trisodium phosphate content was 100 g·L
−1. When the trisodium phosphate content was reduced to 60 g·L
−1 and 80 g·L
−1, Sa was raised to 1.429 μm and 1.150 μm, respectively. As shown in
Figure 2a,b, the height difference of the alloy surface profile is distinct, indicating a larger surface roughness. The concentration of trisodium phosphate usually affects the viscosity of the electropolishing solution. When the trisodium phosphate concentration is low, the viscosity of the electrolyte is reduced, the tungsten alloy dissolves too quickly, and it fails to form a stable passivation film. When the trisodium phosphate content was raised to 120 g·L
−1 and 140 g·L
−1, Sa increased to 0.811 μm and 1.26 μm, respectively. Excessive trisodium phosphate leads to high viscosity in the solution, affecting the ion transfer rate and thereby the polishing effect.
Figure 4 shows the optical microscope images of tungsten–nickel–iron alloy under various trisodium phosphate concentrations. The surface was relatively rough at 60 g·L
−1 of trisodium phosphate but became smooth at 100 g·L
−1, which is consistent with the roughness test results shown in
Figure 2 and
Figure 3.
The additive is important to further improve the polishing effect. Glycerol can adsorb onto the anode surface during the polishing process, occupying specific adsorption sites and forming a stable adsorption layer used as a polisher for electropolishing 316 L steel [
27]. Glycerol and ascorbic acid additives can synergistically enhance copper surface glossiness and smoothness while slowing down the dissolution rate of the copper [
28]. Therefore, in this study, glycerol was chosen as an additive to slow down the polishing rate and make the polishing of tungsten–nickel–iron alloy smoother and more uniform. Molecular dynamics simulations were used to observe the adsorption behavior of additive molecules on the anode surface, which were conducted to study the adsorption process of glycerol on tungsten surfaces. The W(110) characteristic peak of the tungsten alloy was the strongest; therefore, cutting along the W(110) crystal plane simulated the adsorption state of glycerol on the actual tungsten–nickel–iron alloy.
Figure 5 shows the results of the calculation of the glycerol molecule.
Figure 5d displays the lowest unoccupied molecular orbitals (LUMO) of the glycerol molecule. The LUMO energy is −5.90 eV and the HOMO energy is 0.40 eV. The lower HOMO energy and the higher LUMO energy suggest that glycerol can readily accept electrons to participate in oxidation reactions. As shown in
Figure 5a, glycerol contains three hydroxyl groups, and the high electron density of the hydroxyl groups usually indicates strong polarity. The electron enrichment in the hydroxyl region can form an adsorption layer on the surface of tungsten–nickel–iron alloy, which inhibits the formation of microscopic pits and promotes the formation of smooth surfaces. Therefore, glycerol is a promising additive for use in a trisodium phosphate electrolytic polishing solution for tungsten–nickel–iron alloy.
Figure 6 and
Figure 7 show the effect of glycerol on the 3D profile and roughness of the surface of tungsten–nickel–iron alloy after electrochemical polishing. As shown in
Figure 7, with an increase in the glycerol content, the surface roughness of tungsten alloys first increased and then decreased. When the glycerol concentration was 100 mL/L, Sa reached a minimum of 0.617 μm. With a further increase in glycerol content, the Sa of tungsten alloy began to increase. An excessive amount of glycerol adsorbs on the surface of the tungsten alloy, resulting in a slower diffusion rate of the generated WO
42− ions and an increase in roughness. As shown in
Figure 6f, when the glycerol content increased to 250 mL/L, the roughness reached a value of 1.850 μm.
Optical microscope images of the tungsten alloy electropolished under various glycerol contents are shown in
Figure 8. The surface is relatively smooth when the glycerol concentration was 100 mL/L, which is consistent with the results illustrated in
Figure 6 and
Figure 7.
Voltage is an important factor affecting the polishing effect on tungsten–nickel–iron alloy. If the voltage is too low, the anodic process enters the dissolution zone, causing the workpiece to dissolve. Conversely, if the voltage or current density is too high, anodic polarization causes the release of oxygen gas, creating pits on the surface of the workpiece and increasing the roughness.
Figure 9 shows 3D profiles of electrochemical polishing for 35 s at different voltages with electrolyte concentrations of 100 g·L
−1 of trisodium phosphate and 8 g·L
−1 of sodium hydroxide.
Figure 10 demonstrates the corresponding changes in surface roughness of tungsten–nickel–iron alloy. At the optimal working voltage of 15 V, the lowest Sa was 0.560 μm.
In addition to the electrolyte and voltage, the temperature affects the rate of electron transfer and diffusion of components in electrolyte which, in turn, affects roughness. When the temperature rises, the electron transfer rate and the diffusion rate increase, but the thermal motion effect reduces the stability of the viscous film. The relationship between temperature and the diffusion coefficient is shown in the following formula:
In the formula,
D0 is the preceding factor,
Qa is the diffusion activation energy (J/mol),
T is the absolute temperature, and
K,
R is the ideal gas constant (J/mol·K).
D is substituted into the relationship between the limiting current
(A/m
2) and the diffusion coefficient:
where
δ is the thickness of the diffusion layer in meters,
n is the transfer electron number, and
C is the concentration with the unit of mol/L. So,
Therefore, the increase in temperature leads to an exponential increase in current density. When the temperature is low, the viscosity of the electrolyte increases. The anode mucora thickens, which decreases the diffusion of anode products. The bubbles remain on the anode surface, resulting in pockmarks and streaks. As the temperature rises, the viscosity of the diffusion layer decreases, making it difficult to maintain the viscous layer. Therefore, there is an optimal temperature for the electrochemical polishing process.
Figure 11 shows the 3D profile of the tungsten–nickel–iron alloy after electrochemical polishing under different temperatures, and
Figure 12 presents the roughness changes. The Sa of tungsten–nickel–iron alloy reached the lowest value of 0.582 μm at 55 °C. At lower temperatures of 30 °C and 45 °C, the diffusion coefficient decreased, in accordance with Formula (4). Therefore, the diffusion rate of the anode product was low, and the anodic dissolution efficiency was reduced. The Sa was 0.738 μm and 0.744 μm, respectively. At increased temperatures of 65 °C and 80 °C, the Sa was 1.192 μm and 1.639 μm, respectively. The increased temperature caused the viscous film to become unstable, the solution viscosity to decrease, and the viscous film to thin. Meanwhile, the diffusion coefficient increased, and the anode dissolution rate increased. Therefore, under higher temperatures, local corrosion formed rapidly, causing pits on the surface of tungsten–nickel–iron alloy.
Figure 13 shows optical microscope images of tungsten–nickel–iron alloy after electrochemical polishing at different temperatures. The images show that at 55 °C, the difference in the surface contour height of the sample was minimal, the surface morphology was relatively uniform, and the unevenness was significantly reduced.
Moreover, the difference in peak and valley heights on the surface of the tungsten–nickel–iron alloy causes a high current at the beginning of polishing. The height difference gradually decreases, and the difference in current density is reduced, resulting in a slower rate of roughness reduction. Therefore, there is an appropriate polishing time for electrochemical polishing of tungsten–nickel–iron alloy.
Figure 14 shows the 3D profiles of the surface of the tungsten–nickel–iron alloy after electrochemical polishing at different times. At a polishing time of 35 s, the height difference of the tungsten alloy surface profile was the smallest, with an Sa of 0.582 μm. There were no obvious ripples or etching pits on the sample surface. When the polishing time increased to 10 s, the Sa was 0.77 μm. When the polishing time was further increased to 120 s, the Sa increased to 3.078 μm. The effect of the polishing time on the surface roughness of tungsten–nickel–iron alloy is summarized in
Figure 15.
Figure 16 shows surface optical microscopy images of tungsten alloy after electrochemical polishing at different polishing times. With an increase in the polishing time, the surface roughness of the sample first decreased and then increased, which is consistent with the results shown in
Figure 14 and
Figure 15.
In conclusion, the trisodium phosphate–sodium hydroxide–glycerol electrolyte is effective for electrochemical polishing of tungsten–nickel–iron alloy. The polishing effect of tungsten–nickel–iron alloy is greatly influenced by process conditions. The optimized electropolishing parameters for tungsten alloy are summarized in
Table 1.
The mechanism of electropolishing is also crucial, as it can reveal the essential rules and internal connections, providing guidance for subsequent investigations. The electrochemical polishing mechanisms include the viscous film theory [
20], the salt film theory [
23], and the oxide dissolution–equilibrium theory [
21,
24,
25]. When a constant voltage is applied for time t of electrolytic polishing, the current gradually decreases to a stable value i
0. Elmore et al. [
29] believe that the formation of the platform is due to the generation of a viscous film layer. The solubility of the viscous film layer in the electrolyte reaches saturation. The limit of the diffusion rate determines the intensity of the limiting diffusion current. Therefore, the stable electrolytic polishing current is determined by the value of the limiting diffusion current. i
0t
1/2 is a constant value.
Figure 17a,b show the i-t curves measured at different voltages, and the i
0t
1/2 values can be calculated at different voltages, respectively. As shown in
Figure 17a, after applying a certain voltage for electrochemical polishing, the voltage gradually became stable. As shown in
Figure 17b, the i
0t
1/2 values at different voltages were nearly equal. Therefore, electrochemical polishing of the trisodium phosphate electrolyte is considered to be performed through the sticky film mechanism.
Figure 18 shows the scanning electron microscope images of the tungsten–nickel–iron alloy surface before and after electrochemical polishing. Before polishing, there were obvious protrusions and striped mottling distribution on the surface of the sample, thus having a higher roughness. After polishing, the protrusions on the tungsten–nickel–iron alloy surface decreased significantly. Meanwhile, the pitting disappeared, and the height difference between peaks and valleys obviously decreased. All of these factors indicate a decrease in surface roughness. The grains and grain boundaries on the surface of tungsten–nickel–iron alloy could be observed. The Sa was 0.582 μm, which is much lower than the original Sa of 1.134 μm. This shows that the electrolyte with trisodium phosphate, sodium hydroxide, and glycerol is effective for electropolishing tungsten alloy. To the contrary, no obvious improvement in smoothness was observed when using sodium hydroxide electrolyte for electropolishing tungsten alloy [
14].