4.1. Template
- (1)
Surface Roughness and Topography
The optical profilometer was used to observe and measure the surface roughness of the aluminum alloy obtained by different machining methods. The results are shown in
Figure 6. Compared with the surface of the unprocessed aluminum alloy, the surface roughness of the aluminum-alloy plate processed by EDM wire cutting was higher, and that of the workpiece roughed by EDM wire cutting was the highest. The roughness of the workpiece was reduced after the trimming treatment, but it was still higher than that of the unprocessed aluminum-alloy plate. By contrast, the surface roughness of the milled aluminum alloy was reduced compared to that of the unprocessed aluminum-alloy plate.
- (2)
Surface topography
The surface roughness of different specimen is measured by surface profilometer. The surface topography of different specimen is measured by surface profilometer and SEM, as shown in
Figure 7. The surface roughness of an unmachined surface and specimens produced by milling, WEDM rough machining, WEDM single-pass trim machining and WEDM double-pass trim machining were 1.56 μm, 0.77 μm, 2.92 μm, 2.48 μm and 1.80 μm, respectively. From the above results, it can be seen that the surface roughness of samples produced by milling was the lowest. The surface roughness of samples produced by WEDM was higher than that of the unprocessed surface. This is mainly because the micro/submicro discharge topography was constructed on the specimen surface. In addition, as the number of trim machining increased, the surface roughness gradually decreased. This is because the discharge energy of a single pulse in precision machining was lower, the feed rate was smaller, and the erosion of the dielectric was more thorough, resulting in a smaller size of discharge craters and easier removal of discharge erosion residues. Moreover, it can be also found that the micro/submicro discharge topography mainly included pits and protrusions. The size of these pits and protrusions was about 0.5–30 μm. As the surface roughness of the sample decreased, the size of pits and protrusions gradually decreased.
- (3)
Solid−liquid contact angle
The apparent contact angle of different specimens was measured by a high-temperature contact-angle-measuring instrument. The apparent contact angles of the unmachined surface and samples produced by milling, WEDM rough machining, WEDM single-pass trim machining and WEDM double-pass trim machining were 77°, 80.5°, 116.5°, 110°, and 107°, respectively. From this, it can be seen that the apparent contact angle of the samples processed by WEDM was significantly greater than that of the untreated sample surface and the milled sample surface. This is mainly because the micro/submicro discharge topography that formed after WEDM was conducive to the formation of an air-cushion effect during the solid−liquid contact process, reducing the solid−liquid contact area and thereby increasing the solid−liquid contact angle. In addition, the apparent contact angle of the sample after WEDM rough machining was the largest, while the apparent contact angle of the sample after WEDM trim machining was slightly reduced, as shown in
Figure 8. It can be concluded that with the reduction in roughness, the contact angle decreased, that there was a positive correlation between the contact angle and the roughness in a certain range, and that the larger discharge morphology was conducive to promoting the air-cushion effect and increasing the apparent contact angle. Although the roughness of the surface after milling was lower than that of the unmachined surface, during milling, some fine structures on the tool created microstructures on the surface of the aluminum alloy, resulting in an increase in the contact angle.
According to
Figure 8, it can be seen that the contact angle on the specimen surface machined by WEDM rough machining was the highest. Therefore, WEDM rough machining was adopted for processing surface texture. The solid−liquid contact angle on the surface texture of different templates was measured by high-temperature contact angle measuring instrument, as shown in
Table 4. From
Table 4, it can be seen that the maximum contact angle on the triangular surface texture and the rectangular surface texture exceeds 150°, which reach superhydrophobic state. Overall, the contact angle on the triangular surface texture was higher than that on the rectangular surface texture. In the triangular surface texture, when the ratio of height to bottom was small, water droplets tended to collapse and come into contact with the bottom of the surface texture, resulting in a smaller contact angle. The contact angle on the rectangular surface texture processed by WEDM was significantly greater than that of the rectangular surface texture processed by milling. This is mainly because the micro/submicro discharge topography was formed on the surface texture after WEDM rough machining, which was conducive to the formation of air-cushion effect and thus reduces the solid−liquid contact area.
Figure 9 shows the comparison between experimental and simulated values of contact angle. The simulation value of the solid−liquid contact angle was in good agreement with the experimental value, and the average error was 1.14%. From this, it can be seen that the established solid−liquid contact angle simulation model has high accuracy, which can guide the design of superhydrophobic templates.
- (4)
Wear resistance
Figure 10 shows the surface contact angle on the triangular texture template after different wear cycles. It can be seen that there was no obvious decrease in the surface contact angle on the template after 350 wear cycles. This is mainly because the triangular texture on the template surface becomes trapezoidal in texture after sandpaper wear. The discharge topography at the top of the triangular texture will be destroyed. However, the discharge topography on the side of the triangular texture cannot be damaged. Together with the trapezoidal texture, the discharge topography can still form an air-cushion support to reduce the solid−liquid contact area. Hence, it can be said that the template with triangular surface texture prepared by WEDM has good wear resistance.
4.2. Polymer Film
- (1)
Demolding residue
According to the above analysis, the contact angle on triangular surface texture is larger than that on rectangular surface texture. In addition, as shown in
Figure 11, it can be observed that during the demolding process of polymer films, there were very few residues on the triangular surface texture template and that the residues were almost invisible to the human eye. The surface texture of the prepared polymer film was complete and defect-free. However, there were many PDMS residues on the rectangular surface texture template. The surface-texture defects of the prepared polymer film were obvious, and there were many pit defects. Therefore, choosing the triangular surface texture as the final template is more appropriate.
- (2)
Molding rate
Figure 12 shows the measurement results of the surface texture on polymer films by a super depth of field microscope. From
Figure 12, it can be seen that the shape of the surface texture was basically the same. The height and width of different contours were generally the same.
Table 5 shows the size comparison of triangle surface-texture template and polymer film. It was found that the surface texture size on the polymer film was very close to that on the template, with a relative error of less than 3%. This means that polymer films prepared using triangular surface-texture templates have a higher molding rate.
- (3)
Solid−liquid contact angle
Figure 13 shows the measured result of contact angle on polymer films without surface texture. The templates that generated the results shown in
Figure 13a,b were an unprocessed surface and a WEDM surface, respectively. The contact angles on
Figure 13a,b were 119.8° and 131.5°, respectively. This is mainly due to the fact that, although there was no surface texture, the micro/submicro discharge topography of WEDM can be replicated onto the surface of polymer films, where it can enhance the air-cushion effect and reduce the solid−liquid contact angle. The surface energies of the films were calculated by the two-liquid method [
45], and the surface energy of the film was reduced from 22.156 mN/m to 18.632 mN/m. The roughness of the two films was measured using an optical profiler, and the results showed that the roughness of the films prepared by the EDM template was higher than that of the unmachined films (
Figure 14), which indicates that higher roughness is conducive to forming a higher contact angle.
Figure 15 shows the SEM image of the film, and it can be seen that there were many pits and bumps on it. This is because after EDM machining, due to the discharge of electrode wire, pits and bumps formed on the surface of the template and were copied to the film.
Figure 16 shows the measurements of contact angles on polymer films with triangular surface texture. It can be seen that all contact angles exceeded 150°. The maximum contact angle was 154.8°. In addition, it can be observed that the solid−liquid contact states on the surfaces of Size I, Size II, and Size III were the Cassie−Baxter state. The solid−liquid contact state on the surface of Size IV was the Wenzel state. This means that the prepared polymer film attained a superhydrophobic state through the combination of a triangular surface texture and WEDM rough machining.
- (4)
Reusability
The same template was used to repeatedly prepare superhydrophobic polymer film. The number of repetitions was 50. The measured contact angles on the template and the polymer-film surface are shown in
Table 6. Compared to
Figure 16 and
Table 6, after 50 repetitions of preparation, there was no significant change in the contact angle on the surface of the template and the polymer film. All contact angles on the polymer-film surface were larger than 150°. Hence, it can be said that the template with triangular surface texture prepared by WEDM has good reusability.
- (5)
Wear resistance
Figure 17 shows the surface contact angle on polymer film after different numbers of wear cycles. It can be seen that the contact angle on the surface of the polymer film slightly decreased with wear. Besides, the contact angle on the triangular textured surfaces of size I and size III was still larger than 150°, maintaining superhydrophobic state. This is mainly because that the wear resistance of polymer material is not as good as that of metal material. The top of the surface texture on the film is prone to wear. The height of the surface texture was reduced. Water droplets on the surface of polymer films tend to contact the bottom of the surface texture. This may cause the solid−liquid contact state to transition from the Cassie−Baxter state to the Wenzel state. Therefore, it can be said that the prepared superhydrophobic polymer film has high wear resistance.
- (6)
Self-restoring
Figure 18 shows the results from measuring scratches on the polymer-film surface. It can be seen that there was a clear scratch (depth of 13.42 μm) on the surface of the polymer film just after the film was scratched. As the standing time increased, the scratch on the surface of the polymer film gradually reduced in size and the depth of the scratch gradually became shallower. After the film had stood for 120 min, the scratch depth was reduced to 7.09 μm. After the film had stood for 24 h, the scratch was almost invisible to the human eye.
Figure 18d shows the relationship between scratch depth and contact angle. It can be observed that, just after the film was scratched, the contact angle on the polymer-film surface was only 127°. This is mainly because that the scratch damaged the hierarchical structure of the polymer-film surface. As the standing time increased, the surface contact angle on the polymer film gradually increased. After the film had stood for 120 min, the surface contact angle on the polymer film was 154° and the superhydrophobicity of the polymer film was restored. Therefore, it can be said that the prepared superhydrophobic polymer film has good self-healing capacity.
- (7)
Bending resistance
Figure 19 shows the surface contact angle on polymer film after different numbers of bending cycles. It can be observed that the contact angle on the polymer film slightly decreased with the increase in the number of bending cycles. After it had been bent 500 times, there was no obvious crease, crack or fold on the surface of the polymer film. The surface contact angle on the polymer film still exceeded 150°. Therefore, it can be said that the prepared superhydrophobic polymer film has good bending resistance.
- (8)
Ductility
Before the tensile test, the film thickness was measured with vernier caliper, and the average value was taken for five measurements. The film thickness was 2.04 mm.
Figure 20 and
Figure 21 shows the stress-strain curve of polymer film in the tensile test. It can be seen that, unlike metal materials, polymer film will immediately fracture when the stress exceeds the critical value. The maximum stress that the polymer film could withstand was 1.27 MPa, and the elongation was 16.53%. After the tensile test, the surface contact angle near the fracture of the polymer film exceeded 150°, at 151.6° and 156°. That is, polymer film after tensile testing still exhibited superhydrophobicity. Therefore, it can be said that the prepared superhydrophobic film has excellent ductility and tensile strength.
- (9)
Self-cleaning
Figure 22 shows the result of the self-cleaning experiment on different polymer films. As shown in
Figure 22a, after the water droplets had been dropped onto the polymer film, the surface fine sand could not be completely removed with the water droplets. Some of the fine sand mixed with the water and remained on the surface of the polymer film. As shown in
Figure 22b, after the water droplets had fallen on the polymer film, water droplets quickly rolled off the surface of the polymer in a spherical shape. The fine sand on the polymer surface was completely carried away by the water droplets in the path the water droplets passed through. This indicates that the prepared polymer film has good self-cleaning performance.
- (10)
Anti-icing
A drop of water (4 μL) was dropped onto polymer film and placed in a low-temperature test chamber at a temperature of −12 °C. The camera was applied to observe and record the entire process of the water droplet freezing as shown in
Figure 23.
Table 7 shows the freezing schedule of water droplets on different polymer-film surfaces. Comparing the template of the unprocessed surface with the template created by WEDM without surface texture, it can be seen that the micro/submicro discharge topography of WEDM can delay the start of time to freezing but has little effect on the overall time to freezing. This is mainly due to the fact that the single-stage surface microstructure can reduce the solid−liquid contact area and heat-transfer area through the air-cushion effect. Thus, the start time of freezing is delayed. However, as the icing process progresses, the water droplet volume expands and the air-cushion effect of the single-stage surface microstructure is destroyed. The heat-transfer area is the same as that of a regular surface and cannot increase the overall time to freezing. Moreover, comparing the template of Size I with the template created by WEDM without surface texture, it can be seen that the multi-level hierarchical microstructure can obviously increase the start time and overall time of freezing. The start time and overall time of freezing were 892 s and 970 s, respectively. This is mainly because, under the combined effect of the primary surface texture and secondary discharge topography, the contact state between water droplets and polymer films was the Cassie−Baxter state, which can significantly reduce the solid−liquid contact area. In addition, the air layer between the water droplets and the polymer film can reduce the heat-transfer rate. Furthermore, comparing the template of Size I with Size IV, it can be observed that the anti-icing ability of the surface in the Cassie−Baxter state was significantly better than that of the surface in the Wenzel state. This is mainly because there is no air layer between water droplets and the surface of a polymer film in the Wenzel state.