Reversible Superwetting Transition Between Superhydrophilicity and Superhydrophobicity on a Copper Sheet, and Its Corrosion Performance

Introduction

The superwetting surface has attracted considerable research interest due to its important application in self-cleaning, oil/water separation, corrosion resistance, and so on (Forooshani et al., 2017a; Bagheri et al., 2017; Forooshani et al., 2017b; Bagheri et al., 2018; Forooshani et al., 2019; BaratiDarband et al., 2020; Hatte and Pitchumani, 2021). Generally, a surface with water contact angles (WCAs) greater than 150° and slide angles less than 10° is called the superhydrophobic surface (Taghvaei et al., 2021). A rough structure and surface chemical energy are very significant to the composition of the superhydrophobic surface (Siddiqui et al., 2021a). The preparation of the superhydrophobic surface is generally divided into two steps. The first step is to prepare a rough structure on a solid surface through various methods, and the second step is to modify with low surface energy substances (Yu et al., 2021).

With the rapid development of the smart surface with controlled wetting behavior, reversible superwetting transition between superhydrophobicity and superhydrophilicity has received particular attention (Ding et al., 2018; Wan et al., 2018; Brehm et al., 2020; Zhao et al., 2020). UV irradiation (Li et al., 2013; Yang et al., 2017; Jiang et al., 2019), pH (Yu et al., 2005; Chen et al., 2017; Cheng et al., 2019), electric field (Idriss et al., 2020), and heat treatment (Wang et al., 2021) are widely reported as external stimuli for achieving wettability transition in many literatures. Among the mentioned external stimuli, UV has been extensively employed, because some photocatalytic materials, such as ZnO, TiO₂, and SnO₂, can realize wettability transition under UV irradiation (Velayi and Norouzbeigi, 2019). However, these reported methods have many drawbacks, such as long transition time, complex fabrication process, and high costs. For example, Zhou et al. (Zhou et al., 2019) fabricated a superhydrophobic TiO₂ film with excellent UV responsibility by anodic oxidation. The superhydrophobic film could be changed into superhydrophilicity within 13 min under UV irradiation. Nevertheless, the transition time from superhydrophilicity to superhydrophobicity requires 100 h when it was heated at 60°C in the dark. Li et al. (Li et al., 2019a) fabricated the superhydrophobic micro/nano-scale hierarchical structure on brass surfaces by laser ablation. The results revealed that an alternative heating–reheating cycle can lead to a reversible change between superhydrophobicity and superhydrophilicity within 5 h. But the sample preparation process and the instrument used were complicated. In addition, the corrosion performance of reversible superwetting transition is always examined when the surface is superhydrophobic, but few studies have been carried out.

In this study, a superhydrophobic surface composed of copper oxide nanoribbons arrays was successfully fabricated on a copper sheet surface by simple and low-cost solution-immersion methods. The superhydrophobic surface can be achieved by soaking stearic acid. Noteworthy, the reversible transition between superhydrophobicity and superhydrophilicity can be easily achieved by heat treatment and re-modification. In addition, the corrosion current density and impedance spectrum of superwetting surfaces were also studied.

Experimental Procedure

Preparation of a Superhydrophobic Surface Composed of Copper Oxide Nanoribbons Arrays

Copper sheet with a thickness of 0.5 mm was used as a substrate material. First, copper sheets were ultrasonically cleaned with HCl (3 M). Second, the cleaned copper sheets were etched in NH₃·H₂O (0.03 M) at 20°C for one day in a water bath pot, followed through washing with distilled water and drying with blower. Last, the treated copper sheets were placed in the ethanol solution of stearic acid (0.2 mol L⁻¹) for 2 h in order to obtain superhydrophobic properties.

Reversible Superwetting Transition of Copper Oxide Nanoribbons Arrays

The prepared superhydrophobic samples can be converted into superhydrophilic ones after being heated at 400°C for 150 s in a muffle furnace. The wettability properties reversed into superhydrophobicity just by soaking in the ethanol solution of stearic acid for 10 s.

Sample Characterization

The surface morphology of copper sheet was observed by using a scanning electron microscope (SEM) (JEOL JSM-6610LV). The composition of the sample was employed by X-ray diffraction (XRD-600, Japan). The measurement of WCAs was carried out by using a contact angle measuring instrument (JC 2000C1, Shanghai). The standard three-electrode system was used (CHI 760E, Shanghai), in which the samples with an exposed area of 1 cm² served as the working electrode, the Ag/AgCl was the reference electrode, and graphite was the counter electrode.

Results and Discussion

Structures of Surface and Reversible Wettability

Figure 1A presents the SEM micrographs of the bare copper sheet by ultrasonic cleaning with HCl. It can be confirmed that the surface of copper has only a few scratches and some patchy defects. Figure 1B shows the copper oxide nanoribbons arrays well aligned which are fabricated on a copper sheet. It can be seen from the high magnification image in Figure 1C that nanoribbons are bundled together. Figure 1D shows the cross sections of the copper oxide nanoribbons arrays whose thickness is approximately 5 μm. Figure 2 shows the XRD of patterns of copper oxide nanoribbons arrays prepared on the copper sheet. The diffraction peaks of (002) and (200) correspond to the copper oxide crystals, except two peaks (111) and (200) from the copper sheet. This shows that the micro/nano-scale hierarchical structure on the copper sheet is copper oxide.

FIGURE 1

FIGURE 1. SEM micrographs of (A) bare copper, (B) copper oxide nanoribbons arrays, (C) higher magnification image, and (D) cross-sectional image.

FIGURE 2

FIGURE 2. XRD of patterns of copper oxide nanoribbons arrays fabricated on a copper sheet.

Figure 3A shows that the WCA on the modified copper oxide nanoribbons array film is about 153.6°. The formation mechanism of superhydrophobicity can be expressed by Cassie equation (Wenzel, 1936), which is as follows:

$\cos {\theta }^{\ast }=-1+f_1(1+\cos \theta ),(1)$

where θ* is the WCA on the modified copper oxide nanoribbons arrays film, θ is the WCA on the smooth copper sheet, and f₁ is the fraction of solid in contact with the water droplets. It can be estimated from Figure 1 that the value of f₁ is about 0.1. The WCA on the smooth copper sheet is about 85°. The theoretical calculation results are in good agreement with the experimental results. After the heat treatment at 400°C in a muffle furnace for 150 s, the wettability of prepared film becomes superhydrophilic and the WCA is about 0°, as shown in Figure 3B. The film can recover its superhydrophobic properties after re-modification with stearic acid for 10 s. This process can be repeated for at least 4 cycles, as shown in Figure 4.

FIGURE 3

FIGURE 3. Shapes of water droplets on the prepare film (A) superhydrophobic and (B) superhydrophilic under the alternation of heat treatment and re-modification.

FIGURE 4

FIGURE 4. The reversible wettability transition between superhydrophobicity and superhydrophilicity under the alternation of heat treatment and re-modification.

Rough structure and low surface energy organic matter are important factors to obtain the superhydrophobic surface. Stearic acid is a commonly used modifier to obtain a low surface energy (Li H. et al., 2019). Figure 5 shows the Fourier transform infrared (FTIR) spectra of copper oxide nanoribbons arrays, copper oxide nanoribbons arrays after modification by stearic acid, and copper oxide nanoribbons arrays after heat treatment. Figure 5A shows the three characteristic absorption peaks of copper oxide. This indicates nanoribbons arrays fabricated on the copper sheet are copper oxide. As shown in Figure 5B, two absorption peaks at 2,918 and 2,850 cm⁻¹ are derived from the stretching vibration of the C–H bond (Meth and Sukenik, 2003). This indicates that stearic acid forms a self-assembled monolayer on the surface of the sample. A new absorption peak appears at 1,585 cm⁻¹ corresponding to -COOH- groups, indicating that stearic acid forms a chemical bond with copper oxide. When copper oxide was heated, Figure 5C depicts that the three peaks that belong to stearic acid in Figure 5B disappear. To explain the disappearance of the absorption peaks, Figure 6 presents results from the thermogravimetric analysis differential scanning calorimetric (TG-DSC) of stearic acid. A distinct endothermal peak appears at near 300°C. This demonstrates that the stearic acid coating on the surface of copper oxide is totally decomposed. Therefore, it can be inferred that the wettability transition from superhydrophobicity to superhydrophilicity is due to the increase of surface energy after the heat treatment. The wettability of the prepared film will turn into superhydrophobic after re-modification, as shown in Figure 3.

FIGURE 5

FIGURE 5. Fourier transform infrared (FTIR) spectra of copper oxide nanoribbons arrays (A), copper oxide nanoribbons arrays after modification by stearic acid (B), and copper oxide nanoribbons arrays after heat treatment (C).

FIGURE 6

FIGURE 6. Thermogravimetric analysis differential scanning calorimetric (TG-DSC) of stearic acid.

Corrosion Resistance and Mechanism

Figure 7 presents the digital graph of prepared film immersed into 3.5 wt% NaCl solution. It can be seen that the surface of the prepared film is relatively bright due to total reflection. Air is a medium with a lower refractive index relative to the sodium chloride solution. The incident ray will all be reflected if the incident angle is greater than a certain critical angle. This suggests that a lot of air is trapped among the rough structure of the prepared film. Meanwhile, this trapped air can protect the copper sheet through blocking the contact of corrosion solution and copper. Thus, this superhydrophobic film can be used to prevent metal corrosion.

FIGURE 7

FIGURE 7. Digital graph of the superhydrophobic film immersed into 3.5 wt% NaCl solution.

In order to investigate the corrosion resistant property of the prepared film, Figure 8 shows the potentiodynamic polarization curves of a bare copper sheet, superhydrophilic film, and superhydrophobic film. Taking bare copper as an example (Figure 9), the values of E_corr and i_corr can be obtained from Tafel polarization curves. In general, the lower corrosion current and more positive corrosion potential means better corrosion resistance. The corrosion potential of the samples was −0.299, −0.331, and −0.136 V, respectively. The parameters associated with Tafel curves are summarized in Table. 1.

FIGURE 8

FIGURE 8. Potentiodynamic polarization curves of bare copper, superhydrophilic film, and superhydrophobic film.

FIGURE 9

FIGURE 9. Tafel polarization curves of bare copper.

TABLE 1

TABLE 1. Potential dynamic results of different samples after immersion in simulated seawater.

The corresponding corrosion inhibition efficiency can be expressed as follows (Li et al., 2019b):

$\eta =\frac{i_{corr}^o-i_{corr}}{i_{corr}^o},(2)$

where $i_{corr}^o$and $i_{corr}$represent the corrosion current density of bare copper sheet and prepared film, respectively. The corrosion inhibition efficiency of superhydrophilic surface is −41.16%. This indicates that the superhydrophilic surface not only fails to protect the metal surface but also accelerates corrosion. For the bare copper sheet, it is easy to form a dense layer of oxide on the surface. In the preparation of the superhydrophilic surface, the dense layer of oxide will become rough, resulting in a larger contact area with the corrosion solution. Thus, the inhibition efficiency of the superhydrophilic surface is negative. The corrosion of copper substrate is greatly slowed as a result of the separation of the corrosion liquid from the copper sheet by air. Therefore, the inhibition efficiency of the superhydrophobic surface is 93.24%.

Figure 10 shows the Nyquist plots of bare copper sheet, superhydrophilic film, and superhydrophobic film. The Nyquist plots of bare copper sheet and superhydrophilic film are made up of a circular arc at a high frequency and a straight line at a low frequency. It is well known that the larger arc radius means a larger resistance. In addition, the higher the slopes of Warburg impedance, the faster the electrolyte ion diffusion at the electrode interface. Thus, the bare copper sheet exhibits better corrosion resistance than the superhydrophilic film. The impedance semicircle diameter of superhydrophobic film is about tens of thousands of Ω·cm², which is consistent with results in Figure 8 and Table 1. In the Bode plot (as shown in Figure 11), the superhydrophobic surface has the largest impedance modulus. An equivalent circuit shown in Figure 12 was proposed to fit the Nyquist plots of three samples. As shown in Figure 12A, the equivalent circuit model representing the electrochemical behavior of the copper sheet and superhydrophilic film, demonstrated by the similar Nyquist plot. R_s, R_p, R_t, W, and CPE represent solution resistance, corrosion layer resistance, charge transfer resistance, diffusion resistance, and double-layer capacitance, respectively (Siddiqui et al., 2021b). The equivalent circuit of superhydrophobic film is presented in Figure 12B. R_f and C_f represent the resistance and capacitance of the air layer, respectively. After fitting, the electrochemical parameters of three samples are shown in Table. 2. It can be seen that the superhydrophobic film has the best corrosion resistance.

FIGURE 10

FIGURE 10. Nyquist plots of bare copper, superhydrophilic film, and superhydrophobic film.

FIGURE 11

FIGURE 11. Bode plots of bare copper, superhydrophilic film, and superhydrophobic film.

FIGURE 12

FIGURE 12. The equivalent circuit about cooper substrate, superhydrophilic film (A), and superhydrophobic film (B) after immersion in simulated seawater.

TABLE 2

TABLE 2. Corresponding fitted electrochemical parameters of bare copper sheet, superhydrophilic film and superhydrophobic film after immersion in simulated seawater. The three samples are labeled as 1, 2, and 3, respectively.

In order to evaluate the actual anticorrosion behavior of the superhydrophobic film, Figure 13 shows the Tafel curves of superhydrophobic film after in 3.5 wt% NaCl solution for 3 and 5 days. The corresponding corrosion current density (i_corr) and the corrosion potential (E_corr) are summarized in Table 3. With the increase of soaking time from 0 to 5 days, the corrosion inhibition efficiency only decreases from 93.24 to 86.94%. This indicates that the air which is trapped in the micro/nano-scale hierarchical structure can slow the chlorine ion attack on metal surfaces. Figure 14 shows the Nyquist plot of the superhydrophobic film after in 3.5 wt% NaCl solution for different times. The impedance semicircle diameters of the superhydrophobic film decrease slowly even after immersion for 5 days.

FIGURE 13

FIGURE 13. Tafel curves of superhydrophobic film after in 3.5 wt% NaCl solution for 3 and 5 days.

TABLE 3

TABLE 3. Potential dynamic results of the superhydrophobic film after immersion in simulated seawater for different times.

FIGURE 14

FIGURE 14. Nyquist plot of superhydrophobic film after in 3.5 wt% NaCl solution for different times.

Durability of Superhydrophobic Surface

In practical applications, superhydrophobic surfaces are often exposed to acidic or alkaline environments, so it is essential for superhydrophobic surfaces to have a good stability. The prepared superhydropbhobic surfaces are immersed in solutions of pH = 4 and 10 at different times (Figure 15). The WCA decreased slowly with the increase of immersion time in both alkaline and acidic environments. However, the WCA decreases slowly in alkaline solution in comparison with the acidic solution. This behavior indicates that the superhydrophobic surface is more resistant to the alkaline environment than an acidic one.

FIGURE 15

FIGURE 15. The WCA is tested after immersion in solutions of pH = 4 and pH = 10 with different times.

Conclusion

In summary, the copper sheet-based copper oxide nanoribbons arrays are fabricated through a simple low temperature hydrothermal method. The wettability of the prepared film is superhydrophobic after modification by stearic acid with a WCA of 153.6°. In addition, the WCA can reach up to 0° after heat treatment at 400°C for 150 s. The reversible wettability transition between superhydrophobicity and superhydrophilicity can be easily achieved by heat treatment and modification. Meanwhile, the entire transition time requires only 170 s. The electrochemical measurement results illustrate that the superhydrophobic film has higher anticorrosion performance. Even if the superhydrophobic film was immersed in simulated seawater for 5 days, its corrosion inhibition efficiency only decreases from 93.24 to 86.94%. Therefore, this article may provide a useful attempt for corrosion protection.

Data Availability Statement

The original contributions presented in the study are included in the article/Supplementary Material; further inquiries can be directed to the corresponding author.

Author Contributions

TC, YL, XF, XC and QL participated in the discussion and gave useful suggestions. The manuscript was composed by HL and JZ. All authors read and approved the final manuscript.

Funding

This work was supported by the Natural Science Foundation of Anhui Province (1808085ME140), the National Natural Science Foundation of China (11974127 and 51973078), and the Natural Science general Foundation of Anhui Higher Education Institutions of China (KJ2020B09).

Conflict of Interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s Note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

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