Jingming Liua,
Min Wangb,
Chengyu Gub,
Lehua Zhangb and
Ying Yan*b
aShanghai Academy of Fine Arts, Shanghai University, Shanghai 200444, China
bState Environmental Protection Key Laboratory of Environmental Risk Assessment and Control on Chemical Process, East China University of Science and Technology, Shanghai 200237, China. E-mail: wendy0101@126.com
First published on 29th September 2021
With the background of contemporary art, using comprehensive materials to create artworks is becoming more and more common. The new era of digital image-based copperplate artworks, using photosensitive lithography, has given traditional art forms new life and greater popularity in the digital age. However, the patterns and textures of the works created by the new techniques are generally shallow, and the copper surface is easily damaged and loses its aesthetic value, which makes it a practical problem to protect such works more effectively. In this paper, a facile method is adopted, wherein a superhydrophobic film is constructed on the surface of copperplate images by straightforward immersion in (heptadecafluoro-1,1,2,2-tetradecyl)trimethoxysilane (FAS-17) solution to achieve the anticorrosive protection of copperplate artworks. The hydrophobicity of the copper surface was analyzed using an instrument that measures contact angles. The superhydrophobic surface morphology and composition were analyzed with a scanning electron microscope coupled with an energy-dispersive spectrometer, and the corrosion resistance was analyzed using an electrochemical workstation. A systematic study is presented on the effect of the immersion time in FAS-17 and the concentration of FAS-17, and the optimal preparation conditions of the superhydrophobic film were determined, which means that the copper substrates were immersed in 0.7 mol L−1 FAS-17 for 40 min. After the treatment of the surface to make it superhydrophobic, the contact angle and the corrosion inhibition efficiency of the copperplate etching surface reached 161.2° and 95.7%, respectively. The results show that the superhydrophobic film was successfully prepared on the surface of the artwork based on copper, which can effectively improve the corrosion resistance and is beneficial for the long-term protection of artwork.
The art of copper etchings enjoys a worldwide reputation for its advanced technology and cultural connotations over the years, which make it quite precious. In contemporary times, copper etchings appear as new and creative methods and have become a new artistic carrier. Combined with the traditional art of new media and digital technology, the ancient etchings form the digital image-based etchings of the new era. Etchings based on digital images are not the same as traditional techniques; they are no longer in the form of direct hand painting but computers are first used for image creation, then the satisfactory image is output into a film, using the film to expose the copper plate coated with photosensitive adhesive or film to obtain the digital copperplate artwork. Although these artworks created with this new technique have strong availability and popularity, there are also some shortcomings. For example, the patterns and textures formed are generally shallow, and beauty and value are easily lost because the copper surface is corroded. How to more effectively protect copper bases from corrosion is a practical problem for the long-term preservation of such artworks.
Although copper and its alloys are characterized by relatively good corrosion resistance and fouling resistance, they are prone to corrosion and serious surface discoloration due to long-term exposure to humid air or the presence of corrosive media such as CN− and Cl−.1 Corrosion inhibition is one of the effective methods for solving the problem of the corrosion of copper and its alloys. At present, the most extensive method is to select suitable organic compounds as corrosion inhibitors, such as benzotriazole and its derivatives, various thiazole derivatives2 and imidazole.3 However, most of these inhibitors are expensive and toxic and are not good for the environment, so their use is limited. As such, the development of an environmentally friendly and economical metal protective layer on copper surfaces has gradually become a research hotspot in recent years. The superhydrophobic surface method has been attracting more and more attention2 and it is based on the concept of “the Lotus effect” proposed by German botanist Wilhelm Barthlott.1,4 The superhydrophobic surface method that mimics the lotus leaf effect has the advantages of hydrophobicity and self-cleaning.2–6
At present, the preparation of a superhydrophobic surface can be roughly divided into two categories: the construction of a micron-nano-sized rough structure on the surface of hydrophobic materials with low surface energy or modifications of this rough structure using low-surface energy materials.7 Preparation methods for superhydrophobic surfaces mainly include the template method, the electrochemical method, the etching method,8 the gel method,9 the layered self-assembly method10 and so on. Active hydrophobic organic molecular groups used to prepare superhydrophobic films on the surface of metal bases include –SiOH, –SH, and –COOH.9 Common hydrophobic materials include siloxane, fluoroalkyl silane, nutmeg acid, stearic acid,11,12 etc.
The study of superhydrophobic surfaces has generally focused on pure metal or alloys. Recently, the fabrication of superhydrophobic surfaces has been applied to the surfaces of pure copper,13 magnesium alloy14 and other metals. Due to the special structural composition of copperplate artistic works, many difficulties remain in the study of superhydrophobic surfaces. At present, there are few studies in this field.
In this paper, a (heptadecafluoro-1,1,2,2-tetradecyl)trimethoxysilane (FAS-17) solution was used to prepare a superhydrophobic surface on copperplate artworks. The hydrophobicity and corrosion resistance of superhydrophobic surfaces have been investigated. By measuring contact angles, surface hydrophobicity was analyzed, and the superhydrophobic surface morphology characteristics and composition analysis were determined using a scanning electron microscope coupled with an energy-dispersive spectrometer. An electrochemical workstation was used to perform the corrosion resistance analysis to prove that this method has a good inhibitory effect on copper corrosion. This study can be used as a reference for long-term anti-corrosion protection of copperplate artworks by preparing long-acting and durable super-hydrophobic anti-corrosion surfaces and enhancing the cleanliness and aesthetics of the works' surfaces.
The copperplate etching of size 10 mm × 10 mm × 1 mm was polished using 400-1500# abrasive paper and then cleaned with acetone, ethanol, and deionized water for 10 min. The pretreated copper samples were immersed in the mixture of sodium hydroxide with a concentration of 2.50 mol L−1 and ammonium persulphate with a concentration of 0.23 mol L−1 for 15 min to obtain a rougher surface structure, and then cleaned and dried. After immersing in different concentrations of FAS-17 for a certain time, the test pieces were taken out of the solution, washed with ethanol several times, and dried naturally in the air.
The copperplate artworks that were dipped and not dipped were placed in an ozone aging chamber at 30 °C for the corrosion test. The test lasted 7 days and included an ozone concentration of 100 ppm and a humidity of 85%.
A GonloStar200 contact angle measuring instrument was used to measure the contact angle of the sample surface at room temperature. The liquid droplet volume was 14 μL. The superhydrophobic surface morphology was observed using an S-3400 scanning electron microscope coupled with energy-dispersive spectroscopy (SEM-EDS).
The electrochemical impedance spectra (EIS) and the polarization curves (Tafel) were obtained on a CHI600E electrochemical workstation. A standard three-electrode system was adopted. The exposed area of the working electrode was 1.0 cm2, the platinum wire electrode was used as the auxiliary electrode, and the calomel electrode was used as the reference electrode. The corrosive medium was a solution that simulated atmospheric conditions, which contained 0.028 mol L−1 NaCl + 0.01 mol L−1 Na2SO4 + 0.016 mol L−1 NaHCO3. The working electrode was immersed in this solution for 2 h in advance and tested at room temperature after the open circuit potential was stable. The EIS scanning range was 10 mHz to 95 kHz, and the ac amplitude was 10 mV. The scanning range of the polarization curve was ±250 mV (relative to the open circuit potential), and the scanning rate was 1 mV s−1.
The superhydrophobicity can be expressed by the Cassie–Baxter equation (eqn (1)):15
cosθc = f1cosθ − f2 | (1) |
Immersion time | f1 | f2 |
---|---|---|
Blank | 1.000 | 0.000 |
10 min | 0.273 | 0.726 |
20 min | 0.149 | 0.850 |
30 min | 0.116 | 0.883 |
40 min | 0.046 | 0.953 |
50 min | 0.110 | 0.889 |
60 min | 0.139 | 0.860 |
Concentration (mol L−1) | f1 | f2 |
---|---|---|
Blank | 1.000 | 0.000 |
0.1 | 0.140 | 0.859 |
0.3 | 0.064 | 0.935 |
0.5 | 0.031 | 0.968 |
0.7 | 0.026 | 0.973 |
0.9 | 0.040 | 0.959 |
f2 reached the maximum values of 95.3% and 97.3% under the optimal conditions, which indicated that the “air cushion” hinders the direct contact of water droplets with the copperplate artwork.16
Fig. 3 SEM-EDS image of a copper specimen surface. (a) Surface of a copper substrate; (b) surface of a copper substrate with superhydrophobic film. |
Elemental compositions | Cu/wt% | Zn/wt% | C/wt% | O/wt% | F/wt% | Si/wt% |
---|---|---|---|---|---|---|
Blank | 58.34 | 38.63 | 2.11 | 0.93 | — | — |
Copper substrate with superhydrophobic film | 59.55 | 24.37 | 2.32 | 11.00 | 2.28 | 0.49 |
η = (1 − Jcorr/J0corr) × 100% |
Fig. 4 Polarization curves of a copper substrate with superhydrophobic film prepared under different immersion times in a solution simulating atmospheric conditions. |
Immersion time | Ecorr/mV | Jcorr/mA cm−2 | βa/mV | βc/mV | η/% |
---|---|---|---|---|---|
0 min | −0.162 | 5.70 × 10−2 | 489.00 | 75.57 | — |
10 min | −0.077 | 3.28 × 10−2 | 236.29 | 54.74 | 42.5 |
20 min | −0.068 | 8.47 × 10−3 | 190.08 | 68.90 | 85.1 |
30 min | −0.078 | 1.24 × 10−2 | 240.67 | 70.97 | 78.2 |
40 min | −0.062 | 5.07 × 10−3 | 191.46 | 70.35 | 91.1 |
50 min | −0.066 | 7.98 × 10−3 | 208.68 | 56.08 | 86.0 |
60 min | −0.068 | 1.03 × 10−2 | 230.63 | 51.88 | 81.9 |
Fig. 5(a) shows the Nyquist plots and their fitting for the copper substrate samples before and after fabrication of the superhydrophobic surface by immersion in a solution simulating atmospheric conditions. The arc diameter of the capacitive reactance first increased and then decreased with the increasing immersion time. It is worth mentioning that the larger arc diameter represents higher charge transfer resistance.18 As shown in Fig. 5(a), when the immersion time was 40 min, the arc radius of the superhydrophobic sample was the largest, which is consistent with the results of the polarization curves.
It can be seen from Fig. 5(b) that there is one time constant for the untreated copper substrate and there are two time constants for the superhydrophobic specimens, so the measured results can be fitted by the electrical equivalent circuit shown in Fig. 5(c) and (d), respectively. The fitted EIS parameters are listed in Table 5.
Immersion time | Rs/Ω cm2 | YCPEf/Ω−1 cm−2 | nf | Rf/Ω cm2 | YCPEdl/Ω−1 cm−2 | ndl | Rct/Ω cm2 |
---|---|---|---|---|---|---|---|
0 min | 36.13 | — | — | — | 0.001106 | 0.6263 | 609.6 |
10 min | 20.28 | 2.156 × 10−5 | 0.5981 | 106.8 | 1.603 × 10−4 | 0.7285 | 1147 |
20 min | 20.36 | 2.402 × 10−5 | 0.5667 | 214.8 | 1.413 × 10−4 | 0.6426 | 1982 |
30 min | 19.41 | 2.679 × 10−5 | 0.5783 | 218.3 | 1.119 × 10−4 | 0.8211 | 2190 |
40 min | 17.54 | 4.496 × 10−5 | 0.5493 | 272.1 | 7.536 × 10−5 | 0.7871 | 3813 |
50 min | 18.51 | 6.135 × 10−5 | 0.4131 | 204.0 | 8.036 × 10−5 | 0.8679 | 2331 |
60 min | 19.01 | 5.003 × 10−5 | 0.5657 | 204.5 | 9.260 × 10−5 | 0.8250 | 2169 |
Table 5 shows that the Rct (the charge transfer resistance) tended to increase, especially for the immersion time of 40 min, reaching 3813 Ω cm2, which increased by one order of magnitude as compared to the bare copper. The larger the charge transfer resistance, the more difficult it is for the corrosion medium to transfer to the copper surface and to produce an electrochemical corrosion reaction. The Rf (the surface film resistance) had a similar tendency to the Rct. The changes in the values of Rct and Rf indicate that the corrosion resistance of the copper substrate surface after the fabrication of the superhydrophobic surface with FAS-17 was significantly improved.
Fig. 6 Polarization curves of a copper substrate under different concentrations of FAS-17 in solutions simulating atmospheric conditions. |
Concentration | Ecorr/mV | Jcorr/mA cm−2 | βa/mV | βc/mV | η/% |
---|---|---|---|---|---|
0 mol L−1 | −0.162 | 5.70 × 10−2 | 489.00 | 75.57 | — |
0.1 mol L−1 | −0.049 | 6.79 × 10−3 | 189.79 | 63.33 | 88.1 |
0.3 mol L−1 | −0.061 | 5.85 × 10−3 | 193.54 | 47.54 | 89.7 |
0.5 mol L−1 | −0.057 | 3.56 × 10−3 | 172.47 | 56.61 | 93.8 |
0.7 mol L−1 | −0.051 | 2.46 × 10−3 | 171.94 | 70.88 | 95.7 |
0.9 mol L−1 | −0.065 | 2.95 × 10−3 | 173.07 | 52.05 | 94.8 |
The Nyquist plots for samples immersed in different concentrations of FAS-17 are shown in Fig. 7(a). The sample with 0.7 mol L−1 FAS-17 treatment exhibited the largest diameter of capacitive loop, indicating that the copper substrate plate had the best superhydrophobicity under these conditions. Fig. 7(b) represents the Bode plots of the samples. There are two time constants for superhydrophobic samples, so Fig. 5(d) can be used to fit the electrochemical data; the results are listed in Table 7. Compared to the bare copper, both Rct and Rf increased and peaked at about 1.063 × 104 Ω cm2 and 112.2 Ω cm2, respectively, at 0.7 mol L−1 of FAS-17. Combining Tables 5 and 7, it can be seen that the best process for preparing superhydrophobic films on the copper surface is to immerse in a FAS-17 solution with the concentration of 0.7 mol L−1 for 40 min.
Fig. 7 Nyquist (a) plots and Bode (b) plots of the copper substrate in solutions simulating atmospheric conditions. |
Concentration | Rs/Ω cm2 | YCPEf/Ω−1 cm−2 | nf | Rf/Ω cm2 | YCPEdl/Ω−1 cm−2 | ndl | Rct/Ω cm2 |
---|---|---|---|---|---|---|---|
0 mol L−1 | 36.13 | — | — | — | 0.001106 | 0.6263 | 609.6 |
0.1 mol L−1 | 16.87 | 1.449 × 10−5 | 0.6521 | 79.35 | 6.788 × 10−5 | 0.6801 | 5.020 × 103 |
0.3 mol L−1 | 17.92 | 1.687 × 10−5 | 0.5594 | 80.73 | 6.165 × 10−5 | 0.6657 | 5.793 × 103 |
0.5 mol L−1 | 19.52 | 2.679 × 10−5 | 0.5783 | 82.67 | 5.735 × 10−5 | 0.6651 | 2.190 × 103 |
0.7 mol L−1 | 18.28 | 1.376 × 10−5 | 0.6616 | 112.2 | 5.386 × 10−5 | 0.7021 | 1.063 × 104 |
0.9 mol L−1 | 13.24 | 1.691 × 10−5 | 0.6907 | 75.83 | 5.607 × 10−5 | 0.6728 | 8.271 × 103 |
Fig. 8 Nyquist plots (a) and polarization curves (b) for superhydrophobic copper in a solution simulating atmospheric conditions for different immersion times. |
Time | Rs/Ω cm2 | YCPEf/Ω−1 cm−2 | nf | Rf/Ω cm2 | YCPEdl/Ω−1 cm−2 | ndl | Rct/Ω cm2 |
---|---|---|---|---|---|---|---|
Blank | 36.13 | — | — | — | 0.001106 | 0.6263 | 6.096 × 102 |
Immerse for 2 h | 17.54 | 4.496 × 10−5 | 0.5493 | 272.1 | 7.536 × 10−5 | 0.7871 | 3.813 × 103 |
Immerse for 7 d | 18.24 | 4.691 × 10−5 | 0.6907 | 156.83 | 8.407 × 10−5 | 0.6728 | 2.371 × 103 |
Time | Ecorr/V | Icorr/mA cm−2 | βa/mV | βc/mV | η/% |
---|---|---|---|---|---|
Blank | −0.162 | 5.70 × 10−2 | 489.00 | 75.57 | — |
Immerse for 2 h | −0.066 | 5.07 × 10−3 | 191.46 | 70.35 | 91.1 |
Immerse for 7 d | −0.086 | 6.21 × 10−3 | 208.33 | 102.93 | 89.1 |
This journal is © The Royal Society of Chemistry 2021 |