3.1. Characterization of Graphite Powders
A scanning electron microscope (SEM) was used to study the morphology of graphite.
Supplementary Figure S1 shows that graphite powder is composed of a variety of large particles, with an estimating size distribution of 0.65–11.37 μm. The graphite powder was characterized by Raman spectroscopy. The ID/IG value was 0.907, indicating that a relatively high graphitization degree was found in the material. The carbon nitride nanosheets were tested by X-ray diffraction (XRD). As shown in
Supplementary Figure S2, the nanosheets were identified as g-C3N4, corresponding to (100) and (002) plane, respectively.
Using TGA, the thermal stability of the pPy and pPy/C coatings in an N2 atmosphere was studied. In
Figure S3, it was evident that the pPy/C coatings had slightly improved thermal behavior in contrast to pure pPy before 200 °C. At the end of the analysis, the residues in the pPy and pPy/C coatings were 18.19% and 21.79% (
w/
w), respectively. Due to the encapsulation of graphite powder into a polymeric substrate, the pPy/C coating exhibited better thermal stability since the inorganic-oriented particles with rigid structures would inevitably reinforce the intrinsic nature of polymers.
The typical FT-IR spectra of the composite coatings in the range of 4000–400 cm
−1 are shown in
Figure S4a. For comparison, the spectrum of graphite powder is also shown in
Figure S4. From the FT-IR spectrum of CNNS, it can be seen that the strong and wide absorption peak at 3400–3100 cm
−1 corresponds to the stretching vibration peak of the N-H bond, the peak at 1640–1230 cm
−1 corresponds to the stretching vibration peak of the N-H bond, and the peak near 890 cm
−1 corresponds to the tensile vibration peak of the N-H bond on the surface of triazine cyclic compounds. The peak near 806 cm
−1 corresponds to the bending vibration peak of triazine cyclic compounds.
It can be seen from the FT-IR spectrum of PMMA that the peak at 2950 cm−1 corresponds to the stretching vibration peak of methylene, the absorption peak at 1730 cm−1 corresponds to the characteristic absorption peak of carbonyl C=O, the absorption peak at 1630 cm−1 corresponds to the characteristic absorption peak of PMMA, and the absorption peak at 1450 cm−1 corresponds to the characteristic absorption peak of methylene. The characteristic absorption peaks in CNNS and PMMA appeared in the infrared spectrum of the CNNS/PMMA film, respectively, which indicates the successful preparation of the CNNS/PMMA film. The absorption peaks at 3400 cm−1 correspond to the stretching vibration peaks of N-H bonds, and the absorption peaks at 1680 cm−1 and 1540 cm−1 correspond to the stretching vibration peaks of C-N bonds and C-C bonds in pyrrole. The absorption peaks at 1150 cm−1, 1030 cm−1 and 780 cm−1 correspond to the bending vibration peaks in plane and out of plane of the C-H bond. The infrared spectra of the CNNS/PMMA/pPy coating and the CNNS/PMMA/pPy-C coating combined the characteristic absorption peaks of the CNNS/PMMA coating and the pPy coating, indicating the successful preparation of a composite coating.
3.3. The Anti-Corrosive Performance of Synthesized Coatings
With the aim of exploring the general effects,
Figure 2 depicted the curves for an open circuit voltage versus time of bare 316SS and coated 316SS in the simulated PEMFC environment, respectively. In the process of soaking, corrosion occurs continuously, and the metal ions dissolved from the surface of stainless steel cover the surface of stainless steel to form a passive film, and the diffusion of metal cations was limited, which prevented the metal from further corrosion. Therefore, it was observed that the E
ocp of bare 316 stainless steel increased slowly, which indicated that there was a continuous corrosion process during long-term immersion in a corrosive environment. The E
ocp value of the CNNS/PMMA/pPy coatings and the CNNS/PMMA/pPy/C coatings decreased rapidly in the early stage, and then tended to be stable, because there were a large number of micropores on the coating surface, which made water molecules and corrosive ions quickly penetrate into the coating/metal matrix interface. After the open circuit potential was stable, the E
ocp value of coated stainless steel was much higher than that of 316 bare steel, which meant that the coatings had a better anti-corrosion effect. The distribution of micropores and microcracks on the surface of the coating would suppress the penetration and delay the entry path for the corrosion ions into the coating.
Potentiostatic polarization curves for bare 316SS and coated 316SS in the simulated PEMFC environment are provided in
Figure S5. The curves for composite coatings showed that the current density dropped sharply at the beginning. Meanwhile, the curves for bare 316SS and a single coating are apparently identical. During the measurement time, the current density hardly changed.
In order to further explore the protection of the 316SS substrate by various coatings in a corrosive solution, the samples were recorded by electrochemical impedance spectroscopy. At the same time, in order to compare these results with the results of the unprotected stainless steel substrate, the EIS measurement of bare 316SS was also given.
Figure 3 includes the Nyquist plots and Bode plots of bare 316SS, and the CNNS/PMMA, CNNS/PMMA/pPy and CNNS/PMMA/pPy/C coatings before and after soaking in a 0.1 M H2SO4 solution at 70 °C for 1 h.
Figure 3 shows the Nyquist plots and Bode plots of the sample in the simulated PEMFC working environment, and the experimental data were fitted by the equivalent circuit diagram. The derived fitting parameters are summarized in
Table S1. In the equivalent circuit diagram, Rs is the resistance of the solution, and CPE1 and Rcoat are related to the composite/electrolyte interface, where Rcoat represents the micropore resistance on the surface of the film material and CPE1 is the capacitance of the simulated coating material. CPE2 and Rct are related to the charge transfer reaction caused by electrolyte permeation. CPE2 is an electrical double-layer capacitance that simulates the bubble part of the interface, and Rct is attributed to the charge transfer resistance of the base metal corrosion reaction. The Rct in the fitting parameters is inversely proportional to the corrosion rate of the sample, indicating the corrosion rate. It can be seen from the fitting results that the fluctuation of Rs is small, indicating that the testing system is in a relatively stable state. Different from 316SS, the Nyquist plots of anti-corrosion coating consists of a capacitive arc with a large radius of curvature. Usually, the radius of capacitive arc reflects the size of charge transfer resistance during electrochemical corrosion, and the larger the radius of capacitive arc, the greater the charge transfer resistance and the better the corrosion resistance of the material. Analysis of the Bode plots showed that the coating has two time constants, one is the capacitor of the coating itself, and the other is the double-layer capacitor of the metal surface, indicating that the corrosion effect makes the coating change. pPy-0.90, pPy/C-0.80, and CNNS/PMMA/pPy/C-1.00 showed the largest |Z| values in the low-frequency region, with their maximum phase angles corresponding to the lowest frequency, where CNNS/PMMA/pPy/C-1.00 showed optimal corrosion resistance. In the frequency range from 1 to 100 Hz, a linear relationship was observed between the impedance and frequency, with a slope close to one.
Nyquist plots shows a small capacitance loop at high frequency, which indicates that the coating has relatively high conductivity at the beginning, so the surface of 316SS is in a passive state. Generally speaking, a high-frequency capacitive arc reflects the electrolyte/coating interface, while a low-frequency capacitive ring indicates the response of electrochemical process at the coating/316SS interface. According to Nyquist plots, the CNNS/PMMA/pPy/C-1.00 coating-synthesized constant voltage has the largest capacitance loop, which indicates that the coating has the largest resistance (Rct), the best mechanical isolation performance and great corrosion resistance. The increase tendency in the low-frequency region for samples mean that weak Warburg diffusion starts to appear, indicating that the metal has been corroded under the coating, the corrosion product film begins to affect the electrochemical reaction, and the coating has limited protection of the matrix. At the same time, for polypyrrole film layers without a CNNS/PMMA composite coating, pPy-0.90 and pPy/C-0.80 showed the largest capacity loop but not pPy-1.00 and pPy/C-1.00, and this may be related to the interaction between the CNNS/PMMA composite coating and the polypyrrole film layer. The Nyquist plots of 316SS and CNNS/PMMA-316 are similar, maybe indicating that the single CNNS/PMMA coating is insufficient to protect 316SS.
According to previous research, the anti-corrosion coating not only acts as a physical barrier to prevent the penetration of corrosive ions, but also provides anodic protection by the passive coating formed at the coating/metal interface [
18]. The research shows that the pPy coating can improve the corrosion potential of the metal matrix, reduce the corrosion rate and better protect the stainless steel matrix from corrosion. In addition, the pPy coating can homogenize the metal potential, which means that the whole metal has a uniform potential. When the pPy coating on the metal surface becomes imperfect, the traditional coating often forms a small area of anode at the broken part, while the other protected parts can be regarded as the cathode. In this way, so called corrosive pitting at the broken part will occur. Due to the uniform potential of the pPy coating surface, corrosive pitting can be transformed into uniform corrosion. Therefore, it is of great significance to enhance the compactness of the coating by adding new functional moieties.
In order to obtain the corrosion effects of bare 316SS, CNNS/PMMA-, CNNS/PMMA/pPy- and CNNS/PMMA/pPy/C-coated stainless steel in a 0.1 M H
2SO
4 + 2 ppm HF solution, potentiodynamic polarization tests were performed (
Figure 4). For bare 316SS, corrosive ions will erode the passivating coating on the surface of stainless steel. CNNS/PMMA was directly sprayed on the surface of 316 stainless steel, which would significantly slow down the corrosion process of the substrate to a certain extent. It was found that the coating obtained by spraying polypyrrole on 316SS in advance can be useful to improve stability. In
Table 1, E
corr increases first and then decreases, while I
corr decreases first and then increases. According to the contents, CNNS/PMMA/pPy/C-1.00 has the largest E
corr value (109 mv), the smallest I
corr value (2.14 μA·cm
−2), and the best corrosion resistance effect. Compared with bare 316SS, it was clear that the coating caused a positive shift of E
corr by more than 500 mV, and the I
corr value was decreased by more than an order of magnitude. The results verified that the CNNS/PMMA/pPy/C coating can effectively prevent corrosive substances from reaching the metal surface.
In
Figure 5a, the surface morphology of bare 316SS was approximately smooth and a few scratches formed during mechanical polishing. According to
Figure 5b, the distribution of the pPy/C coating was relatively uniform and dense. In essence, the whole structure was homogenous.
Figure 5c presented the rough structure formed after spraying, with micropores and several nanoparticles on the coating surface. The deposited layer induced a more densely packed microstructure and the presence of tiny pores supported the formation of solvent volatilization after spraying.
To further investigate the elemental distribution and composition, EDX mapping of coated 316SS was conducted and presented in
Figure S7. EDX mapping showed the homogeneous distribution of C, N, O and Fe elements.
The hydrophobicity of the coatings can be assessed macroscopically through the contact angle tests.
Figure 6 showed the size of the contact angle of different interfaces. It can be seen that the contact angle of the pPy/C coating increases slightly compared with bare 316SS. After the incorporation of the sprayed coating, the contact angle becomes significantly larger. At the same time, a single CNNS/PMMA coating directly sprayed on the surface of bare 316SS significantly increases the contact angle compared with bare 316SS. This suggests that the CNNS/PMMA coating significantly improves the hydrophobicity of the coating, and the anti-corrosion coating shows a good physical barrier effect. Due to the insulation and hydrophobicity of the CNNS, its steric effect can form a physical barrier for the penetration of corrosive ions by adding it to the coating. In this manner, its diffusion channel in the coating would become narrow, thus enhancing the capability of the organic coating as the resistance to electrochemical corrosion.
We have also explored the interfacial contact resistance (ICR) values (
Figure 7). We selected different samples synthesized at a potential of 1.00 V and bare 316SS.
Table S2 demonstrated that the ICR values were in the range of 22–115 mΩ·cm
2 upon exposure to a compaction pressure of 140 N/cm
2 (this value is a typical loading force requirement for commercial PEMFCs), which were substantially larger than the DOE standard. The variation of ICR depends entirely on the internal structure and composition of the coating itself. Under a pressing pressure of 140 N·cm
−2, the ICR of the pPy coating is 51 mΩ·cm
2; compared to a single pPy coating, the ICR of the pPy/C coating is approximately 22 mΩ·cm
2. Under the same pressure, the significant difference in ICR between the pPy and pPy/C coatings indicates that pPy/C coatings have better electrical conductivity than pPy coatings. This may be related to the excellent conductivity of graphite. The addition of CNNS/PMMA composite coatings significantly increases the ICR value due to the poor conductivity of the materials, which would ultimately gradually increase the electrical resistance.