Abstract
Graphene, a two-dimensional carbon material, possesses exceptional properties such as high electron mobility, exceptional strength that surpasses that of steel, chemical resistance, environmental friendliness, and a large specific surface area. In this study, we used the modified Hummer process to produce graphene oxide, which was applied to an aluminum alloy substrate as a corrosion-resistant coating. The aluminum alloy used in our study is AA2024, which is widely applied in industry and aircraft. The coating layer was characterized by micro-Raman spectroscopy and atomic force microscopy (AFM) before and after the reduction process. Micro-Raman spectroscopy provided information on the degree of reduction and the presence of functional groups in the coating layer. AFM images enabled the study of surface morphology and topography. After the reduction process, achieved by annealing in an argon atmosphere at 140 °C, micro-Raman spectroscopy and AFM were again used to assess structural and morphological changes. The reduction resulted in the formation of reduced graphene oxide (RGO), which exhibited improved conductivity and stability. The combination of micro-Raman spectroscopy and AFM characterization techniques provided detailed information on the properties and effectiveness of the coating layer. This research contributes to developing anti-corrosion methods using advanced materials and surface engineering techniques.
1. Introduction
Aluminum alloys, such as AA2024, are widely used in aerospace and industrial applications due to their excellent strength-to-weight ratio and mechanical properties. However, their susceptibility to corrosion [1,2,3] in aggressive environments poses significant challenges, necessitating the development of effective anti-corrosion coatings. Graphene-based materials, particularly graphene oxide (GO) and reduced graphene oxide (RGO), have garnered considerable attention as it has myriad applications [4,5,6,7,8,9,10,11,12,13,14,15,16,17,18] as potential corrosion-resistant coatings due to their unique properties, including high mechanical strength, chemical stability, and barrier capabilities. Incorporating these materials into protective coatings offers a promising approach to enhancing the corrosion resistance of aluminum alloys.
The atomic force microscope (AFM) is a versatile tool widely used in electrochemistry, capable of investigating the electrode–electrolyte interface in various solutions and monitoring changes in surface topography during electrochemical measurements without disrupting the process [3,19,20,21,22,23,24,25,26,27]. Alongside AFM, the scanning tunneling microscope (STM) has been extensively employed because of its ability to resolve surface morphology under different electrochemical conditions. Electrochemical impedance spectroscopy (EIS) complements these techniques as a powerful [28], non-destructive method for studying corrosion and protection mechanisms, enabling the real-time monitoring of corrosion inhibitors, coatings, and other protective strategies to improve corrosion prevention. Micro-Raman spectroscopy, which combines Raman spectroscopy with the spatial precision of microscopy, provides detailed insights into the chemical composition [29,30,31], structure, and stress states of materials at the micro-scale, making it invaluable for applications in materials science, electrochemistry, and other fields.
In this study, GO and RGO coatings were applied to AA2024 aluminum alloy surfaces to evaluate their potential as anti-corrosion coatings. The reduction of GO to RGO was achieved via thermal annealing in an argon atmosphere, enhancing the conductivity and reducing the oxygen functional groups, thereby improving the coating’s performance. A combination of advanced characterization techniques was employed to comprehensively assess the structural, morphological, and electrochemical properties of the coatings. By combining AFM, micro-Raman spectroscopy, and EIS, this work provides a thorough evaluation of GO and RGO as anti-corrosion coatings for AA2024 alloy. The findings contribute to the growing body of research on graphene-based materials and their potential to enhance the performance and longevity of aluminum alloys in corrosive environments.
2. Materials and Methods
2.1. Materials
Aluminum alloy AA2024-T3 sheets (4 mm thickness) were obtained from Goodfellow (UK). Sodium chloride (NaCl) was purchased from Sigma-Aldrich(Taufkirchen, Germany). Platinum foil (0.5 mm thickness, 99.99% purity) was also acquired from Sigma-Aldrich (Taufkirchen, Germany). Milli-Q water was produced using a Millipore water purifier.
2.2. Sample Preparation
AA2024-T3 sheets with a thickness of 4 mm were cut into 7 mm diameter disks and then prepared and polished according to the procedure outlined in the reference [32]. Briefly, for bare samples were polished with decreasing diamond paste (9–0.25 μm), kept in a dry box, and ultrasonically cleaned in hexane, acetone, and methanol (15 min) before the experiment. The graphene oxide solution was prepared by sonicating graphene oxide (a yellowish-brown paste) in Milli-Q water (18.2 MΩ) for 30 min. The graphene oxide paste was synthesized using a modified Hummer method. The final graphene oxide solution concentration was 1 mg/mL. Then, 20 μL drops of this solution were evenly distributed onto the cleaned–polished AA2024-T3 samples (as described above), followed by air-drying under ambient conditions. Reduced graphene oxide samples were obtained by annealing the graphene oxide-coated samples in an argon atmosphere at 140 °C for one hour.
2.3. AFM Measurements
Surface characterization was performed using an Agilent 5500 Atomic Force Microscope (AFM) working in tapping mode under ambient conditions. A gold-coated MikroMasch tip (MIKROMASCH, Sofia, Bulgaria) with a force constant of 5 N/m and a length of 125 μm was employed to scan both GO and RGO-coated aluminum samples. The AFM scanned a 10 × 10 μm2 area at a frequency of 1 Hz. Subsequently, the AFM images were analyzed to extract surface statistical parameters, including roughness, and skewness following the established procedures.
2.4. Micro-Raman Setup
Micro-Raman measurements were performed using a WITec alpha 300 spectrometer (WITec, Ulm, Germany) with a 532 nm laser excitation line. G-band mapping was performed across a 150 × 150 μm2 area on the samples both before and after annealing.
2.5. Electrochemical Experiments Setup
The electrochemical cell, as described in the reference [20], was thoroughly cleaned using sequential 15 min ultrasonic baths in acetone, isopropanol, and Milli-Q water. Prior to attaching the coated aluminum electrode to the cell, a platinum wire counter electrode was positioned circularly within the cell’s inner frame. A standard Ag/AgCl/NaCl (3M) reference electrode from BASi (West Lafayette, IN, USA) was employed.
After proper electrode placement within the cell, they were connected to a Bio-Logic SP-200 potentiostat (Bio-Logic SAS, Claix, France) for electrochemical measurements. To start the measurements, samples were immersed in 0.5 M NaCl solution for 30 min at open circuit potential (OCP). Subsequently, electrochemical impedance spectroscopy (EIS) was performed at the OCP using a sinusoidal potential signal with an amplitude of 5 mV. The frequency range for the EIS measurements was logarithmically spaced from 7 MHz to 0.1 Hz.
Potentiodynamic polarization curves were obtained utilizing the same experimental configuration of EIS measurements for the bare, GO-coated, and RGO-coated samples. Prior to the scan, the samples were equilibrated at OCP for 1 h. The potential was then swept from cathodic to anodic at a rate of 0.5 mV/s, and the Tafel plot was subsequently derived.
3. Results and Discussion
3.1. Topography Characteristics
The surface topography of the AA2024-T3-coated samples was meticulously examined using atomic force microscopy (AFM) both before and after the annealing process. Surface characteristics significantly influence the performance of a coating system. For instance, surface roughness affects adhesion, with rougher surfaces potentially offering better mechanical interlocking but also increasing the risk of stress concentrations and delamination. Furthermore, surface imperfections can function as nucleation sites for corrosion, while smoother surfaces generally exhibit improved corrosion resistance. In electrically conductive coatings, surface roughness can affect current distribution, potentially leading to localized corrosion. Finally, surface topography is crucial in tribological behavior, with rougher surfaces typically showing higher friction and wear.
The surface statistics of five replicates summarized in Table 1 reveal a reduction in height range from 129 nm to 94 nm following the reduction process, as evident in the topography images shown in Figure 1. The surface topography of GO (Figure 1A,B) displays the characteristic wrinkles of graphene oxide flakes, which become less pronounced after reduction (Figure 1C,D). This change is further reflected in the decreased root mean square (RMS) roughness and skewness values, as detailed in Table 1.
Table 1.
Surface statistics of GO and RGO.
Figure 1.
The 3D and 2D AFM images of GO and RGO coating of AA2024: (A) 3D topography of GO; (B) 2D topography of GO; (C) 3D topography of RGO; (D) 2D topography of RGO.
3.2. Micro-Raman Measurements
Micro-Raman spectroscopy was utilized to evaluate the uniformity of the coating across the entire sample. The samples were scanned to confirm complete coverage with the GO layer, and the G-band, centered around 1600 cm−1, was mapped, as shown in Figure 2A, showing that the GO effectively covers the surface. To verify that the reduction process did not cause any damage to the coating, the sample was rescanned post-reduction, and the G-band was mapped at 1596 cm−1. As illustrated in Figure 2B, the surface remains uniformly covered and undamaged.
Figure 2.
G-band micro-Raman mapping of (A) GO; (B) RGO coatings of AA2024. The black color in the images identifies spots of low intensity, the white is for the maximum intensity; the shades of blue are for the intensity between the maximum and minimum.
3.3. Electrochemical Measurements
The Nyquist plot shown above illustrates the impedance behavior of aluminum samples coated with GO (graphene oxide) and RGO (reduced graphene oxide) coatings. For the GO-coated sample (red circles), the curve demonstrates a higher overall impedance compared to the RGO-coated sample (black squares). This indicates that the GO coating provides greater resistance to charge transfer, which can be attributed to its insulation nature and the presence of oxygen-containing functional groups. In contrast, the RGO-coated sample shows a lower impedance due to its reduced oxygen content and enhanced electrical conductivity, making it more effective for facilitating charge transfer.
EIS data, fitted using an equivalent circuit model shown in Figure 3. As shown in Table 2, the fitting parametersreveal distinct differences between RGO (reduced graphene oxide) and GO (graphene oxide). R1, representing the solution resistance, is higher for RGO (92.6 Ohm) than GO (53.43 Ohm), suggesting a potentially lower ionic conductivity in the RGO system. Q1 and a1, parameters related to the constant phase element (CPE) representing the double-layer capacitance, show similar values for both materials, indicating comparable capacitive behavior. However, the significantly higher R2 value for GO (2215 Ohm) compared to RGO (1326 Ohm) points towards a greater charge transfer resistance, potentially due to a less conductive or more resistive interface. The Q3 and a3 values, also associated with a CPE, reveal a notable difference in the exponent a3, with GO exhibiting a value close to 1, indicating ideal capacitive behavior, while RGO’s a3 is significantly lower (0.2063), suggesting a more diffusive or non-ideal capacitive process. Finally, R3, representing a resistance associated with diffusion or other processes, is substantially higher for GO (64.7 Ohm) than for RGO (11.55 Ohm). Overall, the data implies that while RGO exhibits lower charge transfer and diffusion-related resistances, it shows more non-ideal capacitive behavior compared to GO.
Figure 3.
EIS Nyquist plot of GO and RGO coatings of AA2024 in 0.5 M NaCl and their fitting to the circuit shown.
Table 2.
EIS fitting parameters of GO and RGO.
Tafel plot (Figure 4) illustrates the corrosion behavior of AA2024 aluminum alloy with and without graphene oxide (GO) and reduced graphene oxide (RGO) coatings. The plot compares the bare AA2024, GO-coated, and RGO-coated samples by showing the relationship between the applied potential (V vs. Ag/AgCl) and the logarithm of the current. The data reveal that both the GO and RGO coatings shift the corrosion potential towards more positive values and significantly reduce the corrosion current density compared to the bare AA2024. This indicates that both GO and RGO offer enhanced corrosion protection. The RGO coating appears to provide the most substantial improvement, exhibiting the lowest corrosion current density and the most positive corrosion potential, suggesting it forms a more effective barrier against corrosive electrolytes. This improved performance of RGO over GO is likely due to its higher electrical conductivity and better barrier properties, resulting from the restoration of the graphene’s conjugated structure after reduction. These findings highlight the potential of GO and particularly RGO as effective anticorrosive coatings for AA2024.
Figure 4.
Tafel plot of bare, GO- and RGO-coated AA2024 in 0.5 M NaCl.
Although EIS reveals a lower charge transfer resistance for RGO compared to GO, the former’s substantially higher CPE value implies a more effective barrier layer and/or increased surface homogeneity. This enhanced capacitive effect likely explains the reduced corrosion current and superior protection observed in the potentiodynamic polarization tests.
4. Conclusions
The aluminum alloy used in this study is AA2024, a material widely used in the aerospace and industrial sectors. The coating layer was characterized both before and after the reduction process using micro-Raman spectroscopy and atomic force microscopy (AFM). Micro-Raman spectroscopy provided information on the degree of reduction and the presence of functional groups in the coating, while AFM offered detailed insights into surface morphology and topography. The reduction process was carried out by annealing in an argon atmosphere at 140 °C, resulting in the formation of reduced graphene oxide (RGO). Post-reduction, micro-Raman spectroscopy, and AFM were employed again to assess structural and morphological changes. The RGO coating showed improved conductivity and stability, making it a promising candidate for applications where surface conductivity is critical.
Author Contributions
Conceptualization, A.K.; methodology, A.K.; formal analysis, A.K.; investigation, A.K.; writing—original draft preparation, A.K.; writing—review and editing, A.K., I.J., M.B., A.K.S., M.G. and I.M. All authors have read and agreed to the published version of the manuscript.
Funding
This work was partially sponsored by the Slovenian Research Agency (Research Programs P1-0034 and J1-4401).
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
Data are contained within the article.
Conflicts of Interest
The authors declare no conflicts of interest.
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