Graphene is a single layer of carbon atoms lined up in a hexagonal lattice, and graphite is composed of these multiple layers.
Graphene is a single layer of carbon atoms lined up in a hexagonal lattice, and graphite is composed of these multiple layers. Until the 2000s, graphene was difficult to obtain, and research in this area was slow for many years. However, in 2004, Andre Geim and Konstantin Novoselov succeeded in obtaining graphene by attaching a piece of graphite to cellophane tape (Scotch tape) and peeling it off, and since then, graphene has attracted attention as a new electronic functional material due to its unique electrical properties [1]. Graphene can be obtained not only by direct exfoliation from graphite by tape (as described above) but also by the chemical vapor deposition (CVD) method. However, the former is inefficient and the latter requires large equipment, so both are not suitable for industrial use. On the other hand, the synthesis of graphene via graphene oxide, which is obtained from the oxidation of graphite, has recently attracted much interest due to its suitability for mass-scale synthesis (Figure 1). In this method, graphite oxide is first synthesized by chemical oxidation of graphite. Graphite oxide has many hydrophilic oxygen functional groups inserted between the graphite layers, which weakens the interaction between the layers, and can be easily exfoliated into a monolayer by sonication in water to produce graphene oxide (GO), which is uniformly dispersed in water. Finally, the GO can be reduced to obtain a material with electrical properties similar to graphene. Strictly speaking, however, it is difficult to obtain perfect graphene from this method, so the material obtained from this method is often called “reduced graphene oxide” (rGO).
There are three main methods of GO reduction: (1) chemical reduction, (2) electrochemical reduction, and (3) thermal reduction. Among them, chemical reduction is the most frequently used method to synthesize rGO by the chemical reduction of oxygen functional groups such as epoxy groups in GO using a reducing agent such as hydrazine [2]. However, due to the high toxicity of hydrazine, reduction using hydrazine is not a preferred method from an industrial viewpoint. Recently, reduction using hydrogen iodide has also been attempted [3], but this method is also industrially undesirable because hydrogen iodide is highly corrosive. In addition, a unique reduction method using food-derived substances such as vitamin C [4], glucose [5], and xylitol [6] has been reported, but their reaction efficiency is not very high. More recently, reduction methods of GO using Joule heat and microwaves have also been reported [7].
In contrast, electrochemical reduction is a method of reducing oxygen groups by electrode reaction and is therefore more environmentally friendly than chemical reduction methods in that it does not use toxic reagents. Another feature is that the electronic state of the resulting graphene can be easily manipulated by controlling the reduction level through electrolysis conditions. The thermal reduction method is not exactly a reduction reaction but rather a simple thermal decomposition which removes the oxygen functional groups (hydroxyl, epoxy, carboxyl groups, etc.) in GO. This method can synthesize rGO on a mass scale as long as there is an electric furnace that can provide heat in an inert atmosphere, making it suitable for industrial-scale production processes in addition to being environmentally friendly.
The electrochemical reduction of GO is generally carried out in aqueous electrolyte solutions, but since GO is water dispersible, it is necessary to immobilize GO on the electrode by prior chemical treatment [14]. We carried out the electrochemical reduction of GO in organic solvents, taking advantage of the fact that GO does not detach from the electrode in organic solvents as compared to aqueous systems [15]. For the electrochemical reduction of GO, platinum and indium–tin oxide (ITO) could be used as working electrodes, but the reduction reaction proceeded more effectively when fluorine-doped tin oxide (FTO), which can be applied in a wide potential window, was used. Figure 2 shows the linear sweep voltammetry (LSV) of the system using propylene carbonate (PC) as the organic solvent, tetraethylammonium tetrafluoroborate (Et4NBF4) as the supporting electrolyte, and FTO coated with a drop-cast film of GO as the working electrode. For comparison, the LSV data using only FTO without GO coating (bare FTO) as the working electrode are also shown. The reduction current flowed from around −0.5 V vs. Fc/Fc+, indicating that electrochemical reduction of GO is possible. When the applied potential became more negative than −1.0 V at LSV, the color of the film changed from brown to black, suggesting that GO was changing to rGO (Figure 3). Electrochemically reduced GO is henceforth referred to as “erGO”.
Fourier Transform Infrared (FT-IR) and X-ray photoelectron spectroscopy (XPS) were measured to identify the chemical structure of erGO (Figure 4). Although no significant absorption bands were observed in the raw graphite, absorption bands originating from C=O stretching vibration of the carbonyl group, angular vibration of the carboxyl group, and C–OH stretching vibration of the hydroxyl group were observed in GO powder at 1740, 1370, and 1220 cm−1, respectively. However, after the electrochemical reduction of GO, the characteristic absorption bands were no longer observed in the spectrum of the films as in graphite, suggesting that most of the oxygen-containing groups were removed by the electrochemical reduction. In addition, the C1s spectra in XPS showed that the signal derived from oxidized species in GO almost completely disappeared by electrochemical reduction. In order to investigate the electrical properties of erGO, the electrical conductivity of erGO films was measured by the four-probe method and found to be about 3 S cm−1, which is comparable to that of rGO obtained by chemical reduction with hydrazine.
In addition to its high electrical conductivity, graphene has a large specific surface area of 2600 m2 g−1, which makes it promising as an electrode material for electric double-layer capacitors (EDLCs). EDLC is one of the electronic components used in a wide range of industries as a backup power source for integrated circuit (IC) and large-scale integration (LSI) memories and actuators. The sweep rate dependence of the specific capacity of EDLC prepared using erGO obtained by electrochemical reduction in propylene carbonate (PC) is shown in Figure 5. Although the rate of decrease in specific capacitance was about 20% compared to that at 10 mV s−1, it was found that the specific capacitance was maintained to some extent.
Figure 5. Specific capacitances of erGO/FTO in Et4NBF4 (0.5 M) in propylene carbonate plotted against the scan rate.
This entry is adapted from the peer-reviewed paper 10.3390/coatings11030297