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In-situ conversion of rGO from graphene oxide based on solar mediated enhanced characterization properties
Subramani shanmugam, Sivanandan nanjan Department of Electronics, PSG College of Arts and Science, Coimbatore- 641014, India [email protected], [email protected]
DOI 10.17586/2220-8054-2019-10-5-579-584
A globally acknowledged green synthesis of reduced graphene oxide (rGO) from graphene oxide (GO) is presented in this paper. The graphene oxide powder was synthesized from Graphite powder by a modification of Hummer's method. The GO is exposed to focused sunlight to obtain reduced graphene oxide (rGO). The reduction of GO under solar light is an eco-friendly method to conventional method of rGO preparation. The mechanism of the reduction of GO by sunlight imperative to exfoliation was seen to be well defined. The rGO powder was characterized by X-ray Diffraction (XRD), Field-Emission Scanning Electron Microscopy (FESEM), Raman spectroscopy, Fourier-Transform Infrared Spectroscopy (FTIR) and High-Resolution Transmission Electron Microscopy (HRTEM). This eco-friendly method of synthesizing of rGO paves way for an alternative method of rGO nanosheets preparation and it can be effectively used for fabrication of various electronic devices.
Keywords: reduced graphene oxide, crystal structure, reduction, exfoliation, raman.
Received: 4 July 2019
Revised: 5 September 2019
1. Introduction
Graphene Oxide (GO) is being single-layered carbon atom in a hexagonal lattice has a combination of both aromatic (sp2 hybridized C-C atoms) and aliphatic (sp3 hybridized -OH, C-O-H, C=O, -COOH) groups [1-3]. Thus, it exhibits a wide range of striking properties like optical transmittance, electrical conduction, energy storage, medical diagnosis and treatment, electronic applications, etc. The properties of GO and its reduced form plays a vital role in the multi-disciplinary functionality of these materials. They possess high surface area to volume ratio, high tensile strength, good thermal conduction, tremendous electrical conduction and superb optical properties [4]. The single layer GO and rGO can be synthesized by several methods, such as mechanical exfoliation, electrochemical reactions, thermal treatment and [5], photocatalytic method of preparing of GO and rGO. The solar energy assisted route of synthesis has an advantage of enhancement in its performance, especially when used for energy storage devices and super capacitors. Currently, a metallic oxide in combination with rGO and carbon nanotubes (CNTs), enhances the network performance of the devices. Oxides of tin, zinc, and cobalt are coated on graphene to obtain the desired quality of electrical devices [6-9]. Here, the purest form of solar energy was used to reduce the GO into rGO and this product was thoroughly characterized.
2. Experimental
2.1. Materials and methods
GO was synthesized from graphite powder using a modification of Hummer's method [10]. The reduced GO was prepared by using a convex lens of 100 mm diameter to focus solar radiation [11]. Briefly, 1 g of GO was taken in a glass Petri dish and kept under focused solar radiation at 12 Noon. GO powder was exposed to the focused solar radiation for approximately 10 - 15 minutes. GO was exfoliated into rGO sheets. The power of focused sunlight ranged from 1.8 - 2.5 W and the temperature was about ~ 300 °C [12]. GO was exfoliated into rGO sheets under this high temperature and power [13].
3. Result and discussion 3.1. XRD Analysis
The XRD pattern of synthesized GO/rGO shows diffraction with Cu Ka radiation (A = 1.54178 A) and depicted in Fig. 1 [14]. The GO/rGO exhibits a well-crystalline orthorhombic crystal structure (JCPDS card No. 89-8491).
The GO/rGO featured sharp diffraction peaks indicates that GO at 11.83, 42.78 corresponds to (001) and (100) peaks. The diffraction peaks of rGO at 10.30, 23.31 & 43.76 correspond to (001), (002) & (100) [15]. The diffraction
20(degree)
Fig. 1. X-ray diffraction pattern of GO and rGO nanosheets
plane of the hexagonal crystal structure has lattice constants of value, a = 2.47 and c = 6.79 A. The crystalline size (D) of the GO/rGO was calculated using Scherrer's formula:
0.89A
D = ~o-a (1)
p cos 0
where A is the wavelength of the X-ray radiation, 20 is the diffraction angle and p is the full width at half maximum (FWHM). Measured broadening of the GO/rGO with (001), (100) and 001),(002), (100) X-ray peaks offers average crystalline size about at 72.97, 14.03, and 19.59, 14.31, 21.23 nm for the GO/rGO, respectively [16].
3.2. FESEM/EDS
The morphology of GO/rGO nanosheets was observed using FESEM and shown in Fig. 2(a-b). The morphological feature clearly shows the formation of GO/rGO in 2D sheet-like pattern morphology in the prepared graphene materials similar to commercial materials. 2D wrinkled structure morphology of both GO and rGO sheets were observed to be fine micrometer in size. The rGO has a few broad and highly wrinkled layers with a regular shape and slanting size estimated in the range size of approximately 300 - 500 ^m exclusively [17,18].
The Energy Dispersive X-Ray Spectroscopy (EDS) analysis of the GO and rGO reveals that the atomic percentage of oxygen was considerably reduced in rGO than GO as expected. This is also confirmed by the increased ratio of C/O from 1.6684 to 2.0075.
3.3. HRTEM
Transmission electron microscopic (TEM) study was carried out to obtain the wide-ranging morphological information about the GO/rGO nanosheets and the respective HRTEM images were also showed in Fig. 3(a-d). The TEM image of GO/rGO confirms the nanosheets like morphology with their wrinkle shape with the face end (Fig. 3(a, b)). However, the TEM images of GO/rGO exhibits sheet-like shape with an average size of about 0.2 ^m. In order to obtain that lattice fringes form in the plane (100) indicated, the d-spacing values in three different places are shown in Fig. 3(b). Inset images shows good conformity with TEM images [19].
A clear morphology of rGO was observed, as evidence that is shown in Fig. 3(c). The sheets of rGO obtained by the chemical reduction process possess a few layer forms, such as crumpled sheet-like morphology and the structure were further confirmed by TEM, as shown in Fig. 3(c, d). The uniform and wrinkled sheet-like morphology, as well as the micropores on sheet surface of rGO samples (Fig. 3(c)) were clearly observed. Also, it displays highly interconnected ultrathin silk-like morphology and wrinkled shape [20]. Moreover, the wrinkle of the layers folded over each other was clearly visible, suggesting that these wrinkles were occurred by the crumpling of graphene-like sheets. The results also show that the highly crumbled morphology can effectively prevent the aggregation of the sheets as
Fig. 2. FESEM surface morphology of GO and rGO nanosheets
Fig. 3. HRTEM micrographs of GO and rGO nanosheets
shown in Fig. 3(d). The lattice fringes form was correlated with the reports in the plane about (002) as indicated in the d-spacing value. Inset image Fig. 3(d) clearly shows a well standard SAED pattern in two ring shape with a circle in the poly crystalline nature of the rGO [21]. The HRTEM result is in agreement with the XRD result in Fig. 2(d). These results conclude the morphology of the prepared GO/rGO [22].
3.4. Raman spectroscopy
The structure of GO/rGO was studied using Raman spectroscopy. The GO/rGO nanosheets exhibited a series of bands at 143,493,625,687, 847, 1172, 1369,1617, 1840, 1980,2234 and 2336 cm-1. All these bands were attributed to the fundamental vibration modes existing in graphene oxides. The reduction of GO and rGO sheets were further confirmed through Raman spectra as shown in Fig. 4. The Raman spectra of GO displays two characteristic Raman bands centered at 1369 and 1617 cm-1 were assigned to the well-known D and G bands, respectively [23].
rGO
-1-' i-*-1 '-1-•
500 1000 1 500 2000 2500
Raman Shift (cm 1)
FIG. 4. Raman spectra of GO and rGO nanosheets
The D band 1369 cm-1) corresponds to disorder in the sp2 carbon network, and the G band 1617 cm-1) is associated with the tangential vibrations of the sp2 carbon atoms in the hexagonal planes. In general, the D band is known as an imperfect band that typically arises from the first order diffusion of sp3 hybridized carbon atoms, while the G band is mainly reflects from the stretching vibration of sp2 hybridized C=C bonds. Results show that there is a shift occurring in Raman peaks positions for pure graphene oxide, which confirms the bond formation between graphene layers of rGO. The ID/IG ratio of the D-band to the G-band is related to the disorderliness of the sp2 domain, owing to the removal of the oxygen functional groups (Fig. 4) [24]. The ID/IG ratios for GO and rGO were found to be 0.750 and 1.030 respectively (Fig. 4).
3.5. FTIR spectrum
The major difference between the GO and rGO depicts the presence of specific functional groups like hydroxyl (-OH), carboxyl(C=O), epoxy (C-O-C) molecules attached to the main graphene layer [25]. These groups show the molecular vibrations of a specific characteristic frequency, when exposed to infrared radiation, as shown by the FTIR study in Fig 5.
The GO shows a sharp peak at 1040cm-1 (representing C-O-C), 1713 & 1607 cm-1 (corresponding to C=O) and a board peak around 3000 cm-1 (attributed to -OH groups) apart from oxygen base plane [26]. These have become less broadened with rGO samples due to the reduction in the concentration of vibrational groups.
3.6. PL Spectrum
The PL spectrum of GO nanosheets are depicted in Fig 6(a). The photoluminescence characterized by a broad peak between 600 - 900 nm was observed and the emission sharp peak was detected in GO at 750 nm. Fig. 6(b) shows PL spectra of rGO.
Three emission peaks was observed at 350, 435 and 524 nm, respectively, that are observed in rGO and it is attributed to the recombination of electron hole pairs in local state of sp2 carbon cluster embedded in sp3 matrix [27], in which are clearly known as GO is reduced to become rGO.
F r
Tí
l
h
<h)
1Í9Í. 1 I
<a>
v sJ
1713 If, 117 y
Í4IU J
111411
4000 ,i?nO .11100 2500 2000 15(1(1 1000 Wavt numb«(cm ')
Fig. 5. FTIR spectra of (a) GO and (b) rGO nanosheets
75 I (a) nm
600 650
700 750 800 850
Wavelength (nm)
(b)
435nm
\350nm ^V^^ 524nm
400 450
Wavelength (nm)
Fig. 6. PL spectrum of (a) GO and (b) rGO nanosheets
4. Conclusions
To summarize, we have successfully synthesized and characterized GO/rGO nanosheets. The crystalline structures of GO/rGO have been determined by XRD measurements. The morphological analysis shown by FESEM exhibits conspicuous wrinkled flakes. HRTEM images studies shows SAED patterns and nanosheets like structure in the plane with (002) orientation. The weight percentage of oxygen was reduced in rGO, as compared to GO which confirms the reduction and the formation of reduced graphene oxide. Raman spectra inferred that D/G value of GO 0.750 (< 1) and rGO 1.030(> 1) respectively, which confirms the formation of GO and rGO. Thus, the shallow peaks of rGO observed in FTIR reveals the partial removal of oxygen-linked functional groups from the hexagonal carbon-carbon plane of GO. The PL spectra of GO/rGO peak at 750 and 435 nm shows red and blue shift. Design of hetero-junction photodiode fabrication could be a thought for future amelioration and future scope of this research work. Due to its simplicity, this eco-friendly method of synthesizing rGO paves the way for making enormous rGO supported devices with good characteristics.
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