Van Hoang Luan,
Jin Suk Chung and
Seung Hyun Hur*
School of Chemical Engineering, University of Ulsan, Daehak-ro 93, Nam-gu, Ulsan 680-749, South Korea. E-mail: shhur@ulsan.ac.kr
First published on 23rd February 2015
A three-dimensional (3D) reduced graphene oxide hydrogel (rGOH) was prepared by hydrothermal synthesis based on the electrostatic force and chemical reaction between graphene oxide (GO) and Ni ions in a nickel acetate solution. The Ni–rGOH fabricated in this study exhibited a highly increased surface area compared to NiO nanoparticles owing to the formation of 3D networks. After the reduction of functional groups in Ni–GOH, Ni–rGOH showed highly enhanced capacitance (351 F g−1) at a charge/discharge current density of 0.625 A g−1 and 90% capacitance retention after 1000 cycles. The energy density of Ni–rGOH was 175.5 W h kg−1 at a power density of 1.125 kW kg−1, while maintaining a high-energy density of 118 W h kg−1 at a power density of 4.5 kW kg−1.
In general, carbon materials such as activated carbon, graphene, and carbon nanotubes can be used as active materials for the electrodes of ECs owing to their high electrical conductivity and surface properties.5,6 To achieve high capacitance, surface area, pore size distribution, and pore volume, they should be well designed and controlled to maximize the ion adsorption and minimize the resistance of ion transport. A recent study showed that a reduced graphene oxide hydrogel (rGOH), a 3D structured material with special properties such as being lightweight, and having high surface area and pore volume, can be effectively used as the electrode materials for power storage applications.7–9
Another strategy to enhance the capacitance of ECs is using transition metals that can increase the capacitance by the redox reaction with their oxidized forms. Nickel oxide (NiO) is one example of the transition metals with high redox capacity in aqueous electrolyte. Moreover, when it is hybridized with rGO, the capacitance can be highly increased owing to the high theoretical specific capacitance of NiO and excellent electrical conductivity of rGO.10,11
In this study, highly porous hybrid 3D structures composed of NiO and rGOH were fabricated by the crosslinking between Ni ions and functional groups of graphene oxides (GO) using a simple one-pot hydrothermal process followed by the high-temperature annealing. The chemical bonds between GO and Ni were formed during the hydrothermal process, and GO and Ni(OH)2 were transformed to rGO and NiO, respectively, during the high-temperature annealing. The supercapacitor fabricated by Ni–rGOH exhibited higher capacitance and better stability than that of Ni–GOH not annealed at high temperature, probably because of enhanced electrical conductivity and formation of stable NiO species.
(1) |
Fig. 1 (a) Schematic representation of Ni–GOH fabrication steps and (b) optical images of the Ni–GOHs. |
In our experiments, the formation of graphene oxide hydrogel includes 2 steps: (1) gelation by the interaction between Ni ions and GO sheets and (2) reaction at high temperature. The product of first step can be called “gel” and that of second step can be called “hydrogel”. When we varied the concentration of GO solution (0.5, 1, 2, 5 and 7.5 mg mL−1), the gelation of GO occurred in all concentrations, but hydrogel was not formed when the concentration of GO was below 5 mg mL−1. The minimum gelation concentration was 0.3% (w/v) in this study. As the chemical bonds were formed between GO and Ni ions by applying high temperature, the gel was irreversibly crosslinked.
The XRD patterns of Ni–GOH and Ni–rGOH are shown in Fig. 2. The diffraction peaks of Ni–GOH appeared at 11, 34, 36, 41, 59 and 64°, corresponding to the (003), (012), (015), (018), (110) and (113) planes of Ni(OH)2 (JCPDS file no. 14-0117), respectively,14 indicating that Ni(OH)2 crystals were also formed by the reaction between Ni2+ ions together with a small amount of OH− ions in the GO solution during the hydrothermal synthesis accompanied by the hydrogel formation by the following reactions.15
GO–COO− + H2O → OH− + GO–COOH | (2) |
Ni2+ + 2OH− → Ni(OH)2 | (3) |
The GO in the Ni–GOH sample was slowly reduced to rGO by the soaking in ammonium solution at room temperature. After the thermal annealing at 300 °C for 4 h, new peaks appeared at 37, 43 and 64°, corresponding to the (111), (200) and (220) planes, respectively, of NiO (JCPDS file no. 65-2901) in the Ni–rGOH sample.16 The Ni(OH)2 was decomposed into NiO by the following reaction:15
Ni(OH)2 → NiO + H2O | (4) |
As shown in Fig. S1,† the mass loss of Ni–GOH was more than that of Ni–rGOH, also indicating the dehydration of Ni(OH)2 during the thermal annealing.
The broad peak at ∼25° corresponds to the re-stacked GO sheets, exhibiting a larger layer-to-layer distance than that of graphite because of the presence of functional groups and captured water molecules.7
The morphology of Ni–rGOH was investigated by SEM, and the images are shown in Fig. 3a. Ni–rGOH exhibited a well-developed highly porous structure. Both the wrinkled rGO and smoothly surfaced NiO were observed, indicating that Ni ions contributed to the formation of Ni(OH)2 structures as well as 3D GOH networks during the hydrothermal process. The 2D Raman mapping and TEM images also confirmed the SEM results as shown in Fig. S2 and S3.† The energy dispersive X-ray spectra (EDS) shown in Fig. S4 and Table S1† indicate that a relatively small amount of Ni (∼3.9 atomic%) was present in Ni–rGOH.
The N2 adsorption–desorption isotherm of Ni–rGOH is shown in Fig. 3b. The BET surface area of Ni–rGOH was 132 m2 g−1, which is several times higher than that of pure NiO nanoparticles.17 The increased surface area was attributed to the formation of 3D structure with GO by the chemical crosslinking during the one-pot hydrothermal process. The shape of N2 adsorption–desorption isotherm indicates type H2, owing to the formation of a mesoporous structure connected or nonconnected ink-bottle pores or cavities in the hydrogel structure.7
The chemical structures of the samples fabricated in this study were determined by XPS as shown in Fig. 4a. Both the Ni–GOH and Ni–rGOH exhibited characteristic peaks of C 1s, O 1s, and Ni 2p in the survey spectra. The increased relative intensity of carbon compared to oxygen indicates the reduction of the functional groups of GO during the high-temperature annealing. High resolution C 1s peaks of Ni–GOH and Ni–rGOH were deconvoluted into C–C/CC, C–O, CO, and O–CO bonds at the binding energies of 284.65, 285.4, 286.4, and 288.9 eV, respectively, by a Gaussian function, as shown in Fig. 4b.18 The intensity of the C–O, CO and O–CO peaks of Ni–rGOH was lower than that of Ni–GOH because of the reduction of functional groups. Interestingly, the intensity of C–O peak of Ni–GOH was lower than that of GO because of the loss of functional groups during the reaction between GO and Ni ions, whereas the O–CO intensity of Ni–GOH was higher than that of GO (Fig. S5†), probably because of a transesterification reaction between the hydroxyl groups of GO and ester groups of nickel acetate as described in the following reaction (2):19
(5) |
Fig. 4 (a) XPS survey and high-resolution XPS spectra of (b) C 1s, (c) O 1s, and (d) Ni 2p peaks of Ni–GOH and Ni–rGOH. |
As shown in Fig. 4c, the high-resolution XPS peak of O 1s of Ni–GOH and Ni–rGOHs was deconvoluted into three sub-peaks centered at 529.9, 531.4, and 532.7 eV, corresponding to fully coordinated oxygen species to carbon or nickel atoms, oxygen atoms in the vicinity of an oxygen vacancy, and hydroxyl groups (C–OH), respectively.20 The peak position and intensity were maintained even after the high-temperature annealing, indicating that there was not a noticeable change in Ni–O bonds during the heat treatment. The high-resolution XPS peaks of Ni 2p of NiO and Ni(OH)2 shown in Fig. 4d show that NiO peak appeared at ∼854 eV, and there is a small shift in the satellite peak toward higher binding energy after the thermal annealing as reported in other study.21
The electrochemical properties of Ni–GOH and Ni–rGOH were determined by the CV and galvanostatic charge/discharge systems. The specific capacitance was calculated from both the CV and CD by eqn (6) and (7), respectively.22
(6) |
(7) |
As shown in Fig. 5, Ni–GOH and Ni–rGOH exhibits redox current peaks of Ni(OH)2 and NiO with electrolyte, respectively, corresponding to the Ni(OH)2/NiOOH (A1/A2) and NiO/NiOOH (B1/B2) redox couples according to eqn (8) and (9):15,23
Ni(OH)2 + OH− ↔ NiOOH + H2O + e− | (8) |
NiO + OH− ↔ NiOOH + e− | (9) |
The specific capacitances of Ni–GOH and Ni–rGOH were calculated based on the CV curves at various scan rates and CD curves at various current densities (Fig. S6†), as listed in the Tables 1 and 2. The Ni–rGOH exhibited 20–50% higher specific capacitance than that of Ni–GOH, probably because of the increased conductivity of GOH networks, and the transformation of Ni(OH)2 to NiO in the hydrogel structure after the thermal-annealing process.24 Interestingly, the capacitance of Ni–rGOH was much higher than that of high surface area GOH fabricated by ethylene diamine, attributed to the of redox current of NiO formed in the GOH network.7 The Nyquist plots of Ni–GOH and Ni–rGOH measured by the electrochemical impedance spectroscopy (EIS) are shown in Fig. 5c. At a high frequency, the smaller diameter of the semicircle of Ni–rGOH than that of Ni–GOH indicates the smaller charge transfer resistance of Ni–GOH electrode.25 At a low frequency, Ni–GOH and Ni–rGOH exhibited the similar slopes, indicating the similar ion diffusion/transport in the KOH electrolyte, robust 3D morphology, and pore structure maintained during the thermal annealing process.
Scan rates/mV s−1 | 10 | 50 | 100 |
---|---|---|---|
Ni–GOH/F g−1 | 272 | 203 | 168 |
Ni–rGOH/F g−1 | 323 | 258 | 250 |
Current density/A g−1 | 0.625 | 1.25 | 2.5 |
---|---|---|---|
Ni–GOH/F g−1 | 273 | 218 | 195 |
Ni–rGOH/F g−1 | 351 | 309 | 237 |
Two important parameters of the performance of asymmetric supercapacitor, the energy density (Es) and power density (Ps), were calculated by the following equations:11
(10) |
(11) |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra16598e |
This journal is © The Royal Society of Chemistry 2015 |