Chao Wang
Guobin Zhong- Electric Power Research Institute of Guangdong Power Grid Cooperation, Guangzhou, China
Graphene for energy storage devices suffers from the preparation method and deficient quality, hindering their further widespread application. Here, we report a facile and cost-effective approach to derive three-dimensional porous graphene (3DPG) from biocompatible chitosan for massive production. Taking advantage of the large surface area, excellent electrical conductivity and high electrochemical activity of the 3DPG, an advanced symmetric supercapacitor (3DPG//3DPG SCs) is achieved by coupling two 3DPG electrodes in commercial DLC301 organic electrolyte. The device delivers a remarkable capacitance of 168.9 F g-1 at the scan rate of 10 mV s-1 and displays a superior rate capability, witnessing 81.5% capacitance retention from 10 to 100 mV s-1. Furthermore, the 3DPG//3DPG SCs exhibits prominent cyclic durability, as evidenced by its 96% capacitance after 10,000 cycles. This work might shed light on the probable application of graphene at industrial level for efficient energy storage.
Introduction
Environmental pollution and the increasingly severe energy crisis are stimulating intensive efforts to exploit efficient energy storage devices for conversion fulfillment and storage of renewable energy sources (Wang et al., 2018; Han et al., 2019; Lu et al., 2019). In recent decades supercapacitors (SCs) have attracted particular attention, from both industry and academy, as an emerging candidate for energy storage (Hao et al., 2015; Zhang et al., 2017). This should be attributed to their advantageous features including high power density, fast charge/discharge capability, long-term cycling stability, good safety, and low maintenance cost (Yu et al., 2013; Yan et al., 2016; Chen et al., 2018). Regrettably, the dominating factor impeding the further widespread application of SCs is their low energy density, which can hardly meet the increasing energy density demands of novel electronic devices (Wang et al., 2017; Zhang Q. et al., 2018; Zhang Z. et al., 2018). The key to solving this problem lies in the rational selection of electrode materials, which determine the electrochemical performance of SCs. Among various electrode materials, carbon materials including carbon nanotubes (Sharma et al., 2015), carbon nanosphere (Cui and Zhu, 2014), active carbon (Kołodynska et al., 2016), and graphene (Wang et al., 2017; Yang et al., 2017) have been widely utilized for high-performance SCs constructions because of their impressive merits such as large surface area, prominent electrical conductivity, admirable long-term cycling stability, good mechanical properties, low production cost, and environmental friendliness (Gnanasekaran et al., 2017; Zhao et al., 2017; Guo et al., 2018). Among them, graphene has been considered as the most attractive candidate due to its high theoretical surface area (2,630 m2 g−1), impressive electrical conductivity and unique structure (Cao et al., 2011; Shen et al., 2017; Yu et al., 2017). However, the massive production of graphene with high electrochemical performance by facile and low-cost approaches is still challenging.
Nowadays, common methods for large-scale graphene production still see visible drawbacks. For instance, the chemical vapor deposition (CVD) method allows high-quality graphene synthesis but the experimental conditions are usually harsh (Shen et al., 2017). The mechanical exfoliation method enables graphene preparation with great electrochemical properties but the product thickness of different lots is uncontrollable (Chen et al., 2012). To circumvent these issues, extensive research efforts have been devoted to the exploration of facile and reliable synthetic methods. K. Parvez et al. reported a simple electrochemical expansion approach to synthesize thin-layer graphene based on inorganic salts, and a quasi-solid-state SC with a capacitance of 18.8 F g−1 was obtained (Shao et al., 2016). Ruoff and his co-workers designed a SC based on reduced graphene oxide by solvothermal reaction with a high capacitance of 120 F g−1 (Ruoff et al., 2012). Despite some delightful achievements, the overall performance of the cutting-edge graphene still hardly meets the demand for practical applications, especially at industry levels. Therefore, developing highly efficient approaches is very desirable for graphene preparation with excellent electrochemical properties.
Herein, we report a highly efficient approach allowing the massive production of three-dimensional porous graphene (denoted as 3DPG) as electrode materials for high-performance SCs constructions. The raw material for 3DPG derivation, the chitosan, is biocompatible, and environmentally friendly. The 3DPG electrode is facilely obtained via a three-step process, including the crosslinking of chitosan with acetic acid, the carbonization in the N2 atmosphere and the acid pickling. The porous structure and obvious graphene wrinkles of the 3DPG endow this electrode with a large surface area, which can afford a superior charge transport and adequate electrolyte diffusion into the electrode. Additionally, the nitrogen dopants in 3DPG effectively boost the reactivity and electrical conductivity by creating extrinsic defects, while the introduction of oxygen functional groups improves its electrochemical activity. As a consequence, coupling two 3DPG electrodes in commercial DLC301 organic electrolyte (denoted as 3DPG//3DPG SCs) yields an advanced symmetric SC with both a high capacitance (168.9 F g−1 at the scan rate of 10 mV s−1) and a superior rate capability (81.5% capacitance retention with the scan rate increase from 10 to 100 mV s−1). Besides, the device displays extraordinary cycling durability, retaining 96% capacitance after 10,000 cycles.
Experimental Section
Preparation of 3DPG Sample
All the reagents utilized were of analytical grade and used directly without further purification. The 3DPG was synthesized by three steps, crosslinking, carbonization and pickling. Firstly, 3 g chitosan, 0.01 mmol Ni(NO3)2 and 1 mmol Zn(NO3)2 were dissolved in 50 mL H2O under stirring at room temperature until the solution became turbid. 1.2 mL acetic acid was then added. After crosslinking till gel, the mixed precursor was transferred to a container (~64 mL) and dried in a freezer dryer for 36 h. The as-obtained precursor was soaked in a pure ethanol solution of 6 M KOH for 3 h and dried at 60°C for 3 h. The sample was calcined under a N2 atmosphere at 500°C for 1 h and then slowly heated to 800°C for 1 h. Lastly, the carbonized sample was soaked in 3 M HCl for 3 h at room temperature and completely rinsed with deionized water, in order to fully remove the metal ions and the residual KOH solution to obtain 3DPG (1.21 mg cm−1, BT25S, 0.01 mg).
Electrode Preparation and Device Assembly
3DPG electrodes were prepared by mixing the 3DPG powder with polyvinylidene fluoride (PVDF) binder and carbon black at a weight ratio of 8:1:1 in N, N-dimethylformamide until a homogeneous slurry was formed. Then the slurry was uniformly painted on carbon paper and dried at 80°C overnight. A symmetric SCs was assembled into a button battery by combining two 3DPG electrodes (1.0 ×1.0 cm) and a polypropylene separator in commercial DLC301 organic electrolyte (the details can be seen in Table S1 within the Supporting Information).
Material Characterizations and Electrochemical Measurements
The morphology and microstructures of the 3DPG were analyzed by field-emission scanning electron microscopy (FE-SEM; JSM-6330F) and transmission electron microscope (TEM; FEI Tecnai G2 F30). The chemical composition of the 3DPG was characterized by X-ray diffractometry (XRD; D8 ADVANCE), Raman spectroscopy (Renishaw in Via) and X-ray Photoelectron Spectroscopy (XPS, ESCALab250, Thermo VG). The Brunauer-Emmett-Teller (BET) surface area was measured with an ASAP2020M (Micromeritics Instrument Corp.). All the electrochemical studies of SCs in the potential range of 0–2.5 V were carried out using a button cell with a commercial DLC301 organic electrolyte. Cyclic voltammetry (CV) and galvanostatic charge/discharge measurements (GCD) were conducted on an electrochemical workstation (CHI 760E).
Results and Discussion
Structural and Morphological Properties of Sample
The 3DPG electrode is facilely obtained via a simple three-step process, including crosslinking of chitosan with acetic acid, carbonization in the N2 atmosphere, and acid pickling. Figure 1a presents an optical image of the freeze-dried chitosan after crosslinking with acetic acid, which swells into a sponge shape due to the formation of numerous porous channels during the crosslinking process. More significantly, in order to activate the graphene, the Ni(NO3)2 and Zn(NO3)2 were involved in a synthesis process and removed by sublimating at high temperature as well as soaking in 3 M HCl for 3 h at last, which can form a porous graphene structure with high surface area. The morphology and microstructure of the 3DPG sample was characterized by SEM and TEM. As shown in Figure 1b, the 3DPG sample exhibits notable graphene wrinkles with thickness <1 nm, implying the large specific surface area of the 3DPG sample. The TEM and the high-resolution transmission electron microscopy (HRTEM) images in Figures 1c,d reveal the ultrathin wrinkles and multilayered structure of the 3DPG sample, in accordance with the SEM analysis.
Figure 1. (a) Optical image of freeze-dried chitosan after crosslinking, (b) SEM image of the 3DPG, (c) TEM image, and (d) HRTEM image of 3DPG.
The structure and crystallinity of the 3DPG sample were analyzed by conducting X-ray diffraction (XRD) measurements. As illustrated in Figure 2A, all of the diffraction peaks of the 3DPG sample can be perfectly indexed to hexagonal graphite (JCPDF #41-1487), which is consistent with the commercial graphene (Xiao et al., 2018). No other impurity peaks were detected, indicating that the samples are pure graphene. To evaluate the specific surface area of the 3DPG sample, nitrogen adsorption-desorption measurement was carried out in Figure 2B. More encouragingly, the Brunauer-Emmett-Teller (BET) specific surface area of the 3DPG sample reaches up to 330.0 m2 g−1, which exceeds that of most graphene (Yang et al., 2011, 2014, 2015). Additionally, to gain insight into the chemical composition and valence state of the 3DPG, the sample was investigated by Raman spectroscopy and X-ray photoelectron spectroscopy (XPS). The Raman spectrum in Figure 2C reveals that the two strong peaks at 1352.6 and 1585.2 cm−1 correspond to the sp3-type disordered carbon (D band) and sp2-type ordered graphitic carbon (G band) (Teng et al., 2018). The large ID/IG ratio of ~0.94 and the 2D band observed at 2863.5 cm−1 imply the high defect densities as well as the few-layer nature of the 3DPG sample, which are in good agreement with the SEM and HRTEM analyses (Zhou et al., 2018). The XPS spectrum of the obtained sample is revealed in Figure S1 (Supporting Information), which shows C, O, and N elements corresponding to atomic contents of 82.63, 9.38, and 7.99%, respectively in the 3DPG sample. To further investigate the chemical state of C in the 3DPG sample, we analyze the C 1s spectra in Figure 2D. The C 1s spectrum can be deconvoluted into three peaks ascribed to the sp2 carbon atoms (C-C, 284.8 eV), hydroxy/epoxy groups (C-O, 286.0 eV), and carboxyl group (-COOH, 288.3 eV). The O 1s spectrum of 3DPG in Figure 2E can be deconvoluted into two apparent peaks assigned to C-O (398.6 eV) and -COOH groups (400.2 eV) (Zhu et al., 2015). The oxygen functional groups might endow the 3DPG with high electrochemical activity. The N 1s spectrum of 3DPG in Figure 2F displays two types of binding configurations, including pyridinic-N (511.2 eV) and graphitic-N (532.9 eV). The presence of N 1s and O 1s spectra indicates the successful introduction of N and O in the 3DPG sample, which is capable of boosting electrical conductivity and electrochemical activity (Zhang et al., 2016; Nandan and Nanda, 2017; Xiao et al., 2018).
Figure 2. (A) XRD patterns of 3DPG and commercial graphene, (B) Nitrogen adsorption isotherm at 77 K, (C) Raman spectra and (D) C 1s, (E) N 1s, (F) O 1s XPS spectrums of 3DPG.
Electrochemical Characterization of SCs
The electrochemical performance of the symmetric SCs based on 3DPG electrodes was measured at a voltage of 2.5 V in a button cell with a commercial DLC301 organic electrolyte. The cyclic voltammetry (CV) curves of 3DPG//3DPG SCs presents nearly symmetric rectangular shapes at the scan rates ranging from 10 to 100 mV s−1, suggesting the good capacitive performance of the device (Figure 3A). The GCD profiles of 3DPG//3DPG SCs at the different current densities of 0.25–3 mA cm−2 were collected in Figure 3B. It can be clearly seen that the shape of the profiles is somewhat deviated from the linear slope of an ideal supercapacitor, again demonstrating its excellent Coulombic efficiency and capacitive performance. More interestingly, the 3DPG//3DPG SCs delivers a maximum capacitance of 168.9 F g−1 at the scan rate of 10 mV s−1 and an outstanding rate capability with 81.5% retention of its initial capacitance with the current density increase to 100 mV s−1 (Figure 3C). Furthermore, the cycling performance of the symmetric SC device was investigated continually by CV measurement at a current density of 50 mV s−1 in Figure 3D. Significantly, this 3DPG//3DPG SC exhibits excellent cyclic durability with nearly 96% capacitance retention after 10,000 cycles. Based on the discussion above, such admirable electrochemical performance of the 3DPG//3DPG SC can be ascribed to the following reasons: (1) the N-doping greatly improves the reactivity and electrical conductivity via the generation of extrinsic defects, endowing the electrode with a superior electrochemical performance, (2) the introduction of oxygen functional groups boosts its high electrochemical activity, and (3) Its specific porous structure and notable graphene wrinkles can provide massive electrochemically active sites (Zhu et al., 2016; Zhang et al., 2016; Antink et al., 2017; Chen et al., 2017).
Figure 3. (A) CV curves at different scan rates, (B) GCD curves at different current densities, (C) The rate performance, and (D) Cycling stability at 50 mA s−1 of 3DPG//3DPG SCs.
The Ragone plot in Figure 4 compares the energy and power densities of the symmetric 3DPG//3DPG SCs with some other recently reported energy storage devices. Impressively, our device delivers a maximum energy density of 401.2 Wh kg−1 at a power density of 0.25 kW kg−1. Even at a high-power density of 5.2 W kg−1, it still achieves an exceptionally high energy density of 153.2 Wh kg−1. Notably, the energy-power characteristic of our 3DPG//3DPG SC is superior to that of recently reported energy storage devices, such as γ-MnO2//Zn battery (156.1 Wh kg−1, 0.05 kW kg−1) (Cheng et al., 2005), Ni//Fe battery (100 Wh kg−1, 0.3 kW kg−1) (Liu et al., 2014), Zn-array@graphene foam (115 Wh kg−1, 5.1 kW kg−1) (Chao et al., 2018), LiMn2O4//MoO3@ppy battery (60 Wh kg−1, 0.25 kW kg−1) (Tang et al., 2012), Deposited-Zn@graphite paper (65.1 Wh kg−1, 3.34 kW kg−1) (Fan et al., 2018), CoO@ppy//AC (11.8 Wh kg−1, 5.5 kW kg−1) (Zhou et al., 2013).
Figure 4. Ragone plots of the 3DPG//3DPG SCs and other recently reported energy storage devices for comparison.
Conclusions
In conclusion, a facile and cost-effective approach was demonstrated to implement the large scale production of three-dimensional porous graphene derived from chitosan. The formation of a porous structure after the crosslinking process and the notable graphene wrinkles provide abundant electrochemically active sites for charge storage. Simultaneously, the introduction of oxygen functional groups and N dopants further strengthen the electrochemical activity and the electrical conductivity of the 3DPG electrode. Accordingly, an advanced symmetric SC is rationally constructed by assembling two 3DPG electrodes in commercial DLC301 organic electrolyte. The device shows an excellent capacitance of 168.9 F g−1 at the scan rate of 10 mV s−1 and a superior rate capability with 81.5% capacitance retention, accompanied by superior cyclic durability with 96% capacitance retention after 10,000 cycles. In consequence, such an efficient approach is of great significance in promoting the widespread application of graphene for energy storage.
Author Contributions
CW and GZ conducted the experiments. WS and WZ contributed to scientific discussions and research suggestions. KX helped with writing. CW, SW, ZW, and KX performed the characterization and data analysis. All authors involved the analysis of experimental data and manuscript preparation.
Funding
This work was financially supported by the National Key Research and Development Program of China (Grant No. 2016YFB0901600).
Conflict of Interest
All the authors are now employed by the company Electric Power Research Institute of Guangdong Power Grid Co., Ltd. The authors declare that this study received funding from the National Key Research and Development Program of China (Grant No. 2016YFB0901600). The funder was not involved in the study design, collection, analysis, interpretation of data, the writing of this article or the decision to submit it for publication.
Supplementary Material
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fenrg.2020.00061/full#supplementary-material
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Keywords: three-Dimensional (3D), porous, graphene, chitosan, supercapacitor
Citation: Wang C, Zhong G, Zhao W, Wu S, Su W, Wei Z and Xu K (2020) Chitosan-Derived Three-Dimensional Porous Graphene for Advanced Supercapacitors. Front. Energy Res. 8:61. doi: 10.3389/fenrg.2020.00061
Received: 28 February 2020; Accepted: 31 March 2020;
Published: 30 April 2020.
Edited by:
Teng Zhai, Nanjing University of Science and Technology, ChinaCopyright © 2020 Wang, Zhong, Zhao, Wu, Su, Wei and Xu. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Chao Wang, wangchaomly@163.com; Wei Su, jxhwsu@163.com