Aoping Guo,
Xiaobao Zhang,
Baiyi Shao,
Song Sang and
Xiaojing Yang*
Beijing Key Laboratory of Energy Conversion and Storage Materials, College of Chemistry, Beijing Normal University, No. 19, Xinjiekouwai Street, Haidian District, Beijing 100875, China. E-mail: yang.xiaojing@bnu.edu.cn
First published on 10th March 2022
We report an environmentally friendly strategy for the synthesis of Fe3C/Fe/graphitic carbon based on hydrothermal carbonization and graphitization of carbon spheres with potassium ferrate (K2FeO4) at 800 °C. The obtained sample consisting of Fe3C/Fe nanoparticles and graphitic carbon (FC-1-8) delivered an enhanced pseudocapacitance of 428.0 F g−1 at a current density of 1 A g−1. After removal of the Fe3C/Fe electroactive materials, the graphitic carbon (FC-1-8-HCl) possessed a large specific surface area (SSA) up to 2813.6 m2 g−1 with a capacity of 243.3 F g−1 at 1 A g−1, far outweighing the other amorphous carbon electrodes of FC-0-8 (carbon spheres annealed at 800 °C without the treatment of K2FeO4). The graphitic material with a porous structure could offer more electroactive sites and improved conductivity of the sample. This method provided guidelines for the synthesis of superior performance supercapacitors with synchronous graphitic carbon and electroactive species.
Carbon-based materials, such as activated carbon and graphene, have been regarded as the most common electrode materials. The hydrothermal carbonization technique is a green and soft chemistry method to synthesize carbon-based materials under mild temperature and self-generated pressure.3 The whole process involved a series of reactions, such as hydrolysis, dehydration, polymerization and aromatization, leading to the formation of brown hydrochar and soluble chemicals.4 Biomass-derived carbon materials are low-cost and have been reported as good candidates for carbon-based electrodes.5
The properties of specific surface area (SSA), porosity and conductivity of these materials have a big influence on their performance of electrochemistry.6–8 As we all know, the larger SSA value is favorable to obtaining electrode material with excellent performance. Till now, various strategies have been proposed to develop porous structure, including carbonization under KOH,9 ZnCl2 (ref. 10 and 11) and CO2.12 Despite the remarkable increase in the SSA value and pore size after activation, most materials display unsatisfied specific capacitance because of the low conductivity. Creating graphitic carbon leading to lower internal resistance is a possible method to solve the problem. Generally, the conventional graphitization transformation requires rigorous conditions, like high temperature (>1000 °C) or high vacuum degree, which do not only needs a huge energy input but also leads to a decreased porosity of the host.13,14 However, using transition metal (Fe, Co or Ni) functioned as a catalyst during the pyrolysis process could achieve graphitization transformation at low temperature.15–17 Metal organic frameworks (MOF), as a kind of porous coordination polymers, are promising materials in the field of supercapacitor and battery.18 Pang et al. studied a series of MOF composite as excellent electrochemical energy storage material, such as [Ni(thiophene-2,5-dicarboxylate)(4,4′-bipyridine)]n MOF nanocrystals,19 Co3O4 nanocube@Co-MOF.20 In some cases, the derived species could serve as electroactive species as well and can be used to prepare SCs with high performance. For example, Li et al.21 fabricated carbon hybrids by g-C3N4 and iron oxalate as electrode, which delivered an enhanced pseudocapacitance. In this process, iron oxalate was further reduced to metallic Fe followed by carbide reaction. Fe-based nanomaterials, such as encapsulated FeP nanoparticles with graphene,22 nano Fe7C3 with in situ grown CNT on N doped hollow carbon cube,23 N-doped carbon nanotubes grafted onto MOF-derived carbon nanomaterials (Fe-NCNT) were proved to display efficient electrochemical performance. β-FeOOH@carbon derived multi-shelled Fe2O3 microspheres by calcination in air could deliver a high capacity up to 630 F g−1 at 1 A g−1.24
Herein, we achieved a safe and environmentally friendly transformation from amorphous carbon spheres to graphitic carbon layers with Fe3C/Fe nanoparticles (NPs) through K2FeO4 named as FC-1-8, which showed excellent pseudocapacitance as the electrode for SCs. K2FeO4, in this article, is not only used as the activating agent but also functioned as the precursor of catalyst (Fe) in the graphitic transformation process. The derived Fe3C/Fe NPs serve as electroactive species as well and compared with the other amorphous carbon electrodes of FC-0-8 (carbon spheres annealed without the treatment of K2FeO4), the K2FeO4-derived Fe3C/Fe/graphitic carbon exhibited an outstanding pseudocapacitance of 428.0 F g−1 at 1 A g−1 working as an electrode material for SCs. After removal of the Fe3C/Fe electroactive materials, the graphitic carbon (FC-1-8-HCl) with a much high SSA up to 2813.6 m2 g−1 displayed a capacity of two times higher than that of the other type of amorphous carbon electrode, FC-0-8. Fe3C/Fe/graphitic carbon exhibited synchronous performance of graphitic carbon and electroactive species, which was inspirational and provided a novel route to design electrode material.
Sample designation | Glucose concentration (mol L−1) | Temperature/°C | Time/h |
---|---|---|---|
G1-200-10 | 1.0 | 200 | 10 |
G1-180-10 | 1.0 | 180 | 10 |
G0.5-180-10 | 0.5 | 180 | 10 |
G0.5-140-10 | 0.5 | 140 | 10 |
G0.5-140-20 | 0.5 | 140 | 20 |
The cyclic voltammetry (CV) and galvanostatic charge–discharge (GCD) curves were performed on an electrochemical workstation (CorrTest, China) at a voltage range from −1.2 to −0.3 V. The specific capacitance (C) was obtained from CV curves using the following relationship:
![]() | (1) |
The electrochemical impedance spectroscopy (EIS) was carried out on an electrochemical workstation (CHI660D) at an open circuit potential and a frequency range from 10−2 to 105 Hz.
4K2FeO4 + 10H2O = 8KOH + 4Fe(OH)3 + 3O2 | (2) |
In this step, KOH would react with carbon spheres and develop pores on the surface of samples. The graphitization transformation is as follows: the Fe species are transformed to Fe3O4 when annealed from 400 °C to 600 °C.27,28 In the case of 700 °C, Fe3O4 is converted to metallic Fe as a result of the reduction of amorphous carbon by H2 or CO produced during the pyrolysis process and when the temperature is further increased to 800 °C, graphitized carbon is formed under the catalysis of Fe.29 Apart from the existence of metallic Fe, a portion of Fe transforms into well-crystallized Fe3C. It was reported that the metallic Fe and pyrolytic carbon lead to the formation of Fe3C.30,31 Therefore, the results verified that the FC-1-8 sample was consisted of Fe3C/Fe and graphitic carbon. As displayed in Fig. 2a, the diffraction peaks locating at 37.6°, 42.9°, 43.7°and 45.9° correspond to Fe3C with the standard PDF card of JCPDS no. 35-0772. Two diffraction peaks are detected at 44.6°and 65.0°, which belong to the (110) and (200) planes of Fe (JCPDS no. 06-0696). Furthermore, carbon in the whole process was partly oxidized to CO/CO2 and carbonate and as a result, the porous structure was obtained.32 Obviously, graphitic carbon could be formed when annealed at the temperature of 800 °C.
To investigate the function of K2FeO4, carbon spheres annealed without the treatment of K2FeO4 (FC-0-8) were studied for comparison. From the XRD pattern in Fig. 2a, two relatively broad peaks were existed in the pattern of FC-0-8, implying that the dominant component of the above was amorphous carbon. Validated by the XRD pattern of FC-1-8-HCl, Fe3C/Fe composites were removed successfully. According to the nitrogen adsorption–desorption isotherms plotted in Fig. 2b, FC-1-8-HCl showed IV-type adsorption–desorption isotherm with H4-type hysteresis loop, indicating the presence of mesopores. The SSA of the obtained FC-0-8 is 479.8 m2 g−1, while the chemical activation treatment with K2FeO4 developed more pores making it increased to 545.5 m2 g−1 for FC-1-8. FC-1-8-HCl showed the largest SSA up to 2813.6 m2 g−1, resulting from the pores caused by the removal of Fe3C/Fe NPs. The pore size distribution in Fig. 2c revealed that the pore diameter of these samples was ∼3 nm, suggesting these samples were rich in mesopores.
Raman spectra were conducted to characterize the graphitization degree. Typically, the band at 1350 cm−1, known as D-band, is assigned to defect sites or the disordered sp2 carbon. The G band at 1580 cm−1 is corresponded to the in-plane vibrational mode of sp2 hybridized carbon.33 The intensity ratio of ID/IG values for FC-0-8, FC-1-8 and FC-1-8-HCl are 1.30, 0.99 and 1.00, respectively (Fig. 2d). Compared with FC-0-8, the lower ID/IG values of FC-1-8 and FC-1-8-HCl indicated a relatively short-range order graphitic carbon because of the treatment of K2FeO4. Furthermore, the X-ray photoelectron spectrum verified the existence of C, O and Fe elements in the surface of FC-1-8 (as illustrated in Fig. 2e).32 The high-resolution spectra Fe 2p orbit showed two dominant peaks at 711.0 and 713.1 eV, which were indexed to the 2p3/2 orbitals of Fe2+ and Fe3+, respectively (Fig. 2f). The peaks located at a binding energy of 724.6 eV, 726.4 eV and 718.5 eV were assigned to Fe2+ and Fe3+ for the 2p1/2 band, and a satellite.34
To evaluate the surface morphology and structure of the samples, SEM measurements of FC-0-8, FC-1-8 and FC-1-8-HCl were conducted (Fig. 3). After annealed in Ar atmosphere at 800 °C, the as-prepared carbon spheres (FC-0-8) became black and maintained a similar structure and the carbon spheres interconnected forming the 3D network, which was favorable to electron transfer. Besides, FC-1-8 and FC-1-8-HCl generally inherited their structure except for the rough surface of carbon spheres. Furthermore, a comparison of SEM images revealed that the average diameter of the FC-1-8-HCl sample was a little bit smaller than that of FC-1-8 after the removal of Fe3C/Fe NPs. Convinced by the particle size distributions (Fig. S2†), as measured by a statistical method measuring the diameter of 100 particles, the average size of FC-1-8 decreased from ∼450 nm to ∼240 nm after being etched by HCl.
The TEM images of FC-0-8 presented disordered carbon lattice fringes (Fig. 4a–c), suggesting the existence of amorphous carbon. As shown in Fig. 4d–f, the HRTEM of FC-1-8 was composed of graphitic carbon and Fe NPs. The lattice fringe with a spacing of 0.34 nm corresponded to the (002) plane of carbon and the lattice fringe calculated to be 0.20 nm and 0.24 nm were assigned to the (101) plane of Fe and (111) plane of Fe3C, respectively. Obviously, the existence of metallic Fe contributed to the formation of graphitic carbon. The corresponding elemental mappings of C and Fe further verified that the rough surface of carbon spheres should be Fe3C/Fe NPs (Fig. 4g–i). Part of FC-1-8-HCl NPs showed irregular structure while the HRTEM images in Fig. 4l confirmed the existence of graphitic carbon.
The whole process was economic and environmentally friendly without any toxic or hazardous materials input. FC-1-8 and FC-1-8-HCl were expected to be excellent electrode materials. On the one hand, the partial graphitization with hierarchical porosity structure could offer large SSA value and electroactive sites. On the other hand, the graphitic carbon ensured conductivity of the sample.
Fe3O4 + 4H2O + 2e− ![]() | (3) |
Notably, the graphitic FC-1-8-HCl displayed a much larger integral area than FC-0-8, which convincingly demonstrated excellent energy storage performance. In other words, carbon materials with higher graphitization degree exhibit superior Faraday capacitance. In detail, according to the GCD profiles, the FC-1-8 and FC-1-8-HCl electrodes can deliver the specific capacitance as high as 428.0 and 243.3 F g−1 at 1 A g−1, whereas the specific capacitance of FC-0-8 are only 84.3 F g−1 at 1 A g−1 (Fig. 5b). The capacitance value of FC-1-8 outperforms most reported Fe-based carbon materials in Table 2.
The electrochemical impedance spectroscopy (EIS) analysis was carried out to inspect the kinetic properties of these four samples in the range of 0.01 Hz to 100 kHz, the results were delivered in Fig. 5c. It was found that low frequency part of the region was almost straight, implying the low diffusion resistance.35 In the high frequency part of the EIS plot, FC-1-8 and FC-1-8-HCl display lower Rs values than FC-0-8. It is reasonable that the improved electrochemical performance is related to the higher graphitic degree. The Rct values of 0.21 and 0.22 Ω for FC-1-8 and FC-1-8-HCl were much lower than that of FC-0-8, 0.41 Ω, implying the faster charge transfer at the electrode and electrolyte interface.
As consistent with the CV analysis, the graphitic electrodes of FC-1-8 and FC-1-8-HCl showed a much longer discharge time than the other counterpart demonstrating higher specific capacitance (Fig. S3†). The higher values in specific capacitance can be contributed to the improved conductivity of graphitic carbon, the larger SSA and the porous structure. The CV curves of FC-1-8 at multiple scan rates were accessed in Fig. 5d. CV curves displayed similar shape with the scan rate decreasing from 100 to 5 mV s−1 (Fig. 5d). The reduction and oxidation peaks moved outwards as the increase of scan rates due to the polarization of the electrode. The details of galvanostatic charge/discharge curves were exhibited in Fig. 5e. Likewise, the galvanostatic charge–discharge (GCD) curves showing voltage platforms are believed to the nature of pseudocapacitance. FC-0-8 and FC-1-8-HCl exhibited typical rectangular shape of CV curves and triangular GCD curves, demonstrating a double layer electric capacitive behavior (Fig. S4†). The cycle stability was carried out by performing 10000 times at 5 A g−1 (Fig. 5f). FC-1-8 retained a moderate rate of 51.7% compared with the initial capacitance and the inferior cycle stability of FC-1-8 was probably due to the irreversibly oxidized of Fe3C/Fe to Fe3O4 in KOH electrolyte.21 The morphology of FC-1-8 and FC-1-8-HCl samples after electrochemical activation were conducted to uncover the mechanism of electrochemical performance (Fig. S5†). It was found that both samples presented spherical structure as before, while FC-1-8 sample showed a relatively smooth surface compared with the initial one. The absence of Fe3C/Fe species resulted in the inferior cycling performance.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra08834c |
This journal is © The Royal Society of Chemistry 2022 |