Yuqing Qiao*ab,
Qujiang Suna,
Haiying Cuia,
Debiao Wanga,
Fengyu Yanga and
Xianhui Wang*c
aCollege of Environmental and Chemical Engineering, Yanshan University, Qinhuangdao 066004, P. R. China. E-mail: qiaoyq@ysu.edu.cn; Fax: +86 335 8061569; Tel: +86 335 8061569
bState Key Laboratory of Metastable Material Science and Technology, Yanshan University, Qinhuangdao, 066004, P. R. China
cSchool of Materials Science and Engineering, Xi'an University of Technology, Xi'an, 710048, P. R. China. E-mail: xhwang693@xaut.edu.cn
First published on 20th March 2015
Micro/nano-structured Mn3O4 with an open three-dimensional flower-like morphology were fabricated by a facile solvothermal approach using hexadecyltrimethylammonium bromide as a surfactant and CH3CH2OH as a solvent. The Mn3O4 microspheres were self-assembled by one-dimensional nanowires; in addition, a dandelion-structure formation mechanism of the Mn3O4 microspheres is discussed. The Mn3O4 microspheres used as a supercapacitor electrode in 1 mol L−1 Na2SO4 electrolyte have a specific capacitance value of 286 F g−1 at a low current density of 0.5 A g−1, and can still retain 80% (230 F g−1) and 73% specific capacitance (210 F g−1) when the current densities are increased ten-fold (5 A g−1) and twenty-fold (10 A g−1), respectively. In addition, the capacitance retention is 90% after 1000 cycles at a current density of 5 A g−1. In comparison with Mn3O4 synthesized in N,N-dimethylformamide solvent at 0.5 A g−1 and 5 A g−1, the specific capacitance obtained increased by 18.7% and 17.4%, respectively.
5 have attracted significant attention. Among these transition metal oxides, Mn3O4 is the most promising electrode material for commercial supercapacitors because of its environmental friendliness.6,7 However, poor electronic conductivity limits its application in high-power electrochemical capacitors.8–11 Though high surface areas and readily accessible mesopores can be achieved by embedding or depositing Mn3O4 nanoparticles on to a highly conductive porous matrix, such as graphene,12–14 carbon15 or other materials,16 there are some shortcomings too, such as the synthesis complexity, the relatively low capacitance, and low stability. Wu et al.13 synthesized Mn3O4/graphene nano-composites by a simple solvothermal process, and they exhibited good rate capability, with a capacity of 116 F g−1 at 5 A g−1, as compared with a capacity of 22.5 F g−1 at 5 A g−1 for Mn3O4 without graphene, i.e. nearly a fivefold improvement. Although the high surface area can provide more electrochemically active sites for charge storage/delivery, and although the large tunable porosity is beneficial for ion transportation and electrolyte permeation,17,18 the downsizing strategy and the porosity of the materials reduce the volumetric energy density,19,20 which is an undesirable feature for the use of Mn3O4 as an electrode material in commercial applications.
In our previous work,21 porous nanostructured Mn3O4 particles with a size of about 10 nm were synthesized by a hydrothermal method by adding the surfactant hexadecyltrimethylammonium bromide (CTAB) in to N,N-dimethylformamide (DMF) solvent, and they exhibited a high specific capacitance of 232.5 F g−1 at 0.5 A g−1 and a good rate capability of 190 F g−1 at 5 A g−1. In consideration of the toxicity and the viscidity of DMF, DMF was replaced by CH3CH2OH in the solvothermal method. In the present investigation, the Mn3O4 electrode materials were synthesized by a solvothermal method using CTAB as a surfactant and CH3CH2OH as a solvent. The purpose of the present work is to attain a Mn3O4 electrode material with a high rate discharge-ability, and also to gain more insights into the formation mechanism of the micro/nano-structures.
The phase constituents were determined on a Rigaku D/max 2500pc X-ray diffractometer (XRD). X-ray photoelectron spectroscopy (XPS) was performed with an ESCALAB 250Xi. The morphologies of the synthesized materials were characterized by an S-4800 field emission scanning electron microscopic (FE-SEM). The microstructures of the samples mounted on a Cu grid were observed by a JEM-2100 at 200 kV.
All electrochemical measurements were performed in a three-electrode system. The Mn3O4 activated material was used as the working electrode, and was prepared by mixing the activated material with acetylene black and PVDF at a mass ratio of 7
:
2
:
1; the mass loading of each electrode was about 2 mg cm−2. Pt electrode was used as the counter electrode, and a Hg/Hg2Cl2 electrode was used as the reference electrode in 1 mol L−1 Na2SO4 electrolyte solution. The electrochemical performance was tested on a BTS-5V10 mA system in the range of 0–1 V at 0.5 A g−1 and 5 A g−1 current densities. The electrochemical impedance spectroscopy (EIS) was conducted on a CHI 660E electrochemical workstation with an oscillation voltage of 5 mV and the applied frequency ranged from 0.01 Hz to 100 kHz.
Fig. 2a and b are the XPS spectra of the as-prepared Mn3O4 sample in a region of 0–1200 eV and in the Mn 2p region, respectively. As seen from Fig. 2a, no impurities are present except for the contaminant carbon. It can be seen from Fig. 2b that the binding energy values of Mn 2p2/3 and Mn 2p1/2 are 641.43 eV and 653.53 eV, respectively. The Mn 2p2/3 (641.43 eV) value corresponds to Mn3O4.13,22 In addition, it can be observed that the spin–orbit splitting width (ΔE) of the two peaks (i.e. Mn 2p2/3 and Mn 2p1/2) is 12.10 eV, which is in accordance with the spectrum of Mn3O4.23,24
Fig. 4 shows the TEM images of a single prepared Mn3O4 particle and its surface morphology. It can be seen from Fig. 4a that the Mn3O4 particle is a microsphere with a diameter of about 3–5 μm. As seen from Fig. 4b and in the inset in Fig. 4b, the surfaces of the Mn3O4 microsphere seem to be fabricated by one-dimensional nanowires, and the diameter of the nanowires is less than 10 nm. It can be deduced that one-dimensional nanowires first assemble into two-dimensional petals in the internal part of the materials, and then assemble into three-dimensional micro/nano-structures. When the micro/nano-structured Mn3O4 is used as a supercapacitor electrode, it can be expected to exhibit some advantages, such as: (1) nanoparticles are favorable for electron transport at the interface of the electrode and electrolyte; (2) the porous structures can maintain high electrolyte penetration/diffusion rates; and (3) the large volumetric energy density with the micro/nano-structure is useful for commercial applications.
Fig. 6b shows the galvanostatic charge–discharge curves of the Mn3O4 microspheres at the current density ranging from 0.5 A g−1 to 10 A g−1. It can be seen that the prepared Mn3O4 microspheres have a specific capacitance value of 286 F g−1 at a current density of 0.5 A g−1, and can still retain 80% specific capacitance (230 F g−1) and 73% specific capacitance (210 F g−1) when the current densities are increased tenfold (5 A g−1) and twentyfold (10 A g−1), respectively. In comparison with data from Mn3O4 synthesized in DMF solvent,21 the specific capacitance obtained in the present work increased by 18.7% and 17.4% at 0.5 A g−1 and 5 A g−1, respectively. In comparison with the values reported by Zhang et al.,5 the specific capacitance (286 F g−1) increased by about 40% over that of the Mn3O4 electrode (205 F g−1) at a low current density of 0.5 A g−1, while the specific capacitance (230 F g−1) increased by about 72% over that of the Mn3O4 electrode (134 F g−1) at a high current density of 5 A g−1.
The high rate performance of capacitance is one of the most important electrochemical parameters for the application of supercapacitors, especially for the electrode materials used in electric vehicles. Fig. 7a shows the relationship between the specific capacitance and the current density. It can be seen that the Mn3O4 electrode has an excellent high-rate performance, which is probably ascribed to the one-dimensional nanowire structure of the prepared Mn3O4 microspheres. The nanoparticles and the porous structure can provide a larger surface area and more Mn3O4/electrolyte contact areas.
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| Fig. 7 Discharge capacity of Mn3O4 electrode at different current densities (a) and cycling stability profile of Mn3O4 electrode at a current density of 5 A g−1 (b). | ||
The cycle stability test was carried out by the galvanostatic charge–discharge technique at a current density of 5 A g−1. The specific capacitance as a function of the cycle number is presented in Fig. 7b. It can be seen from Fig. 7b that the capacitance retention is 90% after 1000 cycles. Although the capacitance retention decreases with cycle number, the coulombic efficiency on the charge–discharge cycle numbers almost remains constant at 97%. It is noticed that the Mn3O4 electrode prepared in CH3CH2OH solvent has a specific capacitance of 230 F g−1 on the 12th charge–discharge cycle, while the specific capacitance of the Mn3O4 synthesized in DMF solvent increases continuously for the first 600 cycles. It is clear that the Mn3O4 electrode material obtained in the present work has a better activated property than the Mn3O4 prepared in DMF. This suggests that the dandelion-structure self-assembled by one-dimensional nanowires can provide more active sites for redox reactions.
Fig. 8 presents the electrochemical impedance spectra (EIS) of the as-prepared Mn3O4 electrode materials. The EIS data are fitted by Zview software according to an equivalent circuit (see the inset in Fig. 8), and for details of the equivalent circuit, refer to the literature.21 The semicircle near the high-frequency region (see the inset in Fig. 8) corresponds to the charge transfer resistance Rct at the interface of the electrode and electrolyte. The fitting result shows that the charge-transfer resistance Rct is 2.43 Ω for the Mn3O4 electrode. The charge-transfer resistance (2.43 Ω) is decreased by about 4.1 times than that reported by Wu et al.,13 while the charge-transfer resistance (2.43 Ω) is increased by about 2.7 times than that of the Mn3O4 electrode (0.91 Ω) synthesized in DMF solvent, which has a porous structure with a large surface area.21 Thus, more work is needed to improve the porous structure of the Mn3O4 electrode materials in the future.
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