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Cobalt vanadium oxide thin nanoplates: primary electrochemical capacitor application

Scientific Reports volume 4, Article number: 5687 (2014) | Download Citation

Abstract

Co3V2O8 thin nanoplates are firstly described as a kind of electrode material for supercapacitors. More importantly, from electrochemical measurements, the obtained Co3V2O8 nanoplate electrode shows a good specific capacitance (0.5 A g−1, 739 F g−1) and cycling stability (704 F g−1 retained after 2000 cycles). This study essentially offers a new kind of metal vanadium oxides as electrochemical active material for the development of supercapacitors.

Introduction

Supercapacitors, an advanced safe electrochemical energy storage device, can hold higher power density, longer cycling life and shorter charge/discharge time1,2,3,4,5,6,7,8,9. The device stores energy on the basis of either charge accumulation (electric double layer capacitors) or fast reversible Faradaic reactions (pseudocapacitors) on the surface. Considerable efforts have been devoted to the development and characterization of new electrode materials with lower cost and improved performance.

Transition metal oxides can provide higher energy density in comparison to the electrical double layer capacitors with carbon-based active materials. And recently, binary metal oxides have been demonstrated better performance than single-component oxides due to their feasible oxidation states and high electrical conductivity8,10,11,12,13,14,15,16,17,18,19. Transition metal vanadium oxides and vanadates have been widely investigated as possible active materials for rechargeable lithium batteries20,21,22,23,24,25,26,27. Very recently, Wang et al have reported the successful preparation of cobalt vanadium oxide (Co3V2O8) nanostructures which exhibit outstanding reversible capacity and excellent rate performance for lithium storage26. However, the exploitation of Co3V2O8 nanostructures for supercapacitors has few developments.

This work describes the first investigation of Co3V2O8 nanoplates for supercapacitors. We provide a facile and hydrothermal method to synthesize Co3V2O8 nanoplates by the modified method of Wang et al26. Interestingly, the obtained Co3V2O8 nanoplate electrode shows a good specific capacitance (0.5 A g−1, 739 F g−1) and cycling stability (704 F g−1 retained after 2000 cycles) for supercapacitors.

Results

XRD patterns of as-prepared samples were performed to reveal the phase of the as-prepared samples in Fig. 1a. All intense peaks shown in Fig. 1a can be well indexed to cubic Co3V2O8 (JCPDS No.16-0675). The peaks are strong, which indicates the good crystallinity of the as-prepared samples. Good crystallinity of as-prepared Co3V2O8 might be good to improve the cycle life of electrodes for its crystal structure is stable and it is not easy to be destroyed during the electrochemical process. The EDS result in Fig. 1b demonstrates that the nanoplates are composed of the elements of Co, O, and V.

Figure 1
Figure 1

a) XRD patterns of as-prepared samples and its corresponding JCPDS card No 16-0675; b) corresponding EDS patterns.

The morphology of as-prepared Co3V2O8 is examined by field emission scanning electron microscopy (FESEM), atomic force microscope (AFM) and transmission electron microscopy (TEM). A typical low-magnification FESEM image is shown in Fig. 2a and the morphology of samples is thin nanoplates in 2D microscale with a diameter of 150 ~ 200 nm. The thickness of the thin nanosheet is ~40 nm in Fig. 2b. AFM measurement is further used to confirm the thickness of the single nanoplate in Fig. 2c. It can be seen that the accurate thickness is 42.7 nm in the inset of Fig. 2c, which is consistent with the FESEM result in Fig. 2b. In addition, there are nearly no pores seen from the TEM image in Fig. 2d, e. The selected area electron diffraction (SAED) pattern is shown in the inset of Fig. 2e, which demonstrates the good crystalline nature of the product. The measured distance of neighboring lattice fringes in Fig. 2f is ~0.59 nm, corresponding well to the (110) lattice spacing of Co3V2O8.

Figure 2
Figure 2

a, b) FESEM images of as-prepared Co3V2O8; c) Corresponding AFM image; d, e) TEM images (inset-corresponding SAED pattern); f) Corresponding HRTEM image (inset-the large magnification image).

Discussion

The CVs of Co3V2O8 thin nanoplate electrodes (a mass loading of ~5 mg) in 3.0 M KOH at different scan rates (5 ~ 100 mV s−1) are shown in Fig. 3a. As is seen in Fig. 3a, the shapes are different from that of electric double-layer capacitance, suggesting that the capacity mainly results from pseudocapacitive capacitance. And it is clear that the Faradaic pseudocapacitive property of Co3V2O8 thin nanoplates is based on the surface redox mechanism of Co2+ to Co3+ on the surface. Chronopotentiometry (CP) curves at different current densities are shown in Fig. 3b. Different charge–discharge current densities and times can be clearly seen. As increasing of current densities, short charge–discharge times have been obtained.

Figure 3
Figure 3

a) Cyclic voltammetry within a 0.0–0.42 V range at a scan rate 5–100 mV s−1 were performed on the Co3V2O8 thin nanoplate electrode in 3.0 M KOH at room temperature, b) The galvanostatic charge–discharge curves during current densities, 0.5–4.0 A g−1, c) Specific capacitances derived from the discharging curves at the current density of 0.5–4.0 A g−1, and d) Charge/discharge cycling test at 0.5 A g−1.

The relationship between the specific capacitances calculated by CP curves and current densities is given in Fig. 3c. Based on the curve, Co3V2O8 thin nanoplate electrodes show a good specific capacitance and reach up to 739 F g−1 at the current density of 0.5 A g−1, and 516 F g−1 even at 4.0 A g−1. The specific capacitance of Co3V2O8 thin nanoplates is better than that of our previous cobalt based phosphate nanomaterials, for example, NH4CoPO4·H2O microflowers (<340 F g−1 at 1.5 A g−1)28, cobalt phosphite microarchitectures (<312 F g−1 at 1.5 A g−1)29. However, some materials show larger values than that of ours30,31.

The relationship of the specific capacitance against cycling number of Co3V2O8 thin nanoplate electrodes is shown in Fig. 3d, which shows its good specific capacitance retention at 0.5 A g−1. After 350 continuous charge–discharge cycles, Co3V2O8 thin nanoplate electrodes almost retain the same specific capacitance as its initial value. More importantly, Co3V2O8 thin nanoplate electrodes still retain more than 95.3% of their specific capacitance after 2000 continuous charge–discharge cycles. After the testing of the cycle life, we have measured the morphology and X-ray diffraction of the electrode materials in Supplementary Information (SI) Fig. 1, 2. There are few changes of Co3V2O8 thin nanoplates after 2000 charge–discharge cycles in SI Fig. 1, and the good crystallinity of as-prepared Co3V2O8 has also been maintained. What's more, the nanoplate structure might offer a stable structure for ion intercalation/extraction, which might improve the cycle life of the electrode. We have tried to propose the possible the reaction mechanism of Co3V2O8 in equation (1). To identify the exact electrical conductivity of electrodes, we have measured electrochemical impedance spectra (EIS) of Co3V2O8 thin nanoplate electrodes at room temperature in the frequency range 0.01–105 Hz at different potentials in SI Fig. 4. The impedance plot at 0.42 V in 3 M KOH exhibits a line along the imaginary axis (Z″). At a potential of 0, 0.60 or 0.70 V, the linear characteristic becomes weaker. Thus, the proper potential range, over which electrode can generate desirable capacitance, is below 0.42 V. Fig. 4 shows the EIS of Co3V2O8 thin nanoplate electrodes at room temperature and its calculated curve by the ZSimpWin software. An equivalent circuit used to fit the impedance curve is given in the inset of Fig. 4a, which is similar to the circuit employed for the working electrode of supercapacitors. The EIS data can be fitted by a bulk solution resistance Rs, a charge-transfer Rct and a pseudocapacitive element Cp from the redox process of electrode materials, and a CPE to account for the double-layer capacitance. The charge-transfer resistance Rct is calculated by the ZSimpWin software. From the calculated results, Rct of Co3V2O8 thin nanoplate electrodes is 5.3 Ω. It clearly demonstrates the reduced charge-transfer resistance of the Co3V2O8 thin nanoplate electrode. The nanoplate surface-interface character might decrease the polarization of the electrode, and thus increase the capacity. What's more, the phase angles for impedance plots of Co3V2O8 thin nanoplate electrodes and its calculated curve by ZSimpWin software are observed in Fig. 4b. These phase angles are near 80° in the low frequencies clearly, which means that the Co3V2O8 thin nanoplates allow ions or electrolyte transfer to occur quickly. Compared with the charge-transfer resistance of other Co3V2O8 nano/micro structures in SI Fig. 3, 4, and SI Table 1, it is seen that the Co3V2O8 thin nanoplate can reduce the charge-transfer resistance more effective than other Co3V2O8 nano/micro structures.

Figure 4
Figure 4

The EIS of the electrodes at room temperature and its corresponding calculated curve, in inset of a) The equivalent circuit; and b) The phase angles for impedance plots and its corresponding calculated curve.

In summary, Co3V2O8 thin nanoplates have been successfully synthesized to show the novel nanoplate surface-interface feature, which plays a key role in the ion intercalation/extraction and electrolyte access. The electrochemical investigation of Co3V2O8 thin nanoplates is interesting work, which firstly illustrates Co3V2O8 thin nanoplates can be applied as an electroactive material for supercapacitors. Despite the specific capacitance of Co3V2O8 thin nanoplates are not much larger than some famous materials, it might direct a new generation of nanodevices by exploring the electrochemical characteristics of novel nano/micromaterials.

Methods

In a typical synthesis, 187 mg of NH4VO3 was dissolved into 32 mL deionized water at 80°C. Under severely stirring, 40 mg NaOH was added to the ammonium metavanadate solution. Then, 76 mg Co(OAc)2·4H2O was added to the solution under stirring. After continuous stirring for 10 mins, the resulting yellow precursor suspension was transferred into a 40 mL Teflon-lined autocalve and maintained at 120°C for 12 hours. After reaction, the brown yellow precipitates were obtained. The precipitates were thoroughly washed with distilled water and ethanol to remove ions possibly remaining in the final products, and dried at room temperature in the air.

Characterizations. The morphology of as-prepared samples was observed by a JEOL JSM-6701F field-emission scanning electron microscope (FE-SEM) at an acceleration voltage of 5.0 kV. The phase analyses of the samples were performed by X-ray diffraction (XRD) on a Rigaku-Ultima III with Cu Kα radiation (λ = 1.5418 Å). Transmission electron microscopy (TEM) images were captured on the JEM-2100 instrument microscopy at an acceleration voltage of 200 kV. Atomic force microscope (AFM) images were measured at CSPM4000 (Benyuan, Beijing).

Electrochemical measurement. Electrochemical study on Co3V2O8 thin nanoplates electrodes was carried out on a CHI 660D electrochemical working station (Shanghai Chenhua Instrument, Inc.). All electrochemical performances were carried out respectively in a conventional three-electrode system equipped with a platinum electrode and a saturated calomel electrode (SCE) as counter and reference electrodes. Before electrochemical measurement, we have purged out O2 from the solution by the inert gas-Ar. The working electrode was made by mixing active materials (Co3V2O8 thin nanoplates), acetylene black, and PTFE (polytetrafluoroethylene) at a weight ratio of 80:15:5, coating on a piece of foamed nickel foam of about 1 cm2, and pressed it to be a thin foil at the pressure of 5.0 MPa. The electrolyte was 3.0 M KOH solution. Electrochemical impedance spectroscopy measurements of all the samples were conducted at 0.42 V in the frequency range from 100 kHz to 0.01 Hz with the AC voltage amplitude of 5 mV by using PARSTAT2273.

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Acknowledgements

This work is supported by the Program for New Century Excellent Talents of the University in China (grant no. NCET-13-0645) and National Natural Science Foundation of China (NSFC-21201010), Program for Innovative Research Team (in Science and Technology) in University of Henan Province (14IRTSTHN004), the Science & Technology Foundation of Henan Province (122102210253, 13A150019), and the China Postdoctoral Science Foundation (2012M521115). We are very grateful to Liang Chen from Anyang Normal University in the language modification.

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  1. Key Laboratory for Clearer Energy and Functional Materials of Henan Province, College of Chemistry and Chemical Engineering, Anyang Normal University, Anyang, 455000 Henan, P.R. China

    • Youjuan Zhang
    • , Yuanying Liu
    • , Jing Chen
    • , Qifei Guo
    • , Ting Wang
    •  & Huan Pang
  2. State Key Laboratory of Coordination Chemistry, Nanjing University, Nanjing, 210093, Jiangsu, P.R. China

    • Huan Pang

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Contributions

Y.J.Z., Y.Y.L., J.C., Q.F.G., T.W. and H.P. conceived and designed the experiments., Y.J.Z., J.C. and H.P. analyzed the measurements. H.P. wrote the manuscript in collaboration with all the authors.

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The authors declare no competing financial interests.

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Correspondence to Huan Pang.

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