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Article

Sophisticated Structural Tuning of NiMoO4@MnCo2O4 Nanomaterials for High Performance Hybrid Capacitors

1
School of Materials Science and Engineering, Liaoning University of Technology, Jinzhou 121001, China
2
Liaoning Brother Electronics Technology Co., Chaoyang 122000, China
*
Authors to whom correspondence should be addressed.
Nanomaterials 2022, 12(10), 1674; https://doi.org/10.3390/nano12101674
Submission received: 14 April 2022 / Revised: 9 May 2022 / Accepted: 9 May 2022 / Published: 14 May 2022

Abstract

:
NiMoO4 is an excellent candidate for supercapacitor electrodes, but poor cycle life, low electrical conductivity, and small practical capacitance limit its further development. Therefore, in this paper, we fabricate NiMoO4@MnCo2O4 composites based on a two-step hydrothermal method. As a supercapacitor electrode, the sample can reach 3000 mF/cm2 at 1 mA/cm2. The asymmetric supercapacitor (ASC), NiMoO4@MnCo2O4//AC, can be constructed with activated carbon (AC) as the negative electrode, the device can reach a maximum energy density of 90.89 mWh/cm3 at a power density of 3726.7 mW/cm3 and the capacitance retention can achieve 78.4% after 10,000 cycles.

1. Introduction

With the development of the world economy, environmental pollution is caused by the excessive burning of traditional fossil fuels, which poses a serious threat to the goal of human sustainable development [1]. Supercapacitors (SCs), as a new environmentally friendly electrochemical energy storage device, have attracted extensive attention from researchers. The selection of electrode material is an important factor for energy storage performance. Developing an electrode material with excellent electrochemical performance has become key to the future development of SCs [2,3,4,5]. Transition metal oxides possess high specific capacitance, superior cycling performance and abundant valence states, such as NiMoO4, MnCo2O4, NiCo2O4 and ZnCo2O4. They have been widely reported due to their large theoretical capacitance, excellent redox performance and environmental friendliness [6,7,8,9,10].
NiMoO4 is a very suitable electrode material for SCs because of its advantages of better electrochemical performance and low price [11,12,13]. However, there are still many problems such as low theoretical utilization value, poor cycle life and low conversion performance at a higher rate [14]. Xuan [15] et al. prepared a NiMoO4@Co3O4 composite nanoarray electrode. The pseudocapacitance performance of the prepared NiMoO4@Co3O4-5H composite was 1722.3 F/g at the current density of 1 A/g, and the capacitance retention rate of 91% was realized by the 6000 cycles test. Feng [16] et al. prepared hierarchical flower-like NiMoO4@Ni3S2 composite material on a 3D nickel foam matrix by the hydrothermal method. The specific capacity was 870 C/g at 0.6 A/g, and the capacity retention rate was 81.2% after 8000 cycles. Transition metal oxide MnCo2O4 with excellent electrochemical performance is very suitable for the electrode material of SCs, because its Mn ion can offer high electron conductivity and excellent rate performance, and cobalt ion has high oxidation potential. However, they can also demonstrate poor application, such as poor cycling performance, poor electrical conductivity and so on, which greatly affect the practical application of SCs [17,18]. Cheng [19] et al. prepared porous MnCo2O4@NiO nanosheets by hydrothermal synthesis and calcination. The specific capacitance of the electrode material was 508.3 F/g at 2 A/g current density. The 2000 cycles test was applied at 10 A/g current density, and it presented the capacitance retention performance of 89.7%. Liu [20] et al. prepared MnCo2O4@MnO2 nanosheet arrays with core–shell structure on nickel foam by two-step hydrothermal treatment. The surface capacitance of the electrode was 3.39 F/cm2 at a current density of 3 mA/cm2. Furthermore, the capacity retention rate was 92.5% by 3000 cycles test at a current density of 15 mA/cm2. It could be seen that the composites exhibited excellent electrochemical properties due to their excellent conductivity [21,22,23,24]. It was also confirmed that NiMoO4 and MnCo2O4 have great potential as electrode materials for SCs [25]. The composite electrodes constructed from these two materials can effectively improve the conductivity, specific surface area, and number of reaction sites, thereby improving the overall electrochemical performance. [26,27,28].
In this work, NiMoO4@MnCo2O4 composite electrode material is obtained by the two-step hydrothermal synthesis method. The results show that the NiMoO4@MnCo2O4 electrode has better electrochemical performance than single NiMoO4 or MnCo2O4 electrode, and its electrochemical performance is greatly improved after the composite. At the current density of 1 mA/cm2, the specific capacitance of single NiMoO4 electrode material is 1656 mF/cm2, and the specific capacitance of the single MnCo2O4 electrode material is 224 mF/cm2. Finally, the NiMoO4@MnCo2O4 electrode material is 3000 mF/cm2. After 10,000 cycles, the capacity retention rate of NiMoO4@MnCo2O4 electrode material is 96%. NiMoO4@MnCo2O4//AC devices show high electrochemical performance with a maximum energy density of 90.89 mWh/cm3 and a power density of 3726.7 mW/cm3.

2. Experimental Section

2.1. Preparation of NiMoO4 Nano Pompon-Like Structure Electrode Material

In a typical process, 6 mmol Na2MoO4·2H2O, 6 mmol Ni(NO3)2·6H2O, 1 mmol NH4F, and 1 mmol CO(NH2)2 was added to 50 mL deionized water. After magnetic stirring, the nickel foam was put into the solution and reacted at 120 °C for 12 h, and then it was cleaned by deionized water and anhydrous ethanol to remove surface impurities. The NiMoO4 precursor was obtained by drying for 6 h in a drying oven at 60 °C and annealing for 2 h in air at 350 °C.

2.2. Preparation of NiMoO4@MnCo2O4 Urchin-like Core-Shell Structure Electrode Material

In a similar process to above, 6 mmol Mn(CH3COO)2·4H2O, 6 mmol Co(NO)3·6H2O, 5 mmol NH4F and 5 mmol CO(NH2)2 were dissolved in 50 mL deionized water to obtain a homogeneous solution. The nickel foam with NiMoO4 was put into this solution, and it kept 140 °C for 8 h. After cooling down to room temperature, the samples were washed, dried, and annealed for 2 h at 350 °C. The mass loading of NiMoO4, MnCo2O4, and NiMoO4@MnCo2O4 is 1.27, 1.02, and 1.91 mg/cm2, respectively.

2.3. Materials Characterizations

The elemental composition and valence of the samples were characterized by X-ray powder diffraction (XRD, D/max-2500/PC, Rigaku Corporation, Tokyo, Japan) with Cu Kα (λ = 1.5406 Å) and X-ray photo-electron spectroscopy (XPS, ESCALAB250, FEI Company, Waltham, MA, USA). The structure and morphology were investigated by emission scanning electron microscopy (SEM, Sigma500, Zeiss, Jena, Germany), and high-resolution transmission electron microscopy (HRTEM, Tecnai G2 S-Twin F20, FEI Company, Waltham, MA, USA).

2.4. Electrochemical Measurements

The electrochemical characteristics of the products were tested by Shanghai CHI660E electrochemical workstation. The sample material was applied as the working electrode, the platinum electrode was utilized as the auxiliary electrode, and Hg/HgO electrode was employed as the reference electrode. The working electrode was processed as a circle with a diameter of 1 cm. Moreover, 3 M KOH solution was used as the electrolyte and the ultrasonic-treated nickel foam was served as the collector. Through cyclic voltammetry (CV), galvanostatic charging–discharging (GCD), electrochemical impedance spectroscopy (EIS) and cycling performance measurements, the electrochemical properties of electrode materials and their application value were analyzed.
Energy density (E) can be obtained from the integral area of discharging curves. Specific capacitance (Cs), power density (P), and coulombic efficiency (η) can be calculated by the following equations:
Cs = IΔtd/SΔV
P = 3600E/Δtd
η = Δtd/Δtc
where I is the current value, Δtd and Δtc represent the discharging time and charging time, S is the geometrical area of the electrode, and ΔV denotes the voltage window.

2.5. Fabrication of Asymmetric Supercapacitors

Asymmetric supercapacitors were constructed with NiMoO4@MnCo2O4 as the positive electrode and active carbon as the negative one. The active carbon electrode was made of active carbon, acetylene black, and polyvinylidene fluoride with N-methylpyrrolidone as the solvent in a mass ratio of 7:2:1. The slurry was evenly coated on the nickel foam. The active carbon electrode was vacuum dried for 24 h at 60 °C. The electrolyte of ASCs was PVA-KOH. The preparation process was as follows: 3 g PVA and 3 g KOH were mixed in 30 mL deionized water, and the mixture was heated in an 80 °C water bath for 1 h and stirred continuously until clear.

3. Results and Discussion

The NiMoO4@MnCo2O4 composite electrode was synthesized by a two-step hydrothermal method, as shown in Figure 1. Firstly, NiMoO4 precursor is grown on nickel foam. Secondly, NiMoO4 can be obtained by calcination. Thirdly, the nano needle-like MnCo2O4 precursor was coated on NiMoO4 by the second hydrothermal preparation. Finally, the samples were calcined to obtain NiMoO4@MnCo2O4 on nickel foam.
As seen from the XRD results of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials, it can be observed that the three strong peaks are diffraction peaks of the foamed nickel substrate in Figure 2. When 2θ values are 26.57°, 29.14°, 33.73° and 60.01°, the crystal planes correspond to (220), (310), (22 2 ¯ ) and (060). The crystal structure is consistent with that of NiMoO4 (JCPDS No. 45-0142). Meanwhile, the values of 2θ are 30.53°, 35.99°, 57.90° and 63.62° and the diffraction peaks correspond to (220), (311), (511) and (440) crystal planes, which is consistent with the crystal structure of MnCo2O4 (JCPDS No. 23–1237). Therefore, the diffraction peaks of NiMoO4@MnCo2O4 electrode material prepared under the condition of the best ratio correspond to the diffraction peaks of a single compound.
Figure 3 shows the morphologies of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials. As seen from Figure 3a,b, the NiMoO4 electrode material is nano pompon-like, and there are many intersecting nano needle-like structures densely growing on the nickel foam substrate. As shown in Figure 3c,d, MnCo2O4 electrode material possesses a nano needle-like structure and uniformly grows on the nickel foam substrate. Figure 3e,f show the micromorphology of NiMoO4@MnCo2O4 electrode material. It can be observed that a large number of uniformly distributed nano needle-like MnCo2O4 and nano pompon-like NiMoO4 grow together to form a uniform and orderly arrangement of nano urchin-like morphology, which increases the specific surface area of NiMoO4 electrode and presents a great deal of active sites for rapid transfer between ions and active substances. The gap between the nano needle-like structures allows sufficient Faraday chemical reactions between the active substance and electrolyte, which enhances the electrochemical storage performance. Figure 3g,h show TEM images of NiMoO4@MnCo2O4 electrode material. Figure 3g exhibits the morphology after the composite of NiMoO4 and MnCo2O4. It can be seen from Figure 3h that NiMoO4@MnCo2O4 composite material shows two kinds of lattice fringes; the lattice fringes with the spacing of 0.154 nm correspond to the (060) crystal plane of NiMoO4, and the lattice fringes with the spacing of 0.146 nm correspond to the (440) crystal plane of MnCo2O4. From the stable microstructure of NiMoO4@MnCo2O4, it can be inferred that the composite has multiple ion and electron transport channels and a larger specific surface area, therefore it is beneficial to shorten the ion diffusion path, which makes it advantageous for high storage capacity and rate capacity.
In order to further investigate the elemental component and different valence states of the prepared NiMoO4@MnCo2O4 composite, XPS tests were carried out on the samples. Figure 4a presents the full measurement scanning spectrum showing the presence of Mn 2p, Co 2p, Mo 3d, Ni 2p, O 1s and C 1s, among which O 1s and C 1s elements are mixed impurities in the test process. In order to identify the detailed valence states of Mn, the high resolution XPS spectrum is present in Figure 4b. The Mn 2p3/2 and Mn 2p1/2 are found in the two main peaks, respectively, which can be divided into four peaks after fine fitting. The two peaks with a binding energy of 641.4 eV and 652.9 eV can be ascribed to the presence of Mn2+. The peaks corresponding to Mn3+ are distributed with a binding energy of 644.6 eV and 654.2 eV, respectively. Meanwhile, there is a satellite peak (defined as “Sat.”) at a position with a binding energy of 644.6 eV. According to the Co 2p spectrum of Figure 4c, it was found that two peaks appear at 780 eV and 795.3 eV, corresponding to the two excitation spectra of Co 2p3/2 and Co 2p1/2. The diffraction peaks corresponding to Co2+ have a binding energy of 781.5 eV and 797.3 eV, respectively. The diffraction peaks corresponding to Co3+ have a binding energy of 779.9 eV and 795.2 eV, respectively. In Figure 4d, the peaks of Mo 3d spectrum at 231.6 eV and 234.8 eV belong to Mo 3d5/2 and Mo 3d3/2, respectively. In Figure 4e, Ni 2p spectra can be well fitted into two main peaks, characterized by Ni2+ and Ni3+ oxidation states. Each peak has its own satellite peak (defined as “Sat.”) at 861.6 eV and 879.9 eV, respectively. Two fitting peaks at 855.1 eV (Ni 2p3/2) and 872.9 eV (Ni 2p1/2) belong to Ni2+, and two fitting peaks at 855.9 eV (Ni 2p3/2) and 873.8 eV (Ni 2p1/2) belong to Ni3+. Figure 4f shows the O 1s region, which can be divided into two peaks (529.8 eV and 531.8 eV). For the binding energy of 529.8 eV, it is attributed to the formation of M-O bond (M=Co, Mn). Therefore, XPS data confirm that the synthesis of NiMoO4@MnCo2O4 is successful [29,30,31].
Figure 5a shows the cyclic voltammetry (CV) curves of NiMoO4@MnCo2O4 electrode material, which is measured by a scanning rate of 10–100 mV/s and a voltage window of 0–0.5 V, showing excellent rate performance. The visible redox peaks are seen from the curves, indicating that redox reaction occurs in the process of energy storage. Figure 5b presents the galvanostatic charge–discharge (GCD) curves with current density of 1, 2, 4, 8, and 10 mA/cm2, the areal capacitance is 3000, 1076, 964, 696, and 580 mF/cm2, respectively. The high electrochemical performance is mainly attributed to the nano urchin-like morphology of the material. The nano needle-like structure densely and uniformly distributed on the urchin-like surface provides a larger surface area for electrolyte contact, thus improving the electrochemical performance of the composite.
In order to show the advantages of the composite electrode, NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials are used as working electrodes, respectively, and necessary tests are carried out in a three-system with 3 M KOH solution. Studies have shown that the capacitance of NiMoO4 in an alkaline environment is mainly attributed to the reversible redox reaction between the valence states of Ni element, while Mo element does not participate in any reaction, but it helps to improve the conductivity of molybdate. Figure 5c reveals the CV curves of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrodes at 10 mV/s. Visible redox peaks can be seen from the curves. By comparing the three CV curves, it is obviously observed that the NiMoO4@MnCo2O4 electrode has a larger integral area than NiMoO4 and MnCo2O4 electrode, so it has a larger specific capacitance. These excellent electrochemical properties can be credited to the singular nano urchin-like structure and a series of redox reactions, which not only involve Co2+ and Mn2+, but also come from Ni2+, thus increasing the redox peak. The specific redox reaction mechanism is as follows:
NiMoO4: NiMoO4 → Ni2+ + MoO42−
Ni2+ + 2OH → Ni(OH)2
Ni(OH)2 + OH → NiOOH + H2O + e
MnCo2O4: MnCo2O4 + H2O + OH → MnOOH + 2CoOOH + e
MnOOH + OH → MnO2 + H2O + e
CoOOH + OH → CoO2 + H2O + e
Figure 5d shows the GCD curves of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 composite electrode material measured at the current density of 1 mA/cm2. It is observed that the charge and discharge time of NiMoO4@MnCo2O4 composite electrode material is the longest, which corresponds to the maximum CV curve area of NiMoO4@MnCo2O4 in Figure 5c. By calculation, the specific capacitances of the three electrodes can reach 1656, 224 and 3000 mF/cm2. The specific capacitance of NiMoO4@MnCo2O4 is compared, as shown in Table 1, which is higher than that of some previous literatures [32,33,34,35,36]. The charging–discharging time of NiMoO4@MnCo2O4 composite electrode material is the longest, and the symmetry of the charging and discharging cycle indicates that the electrode has excellent reversibility. The capacitance performance is attributed to the nano urchin-like morphology of the material, which provides a larger electrolyte contact area. Therefore, the electrochemical properties of composite electrode material are improved. To further explore the charge transfer ability of the prepared electrodes, EIS measurements were carried out, as shown in Figure 5e. The inset exhibits that compared with two single electrodes, in the high frequency region, the NiMoO4@MnCo2O4 sample has a smaller semicircle arc and x-axis intercept, which represents the charge transfer resistance (Rct) and solution resistance (Rs), indicating that the composite has a faster ion-electron transfer rate at the electrode and electrolyte interface, and smaller intrinsic resistance. The corresponding Rs values of NiMoO4, MnCo2O4, and NiMoO4@MnCo2O4 are 0.91, 0.77 and 0.67 Ω, respectively. In the low frequency region, the composite material shows the higher straight-line slope, which accounts for faster electrolyte ion mobility. Cycling performance (10 mA cm−2) of the as-prepared electrodes is displayed in Figure 5f. Compared with NiMoO4 (75%) and MnCo2O4 (45%), NiMoO4@MnCo2O4 (96%) shows a better cycling lifespan after undergoing the charging–discharging process 10,000 times.
In order to study the application of NiMoO4@MnCo2O4 in SCs, the positive electrode and negative electrode of ASCs are NiMoO4@MnCo2O4 electrode and active carbon (AC) electrode, respectively. Figure 6 shows the electrochemical curves of the assembled device. Figure 5a shows the CV curves at the scanning rate of 100 mV/s. The voltage windows of the device are 1.1 V, 1.2 V, 1.3 V, 1.4 V, 1.5 V and 1.6 V, respectively. The shapes of all curves are nearly the same, indicating that the device can operate at 1.1 V–1.6 V and the maximum voltage window can reach 1.6 V at the same time. Figure 6b shows the CV curves of NiMoO4@MnCo2O4//AC at scanning rates of 5–100 mV/s. With the increase in scanning rate, the shapes of the CV curves increase, which is mainly attributed to the synergy between materials. These curves have obvious redox peaks, indicating that the asymmetric SCs have pseudocapacitance characteristics. Meanwhile, with increasing scanning rate, the integral area of the curves is enhanced. The GCD curves with different current densities are shown in Figure 6c, which indicates that the linear trend of the curve is obvious at high current densities. The voltage window is 1.5 V, and the surface capacitance of the device can be calculated according to the formula. When the current densities are 1, 2, 4, 8 and 10 mA/cm2, the surface capacitances are 58.53, 22.73, 12.13, 1.9 and 1.13 mF/cm2, respectively. Figure 6d shows the charge transfer characteristics of the prepared electrode studied by EIS test. The slope is larger in the low frequency region, indicating that the diffusion resistance of the assembled asymmetric SC is lower. The inset shows the Rs value is only 1 Ω. Figure 6e shows the long cycling test with 10,000 times at 10 mA cm−2 and coulombic efficiency. The capacity retention rate of the assembled asymmetric SC is 78.4%. The decrease in capacity may be due to the morphology damage caused by long-term redox reaction of electrode materials, which reduces the potential activity of the surface of the material. The coulombic efficiency of ASCs keeps nearly 100% during 10,000 charging–discharging tests. From Figure 6f, the Ragone plot offers an expression of the trend of the energy density with the corresponding power density. Importantly, the maximum energy density of the NiMoO4@MnCo2O4//AC device reaches 90.89 mWh/cm3 at the power density of 3726.7 mW/cm3, which is better than some reported devices [37,38,39,40,41].

4. Conclusions

A new type of NiMoO4@MnCo2O4 composite electrode material has been successfully prepared on nickel foam by the two-step hydrothermal method, and its phase structures, micromorphology and electrochemical properties are characterized and analyzed. Due to the synergistic effect between the NiMoO4 nano pompon-like structure and MnCo2O4 nano needle-like structure, the prepared nano urchin-like NiMoO4@MnCo2O4 core–shell nanostructure presents good pseudocapacitance properties. NiMoO4@MnCo2O4 samples show better electrochemical performance than single NiMoO4 or MnCo2O4 electrode materials, which exhibit a high specific capacitance of 3000 mF/cm2. After 10,000 cycles, the capacity retention rate is 96%. In addition, the NiMoO4@MnCo2O4//AC assembled device delivers a high energy density of 90.89 mWh/cm3 at a power density of 3726.7 mW/cm3.

Author Contributions

Conceptualization, Y.D. and N.B.; methodology, W.Y.; software, N.B. and S.L.; validation, W.Y., S.L. and J.X.; formal analysis, F.W.; investigation, R.Z.; resources, R.Z.; data curation, N.B.; writing—original draft preparation, Y.D.; writing—review and editing, W.Y.; visualization, X.S. and Z.W.; supervision, F.W.; project administration, J.X.; funding acquisition, J.X. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by [Jun Xiang] grant number [51702143], and the APC was funded by [the National Natural Science Foundation of China]. This research was funded by [Fufa Wu] grant number [51971106], and the APC was funded by [the National Natural Science Foundation of China]. This research was funded by [Jun Xiang] grant number [2021-MS-320], and the APC was funded by [the Natural Science Foundation of Liaoning Province]. This research was funded by [Rongda Zhao] grant number [2019-MS-171], and the APC was funded by [the Natural Science Foundation of Liaoning Province]. This research was funded by [Jun Xiang] grant number [LJKQZ2021145], and the APC was funded by [the Youth Project of Education Department of Liaoning Province].

Acknowledgments

This work was funded by the National Natural Science Foundation of China (NSFC, Grant Nos. 51702143 and 51971106), the Natural Science Foundation of Liaoning Province (Grant Nos. 2021-MS-320 and 2019-MS-171), the Youth Project of Education Department of Liaoning Province (No. LJKQZ2021145).

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Synthesis schematic of NiMoO4@MnCo2O4 composite electrode.
Figure 1. Synthesis schematic of NiMoO4@MnCo2O4 composite electrode.
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Figure 2. XRD patterns of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials.
Figure 2. XRD patterns of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials.
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Figure 3. (af) Microstructure of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials at different multiples; (g,h) TEM of NiMoO4@MnCo2O4 electrode material.
Figure 3. (af) Microstructure of NiMoO4, MnCo2O4 and NiMoO4@MnCo2O4 electrode materials at different multiples; (g,h) TEM of NiMoO4@MnCo2O4 electrode material.
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Figure 4. XPS diagram of NiMoO4@MnCo2O4 electrode material: (a) Full measurement spectrum; (b) Mn 2p; (c) Co 2p; (d) Mo 3d; (e) Ni 2p; (f) O 1s.
Figure 4. XPS diagram of NiMoO4@MnCo2O4 electrode material: (a) Full measurement spectrum; (b) Mn 2p; (c) Co 2p; (d) Mo 3d; (e) Ni 2p; (f) O 1s.
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Figure 5. Electrochemical tests of three electrode materials: (a) CV curves of NiMoO4@MnCo2O4; (b) GCD curves of NiMoO4@MnCo2O4; (c) CV curves of three electrode materials; (d) GCD curves of the three electrode materials; (e) EIS curves of the three electrode materials (inset is the high-frequency region); (f) Long cycle curves of the three electrode materials.
Figure 5. Electrochemical tests of three electrode materials: (a) CV curves of NiMoO4@MnCo2O4; (b) GCD curves of NiMoO4@MnCo2O4; (c) CV curves of three electrode materials; (d) GCD curves of the three electrode materials; (e) EIS curves of the three electrode materials (inset is the high-frequency region); (f) Long cycle curves of the three electrode materials.
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Figure 6. Electrochemical testing of NiMoO4@MnCo2O4 composite assembled devices: (a) Cyclic voltammetry curves under different voltage windows; (b) Cyclic voltammetry curves of different scanning speeds; (c) GCD curves with different current densities; (d) Impedance diagram (inset is the high-frequency region); (e) Cycling stability and coulombic efficiency; (f) Ragone plots.
Figure 6. Electrochemical testing of NiMoO4@MnCo2O4 composite assembled devices: (a) Cyclic voltammetry curves under different voltage windows; (b) Cyclic voltammetry curves of different scanning speeds; (c) GCD curves with different current densities; (d) Impedance diagram (inset is the high-frequency region); (e) Cycling stability and coulombic efficiency; (f) Ragone plots.
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Table 1. Electrochemical performance comparison of NiMoO4@MnCo2O4 with previous literatures.
Table 1. Electrochemical performance comparison of NiMoO4@MnCo2O4 with previous literatures.
MaterialsCapacityCurrent DensityElectrolyteCapacitance RetentionRef.
NiCo2O4/rGO/NiO2.644 F cm−21 mA cm−23 M KOH97.5% (3000 cycles)[32]
Fe2O3/Fe dendrite2.166 F cm−21 mA cm−21 M KOH90% (1000 cycles)[33]
NiCo2O4/C2.057 F cm−21 mA cm−22 M KOH81% (10,000 cycles)[34]
rGO/PPy0.807 F cm−21 mA cm−21 M H2SO478% (2000 cycles)[35]
C@MnNiCo-OH/Ni3S22.332 F cm−21 mA cm−23 M KOH89.45% (5000 cycles)[36]
NiMoO4@MnCo2O43 F cm−21 mA cm−23 M KOH96% (10,000 cycles)This work
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Di, Y.; Xiang, J.; Bu, N.; Loy, S.; Yang, W.; Zhao, R.; Wu, F.; Sun, X.; Wu, Z. Sophisticated Structural Tuning of NiMoO4@MnCo2O4 Nanomaterials for High Performance Hybrid Capacitors. Nanomaterials 2022, 12, 1674. https://doi.org/10.3390/nano12101674

AMA Style

Di Y, Xiang J, Bu N, Loy S, Yang W, Zhao R, Wu F, Sun X, Wu Z. Sophisticated Structural Tuning of NiMoO4@MnCo2O4 Nanomaterials for High Performance Hybrid Capacitors. Nanomaterials. 2022; 12(10):1674. https://doi.org/10.3390/nano12101674

Chicago/Turabian Style

Di, Yifei, Jun Xiang, Nan Bu, Sroeurb Loy, Wenduo Yang, Rongda Zhao, Fufa Wu, Xiaobang Sun, and Zhihui Wu. 2022. "Sophisticated Structural Tuning of NiMoO4@MnCo2O4 Nanomaterials for High Performance Hybrid Capacitors" Nanomaterials 12, no. 10: 1674. https://doi.org/10.3390/nano12101674

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