用于超級電容器的層狀Co3O4/Ti納米片柔性電極及其低電荷轉(zhuǎn)移電阻

韓丹丹 趙 遠(yuǎn) 申 燁 丁元生 程振玉 景曉燕 張學(xué)儀

（1吉林化工學(xué)院化學(xué)與制藥工程學(xué)院，吉林 132022）

（2哈爾濱工程大學(xué)材料科學(xué)與化學(xué)工程學(xué)院，哈爾濱 150001）

（3吉林中西醫(yī)結(jié)合醫(yī)院，吉林 132012）

0 Introduction

Theurgent demand for wearable electronic devices has attracted increasing interests in flexible and lightweight energy storage devices[1-2].Supercapacitors emerge from other candidates because of the high power density,charge/discharge rate and efficient cycle stability[3-4].In accordance with the energy storage mechanisms,supercapacitors can be divided into electrochemical double-layer capacitors （EDLCs）which store energy physically at the electrodes surface within electrolyte and pseudocapacitors which store energies by fast redox reactions[5-7].Conventional supercapacitors are usually based on activated carbon electrodes which have high power density,long cycle life,and rapid charging/discharging rate[8].However,among the series of pseudocapacitors electrode materials for supercapacitor applications,transition metal oxides are widely studied due to variable oxidation states of metal ions which facilitate redox transitions and higher charge storage within the potential range of water decomposition[9-10].Generally,the metal oxides with the following characteristics could be a super candidate as supercapacitor electrode materials[11-16]:（1）Metal may coexist in two or more oxidation stateswithout phase transition in a continuous range and without modification of an irreversible three-dimensional structure; （2）The transition metal oxide should be electronically conductive; （3）The protons can be freely released and inserted into the oxidation lattice during the redox.Co3O4is considered to be one of the better alternate materials because of their rich oxidation states,low cost,high theoretical specific capacitances, and environment friendly nature.Since charge storage is directly related to surface properties,controlling the surface morphology of electrode materials has a great influence on their electrochemical properties.Although various structures have been demonstrated to be quite feasible for high performance and stable electrodes,the design of the layered structure plays a more critical role for high performance supercapacitor applications, because layered structures can be flake-off resistant and better tolerant to high rate redox reactions[17-21].

As a method to improve the conventional process,the in situ growth of active materials on a flexible substrate has attracted extensive attention,because they can be used as the finished electrode directly[22-23].As expected,this method improves the performance of the electrodes.Some progress has been made in foam,fiber and paper substrate.The general method of fabricating 3D arrays structures involves chemical preparation of Co3O4and assembly of various architectures[24-26].These processes,however,always bring in some defects and impurities resulting in poor conductivity.

Based on the survey above,a convenient and scalable hydrothermal based approach to deposit layered Co3O4nanosheets directly grown on flexible titanium mesh substrate as a binder-free electrode for low ion-transfer resistance has been designed.The layered Co3O4was composed of uniform rectangular and micrometer length 2D flakes.These highly layered Co3O4materials with nanostructures were functioned directly as supercapacitors electrodes without further treatment delivered lower ion-transfer resistance and good cycle stability.

1 Experimental

1.1 Synthesis procedure

All reagents were purchased from the Aladdin Chemical Reagent Company and were used without further purification.Generally,2.5 mmol Co（NO3）2and 12.5 mmol CO（NH2）2were dissolved in 30 mL distilled water with constant stirring to obtain a settled solution.Then,the pre-treated titanium mesh （1 cm×1 cm）and the settled solution were transferred into a Teflon-lined stainless steel autoclave.The stainless steel autoclave was maintained at 95℃for 8 h,and then cooled to room temperature.Finally,the samples were treated at 350℃for about 3.5 h.

1.2 Characterizations

The crystalline information of the as-prepared products was analyzed by X-ray diffraction（XRD,DX-2700 Dandong Haoyuan,Cu Kα,λ=0.154 05 nm,operating voltage=40 V,operating current=30 mA,the scan rate=0.33°·s-1,2θ=30°～85°）.The structural investigation of the layered Co3O4samples were determined using a scanning electron microscope（SEM,JSM-6480A,Japan Electronics,operating voltage=20 V）and high-resolution transmission electron microscopy （HRTEM,FEI,Tecnai G2F20,120 kV）.

1.3 Electrochem ical measurements

The electrochemical tests were performed by a three-electrode system with a 2.0 mol·L-1KOH electrolyte.Pt foils and a saturated calomel electrode （SCE）were used as the counter electrode and the reference electrode.The loaded weight of the active materials was controlled to be approximately 3.1 mg·cm-2.

The specific capacitance （Cs）of the Co3O4sample was calculated from the cyclic voltammetry （CV）curves according to Equation （1）[10,27]:where I is the current （A）,m is the mass of active material（g）,v and d V are the potential scan rate and the differential of potential.Where I is applied current density （A）,m is the mass of the sample （g）, Δt is discharge time （s）,and ΔV is operating potential （V）.

where I is the current （A）, m is the mass of active material （g）, v and dV are the potential scan rate and the differential of potential.

Where I is applied current density （A）, m is the mass of the sample （g）, Δt is discharge time （s）, and ΔV is operating potential （V）.

2 Results and discussion

2.1 Structural investigation

Fig.1 illustrates the fabrication procedure of the layered Co3O4nanosheets on Ti mesh.Firstly,urea broken down into HCO3-,and then the major precursor of Co2（OH）2CO3were prepared by the reaction of Co2+with CO32-and OH-in the mixed solution.The purple precursor on Ti mesh appeared after the reactions and rinsed with distilled water several times.After calcinations at 350℃for 3.5 h,layered Co3O4electrode was obtained.The advantage of the integrative Co3O4directly grown on flexible substrate is that it can avoid the traditional volume loss caused by the process of mixing active materials with conductive additives and polymer binder[30-31].

Fig.1 Typical fabrication process of flexible layered Co3O4 nanosheet electrodes

The XRD pattern of the layered Co3O4nanosheets on Ti mesh is shown in Fig.2.Except for some diffraction peaks originating from Ti mesh,the welldefined peaks of The peak of Co3O4nanosheet at 31.3°,36.9°,44.8°,59.4°,65.2°and 82.6°could be indexed to （220）, （311）, （400）, （511）, （440）and （444）plane of the layered Co3O4crystalline,respectively,which is in accord with the standard XRD pattern of cubic Co3O4（PDF No.42-1467）.No other crystalline phases could be detected,suggesting that the high purity of the obtained Co3O4nanosheet.

Fig.2 XRD pattern of the layered Co3O4 nanosheet array on Ti mesh

The morphologies of the layered Co3O4nanosheets on Ti mesh were investigated by SEM.It was clear that Co precursor could be grown uniform ly at large scale on skeletons of Ti mesh （Fig.3）.The sample showed the layered morphology with well-arranged 2D microsheets.A detailed observation revealed that the bunches of Co3O4were vertically and regularly distributed but leaving a highly open interspace which endowed fast transport of the electrolyte.These nanosheets had an edge length of 2～3 μm and a uniform thickness of less than 20 nm.

Fig.3 （a,b）Low and （c,d）high magnification SEM images of Co3O4 sample

Fig.4 （a,b）Low-magnification TEM images of the mesoporous Co3O4 nanosheet;（c,d）HRTEM images of the edge part of the Co3O4 nanosheet

The detailed structure of the single Co3O4nanosheets was further investigated by TEM,as shown in Fig.4.It can be seen that Co3O4nanosheet possessed the abundant pores on its surface,which could be attributed to the gas ejection during the themal transformation from precusor to Co3O4nanosheets.The nanosheet was composed of numerous interconnected nanoparticles with diameters of 5～10 nm,and showed a mesoporous structure with a pore size of 2～5 nm.Accordingly,the electrolyte can easily pass in and out of the porous structure and transfer between the layers,forming a shorter diffusion path.The high-resolution TEM （HRTEM）image in Fig.4d revealed the interplanar spacing of～0.24 and ～0.29 nm,corresponding to the （311）and （220）plane of Co3O4given in the standard files.Moreover,the SEM images further proved the flexible nature of the Ti mesh substrate,as shown in Fig.3（b）.

2.2 Electrochem ical measurements

In order to evaluate the electrochemical characteristics of the layered Co3O4samples,the electrochemical measurements were carried out using a three-electrode system in a 2 mol·L-1KOH solution.

Fig.5a shows the CV curves of the layered Co3O4electrode at different scan rates of 5～100 mV·s-1.One pair of redox peaks at various scan rates was clearly observed.Well-fined redox peaks were clearly displayed in all the curves,suggesting the capacitive characteristics of Faradic redox reaction in the electrodes.The possible redox reactions might be described as follows[32]:

The Csat different scan rates in the CV measurements were calculated using the Equation （1）（Fig.5b）.At scan rates of 5～100 mV·s-1,the Csfor layered Co3O4samples are found to be 64～49 F·g-1.The higher Csand～25%capacitance loss when the scan rate increased from 5 to 100 mV·s-1attributee to the larger electroactive surface area of the layered morphology and easy accessibility of OH-ions for highly feasible redox reactions.Galvanostatic constant current charge-discharge curves at various current densities at the electrochemical window of 0～0.45 V are shown in Fig.5c.The linear slopes and presence of triangular symmetry with respect to the charging/discharging curves confirmed a good electrochemical performance.At a current density of 0.1 A·g-1,Csof Co3O4sample was 67 F·g-1,and found that the Csdecreased with increasing current density.The decrease in Csat high current densities was due to an increase in the internal diffusion resistance within the pseudoactive material,which decreased the efficiency of utilization of the active material.

Fig.5 （a）CV curves of layered Co3O4 nanosheet electrode at different scan rates;（b）C s as a function of scan rate;（c）Charge and discharge curves of samples at different current densities;（d）C s as function of discharge current densities of layered Co3O4 electrode

To further evaluate the electrochemical behavior of the electrode material,electrochemical impedance spectroscopy （EIS）was also collected with a frequecy ranging from 100 kHz to 0.1 Hz at open circuit potential,and the corresponding Nyquist plots are exhibited in Fig.6.The inset in Fig.6 was the equivalent circuit fitted by ZSimpWin.The EIS data can be fitted by internal resistance （Rs）,charge transfer resistance （Rct）,double layer capacitor （Cdl）,Warburg impendence （Zw）,and Cpsfor the limited pseudofaradic reaction,as shown in the inset in Fig.6.In the high frequency region,the spectra of layered Co3O4electrode showed a semicircle,and the intercept of arc on the x-axis was represented the Rswith a value of 3.09Ω,which included intrinsic resistance of ionic resistance of electrolyte,and contact resistance with current collector.The Rctrelated to the semicircle was estimated as 0.29Ω,which demonstrated much lower resistance to many other Co3O4electrode reported before （Table 1）[19,33-40].The high-rate capability and excellent reversibility were attributed to the following reasons[41-42]: （1）layered structures can be resisted structural collapse and spalling,which better tolerant to high rate redox reactions during the electrochemical process; （2）layered morphology provided favourable long-range, uniform, stable and smooth oxide conductivity paths; （3）proper porosity of the material is beneficial to the penetration of electrolyte,thus reducing charge transfer resistance.

Fig.6 Nyquist plots of layered Co3O4 nanosheet and Ti mesh

The cycle life is another important factor for evaluating the performance of supercapacitor.The cyclic performance of layered Co3O4sample for 1 000 cycles at current density of 100 mA·g-1is presented in Fig.7.

During the 1 000 charge-discharge processes,the corresponding coulombic efficiency approached 98%,which confirmed that the material possesseed good reversibility.A capacitance retention of 91.8%was observed after 1 000 charge-discharge cycles,indicating the excellent stability of the 2D porous layered nanosheets electrode.

Table 1 R ct for different structured metal oxide

Fig.7 Long cycle performance of Co3O4 nanosheet arrays measured at the current density of 100 mA·g-1

3 Conclusions

In summary,layered Co3O4on Ti mesh have been synthesized by a facile route as flexible supercapacitor electrode.The prepared layered Co3O4nanosheets possessed long-range 2D conductivity paths with high surface area and porous nature,which exhibited excellent electrochemical performance towards the EIS,such as lower charge transfer resistance （Rct）.This layered Co3O4with the excellent structural and electrochemical stability with 98% coulombic effeciency may be very useful for the flexible electrode for the energy storage devices.