Qian Yangab,
Liubing Dongab,
Chengjun Xu*a and
Feiyu Kang*ab
aGraduate School at Shenzhen, Tsinghua University, Shenzhen 518055, China. E-mail: vivaxuchengjun@163.com; fykang@mail.tsinghua.edu.cn
bSchool of Materials Science and Engineering, Tsinghua University, Beijing 100084, China
First published on 25th January 2016
Graphene/MnO2 composites are introduced into activated carbon fiber felt (ACFF) to fabricate composite textile electrodes. Their micro-structure, electrical properties and electrochemical performance for supercapacitor applications in different neutral electrolytes (1 M NaNO3 and Ca(NO3)2 aqueous solutions) have been studied. The composite electrodes have similar pore features to original ACFF textiles, but show notably enhanced electrical and electrochemical performance. The composite textile electrodes show low electrical resistance, high specific capacitance (up to 1516 mF cm−2 in neutral electrolytes) and excellent cycling stability (no capacitance decay after 5000 charge–discharge cycles). Besides, electrochemical capacitance of composite textile electrodes in Ca(NO3)2 electrolyte is higher than that in NaNO3 electrolyte at low scan rates (1–5 mV s−1), but the situation is reversed when scan rates are higher than 10 mV s−1. Above all, the results show that our low-cost composite textile electrodes are high-performance in neutral electrolytes, which is helpful for developing large-scale energy storage devices.
In our previous work, activated carbon fiber felt (ACFF) was used to prepare multiscale carbon composite textiles and all-carbon compressible supercapacitors.34 However, the high-performance supercapacitors were achieved in a strong alkaline electrolyte (6 M KOH aqueous solution), this may increase risk of environmental issues.
In this work, GN/MnO2 composites prepared through self-reacting micro-emulsion method were introduced into ACFF to fabricate GN/MnO2/ACFF composite textile electrodes. Micro-structure, electrical property and electrochemical performance of the prepared GN/MnO2/ACFF composite electrodes in different neutral electrolytes were studied. The composite electrodes have similar pore features to original ACFF but better electrochemical performance. The neutral electrolytes also eliminate the risks and environmental issues of strong alkaline electrolytes. As a whole, our results show that the cheap ACFF, modified by GN/MnO2 composites, is capable to be used as supercapacitor electrodes in neutral electrolytes, which is helpful for developing supercapacitors with high performance and low cost.
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20 (or 20
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80)). Then 0.25 g 80GM (or 20GM) was dispersed in 50 ml deionized water by sonifier cell disrupting for 2 h. A wafer-shaped piece of ACFF, with diameter of 15 mm, was immersed in the 80GM (or 20GM) suspension and then freeze-dried. The obtained GN/MnO2/ACFF composite textile electrodes were denoted as 80GMC (or 20GMC). Weight of ACFF, 20GMC and 80GMC is 21.2 mg, 21.5 mg and 21.7 mg respectively.
The micro-morphology of the obtained GN/MnO2/ACFF composite textiles is displayed in Fig. 2. Fig. 2a and b show the SEM images of ACFF textiles. The images indicate that the original ACFF is fabricated by intertwining and overlapping carbon fibers, giving rise to a great quantity of holes in different sizes in the textiles. The abundance of holes makes ACFF textiles have high specific surface area and other excellent features of foams, such as bendability and compressibility. As observed in our experiments, ACFF textiles have ultrahigh water absorbability, which makes the impregnation process much simpler and quicker than other carbon materials.35 As shown in Fig. 2c–f, the GN/MnO2 composites are successfully introduced into ACFF. As can be seen, GN/MnO2 composites with different weight ratio of GN to MnO2 are attached on the surface of activated carbon fibers. However, when GN content increases, one distinct difference is that volume of nanofillers in 80GMC becomes much more than that in 20GMC. This volume increase makes GN aggregation more serious.
It should be noted that in the assembled full-cell supercapacitors, the electrodes are highly compressed. In this case, GN/MnO2 particles are pinned in local spaces encircled by carbon fibers, thus will not easily fall off the composite electrodes in supercapacitors.
Fig. 3a displays the electrical conductivity of textiles. As can be seen, conductivity is improved after introducing GN/MnO2 composites. The electrical conductivity of 20GMC and 80GMC is 35% and 114% higher than that of ACFF, respectively. Due to the short carbon fibers used in manufacturing ACFF, as well as its porous feature, the electrical conductivity of ACFF is not as high as other carbon fabrics.36,37 The added GN sheets could increase the channels for electron transport. For further consideration of the compressed state of electrodes in full-cell supercapacitors, we also measured the conductivity when the textile samples are manually pressed. It is obvious that the conductivity is higher than that at fluffy state. Although the pressure on the samples cannot be measured precisely, the data does indicate that those composite textiles can achieve higher conductivity when they are used as electrodes in full-cell supercapacitors.
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| Fig. 3 (a) Electrical conductivity of textiles at different states; (b) N2 adsorption/desorption isotherms of 80GMC at 77 K (the inset of (b) exhibits the pore size distribution). | ||
In previous work,34 the SBET, Vp and d of ACFF were measured to be 1528 m2 g−1, 0.65 cm3 g−1 and 1.73 nm respectively. Fig. 3b shows N2 adsorption/desorption isotherms of 80GMC. The type I isotherms indicate the micropore structure of 80GMC.38 The SBET, Vp and d of 80GMC are 1465 m2 g−1, 0.58 cm3 g−1 and 1.57 nm respectively. All of these figures are lower than their counterparts of original ACFF. Because the few-layered GN in our experiments has lower specific surface area than ACFF and the GN sheets can cover some pores of ACFF body materials. As shown in the inset of Fig. 3b, most pore sizes distribute under 2 nm, this reflects the micropore feature of 80GMC again.
Fig. 4a–f show CV curves of supercapacitors at scan rates of 1–20 mV s−1. For ANa and ACa, the quasi-rectangular shape of CV curves only exists at low scan rates (1–2 mV s−1), the deformation of CV curves becomes serious at high scan rates. This reflects the poor electrochemical performance of original ACFF. For 20Na and 20Ca, although the deformation of CV curves is not as serious as ACFF, the narrow areas of CV curves still indicate low capacitance of 20GMC. For 80Na and 80Ca, the rate performance is much better. When the scan rate increases, the CV curves of 80Na and 80Ca maintain rectangular well.
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| Fig. 4 CV curves at different scan rates of (a) ANa, (b) ACa, (c) 20Na, (d) 20Ca, (e) 80Na, (f) 80Ca; (g) areal capacitance of each sample calculated from CV curves. | ||
Fig. 4g displays areal capacitance of the single electrode at scan rates of 1–20 mV s−1. Compared with ACFF, the capacitance of 80GMC is largely enhanced while that of 20GMC is slightly improved. For example, the specific capacitance (Cs) of ACa, 20Ca and 80Ca at 2 mV s−1 is 763 mF cm−2, 918 mF cm−2 and 1516 mF cm−2 respectively. Besides, after introducing GN/MnO2 composites, the capacitance retention of textile electrodes is improved. The rate performance of 80GMC is much better than ACFF, while the improvement of 20GMC is negligible. For example, when the scan rate increases from 1 mV s−1 to 20 mV s−1, about 13.7%, 17.0% and 54.6% of Cs retains for ANa, 20Na and 80Na respectively.
Different electrolytes have different influence on each textiles. For ACFF and 20GMC, the Cs and Cs retention rate between NaNO3 and Ca(NO3)2 electrolytes do not show large distinction. Unlike ACFF and 20GMC, different electrolytes lead to distinguishing electrochemical performance of 80GMC. At low scan rates (1–5 mV s−1), 80Ca possesses higher Cs than 80Na, while at high scan rates (10–20 mV s−1), 80Ca possesses lower Cs than 80Na. Thus when the scan rate increases from 1 mV s−1 to 20 mV s−1, the Cs retention rate of 80Ca is 9.1% lower than that of 80Na. This variation mainly results from the different capacitance of MnO2 in NaNO3 and Ca(NO3)2 electrolytes. The capacitance of MnO2 in Ca(NO3)2 electrolyte is much higher than that in NaNO3 electrolyte at 2 mV s−1.39–41 Due to this reason, the capacitance of 80Ca is higher than that of 80Na at low scan rates (1–5 mV s−1). However, at high scan rates (10–20 mV s−1), the cation diffusion in electrolytes has a significant impact on the electrode capacitance: compared with Na+, Ca2+ has a lower diffusion coefficient and mobility, thus leading to a smaller capacitance of MnO2. Therefore, capacitance of 80GMC electrode in Ca(NO3)2 electrolyte is lower than that in NaNO3 electrolyte at high scan rates.
As shown in Fig. 5a–f, after introducing GN/MnO2 composites, more symmetric GCD curves, longer discharging time and smaller IR drops are achieved, especially for 80GMC. The IR drop reflects internal resistance of supercapacitors. For clear comparison between different textiles, the equivalent series resistance (ESR) is used and can be calculated according to equation:
Because the high resistance of ACFF and 20GMC makes their IR drops theoretically larger than 1 V at the scan rate of more than 2 mA cm−2, the charge–discharge process of them lasts less than 1 second and the Cs cannot be calculated from GCD curves. Therefore Fig. 5 only contains GCD curves and Cs of ACFF and 20GMC at 1–2 mA cm−2. As shown in Fig. 5g, Cs has been improved after introducing GN/MnO2 composites, and Cs of 80GMC is higher than that of 20GMC. Different electrolytes do not have much impact on the Cs of ACFF and 20GMC, but influence the electrochemical performance of 80GMC. The Cs of 80Ca is higher than that of 80Na at low current density, and decreases faster when the current density increases. So when the current density increases from 1 mA cm−2 to 20 mA cm−2, Cs of 80Na is retained about 43%, while that of 80Ca is retained about 23%. 80Na can achieve 25.4 μW h cm−2 of energy density with 895.2 μW cm−2 of power density at current density of 5 mA cm−2. This variation of Cs calculated from GCD curves is as same as that calculated from CV curves. Long-term cycling performance of 80Ca was also evaluated. As presented in Fig. 5h, there is no capacitance decay after 5000 charge–discharge cycles, demonstrating its excellent cycling stability.
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