Bosi
Yin
ab,
Siwen
Zhang
ab,
Ke
Ke
a,
Ting
Xiong
b,
Yinming
Wang
b,
Boon Kiang David
Lim
b,
Wee Siang Vincent
Lee
*b,
Zhenbo
Wang
*a and
Junmin
Xue
*b
aMIIT Key Laboratory of Critical Materials Technology for New Energy Conversion and Storage, School of Chemistry and Chemical Engineering, Harbin Institute of Technology, No. 92 West-Da Zhi Street, Harbin 150001, China. E-mail: wangzhb@hit.edu.cn
bDepartment of Materials Science and Engineering, National University of Singapore, 117576 Singapore, Singapore
First published on 2nd October 2019
Organic compounds, such as polyvinylidene fluoride (PVDF), have been widely used as a binder in battery electrode preparations. While such an approach does not have a significant impact on the performance of the batteries that utilize low valence ions, such as the Li ion battery (LIB), the diffusion of high valence ions (such as Zn2+) will be severely impaired. This will be especially pronounced if the polymeric binder contains highly electronegative atoms, such as fluorine. The high charge density ions, such as Zn2+, tend to adsorb onto these electronegative atoms, thus the mobility of these ions across the material is inevitably affected. As such, it becomes highly necessary to consider the binder-free electrode architecture when designing a high rate performing and cycling-stable zinc ion battery (ZIB) cathode. Herein, this work demonstrates an improved Zn ion battery by adopting a freestanding electrode. The obtained V2O5/CNT paper electrode delivers a specific capacity of 312 mA h g−1, while achieving a respectable 75% retention in capacity after increasing the current density by 10-fold. Furthermore, excellent cycling stability is recorded with 81% capacity retention after 2000 cycles at 1.0 A g−1. Thus, this work clearly demonstrated that the freestanding electrode is a promising approach for high valence ion batteries.
With the recent elevated interest in V2O5 as a zinc ion battery (ZIB) cathode, the magnitude of this sluggish diffusion across the material with an organic binder is greatly increased. Even though the Zn2+ diameter is close to that of Li+, it possesses a higher charge density that can pose a polarizing effect on the material during the diffusion process. Due to the high charge density, Zn2+ tends to be adsorbed to the C–F bonds in the polarizing polymeric binder. This consequently reduces the mobility of Zn2+ and ultimately leads to a poor rate performance and large initial irreversible capacity loss. Thus, it becomes highly necessary to avoid the use of polymeric binders to ensure minimal disruption to the mobility of Zn2+ during the charging/discharging process. In order to achieve this, interest in a freestanding electrode should be renewed, especially for high valence ion batteries such as ZIB. A typical strategy is to introduce a carbonaceous scaffold that can offer structural integrity for the metal oxides, while simultaneously contributing to the overall conductivity of the electrode. As such, one of the favorite carbon monoliths is graphene paper. However, due to its layer-by-layer arrangement, the extent of electrolyte infiltration becomes a challenge as the electrolyte can only enter the material in the planar direction. In order to address such a limitation, carbon nanotube (CNT) paper would hence become an appealing scaffold material for V2O5 due to its random stacking arrangement, which offers better electrolyte infiltration from all directions.
Herein, this work reports a significant electrochemical performance enhancement (especially the rate performance and cycling stability) by adopting a freestanding V2O5/CNT composite paper (VCP) as the ZIB cathode. As a polymer binder is not used in the electrode preparation, the V2O5/CNT paper delivers a specific capacity of 312 mA h g−1, while achieving a respectable 75% retention in capacity after increasing the current density by 10-fold. It is interesting to note that its counterpart with an organic binder demonstrated a poor rate performance of 36% at the same current density. Furthermore, our binder-free composite papers exhibit superior cycling stability, as compared to the counterpart with an organic binder. This work demonstrates a significant progress of the binder-free electrode in achieving excellent electrochemical performance and its potential for high valence ion batteries.
Fig. 2a presents a typical scanning electron microscopy (SEM) image of the VCP. Under the SEM observation, the VCP electrode exhibited a 3-dimensional porous structure that comprised a continuous carbon nanotube network and V2O5 particles. Fig. 2(b–e) show the cross-sectional image of VCP from energy dispersive X-ray spectra (EDX). The thickness of the paper electrode was about 200 μm and the EDX results indicated a uniform distribution of V and C elements across the entire cross-section, which confirmed an even distribution of V2O5 in the CNT conductive network. Fig. 2f is an image of the three-dimensional white light interference surface topography. The appearance of a large number of blue areas confirmed the existence of 3D channels, which were beneficial to the zinc ion transportation. Transmission electron microscopy (TEM) was employed to further study the morphology of the paper electrode. Based on Fig. 2g, the presence of the CNTs and V2O5 particles further confirmed the successful preparation of a freestanding V2O5/CNT paper. The CNT and single-crystalline V2O5 (according to the SAED pattern in Fig. 2h) were entangled together to form a continuous electron conducting network.
To compare the electrode performance with/without a binder, electrochemical testing was conducted for the pristine V2O5 powder (VP), the CNT/V2O5 mixed powder (CVMP) and freestanding V2O5/CNT composite paper (VCP). The CV curves of these three electrodes are presented in Fig. 3a. Under the same scan rate of 0.2 mV s−1, the integrated area of the CV curves for VCP was larger than those of the two control electrodes, suggesting a larger capacity. The cyclic voltammetry (CV) curves of the VCP electrode conducted from 0.2 mV s−1 to 1 mV s−1 were recorded and are presented in Fig. S1a.† Two reduction peaks (around 0.4–0.5 V and 0.8–0.9 V) and two oxidation peaks (around 0.9–1.0 V and 1.2–1.3 V) were observed, which were caused by the zinc ion intercalation/deintercalation during the discharge/charge processes. The galvanostatic charge/discharge (GCD) measurements of VCP were performed in the range of 0.2–1.7 V (as shown in Fig. 3b). An average specific discharge capacity of 312 mA h g−1 was recorded at a current density of 1 A g−1. Even at a higher current density of 10 A g−1, a good specific capacity of 232 mA h g−1 was achieved. The areal and volumetric capacities at various current densities are also shown in Fig. S2a.† An areal capacity of 2.2 mA h cm−2 and a volumetric capacity of 109.2 mA h cm−3 can be obtained at a current density of 1 A g−1. The corresponding energy/power density is presented in Fig. 3c and the areal/volumetric energy/power density are also given in Fig. S2b.† The VCP electrode exhibited an energy density of 891 W h kg−1 at a power density of 278 W kg−1 (Fig. 3c). A maximum power density of 8871 W kg−1 could be reached. The excellent rate capability was further reflected in the Ragone plots by comparison with some recent reports (see ESI Table 1†).22–29 The rate performances of the VP, CVMP and VCP are shown in Fig. 3d. The VCP exhibited superior rate capability with average specific discharge capacities of 312, 303, 281, 253 and 235 mA h g−1 at current densities of 1, 2, 4, 8 and 10 A g−1, respectively. Recently, some studies also demonstrated that structural water could function as a charge screening media in the redox reactions. The H2O-solvated Zn2+ possesses a largely reduced effective charge and thus, reduced electrostatic interactions with the V2O5 framework, effectively promoting its diffusion.24 Based on Fig. 3d, the capacity retention of these three electrodes were calculated and is shown in Fig. 3e. For the VCP electrode, the capacity retention is 75% (at 10 A g−1) of the initial value (at 1 A g−1), while only 42% retention was calculated for CVP and a poor 36% retention for VP. When the current density was decreased from 10 A g−1 to 1 A g−1, the capacity of VCP was fully recovered, which was superior to the 52% and 79% capacity recovery for VP and CVMP, respectively. It was believed that the capacity loss in VP and CVMP was due to the presence of the organic binder, which generated a strong electrostatic attraction with the highly positively charged zinc ions, and thus these electrostatically “glued” zinc ions could not be completely extracted. The capacity fading of electrodes with the polymeric binder could be clearly seen by comparing the discharge capacity of the second and third cycles (Fig. S3†). On the other hand, the capacity loss of the VCP electrode was negligible. To demonstrate the high reversibility of VCP, all three electrodes were cycled at a low current density of 1.0 A g−1 to evaluate the long-term cycling stability (as shown in Fig. 3f). After 2000 cycles, the VCP electrode retained 81% of its initial capacity with ca. 99% coulombic efficiency for all the cycles, suggesting an excellent cycling life. However, the other two powder electrodes demonstrated 80% capacity retention under 250 cycles. The structure and morphology of the V2O5/CNT paper after a long-term cycling process was also an important factor toward the stable electrochemical properties of the Zn ion batteries. After 2000 cycles, compared with the original XRD result (Fig. S4a†), similar peaks were revealed without an obvious change. The morphology of the V2O5 blocks in the CNT network could still be clearly distinguished in Fig. S4b.†
An ex situ XRD technique was employed to explore the structural changes of VCP during the discharge/charge process (Fig. 4a). When the electrode was discharged to a lower voltage, the intensity of the characteristic peaks became weaker, which was ascribed to the intercalation of Zn2+ ions from the layered structure and resulted in lattice distortions. It could be seen that the location of the diffraction peaks corresponding to the (001), (101), and (110) lattice planes were consistent with those in the initial sample, indicating that the sample was still a layered structure of V2O5 after the charge–discharge process.30 The valence state changes of vanadium are also presented in Fig. 4b. When discharged to 0.2 V, the V 2p3/2 peaks were split into two peaks. The reduction in vanadium happened along with the insertion of Zn2+. Then, the vanadium was further oxidized back to its original state during the charging process.31 The SEM images under different potentials are shown in Fig. S5a to S5f.† The morphology of the V2O5/CNT paper remained the same after the discharging–charging process. In order to investigate the mechanical property of our freestanding film electrode, we have performed a simple mechanical fatigue test, as shown in Fig. S6.† After 100 bends, the freestanding film remained intact without flaking. Ultimately, we assembled a flexible zinc ion battery using VCP as the cathode, zinc foil as the anode, filter membrane as the separator and 1 M ZnSO4 aqueous solution as the electrolyte (Fig. 4d and e). The digital watch and white LED were powered by two charged zinc batteries connected in series (as shown in Fig. 4f and inset of Fig. 4g). The unchanged shape of the CV curves under different bending angles also verified the stable performance of this flexible device (Fig. 4g). This paper electrode will open up new opportunities for advanced energy storage systems taking advantage of large mass-loading, flexibility, and long cycling ability.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9nr07458a |
This journal is © The Royal Society of Chemistry 2019 |