Elsevier

Solid State Ionics

Volume 353, 1 October 2020, 115376
Solid State Ionics

Study on low-temperature performances of Nb16W5O55 anode for lithium-ion batteries

https://doi.org/10.1016/j.ssi.2020.115376Get rights and content

Highlights

  • The performances of Nb16W5O55 anode at various temperatures are studied.

  • The charge-transfer impedance and Li+ diffusion coefficient are the key factors.

  • The cyclic stability and structure are almost unaffected by operation temperatures.

Abstract

Niobium tungsten oxide Nb16W5O55 is a competitive anode for lithium-ion batteries, while seldom research on low-temperature electrochemical properties. In this paper, Nb16W5O55 is synthesized by solid phase reaction and the effects of operation temperature (25, 0 and −20 °C) on the coulombic efficiency, cycling stability, rate capacity and crystal structure are studied in detail. At 25 °C, Nb16W5O55 electrode can give good cycling stability of 184 mAh g−1 after 404 cycles and rate capacity of 101 mAh g−1 at 4000 mA g−1. By contrast, the electrochemical properties decrease obviously at subambient temperatures. Electrochemical impedance spectroscopy reveal that the sharp increase of the charge-transfer impedance and the decrease of the solid-phase Li+ diffusion coefficient are the essential factors leading to the deterioration of low temperature performances. However, the low temperature mainly affects specific capacities and rate performances, but has little effect on cyclic stability and crystal structure of Nb16W5O55 electrode, indicated by ex-situ X-ray diffraction analysis. These results provide some new insights for the practical application of Nb16W5O55 anode.

Introduction

At present, graphite is the main anode for commercial lithium-ion batteries (LIBs). The lithium intercalation potential of graphite, however, is similar to that of lithium metal plating, which may lead to the formation of lithium dendrites and safety concerns. Additionally, the low diffusion coefficient of Li+ in graphite inhibits the rapid Li+ migration under high current charging/discharging, resulting in unsatisfactory rate performances [[1], [2], [3], [4]]. As a strong competitor, Li4Ti5O12 anode with high intercalation potential (~1.55 V) can effectively avoid the formation of lithium dendrites and greatly improve battery safety. Moreover, its spinel structure can ensure the efficient Li+ transportation, and has zero-strain characteristics, thus obtaining excellent cycle stability and rate performance. Nevertheless, the lower theoretical capacity (175 mAh g−1) restricts the large-scale application of Li4Ti5O12 anode [[5], [6], [7], [8], [9]]. In order to solve these problems, the development of new anode materials is necessary. Recently, tungsten niobium oxides, such as Nb14W3O44 [10], Nb4W7O31 [11], Nb8W9O47 [12], Nb60WO153 [13], Nb16W5O55 [14], Nb18W16O93 [15], Nb12WO33 [16] and Nb12W11O63 [17], have attracted extensive attention. Niobium tungsten oxides deliver a high intercalation potential (1.57– 1.70 V) similar to Li4Ti5O12 and more redox electron pairs (Nb5+/Nb4+, Nb4+/Nb3+, W6+/W5+ and W5+/W4+) during the cycles, demonstrating an improved safety and higher specific capacity.

Among the niobium tungsten oxide anode materials, Nb16W5O55 reported by Grey’ group exhibits outstanding performances with high energy density, enhanced structural stability and convenient synthesis [14]. Nb16W5O55 belongs to monoclinic structure, consisting of corner-shared NbO6 octahedron and WO6 octahedron arrange into ReO3 configuration, and Nb/W atoms in the center of octahedron are arranged randomly. Each layer plane of Nb16W5O55 is composed of a large number of shear plane units, which contains 4 (wide) × 5 (long) MO6 (M = Nb, W) octahedrons. The layered structure formed between the shear planes is beneficial to lithium ion storage and transportation. During the lithium intercalation, Nb16W5O55 can produce four redox reactions with theoretical capacity of 343 mAh g−1 and structural stability of only 5.5% expansion. As the voltage range is 1.0– 2.5 V, the initial reversible capacity and coulomb efficiency is 226 mAh g−1 and 98%, respectively. Even the current density increases to 6860 mA g−1, the reversible capacity can be maintained 85 mAh g−1, which clearly surpasses that of Li4Ti5O12 [[7], [8], [9]]. Though Nb16W5O55 is inferior to graphite anode in terms of gravimetric capacity and voltage platform, the characteristics of high tap density prompt Nb16W5O55 (2.61 g cm−3 vs 0.72 g cm−3 of graphite [18]) to exhibit an overwhelming volumetric energy density at high current density, indicating a broad prospect for Nb16W5O55 in the development of fast-charging power LIBs.

In addition to the excellent electrochemical performances of Nb16W5O55 anode at room temperature, its low temperature performance should also perform well, however, which has received relatively little attention. Herein, Nb16W5O55 anode is prepared by solid phase reaction and the characteristic properties are analyzed by X-ray diffraction (XRD), Raman spectrum, scanning electron microscopy (SEM), X-ray photoelectron spectroscopy (XPS), and inductively coupled plasma (ICP-AES). Nb16W5O55 anode exhibits high initial coulombic efficiency (92.6%), improved cycling stability (184 mAh g−1 after 404 cycles) and rate performance (101 mAh g−1 at 4000 mA g−1) at 25 °C. Moreover, the low-temperature (0 and − 20 °C) behaviors of Nb16W5O55 anode are studied in detail. It delivers the disappointing performances with the specific capacities of 38 and 18 mAh g−1 at 4000 mA g−1 under 0 and − 20 °C, respectively, which is mainly due to the high charge-transfer impedance and low Li+ diffusion coefficient. Except for the lower capacity, however, Nb16W5O55 anode displays consistent cyclic (retains 92.8% capacity after 404 cycles at 0 °C) and structural stability (no phase changed) even at −20 °C. These results need to be considered in the practical application of Nb16W5O55 anode for LIBs.

Section snippets

Sample preparation and characterizations

For preparation of Nb16W5O55 sample, stoichiometric amounts of WO3 (99.0%, Sinopharm) and Nb2O5 (99.99%, Sinopharm) were mixed, further precalcined at 700 °C for 12 h and finally calcined at 1160 °C for 12 h in air. The structure was investigated by XRD (Cu Ka radiation, Bruker D8) and Raman spectrum (532 nm, Lab-RamHR), corresponding Rietveld refinement was conducted by GSAS program. The microstructure and elemental distributions were examined by SEM (HITACHI, SU8020). The valence and content

Results and discussion

XRD pattern of as-prepared sample is shown in Fig. 1a, in which the high intensity diffraction peaks can be well indexed to monoclinic Nb16W5O55 phase (JCPDS No. 44-0467) with the C121 space group, revealing that the highly crystalline Nb16W5O55 is obtained [14,19]. The crystal structure of Nb16W5O55 sample is analyzed by Rietveld refinement (Rwp = 10.49%, Rp = 8.03%, χ2 = 1.88) and the detailed atomic parameters are tabulated in Table 1, corresponding cell parameters are a = 29.6678 Å,

Conclusions

In conclusion, Nb16W5O55 anode is synthesized by solid state reaction, and electrochemical performances at room and low temperature are systematically investigated by CV, galvanostatic charge-discharge and EIS techniques. The Nb16W5O55 anode exhibits high cycling stability and rate capability at 25 °C, while the obvious deterioration of electrochemical performances occur at low temperature. Combining ex-situ SEM and XRD characterization, the impact of low temperature on the Nb16W5O55 anode is

CRediT authorship contribution statement

Xiao-Hang Ma:Conceptualization, Writing - original draft, Writing - review & editing, Visualization, Funding acquisition.Xian Cao:Validation.Yuan-Yuan Ye:Resources.Fan Qiao:Resources.Men-Fa Qian:Data curation.Yi-Yong Wei:Formal analysis.Yao-Dong Wu:Software.Zhen-Fa Zi:Methodology, Supervision, Funding acquisition.Jian-Ming Dai:Methodology, Supervision.

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgments

This research was financially supported by the NSFC (No. U16321611), the Natural Science Foundation of Anhui Province (No. KJ2019A0723, 1808085QE154, 1808085JQ13 and gxgnfx2019024), and the Research Funds for Hefei Normal University (No. 2019ylkc02, 2019GDTC06, 201814098170, 201914098201).

References (30)

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