Sol-gel synthesis of mesoporous Co3O4 octahedra toward high-performance anodes for lithium-ion batteries
Graphical abstract
Introduction
The need for high-performance rechargeable batteries in electronic devices and electrical/hybrid vehicles has led to dramatic development of lithium-ion batteries (LIBs). Graphite, the widely used commercial anode material, can not fulfill the increasing demand due to its low theoretical capacity (372 mAh g−1). Intensive research efforts have been devoted to developing new high-performance (high capacity, high power and high rate capability) anode materials for the next generation LIBs [1]. Among all the materials applicable for LIBs anodes, transition metal oxides have always been considered as the more promising candidate to replace the commercial graphite anode due to their high theoretical capacity (∼500-1000 mAh g−1) [2], [3], [4], [5], [6], [7], [8], [9]. For instance, as a promising anode material of LIBs, Co3O4 has recently been subjected to extensive research, owing to its low cost, high theoretical capacity (890 mAh g−1, calculated based on the conversion mechanism: Co3O4 +8Li+ + 8e− = 3Co + 4Li2O), good chemical/thermal stability, and environmental benignity [2]. Unfortunately, there remain major challenges for its practical use in LIBs, because Co3O4 electrode usually suffers from bad capacity retention upon cycling and poor rate capability. The electrode failure is mostly attributed to its intrinsic drawback of low ionic and electronic conductivity, which results in slow charge/discharge rate; and the significant volume change during repeated Li uptake and removal reactions leading to electrode pulverization. One generally accepted method to overcome these obstacles is to design composites of Co3O4 mixed with carbon materials or conductive substrates [5], [10], [11], [12], [13]. However, the additional conductive carbon or substrates will sacrifice the capacity of Co3O4, and lead to the emergence of undesirable interfaces and defects, causing lower electron transfer velocities and electrolyte diffusion efficiency. In addition, it is accepted that the electrochemical performance of Co3O4 strongly depends on its particle sizes, shapes and morphological structures. Indeed, it is indicated in many reports that the electrochemical performance of Co3O4 anode, including capacity and stability, will evidently be improved when the materials possess either small size, or appropriate pore-size distribution and special morphology, especially the combination of the above structural characteristics. In this regard, more and more efforts have been made to synthesize novel and diverse tailored nanostructured Co3O4 materials with excellent electrochemical performance [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26]. For instance, Wang et al. prepared a series of multishelled Co3O4 hollow spheres assembled with nanosheets, which exhibited excellent cycle performance and enhanced lithium storage capacity [18]. Du et al. synthesized porous Co3O4 nanotubes with good electrochemical properties [19]. Wang et al. prepared multishelled hollow Co3O4 microspheres as high-performance anode materials in LIBs [20]. All these reports have revealed that the hollow/porous structures can undoubtedly improve the electrochemical performance of Co3O4 materials. According to other literatures, the specific anisotropy morphologies such as nanocube [21], [22] and octahedral [23], [24] will also effectively improve the cyclability and reversible capacity of Co3O4 anode. But the well-defined porous Co3O4 with anisotropy structures for LIBs anodes have rarely been reported. So there is an emergency to develop a method for the synthesis of novel high-performance Co3O4 anode materials with porous anisotropy structures that possess the combined advantages of the above structural characteristics.
In the past few years, Pluromic type triblock copolymer (HO(CH2CH2O)106(CH2CH(CH3)O)70(CH2CH2O)106H) (F127) has been proved to be an efficient capping agent and template to synthesize porous metal oxide anode materials [27], [28], [29]. However, to the best of our knowledge, the anisotropy metal oxides with porous structure have not been reported previously. Herein, for the first time, we demonstrate a soft-chemical sol-gel route for the synthesis of nanosized porous Co3O4 octahedra with F127 as soft-template. The as-obtained unique architecture intrinsically possesses stable octahedral structure and porous features, which can alleviate the pulverization, buffer the drastic volume changes, and shorten the diffusion path of Li+/electron transport, thus leading to improved electrochemical performance.
Section snippets
Sample preparation
All regents are of analytical grade, and are obtained from Sinopharm Chemical Reagent Co., Ltd. They are used as purchased without further purification. The porous Co3O4 octahedra are synthesized via evaporation induced self-assembly (EISA) method. In the typical synthesis route of porous Co3O4 octahedra, 4.76 g CoCl2·6H2O and 1.42 g F127 are dissolved in 30 mL ethanol. The mixture is refluxed at 100 °C for 8 h. The obtained sol is aged at 40 °C for 2-3 days followed by aging at 65 °C for 10-12 days,
Characterization of samples
XRD is carried out to study the phase purity and crystal structure of the as-prepared Co3O4 (Fig. 1a). It is observed that all the diffraction peaks of the Co3O4 octahedra can be identified as cubic phase Co3O4 with space group Fd3 m. (JCPDS card No. 43-1003). No other impurity peaks such as CoO and Co2O3 are detected, showing the high phase purity of the product. And the intense and sharp diffraction peaks confirm the highly crystalline state. It is worth noting that the relative intensity of
Conclusions
In summary, mesoporous Co3O4 octahedra have been successfully prepared with a sol-gel technology with triblock copolymer F127 as the soft template. The simple sol-gel method seems to be scaled up easily for industrial production. The as-prepared sample shows typical octahedral shape with mesoporous structure. The pore-size distribution reveals a narrow distribution centered at 9 nm, resulting in a high BET surface area of 48.5 m2 g−1. Based on the high surface area, the mesoporous structures and
Acknowledgement
We gratefully acknowledge for the National Natural Science Foundation of China (21003079), Research Award Fund for Outstanding Middle-Aged and Young Scientist of Shandong Province (BS2011CL020), Natural Science Foundation of Shandong Province (ZR2011BM018) and Qingdao Project of Science and Technology (12-1-4-3-(20)-jch) for the financial support.
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