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1.
以Ni(NO3)2·6H2O,Co(NO3)2·6H2O,Mn(CH3COO)2·4H2O,LiOH·H2O为原料,采用NaOH-Na2CO3共沉淀的方法,在空气中合成了三元层状锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2.采用XRD研究了所合成材料的结构.考查了不同烧结温度对材料电化学性能的影响.结果表明,所合成的材料具有典型的α-NaFeO2层状结构特征,900℃下合成的材料具有最优的循环性能,初始放电容量为169.4mAh/g,初次库仑效率为83.2%,且20次循环后,容量保持率达到96.3%.  相似文献   

2.
以氢氧化钠为沉淀剂,采用共沉淀法合成了Ni1/3Co1/3Mn1/3(OH)2前驱体,前驱体和LiOH·H2O充分混合高温烧结制备了锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2.采用X射线衍射(XRD)、扫描电子显微镜(SEM)和电化学性能测试对LiNi1/3Co1/3Mn1/3O2正极材料的结构、微观形貌及电化学性能进行了表征.XRD结果表明,所合成的LiNi1/3Co1/3Mn1/3O2物相单一无杂相,具有标准的α-NaFeO2型层状结构.SEM测试显示,颗粒粒度均一,粒径大约在0.5μm,粒径分布窄.以20mA/g电流密度放电,充放电电压在2.8~4.4 V之间,首次放电比容量达到181mAh/g,80次循环之后放电比容量仍然保持在172mAh/g;循环伏安测试显示,LiNi1/3Co1/3Mn1/3O2反应中主要是Ni2 /Ni4 、Co3 /Co4 2个电对在起作用,锰的价态保持不变,起到支撑结构的作用.  相似文献   

3.
采用溶胶凝胶法合成了不同温度下的锂离子电池正极材料LiNi0.05Mn1.95O3.95F0.05.使用X射线衍射对合成材料的结构进行了表征.考察烧结温度对其结构及电化学性能的影响.随着烧结温度的升高,尖晶石型结构越来越完整,初始放电比容量增大,但循环性能却逐渐变差.在750℃T烧结温度12h得到了性能较好的LiNi0.05Mn1.95O3.95F0.05,首次放电比容量为109.7mAh/g,50次循环后,其放电比容量仍保持在101.6mAh/g,适合作为锂离子电池的正极材料.  相似文献   

4.
锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2的合成及性能   总被引:1,自引:0,他引:1  
采用氢氧化物共沉淀法合成了LiNi1/3Co1/3Mn1/3(OH)2前驱体,然后以Ni1/3Co1/3Mn1/3(OH)2和LiOH·H2O为原料,合成出了层状锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2.通过XRD、SEM和电化学测试对LiNi1/3-Co1/3Mn1/3O2材料的结构、形貌及电化学性能进行了测试和表征.结果表明,800℃烧结12h所合成的样品粒度大小分布比较均匀,该材料以0.2C充放电,其首次放电容量为150mAh·g-1,循环30次后容量为137mAh·g-1.  相似文献   

5.
以聚丙烯酸和碳酸盐(Li:Ni:Mn=1.05:0.5:1.5)为主要原料,用溶胶-凝胶法合成了LiNi0.5Mn1.5O4.用X射线衍射、DSC-TGA、SEM和恒电流充放电技术研究了工艺条件对材料结构、微观形貌和电化学性能的影响.碳酸盐溶胶-凝胶法可以制备单相尖晶石结构LiNi0.5Mn1.5O4,其放电比容量高达134 mAh/g,经45次循环后仍然可保持初始放电容量的98%.  相似文献   

6.
采用碳酸盐共沉淀法、草酸盐共沉淀法、溶胶-凝胶法、高温固相法、氢氧化物共沉淀法(pH=10、11、12)制得LiNi1/3Co1/3Mn1/3O2正极材料,通过X射线衍射(XRD)、扫描电镜(SEM)和电化学性能测试对样品的结构和性能进行了表征.结果表明,溶胶-凝胶法合成的样品层状结构较完整,阳离子混排程度低,粒径相对较小,颗粒分布均匀;该样品首次放电比容量较高为151 mAh·g-1,循环30次后容量保持率达到93.31%.  相似文献   

7.
采用溶胶-凝胶法,以聚丙烯酸为络合剂制备纳米尺寸的锂离子电池LiNi1/3Co1/3Mn1/3O2正极材料。考察了聚丙烯酸与阳离子配比和烧结温度对产物LiNi1/3Co1/3Mn1/3O2结 构 与 电 化 学 性 能 的 影 响。结果表明,烧结温度700℃可制备出晶体发育完整、粒径80nm、分 布 均 匀 的α-NaFeO2层 状 结 构 的LiNi1/3Co1/3Mn1/3O2。当聚丙烯酸与金属阳离子摩尔比值为0.75,首次放电比容量达到169.2mAh/g,30次循环后容量保持率为89.3%。  相似文献   

8.
采用化学共沉淀法制备球形前驱体Ni_(0.7)Co_(0.15)Mn_(0.15)(OH)_2,将其与LiOH·H_2O充分混合后高温烧结制备出锂离子电池正极材料球形LiNi_(0.7)Co_(0.15)Mn_(0.15)O_2,用X射线衍射(XRD)、扫描电镜(SEM)、热重-差热分析(TG/DSC)以及恒电流充放电测试对样品进行表征,研究了烧结温度对产物的形貌和电化学性能的影响。结果表明,在750℃合成的LiNi_(0.7)Co_(0.15)Mn_(0.15)O_2物相单一无杂相,具有标准的α-NaFeO_2晶型,为层状嵌锂复合氧化物。SEM测试显示,产物为球形且球形度较好,颗粒粒度均一,分布较窄,平均粒径在10μm左右。在3.0-4.3 V、0.2C充放电条件下,25℃其初始放电容量高达185.2 mA·h/g,30轮循环后容量保持率达到98.32%。可见球形LiNi_(0.7)Co_(0.15)Mn_(0.15)O_2显示了较高的首轮放电容量以及良好的循环性能,表现出较好的电化学性能。  相似文献   

9.
吕睿  王晓清  殷昊曦  张纪梅 《材料导报》2012,26(17):154-158
分别介绍了锂钴氧化物、锂镍氧化物、锂锰氧化物、多元复合层状氧化物及磷酸铁锂的溶胶-凝胶法合成。探讨了采用不同元素掺杂来提高比容量和循环稳定性的改性方法。提出了目前溶胶-凝胶法在锂离子电池正极材料制备中存在的问题,并展望了它未来的发展趋势。  相似文献   

10.
随着社会的迅速发展,能源短缺和环境恶化两大问题严重制约了全球社会文明发展以及经济发展。锂离子电池具有能量密度高、自放电率小、无记忆效应、循环性能好等诸多优点,广泛应用于各种电子设备、新能源汽车、储能系统等领域。锂离子电池的正极材料直接决定了电池的性能,研究正极材料的制备方法至关重要。综述了溶胶-凝胶法制备锂离子电池正极材料的研究进展以及溶胶-凝胶法改性正极材料的制备,并对溶胶-凝胶法制备锂离子电池正极材料未来的研究方向进行展望。  相似文献   

11.
LiNi0.8-x Znx Co0.2 O2的合成及电化学性能研究   总被引:2,自引:0,他引:2  
掺杂改性和表面修饰的LiNi0.8Co0.2O2是锂电池正极换代候选材料.采用共沉淀法制备了系列LiNi0.8-xZnxCo0.2O2材料,并对其进行X射线衍射(XRD)、扫描电镜(SEM)、循环伏安(CV)、电化学阻抗(EIS)和充放电循环性能(CP)测试分析.恒流循环(0.2C、3.0~4.2V)测试结果显示,Zn的掺入使材料的初始放电比容量有大幅增加,循环性能有所改善.其中LiNi0.78Zn0.02Co0.2O2的首次放电比容量达到206.37 mAh·g-1.第30循环时,放电比容量仍为204.03 mAh·g-1,不可逆容量损失仅为2.34 mAh·g-1,显示了很好的初期循环性能.  相似文献   

12.
The layered LiNi1/3CO1/3Mn1/3-xMg(x)O2 (x = 0, 0.01, 0.03, 0.05) cathode materials were prepared by solid state reaction, then copper oxide was coated on the product. The structures, morphologies and electrochemical properties of the LiNi1/3Co1/3Mn1/3-xMg(x)O2 and CuO-coated LiNi1/3Co1/3Mn1/3-xMg(x)O2 were characterized by X-ray diffractometry (XRD), scanning electron microscopy (SEM), and electrochemical tests. The results showed that the electrochemistry properties and cycle performance of magnesium doped LiNi1/3Co1/3Mn1/3O2 and CuO-coated LiNi1/3Co1/3Mn1/3-xMg(x)O2 materials were improved. The optimal doping content of Mg was x = 0.03 in the LiNi1/3Co1/3Mn1/3-xMg(x)O2 samples to achieve high discharge capacity and good cyclic stability, and the first discharge special capacity was 158.5 mAh/g at 0.2 C in the voltage of 2.5-4.3 V, then CuO-coated LiNi1/3Co1/3Mn1/3-0.03Mg0.03O2 was investigated. The electrode reaction reversibility and electronic conductivity were enhanced through Mg-doped and CuO-coated.  相似文献   

13.
介绍了锂离子电池正极材料LiNi1/3Co1/3Mn1/3O2的结构,综述了LiNi1/3Co1/3Mn1/3O2的正极材料制备与改性及其电化学性能研究,并对其应用前景进行了展望.  相似文献   

14.
通过固相自引发基团置换反应——流变相法制备出层状LiNi1/3Co1/3Mn1/3O2正极材料,研究了不同烧结温度对材料的结构特性、微观形貌以及电化学性能的影响。结果表明,850℃煅烧20h的样品具有最佳的二维层状结构和阳离子有序度,产物颗粒呈球形,分布均匀,平均粒径约250nm。在2.8~4.3V区间,以80mA/g充放电,首次放电比容量为169mAh/g,30次循环后容量保持率为82.6%。将充电截止电压提高至4.4V,材料的前几次放电容量明显提高,以32mA/g充放电,10次循环后的放电比容量为174mAh/g,其后容量衰减加快,循环稳定性变差。  相似文献   

15.
《Materials Letters》2006,60(9-10):1209-1212
An electrochemically active LiNi1/3Co1/3Mn1/3VO4 cathode material was synthesized by a citric acid:polyethylene glycol (CA:PEG) polymeric method, followed by calcination at 723 K for 5 h in air. X-ray diffraction (XRD) patterns showed the complete formation of a crystalline phase occurred when heated at 723 K. Scanning electron microscope (SEM) micrographs showed the various stages of morphology for the polymeric intermediates of the LiNi1/3Co1/3Mn1/3VO4 compound. Transmission electron microscope (TEM) imaging exposed that particle size ranged from ∼170 to 190 nm. The cells using LiNi1/3Co1/3Mn1/3VO4 as a cathode could be cycled between 2.8 and 4.9 V (vs. Li) at a current rate of 0.15C. The galvanostatic cycling study suggests that cycle stability and capacity retention were enhanced for LiNi1/3Co1/3Mn1/3VO4 prepared with a CA:PEG ratio of 3 : 1. The dQ/dV vs. voltage plots revealed the redox potentials and slower impedance growth for the synthesized LiNi1/3Co1/3Mn1/3VO4 cathode material.  相似文献   

16.
硅酸盐体系锂离子电池材料是新一代高性能锂离子电池正极材料选择之一,是值得研发的先进电池材料。综述了锂离子电池Li2MSiO4(M=Fe,Mn)系列正极材料的国内外最新研究进展。重点对该系列正极材料的合成方法、结构特点及电化学性能进行了总结和探讨。  相似文献   

17.
In this study, a lithium-rich layered 0.4Li2MnO3·0.6LiNi1/3Co1/3Mn1/3O2 nanotube cathode synthesized by novel electrospinning is reported, and the effects of temperature on the electrochemical performance and morphologies are investigated. The crystal structure is characterized by X-ray diffraction patterns, and refined by two sets of diffraction data (R-3m and C2/m). Refined crystal structure is 0.4Li2MnO3·0.6LiNi1/3Co1/3Mn1/3O2 composite. The inductively coupled plasma optical emission spectrometer and thermogravimetric and differential scanning calorimetry analysis measurement supply reference to optimize the calcination temperature and heat-treatment time. The morphology is characterized by scanning and highresolution transmission electron microscope techniques, and the micro-nanostructured hollow tubes of Li-rich 0.4Li2MnO3·0.6LiNi1/3Co1/3Mn1/3O2 composite with outer diameter of 200-400 nm and the wall thickness of 50-80 nm are synthesized successfully. The electrochemical evaluation shows that 0.4Li2MnO3·0.6LiNi1/3Co1/3Mn1/3O2 sintered at 800 ℃ for 8 h delivers the highest capacity of the first discharge capacity of 267.7 mAh/g between 2.5 V and 4.8 V at 0.1C and remains 183.3 mAh/g after 50 cycles. The electrospinning method with heat-treatment to get micro-nanostructured lithium-rich cathode shows promising application in lithium-ion batteries with stable electrochemical performance and higher C-rate performance for its shorter Li ions transfer channels and stable designed structure.  相似文献   

18.
Structural, magnetic and magnetocaloric properties of sol-gel prepared, nanocrystalline oxides Pr(1-x)A(x)Mn(1-y)Co(y)O3 (A = Ca, Sr) (x = 0.3; y = 0.5) (cubic, space group Fm3m) have been studied. From the X-ray data, the crystallite size of Pro.7Ca0.3Mn0.5Co0,503 and Pr0.7Sr0.3Mn0.5Co0.5O3 samples is found to be approximately 24 nm and approximately15 nm respectively. High resolution transmission electron microscopy image shows average particle size of approximately 34 nm and approximately 20 nm. Magnetization measurements indicate a Curie temperature of approximately 153 K and approximately172 K in applied magnetic field of 100 Oe for Pr0.7Ca0.3Mn0.5Co0.5O3 and Pr0.7Sr0.3Mn0.5Co0.O3 compounds. The magnetization versus applied magnetic field curves obtained at temperatures below 150 K show significant hysteresis and magnetization is not saturated even in a field of 7 T. The magnetocaloric effect is calculated from M versus H data obtained at various temperatures. Magnetic entropy change shows a maximum near T(c) for both the samples and is of the order approximately 2.5 J/kg/K.  相似文献   

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