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1.
Li4Ti5O12/(Ag+C)电极材料的固相合成及电化学性能   总被引:1,自引:0,他引:1  
以Li2CO3,TiO2为原料,葡萄糖为碳源,采用固相煅烧工艺合成了亚微米级的Li4Ti5O12/C复合负极材料。并将之与AgNO3复合,采用固相方法制备出了Ag表面修饰的Li4Ti5O12/(Ag+C)复合材料。采用XRD、SEM和TEM测试方法对材料的微结构进行了表征。结果表明,C的存在对Ag单质在Li4Ti5O12/C颗粒表面的大量形成起到了积极的促进作用,从而很大程度地提高了Li4Ti5O12/C的电导率,因此有效地改善了其电化学性能。在1C倍率下,Li4Ti5O12/(Ag+C)复合材料的首次放电容量达到了164 mAh·g-1。  相似文献   

2.
Li4Ti5O12/(Cu+C)复合材料的制备及电化学性能   总被引:1,自引:0,他引:1  
以Li4Ti5O12,Cu(CH3COO)2·H2O和C6H12O6为前驱体,化学沉积与热分解结合合成锂离子电池负极材料Li4Ti5O12/(Cu+C)。采用X-射线衍射(XRD)、扫描电子显微镜(SEM)、恒流充放电、循环伏安和电化学阻抗方法表征样品的结构、形貌和电化学性能。结果表明,Li4Ti5O12表面包覆的Cu与C提高了Li4Ti5O12电极材料的导电率,其循环性能和倍率性能得到有效地改善。在0.5C、1C和3C倍率下,经过50次充放电循环,放电比容量分别为168.2、160、140.6 mAh·g-1,其容量保持率分别为88.7%、84.4%、71.2%。电化学阻抗测试表明,表面包覆的Cu与C使其电荷转移阻抗大幅度减少。  相似文献   

3.
LiMn2O4表面包覆Li4Ti5O12的制备及倍率特性   总被引:1,自引:0,他引:1       下载免费PDF全文
采用固相法合成了尖晶石型LiMn2O4,并通过溶胶-凝胶法制备了不同物质的量的百分比含量Li4Ti5O12包覆的正极材料。X-射线衍射和扫描电镜结果表明,Li4Ti5O12微粒包覆在LiMn2O4的表面没有产生晶体结构的变化。实验电池在室温下,以1C,2C和5C倍率作充放电循环测试;结果表明,与未包覆的LiMn2O4相比,表面包覆Li4Ti5O12微粒的正极材料在高倍率下具有更好的循环稳定性。  相似文献   

4.
利用具有三维连续纳米孔结构的热剥离石墨烯为骨架制备Li4Ti5O12/石墨烯纳米复合材料。通过乙醇挥发法在热剥离石墨烯的纳米孔道内引入前驱物, 进一步高温热处理, 在热剥离石墨烯的孔道内原位形成Li4Ti5O12纳米粒子。利用复合材料作为锂离子电池电极材料。电化学反应过程中, 热剥离石墨烯的三维连续结构确保了Li4Ti5O12纳米粒子与石墨烯在长循环过程中的有效接触。因此, 复合材料表现出优异的循环稳定性。在5C下, 5 000次循环后, 其容量保持率高达94%。  相似文献   

5.
锂离子电池用Li4Ti5O12-碳复合材料的制备与电化学性能   总被引:6,自引:0,他引:6  
Li4Ti5O12-C composite was prepared by sol-gel method using ethyl alcohol as solvent, lithium acetate and tetrabutyl titanate as raw materials, and graphite as carbon source. Li4Ti5O12-C composites were characterized by thermogravimertric(TG) analysis and differential thermal analysis(DTA), X-ray diffraction(XRD), Fourier transform infrared (FTIR) spectroscopy, scanning electron microscopy (SEM) and electrochemical tests. Results show that Li4Ti5O12-C composite with 5% carbon containing can be obtained by annealing the precursor at 600 ℃ for 6 h in N2 atomsphere. The composites can deliver a specific capacity of 167.1 mAh·g-1, 99.0% and 105.1% of the capacity can be retained after discharged for 80 times at 0.1C and 2.0C, respectively. Compared with pure Li4Ti5O12, Li4Ti5O12-C composite shares larger discharge capacity, better cyclability and rate performance.  相似文献   

6.
陆海纬  周永宁   《无机化学学报》2006,22(10):1802-1806
首次采用电纺丝技术结合高温退火成功地构置了含尖晶石Li4Ti5O12的纳米纤维丝三维(3D)网状结构,并测量了三维电池的充放电性能。X射线衍射谱(XRD)、扫描电子显微镜(SEM)和电池循环性能测试等方法表征纤维丝3D结构和电化学性能。研究结果表明了Li4Ti5O12纳米丝的零应变特性、构建的3D阵列的结构稳定性和在大电流密度下较好的充放电性能。显示了Li4Ti5O12可作为3D电池的电极材料。  相似文献   

7.
以乙二胺四乙酸(EDTA)为配位剂,采用溶胶凝胶和溶剂热法相结合的方法合成了Li2MnSiO4/C纳米复合正极材料。经过EDTA配位的锂锰硅前驱体在氩气中经过700℃煅烧后,产生为颗粒尺寸约为50nm的Li2MnSiO4/C纳米复合粉体。在0.1C=33mA·g-1进行充放电测试时,其首次充电和放电比容量分别为223和140mAh·g-1,第5次循环放电比容量仍为138mAh·g-1;电流密度升至0.2C=66mA·g-1时,在第20次循环的放电比容量仍可稳定在80mAh·g-1左右。这些结果表明,EDTA的配位作用可抑制杂相的形成,这种分散性相对较好的纳米复合粉体Li2MnSiO4正极材料表现出提高的循环稳定性。  相似文献   

8.
低温固相反应合成Li3V2(PO4)3正极材料及其性能   总被引:1,自引:1,他引:1  
利用V2O5·nH2O湿凝胶,LiOH·H2O,NH4H2PO4和C等作原料,通过低温固相还原反应在550 ℃焙烧12 h制备出Li3V2(PO4)3正极材料。采用XRD,SEM和电化学测试对Li3V2(PO4)3样品性能进行研究。XRD研究表明本法所合成的Li3V2(PO4)3同传统的高温固相反应法所合成的Li3V2(PO4)3一样同属于单斜晶系结构。SEM测试表明所合成的样品平均粒径大小约为0.5 μm且粒径分布较窄。电化学测试表明以0.2 C的倍率放电时,样品的首次放电容量为130 mAh·g-1,室温下循环30次后其比容量为124 mAh·g-1。  相似文献   

9.
KCl熔盐法制备LiMn2O4   总被引:4,自引:0,他引:4  
采用熔盐法合成了LiMn2O4。熔盐的使用可以使原来固相反应的高温焙烧时间缩短。合成获得的材料结晶良好,颗粒大小在数百个纳米左右,有较明显的团聚现象。该材料的初始容量为113 mAh·g-1,循环性能优良,前100次的容量平均衰减率在0.05%左右;倍率性能亦非常优秀,8 C放电时的容量为1 C放电容量的93%以上。熔盐的用量在4倍于Li+以上时,对材料的结构形貌和性能都没有明显影响。  相似文献   

10.
Li3V2(PO4)3的溶胶-凝胶合成及其性能研究   总被引:1,自引:0,他引:1  
以LiOH·H2O(LiF、Li2CO3、LiCH3COO·2H2O)、NH4VO3、H3PO4和柠檬酸为原料,采用Sol-gel法合成锂离子电池正极材料Li3V2(PO4)3。优化了锂源、溶胶的pH值、预烧条件、煅烧温度等合成条件,并采用XRD、SEM、恒电流充放电及循环伏安试验等方法,研究了所合成的Li3V2(PO4)3的结构形貌和电化学性能。结果表明,以LiOH·H2O为锂源,溶胶的pH值等于3,于氩气氢气(体积比9∶1)混合气中300 ℃预烧 4 h,并在氩气氢气(体积比9∶1)混合气中600 ℃煅烧8 h合成的Li3V2(PO4)3正极材料为标准的单斜结构,具有较高的放电比容量和较好的循环稳定性,0.1C和1C倍率下首次放电比容量分别为130 mAh·g-1和129 mAh·g-1;1C倍率下循环40次后,容量仍为127 mAh·g-1,容量保持率为98.4%;随后又进行10C倍率放电,10次循环后容量为105 mAh·g-1,容量保有率达98.1%。循环伏安测试表明,该正极材料具有较好的电化学可逆性。  相似文献   

11.
新铌酸盐化合物K6Zr2Nb14O42的合成   总被引:1,自引:1,他引:0  
一些铌酸盐晶体具有优良的非线性光学性质,它们在激光倍频、电光调制、参量振荡、实时全息存贮等领域均具有潜在的广泛的应用前景,因此新铌酸盐晶体的人工合成、结构及性能研究工作受到了重视[1-3],吴伯麟等曾报道了在K2O-Cr2O3-Nb2O5体系中存在一...  相似文献   

12.
K3InF6 is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K3InF6 by decomposition at high temperature. The crystal structure of K3InC12O14H4F18 is characterized by complex anions [In(CF3COO)4(OHx)2](5−2x)− and isolated [CF3COOH2−x](x−1)− molecules with x=2 or 1, surrounded by K+ cations. The crystal structure of K3InC12O12F18 is only constituted by complex anions [In(CF3COO)6]3− and K+ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K2InC10O10H6F9 and K3InC12O12F18 were also performed at room temperature on pulverized crystals.  相似文献   

13.
通过静电纺丝技术制备了多孔软硬磁Ni0.5Zn0.5Fe2O4/SrFe12O19复合纤维,利用综合热重分析仪(TG-DSC)、X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线能谱仪(EDS)和矢量网络分析仪(VNA)等对复合纤维的晶体结构、微观形貌和电磁性能进行了表征,研究了不同软硬磁质量比对纤维结构和性能的影响。结果表明:900℃下制备的复合纤维具有立体多孔结构,软硬磁质量比为1∶3时,复合纤维的比表面积达到55 m2·g-1。吸波性能测试结果显示,当吸波剂涂层厚度为3.5 mm时,复合纤维在10.6 GHz处反射损失(RL)值达到-31.9 dB,在2~18 GHz频率范围内,RL值小于-10 dB的吸收带宽达到10.5 GHz,覆盖了整个X波段(8.2~12.4 GHz)和Ku波段(12.4~18 GHz),显示出优异的宽波段吸收性能。  相似文献   

14.
通过静电纺丝技术制备了多孔软硬磁Ni_(0.5)Zn_(0.5)Fe_2O_4/SrFe_(12)O_(19)复合纤维,利用综合热重分析仪(TG-DSC)、X射线衍射仪(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线能谱仪(EDS)和矢量网络分析仪(VNA)等对复合纤维的晶体结构、微观形貌和电磁性能进行了表征,研究了不同软硬磁质量比对纤维结构和性能的影响。结果表明:900℃下制备的复合纤维具有立体多孔结构,软硬磁质量比为1∶3时,复合纤维的比表面积达到55 m~2·g~(-1)。吸波性能测试结果显示,当吸波剂涂层厚度为3.5 mm时,复合纤维在10.6 GHz处反射损失(RL)值达到-31.9 dB,在2~18 GHz频率范围内,RL值小于-10 dB的吸收带宽达到10.5 GHz,覆盖了整个X波段(8.2~12.4 GHz)和Ku波段(12.4~18 GHz),显示出优异的宽波段吸收性能。  相似文献   

15.
The rate constants of the hydrogen abstraction reactions of CF3CHFCF3 + H (R1) and CF3CF2CHF2 + H (R2) have been calculated by means of the dual-level direct dynamics method. Optimized geometries and frequencies of stationary points and extra points along the minimum-energy path (MEP) are obtained at the MPW1K/6-311+G(d,p) level, and the classical energetic information is further corrected with the interpolated single-point energy (ISPE) approach by the G3(MP2) level of theory. Using the canonical variational transition state theory (CVT) with small-curvature tunneling corrections (SCT), the rate constants are evaluated over a wide temperature range of 200-2000 K. The calculated CVT/SCT rate constants are in good agreement with available experimental values. It is found that the variational effect is very small and almost negligible over the whole temperature region. However, the small-curvature tunneling correction plays an important role in the lower temperature range. Furthermore, the heats of formation of species CF3CF2CHF2 (SC1 or SC2) and CF3CF2CF2 are studied using isodesmic reactions to further elucidate the thermodynamic properties.  相似文献   

16.
一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…  相似文献   

17.
The compound previously reported as Ba2Ti2B2O9 has been reformulated as Ba3Ti3B2O12, or Ba3Ti3O6(BO3)2, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO3:BaTiB2O6 (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F2)=0.039 for 504 unique reflections. Ba3Ti3O6(BO3)2 is isostructural with K3Ta3O6(BO3)2. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba3Ti3O6(BO3)2 is equal to 95% of that of LiNbO3.  相似文献   

18.
Well-developed crystalline LiNi0.5Mn1.5O4 was prepared by solid-state reaction using Li2CO3, NiO and electrolytic MnO2 at high heating and cooling rate. X-ray diffraction (XRD) patterns and scanning electron microscopic (SEM) images showed that LiNi0.5Mn1.5O4 synthesized at 900 ℃ and 950 ℃ had cubic spinel structure with clearly defined shape. LiNi0.5Mn1.5O4 spinel phase decomposed at 1 000 ℃ accompanying with structural and morphological degradation. TG measurement revealed that the weight loss during heating process could be mostly gained in cooling process, and the upward tendency of weight loss during heating process decreased, while that of irreversible weight loss rapidly increased with the increase of temperature. LiNi0.5Mn1.5O4 powders prepared at 900 ℃ for 12 h delivered the maximum discharge capacity of 134 mAh·g-1 with good cyclic performance at 2/7 C. In addition, by adjusting the calcination time at 900 ℃, the capacity and cycling performance of LiNi0.5Mn1.5O4 were further enhanced.  相似文献   

19.
利用XRD、SEM、EDS、BET、激光粒度、循环伏安、恒流充放电、交流阻抗方法研究了葡萄糖为碳源对溶胶凝胶法制备Li1.2Ni0.13Co0.13Mn0.54O2正极材料的结构、形貌以及电化学性能的影响.结果表明:与前驱体中未加入葡萄糖所制备的材料相比,掺葡萄糖后样品颗粒分布相对均匀,粒径变小,D50从11.56减小至9.94 μm,比表面积增加近1倍.经0.05C充放电活化后,未掺葡萄糖和掺葡萄糖样品0.2C放电比容量分别为183.4、211.6 mAh·g-1,2C容量分别为其0.2C的62.2%、77.6%.1C循环50次后放电比容量分别为133.3、173.6 mAh·g-1,容量保持率分别为95.1%、100%.掺葡萄糖可降低首次不可逆容量损失,提高材料的倍率性能与循环稳定性,减少电荷传递阻抗、Warburg阻抗以及双电层弥散效应,但不改变材料的晶型结构.  相似文献   

20.
利用XRD、SEM、EDS、BET、激光粒度、循环伏安、恒流充放电、交流阻抗方法研究了葡萄糖为碳源对溶胶凝胶法制备Li1.2Ni0.13Co0.13Mn0.54O2正极材料的结构、形貌以及电化学性能的影响。结果表明:与前驱体中未加入葡萄糖所制备的材料相比,掺葡萄糖后样品颗粒分布相对均匀,粒径变小,D50从11.56减小至9.94μm,比表面积增加近1倍。经0.05C充放电活化后,未掺葡萄糖和掺葡萄糖样品0.2C放电比容量分别为183.4、211.6mAh·g-1,2C容量分别为其0.2C的62.2%、77.6%。1C循环50次后放电比容量分别为133.3、173.6mAh·g-1,容量保持率分别为95.1%、100%。掺葡萄糖可降低首次不可逆容量损失,提高材料的倍率性能与循环稳定性,减少电荷传递阻抗、Warburg阻抗以及双电层弥散效应,但不改变材料的晶型结构。  相似文献   

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