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1.
以共沉淀法得到的类球形MnCO3为前驱物,制备了类球形正交LiMnO2(So-LiMnO2),采用XRD、SEM和N2吸附技术对样品进行表征;与非球形正交LiMnO2(No-LiMnO2)进行了对比研究。结果表明:o-LiMnO2的堆垛层错度、结晶状况、颗粒形貌和大小与前驱物的微结构密切相关;在80次电化学循环测试过程中,So-LiMnO2经15次循环可达最大的放电容量152 mAh·g-1,其容量衰减平均每次循环0.58 mAh·g-1;而No-LiMnO2要经过38次循环才能达到最大放电容量128 mAh·g-1,容量衰减平均每次循环高达1.24 mAh·g-1。TEM和EDS分析证明:由一次粒子团聚的类球形So-LiMnO2能有效地抑制电解液对材料的腐蚀、减少Mn的溶解,从而提高了电化学循环能力。  相似文献   

2.
MnCl2、LiOH、EDTA和NaClO混合溶液一步水热反应合成锂离子电池正极材料正交LiMnO2(o-LiMnO2),进一步在反应体系中添加碳纳米管(CNTs)制备碳纳米管改性的o-LiMnO2(o-LiMnO2/CNTs复合材料)。采用X-射线衍射和扫描/透射电镜表征产物的晶体结构、微观形貌,循环伏安法和恒流充放电测试得活性材料电化学性能。结果表明,体系中nLi:nMn控制为8:1,在180℃反应24h得到目标产物;反应体系中添加CNTs形成复合材料可降低o-LiMnO2颗粒粒径、提高导电率。o-LiMnO2首次放电容量为76.0mAh·g-1,100周后容量保持为124.1mAh·g-1;o-LiMnO2/CNTs复合材料首次及100周放电容量(基于o-LiMnO2/CNTs的质量)分别高达94.1和159.8mAh·g-1。  相似文献   

3.
钽离子掺杂对LiFePO4 / C物理和电化学性能的影响   总被引:2,自引:0,他引:2  
采用PAM(聚丙烯酰胺)模板-溶胶凝胶法在惰性气氛下合成钽掺杂的LiFePO4/C复合正极材料,考察了钽对目标化合物的物理和电化学性能的影响。研究结果表明,0.33C的电流下充放电时,掺杂前后第2个循环的放电容量分别为138.6 mAh·g-1和155.5 mAh·g-1,循环20次后容量为141 mAh·g-1和156 mAh·g-1。电化学交流阻抗表明,掺杂后的材料阻抗Rct从180 Ω减小到120 Ω。振实密度比掺杂前提高0.312 g·cm-3。  相似文献   

4.
以LiOH·H2O、Ni(OAc)2·4H2O、Co(OAc)2·4H2O和MnO2为原料,在水热反应釜中预处理,然后进行高温固相反应,合成了一系列锂镍钴锰氧化物LiNi0.75-xCoxMn0.25O2(x=0.05,0.10,0.15,0.20,0.25)。通过X射线衍射(XRD)、扫描电子显微镜(SEM)和电化学性能测试对所得样品的结构、形貌、粒径及电化学性能进行了表征。结果表明,当x=0.20时,所合成的正极材料具有很好的α-NaFeO2型层状晶体结构,晶胞参数a=0.286 1 nm,c=1.416 4 nm, V=0.100 4 nm3,以50 mA·g-1的电流密度在3~4.3 V(vs Li/Li+)充放电时,首次放电比容量达172.5 mAh·g-1,首次放电效率高达90.9%,30个循环后其放电比容量依然保持在161.1 mAh·g-1。  相似文献   

5.
层状LiCo1/3Ni1/3Mn1/3O2正极材料的合成及电化学性能研究   总被引:13,自引:0,他引:13  
采用液相法在800 ℃空气中烧结20 h合成出层状LiCo1/3Ni1/3Mn1/3O2正极材料。通过XRD、IR、SEM、XPS和电化学性能测试考察了产物的组成、结构、形貌及电化学性能。结果表明,所合成的LiCo1/3Ni1/3Mn1/3O2为六方单相,层状结构发育完善;产物呈球形且粒度小,分布窄,平均粒径为0.3 μm。以1 mA·cm-2的电流密度,在2.7~4.3 V区间进行充放电测试,前4周的充放电比容量分别为168/160 mAh·g-1、169/162 mAh·g-1、165/160 mAh·g-1、163/158 mAh·g-1,循环性能优良。循环伏安实验表明,该材料在3.9 V附近出现了一对对称性好的氧化还原峰。  相似文献   

6.
微乳液法合成LiFePO4 / C正极材料及其电化学性能   总被引:4,自引:0,他引:4  
本文采用微乳液方法合成了纳米LiFePO4 / C正极材料。制备样品分别用XRD和SEM进行表征,充放电测试其电化学性能。600 ℃制备样品为单一物相,平均粒径90 nm,在室温2.0~4.0 V (vs Li) 放电电压范围和15 mA·g-1放电速率下,首次放电容量达到159 mAh·g-1。制备样品同样展现良好的循环性能。在15 mA·g-1速率下40次循环后,制备样品放电容量仍保持首次放电容量的98.9%。优异的电化学性能得益于样品颗粒的纳米尺寸、均匀分布以及表面碳层包覆提高了活性材料的电子电导率。  相似文献   

7.
为考察不同锰源对所制备尖晶石LiMn2O4(LMO)电化学性能的影响(特别是高温性能),采用沉淀法制备前驱体,通过不同煅烧温度制备得到最常用的锰氧化物(MnO2、Mn2O3和Mn3O4)为锰源,经相同条件制备得到LMO正极材料,通过考察所得LMO形貌及电化学性能来研究锰源与LMO电化学性能的关系。研究结果表明,相同的前驱体在不同煅烧温度下可以得到不同的锰氧化物,且各自具有不同的形貌结构。由这些锰氧化物都可以得到高纯度的LMO,但产物形貌结构以及材料中的八面体晶体含量和尺寸不同。由Mn2O3制备得到的LMO材料中的八面体晶体含量最多,且尺寸最均匀,在3种LMO中容量性能、倍率性能和循环性能最好:0.2C(1C=148 mA·g-1)下首次放电比容量为131.8 mAh·g-1;3C下还有100.4 mAh·g-1的放电比容量。其对应半电池在0.5C下循环100次后,放电比容量还有116.0 mAh·g-1,容量保持率为93.9%,电化学储能性能远远优于其他2种LMO。即使是在高温55 ℃下,由Mn2O3得到的LMO也表现出明显优于其他2种材料的高倍率性能和抗衰减性能。  相似文献   

8.
Li3V2(PO4)3的溶胶-凝胶法合成及其性能研究   总被引:11,自引:0,他引:11  
以LiOH·H2O、NH4VO3、H3PO4和柠檬酸等为原料采用溶胶-凝胶法合成了锂离子二次电池正极材料磷酸钒锂(Li3V2(PO4)3)。考察了煅烧温度和配位剂种类等条件对产物组成及电化学性能的影响。研究了优化条件下制得样品的循环伏安、充放电性能和循环性能。0.1 C条件下,样品首次放电比容量达129.81 mAh·g-1,经过100次循环后容量几乎没有衰减,仍保持在128 mAh·g-1。X射线衍射研究表明合成单一Li3V2(PO4)3晶体所需温度比固相法低;并考察了循环20次后材料充电到各个单相的晶体结构,通过X射线衍射和最小二乘法计算给出了其晶胞参数变化过程,证实了循环嵌Li过程中晶体结构能够得到重现。  相似文献   

9.
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   

10.
采用同时掺杂Tl、Al和M(M=Co、Cr和Ni)三种金属原子和改进固相反应的方法合成了复合尖晶石正极材料 LiMn2-x-y-zTlxAlyMzO4,并采用XRD、SEM、TEM、循环伏安和电化学测试考察了它的物理性质和电化学性能。结果表明,所合成的正极材料具有与母体LiMn2O4尖晶石同样完整的尖晶石结构,规则的形貌和均匀的粒径分布。当M为Co和Cr时,目标材料的平均粒径约800nm,且具有良好的电化学性能,其首次充电容量分别为123.70mAh·g-1和121.30mAh·g-1,首次放电容量分别为117.30mAh·g-1和115.70mAh·g-1。当M为Ni时,材料的电化学性能相对较差。循环伏安和充放电曲线表明该正极材料的充放电分别为两步脱锂和插锂机理。当Li掺杂量较小时,目标材料在充放电过程中均各有两个平台。随着Li掺杂量的增加,充放电平台有由两个逐渐转变为一个的趋势。当M为Co或Cr时,该正极材料不仅拥有较高的比容量和常温循环稳定性能,而且还具有较优良的高温循环稳定性能,这可能主要归因于三种金属的协同作用使目标材料的结构更加稳定,这也使该材料有可能成为电动车电池的较佳正极材料。  相似文献   

11.
娄太平  张乐  郭军兴 《化学学报》2010,68(6):466-470
研究了在不同温度下的NaNO3和AgNO3水溶液中Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3离子交换行为.实验表明Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3均显示出了高选择性与Na+和Ag+进行离子交换的特征,且对Ag+的选择性高于Na+.升高温度可显著提高Ag/Li和Ag/Na的交换反应速度.  相似文献   

12.
Single crystals of K3RESi2O7 (RE=Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu) were grown from a potassium fluoride flux. Two different structure types were found for this series. Silicates containing the larger rare earths, RE=Gd, Tb, Dy, Ho, Er, Tm, Yb crystallize in a structure K3RESi2O7 that contains the rare-earth cation in both a slightly distorted octahedral and an ideal trigonal prismatic coordination environment, while in K3LuSi2O7, containing the smallest of the rare earths, lutetium is found solely in an octahedral coordination environment. The structure of K3LuSi2O7 crystallizes in space group P63/mmc with a=5.71160(10) Å and c=13.8883(6) Å. The structures containing the remaining rare earths crystallize in the space group P63/mcm with the lattice parameters of a=9.9359(2) Å, c=14.4295(4) Å, (K3GdSi2O7); a=9.88730(10) Å, c=14.3856(3) Å, (K3TbSi2O7); a=9.8673(2) Å, c=14.3572(4) Å, (K3DySi2O7); a=9.8408(3) Å, c=14.3206(6) Å, (K3HoSi2O7); a=9.82120(10) Å, c=14.2986(2) Å, (K3ErSi2O7); a=9.80200(10) Å, c=14.2863(4) Å, (K3TmSi2O7); a=9.78190(10) Å, c=14.2401(3) Å, (K3YbSi2O7). The optical properties of the silicates were investigated and K3TbSi2O7 was found to fluoresce in the visible.  相似文献   

13.
通过调节B2O3-Bi2O3-ZnO-Al2O3(BBZA)玻璃的添加量研究其对钛酸钡(BaTiO3)陶瓷烧结条件、晶体结构和介电性能的影响。结果表明:添加适量的BBZA玻璃能够有效地将BaTiO3陶瓷烧结温度由1 350℃降至950℃,并使其致密化。同时,添加BBZA玻璃后,BaTiO3的晶体结构随着烧结温度的升高而发生转变(立方相→四方相)。另外,BBZA玻璃的引入使BaTiO3陶瓷的居里峰得到了有效的抑制和拓宽。陶瓷微观形貌显示,玻璃相均匀分布在BaTiO3晶粒表面。优化的BaTiO3陶瓷制备条件如下:BBZA添加量(质量分数)为2.0%,烧结温度为950℃。在该条件下制备的BaTiO3陶瓷介电常数达到1 364,介电损耗低至1.2%。  相似文献   

14.
YBa2Cu3Ox (Y-123) and Bi2Sr2Ca1Cu2Ox (Bi-2212) films on various substrates have been prepared by Metal-Organic Deposition starting from different metallorganic fluorine-free compounds and using a very simple instrumentation. The processing conditions include a rapid pyrolysis step in air and an annealing step in oxygen for Y-123 and in air for Bi-2212. The films obtained have been characterized by X-ray diffraction (XRD) and the formation of a superconducting phase of Y-123 or Bi-2212 was confirmed measuring the critical temperature (T c) with Ac-susceptibility and resistive measurements. Microstructure and final cationic ratios have been studied by scanning electron microscopy (SEM) and energy dispersive spectroscopy (EDS).  相似文献   

15.
The dimeric title compound decomposes upon heating to give the monomer and desulphurized monomer as shown by FT-Raman and quantum chemical means.  相似文献   

16.
The near infrared spectra of aqueous solutions of the ethylsulfates of La, Nd, Gd, Tb, Er, Yb, Lu, Y, and Na have been determined from about 0.2 mol-dm–3 to nearly saturation. The extinction coefficients of water have been calculated taking into account the absorption of ethylslfate anions determined in separate experiments. Their values appeared to be nearly the same as that of pure water. The relative contents of free OH groups in 0.5 and 0.7M solutions have been estimated from the absorbances at 1160 nm. They were lower in solutions of the heavy rare-earth ethylsulfates (Tb, Er, Yb, Lu) than in equimolar solutions of the lighter ones (La, Nd), confirming our previous view that secondary hydration of the heavy trivalent rare-earth cations is distinctly stronger than that of the lighter ones. A comparison of the spectra of these aqueous ethylsulfates with those of perchlorates shows that the structure-breaking ability of the C2H5SO 4 ion is much smaller than that of perchlorate anion.  相似文献   

17.
The crystal structures of compounds with nominal compositions Bi6FeP2O15+x (I), Bi6NiP2O15+x (II) and Bi6ZnP2O15+x (III) were determined from single-crystal X-ray diffraction data. They are monoclinic, space group I2, Z=2. The lattice parameters for (I) are a=11.2644(7), b=5.4380(3), c=11.1440(5) Å, β=96.154(4)°; for (II) a=11.259(7), b=5.461(4), c=11.109(7) Å, β=96.65(1)°; for (III) a=19.7271(5), b=5.4376(2), c=16.9730(6) Å, β=131.932(1)°. Least squares refinements on F2 converged for (I) to R1=0.0554, wR2=0.1408; for (II) R1=0.0647, wR2=0.1697; for (III) R1=0.0385, wR2=0.1023. The crystals are complexly twinned by 2-fold rotation about , by inversion and by mirror reflection. The structures consist of edge-sharing articulations of OBi4 tetrahedra forming layers in the a-c plane that then continue by edge-sharing parallel to the b-axis. The three-dimensional networks are bridged by Fe and Ni octahedra in (I) and (II) and by Zn trigonal bipyramids in (III) as well as by oxygen atoms of the PO4 moieties. Bi also randomly occupies the octahedral sites. Oxygen vacancies exist in the structures of the three compounds due to required charge balances and they occur in the octahedral coordination polyhedron of the transition metal. In compound (III), no positional disorder in atomic sites is present. The Bi-O coordination polyhedra are trigonal prisms with one, two or three faces capped. Magnetic susceptibility data for compound (I) were obtained between 4.2 and 350 K. Between 4.2 and 250 K it is paramagnetic, μeff=6.1 μB; a magnetic transition occurs above 250 K.  相似文献   

18.
针对银精矿样品复杂,难消解的特点,研究了不同酸溶法和碱熔法对样品的消解情况,建立了硝酸,盐酸,氢氟酸,高氯酸消解银精矿的方法。根据元素灵敏度和抗干扰性,选定各元素的测定波长。通过酸溶样和碱熔样测定结果比对,验证了方法准确性。建立了四酸消解-电感耦合等离子体光谱法测定银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的方法,元素的线性相关系数均在0.9999以上。通过共存元素干扰实验,确定了银精矿中高含量元素(铜、铅、锌、铁、锑、铋等)对测定元素结果没有影响。方法检出限:Cu 0.0063 mg/L, Pb 0.0159 mg/L ,Zn 0.0090 mg/L,As 0.0192 mg/L, Cd 0.0093 mg/L ,Ca 0.0084 mg/L, Mg 0.0075 mg/L, Mn 0.0081 mg/L。测定下限:Cu 0.0105mg/L,Pb 0.0265 mg/L, Zn 0.0150 mg/L, As 0.0320 mg/L, Cd 0.0155 mg/L, Ca 0.0140 mg/L, Mg 0.0125 mg/L,Mn 0.0135 mg/L。3个样品的相对标准偏差在0.87%~3.56%之间,加标回收率在95.00%~103.56%之间。方法流程短,操作简单,快速,灵敏度和再现性高,结果准确可靠,可以满足银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的测定。  相似文献   

19.
The room temperature structures of the five layer Aurivillius phases A2Bi4Ti5O18 (A=Ca, Sr, Ba and Pb) have been refined from powder neutron diffraction data using the Rietveld method. The structures consist of [Bi2O2]2+ layers interleaved with perovskite-like [A2Bi2Ti5O16]2− blocks. The structures were refined in the orthorhombic space group B2eb (SG. No. 41), Z=4, and the unit cell parameters of the oxides are a=5.4251(2), b=5.4034(1), c=48.486(1); a=5.4650(2), b=5.4625(3), c=48.852(1); a=5.4988(3), b=5.4980(4), c=50.352(1); a=5.4701(2), b=5.4577(2), c=49.643(1) for A=Ca, Sr, Ba and Pb, respectively. The structural features of the compounds were found similar to n=2-4 layers bismuth oxides. The strain caused by mismatch of cell parameter requirements for the [Bi2O2]2+ layers and perovskite-like [A2Bi2Ti5O16]2− blocks were relieved by tilting of the TiO6 octahedra. Variable temperature synchrotron X-ray studies for Ca and Pb compounds showed that the orthorhombic structure persisted up to 675 and 475 K, respectively. Raman spectra of the compounds are also presented.  相似文献   

20.
The crystal structures of Bi2.5Na0.5Ta2O9 and Bi2.5Nam-1.5NbmO3m+3 (m=3,4) have been investigated by the Rietveld analysis of their neutron powder diffraction patterns (λ=1.470 Å). These compounds belong to the Aurivillius phase family and are built up by (Bi2O2)2+ fluorite layers and (Am-1BmO3m+1)2- (m=2-4) pseudo-perovskite slabs. Bi2.5Na0.5Ta2O9 (m=2) and Bi2.5Na2.5Nb4O15 (m=4) crystallize in the orthorhombic space group A21am, Z=4, with lattice constants of a=5.4763(4), b=5.4478(4), c=24.9710 (15) and a=5.5095(5), b=5.4783(5), c=40.553(3) Å, respectively. Bi2.5Na1.5Nb3O12 (m=3) has been refined in the orthorhombic space group B2cb, Z=4, with the unit-cell parameters a=5.5024(7), b=5.4622(7), and c=32.735(4) Å. In comparison with its isostructural Nb analogue, the structure of Bi2.5Na0.5Ta2O9 is less distorted and bond valence sum calculations indicate that the Ta-O bonds are somewhat stronger than the Nb-O bonds. The cell parameters a and b increase with increasing m for the compounds Bi2.5Nam-1.5NbmO3m+3 (m=2-4), causing a greater strain in the structure. Electron microscopy studies verify that the intergrowth of mixed perovskite layers, caused by stacking faults, also increases with increasing m.  相似文献   

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