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1.
Al离子掺杂正极材料LiMn2O4的高温循环性能   总被引:1,自引:0,他引:1  
采用固相反应法分别合成正极材料LiMn2O4和LiAlxMn2-xO4(x=0.05,0.1,0.3).对它们进行XRD和SEM测试,并对比了高温下的循环性能.结果显示:除Al掺杂量x=0.3时,合成物出现了LiAlO2杂质相外,其余皆具有单一的尖晶石相结构.掺杂后的晶体颗粒比较圆润.LiMn2O4在高温下经过20次循环后,其比容量降低29%,衰减很快.造成衰减的主要原因是Mn3+歧化反应生成的Mn2+在电解液中的溶解,以及Jahn-Teller效应.通过阳离子Al3+的掺杂,有效的提高了尖晶石LiMn2O4的高温循环性能.  相似文献   

2.
采用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、电池性能测试系统研究了多元稀土掺杂锂锰氧正极材料的相结构、形貌,并对其活化性能、循环稳定性能进行了表征。结果表明:采用Pechini法合成多元稀土掺杂LiMn2O4样品时,只有将掺杂元素的含量严格控制在一定范围内,所合成的LiMn2O4、LiLa0.03Mn1.97O4、LiLa0.012Ce0.012Mn1.976O4、LiLa0.012Nd0.012Mn1.976O4、LiCe0.012Nd0.012Mn1.976O4样品才具有纯尖晶石型LiMn2O4结构。当稀土掺杂元素含量较高时,所合成的LiLa0.015Ce0.015Mn1.97O4、LiLa0.015Nd0.015Mn1.97O4、LiCe0.015Nd0.015Mn1.97O4样品由LiMn2O4相及微量杂质相CeO2、Nd2O3、CeO2+Nd2O3组成。所有样品呈规则的近球形或球形,其粒径范围为0.5~2.8μm。适量的稀土元素掺杂将使LiMn2O4材料的初始容量减小、充放电效率及循环稳定性能增加,LiCe0.012Nd0.012Mn1.976O4样品具有较好的综合电化学性能,其初始容量为123.5mAh/g,经30次循环充放电后的容量为113.2mAh/g,为相同条件下LiMn2O4样品放电容量的1.27倍。  相似文献   

3.
采用固相反应法分别合成正极材料LiMn2O4和LiAl,Mn2-xO4(x=0.05,0.1,0.3)。对它们进行XRD和SEM测试,并对比了高温下的循环性能。结果显示:除Al掺杂量x=0.3时,合成物出现了LiAlO2杂质相外,其余皆具有单一的尖晶石相结构。掺杂后的晶体颗粒比较圆润。LiMn2O4在高温下经过20次循环后,其比容量降低29%,衰减很快。造成衰减的主要原因是Mn^3+歧化反应生成的Mn^2+在电解液中的溶解,以及Jahn—Teller效应。通过阳离子Al^3+的掺杂,有效的提高了尖晶石LiMn2O4的高温循环性能。  相似文献   

4.
掺杂元素La、F对尖晶石LiMn2O4材料结构及性能的影响   总被引:1,自引:0,他引:1  
采用X-射线衍射仪(XRK)、扫描电子显微镜(SEM)、电池测试系统等研究了掺杂元素La、F对高温固相合成尖晶石型LiMn2O4材料的相结构、貌、活化性能、循环稳定性能的影响.结果表明:掺杂元素La、F可有效地提高LiMn2O4样品的充放电效率、循环稳定性能:随着掺杂元素F含量的增加,LiMn2O4-xFx样品的初始容量降低、循环稳定性能呈现出先增后减的变化规律;当掺杂元素La、F的含量较少时,LiLay,Mn2-yO4-xFx样品具有纯的尖晶石LMn2O4结构,样品呈球形或近球形,粒径范围为0.5~2.5 μm,LiLa0.02Mn1.98O3.95F0.05样品的初始放电容量为123.6mAh/g,经30次循环充放电后的容量为114.6mAh/g,容量保持率为92.7%,具有较好的活化性能和循环稳定性能.  相似文献   

5.
Al掺杂Li_2MnSiO_4锂离子电池正极材料的合成和电化学性能   总被引:1,自引:1,他引:0  
以Li2SiO3、Mn(CH3COO)2.4H2O和Al(OH)3为原料,用传统高温固相合成法成功制备出Li2Al0.1Mn0.9SiO4锂离子电池正极材料。采用XRD、FESEM分析了正极材料的相组成、结构和形貌,利用电池测试仪测试了正极材料的电化学性能。研究结果表明,固相合成的产物主相为Li2Al0.1Mn0.9SiO4,同时存在少量的杂质,产物表面形貌为非球形颗粒,颗粒尺寸为100~500 nm。实验结果表明,Al掺杂后,正极材料的可逆容量和循环寿命都得到提高。正极材料电化学性能提高的机理在于Al掺杂稳定了Li2MnSiO4正极材料的结构。  相似文献   

6.
以Mn3O4为前驱体制备尖晶石型LiMn2O4及其性能   总被引:1,自引:0,他引:1  
采用改进的固相反应法合成了高性能的锂离子电池正极材料LiMn2O4。首先,以廉价的MnSO4为原料,通过水解氧化法制备纳米级Mn3O4前驱体;然后,将Mn3O4和Li2CO3混合均匀,在750℃固相反应20 h,得到尖晶石型LiMn2O4。用X射线衍射(XRD)和扫描电镜(SEM)对Mn3O4前驱体和LiMn2O4样品进行表征,用充放电测试和循环伏安技术对LiMn2O4样品进行电化学性能研究。结果表明:所制备的LiMn2O4具有完整的尖晶石型结构,且晶体粒子分布均匀。所制备的LiMn2O4材料在3.0~4.4 V之间,室温(25℃)下,在0.2C倍率下首次放电比容量为130.6 mA.h/g;在0.5C倍率下首次放电比容量为127.1 mA.h/g,30次循环后,容量仍有109.5 mA.h/g,且样品具有较好的高温性能。  相似文献   

7.
采用X射线衍射仪、扫描电子显微镜、电池测试系统等研究了不同稀土掺杂元素La、Ce、Nd等对Pechini法合成的LiMn2O4材料的相结构、形貌及电化学性能的影响规律.结果表明,合成的LiMn2O4、LiLa0.03Mn1.97O4、LiLa0.01Ce0.01Nd0.01Mn1.97O4样品具有纯尖晶石型LiMn2O4结构,LiLa0.015Ce0.015Mn1.97O4样品由LiMn:O.相及微量杂质相CeO2组成;样品呈规则的近球形或球形,其粒径范围为0.5~2.5μm.稀土元素取代使LiMn2O4材料的初始容量略有降低、循环稳定性能有较大增加,LiMn2O4、LiLa0.03Mn1.97O4、LiLa0.015Ce0.015Mn1.97O4、LiLa0.01Ce0.01Nd0.01Mn1.97O42样品的初始容量分别为126.0、120.0、117.3、124.0 mA·h/g,经30次循环充放电后的容量分别为88.9、102.7、101.6、109.1 mA·h/g.  相似文献   

8.
重点研究了室温固相法Co/Mn氢氧化物包覆Ni(OH)2的机理.采用XRD,SEM,TEM和EDS分析检测手段分析了未包覆与表面包覆材料的结构、形貌和表面成分.TEM实验结果表明,LiNiO2颗粒表面包覆了一薄层化合物;XPS实验结果表明,LiNiO2颗粒表面包覆了Co/Mn元素;SEM和EDS实验结果进一步表明,球形LiNiO2颗粒表面均匀包覆了Co/Mn化合物层.电化学性能测试结果表明,经Co/Mn包覆的LiNiO2正极材料显示了优越的循环性能.  相似文献   

9.
本文采用热重分析仪(TGA)、X-射线衍射仪(XRD)、扫描电子显微镜(SEM)、电池测试系统等方法研究了尖晶石LiMn2O4材料的高温固相合成过程的相转变、形貌变化、晶格常数及电化学性能等变化规律.结果表明:合成温度较低时(≤823 K),样品由尖晶石型LiMn2O4相、微量MnO2相(673 K)或Mn2O3相(823 K)组成;当合成温度高于973 K时,样品由热稳定性能较好的纯尖晶石型LiMn2O4相组成.呈规则的球形或近球形,粒径范围为0.5~5μm.随着合成温度的升高,LiMn2O4样品的点阵常数、晶胞体积、颗粒尺寸等有不同程度的增加,放电容量呈先增后减的规律.  相似文献   

10.
以Mn2+和NH4HCO3为原料,通过控制结晶法合成球形MnCO3前驱体模板。以LiNO3和MnCO3为原料,按照一定的摩尔比机械混合,在700°C下煅烧8h,合成高倍率性能和长循环性能的球形尖晶石LiMn2O4材料。分别考查原料的摩尔比、反应时间以及反应温度对前驱体MnCO3形貌和产率的影响。采用X射线粉末衍射和扫描电镜对合成的MnCO3和LiMn2O4进行表征,对LiMn2O4样品进行室温条件下的充放电性能测试。电化学测试结果表明:尖晶石锰酸锂微球在10C的放电倍率下的首次放电容量达90mA·h/g(1C放电容量为148mA/g),800次循环后容量保持率达到75%。该方法合成的LiMn2O4微球作为高功率型锂离子电池的正极材料有着较好的应用前景。  相似文献   

11.
In as-welded state, each region of 2219 aluminum alloy TIG-welded joint shows diff erent microstructure and microhardness due to the diff erent welding heat cycles and the resulting evolution of second phases. After the post-weld heat treatment, both the amount and the size of the eutectic structure or θ phases decreased. Correspondingly, both the Cu content in α-Al matrix and the microhardness increased to a similar level in each region of the joint, and the tensile strength of the entire joint was greatly improved. Post-weld heat treatment played the role of solid solution strengthening and aging strengthening. After the post-weld heat treatment, the weld performance became similar to other regions, but weld reinforcements lost their reinforcing eff ect on the weld and their existence was more of an adverse eff ect. The joint without weld reinforcements after the post-weld heat treatment had the optimal tensile properties, and the specimens randomly crack in the weld zone.  相似文献   

12.
After nearly two years' tense construction, the first phase of industrialized base of Shenyang Research Institute of Foundry (SRIF), located at the Tiexi Casting and Forging Industrial Park in the west of Tiexi District, has now been completed and formally put into operation.  相似文献   

13.
Institute of Process Engineering, Chinese Academy of Sciences, China, has proposed a method for oxidative leaching of chromite with potassium hydroxide. Understanding the mechanism of chromite decomposition, especially in the potassium hydroxide fusion, is important for the optimization of the operating parameters of the oxidative leaching process. A traditional thermodynamic method is proposed and the thermal decomposition and the reaction decomposition during the oxidative leaching of chromite with KOH and oxygen is discussed, which suggests that chromite is mainly destroyed by reactions with KOH and oxygen. Meanwhile, equilibrium of the main reactions of the above process was calculated at different temperatures and oxygen partial pressures. The stable zones of productions, namely, K2CrO4 and Fe2O3, increase with the decrease of temperature, which indicates that higher temperature is not beneficial to thermodynamic reactions. In addition, a comparison of the general alkali methods is carried out, and it is concluded that the KOH leaching process is thermodynamically superior to the conventional chromate production process.  相似文献   

14.
The effect of isochronal heat treatments for 1h on variation of damping, hardness and microstructural change of the magnesium wrought alloy AZ61 was investigated. Damping and hardness behaviour could be attributed to the evolution of precipitation process. The influence of precipitation on damping behaviour was explained in the framework of the dislocation string model of Granato and Lücke.  相似文献   

15.
The motion of melt droplets in spray degassing process was analyzed theoretically. The height of the treatment tank in spray degassing process could be determined by the results of theoretical calculation of motion of melt droplets. To know whether the melt droplets would solidify during spraying process, the balance temperature of melt droplets was also theoretically analyzed. Then proof experiments for theoretical results about temperature of melt droplets were carried. In comparison, the experimental results were nearly similar to the calculation results.  相似文献   

16.
On the basis of the single-particle framework, a new theory on inclusion growth in metallurgical melts is developed to study the kinetics of inclusion growth on account of reaction and collision. The studies show that the early growth of inclusion depends on reaction growth and Brawnian motion collision, and where the former is decisive, the late growth depends on turbulence collision and Stokes' collision, and where the former is dominant; collision growth is very quick during the smelting process, lessened in the refining process, but nearly negligible in the continuous casting process.  相似文献   

17.
An approach based on film buckling under simple uniaxial tensile testing was utilized in this paper to quantitatively estimate the interfacial energy of the nanostructured multilayer films(NMFs) adherent to flexible substrates. The interfacial energies of polyimide-supported NMFs are determined to be *5.0 J/m2 for Cu/Cr, *4.1 J/m2 for Cu/Ta,*2.8 J/m2 for Cu/Mo, *1.1 J/m2 for Cu/Nb, and *1.2 J/m2 for Cu/Zr NMFs. Furthermore, a linear relationship between the adhesion energy and the interfacial shear strength is clearly demonstrated for the Cu-based NMFs, which is highly indicative of the applicability and reliability of the modified models.  相似文献   

18.
A 17 vol% SiCp/Al–Mg–Si–Cu composite plate with a thickness of 3 mm was successfully friction stir welded(FSWed) at a very high welding speed of 2000 mm/min for the first time. Microstructural observation indicated that the coarsening of the precipitates was greatly inhibited in the heat-affected zone of the FSW joint at high welding speed, due to the significantly reduced peak temperature and duration at high temperature. Therefore, prominent enhancement of the hardness was achieved at the lowest hardness zone of the FSW joint at this high welding speed, which was similar to that of the nugget zone. Furthermore, the ultimate tensile strength of the joint was as high as 369 MPa, which was much higher than that obtained at low welding speed of 100 mm/min(298 MPa). This study provides an effective method to weld aluminum matrix composite with superior quality and high welding efficiency.  相似文献   

19.
吴玉梅  熊晓云  靳蓉  孙敬民  杨林  罗晓星 《金属学报》2005,10(10):1100-1103
目的: 观察本实验室合成的一种治疗阿尔茨海默氏症(AD)的药物(1-二甲基磷酰基-2, 2, 2 -三氯)-乙基-1-醇烟酸醋(NMF),对体外培养的皮层神经细胞活性的影响以及对海人藻酸(KA)所致的神经损伤的保护作用。方法: 采用体外培养皮层神经元的方法,解剖分离 15 d胚胎小鼠皮层神经细胞, 接种于 96孔板,48 h 后加药并培养 72 h,以 MIT 法 观察 NMF 对小鼠皮层神经细胞活性的影响;同时将接种于 24 孔板的细胞预先给予 NMF,d 3 时加或不加KA处理后,以台盼蓝染色鉴别并计数死、活细胞,可得出细胞的存活率。结果: NMF 明显促进胎鼠皮层神经元活性,其中 NMF1、0. 1、10nmol·L-1促进神经元活性增殖率分别高达 34.7%、37.4%、36. 7%, NMF 明显促进正常胎鼠皮层神经元存活卒,与对照组比较,10nmol·L-1 NMF 对皮层神经元的存活率分别提高 39.3%、73.5%。 NMF能显著 对抗 KA 所致的神经元损伤,与 KA 损伤组相比, NMF0.1、10、10nmol·L-1对损伤皮层神经元的保护率分别为 77.30%、80.10%、84.15%。结论: NMF 明 显促进胎鼠皮层神经元的洁性、提高正常皮层神经元,的存活卒,并能有效地保护KA所致的神经元损伤,提示 NMF 是一种很有潜力的治疗 AD 的药物。  相似文献   

20.
On the basis of energy and shape method for the determination of the valence bond (VB) structures of crystal, the valence bond structure of titanium is redetermined at room temperature and calculated in the whole temperature range of 0-1943K. The outer shell electronic distribution of Ti is e_c~(2.9907) · (s_c~(0.4980) d_c~(2.4927)) ef1.0093 in crystal. The temperature dependences of the VB structures of hcp and bcc phases are the same. The VB structures of hcp and bcc phases monotonically increase or decrease with the increase in temperature, but show discontinuous changes at the phase-transformation temperature 1155K.  相似文献   

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