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层状LiNi1/3Co1/3Mn1/3O2正极材料合成及电化学性能 总被引:1,自引:0,他引:1
首次提出以碳酸盐为沉淀剂,采用共沉淀法制备Ni1/3Co1/3Mn1/3CO3前驱体,再和锂源混合高温固相合成了锂离子蓄电池层状LiNi1/2Co1/3Mn1/3O2正极材料.采用X射线衍射(XRD)和电子扫描电镜(SEM)对Ni1/3Co1/3Mn1/3CO3前驱体和LiNi1/3Co1/3Mn1/3O2正极材料的结构及形貌进行了表征,SEM测试表明LiNi1/3Co1/3Mn1/3O2的形貌近似为球形,且颗粒分布均匀.并对其进行了充放电性能和循环伏安研究,实验结果表明LiNi1/3Co1/3Mn1/3/3O2在25℃、2.5~4.6
V电压范围,0.1 C倍率下,首次放电比容量达182.97 mAh/g. 相似文献
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以LiNO3、Ni(CH3COO)2·4 H2O、Co(CH3COO)2·4 H2O和Mn(CH3COO)2·4 H2O为原料,采用共沉淀-燃烧法在空气中合成了LiNi1/3Co1/3Mn1/3O2.采用原子吸收光谱仪(AAS)、扫描电子显微镜(SEM)、X射线衍射仪(XRD)和充放电测试仪对合成产物的成份、形貌、结构和性能进行了表征.实验结果表明,所合成的正极材料LiNi1/3Co1/3Mn1/3O2结晶良好,粒度适中,大小均匀,具有α-NaFeO2型层状有序结构和良好的电化学性能,在2.5~4.35 V电压区间充放电,其首次放电比容量达到169.05 mAh/g,第50次循环的放电比容量仍有152.83 mAh/g.在深度充电状态下具有良好的结构稳定性. 相似文献
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球形Ni1/3Co1/3Mn1/3(OH)2是控制结晶-固相合成法制备球形LiNi1/3Co1/3Mn1/3O2的前驱体,Ni1/3Co1/3Mn1/3(OH)2的理化指标对LiNi1/3Co1/3Mn1/3O2综合性能具有深刻影响。为提高电池体积比容量,必须首先合成出高致密、晶型结构完整、颗粒形貌为球形的Ni1/3Co1/3Mn1/3(OH)2前驱体。采用络合共沉淀法制备出了高致密球形Ni1/3Co1/3Mn1/3(OH)2前驱体,研究了制备过程中反应温度、氨碱摩尔比、反应体系pH值、搅拌强度、反应周期等五大因素对高致密球形Ni1/3Co1/3Mn1/3(OH)2合成的影响机理。通过合理优化工艺,控制各项因素,制备出了球形、d50=8.5μm左右、振实密度≥2.3 g/cm3的高致密球形Ni1/3Co1/3Mn1/3(OH)2。 相似文献
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层状LiNi1/3Co1/3Mn1/3O2正极材料合成及电化学性能 总被引:1,自引:0,他引:1
首次提出以碳酸盐为沉淀剂,采用共沉淀法制备Ni1/3Co1/3Mn1/3CO3前驱体,再和锂源混合高温固相合成了锂离子蓄电池层状LiNi1/3Co1/3Mn1/3O2正极材料。采用X射线衍射(XRD)和电子扫描电镜(SEM)对Ni1/3Co1/3Mn1/3CO3前驱体和LiNi1/3Co1/3Mn1/3O2正极材料的结构及形貌进行了表征,SEM测试表明LiNi1/3Co1/3Mn1/3O2的形貌近似为球形,且颗粒分布均匀。并对其进行了充放电性能和循环伏安研究,实验结果表明:LiNi1/3Co1/3Mn1/3O2在25℃、2.5"4.6V电压范围,0.1C倍率下,首次放电比容量达182.97mAh/g。 相似文献
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用共沉淀法制备出(Ni1/3Co1/3Mn1/3)(OH)2,与LiOH·H2O混合后,在900℃下焙烧12
h,得到锂离子电池正极材料Li(Ni1/3Co1/3Mn1/3)O2.在2.70~4.35 V,电流为40 mA/g时,循环性能稳定.当截止电压升高到4.60
V时,容量可达190 mAh/g.循环伏安实验表明,材料的结构在循环过程中保持稳定. 相似文献
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Li(Ni1/3Co1/3Mn1/3)1-ySnyO2材料的合成及性能研究 总被引:1,自引:1,他引:0
采用碳酸盐共沉淀法制备Li(Ni1/3Co1/3Mn1/3)1-ySnyO2(y=0,0.01,0.02,0.05,0.10)。通过XRD、SEM测试对其晶型结构、组织形貌进行了分析,交流阻抗法(AC)和充放电性能测试对其电化学性能进行了研究。实验表明,制备的样品均具有较好的层状结构,其中Li(Ni1/3Co1/3Mn1/3)0.98Sn0.02O2性能最佳,以0.5C循环充放电时,首次放电比容量达到173.31mAh/g,30次循环后,放电比容量为149.55mAh/g,容量保持率为86.29%。 相似文献
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使用锰酸锂(LiMn2O4)、镍钴锰酸锂(LiNi1/3 Co1/3Mn1/3O2)混合正极材料和钛酸锂(Li4 Ti5 O12)负极材料,制备了中倍率1865140型锂离子电池.制备的电池在12 min内可充满电池容量的80%以上,且电池表面温度不超过35℃;在室温下以2.00 C循环1 200次,容量保持率高于91%;在高温55℃下以1.00 C循环1 000次,容量保持率高于82%.FreedomCAR混合脉冲功率特性表明:在放电深度(DOD) 10% ~ 70%内、10s脉冲充放电状态下,电池的阻抗都在9 mΩ以下;50%DOD时的10s放电比功率为372 W/kg,充电比功率为520 W/kg. 相似文献
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以溶胶-凝胶法制备氯阴离子掺杂型正极材料LiNi1/3 Co1/3Mn1/3 O2-xClx(x=0、0.05、0.10和0.15).用TG/DTG测试分析了材料的相形成过程.XRD分析结果表明:在空气气氛中以850℃煅烧20 h制备的材料,具有良好的六方单相层状结构.电化学性能测试结果表明:掺杂抑制了高电压区域的相变过程,提高了材料的可逆性;x=0.10的样品具有良好的循环性能和倍率性能,在2.0~4.6V循环,0.15 C、1.00 C首次放电比容量分别为198.7 mAh/g、166.4 mAh/g,第25次0.15 C循环的放电比容量为197.9 mAh/g. 相似文献
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LiNi1/3Co1/4Mn1/3M1/12O2(M=Al,Ti)的性能研究 总被引:1,自引:0,他引:1
采用共沉淀法在800℃下煅烧9
h,制备出了LiNi1/3Co1/4Mn1/3M1/12O2(M=Al,Ti).利用XRD、DSC和充放电分析方法对其进行了表征.实验结果表明LiNi1/3Co1/3Mn1/3O2中Al和Ti的加入,提高了材料LiNi1/3Co1/4Mn1/3M1/12O2(M=Al,Ti)在4.3
V下热分解反应的热稳定性. 相似文献
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Sandwich structured PbZr0.52Ti0.48O3/Pb(Mg1/3 Ta2/3)0.7Ti0.3O3/PbZr0.52Ti0.48O3 (PZT/PMTT/PZT) thin films have been successfully synthesized via a combined route involving sol-gel and RF magnetron sputtering.
Insertion of the PMTT interlayer effectively suppressed formation of the heterogeneous “rosette” structure of PZT thin film
when deposited onto Pt/Ti/SiO2/Si substrate. While both remanent polarization and coercive field were lowered for the sandwich structured films, the coercive
field was reduced more significantly. Such sandwich structured films exhibit improved fatigue behavior and the relative permittivity
can not be simply described as a series connection of individual components of perovskite layers. 相似文献
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M. Antonova L. Shebanovs M. Livinsh J.Y. Yamashita A. Sternberg I. Shorubalko A. Spule 《Journal of Electroceramics》1999,4(1):179-187
Solid solution series of the (1 - x)Pb(Lu1/2Nb1/2)O3 - x PbTiO3 binary system ceramics (PLuNT) were synthesized and hot-pressed (temperature 950°C to 1130°C, pressure 25 MPa); its structure, dielectric and piezoelectric properties were studied. Pure lutecium niobate PLuN (x = 0) has a pronounced long-range order in the B-sublattice and an antiferroelectric to paraelectric phase transition at 258°C. The phase structure of the PLuNT system, at room temperature, changes from a pseudomonoclinic (psd-M, space group Bmm2) to tetragonal (T, space group P4mm). The pseudomonoclinic phase extends over the 0 x 0.38 interval within which the monoclinic angle proceeds a minimum near to 90° at x 0.2. The morphotropic region covers the interval x = 0.38 - 0.49, the concentration ratio psd-M:T 1 (the morphotropic phase boundary—MPB) corresponds to x = 0.41. Within the morphotropic region, a rather strong distortion of the unit cell—(c/a - 1) 0.02, 90.37º, characteristic of hard piezoelectrics is maintained. Dielectric dispersion and broadening of the phase transition, features typical to relaxors, are observed within the concentration interval of 0.1 x 0.3. The highest electromechanical coupling coefficients: kp = 0.66, kt = 0.48, k31 = 0.34 of (1 - x) PLuN–xPT ceramics are attained in compositions near the MPB at x 0.41. Non-isovalent doping of PLuNT with La3+ in Pb sublattice shifts the MPB to lower values of x. 相似文献