Crossing in the magnetic force-gap hysteresis curve of magnetic levitation systems with a high-Tc superconductor

For the magnetic levitation system consisting of a high-T_c superconductor and permanent magnet, the relation curve of magnetic force with gap between these two components is known as a hysteresis loop, that is, the approaching and departing portions envelop a complete one, and generally these two portions do not cross each other. However, in some special cases this crossing arises, and makes the complete loop broken. In this paper, by the numerical simulation of the magnetic force-gap curve in large numbers of physical and geometrical parameters, two typical crossings were found. To investigate the crossing and explore its physical causes, for one of the crossings, the current density in the superconductor was further calculated and its magnitude and vector distribution at the gaps nearby where the crossing arises were obtained. Based on these calculation results and an adequate discussion, the conclusion was induced that the crossing in the magnetic force-gap hysteresis curve results from applied magnetic field’s incomplete and insufficient penetrating in superconductor.     

Study on the electrochemical performance of LiNi0.5Mn1.5O4 with different precursor

LiNi_0.5Mn_1.5O₄ cathodes were synthesized by three different raw materials at high temperature. The samples were characterized by X-ray diffraction and scanning electron microscopy tests, respectively. The results indicate that the synthesized samples show pure spinel structure, and the samples synthesized by nickel?Cmanganese hydrate and nickel?Cmanganese oxide show regular geometrical shape. The electrochemical performance of sample synthesized by nickel?Cmanganese oxide is best. The first discharge capacity is 141 mAh/g, and the capacity retention is 98.6% after 50 cycles at 0.5?C rate. The discharge capacity at 5?C rate is still 120 mAh/g. Better crystallization, smaller specific surface area, and lower polarization may be responsible for the excellent electrochemical performance of the LiNi_0.5Mn_1.5O₄.     

Direct yaw-moment control for 4WID electric vehicle via finite-time control technique

This paper is concerned with the yaw-moment stabilization for four-wheel independent-drive electric vehicle. A second-order sliding mode observer is first designed to estimate the required sideslip angle in a finite time. Then, the finite-time control technique and nonlinear disturbance observer are applied to construct the upper controller to drive both yaw rate and sideslip angle to their desired values. Finally, the lower controller is developed to distribute the torques to the independent four wheels according to the desired yaw moment obtained by the given upper controller. Comparisons among linear, discontinuous and nonsmooth controllers under different working conditions are given by using CarSim software.     

Effect of Li2CO3 addition on the structural,optical, ferroelectric,and electric-field-induced strain of lead-free BNKT-based ceramics

In this work, we reported the effect of Li₂CO₃ addition on the structural, optical, ferroelectric properties and electric-field-induced strain of Bi_0.5(Na,K)_0.5TiO₃ (BNKT) solid solution with CaZrO₃ ceramics. Both rhombohedral and tetragonal structures were distorted after adding Lithium (Li). The band gap values decreased from 2.91 to 2.69 eV for 5 mol% Li-addition. The maximum polarization and remanent polarization decreased from 49.66 μC/cm² to 27.11 μC/cm² and from 22.93 μC/cm² to 5.35 μC/cm² for un-doped and 5 mol% Li- addition BNKT ceramics, respectively. The maximum S_max/E_max value was 567 pm/V at 2 mol% Li₂CO₃ access. We expected this work will help to understand the role of A-site dopant in lead-free ferroelectric BNKT materials.     

基于柔性多羧酸配体H3TCOPM构筑的Co(Ⅱ)配合物的合成与结构

以三苯甲烷-4,4’,4"-三羧酸（H₃TCOPM）为主配体,以含氮二齿配体4,4’-bipyridine（4,4’-bipy）为辅助配体,与Co（NO₃）₂·6H₂O通过溶剂热反应得到了2个配位聚合物{[Co₂（α-OH-TCOPM）（OH）（H₂O）₄]·DMF}_n（1）（α-OH-H₃TCOPM=三苯甲醇-4,4’,4"-三羧酸）和{[Co₃（α-OH-TCOPM）₂（4,4’-bipy）₃（H₂O）₆]·2H₂O}_n（2）。晶体结构分析表明,配合物1为四边形的二维层状结构,而配合物2为二维网状结构。采用红外光谱、粉末X射线衍射对配合物进行了表征,用热重分析仪研究了其热稳定性。     

芳香基羧酸根桥联的双核铜（Ⅱ）配合物研究

以具有芳香基团的3-（9-甲基-芴基）-丙酸（FluCO₂H）和N-咔唑基丙酸（CarbCO₂H）为配体,合成了5种具有双核铜结构的配合物[Cu₂（FluCO₂）₄（CH₃OH）₂]（1）,[Cu₂（FluCO₂）₄（DMF）₂]（2）,[Cu₂（FluCO₂）₄（4,4’-bipy）₂]_n（3）,[Cu₂（CarbCO₂）₄（CH₃CN）₂]（4）,[Cu₂（CarbCO₂）₃（2,2’-bipy）₂]ClO₄（5）。晶体结构测试表明：配合物1,2和4都具有羧酸桥联的车轮状结构单元,其结构单元轴向位置分别由甲醇,二甲基甲酰胺和乙腈分子占据。配合物3中,车轮状双核铜结构单元通过4,4’-联吡啶连接构成一维链。配合物5的双核铜结构单元则是通过三个羧酸桥联形成。     

多孔软硬磁Ni0.5Zn0.5Fe2O4/SrFe12O19复合纤维制备及吸波性能

通过静电纺丝技术制备了多孔软硬磁Ni_0.5Zn_0.5Fe₂O₄/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（R_L）值达到-31.9 dB,在2~18 GHz频率范围内,R_L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。     

Pt负载钙钛石催化剂上氧空位对CO氧化的促进作用

采用柠檬酸法制备了LaMnO₃、LaFeO₃、La_0.5Sr_0.5MnO₃、La_0.5Sr_0.5FeO₃,通过负载纳米Pt合成了Pt负载钙钛石催化剂,XRD与IR数据表明合成的催化剂具有钙钛石相,TEM数据表明合成的纳米Pt粒径为~3 nm,均匀分散在钙钛石上。在CO氧化反应中,发现钙钛石的氧化-还原性能是影响其活性的重要因素,因而,Mn系钙钛石表现出较高的CO氧化活性。负载纳米Pt后,Fe系钙钛石则显示出更优异的CO氧化活性,CO完全转化的温度从350 ℃降至120 ℃。吸附实验表明钙钛石上氧空位对促进O₂的吸附起着非常重要的作用,也是影响CO低温氧化的重要因素之一。     

1,4-对苯二甲酸根桥联的镉(Ⅱ)配位聚合物研究

使用2-溴-1,4-对苯二甲酸和2-氨基-1,4-对苯二甲酸为配体,在溶剂热条件下得到了两个结构新颖的化合物Cd(BrBDC)(py) (1)和Cd(NH₂BDC)(H₂O) (2)。单晶结构测试表明:化合物1中,Cd(Ⅱ)离子之间通过羧基连接成一维链,链与链之间通过配体连接成二维平面。化合物2中,Cd(Ⅱ)离子之间通过羧基连接成砖块结构的二维层,层与层之间通过氨基连接成三维结构。对化合物的荧光性质进行了表征。     

二茂铁取代卟啉的合成表征及电化学性质

通过吡咯与二茂铁甲醛和对甲基苯甲醛的直接交叉缩合反应,合成并成功分离了6个含有0~4个二茂铁取代基的卟啉化合物:5,10,15,20-四(4-甲苯基)卟啉[(CH3Ph)4PH2]、5-(二茂铁基)-10,15,20-三(4-甲苯基)卟啉[Fc(CH3Ph)3PH2]、cis-5,10-二(二茂铁基)-15,20-二(4-甲苯基)卟啉[cis-Fc2(CH3Ph)2PH2]、trans-5,15-二(二茂铁基)-10,20-二(4-甲苯基)卟啉[trans-Fc2(CH3Ph)2PH2]、5,10,15-三(二茂铁基)-20-(4-甲苯基)卟啉[Fc3(CH3Ph)PH2]、5,10,15,20-四(二茂铁基)卟啉[Fc4PH2]。用紫外-可见和红外光谱、核磁共振及质谱等技术对卟啉化合物进行了表征,用微量光谱滴定法测定了化合物在非水溶剂中的质子化反应常数,研究了它们的电化学和光谱电化学性质。结果表明,二茂铁取代基对化合物的光谱及氧化还原电位有较大的影响。