精确Cosserat弹性杆动力学的分析力学方法

以脱氧核糖核酸和工程中的细长结构为背景, 大变形大范围运动的弹性杆动力学受到关注. 将分析力学方法运用到精确Cosserat弹性杆动力学, 旨在为前者拓展新的应用领域, 为后者提供新的研究方法. 基于平面截面假定, 在弯扭基础上再计及拉压和剪切变形形成精确Cosserat弹性杆模型. 用刚体运动的概念描述弹性杆的变形, 导出弹性杆变形和运动的几何关系; 在定义截面虚位移及其变分法则的基础上, 建立用矢量表达的d’Alembert-Lagrange原理, 在线性本构关系下化作分析力学形式, 并导出Lagrange方程和Nielsen方程, 定义正则变量后化作Hamilton正则方程; 对于只在端部受力的弹性杆静力学, 导出了将守恒量预先嵌入的Lagrange方程, 并讨论了其首次积分. 从弹性杆的d’Alembert-Lagrange原理导出积分变分原理, 在线性本构关系下化作Hamilton原理. 形成的分析力学方法使弹性杆的全部动力学方程具有统一的形式, 为弹性杆动力学的对称性和守恒量的研究及其数值计算铺平道路. 关键词： 精确Cosserat弹性杆 分析动力学方法 变分原理 Lagrange方程     

功能层厚度对叠层有机电致发光器件出光性能影响的数值研究

功能层厚度是影响有机电致发光器件出光效率的主要因素之一,故获得不同功能层厚度对器件出光特性的影响规律是制备高性能器件的重要基础. 本文基于薄膜光学原理、电偶极子辐射理论及Fabry-Pérot微腔原理,建立了结构为glass/ITO/N,N0-bis（naphthalen-1-yl）-N,N0-bis（phenyl）-benzidine（NPB）/tris（8-hydroxyquinoline）aluminum（Alq₃）/molybdenum trioxide（MoO₃）/NPB/Alq₃/Al的叠层有机电致发光器件的光学模型,系统地研究了各个功能层厚度对叠层有机电致发光器件出光强度的影响,得到了功能层厚度对器件出光强度影响的规律. 该模型的建立与所获得的结果可对深入了解叠层有机电致发光器件的工作机理以及制备高性能的器件提供一定的帮助. 关键词： 叠层有机发光器件 出光特性 厚度 数值研究     

Gas source MBE grown wavelength extended 2.2 and 2.5 μm InGaAs PIN photodetectors

Using homo-junction structure and relative thin linear graded In_xGa_1−xAs as the buffer layer, extended wavelength InGaAs PIN photodetectors with cut-off wavelength of 2.2 and 2.5 μm at room temperature have been grown by using GSMBE, and their performance over a wide temperature range have been extensively investigated. For those 2.2 or 2.5 μm detectors with 100 μm diameter, the typical dark current (V_R = 10 mV) and R₀A are 57 nA/10.3 Ω cm² or 67 nA/12.7 Ω cm² at 290 K, and 84 pA/4.70 kΩ cm² or 161 pA/3.12 kΩ cm² at 210 K respectively. The thermal activation energies of the dark current are 0.447 eV or 0.404 eV for 2.2 or 2.5 μm detectors respectively.     

Synthesis of AN-g-casein copolymer in concentrated aqueous solution of sodium thiocyanate and AN-g-casein fiber's structure and property

The main products of graft copolymerization of acrylonitrile (AN) onto casein in concentrated aqueous solution of sodium thiocyanate in homogeneous phase were characterized as a graft copolymer (AN-g-casein) by Fourier transform infrared. The effects of the monomer concentration, initiator concentration, reaction temperature and reaction time on copolymerization were investigated. The result of WAXD showed that the major part of casein in graft copolymer is amorphous. The SDSC determination showed that the lateral order of PAN, the side chain of copolymer, decreases and the lateral order distribution becomes wider with the increase of the casein component in copolymer. It revealed that the two systems of AN-g-casein copolymer are incompatible by an investigation of DMTA, SEM. The two systems of AN-g-casein exist in separating phases, but tie up each other. So the phenomena of characteristic boundary relaxation occur.Direct spinning of graft copolymer in concentrated aqueous solution of sodium thiocyanate in homogeneous phase was successfully carried out. The skin-core layer structure of AN-g-casein fiber cross-section was observed by scanning electron microscope (SEM). In the core layer, the dimension of phase domain of casein is about from 20 to 60 nm. When the fiber was drawn into broken, microfibrillation occurs, the fiber skin layer is compact, and its broken section is flat. Many long and thin casein strips are formed in the surface of the fiber, respective crystalline grade of two components is scarcely effected by the change of the content of casein. AN-g-casein fibers have good hygroscopicity and dyeability, and more, they can be dyed by acidic dyestuff and cationic dyestuff. AN-g-casein fiber still has good mechanical properties, so AN-g-casein fiber is a new type modified “silk-like” fiber for wide application.     

A highly efficient asymmetric Michael addition of anthrone to nitroalkenes with cinchona organocatalysts

A highly efficient asymmetric Michael addition of anthrone to nitroalkenes catalyzed by cinchona alkaloids was described. Up to 99% ee of the corresponding adduct was obtained.     

Resonance-enhanced group delay times in an asymmetric single quantum barrier

It is shown that transmission and reflection group delay times in an asymmetric single quantum barrier are greatly enhanced by the transmission resonance when the energy of incident particles is larger than the height of the barrier. The resonant transmission group delay is of the order of the quasibound state lifetime in the barrier region. The reflection group delay can be either positive or negative, depending on the relative height of the potential energies on the two sides of the barrier. Its magnitude is much larger than the quasibound state lifetime. These predictions have been observed in microwave experiments.     

Ring-opening reactions of diarylvinylidenecyclopropanes by iodine and bromine

Diarylvinylidenecyclopropanes undergo a novel ring-opening reaction upon treatment with iodine or bromine at 0-25 °C in 1,2-dichloroethane to give the corresponding iodinated or brominated naphthalene derivatives in good to high yields within 3 h. The further transformation of the corresponding iodinated or brominated naphthalene derivatives has been disclosed.     

Pulsed field ionisation—ZEKE photoelectron spectrum of o-, m- and p-tolunitrile

Pulsed field ionisation—ZEKE photoelectron spectroscopy has been applied to o-, m- and p-tolunitrile in a supersonic jet. The PFI-ZEKE photoelectron spectra of m- and p-tolunitrile show well-resolved anharmonic structures in the low-frequency region, which are assigned to bands due to internal rotational motion of the methyl group in the cation. Level energies and relative transition intensities are reproduced well by a one-dimensional rotor model with a three-fold axis potential. Potential curves for the internal rotation have been determined. For o-tolunitrile, no band due to internal rotation was found in PFI-ZEKE spectrum. It is suggested that the o-tolunitrile cation has the high barrier for internal rotation and the stable conformation that is the same as that in S₁ and S₀. The barrier height and the conformation are compared with other toluene derivatives, and the relation between the electronic character of –CN and the internal rotational motion has been discussed.