Vapour Recoil Effect on a Vapour Liquid System with a Deformable Interface

A new two-sided model of vapour-liquid layer system with a deformable interface is proposed. In this model, the vapour recoil effect on the Marangoni-Bénard instability of a thin evaporating liquid layer can be examined only when the interface deflexion is considered. The instability of a liquid layer undergoing steady evaporation induced by the coupling of vapour recoil effect and the Marangoni effect is analysed using a linear stability theory. We modify and develop the Chebyshev-Tau method to solve the instability problem of a deformable interface system by introducing a new equation at interface boundary. New instability behaviour of the system has been found and the self-amplification mechanism between the evaporation flux and the interface deflexion is discussed.     

血清钙、镁和微量元素与冠心病

综述了钙、镁和微量元素在动脉粥样硬化、冠心病(包括冠状动脉痉挛)研究的相关报道,以进一步研究钙、镁和微量元素与冠状动脉痉挛的关系。     

荧光光谱结合表面增强拉曼光谱法研究紫檀芪与人血清白蛋白相互作用

在模拟人体生理条件下,应用荧光光谱和表面增强拉曼光谱法研究了紫檀芪(PTE)与人血清白蛋白(HSA)之间相互作用机制.结果表明,HSA的荧光能被PTE静态猝灭,并伴随有非辐射能量转移作用,两者形成了1:1复合物,结合距离r=1.495 nm,结合常数KA=1.12×104(298 K)、4.07×104(304 K)和2.45×105 L/mol(310 K).表面增强拉曼光谱研究揭示,PTE分子通过甲氧基与HSA进行结合;热力学数据表明,二者间的作用主要为疏水作用;标记竞争实验指出PTE优先结合HSA的位点Ⅲ.三维荧光光谱、同步荧光光谱和表面增强拉曼光谱结果显示,与PTE作用后,HSA构象发生变化,导致色氨酸残基周围环境疏水性降低,但对PTE分子构象影响不大.     

壬基酚聚氧乙烯醚型Gemini季铵盐表面活性剂的合成 及其表面性质的研究

合成了系列壬基酚聚氧乙烯醚型Gemini季铵盐表面活性剂(GNPQA), 用核磁、红外和元素分析对它们的结构进行了表征, 考察了反应条件对转化率的影响, 并用表面张力法和稳态荧光探针法对GNPQA的表面性能及胶束聚集数(N)进行了研究. 结果表明, 较优的反应条件: 反应时间为12 h, 反应温度为70 ℃, 反应原料摩尔比为n(双聚壬基酚聚氧乙烯醚)∶n(三乙胺)∶n(环氧氯丙烷)＝1∶1∶1; GNPQA的临界胶束浓度(CMC)值较相应的单体壬基酚聚氧乙烯醚型季铵盐表面活性剂(NPQA)降低了1～2个数量级, 显示了较高的表面活性; 当GNPQA溶液浓度为5～9倍CMC时, N值随浓度增大而线性增大; 随着氧乙烯(EO)单元数的增长, GNPQA的CMC和N值均逐渐减小; 结合GNPQA的表面性能参数和N值的变化规律, 探讨了这类表面活性剂表面及胶束聚集体的结构形态.     

Transmission Properties of W3 Y-Branch Filters in Two-Dimensional Photonic Crystal Slabs

A highly efficient W3 Y-branch filter in a two-dimensional photonic crystal slab with triangular lattice of air holes is designed and fabricated, and its transmission properties are measured. By accurately adjusting the size of the resonant cavities, the minimum wavelength spacing of 7 nm between two channels is realized. The corresponding resonant wavelengths of the two cavities agree well with the calculated ones. This implies that this kind of fiIter may be promising in integrated wavelength division multiplexing system.     

利用252 Cf快裂变室测量BC501A液闪探测器的相对探测效率和响应函数

本文利用²⁵²Cf快裂变室和多参数数据采集系统,逐事例的同时记录了自发裂变中子和瞬发伽马的飞行时间(TOF),脉冲形状甄别(PSD)和反冲能量(RE,裂变中子是通过测量反冲质子;瞬发伽马是通过测量康普顿反冲电子)三维信息.详细介绍了通过离线数据分析完全扣除三维信息中的伽马事例贡献,以获得Φ50.8 mm×50.8 mm的BC501A液闪探测器的相对探测效率和响应函数的方法.在不通过探测器响应函数进行数据转换的条件下,利用中子的能量直接确定了中子的有效测量阈值.得到的中子 关键词： 252Cf快裂变室')" href="#">²⁵²Cf快裂变室 BC501A液闪探测器 相对探测效率 响应函数     

中子学积分实验

从６０年代开始，我所就开展了聚变中子积分实验，完成了造氚率、裂变率、穿透率及泄漏中子能谱测量等研究课题。１９８７年以来承担了“８６３”计划的聚变裂变混合堆包层中子学积分实验，开展了Ｂｅ、Ｐｂ的１４ＭｅＶ中子倍增率实验，其中Ｂｅ实验为中、美、日国际合作，实验误差为２．８％，实验结果为理论计算提供积分检验。     

LiF插层对有机发光二极管磁场效应的调控

制备了有LiF插层的有机发光二极管,以八羟基喹啉铝（Alq₃）作为电子传输层,N, N′-二苯基-N, N′-二(1-萘基)-1,1′-联苯-4,4′-二胺（NPB）作为空穴传输层.通过改变Alq₃与NPB间LiF插层的厚度,研究了不同温度下器件的光电特性及电致发光的磁场效应.测量结果表明:LiF插层可以影响器件内部载流子的输运和激发态的形成.较厚的插层阻碍了空穴的传输,使器件的电流效率变低.但实验中发现, 关键词： LiF插层结构 磁场效应 三重态激子     

Fluent数值模拟在制冷与空调领域中的应用

Fluent软件是流体力学中通用性较强的一种商业CFD软件,应用范围很广。主要介绍Fluent在制冷与空调中的应用。Fluent模拟适用于制冷领域等现代技术对过程模拟的要求,同时满足现代化生产设计,是制冷与空调设计的一个重要发展方向。阐述了Fluent模拟仿真在制冷领域的现状及发展概况;重点对Fluent在工艺过程中的模拟作了介绍。利用模型复现实际系统中发生的本质过程,并通过对系统模型的实验来研究存在的或设计中的系统。     

Measurement and analysis of fission rates in a spherical mockup of uranium and polyethylene

Measurements of the reaction rate distribution were carried out using two kinds of Plate Micro Fission Chamber （PMFC）. The first is a depleted uranium chamber and the second an enriched uranium chamber. The material in the depleted uranium chamber is strictly the same as the material in the uranium assembly. With the equation solution to conduct the isotope contribution correction, the fission rate of 238U and 235U were obtained from the fission rate of depleted uranium and enriched uranium. Then, the fission count of 238U and 235U in an individual uranium shell was obtained. In this work, MCNP5 and continuous energy cross sections ENDF/BV.0 were used for the analysis of fission rate distribution and fission count. The calculated results were compared with the experimental ones. The calculation of fission rate of DU and EU were found to agree with the measured ones within 10% except at the positions in polyethylene region and the two positions near the outer surface. Because the fission chamber was not considered in the calculation of the fission counts of 238U and 235U, the calculated results did not agree well with the experimental ones.