也谈“用惠斯通电桥测电阻”实验

本文主要对杨介信、陈国英编写《普通物理实验(二、电磁学部分)》“用惠斯通电桥测电阻”实验中δR_(x0)=(R_4/R_3)δR_2的含意等五个问题,提出自己的不同看法。     

层流中粉尘的火焰传播速度

建立了筛落式粉尘火焰试验装置和火焰信的号光电测量系统。提出确定火焰前沿位置的“最大斜率切线法”和判定火焰传播稳定性的“相对入射能量法”。测定了硅钙粉和煤粉的火焰传播速度和火焰厚度。结果表明数据合理,测量装置和方法可用于速度范围很宽的粉尘火焰传播研究,用修正的田中达夫模型计算的硅钙粉层流火焰传播速度与实验值接近。     

XapR蛋白在嗜水气单胞菌抗生素耐药性的功能

研究嗜水气单胞菌（Aeromonas hydrophila） LysR型转录调节因子中XapR蛋白抗生素耐药的调控机制。通过测定嗜水气单胞菌ATCC 7966（野生型菌株）与嗜水气单胞菌ATCC 7966 xapR基因缺失株（ΔxapR）对34种抗生素的最低抑菌浓度,系统地评价xapR基因抗生素耐药性;进一步利用定量蛋白质组学技术,探讨xapR参与嗜水气单胞菌调控的生物过程。结果表明：xapR基因缺失后细菌对头孢孟多的耐药性减弱;xapR基因可调控细菌碳代谢、TCA循环等多种代谢途径,此外还与外膜蛋白、TonB、ABC转运系统等抗性基因的表达密切相关。综上,XapR蛋白可通过调节细菌中心代谢途径以及多个抗性基因改变嗜水气单胞菌的耐药性。     

大跨桥梁分离式三箱梁附加攻角效应研究

为研究附加攻角效应对分离式三箱梁颤振性能的影响,结合节段模型风洞试验和理论计算方法获得初始风攻角下的附加攻角,并通过计算流体动力学（Computational Fluid Dynamics, CFD）数值模拟方法求解初始风攻角下的颤振临界风速. 结果表明,分离式三箱梁的初始风攻角及箱梁之间的横梁对附加攻角有较大影响,节段模型在0°~+7°风攻角下存在十分显著的附加攻角效应,且表现为扭转振幅快速增大的硬颤振. 节段模型自由振动风洞试验难以直接获得分离式三箱梁在小风攻角下的准确颤振临界风速. 对于主跨3?300?m的悬索桥,0°初始风攻角下在颤振失稳前的静风附加攻角达到+7°以上,颤振临界风速大大降低,气弹稳定性得不到充分发挥. 因此,对于采用分离式三箱梁断面的超大跨径桥梁,在抗风设计中应对其附加攻角效应予以重视.     

天竺葵绒毡层发育的细胞学及其与花粉发育的关系

本文应用细胞化学和光镜及电子显微镜技术对天竺葵绒毡层发育的全过程进行了系统研究．发现天竺葵变形绒毡层的发育具有如下特点：（１）绒毡层侵入药室的时间在小孢子大液泡时期;（２）侵入后要经历一个细胞质重建过程,并在较长的一段时间内保持生理活跃状态,合成大量的脂类物质;（３）绒毡层合成的营养物质及自身降解的产物均被花粉吸收利用,物质的吸收通过萌发孔进行．     

负载扰动观测器在SF型矢量控制系统中的应用

文章提出广义逆矩阵来设计离散型状态观测器的方法,用该法设计的观测器,可对SF型矢量控制系统的负载力矩进行估计,再进行前馈补偿。实验证明,该法可有效改善系统的动态性能。     

枪口火焰光电测量方法探讨

该文简述了常用枪口火焰测量的几种方法,对各方法存在的问题下作了系统分析,类比于枪口噪声的测量科学地提出了评价枪口火焰大小及强弱的评价指标,在此基础上提出了一种行之有效的光电测试方法,文中阐明了该方法的原理及系统组成,通过枪口火焰的实弹实验,证明了该方法的可行性。     

The v-v energy transfer of highly vibrationally excited states (I)

The relaxation of the highly vibrationally excited CO (v = 1–8) by CO₂ is studied by timeresolved Fourier transform infrared emission spectroscopy (TR FTIR). 193 nm laser photolysis of the mixture of CHBr₃ with O₂ generates the highly vibrationally excited CO(v) molecules. TR FTIR records the intense infrared emission of CO(v→v-1). The vibrational populations of each level of CO(v) have been determined by the method of spectral simulation. Based on the evolution of the time resolved populations and the differential method, 8 energy transfer rate constants of CO(v = 1–8) to CO₂ molecules areobtained: (5.7±0.1), (5.9±0.1), (5.2±0.2), (3.4±0.2), (2.4±0.3), (2.2±0.4), (2.0±0.4) and (1.8±0.6) (10¹⁴ cm³ · molecule⁻¹ · s⁻¹), respectively. A two-channel energy transfer model can explain the feature of the quenching of CO(v) by CO². For the lower vibrational states of CO, the vibrational energy transfers preferentially to the u³ mode of CO² For the higher levels, the major quenching channel changes to the vibrational energy exchange between CO(v→v-1) and the u¹ mode of CO².     

The v-v energy transfer of highly vibrationally excited states (II)

The vibrational energy transfer from highly vibrationally excited CO to H₂O molecules is studied by time-resolved Fourier transform infrared emission spectroscopy (TR FTIR). Following the 193 nm laser photolysis of CHBr₃ and O₂ the secondary reactions generate CO(v). The infrared emission of CO(v → v−1) is detected by TR FTIR. The excitation of H₂O molecules is not observed. By the method of the spectral simulation and the differential technique, 8 rate constants for CO(v)/H₂O system are obtained: (1.7 ±0.1), (3.4 ±0.2), (6.2 ±0.4), (8.0 ±1.0), (9.0 ±2.0), (12 ±3), (16 ±4) and (18 ±7) (10¹³cm³ · molecule^-1· s^-1). At least two reasons lead to the efficient energy transfer. One is the contributions of the rotational energy to the vibational energy defect and the other is the result of the complex collision. With the SSH andab initio calculations, the quenching mechanism of CO(v) by H₂O is suggested.     

伴随矩阵的若干性质

从特殊矩阵的伴随矩阵的关系考察了伴随矩阵的性质。