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.     

Effect of lanthanum ions on tRNAphe structure: Imino proton NMR spectroscopy

The effect of lanthanum ions on the structural and conformational change of yeast tRNA Phe was studied by 1H NMR. The results suggest that the tertiary base pair (G-15)(C-48), which was located in the terminal in the augmented dihydrouridine helix (D-helix), was markedly affected by adding La 3+ and shifted 0.33 downfield. Based pair (U-8)(A-14), which is associated with a tertiary interaction, links the base of the acceptor stem to the D-stem and anchors the elbow of the L structure, shifted 0.20 upfield. Another imino proton that may be affected by La 3+ in tRNA Phe is the tertiary base pair (G-19)(C-56). The assignment of this resonance is tentative since it is located in the region of highly overlapping resonances between 12.6 and 12.2. This base pair helps to anchor the D-loop to the TΨC loop.     

用边界层理论计算平底闸孔出流的流量

应用边界层理论,对闸孔出流的水力计算方法进行了分析,得出了用边界层厚度表示的流量计算的表达式。该计算式物理意义明确、计算简单,经验证与试验结果一致。     

旋风除尘器内锥形扩口芯管对其性能的影响分析和实验研究

用平衡粒径模型分析了旋风除尘器内常用的柱菜芯管结构存在的缺陷,提出了用带锥形扩口和十字板的芯管改进旋风除尘器的内部芯管结构,并用实验研究测得了新型结构减阻效的幅度。     

马尔柯夫链状预测的概率计算及拓广

提出了一种马尔柯夫链状预测中的概率计算新方法：状态划分矩阵法;具有模糊状态的马尔柯夫链的概率计算公式,并用实例计算作了说明。     

红藻藻胆体内部蛋白间的能量传递研究 Ⅰ.人工合成R-PE/R-PC/APC复合物内的能量传递

研究了人工合成的藻胆体模拟复合物的时间分辨荧光光谱,并运用多指数拟合的方法对数据进行了详细的处理和分析,结果表明能量在Ｒ－ＰＥ和Ｒ－ＰＣ之间的传递时间与能量从Ｒ－ＰＣ传递到ＡＰＣ的时间几乎相等（５０ｐｓ）;除此之外,Ｒ－ＰＥ到ＡＰＣ还有两种能量传递的通道,能量在这两个通道的传递时间分别为１１０ｐｓ和４００ｐｓ．即：蛋白之间的能量传递通道是并行的．     

电站凝汽器汽相流动与传热特性的准三维数值分析

为了研究凝汽器流动与传热特性沿轴向的变化,文中发展出一个凝汽器汽相流动与传热特性的准三维数值计算方法,应用该方法对一大型凝汽器汽相流动与传热特性进行了数值模拟．计算结果表明,单流程凝汽器冷却水温度沿流向的变化对蒸汽流动与传热的三维特性会产生明显的影响．     

卟啉—酞菁二元化合物分子内的能量传递

研究了新的以哌嗪连接的含卟啉－酞菁双发色团的分子（Ｐｒ－Ｐｃ）的时间分辨荧光光谱并对所得的结果进行了分析和讨论．在光谱数据的基础上结合分子的结构对非极性溶剂中二元化合物分子内的能量传递过程和机制进行了讨论,并算出发色团的空间相对距离为１．８７ｎｍ．     

半胱氨酸组成的二肽与锌络合的研究(部分二)用电位滴定法研究二肽和锌络合物的结构(英文)

利用电位滴定法测定了溶液中二肽Ｈ－Ｃｙｓ－Ｃｙｓ－ＯＥｔ（１）的ｐＫａ值以及它的锌络合物的稳定常数和组分分布,从而推断出锌络合物的结构