聚腺嘌呤苷酸(Poly A)水化过程的傅里叶变换红外光谱研究 Ⅱ. 动态水化及脱水过程的特性

在研究核酸分子水化作用的工作中,前人及作者的前文都是将样品保持在恒温器中,在静态情况下实现湿度平衡。为了使样品能更充分地吸附水分子,我们设计了一个通气系统,使不同湿度的水蒸气连续通过密封样品池,让样品在动态情况下达到湿度平衡。除了水化过程外,对脱水过程的观察、分析也是研究核酸与水的相互作用的不可缺少的一环,但这方面的实验工作却很少。我们通过对Poly A薄膜动态水化和脱水过程中红外光谱的测定,证实了:(1)与静     

萃取剂阴离子水化过程的傅里埃变换红外光谱研究——2-乙基己基膦酸单2-乙基己基酯钠盐-仲辛醇-煤油-水体系

本文应用FT-IR法测定了酸性膦酸酯钠盐有机相的加水过程,用来模拟极浓的电解质溶液,证实了:(1)P 507(钠皂)阴离子的水化效应,并且明确地观察到水化作用发生在阴离子的极性基团P=O,P—O—C和P—O—H上。(2)离子水化作用使得水分子的红外谱带强度增加,对谱带频率也有影响,这一效应在体系中水含量低时(<2％)更为显著。     

水／AOT／正庚烷微乳体系中磺酸根水化作用的FT—IR研究

运用傅立叶变换红外光谱（FT－IR）对水／琥珀酸（乙基已基）磺酸钠（AOT）／正庚烷微乳体系中磺酸根的水化作用进行了研究．由于微乳体系中水分子与表面活性剂分子的相互作用，S＝O对称伸缩振动的红外吸收峰向低频方向移动．体系中的加水量W0（水与AOT的摩尔比）由0.5增大至25时，磺酸根对称伸缩振动的红外吸收峰由1051．39cm－1向低频移动至1046．15cm－1．同时，由于Na 的不对称作用，AOT分子中磺酸根反对称伸缩振动分裂成两个吸收峰，分别位于正215cm-1及1245cm－1附近，两个劈裂峰的距离及各自的峰面积均随体系中加水量的变化而变化，应用二阶导数、傅立叶退卷积及曲线拟会等分辨率增强技术可更清楚地反映出这个二重峰的变化情况．固体AOT分子中碳酸根反对称伸缩振动分裂的两个峰之间频率的差值约为42cm－1，形成微乳液以后，这两个峰的差值变小，W0为20时，这两个峰频率的差值逐渐减小到29cm-1，这些变化与磺酸根的水化程度直接相关     

直链烷烃近红外光谱的温度效应与应用研究

近红外光谱的温度效应已得到关注,在结构分析和定量分析方面得到了尝试.以直链烷烃为例,对烷烃有机体系近红外光谱的温度效应进行了研究.采集了20~60℃范围内五种直链烷烃(正己烷到正癸烷)及其混合物的近红外光谱并进行了对比分析,仅发现某些谱峰的强度随温度发生微小变化.采用交替三线性分解算法对光谱数据进行了解析,考察了光谱的特征以及随温度和结构的变化.结果表明,链端C₂H₅和链中CH₂基团的光谱受温度的影响不同,但其光谱信号的强度与温度之间都具有良好的线性关系,可根据光谱预测体系的温度;两种基团的光谱信号强度与烷烃分子的碳数或两种基团在分子中相对含量都具有良好的线性关系,可用于直链烷烃混合物组成的估算.     

聚腺嘌呤核苷酸在金电极上的吸附氧化

采用微电极循环伏安法和吸附转移溶出伏安法研究了单链多聚腺瞟吟核苷酸Poly(A)在金电极上的伏安行为.重点考察了Poly(A)的吸附和氧化过程.发现Poly(A)分子在金电极表面能够形成多种状态的特性吸附.影响吸附态和吸附强度的主要因素是吸附电势,吸附时间和溶液浓度.在负电位区,随着吸附时间(T_s)的变化,Poly(A)分子在金电极表面发生不同状态的以腺嘌呤碱基为吸附位点的强吸附,这种以腺嘌呤碱基吸附的Poly(A)分子能够在零伏附近给出很强的氧化电流峰和对应的还原峰.     

聚腺嘌呤核苷酸在金电极上的吸附氧化

采用微电极循环伏安法和吸附转移溶出伏安法研究了单链多聚腺嘌呤核苷酸Poly(A)在金电极上的伏安行为。重点了考察了Poly(A)的吸附和氧化过程。发现Poly(A)分子在金电极表面能够形成多种状态的特性吸附。影响吸附态和吸附强度的主要因素是吸附电势, 吸附时间和溶液浓度。在负电位区, 随着吸附时间(t~s)的变化, Poly(A)分子在金电极表面发生不同状态的以腺嘌呤碱基为吸附位点的强吸附, 这种以腺嘌呤碱基吸附的Poly(A)分子能够在零伏附近给出很强的氧化电流峰和对应的还原峰。     

吸附态和溶液相CO在Pt(110)电极上氧化过程的CV和in situ FTIRS 研究

应用电化学原位傅里叶变换红外反射光谱(in situ FTIRS)研究了酸性介质中Pt(110)单晶电极上吸附态CO(COad)和溶液相CO(COsol)的氧化过程.循环伏安测试表明,COsol氧化的峰电位比COad氧化的正移了168mV,其峰电流密度为后者的6.7倍.电化学原位红外光谱检测到CO主要生成线型的吸附态物种(COL),均匀分布在Pt(110)表面上.当溶液中不存在CO时,COL仅在电位高于0.15V才发生氧化.而且,该谱峰在其稳定吸附的电位区间内随电位增加蓝移,Stark系数为30cm-1·V-1;在COL发生氧化的电位区间,其谱峰强度随电位增加减小、峰位红移,线性变化率为-56cm-1·V-1.溶液中饱和CO时,原位红外光谱在-0.05V即可检测到CO2的存在,显示COL起始氧化的电位提前了200mV;电位高于-0.05V,该谱峰即发生红移,对应的线性变化率为-26.5cm-1·V-1.     

抗坏血酸升温氧化过程的二维相关红外光谱分析

采用傅里叶变换红外光谱法 (FTIR)和二维相关分析 (2DCorrelationAnalysis)技术研究了固态抗坏血酸在 2 0℃～ 1 60℃的升温氧化过程。结果表明 :抗坏血酸随着温度升高的红外光谱的特征峰在一维图上变化不明显。借助于二维相关分析 ,不仅提高了谱图的分辨率 ,将一维红外谱图上 1 674cm- 1 处的单峰分解为两个自相关峰 ,显示了抗坏血酸的互变异构体中酮式结构的CO基团和醇式结构的CC基团的振动 ;还揭示了分子内各官能团之间的相互作用 ,反映了在升温氧化过程中这些基团之间的协同关系和变化的先后顺序。抗坏血酸分子中CO、CC和COC基团发生了相互作用 ,其变化的顺序是CC先于COC发生偶极矩的变化 ,最后是CO发生变化 ,此现象与抗坏血酸的氧化反应机理相一致。总之 ,二维相关红外分析可以作为研究抗坏血酸升温氧化过程中结构动态变化的一种新方法 ,也为抗坏血酸在氧化过程中的机理研究提供了一个重要的理论依据。     

X射线衍射测试样品位置对谱线峰位和强度的影响

鉴于X’Pert Pro MRD多晶X射线衍射仪的样品台5维可移动,研究了样品的位置对物相测试中谱线峰强度和峰位的影响.结果表明,样品表面低于或者高于光路中心,都会造成谱图峰位的偏移,对峰强度影响不明显.当样品表面低于光路中心位置时,峰位呈减小趋势.当样品表面高于光路中心位置时,峰位呈增加趋势.当水平位置放置了不同厚度的样品进行批处理测试时,谱线的峰强度会受到最厚的样品的影响,峰位的变化不明显.     

一种苊并杂环有机小分子嵌入DNA的几何学模式研究

利用圆二色谱(CD)、紫外-可见吸收光谱以及荧光光谱等方法对苊并杂环化合物8-氧-8H-苊并[1,2-b]吡咯-9-腈(A1) 与小牛胸腺DNA(CT DNA) 的相互作用进行了研究. 结果表明, 随着n(A1)/n(CT DNA)的变化存在两种不同的几何学结合构型. 当n(A1)/n(CT DNA)值低于0.20时, A1分子与DNA的结合方式是不均一的, 化合物分子以多种角度嵌入到DNA碱基对之间. 表现为A1-DNA复合物的诱导圆二色光谱图上较小的正峰和紫外吸收光谱图缺省等吸收点. DNA的特征圆二色谱图表明, 在n(A1)/n(CT DNA)≤0.20范围内, CT DNA的构象从标准的B型转化为A-like型; 当n(A1)/n(CT DNA)>0.20时, 诱导圆二色光谱由正峰转变为强度大、波形复杂的负峰, 表明A1分子开始堆积到DNA螺旋的表面, 同时DNA的二级结构发生了进一步变化.     

Micro-Raman studies on the conformational behaviors of monosodium glutamate in dehydration process

The conformational behaviors of monosodium glutamate（MSG） in a dehydration process were studied by Micro-Raman spectroscopy in combination with Hartree-Fock calculations using 6-31+G^* method.The dehydration process of the MSG droplet was performed by decreasing the ambient relative humidity（RH）.The intensity ratio of the 935 cm^-1 band to 884 cm^-1 band(I₉₃₅/ I₈₈₄) kept decreasing when RH decreased.By optimizing the geometries with different fixed dihedral angles,the downtrend of(I₉₃₅/ I₈₈₄) is found to be due to the reduction of MSG molecular volume.     

旋光聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸]的合成及静电自组装

以聚(乙烯-alt-马来酸酐)为原料,通过与R-(+)-α-苯乙胺的酰胺化反应,合成了一种新型的旋光聚电解质聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸],利用红外吸收光谱、紫外吸收光谱、核磁共振氢谱和旋光度数据对其结构进行表征.聚[乙烯-alt-R-N-(1-苯乙基)马来酰胺酸]与聚二甲基二烯丙基氯化铵(PDDA)逐层静电自组装过程的紫外跟踪测试结果表明,带相反电荷的聚电解质间能够形成稳定增长的自组装膜,多层膜组装量随双层数指数增大.     

共聚焦拉曼光谱研究过饱和硝酸铵液滴中NH4+, NO3- 和H2O之间的相互作用

将硝酸铵液滴沉积在石英基底上,通过降低该液滴周围环境的相对湿度,测定了该液滴由低浓度直至过饱和状态下高信噪比的拉曼光谱.其中,相对湿度的变化可以精确控制液滴浓度的改变.在相对湿度(RH)由72.1%降低至37.9%的过程中,硝酸铵液滴v1-NO-3峰位保持在1048cm-1,半峰宽为10cm-1.该现象表明NO-3周围的水分子被NH4+取代后不会对v1-NO-3造成影响,说明水分子和NH4+所形成的氢键具有相同的强度.对2500-4000cm-1范围内的拉曼光谱进行成分分析,2890、3090、3140、3220、3402及3507cm-1分别被指认为NH+4伞状弯曲振动的泛频、NH+4伞状弯曲振动与摇摆振动的组合谱带、NH+4的对称伸缩振动、NH+4的反对称伸缩振动、水峰中强氢键成分和弱氢键成分.从拟合结果得出:强氢键在氢键结构中所占百分含量随液滴相对湿度的降低而减少,弱氢键所占百分含量随液滴相对湿度的降低而增加.该变化趋势是NO-3和NH+4之间复杂相互作用的结果.     

Hydration of phosphatidyl serine multilayers and its modulation by conformational change induced by correlated electrostatic interaction.

Hydration of the various residues of phospholipids was inferred from the shift in the wave number of their vibration bands, obtained from the amplitudes of their positive and negative peaks in the difference spectra between those of the hydrated and the dry phospholipid multibilayers. The effect of aligned phospholipid layers on the orientation of their hydrating water molecules was inferred from the dichroic ratio of the OH stretching band, measured by polarized attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) with a germanium prism, as a function of the water-to-lipid ratio in the surface film. The results indicate that about seven water molecules are oriented by one phosphatidyl serine molecule in the surface film. About 8 to 11 additional water molecules contribute to the hydration of the polar residues as revealed by the effect on the difference spectra. The hydration appears to be cooperative. A water molecule that initiates hydration of a site facilitates access of additional water molecules, until the hydration of the whole site composed of many different interacting polar residues is completed.     

Micro-Raman study on the conformation behavior of succinate in supersaturated sodium succinate aerosols

Micro-Raman spectra of supersaturated aerosols of sodium succinate were obtained. The conformation behavior of the succinate dianion as a function of relative humidity (RH) was investigated by combining micro-Raman spectroscopy with theoretical calculations. A shoulder at 968 cm(-1) of the v(C-CO(2)(-)) band on the rise in more concentrated droplets was believed indicative of conformation transformations. The intensity ratio (I(963)/I(997)) of the v(C-CO(2)(-)) band at 963 cm(-1) to the v(C-C) band at 997 cm(-1), versus the molar water-to-solute ratio (WSR), was used to fathom the equilibrium between gauche and trans conformations. Before saturation (WSR = 25.8) for the droplets, the ratio of I(963)/I(997) retains a value of approximately 2.6 independent of WSR, indicating that the equilibrium was not disturbed in the dilute droplets. In supersaturated droplets (WSR < 25.8), however, the ratio sharply decreases from approximately 2.6 to approximately 1.1 at WSR = 9.6, which was attributed to the formation of contact ion pairs (CIPs).     

Raman spectroscopic studies on single supersaturated droplets of sodium and magnesium acetate

Raman spectroscopy was used to study structural changes, in particular, the formation of contact-ion pairs in supersaturated aqueous NaCH(3)COO and Mg(CH(3)COO)(2) droplets at ambient temperatures. The single droplets levitated in an electrodynamic balance (EDB), lost water, and became supersaturated when the relative humidity (RH) decreased. For NaCH(3)COO droplet the water-to-solute molar ratio (WSR) was 3.87 without solidification when water molecules were not enough to fill in the first hydration layer of Na(+), in favor of the formation of contact-ion pairs. However, the symmetric stretching vibration band (nu(3) mode) of free -COO(-) constantly appeared at 1416 cm(-1), and no spectroscopic information related to monodentate, bidentate, or bridge bidentate contact-ion pairs was observed due to the weak interactions between the Na(+) and acetate ion. On the other hand, the band of methyl deformation blue shifted from 1352 to 1370 cm(-1) (at RH = 34.2%, WSR = 2.43), corresponding to the solidification process of a novel metastable phase in the highly supersaturated solutions. With further decreasing RH, a small amount of supersaturated solution still existed and was proposed to be hermetically covered by the metastable phase of the particle. In contrast, the interaction between Mg(2+) and acetate ion is much stronger. When WSR decreased from 21.67 to 2.58 for the Mg(CH(3)COO)(2) droplet, the band of C-C-symmetric stretching (nu(4) mode) had a blue shift from 936 to 947 cm(-1). The intensity of the two new shoulders (approximately 1456 and approximately 1443 cm(-1)) of the nu(3) band of free -COO(-) at 1420 cm(-1) increased with the decrease of WSR. These changes were attributed to the formation of contact-ion pairs with bidentate structures. In particular, the small frequency difference between the shoulder at approximately 1443 cm(-1) and the nu(3) band of the free -COO(-) group (approximately 1420 cm(-1)) was proposed to be related to the formation of a chain structure based on the contact-ion pairs of bridge bidentate. The continuous formation of various contact-ion pairs started at higher WSR value (WSR = 15.5) greatly reduced the hygroscopic properties of Mg(CH(3)COO)(2) droplet, so that the WSR of Mg(CH(3)COO)(2) droplets was even lower than that of NaCH(3)COO in the RH range of 40-60%.     

CF3Br的红外光化学和光物理

We present the optothermal and optoacoustic spectra of CF_3Br in TEA CO_2 laser 00°1—02°0 R branch. Three absorption peaks has been observed at R(14) line (1074.6 cm~(-1)), R(18) line (1077.3cm~(-1)), and R(22) line (1079.9cm~(-1)) respectively. The peak at R(22) coincides with the position of P branch of CF_3Br linear IR spectrum, but two peaks at R(14) and R(18) can be interpreted as the hot bands.We also studied the multiphoton dissociation of CF_3Br and carbon isotope seperation.     

Micro-Raman observation on the HPO4(2-) association structures in an individual dipotassium hydrogen phosphate (K2HPO4) droplet

A single K(2)HPO(4) droplet with size of ～50 μm on a Teflon substrate was forced to enter into the supersaturated state by decreasing the relative humidity (RH), allowing accurate control over the concentration of the solute within a droplet of a nanogram. The K(2)HPO(4) solutions from dilute (0.1-1.0 mol·L(-1) bulk) to concentrated state (a droplet from RH 98.2% to 25.1%) were studied through micro-Raman spectroscopy in the spectral region of about 200-4000 cm(-1). The area ratio between the water stretching band to the sum of the ν(1)-PO(3), ν(2)-POH, and ν(4)-PO(3) bands of the HPO(4)(2-) at various RHs was used to describe the dehydration behavior of a microsized single K(2)HPO(4) droplet in dehumidifying process. The peak position of the v(1)-PO(3) band for the 1 mol·L(-1) bulk solution appeared at 991 cm(-1) and moved to 986 cm(-1) at 98.2% RH, to 978 cm(-1) at 70.2% RH, and then to 964 cm(-1) at 30.0% RH for a droplet, accompanying an increase of the full width at half-height (fwhh) of this peak from 16.3 to 17.2, 22.2, and then to 24.2 cm(-1), indicating transition of the HPO(4)(2-) anions from monomers to dimers/trimers/oligomers and then to polyanions with chain structures in the K(2)HPO(4) solutions. After 25.1% RH, the solid was proved to be K(2)HPO(4)·3H(2)O according to the Raman spectral features. Furthermore, the O-H stretching envelope of a K(2)HPO(4) droplet showed that the intensity ratios of the strong hydrogen bonding component (3255 cm(-1)) to the weak one (3417 cm(-1)) and the cage-like water (2925 cm(-1)) to the weak one (3417 cm(-1)) were sensitive to the HPO(4)(2-) association structures, which can be used to understand the effects of dimers/trimers/oligomers and chain structures of the HPO(4)(2-) associations on the hydrogen bonding of water molecules.     

稀土HEH[EHP]固体配合物的红外光谱

本文制备了La,Ce,Pr,Nd,Sm,Eu,Gd,Tb,Dy,Ho,Er,Tm,Yb,Lu,Y等十五种稀土与2-乙基己基膦酸单(2-乙基己基)酯的固体配合物,测定了4000-100cm~(-1)的FT-IR光谱,对其主要红外光谱吸收带进行了归属。指认150cm~(-1)为Ln-O键的伸缩振动带,250cm~(-1)附近的谱带为COPO,CCPO骨架扭曲振动与Ln-O键的耦合振动带。结果表明配合物为多聚体系,PO_2与稀土离子可能为桥式配位形式。Ln-O键基本上为离子键。