AOT W/O型微乳液中AOT分子的构象和极性头有效面积的FT-IR研究

运用Fourier变换红外光谱技术对AOT/异辛烷/水油包水型(W/O)微乳液中AOT分子的羰基伸缩振动吸收峰进行最小二乘法曲线分峰拟合. 结果表明AOT分子中酯键上羰基伸缩振动的红外光谱呈现非对称吸收峰, 分别位于(1739±1)和(1725±2) cm^-1, 不同含水量时, 这2个峰与微乳液中AOT分子的trans构象和gauche构象中羰基的不同指向相对应, 2个峰面积的比表明两种不同构象含量的变化. AOT分子的极性头有效面积(A_AOT)随含水量的变化与其两种构象所占的摩尔分数有关.     

水/TX-100/正己醇/正辛烷反相微乳液中水的微环境研究

运用傅立叶变换红外光谱（ＦＴ－ＩＲ）对水／ＴｒｉｔｏｎＸ－１００／正己醇／正辛烷反相微乳液体系中水的微结构进行了研究,结果表明,随着体系加水量的增加,水分子中Ｏ－Ｈ伸缩振动的红外光谱强度在３３６０ｃｍ－１附近增加,而醚上的Ｃ－Ｏ－Ｃ反对称伸缩振动峰则向低频移动,差谱处理后为负峰,对３０３５－３７００ｃｍ－１范围内水分子的羟基伸缩振动峰进行曲线拟合后得到三个子峰,分别位于３５５０±２０ｃｍ－１,３４００±２０ｃｍ－１,３２２０±２０ｃｍ－１,对应着束缚水、结合水、自由水的微环境,并用染料探针对水的微环境加以研究。正己醇的羟基伸缩振动峰无变化说明正己醇在该反相微乳液中与水作用很弱,主要位于反相微乳液的栅状层中。并用电子显微镜对反相微乳液进行了观察。     

聚乙烯吡咯烷酮存在时反相微乳液中水的状态

运用傅立叶变换红外光谱（FTIR）研究不同分子量的聚乙烯吡咯烷酮（PVP）存在时,十二烷基甜菜碱(C12BE)/正庚烷 /正戊醇 /水（Ⅰ）及二（2 乙基）己基磺化琥珀酸钠（AOT）/正庚烷 /水（Ⅱ） 反相微乳液中水的存在状态.采用计算机分峰技术将微乳液中水分子的O－H伸缩振动进行曲线拟合, （Ⅰ）得到三个子峰,分别位于(3560±20)cm－1,(3430±10)cm－1,(3280±10)cm－1附近; （Ⅱ）得到四个子峰,分别位于3618 cm－1, 3550 cm－1, 3446 cm－1和3292 cm－1处.尽管PVP均增溶于W/O型微乳液中表面活性剂分子的极性基团附近,却没有引起长链间自由水的变化.但由于两体系的差异,PVP的存在,导致微乳液（Ⅰ）的本体水减少,结合水增多,却使体系（Ⅱ）的结合水减少,本体水增多.由于W/O型微乳液中水与生物膜中水相似,这些研究有助于理解生物膜界面上的生物化学和生物物理现象.     

水/AOT/正庚烷微乳体系中水结构的FT-IR研究

运用傅立叶变换红外光谱（ＦＴ－ＩＲ）对水／ＡＯＴ／正庚烷微乳体系中水的微结构进行了研究。结果表明，随着体系中加水量的增大，水分子Ｏ－Ｈ伸缩振动的红外光谱由３４９３ｃｍ＾－１向低频移动至３４１７ｃｍ＾－１，微乳体系中，水分子与ＡＯＴ分子的磺酸基作用的同时，与Ｎａ＾＋也有一定的作用，这两种离子对水分子Ｏ－Ｈ键的强度均有一定的影响，磺酸基的作用使水分子中Ｏ－Ｈ伸缩振动向高波数方向移动，而Ｎａ＾＋的作用与     

红外光谱法研究磺化间规聚苯乙烯离聚物离子间相互作用

采用红外光谱法研究了不同金属阳离子及水合作用对磺化间规聚苯乙烯 (SsPS)离聚物阴、阳离子间相互作用的影响 .实验结果表明 :离间相互作用的强弱可通过红外光谱表现出来 ,SsPS离聚物中磺酸根阴离子 (SO-3 )的红外吸收谱带与金属阳离子的性质及离聚物所处的环境有关 .在干燥状态下 ,SsPS离聚物中磺酸根阴离子 (SO-3 )由于受到金属阳离子静电场作用的影响 ,S—O键被极化而使其对称伸缩振动和不对称伸缩振动吸收峰移向高波数 ,移动的幅度与金属阳离子的性质有关 .离聚物吸水后 ,由于水合作用的影响 ,金属阳离子的极化作用减弱 ,因而使S—O键相应的对称伸缩振动和不对称伸缩振动吸收谱带移向低波数 .对于未中和的磺化间规聚苯乙烯 (SsPS H)样品 ,水合作用会使磺酸基团部分离解 ,产生磺酸根阴离子 (SO-3 ) .在干燥状态下 ,磺酸基团仍以—SO3H形式存在 ,红外谱图上出现—SO3H基团的特征吸收     

矿物药金礞石的红外光谱分析

采用傅立叶红外光谱法分析了金礞石试样,对所得图谱进行解析,发现试样的红外光谱具备层状硅酸盐矿物的吸收特征.其吸收带主要分为4个区域:3 700～3 000 cm-1区间的OH伸缩振动吸收,1 620 cm-1左右处的H2O弯曲振动吸收,1 000 cm-1左右处的Si-O伸缩振动吸收和550～400 cm-1区间的Si...     

生物滤池中生物膜和出水悬浮物的元素分析和红外光谱比较

对生物滤池中不同高度的生物膜和出水悬浮物的碳氢氮三元素和红外光谱进行了分析比较.元素分析结果表明,悬浮物的无机成份比生物膜高.悬浮物和生物膜的红外吸收光谱图主要由蛋白质的吸收带、碳水化合物的吸收带组成.1655 cm-1处的吸收峰为酰胺Ⅰ带,是C=O的伸缩振动,1542 cm-1的吸收峰是酰胺Ⅱ带,是N-H的弯曲振动和C-N的伸缩振动,1240 cm-1是酰胺Ⅲ带,是C-N的伸缩振动和N-H的弯曲振动引起的.1460 cm-1处的吸收峰为CH3和CH2的弯曲振动峰.悬浮物的蛋白质特征峰强度比生物膜低,而1050cm-1处的吸收峰强度比生物膜大.     

聚乙烯吡咯烷酮存在时反相微乳液中水的状态 

运用傅立叶变换红外光谱（FTIR）研究不同分子量的聚乙烯吡咯烷酮（PVP）存在时,十二烷基甜菜碱(C12BE)/正庚烷/正戊醇/水（Ⅰ）及二（2-乙基）己基磺化琥珀酸钠（AOT）/正庚烷/水（Ⅱ）反相微乳液中水的存在状态.采用计算机分峰技术将微乳液中水分子的O－H伸缩振动进行曲线拟合,（Ⅰ）得到三个子峰,分别位于(3560±20)cm     

甲烷在MnO2／SiO2催化剂表面吸附的原位FT—IR研究

本文使用付立叶变换红外研究了甲烷在ＭｎＯ２／ＳｉＯ２催化剂表面的吸附，催化剂经高温（７７３Ｋ）抽空处理后，冷却至１７３Ｋ，进２４６６Ｐａ甲烷。在３００８，２９０４和１３０４ｃｍ＾－１吸收峰归属为Ｃ－Ｈ键的对称伸缩振动，这一红外吸收峰的出现说明了甲烷分子的Ｔｄ点群发生畸变，对称性降低。因为红外惰性的２９１７ｃｍ＾－１红外峰显示出红外活性并位移至２９０４ｃｍ＾－１甲烷吸附于ＭｎＯ２／ＳｉＯ２表面后，由     

H2SiCl2分子Si-H振动"基座"SiCl2的有效质量

用傅立叶变换光谱仪和激光腔内吸收光谱仪记录了H2SiCl2分子2000～9000和12000～12900 cm-1的红外吸收光谱.依据局域模理论的非谐性耦合非谐振子(ACAO)模型,分析并拟合了Si-H的对称伸缩振动和反对称伸缩振动,得到描述Si-H伸缩振动的Morse离解能De 、 Morse振子参数α和键振子势能耦合系数frr′.分析中忽略了SiCl2"基座"对Si-H伸缩振动的影响,拟合结果与实验值符合的很好,拟合方差小于 1 cm-1,表明这一近似是可取的.分析拟合结果表明, Si-H振动时"基座"SiCl2的有效质量为75.     

FT-IR studies on the conformation and effective head-group area of AOT molecules in W/O microemulsions

Using Fourier transform infrared(FT-IR) spectroscopy technique, the carbonyl stretching vibration bands of AOT in sodium bis(2-ethylhexyl)sulfosuccinate (AOT)/isooctane/water reverse (W/O) microemulsions system have been investigated by least square curve fitting. The results indicate that an asymmetric adsorbed peak of carbonyl stretching vibration of AOT molecule is situated in (1739 ± 1) and (1725 ± 2) cm-1. The two peaks correspond to different carbonyls in gauche conformation and trans conformation of AOT molecules, respectively. With different water contents (W0), the variations of peak intensity ratio (/= l1739/l1725) reflect the change of the ratio for the two conformation populations and the variations of the effective head-group area of AOT molecule have relations to the ratio of two conformation populations.     

Characteristics of AOT Microemulsion Structure: a Small Angle X-ray Scattering Study

The structure of micelles has attracted renewed attention during the past decade years due to the widespread use of microemulsions in technology1 and life science1,2. To obtain information of the micellar structure, using X-ray scattering (SAXS) whose wavelength is close to the size of the micellar aggregates is one of the most direct method3-5 and SAXS has been proved to be very sensitive for the change of micellar composition6,7. SAXS experiments have been carried out to compare the st…     

Influence of anionic surfactants on the electric percolation of AOT/isooctane/water microemulsions

A study was carried out concerning the influence of sodium alkyl sulfonates on the electric percolation of AOT/isooctane/water microemulsions ([AOT] = 0.5 M and W = [H2O]/[AOT] = 22.2). An important effect was observed with regard to the percolation temperature caused by the addition of small quantities of alkyl sulfonates (rho = [alkyl sulfonate]/[AOT] = 0.01). The short chain alkyl sulfonates (C3-C5) cause an increase in the percolation temperature, which in turn is reduced as we increase the chain length of the additive until we obtain a percolation temperature which is lower than that which is observed in the absence of an additive (C6-C8). For hydrocarbon chains of a greater length we can observe a new increase in the percolation temperature (C10-C18). This behavior has been explained as a consequence of (i) the incorporation of the additives at the interphase of the microemulsion and (ii) the geometric parameters of the different surfactants added to the microemulsion.     

Inclusion-water-cluster in a three-dimensional superlattice of gold nanoparticles

Three-dimensional particle crystals made of dicarboxylic thiolate (MSA)-stabilized gold nanoparticles were formed at an air/water interface. FTIR spectra of this supracrystal showed that three well-resolved peaks existed from 3400 to 3550 cm-1 just falling in a region of OH stretching vibrational mode. Precise analysis showed that all these peaks originated from the water cluster included in the interstice of a particle crystal.     

高岭石结构缺陷的 1H MAS NMR和Raman研究

The structure default of kaolinites was characterized with ¹H MAS NMR and Raman spectra. Although the HI indexes of Suzhou and Maoming kaolinite are similar, their ¹H MAS NMR and Raman spectra are very different. ¹H MAS NMR showed that the hydroxyl proton chemical shifts of Suzhou kaolinite are in the higher field and with larger different between the inner surface hydroxyls protons and inner hydroxyls proton chemical shifts than Maoming kaolinite. Raman spectra showed that the surface hydroxyls stretching vibration bands of Suzhou kaolinite are in the high frequency region, and the half height widths of the bands are 7.0～14 cm^-1. The area ratio S_z/(S_z+S_A), where S_Z and S_A are the areas of bands 3685 cm^-1 and 3695 cm^-1 respectively, is 0.23. But the surface hydroxyls stretching vibration bands of Maoming kaolinite are in the low frequency region, and the half height widths of the bands are 8.9～15.1 cm^-1. The area ratio S_z/(S_z+S_A) is 0.77. Those data proved that Suzhou kaolinite has lower structure default than Maoming kaolinite and ¹H MAS NMR and Raman spectra are effective method for study of kaolinite structure default.     

Fluorescent behavior of B-phycoerythrin in microemulsions of aerosol OT/water/isooctane

Taking advantage of its unusual fluorescent properties, the incorporation of B-phycoerythrin (B-PE) in aerosol OT (AOT, sodium bis-(2-ethylhexyl) sulphosuccinate)/water/isooctane microemulsions was investigated by following their steady-state and time-resolved fluorescence as a function of the water-to-surfactant molar ratio, w(0). The fluorescent intensity at 575 nm increased continuously with increasing water content, saturating at a w(0) around 35 and staying practically constant at w(0)> or =40. The steady-state anisotropy showed an initial increase with increasing water content until w(0)=23 and then decreased strongly, staying practically constant when w(0)> or =40. The values of the fluorescent parameters, anisotropy and fluorescent intensity, were unchanged when the water content of the system increased in the range between w(0)=40 to 50. This implies the effective incorporation of B-PE in the microemulsion droplets with w(0)> or =40, as well as the equilibrium of the dispersion at these water/surfactant ratios, since higher water content does not affect the main surrounding microenvironment of the protein. The overall incorporation in the microemulsion droplets caused minor spectroscopic changes with respect to biliprotein in aqueous solution of 20 mM sodium phosphate buffer, pH 7.0, such as a blue absorption shift of 3 nm and an emission shift of 1.5 nm, as well as a slight increase in excitation anisotropy spectrum mainly caused by a decrease in protein mobility. Therefore, there are no important interactions between the chromophores and the AOT sulfonate head groups. Emission intensity decays followed complex kinetics in both aqueous and dispersion media. The stability with time and temperature of the biliprotein in the microemulsion was higher than in the aqueous solution. All the results can be explained in terms of B-PE inclusion in the water droplets of AOT microemulsions where the protein has similar configuration and conformation to that in aqueous solution but with the chromophores more protected.     

Spectral characteristics of 2-(4'-N,N-dimethylaminophenyl)pyrido[3,4-d]imidazole in AOT/n-heptane/water reverse micelles.

Spectral characteristics of 2-(4'-N,N-dimethylaminophenyl)pyrido[3,4-d]imidazole (DMAPPI) have been studied in AOT/n-heptane/water reverse micelles at w0 > or = 0. Absorption, fluorescence excitation and fluorescence spectra have revealed that the monocation (MC) of DMAPPI, protonated at the imidazole nitrogen (MC2) (Scheme 2) is present in the S0 state at w0 = 0, along with the MC, protonated at pyridine nitrogen (MC3) and only normal emission is observed from both MC2 and MC3. With increase in w0 (water amount), the equilibrium is shifted towards the MC, protonated at -NMe2 group (MC1) and MC3 in the S0 state. Biprotonic phototautomerism is observed in MC1 to generate MC2 in the S1 state. The twisted intramolecular charge transfer (TICT) emission replaces the normal emission in MC3. All the MCs are present near the anionic polar head group of AOT in the bound water region.     

Determination of pH in reversed micelles

The pH in the reversed micellar system of di(ethylhexyl) sodium sulfosuccinate (Aerosol OT, AOT) / phosphate buffer solutions/octane was determined by a P-NMR technique, and pHs in the reversed micelles containing buffer solutions other than the phosphate buffer solution were measured by the spectrophotometric method with the aid of Phenol Red. pHs in reversed micelles were found to be substantially determined by the buffer capacity of buffer solutions solubilized into the systems. By means of both the methods, pKa of Phenol Red in the systems was found to be 7.7, which is almost consistent with that in water. Analysis of Na-NMR spectra indicates that the mobility of the sodium ion of AOT is independent of the molar ratio of water to AOT when the ratio is above 7 and is restricted strongly by the interaction with the sulfonate group of AOT. The relationship between pH and the mobility of the sodium ion was discussed on the basis of the data of Na-NMR spectra.     

FT-IR investigation of the acetamide state in AOT reversed micelles

The state of acetamide nanoparticles encapsulated in the hydrophilic core of sodium bis(2-ethylhexyl) sulfosuccinate (AOT) reversed micelles and dispersed in CCl ₄ has been investigated by Fourier transform infrared spectroscopy. The analysis of the vibrational spectra reveals even at the higher acetamide to AOT molar ratio some changes of the typical H-bonded structure of solid acetamide ascribable to their small size, confinement effects, and acetamide-AOT head group interactions. The stretching modes of acetamide CO and AOT sulfonate groups indicate unambiguously specific acetamide-AOT head group interactions.