多孔介质中甲烷水合物的生成特性的实验研究

在定容的条件下,实验研究了甲烷水合物在不同的多孔介质中的生成特性,所使用的多孔介质平均孔径为9.03,12.95,17.96与33.20 nm,其中孔径为12.95 nm的多孔介质使用了三个粒径范围,分别为0.105～0.150 mm,0.150～0.200 mm,0.300～0.450 mm;其他孔径的多孔介质的粒径...     

3A分子筛对四氢呋喃水合物生成过程的影响

用显微镜从微观角度研究了0℃以下常压四氢呋喃-水体系中加入3A分子筛粉后THF水合物的生成过程,结果表明3A分子筛的存在能诱发水合物的成核,促进THF水合物的生成,提高THF水合物的生长速率;有3A分子筛存在时,THF水合物晶体的生长速率介于0．01～0．05gm／s之间;相对于无3A分子筛存在的体系,THF水合物晶体的生长速率提高约4nm／s;在相同条件下,THF水合物晶体长成后大晶体还会发生部分变化和重组。     

甲烷水合物在静态体系中生成反应的促进

静态体系生成甲烷水合物是个缓慢的、不完全的过程。即使使用表面活性剂也不能实现反应物的100％转化。本文讨论了在静态反应停止后,使用系统温度振荡的方法来促进水合反应的继续进行,直至完全转化。在系统温度从-10～4℃之间周期振荡时,原本停滞的水合反应在水的相变温度附近又开始发生反应,由于水合物合成时铠甲效应的存在,水在样品中的过冷度达到10℃左右。文中对样品的热物性测试表明,在经过几个温度变化周期后,反应非常完全,反应器中样品是100％的甲烷水合物。     

气体分子对甲烷水合物稳定性的影响

通过B3LYP方法, 在6-31G(d,p)水平下, 分别优化了结构I型甲烷水合物十二面体和十四面体晶穴结构. 结果表明, CH4分子使晶穴的相互作用能降低, 增强了晶穴的稳定性. 计算了晶穴中甲烷分子C—H键的对称伸缩振动频率, 计算结果与实验值相符合. 研究发现CH4分子影响晶穴中氧原子的电荷分布, 从而增强了氢键的稳定性. 通过分子动力学方法研究水合物晶胞中气体分子的占有率对水合物稳定性的影响, 进一步说明气体分子对水合物晶穴稳定性的重要作用.     

石英砂中甲烷水合物稳定条件研究

采用不同粒径(160～200目、200～300目、300～400目、400～600目)细颗粒石英砂模拟自然界中沉积物实验合成甲烷水合物, 采用多步升温分解法测定了甲烷水合物的稳定温度-压力(p～T)条件. 结果发现细颗粒石英砂对甲烷水合物的稳定条件有明显影响, 温度最大下降1.5 K. 其中160～200目的石英砂是实验测试条件下石英砂对甲烷水合物稳定条件有无影响的分界目数. 每一种石英砂在不同的温度压力下甲烷水合物p-T数据点较为离散, 并且不同石英砂中p-T数据曲线出现交叉, 这与文献中采用规则的硅胶、玻璃球等测得的结果有所不同. 文献中测定的甲烷水合物p-T数据点温度相对于纯水中甲烷水合物p-T数据点温度向左偏移量相同.     

水合物生成条件下甲烷在水中的吸附

采用悬滴法系统地测定了温度274.2 ~ 282.2 K、压力0.1 ~ 10.1 MPa下甲烷/纯水间界面张力。实验结果表明在恒定温度下界面张力随压力的增加而增大。在高压条件下,压力对界面张力有很大的影响。不同温度和压力下计算出的甲烷在水中的表面过剩浓度结果表明,压力越高,温度越低,甲烷在水溶液中的吸附浓度越高。同时,计算出的甲烷在水溶液中的表面吸附自由能结果表明,在水合物生成条件下,甲烷在水中的吸附比298.2 K更容易。     

磁场特性与作用方式对HCFC-141b气体水合物生成过程的影响

通过实验研究考察了静态磁场和旋转磁场下磁场特性与作用方式对低压制冷剂HCFC-141b气体水合物生成过程特性影响, 重点研究在不同磁场条件下的气体水合物结晶形态、生成温度和引导时间三个重要因素. 试验结果发现, 适当的旋转磁场对提高水合物生成温度、降低过冷度、减少引导时间、提高生成速度有显著的作用, 使结晶形态混杂致密; 而适当的静态磁场则使水合物形态规整, 有利于提高传热性能.     

甲烷水合物膜生长动力学研究

采用水中悬浮气泡法测定了温度为273.4～279.4 K、压力为3.60～11.90 MPa范围内甲烷微小气泡表面水合物膜生长动力学数据. 应用无因次Gibbs自由能差(－ΔG^exp/RT)作为推动力, 提出了具物理意义的水合物膜生长动力学模型, 并回归得到甲烷水合物膜生长动力学反应级数为1.60, 表观活化能为55.95 kJ•mol^－1, 指前因子为1.65×10¹¹ mm²•s^－1. 同时考察了温度和压力对甲烷水合物膜生长速率的影响.     

热力学抑制剂作用下甲烷水合物分解过程的分子动力学模拟

采用正则系综(NVT)分子动力学方法模拟研究277.0 K、11.45 mol·L-1的热力学抑制剂乙二醇(EG)溶液作用下甲烷水合物分解微观过程. 模拟显示甲烷水合物的分解从甲烷水合物固体表面开始, 逐渐向内部推移, 固态水合物在分解过程中逐渐缩小, 直至消失. 固态水合物的分解从晶格扭曲变形开始, 之后笼形框架结构破裂, 最后形成笼形结构碎片. 同时已经分解的甲烷水合物在外层形成水膜, 包裹里层正在分解的甲烷水合物, 增大里层甲烷水合物分解传质阻力.     

甲烷水合物导热机理的分子动力学模拟

甲烷水合物导热系数是甲烷水合物勘探、开采、储运以及其他应用过程中一个十分重要的物理参数.我们采用平衡分子动力学（EMD）方法Green-Kubo理论计算温度203.15～263.15K、压力范围3～100MPa、晶穴占有率为0～1的sI甲烷水合物的导热系数,采用的水分子模型包括TIP4P、TIP4P-Ew、TIP4P-FQ、TIP4P/2005、TIP4P/Ice.研究了主客体分子、外界温压条件等对甲烷水合物导热性能的影响.研究结果显示甲烷水合物的低导热性能由主体分子构建的sI笼型结构决定,而客体分子进入笼型结构后,使得笼型结构导热性能增强,同时进入笼型结构的客体分子越多,甲烷水合物导热性能越强.研究结果还显示在高温区域（T〉TDebye/3）内不同温度作用下,所有sI水合物具有相似的导热规律.压力对导热系数有一定影响,尤其是在较高压力条件下,压力越高,导热系数越大.而在不同温度和不同压力作用过程中,密度的改变对导热系数的增大或减小几乎没有影响.     

静电场诱导十二烷基硫酸钠结晶行为的研究

用透射电镜、X射线衍射及DSC等方法 十二烷基硫酸钠（SDS）极稀水溶液（溶液介于临界聚集浓度和临界胶束浓度之间）在静电场作用下的结晶行为,静电场作用诱导SDS形成规则的四方单晶与从甲醇中重结晶所得样品的晶体结构相同,DSC结果表明,从有序到无序结构变化的一级相转变热焓相同,但由于电场诱导结晶的晶体较小而表现为转变温度的降低,没有施加静电场处理的样品只具有较低的有序程度。     

亚甲蓝与十二烷基硫酸钠变色反应光谱机理

为从分子水平认识亚甲蓝(MB)分子与大分子之间相互作用机理,应用吸收光谱法研究了MB与十二烷基硫酸钠(SDS)之间相互作用机理,考察了乙醇、氯化钠、羟丙基-β-环糊精以及Triton X-100对相互作用的影响。结果表明:MB与SDS之间能发生相互作用形成复合物产生变色反应,乙醇等对相互作用都有影响。认为MB与SDS变色反应机理是在MB与SDS大分子间发生静电相互作用基础上,结合在SDS有序集合体上MB分子定向聚集所引起的。     

SDS对PEO-PPO-PEO嵌段共聚物溶液行为的影响

对PEO-PPO-PEO（127）三嵌段共聚物的水溶液行为及添加十二烷基硫酸钠（SDS）后对共聚物溶液行为的影响进行了研究．利用荧光探针技术对不同SDS浓度下F127／SDS体系的胶来形成进行研究,并研究了SDS对F127浓溶液凝胶化行为的影响．结果表明：随着SDS浓度的增大,F127稀溶液胶束的形成受到抑制,SDS浓度愈大,形成的胶束结构就愈疏松．对F127浓溶液来说,SDS与F127摩尔比小于2时,体系易于凝胶化;但当SDS浓度增大,其与F127摩尔比大于2时,体系开始难于凝胶化,直至摩尔比大于5时,体系不再形成凝胶．     

十二烷基硫酸钠微乳色谱体系中pH值对其电渗流行为与微结构的影响

以十二烷基硫酸钠(SDS)/正己烷/正丁醇/硼砂微乳液为毛细管电色谱运行研究体系,以甲醇峰为微乳体系电渗流峰(EOF),考察不同pH值条件下微乳体系电渗流出峰时间(tEOF)和变化趋势.以微乳液滴粒径和ξ电位考察pH值对SDS缓冲溶液微乳体系微结构的影响,用微乳体系的电导值分析pH值条件下微乳液滴与氢氧根离子之间的相互...     

Micellization of Sodium Dodecyl Sulfate in Glycerol Aqueous Mixtures

The effect of glycerol on both micellar formation and the structural evolution of the sodium dodecyl sulfate (SDS) aggregates in the context of the action mechanism of the cosolvent has been studied. The critical micelle concentration and the degree of counterion dissociation of the surfactant over a temperature range from 20°C to 40°C were obtained by the conductance method. The thermodynamic parameters of micellization were estimated by using the equilibrium model of micelle formation. The analysis of these parameters indicated that the lower aggregation of the surfactant is mainly due to a minor cohesive energy of the mixed solvent system in relation to the pure water. The effect of glycerol on the mean aggregation number of the micelles of SDS was analyzed by the static quenching method. It was found that the aggregation number decreased with the glycerol content. This reduction in the micellar size seems to be controlled by an increase in the surface area per headgroup, which was ascribed to a participation of glycerol in the micellar solvation layer. Studies on the micropolarity of the aggregates, as sensed by the probe pyrene, indicated that this microenvironmental parameter is almost unaffected by the presence of glycerol in the mixture. However, an increase in the micellar microviscosity at the surface region was observed from the photophysical behavior of two different probes, rhodamine B and auramine O. These results suggest a certain interaction of the cosolvent in the micellar solvation of SDS micelles.     

Photophysical Properties of Ethidium Bromide in Low Concentration of Sodium Dodecyl Sulfate

Sodium dodecyl sulfate (SDS) is widely utilized in biomolecules separation, but high residue SDS in biomolecules samples interfere mass analysis. Ethidium bromide (EtdBr) interacts with SDS, and the formation of EtdBr‐SDS complex at low SDS concentration (0–0.1 %) results a large red shift of the n→π* transition of EtdBr from 480 nm to 530 nm. The ion pairs become non‐emissive and cause low emission intensity. While the concentration of SDS is above 0.1 %, SDS starts aggregating to form micelle. Micelle formation destabilizes the complex and the absorption maxima shift back to 513 nm while emission intensity increases. Based on the change of absorption and emission of EtdBr, a SDS concentration assay was developed. If absorption maximizes at 480 nm, the concentration of SDS of the sample is below 0.005 %. If absorption maximum is at longer wavelength than 480 nm, a second parameter, the ratio of absorbance at 513 nm and 550 nm is introduced. If the ratio is smaller than 1.5, the concentration of SDS is between 0.01–0.1 %. If the ratio is larger than 1.5, the concentration of SDS is above 0.15 %. Despite the suitable range is small, the lower limit is around the range of no mass interference.     

Intermolecular Interactions in Self-Assembly Process of Sodium Dodecyl Sulfate by Vertically Polarized Raman Spectra

Molecular self-assembly is extremely important in many fields, but the characterization of their corresponding intermolecular interactions is still lacking. The C-H stretching Raman band can reflect the hydrophobic interactions during the self-assembly process of sodium dodecyl sulfate (SDS) in aqueous solutions. However, the Raman spectra in this region are seriously overlapped by the OH stretching band of water. In this work, vertically polarized Raman spectra were used to improve the detection sensitivity of spectra of C-H region for the first time. The spectral results showed that the first critical micelle concentration and the second critical micelle concentration of SDS in water were 8.5 and 69 mmol/L, respectively, which were consistent with the results given by surface tension measurements. Because of the high sensitivity of vertically polarized Raman spectra, the critical micelle concentration of SDS in a relatively high concentration of salt solution could be obtained in our experiment. The two critical concentrations of SDS in 100 mmol/L NaCl solution were recorded to be 1.8 and 16.5 mmol/L, respectively. Through comparing the spectra and surface tension of SDS in water and in NaCl solution, the self-assembly process in bulk phase and at interface were discussed. The interactions among salt ions, SDS and water molecules were also analyzed. These results demonstrated the vertically polarized Raman spectra could be employed to study the self-assembly process of SDS in water.     

十二烷基磺酸钠对大豆过氧化物酶活性和构象的影响

在不同的pH值体系中, 利用酶活测量、圆二色谱、荧光谱和电子吸收谱研究了十二烷基磺酸钠(SDS)对大豆过氧化物酶(SBP)活性与构象的影响情况. 在pH 2.6和4.2 的体系中, 少量的SDS分子可通过静电作用与SBP结合, 进而与SBP分子中的His169残基结合, 降低其与铁卟啉的配位能力, 使其Soret吸收带蓝移, 二级结构发生轻微的变动, 活性永久丧失. 在pH 5.2体系中, SDS和SBP分子都带负电, 由于静电排斥作用, SDS无法进入SBP的分子内部, 失去与SBP分子中His169残基结合的能力, 对SBP分子的二级结构没有影响, 仅对SBP分子的三级结构有所影响. 当SDS的浓度大于临界胶束浓度时, 由于胶束与SBP的静电排斥作用增强, 限制了铁卟啉中乙烯基的运动, 乙烯基与卟啉环的共轭程度增大, Soret 吸收带红移. 由于SBP活性可完全恢复, 此变化是可逆的.     

十二烷基硫酸钠水溶液的动态表面吸附性质

利用MPTC型气泡压力张仪研究了十二烷基硫酸钠(SDS)溶液在不同NaCl 浓度下的动态表面吸附性质, 分析了离子型表面活性剂在表面吸附层和胶束中形成双电层结构产生表面电荷对动态表面扩散过程和胶束性质的影响. 结果表明, SDS在表面吸附过程中, 表面电荷的存在会产生5.5 kJ·mol^-1的吸附势垒(E_a), 显著降低十二烷基硫酸根离子(DS^-)的有效扩散系数(D_eff). 十二烷基硫酸根离子的有效扩散系数与自扩散系数(D)的比值(D_eff/D)仅为0.013, 这表明SDS与非离子型表面活性剂不同, 在吸附初期为混合动力控制吸附机制. 加入NaCl可以降低吸附势垒. 当加入不小于80 mmol·L^-1 NaCl后, E_a小于0.3 kJ·mol^-1, D_eff/D在0.8-1.2之间, 表现出与非离子型表面活性剂相同的扩散控制吸附机制. 同时, 通过分析SDS胶束溶液的动态表面张力获得了表征胶束解体速度的常数(k₂). 发现随着NaCl 浓度的增大, k₂减小, 表明SDS胶束表面电荷的存在会增加十二烷基硫酸根离子间的排斥力, 促进胶束解体.     

A Simple and Highly Selective Determination of Telmisartan at Sodium Dodecyl Sulfate Modified Pyrolytic Graphite Surface

A simple, facile, selective and cost effective electrochemical method is proposed for the determination of telmisartan (TMS); a drug used for hypertension. A sodium dodecyl sulfate (SDS) modified edge plane pyrolytic graphite (EPPG) is prepared by simple immersion of EPPG in SDS solution at concentration greater than critical micelle concentration (CMC). The modified sensor exhibited superior sensing properties towards the oxidation of TMS. The modified surface was characterized by using the Energy dispersive X‐ray analysis, Field Emission Scanning Electron Microscopy, Electrochemical Impedance Spectroscopy and cyclic voltammetry. The quantitative investigations of the TMS were performed by applying the square wave voltammetry. The micelles of SDS form a pseudo complex with cation radical of TMS and catalyse the oxidation. The proposed sensor shows the linear calibration plot in the concentration range of 5–100 μM with sensitivity 0.2983 μA/μM and the limit of the detection of the sensor was found to be 0.082 μM. The specificity of the developed sensor was also evaluated in the presence of commonly present interfering substances in biological samples. The amount of TMS excreted in urine of the patients undergoing treatment has also been determined. The proposed method can be effectively applied for the investigation of TMS in pharmaceutical formulations and biological samples.