Gemini阴离子表面活性剂水溶液的界面活性

Gemini阴离子表面活性剂水溶液的界面活性;Gemini阴离子表面活性剂;表面张力;CMC;C20;界面张力     

多元体系油水界面上常见表面活性剂行为的分子动力学模拟

采用分子动力学模拟研究了以十二烷基苯磺酸钠(SDBS)为代表的阴离子型表面活性剂,以十二烷基三甲基溴化铵(DTAB)为代表的阳离子型表面活性剂,以壬基酚聚氧乙烯醚(NPE)为代表的非离子型表面活性剂,以十二烷基二甲基甜菜碱(Betaine)为代表的两性表面活性剂及空白实验.模拟了表面活性剂在油水界面上的行为,考察了表面活性剂分子与石油分子之间的径向分布函数(RDF)、石油分子在竖直方向的均方位移(MSD)、油水界面张力(IFT)、石油层与岩石层之间的相互作用能、石油层的相对浓度在竖直方向的分布及石油分子质心位置随模拟时间的变化关系等,讨论了不同表面活性剂的洗油性能.结果表明:(1)SDBS,NPE和Betaine分子初始状态下呈近似的规律排列,非极性端部分插入油相中,极性端延伸进入水相中;随后表面活性剂的极性端表现出聚集趋势,逐渐形成一个外部亲油内部亲水的一个胶束状粒子,粒子随模拟的进行逐渐融入到油层当中;DTAB从开始的近似规则排列逐渐变为无规排列,但是始终保持亲油端插入到油相中,亲水端位于油水界面上.(2)表面活性剂分子与石油分子之间的相互作用强弱顺序为Betaine≈DTABSDBSNPE.(3)由质心高度和动力过程中的图像截图分析,表面活性剂洗油效果的顺序为BetaineSDBSNPEDTABNone.模拟结果与实际的驱油结果一致,从分子层面上解释了不同表面活性剂洗油的规律.     

由表面活性物质溶液的动界面张力外推求平衡界面张力的研究

表面活性物质溶液的界面张力往往随时间而变,难以测得平衡界面张力J。Kloubek^[1]曾应用经验式:1/(δ_H2O-δ_t)=b/(At^1/2)+1/A,以[1/(δ_H2O-δ_t)]对1/t^1/2作图外推求得溶液的平衡表面张力,但所得结果仅与文献值大致相符。本文从理论上分析该经验式的由来,以及产生偏离的原因,并寻求了解决的办法。     

含硒磺基甜菜碱表面活性剂界面性能的氧化-还原响应行为

硒,作为一种新的氧化-还原响应位点因其良好的生物相容性日益引起人们的关注,然而,对这种新型氧化-还原响应型表面活性剂的研究相对较少,尤其是其界面性能的智能调控。本文以含硒两性离子表面活性剂苄基十一烷基磺基甜菜碱(BSeUSB)为对象,研究了其分子结构、Krafft温度、表/界面张力及发泡和乳化性能的氧化-还原刺激响应行为。发现在极微量的H_2O_2(≤体系总质量的0.056%)氧化下,BSeUSB分子中疏水的―Se―C―键转变成了具有一定亲水能力的Se=O键,表面活性剂从单头单尾的还原态变成了类Bola型的氧化态,导致表面活性剂的Krafft温度由(23.5±0.5)°C下降至0°C以下,5.00 mmol?L~(-1)时的表/界面张力分别从45.15、5.52 mN·m~(-1)升高至61.63、18.38 m N·m~(-1)。宏观上,还原态具有良好的发泡和乳化性能,而氧化态的发泡和乳化能力几乎消失。再次加入极少量还原剂Na_2SO_3(≤体系总质量的0.060%)后,分子的微观结构和溶液性能又可恢复到初始状态。总之,通过极微量H_2O_2和Na_2SO_3的交替加入,我们实现了该表面活性剂界面性能的智能调控。     

餐厨废油制备的生物基两性表面活性剂的油水界面性能

以餐厨废油制备了生物基两性表面活性剂,应用界面张力和动态光散射方法,研究了该生物基两性表面活性剂体系的油水界面性能及在溶液中的聚集行为。 在无外加碱条件下,由餐厨废油制备的表面活性剂表现出良好的界面性能,在50~70 ℃以及pH值为7~12的条件下,均可以将油水界面张力降至超低值(<10^-3 mN/m),在不同的油藏模拟地层水中均保持较好的界面活性;分别在50、-20和4 ℃下保存,其界面活性均未受到明显影响。 在水溶液中形成的聚集体的平均流体力学半径为10~30 nm,无机盐离子的加入可使聚集体的粒径上升。 基于其优良的界面性质和可再生来源,由餐厨废油制备的生物基两性表面活性剂在三次采油方面具有重要的应用价值。     

高分子共混体系界面张力的研究

<正> 在高分子多相体系中,相间界面张力(γ_(12))是微区的重要控制因素,无论是Donatelli,Sperling等提出的IPN体系微区尺寸关系式,还是Tokita提出的共混体系中分散相粒径表达式,都含有界面张力因子。 然而,由于高分子体系中界面张力测定的诸多实际困难,当前在国内外非常多的研究工作中,广泛地采用了一些替代的办法,应用较多的有以表面张力差来代替界面张力的Antonow原则延伸及一些近似的计算方法,如Wu及Girifalco和Good提出的由表     

非离子表面活性剂在气液界面的分子动力学模拟

采用分子动力学方法研究了十二烷基醇聚氧乙烯醚系列非离子表面活性剂单分子层在气液界面的微观结构,并通过表面张力的计算考察了表面活性剂分子结构与性能的关系.研究结果表明,随着表面活性剂分子乙氧基基团个数的增加,模拟所得的表面张力的变化趋势与实验一致,所有分子的计算误差在5 mN·m-1以内.同时,随着乙氧基基团数目的增加,...     

阳离子表面活性剂中相微乳的形成和特性

自1943年SdriAn。等人山发现微乳液体系并予以命名以来，对微乳液研究不断深入·微乳液是由油、水、表面活性剂和助表面活性剂组成的各向同性、透明的、热力学稳定的分散体系，微乳液可分为单相微乳液和多相微乳液问．中相微乳液是多相微乳液中，与过剩盐水相和过剩油相达到三相平衡的Winsor皿型微乳液，它在三次采油、日用化工、微环境、酶催化等方面具有特殊重要的应用I‘，‘］．近年来对阴离子表面活性剂中相微乳液的形成和特性进行了较多研究［5。8］．但对阳离子表面活性剂中相微乳液的研究，目前尚未见报导，本文以澳代十四烷基毗…     

正负离子混合表面活性剂双水相界面张力的研究

用旋转滴法测定了正负离子混合表面活性剂形成的双水相界面张力, 研究了双水相界面张力与表面活性剂的分子结构、正负离子表面活性剂的摩尔比、总浓度、外加无机盐及温度的关系. 结果表明, 双水相界面张力在一定正、负离子表面活性剂的摩尔比时属于超低界面张力范围. 观察到三种界面张力曲线类型, 第一类为摩尔比1:1 的两边的两条曲线, 界面张力随过剩表面活性剂组分的比例增加而降低; 第二类为一条跨过摩尔比1:1的马鞍型曲线; 第三类为位于摩尔比1:1的一边的一条马鞍型曲线. 界面张力曲线的类型主要取决于表面活性剂的分子结构, 包括亲水基类型、疏水链长度及对称性.     

表面活性剂双水相界面性质的研究

表面活性剂双水相是指正、负离子表面活性剂混合水溶液在一定浓度及混合比 范围内，自发分离形成的两个互不相溶的水相。前文报道了将其作为一种新型萃取 体系，用于生物活性物质的分离。目前有关其相行为、化学物质和生物大分子的分 配方面已有较多研究，但未见两相之间界面化学性质研究的报道。表面活性剂双水 相的形成是一种奇特的相分离现象，两个稀水溶液（含水量可高达99%以上）互不 相溶、平衡共存，其界面结构和界面张力必有其特殊性。     

OCS表面活性剂在弱碱、无碱条件下的界面张力性能研究

研究了OCS表面活性剂中试产品在弱碱NaCO33及无碱条件下应用于不同油田原油的油-水界面张力特性。结果表明：对于大庆采油四厂原油，当表活剂浓度为0．1％-0．3％，Na2CO3浓度为0．6％-1．2％时，油-水界面张力可达到超低(-l0^-3mN／m数量级)；对于大庆采油二厂原油，当表面活性剂浓度为0．1％-0．3％，Na2CO3浓度为0．8％-1．4％时，油-水界面张力可达到超低；对于华北油田古-联原油，当表面活性剂浓度为0．2％，NaCO3浓度为0．6％-1．2％时，油-水界面张力可达到超低；对于胜利油田孤东采油厂原油，当表面活性剂浓度为0．2％，NaCO3浓度为0．8％-1．4％时，油-水界面张力可达到超低。在无碱条件下，对于大港油田枣园1256断块原油，当OCS表面活性剂浓度达到0．1％时，油-水界面张力即可达到超低；对于江苏油田原油，当OCS表面活性剂浓度在0．1％以上时，油-水界面张力均可以达到10^-2mN／m数量级。聚丙烯酰胺聚合物的加入对油-水超低界面张力的形成和稳定具有促进作用。     

相反电荷聚电解质/表面活性剂体系界面行为研究新进展

介绍了中子反射在相反电荷聚电解质/表面活性剂体系的界面行为研究中的基本原理.在阐述经典的弱相互作用体系的界面吸附行为和表面张力曲线的基础上,分析了聚合物浓度、电解质、表面活性剂疏水基链长对相反电荷聚电解质/表面活性剂体系表面张力曲线的影响,并结合中子反射实验结果,根据相反电荷聚电解质/表面活性剂体系的表面张力曲线是否出现突跃峰,将其界面吸附行为分为两类并提出了两种类型表面张力曲线对应的理论模型.     

钛酸钾晶须界面性质研究

通过乳液聚合的方法对钛酸钾晶须进行表面改性,获得了表面包裹聚甲基丙烯酸甲酯的钛酸钾晶须. FT-IR、SEM、EDS的表征表明,钛酸钾晶须的表面包裹了聚甲基丙烯酸甲酯膜,形成了以钛酸钾晶须为核,聚甲基丙烯酸甲酯为壳的复合粒子.研究表明,改性后的晶须表面能降低,在有机溶液中的界面张力大大降低,与聚甲基丙烯酸甲酯的界面性质相似,说明改性后的晶须基本被聚甲基丙烯酸甲酯完全包裹,因此晶须由亲水性变为疏水性,在有机溶液中的分散性显著提高.     

Interfacial tension and wetting behavior of air/oil/ionic liquid systems

We measured the interfacial tension and the density of air/n-hexane, n-decane, 1-perfluorohexane/1-hexyl-3-methyl-imidazolium hexafluorophosphate systems as a function of temperature. From the air/ionic liquid surface tension values, it was suggested that Coulombic interaction between imidazolium cations and counter anions are not so much different between the surface and bulk. The density values indicated that the decrease of surface tension by saturating organics was closely correlated to the mutual solubility between ionic liquid and organics. Interfacial tension at the oil/ionic liquid interfaces suggested that ionic liquid molecules were more ordered at the oil/ionic liquid interfaces compared to the air/ionic liquid interfaces, but the decrease of the entropy due to the interfacial orientation of ionic liquid was compensated by the increase of the entropy due to the contact of different chemical species. The initial spreading coefficients and the Hamaker constants indicated that all the oil phases spread at the air/ionic liquid interfaces spontaneously, and form the complete wetting films.     

Influence of Gemini Surfactant with Modified TiO2 Nanoparticles on the Interfacial Tension of Oil/Water

The research on the impacts of modified TiO₂ nanoparticles (NPs) on interfacial tension (IFT) is in its infancy. Our work focuses on the IFT of the modified TiO₂ and Gemini surfactant N,N,N′,N′-tetramethyl-N,N′-dimyristyl-1,2-ethane diammonium dichlone (YND1233) complex solutions for reservoir stimulation purposes. The factors of YND1233, modified TiO₂ NPs, temperature, aging stability, adsorption loss, and mineralized degree were explored with the comparison of unmodified TiO₂ NPs and YND1233 as contrast samples. The results indicate that the dynamic IFTs decrease and then increase with the concentrations of YND1233 and modified TiO₂ NPs, and the minimum IFT appears at 0.200 and 0.010 wt%, respectively. YND1233/modified TiO₂ complex solutions show lower and more stable IFTs, better temperature resistance, longer aging time, and lower adsorption on the surface of quartz sand. The modified TiO₂ NPs and YND1233 in the YND1233/modified TiO₂ complex solution can be adsorbed to the interface and decrease the IFTs through synergistic effect. A mixed diffusion-kinetic mechanism is provided for the adsorption and interactions with Ca²⁺/Mg²⁺ involved in YND1233/modified TiO₂ complex solution.     

Interfacial Properties of Aqueous Nonionic Fluorocarbon Surfactant Solutions

The equilibrium, dynamic surface tensions, and surface dilatational elasticity of aqueous solutions of nonionic fluorocarbon surfactant are reported. The critical micellar concentration, CMC (0.023 mM) and equilibrium surface tension (24.6 m N . m^?1) at CMC were measured by Wilhelmy plate method for aqueous solution of C₈F₁₇SO₂N(C₃H₇)(C₂H₄O)_nH (n=20), abbreviated as EF122A. The surface tension decay is slower for C₈F₁₇SO₂N(C₃H₇)(C₂H₄O)_nH (n=10) system, abbreviated as EF122B compared to the EF122A system over short time region, which indicates the slow transport of the surfactant molecules to the surface. The relaxation time for surface tension decay is estimated by fitting a series of exponentials to the dynamic surface tension data and it decreases with temperature for EF122A. Slow exchange of monomers between bulk and interface is reflected in the high elasticity value of the air‐liquid interface for EF122B compared with EF122A within measured frequency window (0.125–1.25 Hz).     

Influence of the non-ionic surfactant PEG-660-12-hydroxy stearate on the surface properties of phospholipid monolayers and their effect on lipid emulsion stability

The effect of the interaction between phospholipid monolayers and PEG-660-12-hydroxy stearate as a non-ionic surfactant on lipid emulsion stability in dynamic and static conditions was studied. The presence of PEG-660-12-hydroxy stearate molecules with phospholipid monolayers (static state) leads to a remarkable increase in the surface pressure (from 5 to 30 mN/m in the initial molecular area), whereas in the dynamic state, when the two emulsifiers are separated and each dissolved in one phase of the two emulsion phases, a sudden decrease in the surface pressures is observed. This indicates that PEG-660-12-hydroxy stearate molecules are intercalated between the phospholipid monolayers forming a molecular mixed film. At the same time, a part of the phospholipid monolayers interacts with the surfactant monomers to form a soluble or partially soluble association complex. This interpretation was also supported by interfacial tension measurements, where the interfacial tension in the dynamic state was lower than that in the static one. This indicates that in static conditions the phospholipids partially interact with PEG-660-12-hydroxy stearate resulting in a non-active association complex. Subsequently there is insufficient utilization of the available surfactants during the emulsification process. In contrast, in dynamic conditions both emulsifiers are available at the free surface from the beginning. This behaviour was substantiated by investigating the stability of emulsions which were prepared either by the static condition or the dynamic one during the autoclaving process. Received: 25 May 1998 Accepted in revised form: 18 September 1998