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The structure and kinetics of oil-in-water microemulsions stabilised by nonionic surfactants

机译:非离子表面活性剂稳定的水包油型微乳液的结构和动力学

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摘要

This thesis is concerned with the behaviour of the single phase (10) alkane oil-in- water (01W) microemulsions stabilised by nonionic surfactants of the general structure H-(CH2)n(OCH2CH2)m-OH, abbreviated to CnEm. The aims were to attempt to characterise their behaviour in terms of the effect of the different constituents n, m, and alkane oil chain length (x).Initially the limiting temperature phase boundaries of the 10 region were established by measurements of turbidity. Turbidity was found to be at a minimum at the lower temperature phase boundary (the solubilisation phase boundary, SPB), and at a maximum at the upper temperature phase boundary (UTPB). The temperature position of the 10 region was found to be increased by increasing m or x, and decreased by increasing n. The width of the temperature range was generally found to be decreased by increasing the ratio of oil to surfactant (R). For a series of decane-inwater microemulsions stabilised by surfactants having a constant ratio n/m=2, the SPB was found to be little affected by an increased overall surfactant length, whereas the UTPB was found to be increased.The microemulsion droplet sizes were determined by both static and dynamic light scattering (turbidity and PCS respectively). The particle size was measured at varying temperatures and was found to be at a minimum at the SPB and to increase with temperature (explaining the increase of turbidity with increasing temperature). The increased particle size was assumed to correspond to clustering or growth of the microemulsion droplets. The size measured at the SPB was assumed to be that of the individual droplets at their preferred size. The hydrodynamic radius (rh) of the droplet at the SPB was used to calculate the area (As) occupied per surfactant molecule at the interface between the droplet core and the surfactant monolayer. As was found to be increased by increasing n, and decreased by increasing x, whereas m was found to have little effect.Turbidity measurements were found to be a simple method of measuring the extent of clustering or growth of the droplets with increasing temperature. From this information the equilibrium constant (K) and the associated standard enthalpy, entropy and Gibbs free energy changes were obtained. A simple scheme of droplet aggregation was postulated in which K for the addition of one droplet to an existing cluster (equating to growth by the equivalent of one droplet at the preferred size) was constant regardless of cluster size. The model was found to fit well to a middle range droplet concentration of 0.04 - 0.10 M. Measurements at lower droplet volume fractions were found to be too inaccurate, and K was found to decrease for fractions greater than this range. A model which would accommodate the decrease in K with higher droplet volume fraction would be highly complex and include further estimated parameters. It was therefore deemed appropriate to employ the simple model for comparison within the relevant range of droplet volume fraction. As expected K was found to increase with increasing temperature for all systems. The large positive enthalpy (of the order of 1000 kJmol-1) obtained for all systems accounts for the strong temperature dependence of the behaviour of these microemulsions. The positive entropy change (of the order of 3 JK4mol-1) was attributed to the increasing disorder of the water molecules following dehydration from the surfactant head group region. The removal of water from the head groups has the additional effect of increasing inter-head group and therefore interdroplet attractions thus promoting clustering or growth. The resulting negative Gibbs free energy (of the order of -14 kJmol-1) indicates that the clustering/growth process is spontaneous and entropically driven. The clustering/growth process was found to be dependent on the packing density of the surfactant head groups at the droplet monolayer surface. Assuming clustering occurs the thermodynamic parameters were calculated per mole of surfactant molecules involved in the droplet contact zone of the clusters. Droplets having the more widely spaced (less closely packed) head groups were found to have a larger enthalpy and entropy change, probably as a result of the greater requirement for dehydration of the head groups.A temperature jump method was employed to study the kinetics of the clustering/growth process. The results were found to be consistent with the equilibrium data, in that the rates of the clustering/growth process were found to be dependent on the packing density of the surfactant head groups. Droplets having the less closely packed head groups were found to cluster more slowly, again an indication of the greater difficulty in dehydrating the head groups. The activation energy was also calculated for the clustering/growth process, and was found to be of the order of a few hundred kJmol4, but no discernible trends with molecular structure of the components were observed.
机译:本论文涉及由一般结构为H-(CH2)n(OCH2CH2)m-OH的非离子表面活性剂稳定的单相(10)烷烃水包油(01W)微乳液的行为,缩写为CnEm。目的是试图通过不同组分n,m和烷烃油链长度(x)的影响来表征它们的行为。最初,通过测量浊度来确定10个区域的极限温度相边界。发现在较低温度相界(增溶相界,SPB)处的浊度最小,而在较高温度相界(UTPB)处的浊度最大。发现10个区域的温度位置通过增加m或x来增加,而通过增加n来降低。通常发现温度范围的宽度通过增加油与表面活性剂(R)的比例而减小。对于以恒定比率n / m = 2的表面活性剂稳定的一系列癸烷-水微乳液,发现SPB几乎不受表面活性剂总长度增加的影响,而UTPB却增加了。由静态和动态光散射(分别是浊度和PCS)确定。在不同的温度下测量粒度,发现在SPB处粒度最小,并且随温度增加而增加(说明浊度随温度增加而增加)。假定增加的粒度对应于微乳液液滴的聚集或生长。假设在SPB处测得的大小是各个液滴在其首选大小处的大小。 SPB处的液滴的流体动力学半径(rh)用于计算在液滴核心和表面活性剂单层之间的界面上每个表面活性剂分子所占的面积(As)。发现随着n的增加,α增加,而随着x的增加而减少,而m影响很小。发现浊度测量是一种测量液滴随温度升高而聚集或生长的程度的简单方法。从该信息获得平衡常数(K)以及相关的标准焓,熵和吉布斯自由能变化。提出了一种简单的液滴聚集方案,其中,与簇的大小无关,用于将一个液滴添加到现有簇中的K(等于以优选大小的一个液滴的等效增长)是恒定的。发现该模型非常适合0.04-0.10 M的中间范围液滴浓度。发现较低液滴体积分数的测量太不准确,并且发现分数大于该范围的K减小。一个能够适应较高的液滴体积分数降低K的模型将非常复杂,并包含更多的估计参数。因此,认为在液滴体积分数的相关范围内采用简单模型进行比较是合适的。不出所料,所有系统的K值都随温度的升高而增加。所有系统获得的大正焓(约1000 kJmol-1)说明了这些微乳状液的行为具有很强的温度依赖性。熵的正变化(约为3 JK4mol-1)归因于从表面活性剂头部基团区域脱水后水分子的无序增加。从头组除去水具有增加头间组的额外效果,并因此增加液滴间的吸引力,从而促进聚集或生长。产生的负吉布斯自由能(约-14 kJmol-1)表明聚簇/生长过程是自发的,并且是熵驱动的。发现聚集/生长过程取决于液滴单层表面上表面活性剂头基的堆积密度。假设发生团簇,每摩尔参与团簇的液滴接触区的表面活性剂分子计算热力学参数。发现头基分布较疏(密排较少)的液滴具有较大的焓和熵变化,这可能是由于头基脱水的要求更高所致。采用温度跳跃法研究分子的动力学聚类/增长过程。发现结果与平衡数据一致,因为发现簇化/生长过程的速率取决于表面活性剂头基的堆积密度。发现具有不太紧密堆积的头基的液滴聚集更慢,这再次表明头基脱水更困难。还计算了聚集/生长过程的活化能,发现活化能约为几百kJmol4,但是没有观察到组分分子结构的明显趋势。

著录项

  • 作者

    Morris Jane Susan;

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  • 年度 1995
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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