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The Dynamics of Water Molecules Confined in the Interior of DMPC Phospholipid Reverse Micelle

机译:局限性在DMPC磷脂反转胶束内部限制的水分子动态

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6.1 Introduction Amphiphilic molecules like surfactants and lipids exhibit a variety of phases in aqueous environment. They undergo self-association under specific conditions to form aggregates such as vesicles, bilayers, micelles, etc. [1-5]. The geometrical form of these aggregates is a consequence of a delicate balance between two opposing forces. The attractive tail-tail hydrophobic interaction is the driving force for the aggregation of surfactant molecules, whereas the electrostatic repulsion between the head group sets a lower limit on the size that an aggregate can attain. A typical micelle is spherical with the hydrophilic "head" regions in contact with surrounding environment, sequestering the hydrophobic single-tail regions in the micelle center. Micelles have been the subject of intense interest for several decades, both from a fundamental physical chemistry point of view and because of their widespread applications in detergent, cosmetic, pharmaceutical, and food industries. In some nonpolar solvents can be formed the spherical aggregates of amphipathic molecules with the hydrophobic part of each molecule pointing outward. These aggregates are called reverse micelles because of the reverse of the situation in normal micelles. Reverse micelles have recently garnered significant attention as model systems to explore the effects of confinement [6-9]. Confined environments occur naturally in many biologically important systems as well as a range of physically interesting materials such as porous glasses. The beauty of the reverse micelle is that it is easily created, shows substantial stability, and provides a well-characterized nanoscale pool for a range of chemistries. In recent years, the molecular dynamics (MD) computer simulation method has become a popular way to study micelles [5, 9-31], because of its ability to simulate phenomena at the atomic scale on very short time periods. In this work we have used MD technique to detailed study of the dynamics
机译:6.1引言含有表面活性剂和脂质等两亲分子在水性环境中表现出各种相。它们在特定条件下进行自我关联,以形成囊泡,双层,胶束等聚集体。[1-5]。这些聚集体的几何形式是两个相对的力之间的微妙平衡的结果。有吸引力的尾部疏水性相互作用是表面活性剂分子聚集的驱动力,而头部基团之间的静电排斥率为聚集体可以达到的尺寸的下限设定下限。典型的胶束是与周围环境接触的亲水性“头部”区域球形,在胶束中心中的疏水单尾区域进行隔离。胶束已经是几十年来强烈兴趣的主题,无论是来自基本的物理化学的观点,也是因为它们在洗涤剂,化妆品,制药和食品工业中的广泛应用。在一些非极性溶剂中,可以用每个分子的疏水部分形成两性分子的球形聚集体。由于正常胶束的情况相反,这些聚集体称为反向胶束。反向胶束最近作为模型系统获得了重大关注,以探索限制的影响[6-9]。狭窄的环境在许多生物学上重要的系统中自然发生,以及一系列物理上有趣的材料,例如多孔玻璃。反向胶束的美是易于创建的,显示出大量稳定性,并为一系列化学物质提供了一种特征的纳米级游戏。近年来,分子动力学(MD)计算机仿真方法已成为研究胶束[5,9-31]的流行方式,因为它能够在非常短的时间段内模拟原子尺度上的现象。在这项工作中,我们使用MD技术对动态的详细研究

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