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Monte Carlo simulations of a polyoxyethylene C_(12)E_2 lamellar bilayer in water

机译:水中聚氧乙烯C_(12)E_2层状双层的Monte Carlo模拟

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摘要

The polyoxyethylene C_(12)E_2/water lamellar phase has been modelled as an aqueous region sandwiched by two bilayers. The bilayers were represented as ethoxy chains attached to a hydrocarbon continuum. Initially, the bilayer separation distance was fixed at 24 A, which is a typical experimental value for the surfactant weight fraction of 71%. Both canonical and Gibbs ensemble simulations have been performed on the system at different temperatures ranging from 298.15 K to 353.15 K. In the Gibbs simulations the bilayer separation was allowed to readjust to an equilibrium value. The results are compared and contrasted with previous studies in which single chains (Kong, Y. C, Nicholson, D., Parsonage, N. G., and Thompson, L., 1994, J. chem Soc. Faraday Trans, 90,2375) and charged OH groups (Cracknell, R. F., Nicholson, D., and Parsonage, N. G., 1992, Molec. Phys., 75, 1023), attached to a hydrocarbon substrate, were simulated. As in the previous work with single chains, there is evidence of water bridging which stabilizes certain chain conformations, but in these multichain systems there is competition between intra- and inter-chain bridging. The water structure is substantially modified, in comparison with bulk water, by the presence of the chains, as evidenced by positional and orientational distributions. In the Gibbs ensemble simulations at 298 K, the bilayer separation contracted by about 1.5 A and appeared to have reached equilibrium at this separation after about 4 x 10~7 configurations. At 343.15 K the bilayer separation was still decreasing when the simulation was terminated at 6 x 10~7 configurations. It is concluded that water restructuring plays an important part in stabilizing the lamellar phase, and that a flexible chain model, with multiple binding sites, is necessary in order to account for bilayer stability.
机译:聚氧乙烯C_(12)E_2 /水层状相已建模为被两个双层夹在中间的水相区域。双层表示为与烃连续体相连的乙氧基链。最初,双层分离距离固定为24 A,这是表面活性剂重量分数为71%的典型实验值。已在298.15 K至353.15 K的不同温度下对系统进行了规范和Gibbs集成仿真。在Gibbs仿真中,双层分离允许重新调整为平衡值。将结果与以前的研究进行比较和对比,在以前的研究中,单链(Kong,Y. C,Nicholson,D.,Parsonage,NG和Thompson,L.,1994,J. chem Soc。Faraday Trans,90,2375)模拟了连接到烃底物上的带电OH基团(Cracknell,RF,Nicholson,D。和Parsonage,NG,1992,Molec.Phys。,75,1023)。就像以前关于单链的研究一样,有证据表明水桥可以稳定某些链构象,但是在这些多链系统中,链内和链间桥之间存在竞争。与链状水相比,与散装水相比,水的结构发生了实质性的变化,如位置和方向分布所证明的。在298 K的Gibbs集成模拟中,双层间距收缩了约1.5 A,并且在经过约4 x 10〜7的构形后,在该间距下似乎已达到平衡。在343.15 K下,当模拟以6 x 10〜7的构型终止时,双层分离仍在减小。结论是,水的重组在稳定层状相中起着重要的作用,并且具有多个结合位点的柔性链模型对于说明双层稳定性是必要的。

著录项

  • 来源
    《Molecular physics》 |1996年第3期|p.835-865|共31页
  • 作者单位

    Department of Chemistry, Imperial College of Science, Technology and Medicine, London SW7 2AY, UK;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 分子物理学;
  • 关键词

  • 入库时间 2022-08-18 01:08:12

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