Moreau P, van Effenterre D, Navailles L, Nallet F, Roux D
Centre de recherche Paul-Pascal, Université Bordeaux-1 CNRS, 115 avenue du Docteur-Schweitzer, Pessac, France.
Eur Phys J E Soft Matter. 2008 Jul;26(3):225-34. doi: 10.1140/epje/i2007-10318-9. Epub 2008 May 7.
The dynamic behaviour of three hydrophilic probes (two dyes and one fluorescently-labelled protein) inserted in the water layers of lyotropic lamellar phases has been studied by confocal fluorescence recovery experiments. Two different, ionic (AOT/NaCl/ H(2)O and non-ionic ( C(12)E(5) /hexanol/ H(2)O host systems were studied. The confinement effect has been carefully monitored using the swelling properties of the lamellar phases. In all cases, we measure the evolution of the probe diffusion coefficient in the layer plane D ( perpendicular) versus the separation between the membranes d(w). Depending on the composition of the lamellar phase, this distance can be continuously adjusted from 500A to about 20A. For all systems, we observe a first regime, called dilute regime, where the diffusion coefficient decreases almost linearly with 1/d (w) . In this regime, the Faxén theory for the friction coefficient of a spherical particle symmetrically dragged between two rigid walls can largely explain our results. More unexpectedly, when the membranes are non-ionic, and also quite flexible ( C(12)E(5) /hexanol in water), we observe the existence of a second, concentrated (or confined) regime, where the diffusion coefficient is nearly constant and different from zero for membrane separations smaller than the particle size. This new regime can be heuristically explained by simple arguments taking into account the membrane fluidity.
通过共聚焦荧光恢复实验研究了插入溶致层状相水层中的三种亲水性探针(两种染料和一种荧光标记蛋白)的动力学行为。研究了两种不同的体系,离子型(AOT/NaCl/H₂O)和非离子型(C₁₂E₅/己醇/H₂O)主体体系。利用层状相的溶胀特性仔细监测了限制效应。在所有情况下,我们测量了探针在层平面内的扩散系数D(垂直方向)与膜间距离d(w)的关系。根据层状相的组成,该距离可在500埃至约20埃之间连续调节。对于所有体系,我们观察到一种初始状态,称为稀溶液状态,其中扩散系数几乎随1/d(w)线性下降。在这种状态下,关于球形粒子在两个刚性壁之间对称拖动时摩擦系数的法克森理论能够很好地解释我们的结果。更出乎意料的是,当膜为非离子型且相当灵活(水中的C₁₂E₅/己醇)时,我们观察到存在第二种状态,即浓溶液(或受限)状态,其中对于膜间距小于粒子尺寸的情况,扩散系数几乎恒定且不为零。考虑到膜的流动性,这个新状态可以通过简单的论据进行直观解释。