Claessens M M A E, van Oort B F, Leermakers F A M, Hoekstra F A, Cohen Stuart M A
Laboratory of Physical Chemistry and Colloid Science, and Laboratory of Plant Physiology, Wageningen University, Wageningen, The Netherlands.
Biophys J. 2004 Dec;87(6):3882-93. doi: 10.1529/biophysj.103.036772. Epub 2004 Sep 17.
The swelling behavior of charged phospholipids in pure water is completely different from that of neutral or isoelectric phospholipids. It was therefore suggested in the past that, instead of multilamellar phases, vesicles represent the stable structures of charged lipids in excess water. In this article, we show that this might indeed be the case for dioleoylphosphatidylglycerol and even for dioleoylphosphatidylcholine in certain salts. The size of the vesicles formed by these lipids depends on the phospholipid concentration in a way that has been predicted in the literature for vesicles of which the curvature energy is compensated for by translational entropy and a renormalization of the bending moduli (entropic stabilization). Self-consistent field calculations on charged bilayers show that the mean bending modulus kc and the Gaussian bending modulus k have opposite sign and /k/>kc, especially at low ionic strength. This has the implication that the energy needed to curve the bilayer into a closed vesicle Eves=4pi(2kc+k) is much less than one would expect based on the value of kc alone. As a result, Eves can relatively easily be entropically compensated. The radii of vesicles that are stabilized by entropy are expected to depend on the membrane persistence length and thus on kc. Experiments in which the vesicle size is studied as a function of the salt and the salt concentration correlate well with self-consistent field predictions of kc as a function of ionic strength.
带电磷脂在纯水中的膨胀行为与中性或等电磷脂完全不同。因此,过去有人提出,囊泡而非多层相代表了过量水中带电脂质的稳定结构。在本文中,我们表明对于二油酰磷脂酰甘油,甚至在某些盐存在下的二油酰磷脂酰胆碱,情况确实如此。由这些脂质形成的囊泡大小取决于磷脂浓度,其方式与文献中预测的囊泡情况一致,即囊泡的曲率能量由平移熵和弯曲模量的重整化(熵稳定化)来补偿。对带电双层的自洽场计算表明,平均弯曲模量kc和高斯弯曲模量k符号相反,且|k|>kc,尤其是在低离子强度下。这意味着将双层弯曲成封闭囊泡所需的能量Eves = 4π(2kc + k)远小于仅基于kc值所预期的能量。结果,Eves可以相对容易地通过熵来补偿。预计由熵稳定的囊泡半径取决于膜持久长度,从而取决于kc。研究囊泡大小随盐和盐浓度变化的实验与kc作为离子强度函数的自洽场预测结果吻合良好。