Lin H N, Li S, Wang G, Brumbaugh E E, Huang C
Department of Biochemistry, University of Virginia, Charlottesville 22908, USA.
Biochim Biophys Acta. 1996 Sep 4;1283(2):199-206. doi: 10.1016/0005-2736(96)00093-4.
In this study, we have semisynthesized the following three molecular species of mixed-chain phosphatidylethanolamine: C(22):C(12)PE, C(16):C(18:1 delta 9)PE, and C(10):C(24:1 delta 15)PE. These lipids share a common structural characteristic, that is, they all have the same total number of carbon atoms in their acyl chains. Aqueous dispersions prepared from three sets of binary lipid mixtures, C(16):C(18:1 delta 9)PE/C(22):C(12)PE, C(10):C(24:1 delta 15)PE/C(22):C(12)PE, and C(16):C(18:1 delta 9)PE/C(10):C(24:1 delta 15)PE, were studied by high-resolution differential scanning calorimetry, leading to the construction of three temperature-composition phase diagrams. A computer program developed on the basis of the thermodynamic equations for non-ideality of mixing (or Brigg-Williams approximation) was applied to fit the calorimetric data, yielding the non-ideality parameters of mixing in the gel and the liquid-crystalline bilayers (pG and pL). Based on the shapes of these phase diagrams and the values of pG and pL, it is concluded that any two of the three molecular species of phosphatidylethanolamines under study can mix nearly ideally in the bilayer plane of the liquid-crystalline bilayer. However, these binary lipid mixtures do exhibit the gel-gel phase immiscibility over an extensive compositional region in the gel-state bilayer. By comparison with experimental data obtained with binary mixtures of saturated identical-chain phospholipids, we can conclude that mixed-chain cis-monounsaturated lipid molecules and saturated lipid molecules are highly demixed in the same two-dimensional plane of the gel-state bilayer, although the bilayer thickness difference between the lipid bilayer composed of cis-monounsaturated lipids and that of saturated lipids may be only one or two C-C bond lengths at T < Tm.
在本研究中,我们半合成了以下三种混合链磷脂酰乙醇胺分子物种:C(22):C(12)PE、C(16):C(18:1 Δ9)PE和C(10):C(24:1 Δ15)PE。这些脂质具有一个共同的结构特征,即它们的酰基链中碳原子总数相同。由三组二元脂质混合物C(16):C(18:1 Δ9)PE/C(22):C(12)PE、C(10):C(24:1 Δ15)PE/C(22):C(12)PE和C(16):C(18:1 Δ9)PE/C(10):C(24:1 Δ15)PE制备的水分散体,通过高分辨率差示扫描量热法进行了研究,从而构建了三个温度-组成相图。基于混合非理想性的热力学方程(或布里格-威廉姆斯近似)开发的计算机程序被用于拟合量热数据,得出凝胶态和液晶双层中的混合非理想性参数(pG和pL)。根据这些相图的形状以及pG和pL的值,可以得出结论,所研究的三种磷脂酰乙醇胺分子物种中的任意两种在液晶双层的双层平面中几乎可以理想混合。然而,这些二元脂质混合物在凝胶态双层的广泛组成区域内确实表现出凝胶-凝胶相不混溶性。通过与饱和同链磷脂二元混合物获得的实验数据进行比较,我们可以得出结论,混合链顺式单不饱和脂质分子和饱和脂质分子在凝胶态双层的同一二维平面中高度分离,尽管在T < Tm时,由顺式单不饱和脂质组成的脂质双层与饱和脂质双层之间的双层厚度差异可能仅为一两个C-C键长。