Xu H, Huang C H
Biochemistry. 1987 Feb 24;26(4):1036-43. doi: 10.1021/bi00378a009.
The asymmetric C(18):C(10)PC molecules are known by X-ray diffraction to self-assemble, in excess water, into a lamellar structure known as the mixed interdigitated bilayer at T less than Tm. In this structure, the long C(18)-acyl chain is interdigitated fully across the entire hydrocarbon width of the bilayer, while the shorter C(10)-acyl chain, which is about half as long as the C(18)-acyl chain, packs end to end with a C(10)-acyl chain of another lipid molecule in the opposing bilayer leaflet. We have synthesized the following asymmetric phosphatidylcholines (PC's): C(16):C(9)PC, C(16):C(10)PC, C(18):C(10)PC, C(18):C(11)PC, C(20):C(11)PC, C(20):C(12)PC, C(22):C(12)PC, C(22):C(13)PC, C(8):C(18)PC, and C(10):C(22)PC. These 10 asymmetric phosphatidylcholines have a common characteristic; i.e., the length of the longer extended acyl chain is about twice as long as that of the shorter acyl chain. On the basis of the known lamellar structure of C(18):C(10)PC, we anticipate that these asymmetric phosphatidylcholines will also form mixed interdigitated bilayers. We have employed high-resolution differential scanning calorimetry (DSC) to investigate the thermotropic behavior of liposomes prepared from these asymmetric phosphatidylcholines. If our anticipation is correct, one would find that the thermodynamic data (Tm, delta H, or delta S) associated with the main thermal phase transitions of these asymmetric phosphatidylcholine dispersions will fit into a continuous curve as they are plotted as a function of the hydrocarbon width of the putative mixed interdigitated bilayer. Experimental data presented in this paper indeed bear this out. For comparison, a DSC study of multilamellar dispersions prepared from a series of saturated symmetric phosphatidylcholines has also been carried out.(ABSTRACT TRUNCATED AT 250 WORDS)
通过X射线衍射可知,不对称的C(18):C(10)磷脂酰胆碱(PC)分子在过量水中于温度T低于熔点(Tm)时会自组装成一种称为混合交错双层的层状结构。在这种结构中,长的C(18) - 酰基链在双层的整个烃类宽度上完全交错,而较短的C(10) - 酰基链长度约为C(18) - 酰基链的一半,它与相对双层小叶中另一个脂质分子的C(10) - 酰基链端对端堆积。我们合成了以下不对称磷脂酰胆碱(PC):C(16):C(9)PC、C(16):C(10)PC、C(18):C(10)PC、C(18):C(11)PC、C(20):C(11)PC、C(20):C(12)PC、C(22):C(12)PC、C(22):C(13)PC、C(8):C(18)PC和C(10):C(22)PC。这10种不对称磷脂酰胆碱有一个共同特征,即较长伸展酰基链的长度约为较短酰基链的两倍。基于已知的C(18):C(10)PC的层状结构,我们预计这些不对称磷脂酰胆碱也会形成混合交错双层。我们采用高分辨率差示扫描量热法(DSC)来研究由这些不对称磷脂酰胆碱制备的脂质体的热致行为。如果我们的预期正确,那么人们会发现与这些不对称磷脂酰胆碱分散体的主要热相变相关的热力学数据(Tm、ΔH或ΔS)在作为假定混合交错双层的烃类宽度的函数绘制时将拟合为一条连续曲线。本文给出的实验数据确实证实了这一点。作为比较,还对由一系列饱和对称磷脂酰胆碱制备的多层分散体进行了DSC研究。(摘要截短于250字)