Virtanen J A, Ruonala M, Vauhkonen M, Somerharju P
Department of Medical Chemistry, University of Helsinki, Finland.
Biochemistry. 1995 Sep 12;34(36):11568-81. doi: 10.1021/bi00036a033.
The lateral organization of fluid cholesterol-dimyristoylphosphatidylcholine (DMPC) bilayers was studied by measuring the response of fluorescent membrane probes, dipyrenylphosphatidylcholines (diPyrxPCs) or merocyanine 540, to the variation of cholesterol concentration. Parallel absorbance and light-scattering measurements were also carried out. The excimer-to-monomer ratio of diPyrxPCs displayed abrupt deviations at particular cholesterol mole fractions (CMFs). The most notable of these occurred at CMFs of 0.15, 0.33, and 0.67. Deviations were also frequently observed at CMFs of 0.12, 0.20, 0.25, and 0.40. Merocyanine 540 reproducibly reported deviations at CMFs of 0.15 and 0.33 and frequently reported values close to 0.12, 0.20, and 0.25. In absorbance (turbidity) and light scattering versus CMF plots, well-defined kinks were observed at CMFs of 0.16, 0.33, 0.52, and 0.67. The occurrence of kinks or other deviations at those particular CMFs is most readily explained in terms of a superlattice model previously developed to explain the lateral distribution of pyrenylphospholipids in bilayers [Somerharju, et al. (1985) Biochemistry 24, 2773-2781; Virtanen, J. A., et al. (1988) J. Mol. Electron. 4, 233-236]. This model is based on the assumptions that (i) each cholesterol molecule replaces a single acyl chain in a hexagonal lattice, (ii) cholesterol molecules, because of their larger size, perturb the lattice, (iii) this perturbation is minimized when the cholesterol molecules are maximally separated from each other, and (iv) the maximal separation is achieved when the cholesterol molecules form a hexagonal or centered rectangular superlattice. All detected critical CMFs, except that at CMF 0.67, are predicted by the model, thus strongly supporting its validity. The critical CMF at 0.67 is a limiting case, which can be accounted for by assuming that cholesterol and phospholipid molecules form alternating rows, i.e., formation of a cholesterol superlattice with rectangular symmetry. As predicted by the superlattice model, composition-driven order-to-disorder transitions occur between the critical CMFs, as indicated by increased data scatter and sample fluctuations in those regions. Another important prediction of the superlattice model is that domains with different cholesterol superlattices should coexist at most cholesterol concentrations. Such domains do not have to be extensive to account for the critical events observed here; rather, they are expected to be dynamic entities of limited size. It is very likely that such microscopic domains with distinct cholesterol superlattices also coexist in biological membranes. This is expected to have remarkable effects on both the structure and functions of these membranes.
通过测量荧光膜探针二芘基磷脂酰胆碱(diPyrxPCs)或部花青540对胆固醇浓度变化的响应,研究了流体胆固醇 - 二肉豆蔻酰磷脂酰胆碱(DMPC)双层膜的横向组织。还进行了平行吸光度和光散射测量。diPyrxPCs的准分子与单体比率在特定的胆固醇摩尔分数(CMF)处显示出突然的偏差。其中最显著的偏差发生在CMF为0.15、0.33和0.67时。在CMF为0.12、0.20、0.25和0.40时也经常观察到偏差。部花青540在CMF为0.15和0.33时可重复地报告偏差,并且经常报告接近0.12、0.20和0.25的值。在吸光度(浊度)和光散射与CMF的关系图中,在CMF为0.16、0.33、0.52和0.67时观察到明确的拐点。根据先前为解释双层膜中芘基磷脂的横向分布而开发的超晶格模型[Somerharju等人(1985年)《生物化学》24卷,2773 - 2781页;Virtanen,J. A.等人(1988年)《分子电子学杂志》4卷,233 - 236页],最容易解释这些特定CMF处拐点或其他偏差的出现。该模型基于以下假设:(i)每个胆固醇分子在六边形晶格中取代单个酰基链;(ii)胆固醇分子由于其较大的尺寸会扰乱晶格;(iii)当胆固醇分子彼此最大程度分离时,这种扰动最小化;(iv)当胆固醇分子形成六边形或中心矩形超晶格时达到最大分离。除了CMF为0.67处的临界值外,该模型预测了所有检测到的临界CMF,从而有力地支持了其有效性。CMF为0.67处的临界值是一个极限情况,可以通过假设胆固醇和磷脂分子形成交替行来解释,即形成具有矩形对称性的胆固醇超晶格。如超晶格模型所预测的,在临界CMF之间发生了由组成驱动的有序 - 无序转变,这些区域中数据散射增加和样品波动表明了这一点。超晶格模型的另一个重要预测是,在大多数胆固醇浓度下,具有不同胆固醇超晶格的区域应该共存。这样的区域不一定广泛到足以解释此处观察到的临界事件;相反,它们预计是有限大小的动态实体。很可能这种具有不同胆固醇超晶格的微观区域也共存于生物膜中。预计这将对这些膜的结构和功能产生显著影响。