Spiker R C, Levin I W
Biochim Biophys Acta. 1976 May 21;433(3):457-68. doi: 10.1016/0005-2736(76)90273-x.
Raman spectroscopic frequency differences between selected carbon-carbon stretching modes of lipid hydrocarbon chains were determined as a function of temperature for use in monitoring lipid phase transition behavior and acyl chain disorder in both multilamellar and single-wall vesicles. Transition temperatures detected by this procedure for pure dipalmitoyl phosphatidylcholine and dimyristoyl phosphatidylcholine multilayers were observed at 39 +/- 1 degrees C and 23 +/- 1 degrees C, respectively. Although the phase transition for unilamellar vesicles of dipalmitoyl phosphatidylcholine occurred at nearly the same temperature as the multilayers, the crystal-liquid crystalline transition for the single-shell vesicles appeared to span a slightly broader temperature range, a characteristic consistent with irregularities in the packing arrangement of the hydrocarbon chains. Within the precision of the Raman spectroscopic method, however, the temperature behavior of both the multilamellar and the unilamellar dimyristoyl phosphatidylcholine assemblies appeared nearly identical. The temperature profile for the Raman frequency differences of an excess water sonicate of 25 mol percent cholesterol in dipalmitoyl phosphatidylcholine served as an example of the effect upon lipid phase transition characteristics of a bilayer component intercalated between the acyl chains. For this particular cholesterol-lipid system the phase transition was broadened over a 30 degrees C temperature range, in contrast to the marrow 2-4 degrees C range observed for pure multilayer and single-shell vesicle particles.
测定了脂质烃链中选定碳-碳伸缩模式之间的拉曼光谱频率差异与温度的函数关系,用于监测多层和单壁囊泡中的脂质相变行为和酰基链无序状态。通过该方法检测到的纯二棕榈酰磷脂酰胆碱和二肉豆蔻酰磷脂酰胆碱多层膜的转变温度分别为39±1℃和23±1℃。虽然二棕榈酰磷脂酰胆碱单层囊泡的相变温度与多层膜几乎相同,但单壳囊泡的晶态-液晶态转变似乎跨越了略宽的温度范围,这一特征与烃链堆积排列的不规则性一致。然而,在拉曼光谱方法的精度范围内,多层和单层二肉豆蔻酰磷脂酰胆碱组装体的温度行为几乎相同。以二棕榈酰磷脂酰胆碱中25摩尔百分比胆固醇的过量水超声处理物的拉曼频率差异的温度曲线为例,说明了插入酰基链之间的双层组分对脂质相变特性的影响。对于这个特定的胆固醇-脂质系统,相变在30℃的温度范围内变宽,而纯多层和单壳囊泡颗粒观察到的狭窄的2-4℃范围则不同。