Simon S A, Advani S, McIntosh T J
Department of Neurobiology, Duke University Medical Center, Durham, North Carolina 27710, USA.
Biophys J. 1995 Oct;69(4):1473-83. doi: 10.1016/S0006-3495(95)80017-2.
Bilayer structure and interbilayer repulsive pressure were measured from 5 to 50 degrees C by the osmotic stress/x-ray diffraction method for both gel and liquid crystalline phase lipid bilayers. For gel phase dibehenoylphosphatidylcholine (DBPC) the bilayer thickness and pressure-distance relations were nearly temperature-independent, and at full hydration the equilibrium fluid spacing increased approximately 1 A, from 10 A at 5 degrees C to 11 A at 50 degrees C. In contrast, for liquid crystalline phase egg phosphatidylcholine (EPC), the bilayer thickness, equilibrium fluid spacing, and pressure-distance relation were all markedly temperature-dependent. As the temperature was increased from 5 to 50 degrees C the EPC bilayer thickness decreased approximately 4 A, and the equilibrium fluid spacing increased from 14 to 21 A. Over this temperature range there was little change in the pressure-distance relation for fluid spacings less than approximately 10 A, but a substantial increase in the total pressure for fluid spacings greater than 10 A. These data show that for both gel and liquid crystalline bilayers there is a short-range repulsive pressure that is nearly temperature-independent, whereas for liquid crystalline bilayers there is also a longer-range pressure that increases with temperature. From analysis of the energetics of dehydration we argue that the temperature-independent short-range pressure is consistent with a hydration pressure due to polarization or electrostriction of water molecules by the phosphorylcholine moiety. For the liquid crystalline phase, the 7 A increase in equilibrium fluid spacing with increasing temperature can be predicted by an increase in the undulation pressure as a consequence of a temperature-dependent decrease in bilayer bending modulus.
采用渗透压/ X射线衍射法,在5至50摄氏度范围内测量了凝胶相和液晶相脂质双层的双层结构和双层间排斥压力。对于凝胶相的二山嵛酰磷脂酰胆碱(DBPC),双层厚度和压力-距离关系几乎与温度无关,在完全水合时,平衡流体间距增加约1埃,从5摄氏度时的10埃增加到50摄氏度时的11埃。相比之下,对于液晶相的卵磷脂(EPC),双层厚度、平衡流体间距和压力-距离关系均明显依赖于温度。当温度从5摄氏度升高到50摄氏度时,EPC双层厚度减少约4埃,平衡流体间距从14埃增加到21埃。在这个温度范围内,对于小于约10埃的流体间距,压力-距离关系变化不大,但对于大于10埃的流体间距,总压力大幅增加。这些数据表明,对于凝胶相和液晶相双层,都存在一个几乎与温度无关的短程排斥压力,而对于液晶相双层,还存在一个随温度升高的长程压力。通过对脱水能量学的分析,我们认为与温度无关的短程压力与由于磷酰胆碱部分对水分子的极化或电致伸缩而产生的水合压力一致。对于液晶相,随着温度升高平衡流体间距增加7埃,可以通过双层弯曲模量随温度降低导致的起伏压力增加来预测。