Gershfeld N L, Mudd C P, Tajima K, Berger R L
Laboratory of Physical Biology, National Institute of Arthritis and Musculoskeletal and Skin Diseases, National Institutes of Health, Bethesda, Maryland 20892.
Biophys J. 1993 Sep;65(3):1174-9. doi: 10.1016/S0006-3495(93)81157-3.
Using a heat conduction calorimeter with very high resolution (+/- 0.00005 J/degrees C.cm3), we have measured the specific heat CpL between 25 and 35 degrees C of dimyristoylphosphatidylcholine (DMPC) in aqueous dispersions. Previous studies of the temperature dependence of the chemical potential of DMPC in the L alpha phase (lamellar, liquid crystalline) indicated that a dispersion consisting only of unilamellar vesicles forms spontaneously at a critical temperature T* of 29.0 degrees C. Our present measurements show an anomaly in CpL between 28.70 and 29.50 degrees C: the curve for CpL versus T first decreases and then exhibits an inflection point at 28.96 degrees C before it flattens. This anomaly is attributed to the transformation from multilamellar dispersion to unilamellar vesicles at T* = 28.96 degrees C. Two independent properties of the CpL data also indicate T* is a critical point for the formation of unilamellar vesicles: (a) the time to reach equilibrium upon changing temperature increased dramatically between 28.7 and 28.96 degrees C, increasing as (T* - T)-1; at T > T* the dramatic "slowing-down" phenomenon was not observed. This slowing-down near T* is a general characteristic of critical phenomena. (b) The free energy change for the multilamellar-unilamellar transformation was obtained from the CpL-T data over this temperature interval and found to be 3.2 J/mol or 0.016 ergs/cm2 of bilayer, in agreement with other estimates of the interaction energy between neutral bilayers. We conclude with a discussion of the implications for membrane bilayer stability of these newly identified dynamic properties of the transformation.
我们使用分辨率极高(±0.00005 J/℃·cm³)的热传导量热计,测量了二肉豆蔻酰磷脂酰胆碱(DMPC)在水分散体系中25至35℃之间的定压比热容CpL。先前对DMPC在Lα相(层状液晶相)中化学势随温度变化的研究表明,仅由单层囊泡组成的分散体系在29.0℃的临界温度T下自发形成。我们目前的测量结果显示,在28.70至29.50℃之间CpL存在异常:CpL随温度T的曲线先下降,然后在28.96℃处出现拐点,之后趋于平缓。这种异常归因于在T = 28.96℃时从多层分散体系向单层囊泡的转变。CpL数据的两个独立特性也表明T是单层囊泡形成的临界点:(a)温度变化时达到平衡的时间在28.7至28.96℃之间急剧增加,按(T - T)-1的规律增长;在T > T时未观察到这种急剧的“变慢”现象。T附近的这种变慢是临界现象的一个普遍特征。(b)通过该温度区间内的CpL - T数据获得了多层 - 单层转变的自由能变化,结果为3.2 J/mol或0.016 ergs/cm²双层,与中性双层之间相互作用能的其他估计值一致。我们最后讨论了这些新发现的转变动态特性对膜双层稳定性的影响。