Tristram-Nagle S, Wiener M C, Yang C P, Nagle J F
Department of Biological Sciences, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213.
Biochemistry. 1987 Jul 14;26(14):4288-94. doi: 10.1021/bi00388a016.
The kinetics of the interconversions of the subgel and gel phases in dipalmitoylphosphatidylcholine have been studied by using differential dilatometry, differential scanning calorimetry (DSC), and neutral buoyancy centrifugation as a function of incubation temperature and deuteriation of the solvent. As seen by others, DSC scans show two peaks in the subgel transition region for incubation temperatures below 1 degree C. After incubation at 0.1 degree C, the DSC peak that occurs at the lower scanning temperature appears with an incubation half-time of 0.5 day and eventually converts into a peak at higher scanning temperature with an incubation half-time of 18 days. By varying the scanning rate, we show that these two peaks merge into one at slow scanning rates with a common equilibrium transition temperature of 13.8 degrees C, in agreement with equilibrium calorimetry and dilatometry (delta V = 0.017 +/- 0.001 mL/g). For incubation temperatures above 4.6 degrees C, only one peak appears in both scanning dilatometry and calorimetry. While the initial rate of subgel conversion is smaller at the higher incubation temperatures, after 300 h a higher percentage of the sample has converted to subgel than at the lower incubation temperatures. We suggest that higher incubation temperatures (near 5 degrees C) are preferable for forming the stable subgel phase, and we present a colliding domain picture that indicates why this may be so. Our results in D2O and the similarity of the kinetics of volume decrease with the kinetics of wide-angle diffraction lines also support the suggestion that the partial loss of interlamellar water plays a kinetic role in subgel formation.
通过使用差示膨胀法、差示扫描量热法(DSC)以及中性浮力离心法,研究了二棕榈酰磷脂酰胆碱中亚凝胶相和凝胶相相互转化的动力学,该动力学是作为孵育温度和溶剂氘化的函数。正如其他人所观察到的,对于低于1℃的孵育温度,DSC扫描在亚凝胶转变区域显示出两个峰。在0.1℃孵育后,出现在较低扫描温度的DSC峰以0.5天的孵育半衰期出现,并最终在18天的孵育半衰期后转化为较高扫描温度下的峰。通过改变扫描速率,我们表明这两个峰在慢扫描速率下合并为一个,共同的平衡转变温度为13.8℃,这与平衡量热法和膨胀法一致(ΔV = 0.017±0.001 mL/g)。对于高于4.6℃的孵育温度,在扫描膨胀法和量热法中都只出现一个峰。虽然在较高孵育温度下亚凝胶转化的初始速率较小,但在300小时后,与较低孵育温度相比,有更高百分比的样品转化为亚凝胶。我们认为较高的孵育温度(接近5℃)更有利于形成稳定的亚凝胶相,并且我们提出了一个碰撞域模型来说明原因。我们在D2O中的结果以及体积减小动力学与广角衍射线动力学的相似性也支持了层间水的部分损失在亚凝胶形成中起动力学作用的观点。