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Structural insights into the cubic-hexagonal phase transition kinetics of monoolein modulated by sucrose solutions

机译:蔗糖溶液调节单油精的立方六方相变动力学的结构见解

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Using DSC (differential scanning calorimetry), we measure the kinetics of the cubic-H-II phase transition of monoolein in bulk sucrose solutions. We find that the transition temperature is dramatically lowered, with each 1 mol kg(-1) of sucrose concentration dropping the transition by 20 degrees C. The kinetics of this transition also slow greatly with increasing sucrose concentration. For low sucrose concentrations, the kinetics are asymmetric, with the cooling (H-II-cubic) transition taking twice as long as the heating (cubic-H-II) transition. This asymmetry in transition times is reduced for higher sucrose concentrations. The cooling transition exhibits Avrami exponents in the range of 2 to 2.5 and the heating transition shows Avrami exponents ranging from 1 to 3. A classical Avrami interpretation would be that these processes occur via a one or two dimensional pathway with variable nucleation rates. A non-classical perspective would suggest that these exponents reflect the time dependence of pore formation (cooling) and destruction (heating). New density measurements of monoolein show that the currently accepted value is about 5% too low; this has substantial implications for electron density modeling. Structural calculations indicate that the head group area and lipid length in the cubic-H-II transition shrink by about 12% and 4% respectively; this reduction is practically the same as that seen in a lipid with a very different molecular structure (rac-di-12:0 beta-GlcDAG) that makes the same transition. Thermodynamic considerations suggest there is a hydration shell about one water molecule thick in front of the lipid head groups in both the cubic and H-II phases.
机译:使用DSC(差示扫描量热法),我们测量了散装蔗糖溶液中单油精的立方-H-II相转变的动力学。我们发现,转变温度显着降低,每1 mol kg(-1)的蔗糖浓度会使转变温度降低20摄氏度。随着蔗糖浓度的增加,转变的动力学也大大减慢。对于低蔗糖浓度,动力学是不对称的,冷却(H-II-立方)转变所需时间是加热(立方-H-II)转变时间的两倍。对于更高的蔗糖浓度,过渡时间的这种不对称性减小了。冷却转变的Avrami指数范围为2到2.5,加热转变的Avrami指数范围为1到3。经典的Avrami解释是,这些过程是通过一维或二维路径以成核速率发生的。非经典观点认为这些指数反映了孔形成(冷却)和破坏(加热)的时间依赖性。单油精的新密度测量结果表明,目前接受的值太低了约5%;这对电子密度建模具有重要意义。结构计算表明,立方-H-II过渡区的头基面积和脂质长度分别减少了约12%和4%。这种减少实际上与在具有相同转变的分子结构非常不同的脂质(rac-di-12:0 beta-GlcDAG)中看到的减少相同。热力学考虑表明,在立方相和H-II相中,在脂质头基团的前面都有一个大约一个水分子厚的水合壳。

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