Reese Caleb W, Strango Zachariah I, Dell Zachary R, Tristram-Nagle Stephanie, Harper Paul E
Department of Physics and Astronomy, Calvin College, 1734 Knollcrest Circle SE, Grand Rapids, MI, USA.
Phys Chem Chem Phys. 2015 Apr 14;17(14):9194-204. doi: 10.1039/c5cp00175g. Epub 2015 Mar 11.
Using DSC (differential scanning calorimetry), we measure the kinetics of the cubic-HII 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 °C. The kinetics of this transition also slow greatly with increasing sucrose concentration. For low sucrose concentrations, the kinetics are asymmetric, with the cooling (HII-cubic) transition taking twice as long as the heating (cubic-HII) 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-HII 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 β-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 HII phases.
我们使用差示扫描量热法(DSC)来测量单油酸甘油酯在大量蔗糖溶液中从立方相到六方相II转变的动力学过程。我们发现,转变温度显著降低,每1 mol kg⁻¹的蔗糖浓度会使转变温度下降20°C。随着蔗糖浓度的增加,这种转变的动力学过程也大幅减慢。对于低蔗糖浓度,动力学过程是不对称的,冷却(六方相II - 立方相)转变所需时间是加热(立方相 - 六方相II)转变的两倍。对于较高的蔗糖浓度,转变时间的这种不对称性会减小。冷却转变的阿弗拉米指数在2到2.5之间,加热转变的阿弗拉米指数在1到3之间。传统的阿弗拉米解释是,这些过程通过具有可变成核速率的一维或二维途径发生。一种非传统的观点认为,这些指数反映了孔形成(冷却)和破坏(加热)的时间依赖性。单油酸甘油酯的新密度测量结果表明,目前公认的值低了约5%;这对电子密度建模有重大影响。结构计算表明,在立方相到六方相II的转变过程中,头部基团面积和脂质长度分别收缩了约12%和4%;这种收缩与具有非常不同分子结构(rac - 二 - 12:0 β - 葡萄糖二酰甘油)且发生相同转变的脂质几乎相同。热力学考虑表明,在立方相和六方相II相中,脂质头部基团前方都存在一个约一个水分子厚度的水合层。