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Dynamic and 2D NMR studies on hydrogen-bonding aggregates of cholesterol in low-polarity organic solvents

机译:动态和二维NMR研究低极性有机溶剂中胆固醇的氢键聚集体

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Self-diffusion coefficients (D) are measured for normal (nondeuterated) and deuterated cholesterol-d(6) (C26 and C27 methyl groups deuterated) in 1-octanol, chloroform, and cyclohexane at concentrations of 1-700 mM by varying the impurity water concentration (> 2 mM) and temperature (30-50 degrees C). The pulsed field gradient spin-echo (PGSE) H-1 and H-2 NMR were used, respectively, at 600 and 92 MHz. At 30 degrees C, the hydrodynamic radius ( R) obtained at 20 mM from the D value and solvent viscosity is 5.09, 7.07, and 6.17 angstrom, respectively, in 1-octanol, chloroform, and cyclohexane when the impurity water is negligible. The R value in 1-octanol is the smallest and comparable with the average length of the molecular axes for the cholesterol molecule. In 1-octanol, R is invariant against the concentration variation, whereas in chloroform, R is larger and increases almost linearly with cholesterol concentration. At the highest concentration, 700 mM, the R in chloroform is 13.5 and 16.7 angstrom, respectively, when the impurity water is at negligible and saturated concentrations. The R value larger than that in hydrogen-bonding 1-octanol indicates that cholesterol forms an aggregate through hydrogen bonding. The aggregate structure is confirmed by comparing NOESY spectra in chloroform and 1-octanol. The NOESY analysis reveals the presence of one extra cross peak (C4-C19) in chloroform compared to 1-octanol. Because the carbon atoms related to the cross peak are close to the hydroxyl group (C3-OH), cholesterol molecules are considered to be not piled but are found to be OH-centered in the aggregate. This is supported also by larger rotational hydrodynamic radii measured on cholesterol deuterated at positions C2, C3, C4, and C6. This shows that the aggregate formation is driven by the hydrogen-bonding between cholesterol molecules.
机译:通过改变杂质,测量1-辛醇,氯仿和环己烷中浓度为1-700 mM的正常(非氘代)和氘代胆固醇-d(6)(C26和C27甲基氘代)的自扩散系数(D)水浓度(> 2 mM)和温度(30-50摄氏度)。分别在600和92 MHz下使用脉冲场梯度自旋回波(PGSE)H-1和H-2 NMR。在30摄氏度时,当杂水可忽略不计时,在20 mM下从D值和溶剂粘度获得的流体力学半径(R)在1-辛醇,氯仿和环己烷中分别为5.09、7.07和6.17埃。 1-辛醇中的R值最小,可与胆固醇分子的分子轴平均长度相比较。在1-辛醇中,R对浓度变化不变,而在氯仿中,R较大,并且几乎随胆固醇浓度线性增加。在最高浓度700 mM处,当杂质水的浓度可忽略不计且处于饱和浓度时,氯仿中的R分别为13.5和16.7埃。 R值大于与氢键合的1-辛醇中的R值,表明胆固醇通过氢键形成聚集体。通过比较氯仿和1-辛醇中的NOESY光谱可以确定聚集体结构。 NOESY分析表明,与1-辛醇相比,氯仿中存在一个额外的交叉峰(C4-C19)。因为与交叉峰有关的碳原子靠近羟基(C3-OH),所以胆固醇分子被认为没有堆积,但发现它们以OH为中心。在位置C2,C3,C4和C6氘化的胆固醇上测得的更大的旋转流体力学半径也支持了这一点。这表明聚集体形成是由胆固醇分子之间的氢键驱动的。

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