Roberts Mary F, Redfield Alfred G, Mohanty Udayan
Merkert Chemistry Center, Boston College, Chestnut Hill, Massachusetts, USA.
Biophys J. 2009 Jul 8;97(1):132-41. doi: 10.1016/j.bpj.2009.03.057.
The magnetic field dependence of the 31P spin-lattice relaxation rate, R1, of phospholipids can be used to differentiate motions for these molecules in a variety of unilamellar vesicles. In particular, internal motion with a 5- to 10-ns correlation time has been attributed to diffusion-in-a-cone of the phosphodiester region, analogous to motion of a cylinder in a liquid hydrocarbon. We use the temperature dependence of 31P R1 at low field (0.03-0.08 T), which reflects this correlation time, to explore the energy barriers associated with this motion. Most phospholipids exhibit a similar energy barrier of 13.2 +/- 1.9 kJ/mol at temperatures above that associated with their gel-to-liquid-crystalline transition (Tm); at temperatures below Tm, this barrier increases dramatically to 68.5 +/- 7.3 kJ/mol. This temperature dependence is broadly interpreted as arising from diffusive motion of the lipid axis in a spatially rough potential energy landscape. The inclusion of cholesterol in these vesicles has only moderate effects for phospholipids at temperatures above their Tm, but significantly reduces the energy barrier (to 17 +/- 4 kJ/mol) at temperatures below the Tm of the pure lipid. Very-low-field R1 data indicate that cholesterol inclusion alters the averaged disposition of the phosphorus-to-glycerol-proton vector (both its average length and its average angle with respect to the membrane normal) that determines the 31P relaxation.
磷脂的31P自旋晶格弛豫率R1对磁场的依赖性可用于区分这些分子在各种单层囊泡中的运动。特别是,具有5至10纳秒相关时间的内部运动被归因于磷酸二酯区域的锥形扩散,类似于圆柱体在液态烃中的运动。我们利用低场(0.03 - 0.08 T)下31P R1的温度依赖性(其反映了这种相关时间)来探索与该运动相关的能垒。大多数磷脂在高于其凝胶 - 液晶转变温度(Tm)时表现出类似的13.2±1.9 kJ/mol的能垒;在低于Tm的温度下,该能垒急剧增加至68.5±7.3 kJ/mol。这种温度依赖性被广泛解释为源于脂质轴在空间粗糙的势能景观中的扩散运动。在这些囊泡中加入胆固醇,对于高于其Tm温度的磷脂只有适度影响,但在低于纯脂质Tm的温度下显著降低了能垒(降至17±4 kJ/mol)。极低场R1数据表明,加入胆固醇会改变决定31P弛豫的磷 - 甘油 - 质子矢量的平均取向(其平均长度及其相对于膜法线的平均角度)。