Brown M F, Ribeiro A A, Williams G D
Proc Natl Acad Sci U S A. 1983 Jul;80(14):4325-9. doi: 10.1073/pnas.80.14.4325.
Natural abundance 13C spin-lattice (T1) relaxation time measurements are reported for unilamellar vesicles of 1,2-dipalmitoylphosphatidylcholine (1,2-dipalmitoyl-sn-glycero-3-phosphocholine), in the liquid crystalline phase, at magnetic field strengths of 1.40, 1.87, 2.35, 4.23, 7.05, 8.45, and 11.7 tesla (resonance frequencies of 15.0, 20.0, 25.1, 45.3, 75.5, 90.5, and 126 MHz, respectively), and the results are compared to previous 2H T1 studies of multilamellar dispersions. For both the 13C and 2H T1 studies, a dramatic frequency dependence of the relaxation was observed. At superconducting magnetic field strengths (4.23-11.7 tesla), plots of the 13C T1(-1) relaxation rates as a function of acyl chain segment position clearly reveal the characteristic "plateau" signature of the liquid crystalline phase, as found previously from 2H NMR studies. The dependence of T1(1) on ordering, determined previously from 2H NMR, and the T1(-1) dependence on frequency, determined from both 13C and 2H NMR studies, suggest that a unified picture of the bilayer molecular dynamics can be provided by a simple relaxation law of the form T1(-1) approximately equal to A tau f + BS2C-H omega -1/2(0). In the above expression, A and B are constants, SC-H (= SC-D) is the bond segmental order parameter, and omega 0 is the nuclear Larmor frequency. The first (A) term includes contributions from fast, local segmental motions characterized by the effective correlation time tau f, whereas the second (B) term describes slower, collective fluctuations in the local ordering. The value of tau f approximately equal to 10(-11) sec, obtained by extrapolating T1(-1) to infinite frequency, suggests that the segmental microviscosity of the bilayer hydrocarbon region does not differ appreciably from that of the equivalent n-paraffinic liquids of similar chain length.
报告了在1.40、1.87、2.35、4.23、7.05、8.45和11.7特斯拉(共振频率分别为15.0、20.0、25.1、45.3、75.5、90.5和126兆赫兹)的磁场强度下,处于液晶相的1,2 - 二棕榈酰磷脂酰胆碱(1,2 - 二棕榈酰 - sn - 甘油 - 3 - 磷酸胆碱)单层囊泡的天然丰度13C自旋 - 晶格(T1)弛豫时间测量结果,并将结果与之前关于多层分散体的2H T1研究进行了比较。对于13C和2H T1研究,均观察到弛豫存在显著的频率依赖性。在超导磁场强度(4.23 - 11.7特斯拉)下,13C T1(-1)弛豫率作为酰基链段位置函数的图清楚地揭示了液晶相的特征“平台”特征,这与之前2H NMR研究中发现的一致。先前从2H NMR确定的T1(1)对有序性的依赖性,以及从13C和2H NMR研究确定的T1(-1)对频率的依赖性表明,可以通过形式为T1(-1)≈Aτf + BS2C - Hω - 1/2(0)的简单弛豫定律提供双层分子动力学的统一图像。在上述表达式中,A和B是常数,SC - H(= SC - D)是键段序参数,ω0是核拉莫尔频率。第一项(A)包括以有效相关时间τf为特征的快速局部链段运动的贡献,而第二项(B)描述局部有序性中较慢的集体涨落。通过将T1(-1)外推到无限频率获得的τf≈10(-11)秒的值表明,双层烃区域的链段微观粘度与类似链长的等效正构烷烃液体的链段微观粘度没有明显差异。