Department of Chemistry, Durham University, South Road, Durham DH1 3LE, United Kingdom.
J Am Chem Soc. 2010 Apr 14;132(14):5179-85. doi: 10.1021/ja910526z.
X-ray diffraction (XRD), molecular dynamics simulations (MD), and (19)F NMR have been used to investigate structure and dynamics in solid octafluoronaphthalene, C(10)F(8). Two distinct processes are observed via measurements of (19)F relaxation times as a function of temperature; a faster process from T(1) relaxation with a correlation time of the order of ns at ambient temperature (fitting to Arrhenius-type parameters E(a) = 20.6 +/- 0.4 kJ mol(-1) and tau(0) = 8 +/- 1 x 10(-14) s) and a much slower process from T(1rho) relaxation with a correlation time of the order of mus (fitting to E(a) = 55.1 +/- 1.3 kJ mol(-1) and tau(0) = 4 +/- 2 x 10(-16) s). Atomistic molecular dynamics reveals the faster process to involve a small angle jump of 40 degrees of the molecules, which is in perfect agreement with the X-ray diffraction study of the material at ambient temperature. The MD study reveals the existence of more extreme rotations of the molecules, which are proposed to enable the full rotation of the octafluoronaphthalene molecules. This explains both the T(1rho) results and previous wide-line (19)F NMR studies. The experimental measurements (NMR and XRD) and the MD computations are found to be strongly complementary and mutally essential. The reasons why a process on the time scale of microseconds, and associated with such a large activation barrier, can be accessed via classical molecular dynamics simulations are also discussed.
X 射线衍射(XRD)、分子动力学模拟(MD)和(19)F NMR 已被用于研究固体全氟萘(C(10)F(8))的结构和动力学。通过测量(19)F 弛豫时间随温度的变化,观察到两个不同的过程;在环境温度下,较快的过程来自 T(1)弛豫,相关时间约为 ns(拟合为 Arrhenius 型参数 E(a)=20.6±0.4 kJ mol(-1)和 tau(0)=8±1 x 10(-14)s),而较慢的过程来自 T(1rho)弛豫,相关时间约为 mus(拟合为 E(a)=55.1±1.3 kJ mol(-1)和 tau(0)=4±2 x 10(-16)s)。原子分子动力学揭示了较快的过程涉及分子的 40 度小角度跳跃,这与环境温度下材料的 X 射线衍射研究完全一致。MD 研究揭示了分子更极端的旋转的存在,这被认为可以使全氟萘分子完全旋转。这解释了 T(1rho)结果和以前的宽线(19)F NMR 研究。实验测量(NMR 和 XRD)和 MD 计算被发现是强互补和相互必要的。还讨论了为什么可以通过经典分子动力学模拟访问时间尺度为微秒的过程,以及与如此大的活化能垒相关的过程的原因。