Wang Chi-Wei, Kuo Yu-Wei, Zeng Jing-Rong, Tang Ping-Han, Wu Ten-Ming
Institute of Physics, National Yang Ming Chiao Tung University, Hsinchu 300, Taiwan.
J Phys Chem B. 2024 Oct 3;128(39):9525-9535. doi: 10.1021/acs.jpcb.4c03898. Epub 2024 Sep 22.
Molecular dynamics simulations were used to investigate the reorientation dynamics of water confined within graphite nanoslits of size less than 2 nm, where molecules formed inner and interfacial layers parallel to the confining walls. Significantly related to molecular reorientations, the hydrogen-bond (HB) network of nanoconfined water therein was scrutinized by HB configuration fractions compared to those of bulk water and the influences on interfacial-molecule orientations relative to a nearby C atom plate. The second-rank orientation time correlation functions (OTCFs) of nanoconfined water were calculated and found to follow stretched-exponential, power-law, and power-law decays in a time series. To understand this naïve behavior of reorientation relaxation, the approach of statistical mechanics was adopted in our studies. In terms of the orientation Van Hove function (OVHF), an alternative meaning was given to the second-rank OTCF, which is a measure of the deviation of the OVHF between a molecular system and free molecules in random orientations. Indicated by the OVHFs at related time scales, the stretched-exponential decay of the second-rank OTCF resulted from molecules evacuating out of HB cages formed by their neighbors. After the evacuations, the inner molecules relaxed at relatively fast rates toward random orientations, but the interfacial molecules reoriented at slow rates due to restrictions by hydrophobic interactions with graphite walls. The first power-law decay of the second-rank OTCF was attributed to the distinct relaxation rates of inner and interfacial molecules within a graphite nanoslit. When the inner molecules were completely random in orientation, the second-rank OTCFs changed to another power law decay with a power smaller than the first one.
分子动力学模拟用于研究限制在尺寸小于2nm的石墨纳米狭缝内的水的重排动力学,其中分子形成了与限制壁平行的内层和界面层。与分子重排密切相关的是,通过氢键(HB)构型分数,将其中纳米受限水的氢键网络与 bulk 水的氢键网络进行了比较,并研究了其对相对于附近碳原子板的界面分子取向的影响。计算了纳米受限水的二阶取向时间关联函数(OTCFs),发现其在时间序列中遵循拉伸指数、幂律和幂律衰减。为了理解这种重排弛豫的简单行为,我们的研究采用了统计力学方法。根据取向范霍夫函数(OVHF),对二阶OTCF赋予了另一种含义,它是分子系统与随机取向的自由分子之间OVHF偏差的一种度量。在相关时间尺度上由OVHFs表明,二阶OTCF的拉伸指数衰减是由于分子从其相邻分子形成的HB笼中逸出。逸出后,内层分子以相对较快的速率弛豫到随机取向,但由于与石墨壁的疏水相互作用的限制,界面分子以较慢的速率重新取向。二阶OTCF的第一个幂律衰减归因于石墨纳米狭缝内内层和界面分子不同的弛豫速率。当内层分子在取向上完全随机时,二阶OTCFs变为另一个幂律衰减,其幂小于第一个幂律衰减。