Department of Physics, School of Science , Tokai University , 4-1-1 Kitakaname , Hiratuka-shi , Kanagawa 259-1292 , Japan.
Micro/Nano Technology Center , Tokai University , 4-1-1 Kitakaname , Hiratuka-shi , Kanagawa 259-1292 , Japan.
J Phys Chem B. 2020 Feb 27;124(8):1521-1530. doi: 10.1021/acs.jpcb.9b11552. Epub 2020 Feb 17.
In this study, we investigated the cooperative molecular dynamics of poly(vinylpyrrolidone) (PVP), ice, and uncrystallized water (UCW) in partially crystallized PVP-water mixtures by means of broadband dielectric spectroscopy. Three relaxation processes, denoted I, II, and III, were observed at temperatures ranging from immediately below the crystallization temperature () to approximately 200 K. At temperatures of 173-193 K, processes I and II cannot be distinguished. Below 168 K, process II separates into two processes: process IV at higher frequencies and process V at lower frequencies. Process I contributes to process V. In partially crystallized mixtures, process I originates from UCW in an uncrystallized phase with PVP. Process II is attributed to ice in the mixture, with a relaxation time that is 2 orders of magnitude smaller than that of pure ice. The concentration dependence of the strength of process II and the relaxation time relative to that of ice in bovine serum albumin (BSA)-water and gelatin-water mixtures strongly support this conclusion. Observation of processes IV and V indicates the presence of multiple ice relaxation processes. Process III is attributed to the α process of PVP in the uncrystallized phase in 40 and 50 wt % PVP mixtures. For mixtures with 30 wt % PVP or less, process III is attributed not only to the α process of PVP but also to interfacial polarization.
在这项研究中,我们通过宽带介电谱研究了部分结晶的聚乙烯吡咯烷酮(PVP)-水混合物中 PVP、冰和非结晶水(UCW)的协同分子动力学。在从结晶温度以下()到大约 200 K 的温度范围内,观察到三个弛豫过程,分别表示为 I、II 和 III。在 173-193 K 的温度下,过程 I 和 II 无法区分。在 168 K 以下,过程 II 分离成两个过程:高频的过程 IV 和低频的过程 V。过程 I 有助于过程 V。在部分结晶混合物中,过程 I 来自 PVP 无定形相中的 UCW。过程 II 归因于混合物中的冰,其弛豫时间比纯冰小 2 个数量级。牛血清白蛋白(BSA)-水和明胶-水混合物中过程 II 的强度和相对冰的弛豫时间的浓度依赖性强烈支持这一结论。观察到过程 IV 和 V 表明存在多个冰弛豫过程。过程 III 归因于 40 和 50 wt % PVP 混合物中非晶相 PVP 的α过程。对于 30 wt % PVP 或更少的混合物,过程 III 不仅归因于 PVP 的α过程,还归因于界面极化。