Sasaki Kaito, Matsui Yurika, Miyara Masahiko, Kita Rio, Shinyashiki Naoki, Yagihara Shin
Department of Physics, School of Science, Tokai University , 4-1-1 Kitakaname, Hiratsuka-shi, Kanagawa 259-1292, Japan.
J Phys Chem B. 2016 Jul 14;120(27):6882-9. doi: 10.1021/acs.jpcb.6b05347. Epub 2016 Jun 30.
In this study, broadband dielectric spectroscopy and differential scanning calorimetry (DSC) measurements are performed to study the dynamics of water and polymers in an aqueous solution of poly(vinylpyrrolidone) (PVP) with concentrations of 60, 65, and 70 wt % PVP in a temperature range of 123-298 K. Two distinct relaxation processes, l- and h-processes, which originate from the segmental chain motion of PVP and the primary relaxation process of water, respectively, are observed simultaneously. The relationship between l- and h-processes and their temperature dependences mimic those of the α-process and Johari-Goldstein β-process, which are observed in ordinal glass formers. The relaxation time of the l-process, τl, obeys the Vogel-Fulcher (VF)-type temperature dependence, and the glass-transition temperature of the l-process, Tg,l, which is defined by the temperature that is reached in a τl of 100-1000 s, shows good agreement with the calorimetric Tg obtained by DSC. The temperature dependence of the relaxation time of the h-process, τh, exhibits a crossover from VF to Arrhenius behavior at the so-called fragile-to-strong transition (FST) of water at Tg,l. The temperature dependence of the relaxation strength of the h-process, Δεh, increases with a decrease in temperature from 298 K to Tg,l. Below Tg,l, Δεh is nearly constant or slightly decreases with decreasing temperature. According to previous studies on aqueous solutions of sugars and alcohols, the Δε of the ν-process, which originates from local motion of water, decreases with decreasing temperature above the Tg of the α-process, which originates from the cooperative motion of the solute and water. Therefore, the l-process in the PVP-water mixture is not a result of the cooperative motion of PVP and water but rather a result of the polymer-polymer cooperative motion of PVP. In addition, agreement among Tg,l, the temperature of the FST of water, and calorimetric Tg suggests that the FST of water occurs at Tg.
在本研究中,进行了宽带介电谱和差示扫描量热法(DSC)测量,以研究在123 - 298 K温度范围内,浓度为60、65和70 wt%聚乙烯吡咯烷酮(PVP)的水溶液中水和聚合物的动力学。同时观察到两个不同的弛豫过程,即l - 过程和h - 过程,它们分别源于PVP的链段运动和水的初级弛豫过程。l - 过程和h - 过程之间的关系及其温度依赖性与在普通玻璃形成体中观察到的α - 过程和乔哈里 - 戈尔茨坦β - 过程相似。l - 过程的弛豫时间τl遵循Vogel - Fulcher(VF)型温度依赖性,l - 过程的玻璃化转变温度Tg,l由τl达到100 - 1000 s时的温度定义,与DSC获得的量热Tg显示出良好的一致性。h - 过程的弛豫时间τh的温度依赖性在水在Tg,l处的所谓脆弱到强转变(FST)时表现出从VF行为到阿伦尼乌斯行为的转变。h - 过程的弛豫强度Δεh的温度依赖性随着温度从298 K降低到Tg,l而增加。在Tg,l以下,Δεh几乎恒定或随着温度降低而略有下降。根据先前对糖和醇水溶液的研究,源于水的局部运动 的ν - 过程的Δε在源于溶质和水的协同运动的α - 过程的Tg以上随着温度降低而降低。因此,PVP - 水混合物中的l - 过程不是PVP和水协同运动的结果,而是PVP的聚合物 - 聚合物协同运动的结果。此外,Tg,l、水的FST温度和量热Tg之间的一致性表明水的FST发生在Tg处。