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对比两种不同的二进制玻璃形成混合物动力学解释。

Contrasting two different interpretations of the dynamics in binary glass forming mixtures.

机构信息

Dipartimento di Fisica, Università di Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.

CNR-IPCF, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy.

出版信息

J Chem Phys. 2018 Feb 7;148(5):054504. doi: 10.1063/1.5012088.

Abstract

In a series of papers on binary glass-forming mixtures of tripropyl phosphate (TPP) with polystyrene (PS), Kahlau et al. [J. Chem. Phys. 140, 044509 (2014)] and Bock et al. [J. Chem. Phys. 139, 064508 (2013); J. Chem. Phys. 140, 094505 (2014); and J. Non-Cryst. Solids 407, 88-97 (2015)] presented the data on the dynamics of the two components studied over the entire composition range by several experimental methods. From these sets of data, obtained by multiple experimental techniques on mixtures with a large difference ΔT ≈ 200 K between the glass transition temperatures of two starting glass formers, they obtained two α-relaxations, α1 and α2. The temperature dependence of the slower α1 is Vogel-Fulcher like, but the faster α2 is Arrhenius. We have re-examined their data and show that their α2-relaxation is the Johari-Goldstein (JG) β-relaxation with Arrhenius T-dependence admixed with a true α2-relaxation having a stronger temperature dependence. In support of our interpretation of their data, we made dielectric measurements at elevated pressures P to show that the ratio of the α1 and α2 relaxation times, τ(T,P)/τ(T,P), is invariant to variations of T and P, while τ(T,P) is kept constant. This property proves unequivocally that the α2-relaxation is the JG β-relaxation, the precursor of the α1-relaxation. Subsequently, the true but unresolved α2-relaxation is recovered, and its relaxation times with much stronger temperature dependence are deduced, as expected for the α-relaxation of the TPP component. The results are fully compatible with those found in another binary mixture of methyltetrahydrofuran with tristyrene and PS with ΔT ≈ 283 K, even larger than ΔT ≈ 200 K of the mixture of TPP with PS, and in several polymer blends. The contrast between the two very different interpretations brought out in this paper is deemed beneficial for further progress in this research area.

摘要

在一系列关于三丙磷酸酯(TPP)与聚苯乙烯(PS)二元玻璃形成混合物的论文中,Kahlau 等人 [J. Chem. Phys. 140, 044509 (2014)] 和 Bock 等人 [J. Chem. Phys. 139, 064508 (2013); J. Chem. Phys. 140, 094505 (2014); 和 J. Non-Cryst. Solids 407, 88-97 (2015)] 通过多种实验方法研究了两种成分的动力学,报道了整个组成范围内的数据。从这些数据集,由两种起始玻璃形成体的玻璃化转变温度之间差异约为 200 K 的混合物的多种实验技术获得,他们得到了两个 α 弛豫,α1 和 α2。较慢的 α1 的温度依赖性类似于 Vogel-Fulcher,但较快的 α2 是 Arrhenius 型的。我们重新检查了他们的数据,并表明他们的 α2-弛豫是 Johari-Goldstein (JG) β-弛豫,具有 Arrhenius T 依赖性,混合了具有更强温度依赖性的真正 α2-弛豫。为了支持我们对他们数据的解释,我们在升高的压力 P 下进行了介电测量,以证明 α1 和 α2 弛豫时间之比 τ(T,P)/τ(T,P),对 T 和 P 的变化是不变的,而 τ(T,P)是保持不变的。这个特性无可争议地证明了 α2-弛豫是 JG β-弛豫,是 α1-弛豫的前体。随后,恢复了真正但未解决的 α2-弛豫,并推导了其弛豫时间,其温度依赖性更强,这与 TPP 成分的 α-弛豫预期相符。结果与另一种二元混合物甲基四氢呋喃与三苯乙烯和 PS 与 ΔT ≈ 283 K 的结果完全兼容,甚至比 TPP 与 PS 的混合物的 ΔT ≈ 200 K 还要大,以及几种聚合物共混物。本文提出的两种截然不同的解释之间的对比,被认为有利于该研究领域的进一步进展。

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