过冷P-Se玻璃形成液体的流变学:从网络到分子和幂律松弛行为的出现。

Bing Yuan, B. Aitken, S. Sen
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引用次数: 2

摘要

采用振荡剪切流变法研究了PxSe100-x(30≤x≤67)过冷液体中随着磷含量的增加,网络-分子结构转变对其剪切-力学响应的影响。30≤x≤40的网络液体的特征是通过网络键断裂/更新过程进行剪切松弛,存储(G')和损失(G″)剪切模量的麦克斯韦缩放,以及低频时与频率无关的粘度,而中间成分(45≤x≤50)的液体出现了新的松弛过程。这一过程归因于网络和分子结构之间的相互转换。另一方面,x≥63的分子液体的主要特征是偏离麦克斯韦行为,因为存储模量在G'-G″交叉点以下的几乎整个频率范围内显示线性频率标度G'(ω) ~ ω,并且在终端区域G″/G'的比值几乎恒定。此外,这些相当脆弱的分子液体的动态粘度在低于动态起始频率的频率下比网络液体表现出显著的增强,即使在比起始频率低4个数量级的频率下也不能达到与频率无关的状态。分子液体的这种幂律弛豫行为归因于弛豫时间尺度分布极其广泛,同时存在单个分子的快速旋转运动和瞬态分子团簇的合作动力学,后者明显慢于剪切弛豫时间尺度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Rheology of supercooled P-Se glass-forming liquids: From networks to molecules and the emergence of power-law relaxation behavior.
The effect of the network-to-molecular structural transformation with increasing phosphorus content in PxSe100-x (30 ≤ x ≤ 67) supercooled liquids on their shear-mechanical response is investigated using oscillatory shear rheometry. While network liquids with 30 ≤ x ≤ 40 are characterized by shear relaxation via a network bond scission/renewal process, a Maxwell scaling of the storage (G') and loss (G″) shear moduli, and a frequency-independent viscosity at low frequencies, a new relaxation process emerges in liquids with intermediate compositions (45 ≤ x ≤ 50). This process is attributed to an interconversion between network and molecular structural moieties. Predominantly molecular liquids with x ≥ 63, on the other hand, are characterized by a departure from Maxwell behavior as the storage modulus shows a linear frequency scaling G'(ω) ∼ ω over nearly the entire frequency range below the G'-G″ crossover and a nearly constant ratio of G″/G' in the terminal region. Moreover, the dynamic viscosity of these rather fragile molecular liquids shows significant enhancement over that of network liquids at frequencies below the dynamical onset and does not reach a frequency-independent regime even at frequencies that are four orders of magnitude lower than that of the onset. Such power-law relaxation behavior of the molecular liquids is ascribed to an extremely broad distribution of relaxation timescales with the coexistence of rapid rotational motion of individual molecules and cooperative dynamics of transient molecular clusters, with the latter being significantly slower than the shear relaxation timescale.
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