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过冷水的两体熵与弛豫时间之间的关系。

Relation between the two-body entropy and the relaxation time in supercooled water.

作者信息

Gallo P, Rovere M

机构信息

Dipartimento di Matematica e Fisica, Università Roma Tre, Via della Vasca Navale 84, I-00146 Roma, Italy.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2015 Jan;91(1):012107. doi: 10.1103/PhysRevE.91.012107. Epub 2015 Jan 6.

Abstract

The two-body excess entropy of supercooled water is calculated from the radial distribution functions obtained from computer simulation of the TIP4P model for different densities upon supercooling. This quantity is considered in connection with the relaxation time of the self intermediate scattering function. The relaxation time shows a mode coupling theory (MCT) behavior in the region of mild supercooling and a strong behavior in the deep supercooled region. We find here that the two-body entropy is connected to the relaxation time and shows a logarithmic behavior with an apparent asymptotic divergence at the mode coupling crossover temperature. There is also evidence of a change in behavior of the two-body entropy upon crossing from the fragile (hopping-free) state to the strong (hopping-dominated) state of supercooled water, and the relation that connects the two-body entropy and the relxation time in the MCT region no longer holds.

摘要

过冷水的两体过量熵是根据TIP4P模型在不同密度下过冷时通过计算机模拟得到的径向分布函数计算得出的。该量与自中间散射函数的弛豫时间相关联。弛豫时间在轻度过冷区域呈现出模式耦合理论(MCT)行为,而在深度过冷区域呈现出强烈行为。我们在此发现,两体熵与弛豫时间相关联,并且在模式耦合交叉温度处呈现出对数行为以及明显的渐近发散。也有证据表明,当过冷水从脆弱(无跳跃)状态转变为强(跳跃主导)状态时,两体熵的行为会发生变化,并且在MCT区域连接两体熵和弛豫时间的关系不再成立。

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