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Anomalies in bulk supercooled water at negative pressure

机译:负压下散装过冷水中的异常

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摘要

Water anomalies still defy explanation. In the supercooled liquid, many quantities, for example heat capacity and isothermal compressibility κT, show a large increase. The question arises if these quantities diverge, or if they go through a maximum. The answer is key to our understanding of water anomalies. However, it has remained elusive in experiments because crystallization always occurred before any extremum is reached. Here we report measurements of the sound velocity of water in a scarcely explored region of the phase diagram, where water is both supercooled and at negative pressure. We find several anomalies: maxima in the adiabatic compressibility and nonmonotonic density dependence of the sound velocity, in contrast with a standard extrapolation of the equation of state. This is reminiscent of the behavior of supercritical fluids. To support this interpretation, we have performed simulations with the 2005 revision of the transferable interaction potential with four points. Simulations and experiments are in near-quantitative agreement, suggesting the existence of a line of maxima in κT (>LMκT). This >LMκT could either be the thermodynamic consequence of the line of density maxima of water [Sastry S, Debenedetti PG, Sciortino F, Stanley HE (1996) Phys Rev E 53:6144–6154], or emanate from a critical point terminating a liquid–liquid transition [Sciortino F, Poole PH, Essmann U, Stanley HE (1997) Phys Rev E 55:727–737]. At positive pressure, the >LMκT has escaped observation because it lies in the “no man’s land” beyond the homogeneous crystallization line. We propose that the >LMκT emerges from the no man’s land at negative pressure.
机译:水异常仍然无法解释。在过冷的液体中,例如热容和等温压缩率κT的许多数量都显示出很大的增加。问题是这些数量是否发散或是否达到最大值。答案是我们了解水异常的关键。但是,由于结晶总是在到达任何极值之前发生的,因此在实验中仍然难以捉摸。在这里,我们报告在相图很少探索的区域中水的声速的测量结果,在该区域中,水都是过冷的,并且处于负压状态。我们发现了几个异常:与状态方程的标准外推法相比,绝热压缩率的最大值和声速的非单调密度依赖性。这让人联想到超临界流体的行为。为了支持这种解释,我们在2005年修订版中对可转让互动潜力进行了四点模拟。模拟和实验接近定量,表明κT(> LM κT)中存在一条最大值线。 > LM κT可能是水的密度最大值线的热力学结果[Sastry S,Debenedetti PG,Sciortino F,Stanley HE(1996)Phys Rev E 53:6144-6154],或从终止液-液转变的临界点发出[Sciortino F,Poole PH,Essmann U,Stanley HE(1997)Phys Rev E 55:727-737]。在正压力下,> LM κT逃脱了观察,因为它位于均匀结晶线之外的“无人区”。我们建议> LM κT在无压力的情况下从无人区出现。

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