4.8 Article

Anomalies in bulk supercooled water at negative pressure

出版社

NATL ACAD SCIENCES
DOI: 10.1073/pnas.1323366111

关键词

scenarios for water; Widom line; Berthelot tube

资金

  1. European Research Council under the European Community [240113]
  2. Agence Nationale de la Recherche [09-BLAN-0404-01]
  3. Marie Curie Integration [PCIG-GA-2011-303941]
  4. Ministerio de Educacion y Ciencia
  5. Universidad Complutense de Madrid
  6. Ministerio de ciencia e innovacion (MCINN) [FIS2013-43209-P]
  7. [QCM-2014-1-0038]

向作者/读者索取更多资源

Water anomalies still defy explanation. In the supercooled liquid, many quantities, for example heat capacity and isothermal compressibility kappa(T), 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 super-critical 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 kappa(T) (LM kappa(T)). This LM kappa(T) 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 LM kappa(T) has escaped observation because it lies in the no man's land beyond the homogeneous crystallization line. We propose that the LM kappa(T) emerges from the no man's land at negative pressure.

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