CORE-SOFTENED POTENTIALS AND THE ANOMALOUS PROPERTIES OF WATER

We study the phase diagram of a system of spherical particles interacting in three dimensions through a potential consisting of a strict hard core plus a linear repulsive shoulder at larger distances. The phase diagram (obtained numerically, and analytically in a limiting case) shows anomalous properties that are similar to those observed in water. Specifically, we find maxima of density and isothermal compressibility as a function of temperature, melting with volume contraction, and multiple stable crystalline structures. If in addition a long range attraction between the particles is included, the usual liquid–gas coexistence curve with its critical point is obtained. But more interestingly, a first order line in the metastable fluid branch of the phase diagram appears, ending in a new critical point, as it was suggested to occur in water. In this way the model provides a comprehensive, consistent and unified picture of most of the anomalous thermodynamical properties of water, showing that all of them ...

[1]  Peter H. Poole,et al.  Line of compressibility maxima in the phase diagram of supercooled water , 1997 .

[2]  B. D. Kay,et al.  The evaporation rate, free energy, and entropy of amorphous water at 150 K , 1996 .

[3]  Hideki Tanaka,et al.  A self-consistent phase diagram for supercooled water , 1996, Nature.

[4]  R. J. Speedy,et al.  On the reproducibility of glasses , 1994 .

[5]  Cho,et al.  An explanation of the density maximum in water. , 1996, Physical review letters.

[6]  Roberts,et al.  Liquid-Liquid Immiscibility in Pure Fluids: Polyamorphism in Simulations of a Network-Forming Fluid. , 1996, Physical review letters.

[7]  Shlomo Havlin,et al.  Local Structural Heterogeneities in Liquid Water under Pressure , 1998 .

[8]  C. Angell,et al.  Formation of Glasses from Liquids and Biopolymers , 1995, Science.

[9]  H. Eugene Stanley,et al.  Phase behaviour of metastable water , 1992, Nature.

[10]  Stanley,et al.  Effect of hydrogen bonds on the thermodynamic behavior of liquid water. , 1994, Physical review letters.

[11]  Srikanth Sastry,et al.  SINGULARITY-FREE INTERPRETATION OF THE THERMODYNAMICS OF SUPERCOOLED WATER , 1996 .

[12]  H. Eugene Stanley,et al.  Interpretation of the unusual behavior of H2O and D2O at low temperatures: Tests of a percolation model , 1980 .

[13]  E. A. Jagla PHASE BEHAVIOR OF A SYSTEM OF PARTICLES WITH CORE COLLAPSE , 1998 .

[14]  G. Stell,et al.  Phase Transitions Due to Softness of the Potential Core , 1972 .

[15]  G. Stell,et al.  Isostructural phase transitions due to core collapse. II. A three‐dimensional model with a solid–solid critical point , 1976 .

[16]  Felix Franks,et al.  Water:A Comprehensive Treatise , 1972 .

[17]  C. Angell,et al.  Isothermal compressibility of supercooled water and evidence for a thermodynamic singularity at −45°C , 1976 .

[18]  R. J. Speedy Two waters and no ice please , 1996, Nature.

[19]  Hajime Tanaka SIMPLE PHYSICAL EXPLANATION OF THE UNUSUAL THERMODYNAMIC BEHAVIOR OF LIQUID WATER , 1998 .

[20]  Osamu Mishima,et al.  Reversible first‐order transition between two H2O amorphs at ∼0.2 GPa and ∼135 K , 1994 .

[21]  H. Stanley,et al.  The relationship between liquid, supercooled and glassy water , 1998, Nature.

[22]  E. Jagla Minimum energy configurations of repelling particles in two dimensions , 1998, cond-mat/9806332.

[23]  H. Eugene Stanley,et al.  Liquid-State Anomalies and the Stell-Hemmer Core-Softened Potential , 1998 .