Experimental superheating of water and aqueous solutions

Abstract The metastable superheated solutions are liquids in transitory thermodynamic equilibrium inside the stability domain of their vapor (whatever the temperature is). Some natural contexts should allow the superheating of natural aqueous solutions, like the soil capillarity (low T superheating), certain continental and submarine geysers (high T superheating), or even the water state in very arid environments like the Mars subsurface (low T) or the deep crustal rocks (high T). The present paper reports experimental measurements on the superheating range of aqueous solutions contained in quartz as fluid inclusions (Synthetic Fluid Inclusion Technique, SFIT) and brought to superheating state by isochoric cooling. About 40 samples were synthetized at 0.75 GPa and 530-700 °C with internally-heated autoclaves. Nine hundred and sixty-seven inclusions were studied by micro-thermometry, including measuring the temperatures of homogenization (Th: L + V → L) and vapor bubbles nucleation (Tn: L → L + V). The Th–Tn difference corresponds to the intensity of superheating that the trapped liquid can undergo and can be translated into liquid pressure (existing just before nucleation occurs at Tn) by an equation of state. Pure water (840–935 kg m−3), dilute NaOH solutions (0.1 and 0.5 mol kg−1), NaCl, CaCl2 and CsCl solutions (1 and 5 mol kg−1) demonstrated a surprising ability to undergo tensile stress. The highest tension ever recorded to the best of our knowledge (−146 MPa, 100 °C) is attained in a 5 m CaCl2 inclusion trapped in quartz matrix, while CsCl solutions qualitatively show still better superheating efficiency. These observations are discussed with regards to the quality of the inner surface of inclusion surfaces (high P–T synthesis conditions) and to the intrinsic cohesion of liquids (thermodynamic and kinetic spinodal). This study demonstrates that natural solutions can reach high levels of superheating, that are accompanied by strong changes of their physico-chemical properties.

[1]  Zilberbrand A Nonelectrical Mechanism of Ion Exclusion in Thin Water Films in Finely Dispersed Media , 1997, Journal of colloid and interface science.

[2]  Katalin Martinás,et al.  Thermodynamics of Negative Pressures in Liquids , 1998 .

[3]  R. Bakker,et al.  Experimental post-entrapment water loss from synthetic CO2-H2O inclusions in natural quartz , 1991 .

[4]  R. Pugh,et al.  Surface Tension of Aqueous Solutions of Electrolytes: Relationship with Ion Hydration, Oxygen Solubility, and Bubble Coalescence , 1996, Journal of colloid and interface science.

[5]  W. Wagner,et al.  The IAPWS Formulation 1995 for the Thermodynamic Properties of Ordinary Water Substance for General and Scientific Use , 2002 .

[6]  Kai Giese,et al.  ジクロロトロポロンにおける動的水素原子トンネリング 量子的,半古典的及び古典的研究を組み合せた研究 , 2005 .

[7]  R. Bakker,et al.  A mechanism for preferential H2O leakage from fluid inclusions in quartz, based on TEM observations , 1994 .

[8]  R. Goldstein,et al.  Systematics of fluid inclusions in diagenetic minerals , 1994 .

[9]  Yigang Zhang,et al.  Determination of the homogenization temperatures and densities of supercritical fluids in the system NaClKClCaCl2H2O using synthetic fluid inclusions , 1987 .

[10]  Roger M. Smith Superheated water: the ultimate green solvent for separation science , 2006, Analytical and bioanalytical chemistry.

[11]  E. Roedder Metastable Superheated Ice in Liquid-Water Inclusions under High Negative Pressure , 1967, Science.

[12]  B. Yardley,et al.  Solubility of quartz in crustal fluids: experiments and general equations for salt solutions and H2O–CO2 mixtures at 400–800°C and 0.1–0.9 GPa , 2006 .

[13]  Á. Horváth,et al.  Solid–fluid phase transitions under extreme pressures including negative ones , 2008 .

[14]  Y. Shibue Vapor pressures of aqueous NaCl and CaCl2 solutions at elevated temperatures , 2003 .

[15]  L. Briggs Maximum Superheating of Water as a Measure of Negative Pressure , 1955 .

[16]  M. Azaroual,et al.  Capillary geochemistry in non-saturated zone of soils. Water content and geochemical signatures , 2008 .

[17]  Zhenhao Duan,et al.  A high temperature equation of state for the H2O-CaCl2 and H2O-MgCl2 systems , 2006 .

[18]  O. Chienthavorn,et al.  Modified superheated water extraction of pesticides from spiked sediment and soil , 2006, Analytical and bioanalytical chemistry.

[19]  Pablo G. Debenedetti,et al.  Metastable Liquids: Concepts and Principles , 1996 .

[20]  Alan T. J. Hayward,et al.  Negative Pressure in Liquids: Can It Be Harnessed to Serve Man? , 1971 .

[21]  R. Bodnar,et al.  Synthetic fluid inclusions in natural quartz. II. Application to PVT studies , 1985 .

[22]  Zhenhao Duan,et al.  The P,V,T,x properties of binary aqueous chloride solutions up to T=573 K and 100 MPa , 2008 .

[23]  R. Bodnar,et al.  Elastic properties of water under negative pressures , 1993 .

[24]  M. Azaroual,et al.  Geochemistry of unsaturated soil systems: Aqueous speciation and solubility of minerals and gases in capillary solutions , 2005 .

[25]  W. D'angelo,et al.  Effect of pressure on ore mineral solubilities under hydrothermal conditions , 1986 .

[26]  K. Shelton,et al.  Synthetic fluid inclusions in natural quartz , 1979 .

[27]  S. B. Kiselev,et al.  Curvature effect on the physical boundary of metastable states in liquids , 2001 .

[28]  D. Pinti,et al.  The effect of the negative pressure of capillary water on atmospheric noble gas solubility in ground water and palaeotemperature reconstruction , 2004 .

[29]  K. Pitzer,et al.  Equation-of-state representation of phase equilibria and volumetric properties of the system NaCl-H2O above 573 K , 1993 .

[30]  R. Bodnar,et al.  Synthetic fluid inclusions ‐ VI. Quantitative evaluation of the decrepitation behaviour of fluid inclusions in quartz at one atmosphere confining pressure , 1989 .

[31]  C. Angell,et al.  Water and Solutions at Negative Pressure: Raman Spectroscopic Study to -80 Megapascals , 1990, Science.

[32]  Frédéric Caupin,et al.  Cavitation in water: a review , 2006 .

[33]  C A Angell,et al.  Liquids at Large Negative Pressures: Water at the Homogeneous Nucleation Limit , 1991, Science.

[34]  L. Mercury,et al.  Explosive properties of water in volcanic and hydrothermal systems , 2009 .

[35]  M. Zilberbrand On Equilibrium Constants for Aqueous Geochemical Reactions in Water Unsaturated Soils and Sediments , 1999 .

[36]  A. R. Imre,et al.  Liquid–liquid equilibria in polymer solutions at negative pressure , 1998 .

[37]  C. Ramboz,et al.  Superheating in the Red Sea? The heat-mass balance of the Atlantis II Deep revisited , 1990 .

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

[39]  A. R. Imre,et al.  Stability limits in binary fluids mixtures. , 2005, The Journal of chemical physics.

[40]  Robert E. Apfel,et al.  The Tensile Strength of Liquids , 1972 .

[41]  Albert van den Berg,et al.  Capillarity Induced Negative Pressure of Water Plugs in Nanochannels , 2003 .

[42]  L. Mercury,et al.  Explosivity Conditions of Aqueous Solutions , 2009 .

[43]  D H Trevena,et al.  Cavitation and Tension in Liquids , 1987 .

[44]  K. Shmulovich,et al.  An experimental study of phase equilibria in the systems H2O–CO2–CaCl2 and H2O–CO2–NaCl at high pressures and temperatures (500–800 °C, 0.5–0.9 GPa): geological and geophysical applications , 2004 .

[45]  G. Robinson,et al.  Hydrothermal ore-forming processes in the light of studies in rock-buffered systems; I, Iron-copper-zinc-lead sulfide solubility relations , 1992 .

[46]  G. Kell Early observations of negative pressures in liquids , 1983 .

[47]  Lyman J. Briggs,et al.  Limiting Negative Pressure of Water , 1950 .

[48]  M. Azaroual,et al.  Thermodynamic properties of solutions in metastable systems under negative or positive pressures , 2003 .

[49]  Y. Tardy,et al.  Negative pressure of stretched liquid water. Geochemistry of soil capillaries , 2001 .