Ionic Vapor Composition in Critical and Supercritical States of Strongly Interacting Ionic Compounds Vitaly V. Chaban and Oleg V. Prezhdo* , Instituto de Ciê ncia e Tecnologia, Universidade Federal de Sã o Paulo, 12231-280, Sã o Jose ́ dos Campos, SP, Brazil Department of Chemistry, University of Southern California, Los Angeles, California 90089, United States ABSTRACT: The critical point, CP (T, P), of the phase diagram quanties the minimum amount of kinetic energy needed to prevent a substance from existing in a condensed phase. Therefore, the CP is closely related to the properties of the uid far below the critical temperature. Approaches designed to predict thermophysical properties of a system necessarily aim to provide reliable estimates of the CP. Vice versa, CP estimation is impossible without knowledge of the vapor phase behavior. We report ab initio Born-Oppenheimer molecular dynamics (BOMD) simulations of sodium and potassium chlorides, NaCl and KCl, at and above their expected CPs. We advance the present knowledge regarding the existence of ionic species in the vapor phase by establishing signicant percentages of atomic clusters: 29-30% in NaCl and 34-38% in KCl. A neutral pair of counterions is the most abundant cluster in the ionic vapors (ca. 35% of all vaporized ions exist in this form). Unexpectedly, an appreciable fraction of clusters is charged. The ionic vapor composition is determined by the vapor density, rather than the nature of the alkali ion. The previously suggested CPs of NaCl and KCl appear overestimated, based on the present simulations. The reported results oer essential insights into the ionic uid properties and assist in development of thermodynamic theories. The ab initio BOMD method has been applied to investigate the vapor phase composition of an ionic uid for the rst time. INTRODUCTION Ionic compounds (ICs) are omnipresent in chemistry. They are generally known for lower volatility and ammability and a larger liquid-state temperature range, as compared to molecular compounds. 1-19 ICs can be inorganic, organic, and mixed. For instance, many room-temperature ionic liquids (RTILs) 20-28 comprise an organic cation and inorganic anion, whereas inorganic crystals are essential for the Earth crust. Most ICs exhibit hydrophilic properties, to a larger or smaller extent. Furthermore, ICs are signicantly miscible with each other, due to electrostatic forces. The latter feature permits tunability of the physicochemical properties, and, thus, opens up a wide avenue of possible applications. Purely inorganic ICs have high melting, boiling, and critical temperatures, 2,3,6,14 and are used predominantly as solid materials. In turn, mixed and organic ICs can be low melting salts due to unfavorable ionic packing for steric and symmetry reasons. They serve as versatile solvents and tunable reaction media. Because of their organic nature, these ICs thermally decompose well below their critical and even normal boiling points. An accurate knowledge of the critical points (CPs), triple points, and all their parameters constitutes a starting point of many investigations aiming to predict thermophysical proper- ties of ICs, most important of which are liquid state density and surface tension. The thermodynamic behavior of the majority of simple uids is quite universal, provided that the corresponding state variables are expressed in the reduced form. This reduction is achieved by scaling all parameters by their respective values at the CP. Specic intermolecular and interionic interactions, such as hydrogen bonding, dipole- dipole association, and π-electron interactions between relatively large species, complicate correlations of the thermophysical properties and give rise to deviations that are dicult to predict, although major trends still persist. Roman and co-workers 29 published an encouraging theoreti- cal advance, demonstrating a universal behavior of the thermodynamic properties of a wide class of pure uids along the entire vapor-liquid coexistence curve. The CP and triple point parameters are used to convert surface tension (ST), enthalpy of vaporization (EV), and coexistence densities dierence (CEDD) into the corresponding reduced values. Once reduced, the experimental data can be described by a relatively simple expression containing only two empirical parameters, which are specic for every thermodynamic property: the critical-point exponent and the slope at the triple point. Noteworthy, saturation pressure (SVP) does not obey the established universal behavior. SVP is conventionally tted by the three-parameter Antoine equation, whereby the parameters are dierent below and above the normal boiling point. The analyzed uids include noble gases, short-chain alkanes, molecular nitrogen, carbon dioxide, and aprotic polar uids, which may be expected to exhibit more sophisticated trends. Hydrogen-bonded uids, such as water, hydrouoric acid, methanol, carboxylic acids, etc., were omitted from the analysis, together with other uids exhibiting various types of specic site-site intermolecular interactions. Recently, Weiss 30 published an analytic solution of the reformulated problem for selected molecular and ionic Received: March 7, 2016 Revised: April 19, 2016 Published: April 21, 2016 Article pubs.acs.org/JPCB © 2016 American Chemical Society 4302 DOI: 10.1021/acs.jpcb.6b02405 J. Phys. Chem. 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