Vapor–liquid equilibrium for the ternary carbon dioxide–ethanol–nonane and decane systems
Graphical abstract
Highlights
► Equilibrium (p, T, xi, yi) data is reported for ternary systems. ► VLE for CO2–ethanol–nonane, and decane were measured from 313 to 373 K. ► Separation factors for ethanol over decane are higher than ethanol over nonane.
Introduction
The study of phase equilibrium behavior of multicomponent systems is necessary in order to understand and establish the temperature (T) and pressure (p) conditions where phases coexist. Thermodynamic models are used to represent the phase behavior of multicomponent mixtures; however, in some cases these models are not enough accurate and give an approximation of the phase behavior. Therefore, experimental data is the basic information that can be obtained accurately [1], [2]. Experimental methods for the determination of phase equilibrium data are classified with the aim of selecting the one suitable based on the involved phases [3], [4].
The vapor liquid equilibrium behavior for carbon dioxide + alkanol + alkane systems is scarcely available in the literature [5], [6], [7], [8], [9]. These studies are about critical end points, critical lines, miscibility windows and isothermal phase diagrams utilizing linear alkanols (pentanol to dodecanol) and alkanes (tetradecane to tetracosane). However, there is a lack of VLE data for short carbon chains of alkanes and alkanols.
As a continuation of a previous work, we present the vapor–liquid equilibrium behavior for the ternary systems carbon dioxide + ethanol + nonane or decane at three temperatures in a wide range of pressure. The experimental VLE results are compared with the prediction using the Peng–Robinson equation of state with classical and Wong–Sandler mixing rules. Separation factors between solutes are calculated from experimental vapor and liquid phase compositions.
Section snippets
Materials
Properties of chemicals [10] are listed in Table 1. Carbon dioxide of supercritical grade was supplied from Infra Air-Products. Ethanol was purchased from Merck Chemicals and alkanes were provided by Sigma–Aldrich. These were used as received with no previous purification stage. Water content was determined in a Karl–Fisher coulometer and are presented in Table 1 as well as certified purities.
Apparatus
The experimental apparatus where measurements were carried out is based on the static–analytic
Results and discussion
Liquid and vapor equilibrium phase compositions for the carbon dioxide–ethanol–nonane are listed in Table 2 at 313.33, 344.61, and 373.94 K. The corresponding data for the carbon dioxide–ethanol–decane are summarized in Table 3 at 314.98, 344.77, and 373.98 K; uncertainties in composition are also reported at each pressure in both tables based on the carbon dioxide.
Equilibrium ratios Ki = yi/xi for the carbon dioxide–ethanol–nonane are depicted in Fig. 1 and for the carbon dioxide–ethanol–decane in
Conclusions
Equilibrium liquid and vapor phase compositions are reported for the ternary carbon dioxide–ethanol–nonane and carbon dioxide–ethanol–decane systems at temperatures ranging from 313.33 to 373.94 K and 314.98 to 373.98 K, respectively. The Peng–Robinson equation of state using the classical (one and two parameters) and Wong–Sandler mixing rules predict acceptable deviations in pressure and composition the experimental VLE data; nevertheless, two parameter classical mixing rules have a better
Acknowledgments
Instituto Politécnico Nacional and CONACyT are acknowledged for the financial support of this research. Miguel G. Arenas-Quevedo thanks the grant provided by “Programa DELFIN” in 2011.
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