Elsevier

Fluid Phase Equilibria

Volume 502, 15 December 2019, 112285
Fluid Phase Equilibria

Phase equilibrium measurements and thermodynamic modeling of {CO2 + diethyl succinate + cosolvent} systems

https://doi.org/10.1016/j.fluid.2019.112285Get rights and content

Abstract

This work reports experimental phase equilibrium data for the binary systems {CO2(1) + diethyl succinate(2)} and {CO2(1) + ethyl acetate(2)}, and for the ternary systems {CO2(1) + diethyl succinate(2) + ethanol(3)} and {CO2(1) + diethyl succinate(2) + ethyl acetate(3)}. The experiments for the binary system {CO2(1) + diethyl succinate(2)} were carried out at temperatures ranging from 308 K to 358 K, and temperatures ranging from 303 K to 343 K for {CO2(1) + ethyl acetate(2)} as well as for all ternary systems. Only vapor-liquid equilibria were observed for all systems. The experimental measurements were carried out in a high-pressure variable-volume view cell containing a movable piston, which allows pressure control inside the cell. Binary and ternary systems were modeled with the Peng-Robinson cubic equation of state with the van der Waals quadratic mixing rule (vdW2). The presence of a cosolvent (ethanol and ethyl acetate) decreased the saturation pressures of either bubble or dew points compared to the binary system CO2 + diethyl succinate, increasing the solubility of diethyl succinate in CO2.

Introduction

Diethyl succinate (DES) is a diester that occurs naturally in plants. It can be used as a flavoring agent, in fragrances, synthesis of polyesters, plasticizers, food additives, chemical intermediates [[1], [2], [3], [4]], and as a solvent to recover carboxylic acids [5]. A potential method of recovery of DES from plants is via extraction with supercritical carbon dioxide (scCO2). On the other hand, esters such as DES can be synthesized from the esterification of carboxylic acids either catalyzed by enzymes or chemical catalysts in scCO2 medium [[6], [7], [8], [9]]. Another very promising process involving is the CO2 capture with DES as solvent [10]. In all these processes mentioned, a cosolvent use can be an interesting technical strategy in order to enhance the DES solubility in CO2 at high pressure conditions or to promote a synergic effect of mixed solvents. However, phase equilibrium data are imperative for the design of a larger scale process. Phase equilibrium data at high pressures for supercritical fluid systems are scarce and as supercritical fluid applications are increasing, the collection of such data has becoming more important. Supercritical carbon dioxide in particular has been widely studied as a promising alternative solvent for chemical reaction and separation processes because it is nontoxic, inexpensive, easily recycled and has low critical temperature and pressure (Tc = 304.2 K, pc = 7.38 MPa, respectively) [11]. Favorable large-scale application solvents should ideally be highly selective, non-viscous, chemically stable and non-corrosive. CO2 fulfills these requirements. Moreover, as opposed to organic chemical solvents such as methanol, propylene carbonate, and polyethylene glycol dimethyl ether (Selexol) the recovery of which in the desorption stage can be problematic and/or energy intensive, CO2 can be easily recovered by a change in temperature or pressure in the desorption process [10]. Thus, it forms an effective and low-cost physical absorbent, suitable for large-scale industrial applications.

Literature has reported that diethyl succinate (DES) is considered an environmentally adequate solvent because of its low volatility and nearly zero solvent loss, as stated by Li et al. [10]. Feng et al. [3] presented vapor-liquid equilibrium (VLE) data from 308.15 to 328.15 K and pressures up to 13 MPa for the system CO2+DES using a semi-flow type apparatus. Li et al. [10] used a gas-phase recirculation method to determine the VLE data from 288.15 to 318.15 K and pressures up to 2.99 MPa. Gui et al. [12] used the constant-volume method to perform VLE experiments at different temperatures in the range of 285.19–313.26 K and up to 6 MPa. However, a high discrepancy between the VLE data of CO2 + DES presented by those authors can be noted; the most likely reason for such differences in the phase equilibrium measured is because they used a technique with phase sampling. To the best of our knowledge, VLE data of CO2 + DES have not been reported in the literature so far using a synthetic variable-volume view cell (without sampling). Furthermore, no experimental information has been reported on ternary systems involving CO2 + DES + cosolvents.

In this context, the main goal of this work is to report experimental phase equilibrium data for the binary systems {CO2(1)+DES(2)} and {CO2(1)+ ethyl acetate(2)} and for the ternary systems {CO2(1) + DES(2) + ethanol(3)} and {CO2(1) + DES(2) + ethyl acetate(3)}. The experimental results for the systems investigated were modeled using the Peng-Robinson equation of state (PR-EoS) with the conventional quadratic van der Waals mixing rule (vdW2).

Section snippets

Materials

All chemicals employed in this study, their purity, and supplier are presented in Table 1. All compounds were used without further purification.

Apparatus and experimental procedure

The experimental apparatus and procedure used in this work were presented and described in previous publications [[13], [14], [15], [16], [17]]. Briefly, the experimental data measurements were performed in a high-pressure variable-volume view cell containing a movable piston, which allows the pressure control inside the cell. The apparatus also

Thermodynamic modeling

The Peng-Robinson equation of state (PR-EoS) [19], with the conventional quadratic van der Waals mixing rule (vdW2) for both attractive (a) and repulsive (b) terms (equations (1), (2)) was used in this work for modeling the VLE data of both binary and ternary systems investigated.a=ijxixjaiaj(1kij)b=ijxixj(bi+bj2)(1lij)In equations (1), (2), ai and bi stand for pure component parameters related to the PR-EoS [19]. Pcal,i and Pexp,i represent for the calculated and experimental values of

Results and discussion

In order to verify the experimental apparatus and procedure reliability, experimental phase equilibrium data for the system {CO2(1) + ethyl acetate(2)} were obtained (Table 3) and compared to data available in the literature, as presented in Fig. 1. Table 3 presents the reading average temperature (T) and average pressure (P) ± its standard deviations, at a fixed molar composition (x) calculated using the solute mass weighted (±0.0001 g uncertainty, RADWAG AS220/C/2) and the CO2 amount injected

Conclusions

This work reported phase equilibrium data for CO2 + ethyl acetate and CO2 + diethyl succinate (CO2 + DES) binary systems at temperatures ranging from 308 K to 358 K, and CO2 + DES + ethanol and CO2 + DES + ethyl acetate ternary systems at temperatures ranging from 303 K to 343 K. Vapor-liquid equilibrium data (bubble and dew points) were observed for all binary and ternary systems investigated over the temperature and composition ranges evaluated. All systems were modeled with the Peng-Robinson

Acknowledgments

The authors thank the Brazilian agencies CNPq (Grant numbers 305393/2016-2, 408836/2017-2 and 435873/2018-0), Fundação Araucária – State of Paraná (Grant number 004/2019) for financial support and scholarships. E.G., M.L.C., and M.P. acknowledge the funding received from the European Union's Horizon 2020 research and innovation program under the Marie Sklodowska-Curie grant agreement No 778168.

References (29)

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