Fluid Phase Equilibria 338 (2013) 30–36
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Fluid Phase Equilibria
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Vapor–liquid equilibrium for the ternary carbon dioxide–ethanol–nonane and
decane systems
Miguel G. Arenas-Quevedo
a
, Luis A. Galicia-Luna
a,∗
, Octavio Elizalde-Solis
b
, José A. Pérez-Pimienta
c
a
Laboratorio de Termodinámica, SEPI-ESIQIE, Instituto Politécnico Nacional, UPALM, Ed. Z, Secc. 6, 1
ER
piso, Lindavista, C.P. 07738 México, D.F., Mexico
b
Departamento de Ingeniería Química Petrolera, ESIQIE, Instituto Politécnico Nacional, UPALM, Edif. 8, 2
◦
piso, Lindavista, C.P. 07738 México, D.F., Mexico
c
Departamento de Ingeniería Química, Área de Ciencias Básicas e Ingenierías, Universidad Autónoma de Nayarit, Edificio E2, Ciudad de la Cultura Amado Nervo, C.P. 63155 Tepic,
Nayarit, Mexico
a r t i c l e i n f o
Article history:
Received 18 May 2012
Received in revised form 8 October 2012
Accepted 16 October 2012
Available online 23 October 2012
Keywords:
Vapor–liquid equilibrium
Carbon dioxide
Ethanol
Nonane
Decane
a b s t r a c t
In this work, experimental vapor–liquid equilibrium (T, p, x
i
, y
i
) data for the ternary carbon
dioxide–ethanol–nonane and carbon dioxide–ethanol–decane systems are reported in the temperature
range of 313–373 K from low pressures to the nearest of the corresponding critical pressure. Measure-
ments were performed in an apparatus based on the static-analytic method with an on-line ROLSI
sampler-injector device. Vapor–liquid equilibrium (VLE) data for both ternary systems are predicted
using the Peng–Robinson equation of state coupled to the Wong–Sandler, one parameter van der Waals
and two parameters van der Waals mixing rules. Binary interaction parameters are obtained from the
VLE data of binary mixtures reported in the literature.
© 2012 Elsevier B.V. All rights reserved.
1. Introduction
The study of phase equilibrium behavior of multicomponent
systems is necessary in order to understand and establish the tem-
perature (T) and pressure (p) conditions where phases coexist.
Thermodynamic models are used to represent the phase behav-
ior 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 informa-
tion 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 diox-
ide + alkanol + alkane systems is scarcely available in the literature
[5–9]. These studies are about critical end points, critical lines, mis-
cibility windows and isothermal phase diagrams utilizing linear
alkanols (pentanol to dodecanol) and alkanes (tetradecane to tetra-
cosane). 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
∗
Corresponding author. Tel.: +52 55 5729 6000x55133; fax: +52 55 5586 2728.
E-mail address: lgalicial@ipn.mx (L.A. Galicia-Luna).
dioxide + ethanol + nonane or decane at three temperatures in a
wide range of pressure. The experimental VLE results are com-
pared with the prediction using the Peng–Robinson equation of
state with classical and Wong–Sandler mixing rules. Separation fac-
tors between solutes are calculated from experimental vapor and
liquid phase compositions.
2. Experimental
2.1. 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.
2.2. Apparatus
The experimental apparatus where measurements were car-
ried out is based on the static–analytic technique. Details of the
operating principle and its reliability for VLE measurements were
described in previous papers [11,12]. The apparatus is mainly con-
stituted by a 100 cm
3
high-pressure view-cell made of titanium
alloy, a gas chromatograph (Hewlett-Packard, 5890 series II). Both
0378-3812/$ – see front matter © 2012 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.fluid.2012.10.012