Fluid Phase Equilibria 363 (2014) 199–206
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Fluid Phase Equilibria
j ourna l ho me page: www.elsevier.com/locate/fluid
Liquid–liquid equilibrium of the CuSO
4
+ PEG 4000 + H
2
O system at
different temperatures
Martha Claros, María Elisa Taboada, Héctor R. Galleguillos, Yecid P. Jimenez
∗
Department of Chemical and Mineral Process Engineering, Universidad de Antofagasta, Av. Angamos 601, Antofagasta, Chile
a r t i c l e i n f o
Article history:
Received 29 August 2013
Received in revised form
27 November 2013
Accepted 28 November 2013
Available online 11 December 2013
Keywords:
Aqueous two-phase system
Liquid–liquid equilibrium
Polyethylene glycol
Copper sulfate
a b s t r a c t
Phase diagram and liquid–liquid equilibrium (LLE) data for the CuSO
4
+ polyethylene glycol 4000 (PEG
4000) + H
2
O system were determined experimentally at T = 288.15, 298.15 and 308.15 K. The effect of
temperature on the binodal curves and tie-lines was studied and it was found that an increasing in
temperature caused the expansion of two-phase region. The Chen-NRTL and modified Wilson models
were used to correlate the experimental tie-line data. The results show that the quality of fitting is better
with the modified Wilson model.
© 2013 Elsevier B.V. All rights reserved.
1. Introduction
An alternative of liquid/liquid separation process is by aqueous
two phase systems (ATPS), which are usually formed by combining
incompatible polymer/polymer, polymer/salt or salt/salt dissolved
above a certain critical concentration [1]. These systems have
been widely studied [2–5] and are recognized as an economical
and efficient downstream processing method and they offer many
advantages such as short process time, low energy consumption
and are environmentally friendly [6].
Poly(ethylene glycol) (PEG), which is a hydrophilic polymer, is
the most common polymers used with kosmotropic (water struc-
turing) salt to form the polymer–salt ATPSs. The applications of
the polymer based ATPS includes separation, concentration and
fractionation of biological solutes and particles such as cells and
proteins [7–9]. Also, they are used in selective distribution and
separation of metal ion species [10,11].
Currently, organic solvents are the most widely used in cop-
per hydrometallurgical process, but unfortunately these solvents
are highly volatile and pollutants. Whereby, the ATPS represent
an alternative to the traditional solvent extraction process, where
the organic solvents are used. As part of a long-term study, the
liquid–liquid equilibrium data for the ATPS formed by CuSO
4
+ PEG
4000 + H
2
O at T = 288.15, 298.15 and 308.15 K are reported. In future
∗
Corresponding author. Tel.: +56 55 2637902.
E-mail address: yecid.jimenez@uantof.cl (Y.P. Jimenez).
works, these liquid–liquid equilibrium (LLE) data will allow to plan
the partition experiences of metal ions.
Mohsen-Nia et al. [12] reported the phase diagram of the
CuSO
4
+ PEG 20000 + H
2
O system at T = 290.15, 299.15, 308.15, and
317.15 K and the UNIQUAC model was used to correlate the exper-
imental data. de Oliveira et al. [13] reported the equilibrium data
of the poly(ethylene oxide) 4000 + copper sulfate + water system at
T = 278.15, 283.15, 308.15, and 318.15 K. In both works, there is not
report about physical properties in the equilibrium and in the last
work the binodal curves neither were determined.
Regarding to the phase diagram of CuSO
4
+ PEG 4000 + H
2
O sys-
tem, there is no report of this at T = 288.15, 298.15 and 308.15 K.
Moreover, the refractive index, density and kinematic viscosity of
each phase in the equilibrium at T = 288.15, 298.15 and 308.15 K
were measured.
Over the years, the LLE phase diagrams of polymer–salts ATPS
were modeling with models based on the lattice theories, the
Flory–Huggins theory, and on the local composition concepts and
their modifications [14–18], the latter being the most familiar
ones used to represent this kind of LLE phase diagram. In the
present work the Chen-NRTL [19] and modified Wilson [20] mod-
els were applied for the correlation of experimental LLE data of
the aqueous CuSO
4
+ PEG 4000 + H
2
O system at T = 288.15, 298.15
and 308.15 K. The entropy of mixing molecules of different sizes
was represented by the Flory–Huggins expression [21] and to
account for the long-range electrostatic interactions of the ions
the Pitzer–Debye–Hückel equation [22] was used. Additionally, the
effect of temperature on the LLE of the system above mentioned
was also study.
0378-3812/$ – see front matter © 2013 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.fluid.2013.11.038