Elsevier

Fluid Phase Equilibria

Volume 338, 25 January 2013, Pages 128-134
Fluid Phase Equilibria

Vapor–liquid equilibrium of the ethanol + 3-methyl-1-butanol system at 50.66, 101.33 and 151.99 kPa

https://doi.org/10.1016/j.fluid.2012.11.004Get rights and content

Abstract

In this work, the isobaric vapor–liquid equilibrium (VLE) for the ethanol (1) + 3-methyl-1-butanol (2) system at three different pressures is reported. Measurements were done in a dynamic equilibrium cell (Fischer Labodest VLE 602) at 50.66, 101.33 and 151.99 kPa. The experimental data were tested for thermodynamic consistency with total area, point, Van Ness, and Herington tests. Herington test was slightly modified considering the ΔHm/ΔGmE relation. Data were correlated using the NRTL and UNIQUAC activity models. NTRL showed the lowest deviation with respect to the experimental data at the three operating pressures. Quality of regressed parameters for this system was tested comparing results with isothermal equilibrium data reported elsewhere.

Highlights

► The VLE data of ethanol + 3-methyl-1-butanol were measured at three different pressures (50.66, 101.33 and 151.99 kPa). ► Equilibrium measurements were done in a dynamic equilibrium cell (Fischer Labodest VLE 602). ► Total area, Van Ness, point and Herington tests were used as thermodynamic consistency tests. ► NRTL and UNIQUAC were used as activity models to fit the experimental data.

Introduction

In recent years due to the current efforts for making biofuels as an alternative for fossil fuels, ethanol industry and its by-products have been growing very fast. Among them, fusel oil obtained during bioethanol distillation can be considered a valuable raw material for several by-products of industrial interest. It is mainly composed of isoamyl alcohol, water, isobutanol, ethanol and other short-chain alcohols (C2single bondC5). Yields of fusel oil in an industrial plant may vary between 1 and 11 L/1000 L of ethanol produced (absolute basis) depending on the substrate, nitrogen-containing additives and conditions used during fermentation, and also on distillation conditions [1]. Regarding to the composition, Patil et al. [1] presents a characterization of fusel oil in terms of two main fractions: a low boiling fraction (LBF) and a high boiling fraction (HBF). The first one corresponds to 95–98% (v/v) and is mainly composed by isoamyl alcohol (60–80%), ethanol (5–15%) and water (8–20%) [1]. The other fraction is composed by fatty acids and their esters, some pyrazines and unsaponificable material. Due to the low yield and the difficulties related to the isolation of pure alcohols from fusel oil, it is traditionally burned in steam boilers or blended with the fuel ethanol. However, fusel alcohols can be used as low cost and renewable sources for the production of biosolvents, flavoring agents, pharmaceuticals and plasticizers. These higher added-value products have the potential for improving the overall economics of the bioethanol plants [2]. According to this, it is expected that in the future, bioethanol plants will be able to tune the fermentation process in order to generate the ethanol by-products profile that maximizes profits depending on market demands.

In order to develop separation and purification strategies for isoamyl alcohol from fusel oil, a good representation of vapor–liquid equilibrium in mixtures with water and ethanol is required. Systems containing ethanol, water and other alcohols have been widely studied [3], [4], [5], [6], [7], [8]. Specifically, the system isoamyl alcohol + ethanol has been studied by Martinez et al. [9] and Sanz and Gmehling [10]. Martinez et al. [9] worked on the equilibrium with 2-methyl-1-butanol + ethanol at 33.6, 66.6 and 101.3 kPa in a modified Othmer still, while Sanz and Gmehling [10] worked on isothermal VLE of both isoamyl alcohols, 2-methyl-1-butanol and 3-methyl-1-butanol, determined experimentally by head space gas chromatography. In this work isobaric VLE for ethanol with isoamyl alcohol was measured experimentally using a VLE 602 Fischer Labodest apparatus at 50.66, 101.33 and 151.99 kPa.

In order to validate the quality of data, thermodynamic consistency tests were used. Several consistency tests have been investigated over the past years [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22]. Samuels [11] and Kojima et al. [12] have presented area tests while other authors suggested the use of point tests or tests based on activity coefficients at infinity dilution [15], [16], [17], [18], [19]. Kang et al. [13] presented a wide review of commonly used consistency tests and introduced a data–quality criterion in order to summarize different tests results. Taking into account the above, consistency of experimental data was evaluated using an area test according to the accepted criteria of Kojima, Wisniak, Redlich–Kister [12], [13], [19], [20], [21], [22], point test [15], [16] and Van Ness test [18].

Section snippets

Materials

Ethanol (>99.0% weight, assay GC) was purchased from Quisol Ltd. 3-Methyl-1-butanol (>99.5% weight, assay GC) was supplied by J.T. Baker. 1,4-Dioxane (>99.8% weight, assay GC) and methyl ethyl ketone (>99.8% weight, assay GC) were used as internal standard and solvent for chromatographic analyses, respectively, and were provided by Merck KGaA. Ethanol was purified to >99.8% weight by dehydration with zeolite A (W.R. Grace & Co.) and then by distillation in a batch system. Other reagents were

Thermodynamic consistency tests

Despite the availability of vapor pressure data for 3-methyl-1-butanol reported in the open literature [23], [24], [25], [26], [27], measurement of the vapor pressure for this alcohol was done in order to test the performance and reliability of the equilibrium still used in this work. Experimental results are listed in Table 3. A numerical regression was performed to fit vapor pressure data with the Antoine equation and the parameters obtained are presented in Eq. (1). A maximum error of 1.3 kPa

Conclusions

Isobaric vapor–liquid equilibrium of ethanol + 3-methyl-1-butanol at three different pressures has been investigated. Also, vapor pressure data for 3-methyl-1-butanol were measured and well correlated with Antoine equation. Agreement between the experimental and calculated VLE at three different pressures, was found. Equilibrium data were tested for thermodynamic consistency using Redlich–Kister area test, Van Ness test and point test. Measured data were found to be thermodynamically consistent

List of symbols

    A*

    total area of Redlich–Kister test (Eq. (4))

    A12, A21

    parameters of Margules model (Eq. (7))

    a, b

    parameters of NRTL activity model

    D, J

    parameters of Wisniak test

    G

    Gibbs free energy (J mol−1)

    H

    enthalpy (J mol−1)

    L

    area upon abscissa in area test plot

    n

    polynomial order (Eq. (6))

    OF

    objective function

    P

    pressure (kPa)

    q

    surface parameter of the UNIQUAC model

    r

    size parameter of the UNIQUAC model

    R

    universal gas constant (J mol−1 K−1)

    T

    temperature (K)

    W

    area below abscissa in area test plot

    x

    mole fraction in liquid

    y

    mole

Acknowledgements

This work has been supported by Colciencias, Ecopetrol S.A. and Universidad Nacional de Colombia (Project No. 1101-490-26038). J. Duran acknowledges to Rotary Club Intl. Bogota – Chapinero for financial support received during his postgraduate studies.

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