Journal Pre-proof [DCA]-based ionic liquids for the extraction of sulfur and nitrogen compounds from fuels: Activity coefficients at infinite dilution Urszula Domańska, Michał Wlazło, Monika Karpińska PII:
S0378-3812(19)30486-8
DOI:
https://doi.org/10.1016/j.fluid.2019.112424
Reference:
FLUID 112424
To appear in:
Fluid Phase Equilibria
Received Date: 18 September 2019 Revised Date:
21 November 2019
Accepted Date: 22 November 2019
Please cite this article as: U. Domańska, Michał. Wlazło, M. Karpińska, [DCA]-based ionic liquids for the extraction of sulfur and nitrogen compounds from fuels: Activity coefficients at infinite dilution, Fluid Phase Equilibria (2019), doi: https://doi.org/10.1016/j.fluid.2019.112424. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2019 Published by Elsevier B.V.
Fluid Phase Equilibria
[DCA]-based ionic liquids for the extraction of sulfur and nitrogen compounds from fuels: activity coefficients at infinite dilution Urszula Domańskaa,b*, Michał Wlazłoc, Monika Karpińskac,d a
Industrial Chemistry Research Institute, Rydygiera 8, 01-793 Warsaw, Poland.
b
Thermodynamic Research Unit, School of Chemical Engineering, University of KwaZulu-
Natal, Howard College Campus, King George V Avenue, Durban 4001, South Africa. c
Department of Physical Chemistry, Faculty of Chemistry, Warsaw University of Technology,
Noakowskiego 3, 00-664 Warsaw, Poland. d
The Kielanowski Institute of Animal Physiology and Nutrition, Polish Academy of Sciences,
Instytucka 3, 05-110 Jabłonna, Poland.
Received: 18 September 2019 Keywords: Ionic liquids [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA]
Activity coefficients at infinite dilution Thermodynamics Extraction
*
Corresponding author
E-mail address:
[email protected] (U.Domańska).
1
ABSTRACT Some petroleum processes need the removal of low level aromatic-sulfur and nitrogen compounds for many products, which are extremely important according to the new strict environmental regulations to reduce sulfur and nitrogen content compounds in liquid fuels. Thus the new, alternative solvents such as ionic liquids (ILs) have been proposed. ILs reveal a high selectivity and capacity of extraction of sulfur- and nitrogen-compounds from alkanes with little solvent loss during the process. The measurements of activity coefficients γ 13∞ at infinite dilution of different solutes in the IL shows the effect of interactions between organic solutes, or water on the interfacial and bulk properties of the IL. The new (3cyanopropyl)pyridinium
dicyanamide,
[N-C3CNPy][DCA]
and
(3-
cyanopropyl)methylpyrrolidinium dicyanamide, [N-C3CNMPyr][DCA] were investigated in this work. The data were obtained using the gas-liquid chromatography technique. Measurements were undertaken at six temperatures, in 10 K intervals, in the range of (318.15 to 368.15) K. The solutes studied included both non-polar and polar compounds, as alkanes, alkenes, alkynes, as well as aromatic hydrocarbons, alcohols, water, ethers, ketones, and esters. The most important solutes used were thiophene, pyridine, and 1-nitropropane. Densities, ρ, measurements for a range of temperatures, T (298.15 -368.15) K for the chosen ILs were undertaken at pressure, p = 101 kPa. The gas-liquid partition coefficients, K L at infinite dilution were calculated. The fundamental thermodynamic functions such as partial molar excess Gibbs energy, enthalpy and entropy at infinite dilution were calculated from the experimental data measurements to discuss the interaction between solutes and the ILs. The values of selectivity and capacity for three separation cases, viz. heptane/thiophene, heptane/pyridine, and heptane/1-nitropropane were calculated from γ 13∞ values and compared to literature data for dicyanamide-based ILs. The Abraham solvation parameter model was
2
presented for all solutes. The obtained results indicated that [N-C3CNPy][DCA] has large selectivity and capacity values for all three of the separation cases studied.
3
1.
Introduction In recent years, the deep desulfurization of diesel fuel has become the most studied process
with different techniques (extraction, liquid-liquid separation, oxidative desulfurization, adsorption). The emission of sulphur- and nitrogen- compounds from petrol and diesel oils, which is linked to acid rain phenomena, plays a crucial role in pollution problems of large conglomerates. From decades the new regulations regarding of sulfur content in fuels are restricted in USA and Europe [1,2]. Ionic liquids (ILs) have the ability of extracting aromatic sulfur- and nitrogen-containing compounds at ambient conditions. Additionally, ILs are immiscible with fuel, are non-volatilate and can be regenerated and recycled by solvent washing. At present, hydrodesulfurization (HDS) processes is the established method used in some industrial technologies to remove organic sulphur-compounds but without polycyclic organic sulfides such as thiophene, benzothiophene, methyldibenzothiophenes, 4,6dibenzothiophenethiols, thioethers, and disulfides [3]. The HDS technology needs high temperature, high pressure, large reactor volumes, and expensive active catalyst [3]. Therefore, new scientific achievements for deep desulfurization and denitrogenation of fuels have become very important. The use of ILs as a ne solvents is suggested by many authors [416]. Preliminary information about suitable solvents for separation can be obtained from activity coefficients at infinite dilution ( γ 13∞ ) measurements using the gas-liquid chromatography (GLC) technique. The information obtained from infinite dilution activity coefficients is generally the first step in the engineering design process to determine the most suitable extraction and separation processes. The use of predictive models, such as Mo UNIFAC, PC SAFT, or COSMO RS are to date not accurate and reliable enough for the design of separation processes and restricted to the description of simple systems only [17-20]. Thus, the importance and need for experimental data is observed.
4
Solvent suitability can also be determined from liquid-liquid phase equilibrium measurements in ternary systems (LLE) [21-28]. The suitability of using four different, more specific
ILs,
such
as
trisfluorotris(perfluoroethylphosphate methylmorpholinium
4-(2-methoxyethyl)-4-methylmorpholinium [COC2MMOR][FAP],
bis{(trifluomethyl)sulfonyl}imide
methoxyethyl)-1-methylpyrrolidinium [COC2MPYR][FAP]
4-(2-methoxyethyl)-4-
[COC2MMOR][NTf2],
1-(2-
trisfluorotris(perfluoroethylphosphate,
and
1-(2-methoxyethyl)-1-methylpyrrolidinium
bis{(trifluomethyl)sulfonyl}imide [COC2MPYR][NTf2] as solvents in liquid–liquid extraction at T = 298.15 K was presented by our group [21,22]. The results in that research showed that out of these four ILs, the [COC2MMOR][NTf2] was the best solvent for the sulfur compounds/aliphatic hydrocarbons separation [21,22]. Attractive extraction selectivities were obtained
for
1-ethyl-3-methylimidazolium
bis{(trifluoromethyl)sulfonyl}imide,
[EMIM][NTf2] ([23] and references therein), 1-ethyl-3-methylimidazolium thiocyanate, [EMIM][SCN] [7] and 1,3-dimethylimidazolium methylphosphonate [DMIM][MP] [7]. The pyrrolidinium-based ILs with different anions [25], or 1-alkylpiperidinium-based [28], or 1alkylcyanopyridinium-based ILs [27] have been studied in our laboratory in ternary LLE {IL + thiophene, or benzothiophene + heptane) with high selectivities, especially for 1alkylcyanopyridinium-based ILs [27]. Even better results of extraction of thiophene and benzothiophene were obtained with 1-ethyl-3-methylimidazolium tricyanomethanide, [EMIM][TCM] IL [26]. Promising results were obtained with tricyanomethanide-based, [TCM]- and dicyanamide-based [DCA]- ILs in ternary LLE [10]. The investigated in that work ILs revealed as high as 78 and 87 mass % of extracted thiophene and benzothiophene, respectively. The selectivity was in the order [M3BPY][DCA] ~ [BMIM][TCM] > [M4BPY][DCA] > [M4BPY][SCN] > [BMIM][DCA] > [BMIM][SCN] [7]. Many works reported that there is a great potential for using ILs with cyano group, CN- in the cation, or in
5
the anion as good solvents for the separation of sulfur compounds from aliphatic hydrocarbons due to their remarkable selectivity towards sulfur compounds [11,21,22,25,26]. ∞ Selectivities, S12∞ = γ 13∞ / γ 23 and capacities, k 2∞ = 1 / γ 2∞ for the heptane/thiophene separation
problem, calculated from the limiting activity coefficient at T = 328.15 K for the best [DCA]based ILs are as follows: for [N-C3OHMMor][DCA] ( S12∞ = 417, k 2∞ = 0.32 at T = 308.15K) [29], [EMMor][DCA] ( S12∞ = 273, k 2∞ = 0.42) [30], [N-C3OHPy][DCA] ( S12∞ = 163, k 2∞ = 0.37) [31], [N-C3OHMIM][DCA] ( S12∞ = 156, k 2∞ = 0.39) [29], and for [N-C3CNMIM][DCA] ( S12∞ = 138, k 2∞ = 0.41) [32]. The aim of this study is to overcome the solvent separation ability for new [DCA]-based ILs by an analysis of their selectivities and capacities, calculated from γ 13∞ values. Solutes, heptane, thiophene, pyridine, 1-nitropropane used in this work are model substances for fuel and sulphur- or nitrogen-organic compounds, respectively. In this work we continue our investigations on the measurements of γ 13∞ and an analysis of the obtained selectivities and capacities for heptane/thiophene heptane/pyridine, and heptane/1-nitropropane separation processes. This work proposes to study a particular type of ILs, synthesized in our laboratory, (3-cyanopropyl)pyridinium
dicyanamide,
[N-C3CNPy][DCA]
and
(3-
cyanopropyl)methylpyrrolidinium dicyanamide, [N-C3CNMPyr][DCA] as a function of temperature at ambient pressure to compare the results with data previously measured in our laboratory. According to many sources in literature, the high interaction of cyano group of the IL is causing the strong interaction between the cation of the IL and aromatic compounds. In this paper we report the activity coefficients, γ 13∞ at infinite dilution, the gas-liquid partition coefficients K L and thermodynamic functions at infinite dilution for all measured solutes. The thermodynamic properties obtained are analyzed with regard to the intermolecular
6
interactions. The Abraham solvation parameter model was also presented for all solutes. The densities of the ILs were performed as a function of temperature.
2.
Materials and methods
2.1.
Chemicals
The ILs used in this work were synthesized in our laboratory. Synthesis, 1H NMR, 13C NMR spectra were described earlier [33]. The structure, name, abbreviation and molar mass results and purification method and purity are shown in Table 1. The different solutes, purchased from Aldrich or Fluka, had purities better than 0.97 mass fraction and were used without further purification due to the fact that the GLC technique separates any impurities on the column. The specification and purity is shown in Table 1S in the Supplementary Material (SM).
2.2. Water content The water content of the solvents was analyzed by the Karl-Fischer titration technique (method TitroLine KF). The sample of IL, or solvent was dissolved in methanol and titrated in steps of 0.0025 cm3. The uncertainty on the water content was u (w.c.) = 10 ppm for the 3 cm3 sample of IL injected. The water content in ILs was < 500 x10-6 in mass fraction.
2.3. Density measurements The density of the ILs was measured using an Anton Paar GmbH 4500 vibrating-tube densimeter (Graz, Austria), thermostated over a temperature range of (298.15-368.15) K. Two integrated Pt-100 platinum thermometers provided good precision in temperature control internally (T± 0.01 K). The densimeter has an automatic correction for the viscosity of the 7
sample. The apparatus is precise to within 1⋅10-5g cm-3, and the uncertainty of the measurements was estimated to be u (ρ) = ± 1.1· 10−3g cm-3. The densimeter’s calibration was performed at atmospheric pressure using doubly distilled and degassed water (PURE LAB Option Q Elga Water System), specially purified benzene (CHEMIPAN, Poland 0.999), and dried air. The densities of ILs are listed in Table 2. The only literature data was found for [NC3CNPy][DCA], ρ/g cm–3 = 1.168 at 293.15 K, which agreed very well to our measurements [34] and for [N-C3OHPy][DCA], ρ/g cm–3 = 1.17636 at 298.15 K [31]. The information in the whole temperature range for [N-C3OHPy][DCA] is shown in Table 2S and in Fig. 1S in the SM [31].
2.4. Apparatus and experimental procedure Experiments were performed using a Perkin Elmer Clarus 500 gas chromatograph equipped with a thermal conductivity detector (TCD). The data were collected and processed using the TotalChrom Workstation software. The column preparation and the packing method used in this work have been described in detail in our previous work [30,31]. Glass columns of length 1 m, with a 4 mm internal diameter were used. The solid support Chromosorb W/AW-DCMS 100/120 mesh was supplied by Sigma-Aldrich. Coating of the solid support material with the IL was performed by dispersing a certain portion of the IL in methanol, followed by evaporation of the solvent using a rotary evaporator. The masses of the stationary phase and of the solid support were weighed with a precision ±0.0001 g, achieving an uncertainty in the IL loading on the column in the order of 2 × 10–4mmol. The solvent loading on the column for [N-C3CNPy][DCA] was 50.30% and 45.42% mass percent, and for [N-C3CNMPyr][DCA] it was 44.88% and 49.82% mass percent. In our experimental work we always use the large column loading, which prevents possible residual adsorption of solute onto the column packing. The methanol was completely evaporated from the IL-coated solid support prior to 8
column fabrication. Prior to each experiment, the column was conditioned by blowing hot carrier gas through it at a high flow rate (~2.0 cm3⋅s–1) at T = 370 K for about 8 h. The pressure drop (pi – po) was varied between 10 and 80 kPa depending on the flow rate of the carrier gas. The inlet pressure, pi, was measured by a pressure gauge installed on the gas chromatograph with an uncertainty of ±0.1 kPa and the outlet pressure, po, was measured using an Agilent Precision Gas Flow Meter having an uncertainty of ±0.07 kPa. The mean column pressure, p inlet column pressure, pi, outlet column pressure, po and standard state of solutes at given temperatures and standard state are listed in Table 3S in the SM. Helium was the carrier gas used in the measurements. The flow rate of carrier gas was determined using an Agilent precision gas flow meter, which was placed at the outlet after the detector and had an uncertainty of ±0.1 ml min–1. The flow rate was set for a series of runs and was allowed to stabilize for at least 15 min before any γ 13∞ determinations were made. Solute injections ranged from 0.01 to 0.3 µl and can be considered to be at “infinite dilution” on the column. Temperature-dependent experiments were carried out in 10 K steps from (318.15 to 368.15) K. The temperature of the column was maintained constant to within ±0.02 K. Each experiment was repeated at a given temperature, two to three times to establish reproducibility. Retention times were generally reproducible to within 10–3 to 10–2 min depending upon the temperature and the individual solute. At each temperature, values of the dead time, tG, equivalent to the retention time of a completely non-retained component were also measured. While our GC was equipped with a TCD detector, air was used as a nonretainable component. The estimated overall error in γ 13∞ was less than 3%, taking into account the possible errors in determining the column loading, the retention times, and solute vapor pressure. The resultant activity coefficient values as a function of temperature are
9
summarized in Tables 3 and 4 for [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively.
3. Theoretical basis The well known equations developed by Everett [35] and Cruickshank et al. [36] were used as in all our works to calculate γ 13∞ for solutes in ILs:
(
)
(
n RT p * B − V * p J 3 2 B12 − V1∞ ln γ 13∞ = ln 3 * − 1 11 1 + o 2 RT RT V N p1
)
(1)
In this expression, n3 is the number of moles of solvent on the column packing, R is the Universal Gas Constant, T is the column temperature, VN denotes the net retention volume of the solute, p1* is the saturated vapor pressure of the solute at temperature T, B11 is the second virial coefficient of pure solute, V1* is the molar volume of the solute, po is the outlet pressure, p o J 23 is the mean column pressure, B12 (where the subscript “2” refers to the carrier gas, in
this case helium) is the mixed second virial coefficient of the solute and carrier gas, and V1∞ is the partial molar volume of the solute at infinite dilution in the solvent. The thermophysical properties required in developing the activity coefficients at infinite dilution were calculated using equations and constants known from literature [37]. The values of B12 were calculated using the Tsonopolous equation [38]. Most of the calculated data were presented in our earlier work [39]. The pressure correction term, J 23 , is given by:
2 ( pi / po ) − 1 3 ( p i / p o )2 − 1 3
J 23 =
(2)
10
The net retention volume of the solute, VN, is given by:
V N = ( J 23 ) −1U o (t R − t G )
(3)
where tR and tG are the retention times for the solute and an unretained gas, respectively, and Uo is the column outlet flow rate, corrected for the vapor pressure of water by: p T U o = U 1 − w po T f
(4)
where Tf is the temperature at the column outlet, pw is the vapor pressure of water at Tf, and U is the flow rate measured with the flow meter. While the activity coefficients at infinite dilution are determined as a function of temperature, ln γ 13∞ can be split to its respective partial molar excess thermodynamic functions:
ln γ 13∞ =
∆H 1E ,∞ ∆S1E ,∞ − RT R
(5)
Assuming that the temperature dependence follows a linear van’t Hoff plot:
ln γ 13∞ = a T + b
(6)
the partial molar excess enthalpy, ∆H1E , ∞ = Ra , at infinite dilution can be obtained from the slope.
11
(
)
The gas-liquid partition coefficient K L = c1L c1G for a solute partitioning between a carrier gas and the ILwas calculated from the solute retention according to the following equation
(
V ρ P J 3 2 B12 − V1∞ ln (K L ) = ln N 3 − o 2 RT m3
)
(7)
In which ρ3 is the density of the IL and m3 is the mass of the IL and V1∞ is the partial molar volume of the solute at infinite dilution.
3.1. The Abraham solvation parameter model The Abraham solvation parameter model is presented by the eqn. (8) [40,41]:
Log KL = c + e E + s S + a A + b B + l L
(8)
The independent variables in eqn. (8) are the solute descriptors [40-45], which are as follow: E is the solute excess molar refraction in units of (cm3 mol–1)/10, S is the solute dipolarity/polarizability, A and B are the overall or summation solute hydrogen bond acidity and basicity, and L is the logarithm of the gas-hexadecane partition coefficient at temperature T = 298 K. Solute descriptors are available for more than 4000 organic and organometallic compounds. The six regression coefficients (c, e, s, a, b, and l) relate to the properties of the solvent phase and they are determined by regression analysis from experimental KL values. The c coefficient is the model constant taking into account opposing contributions of different effects: e – interactions with lone pair electrons, s – dipole-type interactions, a and b – the hydrogen-bond basicity and acidity of the stationary phase respectively, l – cavity formation and dispersion interactions.
12
4. Results and discussion
Densities of [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA] were measured in this work as a function of temperature and are listed in Table 2 together with the information from literature for one data point. The density measurements were carried out in the temperature range from (298.15 to 368.15) K at pressure p = 101 kPa. The values obtained at T = 298.15 K are 1.16664 g cm–3 and 1.09640 g cm–3for [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively. The average values of γ 13∞ for the measured solutes in [N-C3CNPy][DCA] and [NC3CNMPyr][DCA], determined at six temperatures in a range of temperature from (318.15 to 368.15) K at pressure p = 101 kPa are listed in Tables 3 and 4, respectively. An analysis of the values of γ 13∞ shows large differences in possible interaction between a solute and the IL at infinite dilution. The data for [N-C3CNPy][DCA] shows almost two times larger values of γ 13∞ for the non-polar solutes in comparison with
[N-C3CNMPyr][DCA], which means much lower
interaction between the pyridinium-based cation with hydrocarbons than those of the pyrrolidinium-based cation. Aromatic hydrocarbons show also higher values of γ 13∞ for [NC3CNPy][DCA] in comparison with [N-C3CNMPyr][DCA], but the differences are not so large. The interaction between solutes and the IL for polar substances, such as alcohols and water is similar for both ILs. Important values of the discussed in this paper solutes at T = 328.15 K are: for heptane γ 13∞ = 702 or γ 13∞ = 417 in [N-C3CNPy][DCA] and [NC3CNMPyr][DCA], respectively; for thiophene γ 13∞ = 3.14 or γ 13∞ = 1.98 in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively; for pyridine γ 13∞ = 2.02 or γ 13∞ = 3.08 in [N-
13
C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively and for 1-nitropropane γ 13∞ = 1.54 or
γ 13∞ = 2.12 in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively. For all these solutes, the interaction with the ILs is almost the same for both ILs discussed. This my suggests that the differences in selectivity will be not very large for the selected ILs. Similar values were observed in our earlier work for 1-benzyl-3-methylimidazolium dicyanamide, [BzMIM][DCA]. For example for pyridine it was ( γ 13∞ = 1.03) at T = 328.15 K [46]. The influence of the alkyl chain length in a series of alkanes, cycloalkanes, alkenes, alkynes, aromatic hydrocarbons (increasing radicals), alcohols, ethers, and ketones drawn from Tables 3 and 4 shows that the γ 13∞ values increase with the alkyl chain length, which is an indication of the decrease of interactions between the solute and the IL at infinite dilution. Furthermore, despite the lower number of alkyl chains, the higher measured retention time is an evident observation of the decrease of the γ 13∞ values, and of an increase in the interactions between the IL and solute. The strongest interaction (the lowest values of γ 13∞ at all temperatures) is observed for water ( γ 13∞ = 0.434) and ( γ 13∞ = 0.338) for [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively. The largest values of γ 13∞ provide the initial information about the lower interactions. As for all ILs, measured by us, the largest values are observed for nonane ( γ 13∞ = 1390), or ( γ 13∞ = 928), decane ( γ 13∞ = 1839), or ( γ 13∞ = 1329), and dec-1-ene ( γ 13∞ = 1077), or ( γ 13∞ = 695) for [NC3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively. The values for [BzMIM][DCA] were lower: for nonane ( γ 13∞ = 332), for decane ( γ 13∞ = 509) and dec-1-ene ( γ 13∞ = 220) at T = 328.15 K [46]. An interesting features worth to be mentioned are the values obtained for the IL, 1allyl-3-methylimidazolium dicyanamide, [AMIM][DCA], which shows the same relations in
14
the interactions for the measured solutes. Strong interactions of [AMIM][DCA] were observed with water ( γ 13∞ = 0.341 at T = 328.15 K), all alcohols, thiophene, pyridine and 1nitropropane with γ 13∞ < 2 at T = 328.15 K [47]. Nonetheless, the low values of γ 13∞ for polar solutes such as thiophene, pyridine, and 1-nitropropane obtained for the measured ILs suggest the high potential for the extraction of these compounds from alkanes, which is important in petrochemical processes, e.g. desulphurization and denitrification of fuels. The endothermic and exothermic effects accompanying the interactions of solutes with the IL are presented in Figs 2S-15S in the SM. These diagrams show the plot of the natural logarithm of the γ 13∞ as a function of the inverse absolute temperature for all investigated solutes. The γ 13∞ values decrease with an increasing temperature for alkanes, alkenes, cycloalkanes and cylcloalkenes (see Figs. 2S and 3S in the SM for [N-C3CNPy][DCA] and Figs. 9S and 10S for [N-C3CNMPyr][DCA]). The opposite influence of temperature is presented for alkynes in both ILs (see Figs. 3S and 10S in the SM) and for aromatic hydrocarbons (see Figs. 4S and 11S in the SM). Only for propylbenzene and isopropylbenzene in [N-C3CNPy][DCA] the γ 13∞ values decrease with an increasing temperature as it is illustrates in Fig. 4S in the SM. The values of γ 13∞ for methanol and water (Fig 5S and 12S in the SM) as well as for diethyl ether, di-iso-propyl ether and MTBE (Fig 6S and 13S in the SM) for both ILs increase with an increasing temperature. The values of γ 13∞ for esters, ketones, THF, 1,4-dioxane and thiophene in both ILs increase with an increasing temperature (see Fig. 7S for [N-C3CNPy][DCA] and Figs. 14S and 15S for [N-C3CNMPyr][DCA] in the SM). The gas-liquid partition coefficient, K L , calculated from eqn. 7 is an important property of the IL. This property shows the suitability of the IL for particular application in extraction. The data for [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], are listed in Tables 5 15
and 6. From these Tables we can see that the lowest values are observed for alkanes ( K L = 0.927 and K L = 1.43 for heptane at T = 328.15 K in [N-C3CNPy][DCA] and [NC3CNMPyr][DCA], respectively) cycloalkanes, cylcloalkenes, alkenes, alkynes and ethers. The large values of K L are observed for water ( K L = 2158 and K L = 2533 at T = 328.15 K in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively), for 1-pentanol ( K L = 824 and K L = 1265 at T = 328.15 K in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively),
and for 1-nitropropane ( K L = 753 and K L = 1001 at T = 328.15 K in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively). These values are much lower than those observed for [AMIM][DCA] [47]. The large K L values correspond to a large affinity of the solute to the liquid phase. The K L value increases with a decrease of temperature and with an increase of the alkane chain length for alkanes, alkenes, alkynes, cycloalkanes, alcohols, esters and ethers. The K L values increase with an increase of the radicals in the aromatic compounds. Table 7 lists the partial molar excess Gibbs energies, ∆G1E,∞ , at infinite dilution, the partial molar excess enthalpies, ∆ H 1E, ∞ , at infinite dilution, and the partial molar excess entropies at infinite dilution, Tref ∆S1E , ∞ , for all the solutes studied at reference temperature T = 328.15 K. These thermodynamic functions describe the interaction between solute and the IL and are an important pointer in determining the suitability of the IL for extraction. The ∆G1E,∞ was calculated from the temperature dependence of γ 13∞ from eqns. 5 and 6. The values of ∆G1E,∞ are positive for all solutes except methanol, water for both ILs and acetonitrile in
pyrrolidynium-based IL. This is similar to the earlier measured data for [BzMIM][DCA] [46] and [AMIM][DCA] [47]. The infinite dilution activity coefficient values are lower than one for these solutes, i.e. γ 13∞ < 1, which corresponds to the (IL + solute) binary system with negative deviations from Raoult's law. For the remaining solutes, including decane ( ∆G1E,∞ =
16
20.5 kJ mol-1 and ∆G1E,∞ = 19.6 kJ mol-1 in [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA], respectively) positive deviations from ideality are obtained. The partial excess molar enthalpies at infinite dilution, ∆ H 1E, ∞ , determined from the Gibbs-Helmholtz equation exhibit negative values for alkynes, aromatic hydrocarbons (excluding propylbenzene and isopropylbenzene in [N-C3CNPy][DCA]), esters some ethers, ketones and 1-nitropropane for both ILs. For these solutes relatively strong energetic solute-solvent interactions are observed. Additionally, there are negative ∆ H 1E, ∞ values for both ILs with water and methanol. As expected, the ILs used in this work, exhibits possible π - π, or n - π interactions with most of the solutes, which leads to negative values of ∆ H 1E, ∞ and
Tref ∆S1E , ∞ . Mainly for aliphatic
hydrocarbons, the endothermic interaction, resulting from the energetic weakness of their interaction with the IL is observed. The partial excess molar entropies at infinite dilution, Tref ∆S1E , ∞ , are small and negative for almost all solutes studied for both ILs. The solution of the majority of the solutes in both ILs is accompanied by entropy losses, which may suggest that the solute molecule arranges itself in the IL structure.
5. Separation of heptane/thiophene, heptane/pyridine and heptane/1-nitropropane The comparison of the values of activity coefficients, γ 13∞ for both ILs measured in this work with similar [DCA]- based ILs such as [N-C3OHPY][DCA] [31], [N-C3CNMIM][DCA] [48], [BMPy][DCA] [49] and [BMPyr][DCA] [50] is presented in Fig.1. As we can see, the highest values of γ 13∞ for almost all solutes are for [N-C3CNPy][DCA] and lower than these values (stronger interaction) are for [N-C3CNMPyr][DCA]. The lowest values (the stronger interaction) was however observed for [BMPy][DCA] [49]. To make the analysis of the
17
performance of the [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA] ILs as an extraction solvents for the discussed in this work separation processes, the characteristic parameters for the separation, the selectivity ( S 12∞ = γ 1∞ / γ 2∞ ) and the capacity ( k 2∞ = 1 / γ 2∞ ) were calculated from the experimental γ 13∞ values. The results are presented in comparison with different ILs for heptane (1)/thiophene (2) at temperature T = 328.15 K, along with literature data for some ILs with the same anion, [DCA]-. The analysis presented in Fig. 2 included [NC3OHMMor][DCA]
[29],
[N-C3OHMIM][DCA]
[29],
[EMMor][DCA]
[30],
[N-
C3OHPy][DCA] [31], [EMIM][DCA] [32], [BzMIM][DCA] [46] [AMIM][DCA] [47], [NC3CNMIM][DCA] [48], [BMPy][DCA] [49], [BMPyr][DCA] [50], [C2OHMIM][DCA] [51], [C2ClMIM][DCA] [51], and [BMIM][DCA] [52]. The list of ILs cations and anions used in comparison of γ 13∞ , S12∞ and k12∞ with their abbreviations and structures is shown in Table 5. Studying the effect of the cation structure on the extractive properties we can observed from Fig. 2 that the best selectivity for heptane (1)/thiophene (2) at temperature T = 328.15 K is for [N-C3OHMMor][DCA] [29], [N-C3CNMIM][DCA] [48] and for [EMMOR][DCA] [30]. The ILs used in this work have selectivity >200, but lower than those observed for ILs mentioned above. In addition, to evaluate the potential of the ILs to be used at industrial scale, a comparison of capacity has to be performed. The best capacities were observed for [BMPYR][DCA] [50] and [BMPy][DCA] [49] but with very low selectivity, lower than < 100. Fig. 3 presents selectivity and capacity of the extraction of pyridine from heptane at temperature T = 328.15 K. The best selectivity is for [N-C3OHMMor][DCA] [29] and for [C2OHMIM][DCA] [51]. The best capacity is observed for [BMPy][DCA] [49] and for [BMIM][DCA] [52], again with the selectivity lower than < 100. Better results for the ILs, measured in this work, were for [N-C3CNPy][DCA] with the selectivity larger than >300. 18
Fig. 4 presents selectivity
and capacity for heptane/1-nitropropane problem at
temperature T = 328.15 K. The results are similar to mentioned above. High selectivity was obtained also for [N-C3CNMIM][DCA] [48]. Table 8 presents the results for all three separation processes, discussed in this work, at temperature T = 328.15 K. Even though the experimental data present large discrepancies among different literature sources, one can conclude that the selectivities for the heptane (1)/thiophene (2) separation, obtained with morpholinium-based ILs is high with the best value for the [N-C3OHMMor][DCA] ( S12∞ = 274; k12∞ = 0.30) [29] and for the [EMMor][DCA] ( S12∞ = 273; k12∞ = 0.42) [30]. The selectivity for [N-C3CNPy][DCA] is larger than that for [NC3CNMPyr][DCA] ( S12∞ = 224; k12∞ = 0.32). The largest values of selectivity for the heptane (1)/pyridine (2) separation are also for [NC3OHMMor][DCA] ( S12∞ = 514; k12∞ = 0.56) [29] and for [C2OHMIM][DCA] ( S12∞ = 485; k12∞ = 0.77) [51]. The selectivity for [N-C3CNPy][DCA] is larger than that for [NC3CNMPyr][DCA] ( S12∞ = 348; k12∞ = 0.50). The largest values of selectivity for the heptane (1)/1-nitropropane (2) separation are for [N-C3CNMIM][DCA] ( S12∞ = 287; k12∞ = 0.44) [48] and for [N-C3OHMMor][DCA] ( S12∞ = 276; k12∞ = 0.30) [29]. The selectivity for [N-C3CNPy][DCA] is larger than that for [NC3CNMPyr][DCA] ( S12∞ = 228; k12∞ = 0.46). Summing up, for all three separation cases, the [DCA]--based ILs used in this work reveal large selectivities and acceptable capacities. This is the result of the interaction of thiophene, pyridine and 1-nitropropane with [DCA]--based ILs. It is widely known that alkanes
are not soluble in the ILs. The introduction of a OH or CN group in the
morpholinium, or imidazolium, or pyridinium or pyrrolidinium cation slightly increases selectivity and the capacity, especially for morpholinium-based ILs.
19
6. Results of the Abraham Solvation Parameter Model
The linear solvation energy relationship (LFER) system constants as a function of temperature for the [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA] ILs, investigated in this work, are presented in Tables 9 and 10. The solute descriptors are listed in Table 6S in the SM. The analysis of the selectivity of solvents and ILs towards pairs of gaseous compounds in terms of the log KL values was shown by Abraham and Acree [43]. The results of calculations are presented in Figs. 5 and 6. Table 5S in the SM presents cations of the discussed ILs. This work is the continuation of the presentation of the Abraham solvation parameter model for new, synthesized by us ILs. In our earlier work, the description was presented for 1-ethyl-3methylimidazolium tricyanomethanide [53], 1-ethyl-3-methylimidazolium tetracyanoborate [39],
1-butyl-4-methylpyridinium
tricyanomethanide,
1-butyl-3-methylimidazolium
tricyanomethanide [54], 1-butyl-1-methylpyrrolidynium tetracyanoborate [55], for 1-butyl-1methylpiperidynium bis{(trifluoromethyl)sulfonyl}imide in comparison with 1-butyl-1methylpiperidynium thiocyanate [56], for [DoMIM][NTf2] [57], and for [N-C3OHPY][DCA] [31].
7. Conclusions In this work, we have studied the potential use of (3-cyanopropyl)pyridinium dicyanamide, [N-C3CNPy][DCA] and (3-cyanopropyl)methylpyrrolidinium dicyanamide, [NC3CNMPyr][DCA] in three processes of separation, viz. heptane/thiophene, heptane/pyridine
and heptane/1-nitropropane as a model compounds for the desulfurization and denitrogenation of fuels. The data of the activity coefficients at infinite dilution were obtained using the gasliquid chromatography technique for 60 solutes in both ILs at six temperatures ranging between (318.15 and 368.15) K. In addition, densities of both ILs were measured as a 20
function of temperature. The interactions of various types of organic solutes and water with two ionic liquids at infinite dilution were discussed and shown with regard to the activity coefficients at infinite dilution, the gas liquid-partition coefficients and the thermodynamic functions at infinite dilution. Using the reported experimental data, along with other data from literature, the impact of the ILs cation in the three chosen separation problems was analyzed. The reported results show high values of selectivity for both ILs used with larger effects for [N-C3CNPy][DCA]. The presence of the CN group in the cation increased the selectivity in
both ILs in comparison with the simple pyridinium-based and pyrrolidinium-based cations of the ILs.
Supplementary Material: The sources and mass fraction purities of materials. Mean column pressure, p , inlet column pressure, pi, outlet column pressure, po and standard state of solutes at given temperatures, at standard state. Densities of ILs as a function of temperature. Plots of ln(γ13∞) versus 1/T for the organic solutes in ILs. The list of ILs cations and anions used in comparison of γ 13∞ , S12∞ and k12∞ with their abbreviations and structures. Solute descriptors for equation of the Abraham Solvation Model. Supplementary data associated with this article can be found, in the online version, at http:/dx.doi.org/ Acknowledgements This work has been supported by the National Science Center (NCN) in Poland in the years 2017–2020 (UMO-2016/23/B/ST5/00145). CRediT author statement Urszula Domańska: Conceptualization, Methodology, Supervision, Writing- Reviewing and Editing, Funding acquisition. Michal Wlazło: Metodology, Data curation, Visualization, Investigation. Monika Karpińska: Metodology, Formal analysis, Investigation, Validation.
21
Conflict of interest The authors have no conflict of interest. Appendix A. Supplementary data Supplementary data to this article can be found online at https://
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28
Table 1 The name, abbreviation, structure, supplier, molar mass, mass fraction purity, water content and purification method of investigated ionic liquids. Structure
+
N
CN
M/(g mol-1)
(3-cyanopropyl)pyridinium dicyanamide, [N-C3CNPy][DCA]
213.24
495x 10-6
Purification method/meth od of analysis Low pressure 24 h 320 K (Analysis: 1 HNMR, 13 CNMR, ChA)
N N+
CN
N-
(3cyanopropyl)methylpyrrolidi nium dicyanamide, [N-C3CNMPyr][DCA] Synthesis [33]
N
Mass fraction purity /water content (mass fraction) >0.95/
Synthesis [33]
NN
Name, abbreviation, supplier,
N
29
219.29
>0.97/ 495x 10-6
Low pressure 24 h 320 K (Analysis: 1 HNMR, 13 CNMR, ChA)
Table 2 Density, ρ as a function of temperature, T for investigated ILs [N-C3CNPy][DCA] and [Na C3CNMPyr][DCA] at pressure p = 101 kPa.
[N-C3CNPy][DCA]
[N-C3CNMPyr][DCA]
T/K ρ/g cm–3
a
b
ρ/g cm–3
298.15b
1.16664b
1.09640
303.15
1.16348
1.09353
308.15
1.16033
1.09067
313.15
1.15720
1.08784
318.15
1.15411
1.08502
323.15
1.15103
1.08222
328.15
1.14798
1.07945
333.15
1.14495
1.07668
338.15
1.14195
1.07394
343.15
1.13896
1.07120
348.15
1.13598
1.06847
353.15
1.13301
1.06575
358.15
1.13006
1.06305
363.15
1.12712
1.06036
368.15
1.12419
1.05768
Standard uncertainties u are u (T) = ± 0.1 K u (ρ) = ± 1.1· 10−3 g cm−3, u (p) = ±1 kPa.
ρ/g cm–3 = 1.168 at 293.15 K in Ref. [34].
30
Table 3 The experimental activity coefficients at infinite dilution γ 13∞ for the solutes in ionic liquid [NC3CNPy][DCA] at different temperatures for the hypothetical liquid at zero pressure. a T/K Solute 318.15
328.15
338.15
348.15
358.15
Heptane
777
702
638
Octane
1071
997
Nonane
1480
Decane
930
869
818
1390
1315
1244
1182
1130
1943
1839
1745
1655
1578
1512
Cyclohexane
193
176
161
148
137
127
Methylcyclohexane
308
289
271
255
242
230
Cycloheptane
235
221
208
197
187
178
Cyclooctane
326
303
285
267
253
239
Cyclohexene
55.8
53.9
52.3
368.15
50.6
Hept-1-ene
322
312
301
292
284
Oct-1-ene
521
495
472
450
432
415
Dec-1-ene
1166
1077
1002
934
880
828
Pent-1-yne
18.8
19.6
20.3
21.0
21.7
22.4
Hex-1-yne
32.5
33.8
35.0
36.2
37.4
38.5
Hept-1-yne
59.4
60.9
62.4
63.6
65.0
66.2
Oct-1-yne Benzene
112 6.14
113
114
6.20
6.26
115 6.31
116 6.37
117 6.44
Toluene
10.1
10.3
10.6
10.8
11.0
11.3
Ethylbenzene
21.2
21.1
21.0
20.9
20.9
20.8
o-Xylene
14.0
14.2
14.3
14.5
14.6
14.7
m-Xylene
18.6
18.8
18.9
19.1
19.2
19.4
p-Xylene
17.6
17.7
17.9
17.9
18.0
18.1
Propylbenzene
43.0
42.2
41.5
40.9
40.3
39.7
iso-Propylbenzene
40.3
39.6
39.1
38.6
38.2
37.7
Styrene
8.89
9.04
31
9.17
9.31
9.44
9.58
T/K Solute α-Methylstyrene
318.15
328.15
338.15
348.15
358.15
368.15
14.9
15.4
15.9
16.4
17.0
17.4
Thiophene
3.03
3.14
3.26
3.37
3.47
3.57
Pyridine
1.97
2.02
2.08
2.14
2.18
2.24
Methanol
0.762
0.766
0.769
0.773
0.775
0.779
Ethanol
1.63
1.60
1.57
1.55
1.52
1.50
Propan-1-ol
2.69
2.61
2.55
2.48
2.43
2.38
Propan-2-ol
3.05
2.94
2.85
2.76
2.68
2.61
Butan-1-ol
4.57
4.37
4.20
4.04
3.90
3.77
Butan-2-ol
4.63
4.47
4.31
4.18
4.05
3.94
2-Methyl-1-propanol
4.71
4.45
4.23
4.04
3.86
3.71
tert-Butanol
4.67
4.54
4.43
4.32
4.23
4.14
Pentan-1-ol
7.37
7.05
6.76
6.49
6.26
6.06
Water
0.428
0.434
0.440
0.446
0.452
0.458
Methyl acetate
3.42
3.56
3.68
3.82
3.94
4.07
Methyl propanoate
6.42
6.62
6.81
7.00
7.19
7.36
Methyl butanoate
12.2
12.4
12.6
12.8
13.0
13.1
Ethyl acetate
7.40
7.62
7.82
8.04
8.22
8.42
Vinyl acetate
5.73
5.90
6.05
6.19
6.32
6.48
Tetrahydrofuran
3.85
3.97
4.08
4.17
4.27
4.36
1.4-Dioxane
1.78
1.91
2.04
2.17
2.30
2.43
tert-Butyl methyl ether tert-Butyl ethyl ether
39.0 142
40.1
41.1
139
136
42.2 133
43.2
44.2
131
tert-Amyl methyl ether
68.1
69.5
70.8
72.0
73.2
74.3
Diethyl ether
32.3
33.1
33.9
34.8
35.6
36.3
Di-n-propyl ether
155
150
146
142
Di-iso-propyl ether
169
157
147
138
Di-n-butyl ether
417
405
395
385
138
135
375
368
Acetone
1.99
2.07
2.15
2.23
2.32
2.39
Pentan-2-one
6.65
6.77
6.88
7.00
7.11
7.20
Pentan-3-one
6.68
6.89
7.06
7.23
7.40
7.56
32
T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Butanal
4.52
4.66
4.78
4.90
5.03
5.15
Acetonitrile
1.15
1.20
1.24
1.28
1.32
1.36
1-Nitropropane
3.01
3.08
3.13
3.20
3.26
3.31
a
Standard uncertainties u are u( γ 13∞ ) = 3%, u(T) = 0.02 K.
33
Table 4 The experimental activity coefficients at infinite dilution γ 13∞ for the solutes in ionic liquid [NC3CNMPyr][DCA] at different temperatures for the hypothetical liquid at zero pressure. a T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Heptane
283 464
417
379
346
Octane
704
640
587
541
500
465
Nonane
1031
928
842
767
704
649
Decane
1489
1329
1198
1085
988
906
Hexane
Cyclopentane
81.2
70.3
61.8
96.0
89.3
Cyclohexane
104
Methylcyclohexane
180
168
156
147
138
Cycloheptane
138
128
119
111
104
Cyclooctane
197
184
174
164
156
Hex-1-ene
104
100
Cyclohexene
35.5
34.6
83.6
78.5
96.9
93.7
90.9
33.7
32.9
32.2
74.0 130 98.1 148
31.6
Hept-1-ene
184
172
162
152
144
137
Oct-1-ene
300
281
265
250
237
226
Dec-1-ene
731
695
664
634
609
586
Pent-1-yne
10.0
10.4
10.8
11.2
11.6
12.0
Hex-1-yne
17.2
17.7
18.1
18.6
19.0
19.5
Hept-1-yne
31.2
31.8
32.3
32.7
33.2
33.6
Oct-1-yne
56.2
56.3
56.4
56.5
56.6
56.7
Benzene
3.60
3.73
3.85
3.98
4.10
4.22
Toluene
6.41
6.62
6.83
7.02
7.23
7.42
Ethylbenzene o-Xylene
12.1 9.10
12.3
12.5
9.34
9.58
12.7 9.82
12.8
13.0
10.1
10.3
m-Xylene
11.6
11.9
12.2
12.4
12.7
12.9
p-Xylene
11.2
11.4
11.6
11.8
12.1
12.3
Propylbenzene
23.0
23.1
23.2
23.3
23.4
23.5
34
T/K Solute iso-Propylbenzene
318.15
328.15
338.15
348.15
358.15
368.15
21.4
21.5
21.7
21.9
22.0
22.2
Styrene
5.19
5.41
5.61
5.81
α-Methylstyrene
8.76
9.23
9.69
Thiophene
1.88
1.98
2.08
2.18
2.28
2.38
Pyridine
1.48
1.54
1.60
1.65
1.71
1.77
Methanol
0.571
0.581
0.591
0.599
0.608
0.617
Ethanol
1.12
1.12
1.11
1.11
1.11
1.11
Propan-1-ol
1.70
1.69
1.69
1.68
1.67
1.67
Propan-2-ol
1.87
1.85
1.84
1.82
1.81
1.80
Butan-1-ol
2.8
2.74
2.68
2.64
2.59
2.55
Butan-2-ol
2.71
2.68
2.65
2.62
2.60
2.58
2-Methyl-1-propanol
2.70
2.63
2.57
2.51
2.46
2.41
tert-Butanol
2.60
2.59
2.57
2.56
2.55
2.54
Pentan-1-ol
4.29
4.19
4.11
4.02
3.95
3.88
Water
0.326
0.338
0.349
0.36
0.371
0.382
Methyl acetate
2.604
2.732
2.860
2.983
3.108
3.231
Methyl propanoate
4.50
4.69
4.88
5.06
5.24
5.43
Methyl butanoate
7.98
8.23
8.48
8.72
8.94
9.17
Ethyl acetate
5.263
5.437
5.613
5.784
5.951
6.122
Vinyl acetate
3.87
4.03
4.19
4.35
4.49
4.64
Tetrahydrofuran
2.85
2.96
3.09
3.21
3.33
3.45
1.4-Dioxane
1.42
1.52
1.62
1.73
1.83
1.93
10.1
6.01 10.6
6.22 11.1
tert-Butyl methyl ether
23.5
23.9
24.2
24.6
24.9
25.2
tert-Butyl ethyl ether
80.8
78.7
76.8
75.1
73.5
71.9
tert-Amyl methyl ether
40.7
40.7
40.8
40.9
41.0
41.1
Diethyl ether
21.2
21.2
21.2
21.2
21.2
21.2
Di-n-propyl ether
90.5
86.2
82.3
78.9
75.8
73.0
Di-iso-propyl ether
95.0
91.6
88.4
85.5
83.0
Di-n-butyl ether Acetone
263 1.53
243
225
1.60
35
1.67
210 1.74
196 1.81
184 1.88
T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Pentan-2-one
4.58
4.70
4.83
4.96
5.08
5.20
Pentan-3-one
4.53
4.70
4.86
5.03
5.19
5.35
Butanal
3.17
3.27
3.36
3.46
3.55
3.64
Acetonitrile
0.876
0.91
0.941
0.973
1.00
1.04
1-Nitropropane
2.04
2.12
2.19
2.26
2.33
2.40
a
Standard uncertainties u are u( γ 13∞ ) = 3%. u(T) = 0.02 K
36
Table 5 The experimental gas-liquid partition coefficients KL for the solutes in ionic liquid [NC3CNMPy][DCA] at different temperatures. T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Heptane
1.23
0.927
0.719
Octane
2.54
1.77
1.27
0.938
0.707
Nonane
5.22
3.41
2.29
1.59
1.14
0.83
6.93
4.42
2.93
1.99
1.39
Decane
11.3
Cyclohexane
2.53
1.97
1.57
1.27
1.05
0.879
Methylcyclohexane
3.11
2.30
1.73
1.34
1.06
0.847
Cycloheptane
8.00
5.70
4.16
3.12
2.38
1.86
9.27
6.64
4.87
3.66
Cyclooctane
19.6
13.3
Cyclohexene
9.40
6.88
5.16
3.96
Hept-1-ene
2.45
1.75
1.29
0.969
0.746
Oct-1-ene
4.36
3.00
2.12
1.55
1.15
0.879
9.60
6.36
4.36
3.05
2.19
4.82
3.58
2.71
2.10
1.65
7.66
5.43
3.93
2.92
2.22
7.82
5.51
3.96
2.92
7.40
5.16
3.69
Dec-1-ene Pent-1-yne
14.9 6.68
Hex-1-yne
11.1
Hept-1-yne
17.3
11.4
Oct-1-yne
25.9
16.5
10.9
Benzene
79.7
55.5
39.8
29.2
21.9
16.8
95.1
64.4
44.7
31.9
23.3
78.6
53.9
37.9
27.3
71.2
50.0
65.9
45.7
32.3
68.0
47.4
33.8
Toluene
145
Ethylbenzene
184
119
o-Xylene
388
242
m-Xylene
238
150
p-Xylene
240
153
Propylbenzene
227
142
92.0
61.4
42.1
29.8
iso-Propylbenzene
187
118
76.5
51.4
35.5
25.2
Styrene
647
398
156 98.0 100
254
37
104
167
114
79.3
T/K Solute 318.15
328.15
338.15
348.15
358.15
α-Methylstyrene
850
501
307
194
127
Thiophene
188
127
Pyridine
961
613
403
273
Methanol
432
287
197
138
99.6
73.3
Ethanol
386
251
168
116
82.4
59.9
Propan-1-ol
581
362
234
157
Propan-2-ol
260
167
111
Butan-1-ol
930
557
346
224
Butan-2-ol
383
236
152
102
2-Methyl-1-propanol
586
357
227
150
tert-Butanol
171
109
Pentan-1-ol
1432
824
495
310
202
135
Water
3497
2158
1375
904
611
423
87.5
71.8
62.1
76.5
49.2
45.3 190
108 54.3 150 70.4 102 34.9
368.15 85.0 33.8 136
76.5 39.5 104 50.2 72.2 25.5
Methyl acetate
66.4
45.8
32.6
23.7
17.7
13.5
Methyl propanoate
80.5
53.8
37.1
26.3
19.2
14.3
66.5
44.7
31.0
22.0
16.1
Methyl butanoate
102
Ethyl acetate
64.5
43.3
30.0
21.3
15.6
11.6
Vinyl acetate
70.3
47.6
33.3
23.9
17.6
13.2
Tetrahydrofuran
77.9
54.3
38.8
28.5
21.4
16.4
1.4-Dioxane
626
395
257
172
119
83.8
tert-Butyl methyl ether
5.33
3.81
2.81
2.11
1.62
tert-Butyl ethyl ether
2.67
1.94
1.46
1.11
0.872
tert-Amyl methyl ether
8.92
6.12
4.32
3.13
2.33
1.77
Diethyl ether
3.24
2.40
1.81
1.40
1.10
0.884
Di-n-propyl ether
4.60
3.27
2.39
1.79
1.37
1.08
Di-iso-propyl ether
1.96
1.51
1.19
0.953
8.47
5.58
3.80
2.67
1.91
Di-n-butyl ether
13.3
Acetone
110
Pentan-2-one
175
Pentan-3-one
170
76.6
1.27
54.7
40.0
29.9
22.9
115
78.4
54.7
39.2
28.8
111
75.5
52.5
37.3
27.2
38
T/K Solute Butanal Acetonitrile 1-Nitropropane
318.15
328.15
338.15
348.15
358.15
368.15
92.5
63.5
44.9
32.6
24.2
18.3
463
315
221
158
116
1210
753
486
322
220
39
86.9 155
Table 6 The experimental gas-liquid partition coefficients KL for the solutes in ionic liquid [NC3CNMPyr][DCA] at different emperatures. T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Hexane
1.05
Heptane
1.88
1.43
1.11
0.876
Octane
3.54
2.52
1.84
1.38
1.06
0.826
Nonane
6.85
4.67
3.27
2.36
1.75
1.32
8.77
5.89
4.08
2.91
2.13
Decane
13.5
Cyclopentane
1.90
1.63
1.42
Cyclohexane
4.29
3.30
2.59
2.06
1.67
1.38
Methylcyclohexane
4.86
3.61
2.75
2.14
1.7
1.37
9.00
6.66
5.04
3.90
3.08
9.89
7.23
5.39
Cycloheptane
12.5
Cyclooctane
29.7
Hex-1-ene Cyclohexene
2.43 13.5
20.0
13.9
1.83
1.41
1.11
0.885
9.82
7.32
5.58
4.34
3.43
Hept-1-ene
3.92
2.9
2.19
1.70
1.34
1.08
Oct-1-ene
6.92
4.83
3.46
2.55
1.92
1.48
8.79
5.87
4.03
2.84
6.14
4.65
3.59
2.82
9.58
7.02
5.26
4.01
9.79
7.10
5.27
9.66
6.96
Dec-1-ene
21.7
13.6
Pent-1-yne
11.5
Hex-1-yne
19.3
13.4
Hept-1-yne
30.0
20.1
13.8
Oct-1-yne
46.9
30.2
20.1
13.7
84.4
59.1
42.4
31.2
23.4
91.3
63.1
44.6
32.3
81.5
56.4
40.0
94.5
65.6
8.29
Benzene
124
Toluene
209
136
Ethylbenzene
294
186
121
o-Xylene
545
335
213
m-Xylene
347
217
139
92.8
63.5
44.6
p-Xylene
346
217
141
94.0
64.6
45.6
40
140
T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
Propylbenzene
387
237
150
98.3
66.3
45.9
iso-Propylbenzene
323
198
126
83.0
56.3
39.2
Styrene
1012
608
380
245
163
112
α-Methylstyrene
1320
767
462
288
185
123
277
183
125
Pyridine
1171
737
480
322
222
Methanol
527
346
234
163
116
84.6
Ethanol
512
328
217
148
104
74.2
Propan-1-ol
839
511
323
212
144
Propan-2-ol
387
242
157
106
Butan-1-ol
1389
813
496
315
207
Butan-2-ol
599
361
227
148
101
2-Methyl-1-propanol
934
553
342
220
147
tert-Butanol
281
174
113
Pentan-1-ol
2246
1265
746
458
292
193
Water
4196
2533
1584
1024
680
464
Thiophene
Methyl acetate
79.7
87.7
76.0
63.1
73.3
52.9
46.4 157
100 52.4 140 70.2 102 38.0
54.5
38.4
27.7
20.5
15.5
Methyl propanoate
105
69.4
47.4
33.3
24.0
17.7
Methyl butanoate
143
91.5
60.7
41.5
29.2
21.0
Ethyl acetate
82.9
55.4
38.2
27.1
19.7
14.7
Vinyl acetate
95.0
63.6
44.0
31.2
22.7
16.9
Tetrahydrofuran
96.4
66.4
46.9
33.9
25.1
19.0
1.4-Dioxane
718
453
295
198
136
96.2
tert-Butyl methyl ether
8.07
5.85
4.35
3.31
2.58
2.05
tert-Butyl ethyl ether
4.29
3.14
2.36
1.81
1.42
1.14
9.54
6.85
5.04
3.80
2.92
tert-Amyl methyl ether
13.7
Diethyl ether
4.51
3.42
2.66
2.10
1.70
1.39
Di-n-propyl ether
7.19
5.21
3.88
2.95
2.29
1.81
Di-iso-propyl ether
3.18
2.37
1.81
1.41
1.12
8.96
6.38
4.67
Di-n-butyl ether
19.2
12.9
41
3.49
T/K Solute 318.15
328.15
338.15
348.15
358.15
368.15
90.7
64.5
47.0
35.0
26.6
Acetone
131
Pentan-2-one
233
152
102
70.6
50.2
36.5
Pentan-3-one
230
150
100
68.9
48.7
35.1
Butanal
121
42.3
31.3
23.8
Acetonitrile
556
379
265
190
140
104
1634
1001
636
417
282
195
1-Nitropropane
82.7
58.3
42
Table 7 Limiting partial molar excess Gibbs energies ∆G1E , ∞ , enthalpies ∆H1E , ∞ and entropies Tref ∆S1E , ∞ for the solutes in ionic liquids [N-C3CNPy][DCA] and [N-C3CNMPyr][DCA] at the
reference temperature Tref = 328.15 K. [N-C3CNPy][DCA] Solute
Heptane Octane Nonane Decane Cyclopentane Cyclohexane Methylcyclohexane Cycloheptane Cyclooctane Hex-1-ene Cyclohexene Hept-1-ene Oct-1-ene Dec-1-ene Pent-1-yne Hex-1-yne Hept-1-yne Oct-1-yne Benzene Toluene Ethylbenzene o-Xylene m-Xylene p-Xylene Propylbenzene iso-Propylbenzene Styrene α-Methylstyrene Thiophene Pyridine Methanol Ethanol Propan-1-ol Propan-2-ol Butan-1-ol Butan-2-ol 2-Methyl-1-propanol tert-Butanol Pentan-1-ol Water
[N-C3CNMPyr][DCA]
∆G1E , ∞ / kJ
∆H1E , ∞ / kJ
Tref ∆S1E , ∞ /kJ
∆G1E , ∞ / kJ
∆H1E , ∞ / kJ
Tref ∆S1E , ∞ /
mol–1
mol–1
mol–1
mol–1
mol–1
kJ mol–1
17.9 18.8 19.8 20.5 14.1 15.5 14.7 15.6 14.1
8.8 6.4 5.3 4.9 8.1 5.7 5.5 6.0 8.1
-9.05 -12.42 -14.47 -15.59 -5.98 -9.76 -9.25 -9.54 -5.98
10.9 15.7 16.9 19.1 8.12 9.61 11.2 12.9 4.98 6.36 8.32 7.24 8.00 7.84 10.2 10.0 6.01 7.46 3.12 1.92 -0.73 1.28 2.62 2.94 4.02 4.09 4.07 4.13 5.33 -2.28
3.0 3.0 4.4 6.7 -3.4 -3.3 -2.1 -0.9 -0.9 -2.2 0.4 -1.0 -0.9 -0.5 1.6 1.3 -1.4 -3.0 -3.2 -2.5 -0.4 1.6 2.4 3.1 3.7 3.2 4.6 2.3 3.8 -1.3
-7.90 -12.7 -12.5 -12.4 -11.5 -12.9 -13.3 -13.8 -5.90 -8.56 -7.96 -8.25 -8.87 -8.30 -8.66 -8.76 -7.45 -10.5 -6.33 -4.40 0.31 0.27 -0.26 0.12 -0.30 -0.91 0.58 -1.82 -1.50 0.97
16.5 17.6 18.6 19.6 11.6 12.5 14.0 13.2 14.2 12.6 9.67 14.0 15.4 17.9 6.39 7.84 9.44 11.0 3.59 5.16 6.85 6.10 6.76 6.64 8.57 8.37 4.61 6.06 1.86 1.18 -1.48 0.31 1.43 1.68 2.75 2.69 2.64 2.60 3.91 -2.96
9.05 8.08 9.00 9.67 12.2 6.56 6.39 6.67 5.55 3.24 2.30 5.76 5.48 4.32 -3.42 -2.40 -1.41 -0.17 -3.08 -2.85 -1.39 -2.38 -2.07 -1.74 -0.43 -0.72 -3.49 -4.52 -4.55 -3.76 -1.50 0.24 0.41 0.75 1.78 0.95 2.24 0.48 1.97 -3.06
-7.41 -9.55 -9.64 -9.95 0.60 -5.89 -7.59 -6.57 -8.68 -9.33 -7.37 -8.28 -9.90 -13.5 -9.81 -10.2 -10.9 -11.2 -6.67 -8.01 -8.24 -8.47 -8.83 -8.38 -9.00 -9.09 -8.10 -10.6 -6.41 -4.69 -0.02 -0.07 -1.02 -0.93 -0.97 -1.74 -0.39 -2.12 -1.94 -0.10
43
[N-C3CNPy][DCA] Solute
Methyl acetate Methyl propanoate Methyl butanoate Ethyl acetate Vinyl acetate Tetrahydrofuran 1.4-Dioxane tert-Butyl methyl ether tert-Butyl ethyl ether tert-Amyl methyl ether Diethyl ether Di-n-propyl ether Di-iso-propyl ether Di-n-butyl ether Acetone Pentan-2-one Pentan-3-one Butanal Acetonitrile 1-Nitropropane
[N-C3CNMPyr][DCA]
∆G1E , ∞ / kJ
∆H1E , ∞ / kJ
Tref ∆S1E , ∞ /kJ
∆G1E , ∞ / kJ
∆H1E , ∞ / kJ
Tref ∆S1E , ∞ /
mol–1
mol–1
mol–1
mol–1
mol–1
kJ mol–1
3.46 5.16 6.87 5.54 4.84 3.76 1.77 10.1 13.5 11.6 9.55 13.7 13.8 16.4 1.99 5.22 5.27 4.20 0.50 3.07
-3.4 -2.7 -1.5 -2.5 -2.4 -2.4 -6.0 -2.4 1.9 -1.7 -2.3 2.7 6.1 2.5 -3.6 -1.6 -2.4 -2.5 -3.2 -1.9
-6.86 -7.81 -8.34 -8.06 -7.22 -6.18 -7.76 -12.5 -11.5 -13.3 -11.9 -11.0 -7.74 -13.9 -5.55 -6.78 -7.64 -6.73 -3.72 -4.93
2.74 4.22 5.75 4.62 3.80 2.96 1.14 8.66 11.9 10.1 8.33 12.2 12.3 15.0 1.28 4.22 4.22 3.23 -0.26 2.05
-4.19 -3.63 -2.71 -2.94 -3.52 -3.76 -5.98 -1.33 2.27 -0.22 0.00 4.16 3.22 6.99 -4.00 -2.48 -3.24 -2.69 -3.24 -3.20
-6.94 -7.85 -8.46 -7.56 -7.10 -6.72 -7.12 -9.99 -10.3 -8.33 -8.00 -9.11 -8.00 -7.12 -5.28 -6.70 -7.46 -5.92 -2.98 -5.25
44
Table 8 Selectivities, S12∞ and capacities, k 2∞ for heptane/thiophene, heptane/pyridine and heptane/1nitropropane separation problems for selected ionic liquids at T = 328.15 K. S12∞
k 2∞
Ionic liquid abbreviation heptane / thiophene
heptane / pyridine
heptane / 1-nitropropane
thiophene
pyridine
1-nitropro
Ref.
pane
[N-C3CNPy][DCA]
224
348
228
0.32
0.50
0.46
this work
[N-C3CNMPyr][DCA]
211
271
197
0.51
0.65
0.47
this work
[N-C3OHPy][DCA]
163
298
143
0.37
0.68
0.32
[31]
[N-C3CNMIM][DCA]
268
421
287
0.41
0.65
0.44
[48]
62.2
1.15
1.43
0.87
[49]
[BMPy][DCA]
80.5
100
[BMPyr][DCA] [N-C3OHMMor][DCA]
80.4
‒
‒
1.13
‒
‒
[50]
274
514
276
0.30
0.56
0.30
[29]
[N-C3OHMIM][DCA]
156
285
144
0.39
0.71
0.36
[29]
[C2OHMIM[DCA]
233
485
227
0.37
0.77
0.36
[51]
[C2ClMIM][DCA] [EMMor][DCA]
246
390
251
0.34
0.53
0.34
[51]
273
356
270
0.42
0.55
0.42
[30]
[EMIM][DCA]
109
277
113
0.64
1.63
0.66
[32]
[AMIM][DCA]
122
182
123
0.56
0.83
0.56
[47]
66.6
0.82
1.12
0.76
[52]
91.1
0.69
0.97
0.63
[46]
[BMIM][DCA] [BzMIM][DCA]
71.5 100
98.0 140
45
Table 9 LFER system constants as a function of temperature for ionic liquid [N-C3CNPy][DCA]. System constantsa
Statisticsb
T/K
l
b
a
s
e
c
r2
SD
F
df
318.15
0.443 (0.027) 0.405 (0.026) 0.369 (0.025) 0.337 (0.025) 0.310 (0.025) 0.280 (0.025)
0.345 (0.101) 0.322 (0.097) 0.301 (0.094) 0.285 (0.095) 0.307 (0.096) 0.346 (0.101)
4.16 (0.12) 3.98 (0.12) 3.8 (0.11) 3.65 (0.11) 3.49 (0.11) 3.33 (0.11)
2.98 (0.10) 2.89 (0.09) 2.81 (0.09) 2.73 (0.09) 2.65 (0.09) 2.54 (0.09)
0.546 (0.096) 0.567 (0.092) 0.583 (0.089) 0.601 (0.088) 0.610 (0.088) 0.640 (0.088)
-1.27 (0.10) -1.29 (0.10) -1.30 (0.09) -1.31 (0.10) -1.34 (0.10) -1.34 (0.10)
0.987
0.111
762
52
0.987
0.107
781
52
0.987
0.104
794
52
0.986
0.102
730
51
328.15 338.15 348.15 358.15 368.15 a
0.986 0.984
0.100 0.100
685
49
565
Values in parentheses are standard uncertainties of the parameters.
b
r2, the coefficient of determination; SD, the standard error; F, the F statistic; df, the degrees of freedom.
46
46
Table 10 LFER system constants as a function of temperature for ionic liquid [N-C3CNMPyr][DCA]. System constantsa
Statisticsb
T/K
l
b
a
s
e
c
r2
SD
F
df
318.15
0.456 (0.022) 0.415 (0.021) 0.379 (0.02) 0.341 (0.02) 0.313 (0.019) 0.251 (0.024)
0.407 (0.086) 0.363 (0.082) 0.332 (0.077) 0.298 (0.074) 0.278 (0.074) 0.486 (0.118)
4.19 (0.10) 3.98 (0.1) 3.79 (0.09) 3.60 (0.09) 3.44 (0.09) 3.22 (0.09)
2.85 (0.08) 2.75 (0.08) 2.65 (0.07) 2.56 (0.07) 2.48 (0.07) 2.43 (0.08)
0.639 (0.083) 0.639 (0.078) 0.643 (0.073) 0.652 (0.071) 0.65 (0.07) 0.804 (0.088)
-1.143 (0.078) -1.133 (0.076) -1.131 (0.071) -1.114 (0.072) -1.121 (0.072) -1.178 (0.109)
0.990
0.098
1135
55
0.991
0.092
1126
54
0.991
0.086
1190
54
0.991
0.083
1166
53
0.991
0.081
1086
52
0.987
0.075
531
35
328.15 338.15 348.15 358.15 368.15 a
Values in parentheses are standard uncertainties of the parameters.
b
r2, the coefficient of determination; SD, the standard error; F, the F statistic; df, the degrees of freedom.
47
Figure Captions
Fig. 1. Comparison of γ 13∞ at T = 328.15 K for selected solutes in ionic liquids: (○) [NC3CNPy][DCA]; (□) [N-C3CNMPyr][DCA]; (∆) [N-C3OHPY][DCA] [31]; (◊) [NC3CNMIM][DCA] [48]; (×) [BMPy][DCA] [49]; (+) [BMPyr][DCA] [50]. Fig. 2. Selectivity versus capacity in extraction of heptane/thiophene problem at T = 328.15 K for [DCA]‒ ionic liquids: (●) [N-C3CNPy][DCA]; (■) [N-C3CNMPyr][DCA]; ( ) [NC3OHPy][DCA] [31]; (◊) [N-C3CNMIM][DCA] [48]; (□) [BMPy][DCA] [49]; (×) [BMPyr][DCA] [50]; (○) [N-C3OHMMor][DCA] [29]; (∆) [N-C3OHMIM][DCA] [29]; (▲) [C2OHMIM][DCA] [51]; (♦) [C2ClMIM][DCA] [51]; (‒) [EMMor][DCA] [30]; (+) [EMIM][DCA] [32]; (-) [AMIM][DCA] [47]; ( ) [BMIM][DCA] [52]; (×) [BzMIM][DCA] [46]. Fig. 3. Selectivity versus capacity in extraction of heptane/pyridine problem at T = 328.15 K for [DCA]‒ ionic liquids: (●) [N-C3CNPy][DCA]; (■) [N-C3CNMPyr][DCA]; ( ) [NC3OHPy][DCA] [31]; (◊) [N-C3CNMIM][DCA] [48]; (□) [BMPy][DCA] [49]; (○) [NC3OHMMor][DCA] [29]; (∆) [N-C3OHMIM][DCA] [29]; (▲) [C2OHMIM][DCA] [51]; (♦) [C2ClMIM][DCA]
[51];
(‒)
[EMMor][DCA]
[30];
(+)
[EMIM][DCA]
[32];
(-)
[AMIM][DCA] [47]; ( ) [BMIM][DCA] [52]; (×) [BzMIM][DCA] [46]. Fig. 4. Selectivity versus capacity in extraction of heptane/1-nitropropane problem at T = 328.15 K for [DCA]‒ ionic liquids: (●) [N-C3CNPy][DCA]; (■) [N-C3CNMPyr][DCA]; ( ) [N-C3OHPy][DCA] [31]; (◊) [N-C3CNMIM][DCA] [48]; (□) [BMPy][DCA] [49]; (○) [N-C3OHMMor][DCA] [29]; (∆) [N-C3OHMIM][DCA] [29]; (▲) [C2OHMIM][DCA] [51]; (♦) [C2ClMIM][DCA] [51]; (‒) [EMMor][DCA] [30]; (+) [EMIM][DCA] [32]; (-) [AMIM][DCA] [47]; ( ) [BMIM][DCA] [52]; (×) [BzMIM][DCA] [46].
48
Fig. 5. Calculated versus experimental logarithmic gas-liquid partition coefficients for 57 solutes in [N-C3CNPy][DCA] at T = 328.15 K using the LFER Solvation Model. Fig. 6. Calculated versus experimental logarithmic gas-liquid partition coefficients for 57 solutes in [N-C3CNMPyr][DCA] at T = 328.15 K using the LFER Solvation Model.
49
Fig. 1.
50
Fig. 2.
51
Fig. 3.
52
Fig. 4.
53
Fig. 5.
54
Fig. 6.
55
Author Contribution Statement CRediT author statement Urszula Domańska: Conceptualization, Methodology, Supervision,Writing- Reviewing and Editing, Funding acquisition. Michal Wlazło: Metodology, Data curation, Visualization, Investigation. Monika Karpińska: Metodology, Formal analysis, Investigation, Validation.
Declaration of interests x☐ The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper. ☐The authors declare the following financial interests/personal relationships which may be considered as potential competing interests: