Document Type: Research Paper
Authors
^{1} Faculty of Petroleum, Gas and Petrochemical Engineering, Persian Gulf University, Bushehr, Iran
^{2} Parsian Gas Refining Company, Mohr, Fars, Iran
Abstract
Keywords
1. Introduction
Ionic liquids (ILs) are organic salts that are liquids at room temperature, including at least one large and asymmetric organic cation or anion. ILs have unique properties such as negligible vapor pressure, good thermal stability, and capability to remain liquid over 300 K. Because of these advantages ILs have many different applications and in comparison to other solvents ILs can be used for capturing greenhouse gases such as CO_{2} [1].
In order to use ILs for capturing CO_{2}, thermodynamic models must be available to calculate the solubility of CO_{2} in ILs. Different authors model the solubility of gases in ILs with equation of states (EOS) at different thermodynamic conditions; however, some EOS, such as the classical cubic EOS because of its simplicity, they do not take into account the effect of polarity and hydrogen bonding of ILs in an explicit manner [2]. In addition, these kinds [3] of model have some limitations: the critical parameters needed are not available for ILs, most of ILs tend to degrade before reaching the critical point [3]
Recently, statistical associating fluid theory (SAFT) EOS [4, 5] have also been used for modeling of CO_{2} solubility in ILs [6, 7]. In the 1990s, studies led to different versions of the equation with different acronyms such as tPCPSAFT [6, 8, 9], SAFTVR [10], heteroSAFT [11], PCPSAFT [12], softSAFT [7, 13, 14] and, later, PCSAFT [15]. Kroon, et al. [8] used the tPCPSAFT equation of state to study the phase behaviour of ionic liquid + CO2 systems. Llovell, et al. [16] used the softSAFT equation to estimate the thermodynamic properties of pure ILs and mixtures containing ILs. Also, Andreu and Vega [7, 13] checked the ability of the softSAFT EOS to describe the solubility of CO_{2} in ionic liquids. Paduszynski, et al. [12] used PCPSAFT EOS for modelling systems with ionic liquids.
In this work, the simplified perturbed chain statistical associating fluid theory (sPCSAFT) was used to model systems containing ILs. EOS parameters for ILs were estimated by fitting available experimental liquid density data over a wide range of temperatures and atmospheric pressures. Furthermore, the model was utilized and extended for modeling phase behavior of imidazolium based ILs + CO_{2} systems.
2. Model Description
2.1. PCSAFT Modeling
After Chapman, et al. [4] who introduced the SAFT EOS based on Wertheim’s first order thermodynamic perturbation theory [17], in 2001 the PCSAFT EOS was developed by Gross and Sadowski [15, 16, 18]
PCSAFT model has received a lot of attention because this model can predict and correlate different thermodynamic properties of a great variety of simple and complex molecular systems [19]. They derived a dispersion expression for chain molecules and used a hardchain reference fluid. Then, Von Solms, et al. [20] simplified this equation of state (sPCSAFT) by introducing average diameter of segments in the mixture and simplifying the radial distribution function of mixture. They replaced the radial distribution function of mixture by radial distribution function of the pure component.
The sPCSAFT equation is usually written in terms of the residual Helmholtz free energy. The equation is given by:
(1) 
where a^{res} is the dimensionless residual Helmholtz free energy of the system. The superscripts hc, disp, and assoc refer to a reference hardchain contribution, a dispersion contribution, and an associating contribution, respectively.
The hard chain contribution to the Helmholtz free energy is defined by Gross and Sadowski [15, 18] as
(2) 
The Helmholtz free energy of the hardsphere fluid and the radial distribution function of the hardsphere fluid are defined as:
(3) 

(4) 
Equations (3) and (4) obtained by the assumption of Von Solms, et al. [20] that all of the segments in the mixture have the same diameter.
In equations (3) and (4) represents a reduced segment density
(5) 
and is the mean segment number
(6) 
a^{disp}^{ }is based on expanding the secondorder perturbation theory of Barker and Henderson [21] to chain molecules.
The perturbation contribution is the sum of the firstand secondorder term, according to
(7) 
In these equations, the integrals of the perturbation theory are substituted by simple power series in density of sixth order
(8) 

(9) 
Where the coefficients of the power series in density a_{i} and b_{i} depend on the chain length according to:
(10) 

(11) 
The universal model constants for the above equations are given in literature [15]
Conventional combining rules for ε_{ij} and σ_{ij} were employed
(12) 

(13) 
Where k_{ij} is the binary interaction parameter
The Helmholtz free energy due to association is defined by Huang and Radosz as [5, 22]:
(14) 
Where is the number of association sites per molecule, and is the mole fraction of molecules i not bonded at site A. The parameter is calculated from
(15) 
The association strength is given by
(16) 
where is the effective association volume and is the association energy.
3. Results and Analysis
3.1. Pure Components.
In this work in the sPCSAFT framework, ILs were considered as neutral ion paires, and they were considered as molecule.[7,8,13]. To describe specific interaction because of the charge and asymmetry of ILs molecules, an association site was considered on the ILs Molecule.
The sPCPSAFT EOS has three parameters for nonassociating compounds i.e., the segment number (m_{i}), the segment hardsphere diameter (σ_{i}) and dispersion energy parameter (ε/k_{B}), and two additional parameters for association compounds i.e., the association energy (), and the association volume ().
Tow imidazolium based ILs ie. 1ethyl3methylimidazolium tetrafluoroborate [C_{2}mim][BF_{4}] and 1buthyl3methylimidazolium tetrafluoroborate [C_{4}mim][BF_{4}] were used in this work. Figure 1 demonstrates chemical structures of the investigated ILs.
Figure 1. Chemical structure of the 1ethyl3methylimidazolium tetrafluoroborate and 1butyl3methylimidazolium tetrafluoroborate 
In the first step, the ILs were considered as nonassociating compounds. Three parameters m, σ, and ε/k_{B} were obtained by fitting liquid density data of ILs at atmospheric pressure. Table 1. shows the obtained parameters for the ILs studied in this work and percent average absolute relative error (AARE %) are provided. Good agreement with the experimental density data is observed.
In the second step, the ILs were considered as selfassociation compounds. To reduce the number of parameters that are fitted to experimental density data at atmospheric pressure, the values of association parameters were kept constant. They were teken from reference [] and only three nonassociating parameters of pure imidazolium based ionic liquids were estimated. [C_{2}mim][BF_{4}] and [C_{4}mim][BF_{4}] were modelled using different association scheme according to terminology of Huang and Radosz [5, 22].
Table 2 shows the molecular parameters and AARE % in the density at atmospheric pressure. However, as the number of association site increases, more accuracy is shown. So, the best model with the minimum error is 10C (5 electron donor sites and 5 electron acceptor sites on ILs) and the ARRE% is 0.308% for 1ethyl3methylimidazolium tetrafluoroborate ([C_{2}mim][BF_{4}]) and 0.311% for 1butyl3methylimidazolium tetrafluoroborate ([C_{4}mim][BF_{4}]).
The resulting density− temperature diagrams at atmospheric pressure are shown in Figures 2a and 2b for the [C_{2}mim][BF_{4}] and [C_{4}mim][BF_{4}]. In Figure 2a ILs were considered as nonassociating compound and in Figure 2b ILs were modelled using the 10C association scheme.
(17) 
Table 1. Optimized sPCSAFT Parameters of Pure ILs Considered As NonAssociating Compounds and AARE% in density of ILs at atmospheric pressure
Systems 
Mw (g.mol^{1}) 
σ (A°) 
ε/k_{B} (K) 
m 
AARE % in ρ^{liquid} 
[C_{2}mim][BF_{4}] 
197.97 
3.53 
492.81 
5.84 
0.268 
[C_{4}mim][BF_{4}] 
226.03 
3.71 
498.71 
5.951 
0.274 
Table 2. Optimized sPCSAFT Parameters of Pure ILs Considered As SelfAssociating Molecules and AARE% in density of ILs at atmospheric pressure
Systems 
scheme 
Mw (g.mol^{1}) 
σ (A°) 
ε/k_{B} (K) 
m 
K_{AB} 
ε_{AB}/k_{B} (K) 
AARE % in ρ^{liquid} 

1A 
197.97 
2.9 
292.59 
9.55 
0.00225 
3450 
0.394 

2A 
197.97 
2.91 
292.93 
9.54 
0.00225 
3450 
0.347 

3A 
197.97 
2.92 
292.25 
9.52 
0.00225 
3450 
0.298 

4A 
197.97 
2.92 
292.91 
9.61 
0.00225 
3450 
0.252 
[C_{2}mim][BF_{4}] 
2B 
197.97 
2.9 
292.67 
9.63 
0.00225 
3450 
0.378 

3B 
197.97 
2.91 
292.3 
9.55 
0.00225 
3450 
0.302 

4B 
197.97 
2.91 
292.91 
9.53 
0.00225 
3450 
0.304 

4C 
197.97 
2.92 
292.91 
9.6 
0.00225 
3450 
0.294 

10C 
197.97 
2.93 
292.52 
9.59 
0.00225 
3450 
0.207 










1A 
226.03 
3.03 
294.56 
9.89 
0.00225 
3450 
0.433 

2A 
226.03 
3.05 
293.53 
9.77 
0.00225 
3450 
0.392 

3A 
226.03 
3.06 
294.89 
9.77 
0.00225 
3450 
0.345 

4A 
226.03 
3.07 
294.91 
9.76 
0.00225 
3450 
0.309 
[C_{4}mim][BF_{4}] 
2B 
226.03 
3.05 
294.47 
9.77 
0.00225 
3450 
0.419 

3B 
226.03 
3.05 
294.91 
9.8 
0.00225 
3450 
0.351 

4B 
226.03 
3.05 
294.86 
9.77 
0.00225 
3450 
0.347 

4C 
226.03 
3.07 
294.25 
9.74 
0.00225 
3450 
0.339 

10C 
226.03 
3.08 
294.55 
9.74 
0.00225 
3450 
0.258 
(a) 
(b) 
Figure 2. densityTemperature diagrams for ILs at atmospheric pressure.(a) ILs considered as nonassociating compounds and (b) ILs considered as selfassociating compounds with 10C association scheme 
After obtaining parameters at atmospheric pressure these parameters were used to predict the density of these two ILs at high pressure. Tables 3 and 4 present the AARE % between experimental and calculated liquid densities of these two ILs at wide range of temperatures and high pressures up to 60 MPa for nonassociation and selfassociating compound with 10C association scheme, respectively. Figures 3a and 3b show density Pressure diagrams for selfassociating and nonassociating compounds at high pressure up to 60 MPa respectively. The results show t good agreement with the experimental data.
Table 3. AARE% in liquid density of pure ILs considered as NonAssociating Compounds at high pressure
Systems 
AARE % in ρ^{liquid } 
T (K) 
P (MPa) 
No of data points 
refrences 
[C_{2}mim][BF_{4}] 
2.803 
283.15323.15 
0.160 
52

[23] 
[C_{4}mim][BF_{4}] 
0.549 
283.15333.15 
0.140 
50 
[24] 






Table 4. AARE% in liquid density of pure ILs considered as SelfAssociating Molecules with 10C association scheme at high pressure
Systems 
AARE % in ρ^{liquid} 
T (K) 
P (MPa) 
No of data points 
refrences 
[C_{2}mim][BF_{4}] 
2.902 
283.15323.15 
0.160 
52

[23] 
[C_{4}mim][BF_{4}] 
0.439 
283.15333.15 
0.140 
50 
[24] 








(a) 
(b) 
Figure 3. density Pressure diagrams for [C_{4}mim][BF_{4}] at different temperature and high pressure.(a) considered as nonassociating compounds, (b) considered as selfassociating compounds with 10C association scheme 
After tuning paratemrs of sPCSAFT EOS for ILs, these parameters were tested against prediction/correlation of solubility of CO_{2} in these two ILs. CO_{2} was considered as a nonassociating molecule. Parameters for CO_{2} were adapted from the literature [15]
We first studied the mixture {[C_{2}mim][BF_{4}]+CO_{2}} at pressures up to 5 MPa and at three different temperatures :T= 323.15343.15 K. Figure 4 shows the solubility isotherms obtained for these mixtures as compared to experimental data [25]. It is obvious to see the accuracy of these calculations at low pressures as compared to the experimental data. Within the same family, we studied {[C_{4}mim][BF_{4}]+CO_{2}} at five different temperatures between 323.15368.15. As shown in Figure 5, good agreement between the experimental data and the calculated values can be observed at low pressure.
A comparison between Tables 5 and 6 shows that when association term is used, the solubility of carbon dioxide in these ILs increases and a higher accuracy is shown. Another comparison between low and high pressure is shown in Tables 57. High accuracy in correlation of solubility of CO_{2} in ILs is shown when association term is used.
The results presented show that the sPCSAFT model can be used to predict with high accuracy the phase diagrams of these ionic liquids with carbon dioxide. However, as shown in Table 7 a small deviation is observed at high pressure when mole fraction of CO_{2} is greater than 0.5.
Table 5. AARE% in bubble point pressures for the different systems as NonAssociating Compounds at low pressures
Systems 
T (K) 
P(MPa) 
No. of data points 
AARE in P % 
[C_{2}mim][BF_{4}] +CO_{2} 
323.2343.2 
050 
15 
9.657 
[C_{4}mim][BF_{4}] + CO_{2} 
323.15368.15 
016 
44 
12.493 
Table 6. AARE% in bubble point pressures for the different systems as SelfAssociating Molecules with 10C association scheme at low pressures
Systems 
T (K) 
P(MPa) 
No. of data points 
AARE in P % 
[C_{2}mim][BF_{4}] + CO_{2} 
323.2343.2 
05 
15 
4.607 
[C_{4}mim][BF_{4}] + CO_{2} 
323.15368.15 
015 
44 
2.047 
Table 7. AARE% in bubble point pressures for CO2+ [C_{4}mim][BF_{4}] at high pressures
ILs 
T (K) 
P(MPa) 
No. of data points 
AARE in P % 
Nonassociation 
323.15363.15 
065 
49 
19.608 
Association 
323.15363.15 
065 
49 
4.988 


(a) 
(b) 
Figure 4. Solubility of CO2 in [C_{2}mim][BF_{4}] at different temperatures with a temperaturedependent kij parameter.(a) considered as nonassociating compounds, (b) considered as selfassociating compounds with 10C association scheme 

Figure 5. Solubility of CO_{2} in [C_{4}mim][BF_{4}] as as selfassociating compounds with 10C association scheme at different temperatures with a temperaturedependent kij parameter. 
The values for the binary interaction parameter, k_{ij}, were initially fitted at various temperatures. As shown in Figures 6a and 6b, the binary interaction parameters vary linearly with temperature according to the equation 18. The values of all parameters C_{1} and C_{2} are given in Tables 8 and 9 for nonassociation and association scheme, respectively.
(18) 
Table 8. Binary interaction parameter temperature dependence for nonAssociating Molecules
Systems 
C_{1} 
C_{2} 
[C_{2}mim][BF_{4}] + CO_{2} 
0.0004 
0.1983 
[C_{4}mim][BF_{4}] + CO_{2} 
0.0002 
0.0064 
Table 9. Binary interaction parameter temperature dependence for SelfAssociating Molecules with 10C association scheme
Systems 
C_{1} 
C_{2} 
[C_{2}mim][BF_{4}] + CO_{2} 
0.0005 
0.1968 
[C_{4}mim][BF_{4}] + CO_{2} 
0.0001 
0.1073 


(a) 
(b) 
Figure 6. Dependence on temperature of the binary interaction parameter for different ILs mixed with CO_{2 }.(a) [C_{2}mim][BF_{4}] and (b) [C_{4}mim][BF_{4}] 
Finally, in order to realize the precision of our work compared to others, the results were compared to some models in the literature. Figure 7 shows the density Pressure diagrams for [C_{4}mim][BF_{4}] considered as selfassociating compounds with 10C association scheme at T=323.15 compared to Curras, et al [24]. Our result is more accurate than experimental data obtained in Curras et al. [24] Figure 8 shows CO_{2} solubility in [C_{4}mim][BF_{4}] compared to Ashrafmansouri and Raeissi [30] at T=333.15 . In this case, our result is close to experimental data and slightly better than Ashrafmansouri and Raeissi [30].
Figure 7. density Pressure diagrams for [C_{4}mim][BF_{4}] considered as selfassociating compounds with 10C association scheme at T=323.15 and high pressure compared to Curras, et al. 
Figure 8. CO_{2} solubility in [C4mim][BF4] as selfassociating compounds with 10C association scheme compared to Ashrafmansouri and Raeissi at T=333.15 
4. Conclusion
sPCSAFT EOS was used for 1ethyl3methylimidazolium tetrafluoroborate and 1butyl3methylimidazolium tetrafluoroborate to check the capability of this model to correlate solubility of CO_{2} in these ILs in a wide range of temperatures and pressures. Results were compared to available experimental data. In this model, molecular parameters of pure ILs were estimated from experimental liquid density data over a wide range of temperatures at atmospheric pressure, good agreement with the experimental data is obtained at both atmospheric and high pressure.Then, solubility of carbon dioxide in ILs was studied. The binary interaction parameter is highly temperaturedependent and changes linearly with temperature. Finally, at specific temperatures, the results were compared to other authors and good agreement with better accuracy was observed.
Acknowledment
The authors gratefully acknowledge the National Iranian Gas Company Parsian Gas Refining Company for their financial support of this MSc thesis by finance number 936010, date: 451393.