# Influence of Ionic Liquid Structure on Supported Ionic Liquid Membranes Effectiveness in Carbon Dioxide/Methane Separation

Authors: Iwona Cichowska-Kopczyńska; Monika Joskowska; Bartosz Dębski; Justyna Łuczak; Robert Aranowski
Journal: Journal of Chemistry
 (2013)

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## Abstract

This paper indicates the possibility of application of imidazolium ionic liquids immobilized in polymeric supports—supported ionic liquid membranes—in CO2 separation from gaseous streams (e.g., biogas). Imidazolium salts containing alkyl fluoride anions, bis(trifluoromethylsulfonyl)imide and trifluoromethanesulfonate, selectively separating CO2 were used. The permeability of CO2 through membranes was investigated under gas pressure of 30 kPa and temperature range 283–298 K. Permeability values occurred to be higher for ionic liquids containing bis(trifluoromethylsulfonyl)imide anion. Moreover, CO2 permeability exhibited an increase with increasing temperature for all investigated systems. Stability of supported ionic liquid membranes was studied. In total, polypropylene membrane revealed the best properties, mechanical stability and observed wettability of this support were better than for polyamide and polyvinylidene fluoride ones. Polyethersulfone supports showed similar contact angles; however, its mechanical stability was significantly lower. Obtained results allowed to evaluate the effectiveness of separation process using selected ILs and supports.


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## Body

## 1. Introduction

Increasing ecological awareness and legislative changes over the last decade resulted in the development of innovative technologies for purification of exhaust gas streams and air. Due to relatively easy tuning for specific application, absorption is one of the most commonly applied methods of carbon dioxide separation. Recently, the main direction of research is finding more efficient solvents that are crucial in cost reduction of carbon dioxide capture from gas mixtures. It was demonstrated that ionic liquids (ILs) can be applied as effective solvents for such purposes [1–6]. ILs consist of large, highly asymmetric cation and small organic or inorganic anion. This structure inhibits crystallization and ensures that ILs stay in aliquid state over a wide range of temperatures. Unique properties of ionic liquids are highly desired in a physical and chemical absorption processes. They can be easily adjusted by substituting cations and anions in their structure. Still, ionic liquids present high sorption capacity, thermal stability, and negligible vapour pressure. Application of ILs as absorbents allows avoiding contamination of outlet gas streams by absorbent vapours. This advantage gives ILs huge predominance over traditional volatile organic solvents used in purification of gaseous mixtures [7–11], especially in carbon dioxide removal. An excellent media for this purpose are imidazolium ionic liquids. These compounds selectively absorb CO2 with lower coabsorption of other gases such as C2H4, C2H6, O2, and CH4 [7, 12–15]. Experimental solubility values of gases in [BMIM][Tf2N] (1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide) expressed by Henry’s constants KH [MPa] at 298 K for CO2, C2H4, C2H6, O2, and CH4 are 3.4, 7.0, 9.7, 173.0, and 40.3 respectively [14, 16, 17]. Moreover, gas solubility and diffusivity of the ammonium ionic liquids is of the same magnitude as of the imidazolium ones [18]. Ionic liquids are suitable solvents for upgrading biogas that can be further used in industry. Upgraded biogas can be injected in the gas grid or used as vehicle fuel and eventually for electricity and heat production. Apart from 50 to 75% of methane, biogas contains about 25–45% of carbon dioxide and some amounts of hydrogen sulphide, ammonia, nitrogen, hydrogen, carbon monoxide, and oxygen. Presence of these gases results in a lower energy content of biogas per unit volume when comparing to the natural gas and therefore removal of CO2, that significantly reduces its calorific value and increases corrosion, is required in many applications.However, the high price of ILs and toxicity remain the limitations of their application in industrial scale. Thus, membrane processes allow reducing these issues. Ionic liquids can be embedded in pores of polymer supports where they are kept by capillary forces (supported ionic liquid membrane (SILM)). Therefore, membrane technology enables decrease of solvent consumption, and in consequence, costs of separation processes are lower [19–24]. There are several membrane technologies than can be used in CO2 separation, for example, membrane contactors preventing dispersion of one phase into another [25]. There can be two kinds of contactors: parallel and cross-flow, depending on the flow direction. Cross flow contactors are considered to have some advantages over parallel contactors: higher mass transfer coefficients, lower shell-side pressure drop [26, 27]. Supported liquid membrane systems contain thin barrier of ionic liquid that enables selective permeation of CO2 and H2S if present [28, 29]. SILMs became a good alternative to nonporous polymer membranes due to increased gas diffusion rate [30–32]. However, some authors find polymerizing of room temperature ionic liquids as a solution for low stability of SILMs in high operating pressures [33].Usually, scientific publications present Henry’s constant values as the main parameter determining absorption of CO2 in several types of ILs (imidazolium, ammonium, pyridinium, pyrrolidinium, and phosphonium) [2, 12, 14, 16, 17, 37–40]. However, taking into account the mechanisms of mass transport through the liquid membranes, Henry’s constant is not the only parameter governing the possibility of solvent application in membrane separation processes. In fact, possibility of CO2 capture from gas streams is determined also by the diffusion coefficient that characterises rate of transport of gas molecules through liquid membrane. From a thermodynamic point of view, separation process in liquid membrane can be described best by the diffusion coefficient formula based on solution-diffusion model (SDM) [32, 35] as follows:
(1)Pi=Di·Si,
where  Di is  diffusion coefficient [m2/s], and Si is solubility of gas i in the membrane [mol/m3·Pa], and Pi is permeation through the membrane [mol/s·m·Pa].One has(2)Pi=Ji·l(pi,f-pi,p),
where  Ji is molar diffusion flux of component i through the membrane [mol/m2s], l is thickness of the membrane [m], pi,f is partial pressure of component i in the feed stream [Pa], and pi,p is partial pressure of component i in permeate stream [Pa].Table1 presents exemplary permeation values published in the literature.Table 1
Gas permeation values in 298 K described in literature.
Ionic liquid
Permeation, barrer
Carbon dioxide
[EMIM][TfO]
920 [24]; 1171 [21, 34]
[EMIM][Tf2N]
960; 1702 [21, 34]
[EMIM][BF4]
9699 [21, 34]
[BMIM][PF6]
500 [35]; 544 [34]
[BMIM][Tf2N]
1344 [34]
[BMIM][BF4]
200 [29]
[HMIM][Tf2N]
1136 [21]
Methane
[EMIM][TfO]
63 [34]
[EMIM][Tf2N]
94; 39 [34]
[EMIM][BF4]
44 [34]
[BMIM][PF6]
40 [35]; 41 [34]
[BMIM][BF4]
3 [29]
[HMIM][Tf2N]
134 [34]Differences between permeation values can be a result of differences in operational conditions, for example, pressure, humidity of gas streams, and purity of ionic liquids used in experiments.Literature data suggest that as a result of good solubility of CO2 and low absorption of other gases, selective absorption of CO2 from biogas and exhaust gas streams is possible [41]. Carbon dioxide/methane selectivity for [EMIM][TfO] and [EMIM][Tf2N] reported in the literature is about 18.5 and 12, respectively [21, 34].As pointed out by Zhao et al. the outlook for carbon dioxide capture is to study the low pressure transport in ionic liquids [42]. This research deals with the issue of low pressure separation of carbon dioxide from CO2/CH4 gas mixtures, like for example biogas streams. As indicated previously, high selectivity of separation enables efficient biogas upgrading using ionic liquids.


## 2. Experimental

### 2.1. Materials

Supported ionic liquids membranes were prepared using selected polymeric supports:GH Polypro (polypropylene) (PP), FP Vericel (polyvinylidene fluoride) (PVDF), Nylaflo (polyamide) (PA), and Supor (polyethersulphone) (PES), (Pall, Gelman Laboratory, USA). For permeation experiments PP membrane was selected in order to good wettability and low swelling as indicated in results section. Four ionic liquids were applied as a membrane phase: 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide [EMIM][Tf2N],1-ethyl-3-methylimidazolium trifluoromethanesulfonate [EMIM][TfO],1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide [BMIM][Tf2N],1-butyl-3-methylimidazolium trifluoromethanesulfonate [BMIM][TfO].Imidazolium ionic liquids with [Tf2N] and [TfO] anions were selected, as they exhibit very good carbon dioxide absorption in comparison to [BF4], [PF6] [14, 17, 43]. All chemicals were supplied by IOLITEC, Heilbronn, Germany, with purity above 99%. In order to determine the effect of chemical structure of the ionic liquids on CO2 diffusion, different alkyl chain lengths of the cations and different anions were selected.Physical and chemical properties of polymeric supports and ionic liquids applied in experiments are presented in Tables2 and 3.Table 2
Physicochemical parameters of polymeric supports reported by producer.
Support
Density, kg/m3
Pore diameter, µm
Total porosity, %
Thickness, µm
PP
900
0.2
80
92
PVDF
1790
0.2
80
123
PA
1130
0.2
80
110
PES
1370–1510
0.2
80
148Table 3
Physicochemical properties of ionic liquids used in the experiments at 298 K.
Ionic liquids
Chemical formula
Density, g/cm3*
Viscosity, mPa·s
Surface tension, mN/m
[EMIM][Tf2N]
[C6N2H11]+[(CF3SO2)2N]−
1.52
32.60
32.56
[EMIM][TfO]
[C6N2H11]+[CF3SO3]−
1.39
40.40
37.82
[BMIM][Tf2N]
[C8N2H15]+[(CF3SO2)2N]−
1.43
48.06
30.83
[BMIM][TfO]
[C8N2H15]+[CF3SO3]−
1.29
74.30
34.67
*Data provided by producer.


### 2.2. Methods

#### 2.2.1. Viscosity, Surface Tension, and Contact Angles Measurements

Measurements of dynamic viscosity coefficient of selected ionic liquids were conducted using Brookfield Rheometer LV III. The dependence of shear stress (Pa) on shear rate (1/s) was determined. Ionic liquids viscosity remains constant with increasing shear rates. Such linear relationship between shear stress and shear rate is related to newtonian character of the liquid. Surface tensions of selected ionic liquids were determined by the pendant drop method using Tensiometer Krüss DSA 10. Contact angles measurements were carried out using dynamic sessile drop method using Tensiometer  Krüss  DSA 10. Results are shown in Tables3 and 4.Table 4
Wettability of polymeric supports by ionic liquids determined by sessile drop method at 298 K [36].
Ionic liquid
Support
Advancing angleθa, deg
Receding angleθr, deg
Hysteresisθa−θr, deg
[EMIM][Tf2N]
PES
16.6 ± 0.2
9.6 ± 0.2
7.0
PVDF
12.5 ± 0.7
7.4 ± 0.1
5.1
PA
10.3 ± 0.5
6.8 ± 0.6
3.5
PP
12.3 ± 0.5
7.8 ± 0.6
4.5
[EMIM][TfO]
PES
14.5 ± 0.6
8.3 ± 0.2
6.2
PVDF
15.5 ± 0.6
8.4 ± 0.2
7.1
PA
14.2 ± 0.3
8.1 ± 0.2
6.1
PP
11.8 ± 0.9
5.6 ± 0.7
6.2
[BMIM][Tf2N]
PES
16.9 ± 0.2
8.2 ± 0.2
8.7
PVDF
19.2 ± 0.5
10.9 ± 0.5
8.3
PA
10.7 ± 0.4
8.4 ± 0.3
2.3
PP
13.9 ± 0.4
8.0 ± 0.3
5.9
[BMIM][TfO]
PES
15.5 ± 0.2
8.1 ± 0.2
7.4
PVDF
18.3 ± 0.6
10.4 ± 0.7
7.9
PA
8.1 ± 0.3
6.6 ± 0.1
1.5
PP
10.5 ± 0.3
8.8 ± 0.5
1.7


#### 2.2.2. Supported Ionic Liquid Membranes Preparation Procedure

Polymer supports and ionic liquids were degassed in vacuum dryerVacucell 55 according to procedure described in the literature [44–46]. After degassing water content in ionic liquids was determined using Karl-Fischer coulometric titration method with Metrohm 831 KF Coulometer: [EMIM][TfO]-0.370%, [BMIM][TfO]-0.134%, [EMIM][Tf2N]-0.001%, [BMIM][Tf2N]-0.109%. Nevertheless, ionic liquids are hygroscopic, so the water content could change during the experiments.The literature data suggest that the small addition of water improves the performance of membrane. Carbon dioxide permeation increases when the molar fraction of water increases from 0 to 0.1. This improvement can be attributed to increased diffusivity due to the lower viscosity of ionic liquid [47].Degassed polymeric supports were saturated with 0.1cm3 of ionic liquids per 1.0 cm2 of support surface. The excess of ionic liquid was removed from membrane surface using blotting paper until weight of immobilized membrane was stable. The procedure was repeated three times in order to provide complete pores saturation.


#### 2.2.3. Determination of Supports Swelling

Swelling of supports was determined on the basis of supports thickness. Thickness was determined by optical method using epi-fluorescent microscope L3001 equipped with digital camera Canon Power Shot A650 SI. Membrane was placed in glass holder inZ direction according to the procedure described in the literature [48]. In previous work membrane swelling after 24 hours was determined. In present paper, in order to evaluate the time period of swelling effect, data obtained after 72 and 120 hours are presented.


#### 2.2.4. Evaluation of SILMs Stability

Mechanical resistance of membrane systems on pressure difference over the membrane was investigated in laboratory test unit presented in Figure1. Both sides of the chamber were evacuated using vacuum pump, and inert gas was released to the feed side at a rate of 50 Pa/s. Pressure difference was recorded using pressure sensors MPX 5100DP and software using Glanguage. Experiments were conducted in 283, 288, and 298 K.Figure 1
Diagram of the laboratory unit for the determination of CO2/CH4 permeation: 1: CO2/CH4 gas container, 2: gas sample container, 3: pressure sensor, 4: computer, 5: CO2 analyser, 6: thermostat, 7: A/D converter, 8: vacuum pump, 9: chamber, 10: SILM, and 11: valves.


#### 2.2.5. Determination of Carbon Dioxide/Methane Permeation

Permeation was determined using laboratory unit shown in Figure1. Polymeric support saturated with ionic liquid (10) was placed in a stainless steel chamber (9), consisting of two parts: upper (feed side) and bottom (permeate side). The chamber was equipped with heating jacket coupled with thermostat (6). The experiments were carried out in 283, 288, and 298 K with 0.1 K accuracy. Both sides of the chamber were equipped with electronic temperature sensors and connected to vacuum oil pump (8). Gas container (1) was attached through differential pressure regulator with thermostatic gas sample container (2) connected to the feed part of the chamber. Pressure sensor signal (MPX 5100 DP)was transmitted to the A/D converter (7) and was recorded with software using G-language (4). The CO2 concentration in gas sample container was measured using IR analyser (5) in order to ensure that there are no other gases present in the container apart from carbon dioxide.Experiments were carried out as the following:(i)
obtaining vacuum in feed and permeate sides (to remove CO2, O2, N2, and other gases),(ii)
filling gas sampler (2) with CO2/CH4,(iii)
obtaining desirable temperature in the chamber and gas sampler containing CO2/CH4,(iv)
filling the feed side of the chamber with CO2from gas sample container at a rate of 50 Pa/s, to obtain 30 kPa pressure difference between feed and permeate side. The pressure of 30 kPa was the maximum pressure that did not cause SILM deformation.The drop of pressure in feed chamber and increase of pressure in permeate chamber were determined with differential pressure sensor during the experiment.Permeation was determined on the basis of pressure difference between the feed and permeate side in time period when the pressure drop was linear.Figure2 presents the linear approximation of pressure difference included in (2).Figure 2
Linear approximation of pressure difference.Thickness of the membrane was determined before each measurement.Application of freshly prepared SILM membrane for each experiment allowed to use the same volume of feed stream and permeate stream in every single experiment and to eliminate necessity of determination of the CO2 amount already dissolved in the ionic liquid.


## 2.1. Materials

Supported ionic liquids membranes were prepared using selected polymeric supports:GH Polypro (polypropylene) (PP), FP Vericel (polyvinylidene fluoride) (PVDF), Nylaflo (polyamide) (PA), and Supor (polyethersulphone) (PES), (Pall, Gelman Laboratory, USA). For permeation experiments PP membrane was selected in order to good wettability and low swelling as indicated in results section. Four ionic liquids were applied as a membrane phase: 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide [EMIM][Tf2N],1-ethyl-3-methylimidazolium trifluoromethanesulfonate [EMIM][TfO],1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide [BMIM][Tf2N],1-butyl-3-methylimidazolium trifluoromethanesulfonate [BMIM][TfO].Imidazolium ionic liquids with [Tf2N] and [TfO] anions were selected, as they exhibit very good carbon dioxide absorption in comparison to [BF4], [PF6] [14, 17, 43]. All chemicals were supplied by IOLITEC, Heilbronn, Germany, with purity above 99%. In order to determine the effect of chemical structure of the ionic liquids on CO2 diffusion, different alkyl chain lengths of the cations and different anions were selected.Physical and chemical properties of polymeric supports and ionic liquids applied in experiments are presented in Tables2 and 3.Table 2
Physicochemical parameters of polymeric supports reported by producer.
Support
Density, kg/m3
Pore diameter, µm
Total porosity, %
Thickness, µm
PP
900
0.2
80
92
PVDF
1790
0.2
80
123
PA
1130
0.2
80
110
PES
1370–1510
0.2
80
148Table 3
Physicochemical properties of ionic liquids used in the experiments at 298 K.
Ionic liquids
Chemical formula
Density, g/cm3*
Viscosity, mPa·s
Surface tension, mN/m
[EMIM][Tf2N]
[C6N2H11]+[(CF3SO2)2N]−
1.52
32.60
32.56
[EMIM][TfO]
[C6N2H11]+[CF3SO3]−
1.39
40.40
37.82
[BMIM][Tf2N]
[C8N2H15]+[(CF3SO2)2N]−
1.43
48.06
30.83
[BMIM][TfO]
[C8N2H15]+[CF3SO3]−
1.29
74.30
34.67
*Data provided by producer.


## 2.2. Methods

### 2.2.1. Viscosity, Surface Tension, and Contact Angles Measurements

Measurements of dynamic viscosity coefficient of selected ionic liquids were conducted using Brookfield Rheometer LV III. The dependence of shear stress (Pa) on shear rate (1/s) was determined. Ionic liquids viscosity remains constant with increasing shear rates. Such linear relationship between shear stress and shear rate is related to newtonian character of the liquid. Surface tensions of selected ionic liquids were determined by the pendant drop method using Tensiometer Krüss DSA 10. Contact angles measurements were carried out using dynamic sessile drop method using Tensiometer  Krüss  DSA 10. Results are shown in Tables3 and 4.Table 4
Wettability of polymeric supports by ionic liquids determined by sessile drop method at 298 K [36].
Ionic liquid
Support
Advancing angleθa, deg
Receding angleθr, deg
Hysteresisθa−θr, deg
[EMIM][Tf2N]
PES
16.6 ± 0.2
9.6 ± 0.2
7.0
PVDF
12.5 ± 0.7
7.4 ± 0.1
5.1
PA
10.3 ± 0.5
6.8 ± 0.6
3.5
PP
12.3 ± 0.5
7.8 ± 0.6
4.5
[EMIM][TfO]
PES
14.5 ± 0.6
8.3 ± 0.2
6.2
PVDF
15.5 ± 0.6
8.4 ± 0.2
7.1
PA
14.2 ± 0.3
8.1 ± 0.2
6.1
PP
11.8 ± 0.9
5.6 ± 0.7
6.2
[BMIM][Tf2N]
PES
16.9 ± 0.2
8.2 ± 0.2
8.7
PVDF
19.2 ± 0.5
10.9 ± 0.5
8.3
PA
10.7 ± 0.4
8.4 ± 0.3
2.3
PP
13.9 ± 0.4
8.0 ± 0.3
5.9
[BMIM][TfO]
PES
15.5 ± 0.2
8.1 ± 0.2
7.4
PVDF
18.3 ± 0.6
10.4 ± 0.7
7.9
PA
8.1 ± 0.3
6.6 ± 0.1
1.5
PP
10.5 ± 0.3
8.8 ± 0.5
1.7


### 2.2.2. Supported Ionic Liquid Membranes Preparation Procedure

Polymer supports and ionic liquids were degassed in vacuum dryerVacucell 55 according to procedure described in the literature [44–46]. After degassing water content in ionic liquids was determined using Karl-Fischer coulometric titration method with Metrohm 831 KF Coulometer: [EMIM][TfO]-0.370%, [BMIM][TfO]-0.134%, [EMIM][Tf2N]-0.001%, [BMIM][Tf2N]-0.109%. Nevertheless, ionic liquids are hygroscopic, so the water content could change during the experiments.The literature data suggest that the small addition of water improves the performance of membrane. Carbon dioxide permeation increases when the molar fraction of water increases from 0 to 0.1. This improvement can be attributed to increased diffusivity due to the lower viscosity of ionic liquid [47].Degassed polymeric supports were saturated with 0.1cm3 of ionic liquids per 1.0 cm2 of support surface. The excess of ionic liquid was removed from membrane surface using blotting paper until weight of immobilized membrane was stable. The procedure was repeated three times in order to provide complete pores saturation.


### 2.2.3. Determination of Supports Swelling

Swelling of supports was determined on the basis of supports thickness. Thickness was determined by optical method using epi-fluorescent microscope L3001 equipped with digital camera Canon Power Shot A650 SI. Membrane was placed in glass holder inZ direction according to the procedure described in the literature [48]. In previous work membrane swelling after 24 hours was determined. In present paper, in order to evaluate the time period of swelling effect, data obtained after 72 and 120 hours are presented.


### 2.2.4. Evaluation of SILMs Stability

Mechanical resistance of membrane systems on pressure difference over the membrane was investigated in laboratory test unit presented in Figure1. Both sides of the chamber were evacuated using vacuum pump, and inert gas was released to the feed side at a rate of 50 Pa/s. Pressure difference was recorded using pressure sensors MPX 5100DP and software using Glanguage. Experiments were conducted in 283, 288, and 298 K.Figure 1
Diagram of the laboratory unit for the determination of CO2/CH4 permeation: 1: CO2/CH4 gas container, 2: gas sample container, 3: pressure sensor, 4: computer, 5: CO2 analyser, 6: thermostat, 7: A/D converter, 8: vacuum pump, 9: chamber, 10: SILM, and 11: valves.


### 2.2.5. Determination of Carbon Dioxide/Methane Permeation

Permeation was determined using laboratory unit shown in Figure1. Polymeric support saturated with ionic liquid (10) was placed in a stainless steel chamber (9), consisting of two parts: upper (feed side) and bottom (permeate side). The chamber was equipped with heating jacket coupled with thermostat (6). The experiments were carried out in 283, 288, and 298 K with 0.1 K accuracy. Both sides of the chamber were equipped with electronic temperature sensors and connected to vacuum oil pump (8). Gas container (1) was attached through differential pressure regulator with thermostatic gas sample container (2) connected to the feed part of the chamber. Pressure sensor signal (MPX 5100 DP)was transmitted to the A/D converter (7) and was recorded with software using G-language (4). The CO2 concentration in gas sample container was measured using IR analyser (5) in order to ensure that there are no other gases present in the container apart from carbon dioxide.Experiments were carried out as the following:(i)
obtaining vacuum in feed and permeate sides (to remove CO2, O2, N2, and other gases),(ii)
filling gas sampler (2) with CO2/CH4,(iii)
obtaining desirable temperature in the chamber and gas sampler containing CO2/CH4,(iv)
filling the feed side of the chamber with CO2from gas sample container at a rate of 50 Pa/s, to obtain 30 kPa pressure difference between feed and permeate side. The pressure of 30 kPa was the maximum pressure that did not cause SILM deformation.The drop of pressure in feed chamber and increase of pressure in permeate chamber were determined with differential pressure sensor during the experiment.Permeation was determined on the basis of pressure difference between the feed and permeate side in time period when the pressure drop was linear.Figure2 presents the linear approximation of pressure difference included in (2).Figure 2
Linear approximation of pressure difference.Thickness of the membrane was determined before each measurement.Application of freshly prepared SILM membrane for each experiment allowed to use the same volume of feed stream and permeate stream in every single experiment and to eliminate necessity of determination of the CO2 amount already dissolved in the ionic liquid.


## 2.2.1. Viscosity, Surface Tension, and Contact Angles Measurements

Measurements of dynamic viscosity coefficient of selected ionic liquids were conducted using Brookfield Rheometer LV III. The dependence of shear stress (Pa) on shear rate (1/s) was determined. Ionic liquids viscosity remains constant with increasing shear rates. Such linear relationship between shear stress and shear rate is related to newtonian character of the liquid. Surface tensions of selected ionic liquids were determined by the pendant drop method using Tensiometer Krüss DSA 10. Contact angles measurements were carried out using dynamic sessile drop method using Tensiometer  Krüss  DSA 10. Results are shown in Tables3 and 4.Table 4
Wettability of polymeric supports by ionic liquids determined by sessile drop method at 298 K [36].
Ionic liquid
Support
Advancing angleθa, deg
Receding angleθr, deg
Hysteresisθa−θr, deg
[EMIM][Tf2N]
PES
16.6 ± 0.2
9.6 ± 0.2
7.0
PVDF
12.5 ± 0.7
7.4 ± 0.1
5.1
PA
10.3 ± 0.5
6.8 ± 0.6
3.5
PP
12.3 ± 0.5
7.8 ± 0.6
4.5
[EMIM][TfO]
PES
14.5 ± 0.6
8.3 ± 0.2
6.2
PVDF
15.5 ± 0.6
8.4 ± 0.2
7.1
PA
14.2 ± 0.3
8.1 ± 0.2
6.1
PP
11.8 ± 0.9
5.6 ± 0.7
6.2
[BMIM][Tf2N]
PES
16.9 ± 0.2
8.2 ± 0.2
8.7
PVDF
19.2 ± 0.5
10.9 ± 0.5
8.3
PA
10.7 ± 0.4
8.4 ± 0.3
2.3
PP
13.9 ± 0.4
8.0 ± 0.3
5.9
[BMIM][TfO]
PES
15.5 ± 0.2
8.1 ± 0.2
7.4
PVDF
18.3 ± 0.6
10.4 ± 0.7
7.9
PA
8.1 ± 0.3
6.6 ± 0.1
1.5
PP
10.5 ± 0.3
8.8 ± 0.5
1.7


## 2.2.2. Supported Ionic Liquid Membranes Preparation Procedure

Polymer supports and ionic liquids were degassed in vacuum dryerVacucell 55 according to procedure described in the literature [44–46]. After degassing water content in ionic liquids was determined using Karl-Fischer coulometric titration method with Metrohm 831 KF Coulometer: [EMIM][TfO]-0.370%, [BMIM][TfO]-0.134%, [EMIM][Tf2N]-0.001%, [BMIM][Tf2N]-0.109%. Nevertheless, ionic liquids are hygroscopic, so the water content could change during the experiments.The literature data suggest that the small addition of water improves the performance of membrane. Carbon dioxide permeation increases when the molar fraction of water increases from 0 to 0.1. This improvement can be attributed to increased diffusivity due to the lower viscosity of ionic liquid [47].Degassed polymeric supports were saturated with 0.1cm3 of ionic liquids per 1.0 cm2 of support surface. The excess of ionic liquid was removed from membrane surface using blotting paper until weight of immobilized membrane was stable. The procedure was repeated three times in order to provide complete pores saturation.


## 2.2.3. Determination of Supports Swelling

Swelling of supports was determined on the basis of supports thickness. Thickness was determined by optical method using epi-fluorescent microscope L3001 equipped with digital camera Canon Power Shot A650 SI. Membrane was placed in glass holder inZ direction according to the procedure described in the literature [48]. In previous work membrane swelling after 24 hours was determined. In present paper, in order to evaluate the time period of swelling effect, data obtained after 72 and 120 hours are presented.


## 2.2.4. Evaluation of SILMs Stability

Mechanical resistance of membrane systems on pressure difference over the membrane was investigated in laboratory test unit presented in Figure1. Both sides of the chamber were evacuated using vacuum pump, and inert gas was released to the feed side at a rate of 50 Pa/s. Pressure difference was recorded using pressure sensors MPX 5100DP and software using Glanguage. Experiments were conducted in 283, 288, and 298 K.Figure 1
Diagram of the laboratory unit for the determination of CO2/CH4 permeation: 1: CO2/CH4 gas container, 2: gas sample container, 3: pressure sensor, 4: computer, 5: CO2 analyser, 6: thermostat, 7: A/D converter, 8: vacuum pump, 9: chamber, 10: SILM, and 11: valves.


## 2.2.5. Determination of Carbon Dioxide/Methane Permeation

Permeation was determined using laboratory unit shown in Figure1. Polymeric support saturated with ionic liquid (10) was placed in a stainless steel chamber (9), consisting of two parts: upper (feed side) and bottom (permeate side). The chamber was equipped with heating jacket coupled with thermostat (6). The experiments were carried out in 283, 288, and 298 K with 0.1 K accuracy. Both sides of the chamber were equipped with electronic temperature sensors and connected to vacuum oil pump (8). Gas container (1) was attached through differential pressure regulator with thermostatic gas sample container (2) connected to the feed part of the chamber. Pressure sensor signal (MPX 5100 DP)was transmitted to the A/D converter (7) and was recorded with software using G-language (4). The CO2 concentration in gas sample container was measured using IR analyser (5) in order to ensure that there are no other gases present in the container apart from carbon dioxide.Experiments were carried out as the following:(i)
obtaining vacuum in feed and permeate sides (to remove CO2, O2, N2, and other gases),(ii)
filling gas sampler (2) with CO2/CH4,(iii)
obtaining desirable temperature in the chamber and gas sampler containing CO2/CH4,(iv)
filling the feed side of the chamber with CO2from gas sample container at a rate of 50 Pa/s, to obtain 30 kPa pressure difference between feed and permeate side. The pressure of 30 kPa was the maximum pressure that did not cause SILM deformation.The drop of pressure in feed chamber and increase of pressure in permeate chamber were determined with differential pressure sensor during the experiment.Permeation was determined on the basis of pressure difference between the feed and permeate side in time period when the pressure drop was linear.Figure2 presents the linear approximation of pressure difference included in (2).Figure 2
Linear approximation of pressure difference.Thickness of the membrane was determined before each measurement.Application of freshly prepared SILM membrane for each experiment allowed to use the same volume of feed stream and permeate stream in every single experiment and to eliminate necessity of determination of the CO2 amount already dissolved in the ionic liquid.


## 3. Results and Discussion

### 3.1. Determination of Supports Swelling and Wettability

We have previously reported data on swelling of the membrane after 24 hours from immobilization procedure [36]. All the investigated supports showed higher thickness after immobilization with ionic liquid.In present paper, data on thickness after 2, 72, and 120 hours from saturation are presented. The initial thickness of the membranes is as follows: PP75±1, PA 115±1, PES 118±1, and PVDF 160±1. Considering data presented in Figure 3, rapid increase of thickness is observed immediately after impregnation, further differences are rather less distinct; however, the trend is preserved. Polyamide support shows similar thickness for all ionic liquids used in this study, the rate of swelling is the lowest, and it corresponds to incomplete pores saturation with the liquid, that was calculated on the basis of ratio of the real mass of IL embedded in the support pores and the theoretical value of the maximum amount of IL possible to immobilize.Figure 3
Increase of polypropylene membrane thickness.Swelling of polymeric membranes can affect mechanical stability of the supports decreasing the maximum transmembrane pressure possible to apply without causing membrane damage.The rate of swelling for all ionic liquids used in the study is similar and stays with correlation to wetting of the supports. All the values of contact angles calculated from sessile drop measurements (Table4) were below 20 deg., therefore all the examined ionic liquids are suitable for perfect wetting of supports. The best wettability was observed for PA membrane, successively for PP, PVDF, and PES; however, the differences are not significant.According to Young equation assumptions, equilibrium contact angle does not change when changing the drop volume. Supports examined in this study do not meet Young equation foundations, the drop is in the metastable state, and the hysteresis is observed. There are two components of the hysteresis value, the first one is the thermodynamic hysteresis dependent on the surface roughness and heterogeneity, whereas the second one is the dynamic hysteresis that is connected to chemical interactions of liquid and solid, penetration of liquid into polymer pores, and the ability of atoms or functional groups to change its positions.The first component is not affected by the time of solid-liquid drop contact, whereas dynamic hysteresis is, and moreover is dependent on the properties of polymer and ionic liquid.Taking into account swelling of the supports, it is observed that the polypropylene membrane gains almost the same thickness immediately after impregnation for all ionic liquids used in the study, and it can be assumed that the hysteresis is dependent only on the surface roughness and heterogeneity. Further changes in thickness of the supports are connected to the liquid penetration into the pores and free space between polymer molecules and reorientation of functional groups of ionic liquids, so the particles in the ionic liquid-polymer interface reach the minimum of free interface energy. Polypropylene supports gain about 30–40% of thickness and yet PA ones gain only about 4% (Figure4).Figure 4
Increase of thickness of different supports saturated with ionic liquids after 120 hours.


### 3.2. Determination of Mechanical Stability

The mechanical stability of investigated supports was determined in order to check the potential of technological application. Figure5 presents maximum transmembrane pressure not causing polypropylene support damage. Supported ionic liquid membranes based on polypropylene support present the highest mechanical stability for operating pressures between 40 and 50 kPa. Pressure changes in course of experiment are shown in Figure 6. The peak at the curve is a result of pushing the solvent out of the pores of the support, and the gas leakage is observed. Further increase of feed stream pressure applied over the membrane leads to the polypropylene support damage, whereas for other SILMs the transmembrane pressure possible to apply without support degradation is lower than pressure required to push the impregnating liquid out of the pores. The highest pressure difference across the membrane obtained during the experiments reached 59 kPa. Data presented in Table 5 suggest that polypropylene membrane is more stable in lower temperatures. Higher stability for PP-[EMIM][TfO] membrane stays in correlation with swelling of the membrane. Swelling rate of the PP membrane is lower for [EMIM][TfO] than for [EMIM][Tf2N]. Structure changes of PP impregnated with [EMIM][Tf2N] caused lower mechanical stability of this system. However, experiments conducted in higher temperatures with different ionic liquids need to be done. Polyethersulphone membrane was damaged even if minimum pressure was applied.Table 5
Mechanical stability of supports.
Membrane
Ionic liquid
Maximum pressure difference obtained, kPa
Average pressure difference in 283 K, kPa
Average pressure difference in 288 K, kPa
Average pressure difference in 298 K, kPa
PES
[EMIM][Tf2N]
4.70
n/a
n/a
4.70 ± 0.30
[EMIM][TfO]
5.21
n/a
n/a
5.10 ± 0.20
PVDF
[EMIM][Tf2N]
22.81
22.14 ± 1.05
21.57 ± 1.24
20.18 ± 1.53
[EMIM][TfO]
21.82
21.10 ± 0.63
20.60 ± 0.43
20.15 ± 0.87
PA
[EMIM][Tf2N]
22.30
n/a
n/a
20.31 ± 1.21
[EMIM][TfO]
13.42
n/a
n/a
11.20 ± 0.96
[EMIM][Tf2N]
55.75
51.97 ± 3.48
47.68 ± 3.06
43.31 ± 4.77
PP
[EMIM][TfO]
59.53
53.68 ± 1.87
51.78 ± 3.39
49.43 ± 6.23
[BMIM][Tf2N]
47.64
46.40 ± 1.02
45.08 ± 1.73
44.59 ± 2.89
[BMIM][TfO]
51.78
50.65 ± 1.16
48.28 ± 1.48
47.07 ± 1.00Maximum transmembrane pressure obtained for PP support in different temperatures.
(a)
(b)Figure 6
Pressure changes during stability measurements of SILMs.In order to determine the impact of cation structure on stability of the system, polypropylene membrane was also impregnated with ionic liquids based on 1-butyl-3-methylimidazolium cation. For PP-based systems, maximum pressure difference between feed and permeate side was higher when using [TfO] based ionic liquids: about 60 kPa for [EMIM][TfO] and 48 kPa for [BMIM][TfO], than for systems using [Tf2N] ionic liquids as a membrane phase: 56 kPa for [EMIM][Tf2N] and 46 kPa for [BMIM][Tf2N]. The differences are not significant; however, when related to all examined temperatures, in total, membranes using ionic liquids based on [TfO] anion are slightly more stable, nevertheless it stays with a disagreement to the swelling data. However, it is likely that [TfO] anion-based ionic liquids make polypropylene more elastic enhancing the pressure resistance. The membrane is then deformed under the pressure before cracking.The cation structure also affects mechanical properties. It can be seen that the longer hydrocarbon chain in cation structure is, the more disruptions in membrane structure occur, and the lower the mechanical stability is. Ionic liquid penetrates into the support pores and between polymer particles and fibers reorientating its structure to energetically favorable position. The longer alkyl chain length, the greater space is occupied with the ionic liquid, and the greater support expansion is observed.Obtained results suggest that it is possible to use such SILMs without any additional mechanical supports in ventilation systems that reveal only slight pressure fluctuations. Moreover, applying SILMs to improve biogas quality directly in outlets of fermentation reactors without gas compression would also bring some profits. In many cases for the proper work of electric generators it is necessary to increase the methane content in biogas. That is why the application of SILMs is considered to be a promising perspective, especially when comparing to other methods requiring pressure increasing and regeneration of absorbent.


### 3.3. Determination of Carbon Dioxide and Methane Permeation

Permeability of the supported ionic liquid membranes at different temperatures is presented in Table6. It can be seen that for each SILM system permeability increases with the increase of temperature.Table 6
Permeability of carbon dioxide and methane through SILMs (with PP support) at different temperatures.
Ionic liquid
Temperature, K
Permeability, barrer
Viscosity of ionic liquid, mPa·s
Carbon dioxide
Methane
283
749 ± 14
n/a
56.36 ± 1.93
[EMIM][Tf2N]
288
811 ± 14
n/a
51.55 ± 1.27
298
1888 ± 117
101 ± 1
40.40 ± 1.80
283
636 ± 69
n/a
44.77 ± 0.63
[EMIM][TfO]
288
684 ± 31
n/a
42.26 ± 0.61
298
1076 ± 111
60 ± 17
32.60 ± 1.07
[BMIM][Tf2N]
298
936 ± 26
77 ± 2
74.30 ± 0.71
[BMIM][TfO]
298
754 ± 33
43 ± 2
48.06 ± 1.95Carbon dioxide permeability of the PP membrane-[EMIM][TfO] system increases from 636 to 1076 barrers, as the temperature increases from 283 to 298 K and from 749 to 1888 barrers for PP membrane-[EMIM][Tf2N] system. Temperature increase causes an increase of ions activity and decrease of ionic liquid viscosity and therefore an increase of CO2 permeation. According to presented data it can be concluded that the longer is hydrocarbon chain in the cation structure, the lower permeability is observed. Scovazzo et al. reported similar permeability for PES support impregnated with [EMIM][Tf2N], 960 barrers at room temperature. Ilconich et al. in their study of PS membranes immobilized with [HMIM][Tf2N] reported a CO2 permeability 744 barrers at 310 K and 1200 barrers at 398 K [49].It can be concluded that choosing proper polymer support is essential for obtaining satisfactory CO2 permeation. For example  Baltus et al. used an inorganic (γ-alumina) support with [BMIM][Tf2N] and obtained significantly lower values of permeation-70 barrers [4].Methane permeation values stay in agreement with literature data. They are significantly lower than carbon dioxide permeation values. Selectivity obtained by dividing the permeabilities of two pure gases is about 16 for [EMIM] [TfO] and 17 for [EMIM] [Tf2N].


## 3.1. Determination of Supports Swelling and Wettability

We have previously reported data on swelling of the membrane after 24 hours from immobilization procedure [36]. All the investigated supports showed higher thickness after immobilization with ionic liquid.In present paper, data on thickness after 2, 72, and 120 hours from saturation are presented. The initial thickness of the membranes is as follows: PP75±1, PA 115±1, PES 118±1, and PVDF 160±1. Considering data presented in Figure 3, rapid increase of thickness is observed immediately after impregnation, further differences are rather less distinct; however, the trend is preserved. Polyamide support shows similar thickness for all ionic liquids used in this study, the rate of swelling is the lowest, and it corresponds to incomplete pores saturation with the liquid, that was calculated on the basis of ratio of the real mass of IL embedded in the support pores and the theoretical value of the maximum amount of IL possible to immobilize.Figure 3
Increase of polypropylene membrane thickness.Swelling of polymeric membranes can affect mechanical stability of the supports decreasing the maximum transmembrane pressure possible to apply without causing membrane damage.The rate of swelling for all ionic liquids used in the study is similar and stays with correlation to wetting of the supports. All the values of contact angles calculated from sessile drop measurements (Table4) were below 20 deg., therefore all the examined ionic liquids are suitable for perfect wetting of supports. The best wettability was observed for PA membrane, successively for PP, PVDF, and PES; however, the differences are not significant.According to Young equation assumptions, equilibrium contact angle does not change when changing the drop volume. Supports examined in this study do not meet Young equation foundations, the drop is in the metastable state, and the hysteresis is observed. There are two components of the hysteresis value, the first one is the thermodynamic hysteresis dependent on the surface roughness and heterogeneity, whereas the second one is the dynamic hysteresis that is connected to chemical interactions of liquid and solid, penetration of liquid into polymer pores, and the ability of atoms or functional groups to change its positions.The first component is not affected by the time of solid-liquid drop contact, whereas dynamic hysteresis is, and moreover is dependent on the properties of polymer and ionic liquid.Taking into account swelling of the supports, it is observed that the polypropylene membrane gains almost the same thickness immediately after impregnation for all ionic liquids used in the study, and it can be assumed that the hysteresis is dependent only on the surface roughness and heterogeneity. Further changes in thickness of the supports are connected to the liquid penetration into the pores and free space between polymer molecules and reorientation of functional groups of ionic liquids, so the particles in the ionic liquid-polymer interface reach the minimum of free interface energy. Polypropylene supports gain about 30–40% of thickness and yet PA ones gain only about 4% (Figure4).Figure 4
Increase of thickness of different supports saturated with ionic liquids after 120 hours.


## 3.2. Determination of Mechanical Stability

The mechanical stability of investigated supports was determined in order to check the potential of technological application. Figure5 presents maximum transmembrane pressure not causing polypropylene support damage. Supported ionic liquid membranes based on polypropylene support present the highest mechanical stability for operating pressures between 40 and 50 kPa. Pressure changes in course of experiment are shown in Figure 6. The peak at the curve is a result of pushing the solvent out of the pores of the support, and the gas leakage is observed. Further increase of feed stream pressure applied over the membrane leads to the polypropylene support damage, whereas for other SILMs the transmembrane pressure possible to apply without support degradation is lower than pressure required to push the impregnating liquid out of the pores. The highest pressure difference across the membrane obtained during the experiments reached 59 kPa. Data presented in Table 5 suggest that polypropylene membrane is more stable in lower temperatures. Higher stability for PP-[EMIM][TfO] membrane stays in correlation with swelling of the membrane. Swelling rate of the PP membrane is lower for [EMIM][TfO] than for [EMIM][Tf2N]. Structure changes of PP impregnated with [EMIM][Tf2N] caused lower mechanical stability of this system. However, experiments conducted in higher temperatures with different ionic liquids need to be done. Polyethersulphone membrane was damaged even if minimum pressure was applied.Table 5
Mechanical stability of supports.
Membrane
Ionic liquid
Maximum pressure difference obtained, kPa
Average pressure difference in 283 K, kPa
Average pressure difference in 288 K, kPa
Average pressure difference in 298 K, kPa
PES
[EMIM][Tf2N]
4.70
n/a
n/a
4.70 ± 0.30
[EMIM][TfO]
5.21
n/a
n/a
5.10 ± 0.20
PVDF
[EMIM][Tf2N]
22.81
22.14 ± 1.05
21.57 ± 1.24
20.18 ± 1.53
[EMIM][TfO]
21.82
21.10 ± 0.63
20.60 ± 0.43
20.15 ± 0.87
PA
[EMIM][Tf2N]
22.30
n/a
n/a
20.31 ± 1.21
[EMIM][TfO]
13.42
n/a
n/a
11.20 ± 0.96
[EMIM][Tf2N]
55.75
51.97 ± 3.48
47.68 ± 3.06
43.31 ± 4.77
PP
[EMIM][TfO]
59.53
53.68 ± 1.87
51.78 ± 3.39
49.43 ± 6.23
[BMIM][Tf2N]
47.64
46.40 ± 1.02
45.08 ± 1.73
44.59 ± 2.89
[BMIM][TfO]
51.78
50.65 ± 1.16
48.28 ± 1.48
47.07 ± 1.00Maximum transmembrane pressure obtained for PP support in different temperatures.
(a)
(b)Figure 6
Pressure changes during stability measurements of SILMs.In order to determine the impact of cation structure on stability of the system, polypropylene membrane was also impregnated with ionic liquids based on 1-butyl-3-methylimidazolium cation. For PP-based systems, maximum pressure difference between feed and permeate side was higher when using [TfO] based ionic liquids: about 60 kPa for [EMIM][TfO] and 48 kPa for [BMIM][TfO], than for systems using [Tf2N] ionic liquids as a membrane phase: 56 kPa for [EMIM][Tf2N] and 46 kPa for [BMIM][Tf2N]. The differences are not significant; however, when related to all examined temperatures, in total, membranes using ionic liquids based on [TfO] anion are slightly more stable, nevertheless it stays with a disagreement to the swelling data. However, it is likely that [TfO] anion-based ionic liquids make polypropylene more elastic enhancing the pressure resistance. The membrane is then deformed under the pressure before cracking.The cation structure also affects mechanical properties. It can be seen that the longer hydrocarbon chain in cation structure is, the more disruptions in membrane structure occur, and the lower the mechanical stability is. Ionic liquid penetrates into the support pores and between polymer particles and fibers reorientating its structure to energetically favorable position. The longer alkyl chain length, the greater space is occupied with the ionic liquid, and the greater support expansion is observed.Obtained results suggest that it is possible to use such SILMs without any additional mechanical supports in ventilation systems that reveal only slight pressure fluctuations. Moreover, applying SILMs to improve biogas quality directly in outlets of fermentation reactors without gas compression would also bring some profits. In many cases for the proper work of electric generators it is necessary to increase the methane content in biogas. That is why the application of SILMs is considered to be a promising perspective, especially when comparing to other methods requiring pressure increasing and regeneration of absorbent.


## 3.3. Determination of Carbon Dioxide and Methane Permeation

Permeability of the supported ionic liquid membranes at different temperatures is presented in Table6. It can be seen that for each SILM system permeability increases with the increase of temperature.Table 6
Permeability of carbon dioxide and methane through SILMs (with PP support) at different temperatures.
Ionic liquid
Temperature, K
Permeability, barrer
Viscosity of ionic liquid, mPa·s
Carbon dioxide
Methane
283
749 ± 14
n/a
56.36 ± 1.93
[EMIM][Tf2N]
288
811 ± 14
n/a
51.55 ± 1.27
298
1888 ± 117
101 ± 1
40.40 ± 1.80
283
636 ± 69
n/a
44.77 ± 0.63
[EMIM][TfO]
288
684 ± 31
n/a
42.26 ± 0.61
298
1076 ± 111
60 ± 17
32.60 ± 1.07
[BMIM][Tf2N]
298
936 ± 26
77 ± 2
74.30 ± 0.71
[BMIM][TfO]
298
754 ± 33
43 ± 2
48.06 ± 1.95Carbon dioxide permeability of the PP membrane-[EMIM][TfO] system increases from 636 to 1076 barrers, as the temperature increases from 283 to 298 K and from 749 to 1888 barrers for PP membrane-[EMIM][Tf2N] system. Temperature increase causes an increase of ions activity and decrease of ionic liquid viscosity and therefore an increase of CO2 permeation. According to presented data it can be concluded that the longer is hydrocarbon chain in the cation structure, the lower permeability is observed. Scovazzo et al. reported similar permeability for PES support impregnated with [EMIM][Tf2N], 960 barrers at room temperature. Ilconich et al. in their study of PS membranes immobilized with [HMIM][Tf2N] reported a CO2 permeability 744 barrers at 310 K and 1200 barrers at 398 K [49].It can be concluded that choosing proper polymer support is essential for obtaining satisfactory CO2 permeation. For example  Baltus et al. used an inorganic (γ-alumina) support with [BMIM][Tf2N] and obtained significantly lower values of permeation-70 barrers [4].Methane permeation values stay in agreement with literature data. They are significantly lower than carbon dioxide permeation values. Selectivity obtained by dividing the permeabilities of two pure gases is about 16 for [EMIM] [TfO] and 17 for [EMIM] [Tf2N].


## 4. Conclusions

It has been shown that the supported ionic liquid membranes prepared with ionic liquids based on the 1-alkyl-3-methylimidazolium cation are stable, especially when using polypropylene support. The effect of alkyl chain length in IL structure on the permeability was studied. The pure gas permeation results have shown that the increase in alkyl chain length and therefore increase in viscosity of ionic liquid cause the decrease in permeation values. The effect of using different ILs anions on the permeability of carbon dioxide was also evaluated, and lower permeability was observed for [TfO] anion, mainly due to higher viscosity and lower solubility of carbon dioxide. Results have also shown that the SILMs used in this study are highly CO2 selective in CO2/CH4 system. This fact indicated the possibility of SILMs application in selective separation of carbon dioxide, especially from gas mixtures containing methane such as biogas streams.SILMs systems used in this study occurred to be more stable when applying lower temperatures. When choosing proper support and type of ionic liquid, it is important to take into account properties of both. Due to interactions between them, effectiveness and lifetime of the membranes can differ significantly in connection to wettability and swelling of the support. Mechanical stability is strongly dependent on those interactions that are expressed by the rate of swelling and contact angles. Structural changes in the polymer usually result in the decrease of mechanical stability and increase of the length of permeation path. Additionally poor wetting can cause interruption of continuity of liquid membrane.



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*Source: 980689-2013-03-12.xml*