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Membranes 2018, 8(4), 124; https://doi.org/10.3390/membranes8040124
Towards Biohydrogen Separation Using Poly(Ionic Liquid)/Ionic Liquid Composite Membranes
Centro de Química Estrutural, Instituto Superior Técnico, Universidade de Lisboa, Avenida Rovisco Pais, 1049-001 Lisboa, Portugal
Instituto de Tecnologia Química e Biológica António Xavier, Universidade Nova de Lisboa, Av. da República, 2780-157 Oeiras, Portugal
Present address: POLYMAT, University of the Basque Country UPV/EHU, Joxe Mari Korta Center, Avda. Tolosa 72, 20018 Donostia-San Sebastian, Spain.
Received: 19 October 2018 / Accepted: 28 November 2018 / Published: 2 December 2018
Considering the high potential of hydrogen (H2) as a clean energy carrier, the implementation of high performance and cost-effective biohydrogen (bioH2) purification techniques is of vital importance, particularly in fuel cell applications. As membrane technology is a potentially energy-saving solution to obtain high-quality biohydrogen, the most promising poly(ionic liquid) (PIL)–ionic liquid (IL) composite membranes that had previously been studied by our group for CO2/N2 separation, containing pyrrolidinium-based PILs with fluorinated or cyano-functionalized anions, were chosen as the starting point to explore the potential of PIL–IL membranes for CO2/H2 separation. The CO2 and H2 permeation properties at the typical conditions of biohydrogen production (T = 308 K and 100 kPa of feed pressure) were measured and discussed. PIL–IL composites prepared with the [C(CN)3]− anion showed higher CO2/H2 selectivity than those containing the [NTf2]− anion. All the membranes revealed CO2/H2 separation performances above the upper bound for this specific separation, highlighting the composite incorporating 60 wt % of [C2mim][C(CN)3] IL.
Keywords:biohydrogen purification; CO2/H2 separation; PIL–IL composite membranes; gas permeation properties
Due to its outstanding intrinsic features, hydrogen (H2) is considered to be the energy carrier of the future. Besides being the simplest element in the universe, the H2 molecule has the highest energy content per unit weight of any known fuel. However, H2 is not a primary fuel source, which means that it is not available in nature and thus needs to be produced . Hydrogen has been produced mainly on an industrial scale from fossil fuels, through natural gas reforming or coal gasification, and from water, using electrolysis in which water (H2O) can be split into hydrogen and oxygen (O2) . Although water splitting is an ecologically clean process compared to the previously mentioned H2 production processes, it is a highly energy-demanding technology .
Hydrogen production using biological processes has been attracting growing attention since it is more environmentally friendly and less energy intensive than the other described H2 production systems because its conditions are close to room temperature (303–313 K) and ambient pressure (100 kPa) . BioH2 production can be divided into two main categories: light-dependent (direct or indirect biophotolysis and photo fermentation) and -independent (dark fermentation) methodologies [4,5,6]. The dark fermentation process has several advantages compared to the other biological processes namely, its potential for cost-effective hydrogen production, the high rate of cell growth, and the non-requirement of light energy . In spite of the recognized potential of biohydrogen for sustainable development, there are still issues regarding its production and purification , such as the elimination of CO2, N2, and other impurities (H2O and H2S), so that an enriched H2 stream can be obtained for efficient energy generation, mostly through fuel cells . Among the several methodologies for separating hydrogen, such as pressure swing adsorption (PSA), cryogenic distillation, and membrane separation, the first two are designed mainly for large-scale hydrogen production and cannot be used without modification for an upgrade of relatively small amounts of biohydrogen . Thus, membrane technology has been reported as an attractive alternative for biohydrogen separation and purification  since it can be introduced easily into hydrogen-producing bioreactors, leading to an integrated process of bioH2 production and purification [11,12], not omitting its important engineering and economic advantages. Particularly, polymeric membranes, such as polysulfone (PSF) and polyimide (PI) , have been considered a suitable choice for biohydrogen separation as they can not only be used at the bioreactors’ operating conditions but they also have low cost, high energy efficiency, and a smaller ecological footprint than conventional separation processes [14,15,16].
Few articles have been published using membranes for bioH2 separation. Among them, the combination of different polymers and ionic liquids (ILs) to prepare polymer/IL composite membranes is one of the most promising approaches, which takes into account the inherent CO2-philicity of ILs . For instance, Kanehashi et al.  prepared different membranes based on a fluorine-containing polyimide and different amounts of [C4mim][NTf2] IL up to 81 wt %, and studied their gas separation performance at 308 K and 100 kPa of feed pressure. The highest CO2/H2 permselectivity (6.6) was obtained for the membrane that contained the maximum amount of IL (81 wt %) . Moreover, Friess et al.  studied the gas permeation properties at 298 K and 100 kPa of feed pressure through membranes composed of poly(vinylidene fluoride-co-hexafluoropropylene) and 20 to 80 wt % of [C2mim][NTf2] IL. Again, the largest CO2 permeability (533 Barrer) and CO2/H2 permselectivity (12.1) were obtained when the highest amount of IL (80 wt %) was used .
With the aim of designing efficient CO2/H2 separation membranes, this work explores the use of poly(ionic liquid)s (PILs), which are well recognized by their high CO2 affinity and designer nature . Different approaches have been proposed to produce PIL-based CO2 separation membranes, such as neat PIL membranes [20,21,22,23], PIL copolymer membranes [19,24], and the incorporation of ILs alone or together with nanoporous materials as fillers, including zeolites or metal-organic frameworks (MOFs), to form PIL/IL/filler mixed matrix membranes (MMMs) [25,26,27]. Among all these approaches, the blend of PILs and ILs to produce homogeneous PIL–IL composite membranes is the most promising due to their high CO2 separation performance, as well as the good mechanical stability of the membranes . Notwithstanding the potential of PILs for CO2 separation [28,29,30,31,32], only a reduced number of works concerning CO2/H2 separation have been reported in the literature. For instance, Carlisle et al.  explored the CO2/H2 separation through imidazolium PIL–IL gel membranes produced by UV polymerization. The time-lag experiments performed at room temperature and 200 kPa of feed pressure showed ideal CO2/H2 selectivities ranging from 6.6 to 12 for membranes prepared with 5 to 100 mol% of a cross-linking monomer and different amounts of free IL and IL monomer. Their best result (CO2 permeability of 540 Barrer and CO2/H2 selectivity of 12) was achieved for the composite containing 100 mol% of cross-linking monomer and 75 wt % of IL . Moreover, Kharul et al.  studied the CO2 and H2 separation properties of polybenzimidazole-based PILs. The different synthesized polybenzimidazole-based PILs exhibited very similar CO2 and H2 permeabilities (<30 Barrer) and, consequently, CO2/H2 selectivities approximately equal to 1 .
Amongst the PIL–IL membranes developed so far for CO2/N2 separation, the most widely explored are those composed of imidazolium-based PILs with fluorinated or cyano-functionalized anions [35,36,37]. However, our group reported PIL–IL membranes made of pyrrolidinium-based PILs combining the same anions, which are particularly simple to prepare through a metathesis reaction of a commercially available polyelectrolyte. The PIL–IL membranes displayed CO2/N2 separation performances near or even above the Robeson upper bound [38,39,40,41]. In fact, the CO2-phylic behavior of the [NTf2]− anion and the CO2 separation efficiency of the [C(CN)3]− anion  motivated us to explore the most promising pyrrolidinium-based PIL–IL composites based on these two anions for CO2/N2 separation, now for CO2/H2 separation.
In this work, solvent casting method was used to prepare composite membranes composed of two pyrrolidinium-based PILs: poly([Pyr11][NTf2]) and poly([Pyr11][C(CN)3]). The poly([Pyr11][NTf2]) was blended with 40 and 60 wt % of the structurally similar [C4mpyr][NTf2] IL and also with 40 wt % of an imidazolium-based IL ([C2mim][NTf2]), while poly([Pyr11][C(CN)3]) was mixed with 40 and 60 wt % of [C2mim][C(CN)3] IL. The chemical structures of the PILs and ILs used are shown in Figure 1. The CO2 and H2 permeation properties (permeability, diffusivity and solubility) were determined at two different temperatures (T = 293 K and T = 308 K) under a transmembrane pressure differential of 100 kPa. A temperature of 293 K was used first so that the results obtained herein could be compared to those previously reported by our group, while T = 308 K was chosen to reproduce the hydrogen bioproduction conditions .
2. Experimental Section
Poly(diallyldimethylammonium) chloride solution (average Mw 400,000–500,000, 20 wt % in water), acetone (99.8%), and acetonitrile (99.8%) were purchased from Sigma-Aldrich (St. Louis, MO, USA). Lithium bis(trifluoromethylsulfonyl)imide (LiNTf2, 99 wt % pure) and sodium tricyanomethanide (NaC(CN)3, 98 wt % pure) were supplied by IoLiTec GmbH (Heilbronn, Germany). The PILs used were previously synthesized by anion metathesis reactions, as described in previous studies [39,43]. All the starting materials used for PIL syntheses, as well as the organic solvents, were used as received. The water was double distilled. The ILs, 1-ethyl-3-methylimidazolium tricyanomethanide ([C2mim][C(CN)3], >98 wt % pure), 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([C2mim][NTf2], >99 wt % pure), and 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)imide ([C4mpyr][NTf2], >99 wt % pure) were provided by IoLiTec GmbH. Carbon dioxide (CO2) and hydrogen (H2) were supplied by Air Liquide with a minimum purity of 99.99%. Gases were used with no further purification.
2.2. Preparation of PIL–IL Membranes
Several free-standing membranes composed of the synthesized PILs and specific quantities of different ILs containing the same anions were produced by solvent casting. The first step was the preparation of 6 (w/v)% and 12 (w/v)% solutions of poly([Pyr11][C(CN)3]) and poly([Pyr11][NTf2]), respectively, in the most suitable solvents and the addition of the respective IL amounts (Table 1). The solutions were mixed using a magnetic stirrer until complete dissolution of the PIL and IL components and then poured into Petri dishes for slow evaporation of the solvent at room temperature. With the aim of obtaining homogeneous membranes, the solvent evaporation took place slowly, for 2/3 days, depending on the solvent used (Table 1), and in a saturated solvent environment. The thicknesses of the prepared membranes (70–210 μm) were measured using a digital micrometer (Mitutoyo, model MDE-25PJ, Kanagawa, Japan). Average thickness was calculated from six measurements taken at different locations of each PIL–IL membrane. All the PIL–IL membranes studied were considered to have good stability since they were malleable and flexible enough to be used in the gas permeation measurements, even for the composites with 60 wt % of IL. Moreover, the evaluation of the mechanical stability of the PIL–IL composite membranes having the [C(CN)3]− anion was recently reported by Tomé et al.  (Young’s modulus (PIL–40IL) ~14 MPa; Young’s modulus (PIL–60IL) ~5).
2.3. Gas Permeation Experiments
A time lag equipment described in detail elsewhere  was used to measure and determine the ideal CO2 and H2 permeabilities and diffusivities through the prepared PIL–IL composites. Initially, each membrane was degassed under vacuum inside the permeation cell for at least 12 h before testing. The gas permeation experiments were performed at 293 K and 308 K with an upstream pressure of 100 kPa (feed) and vacuum (<0.1 kPa) as the initial downstream pressure (permeate). Three separate CO2 and H2 experiments on a single composite membrane were measured. Between each run, the permeation cell and lines were evacuated until the pressure was below 0.1 kPa.
The gas transport through the PIL–IL membranes was assumed to occur according to the solution-diffusion mass transfer mechanism . Thus, the permeability (P) is related to diffusivity (D) and solubility (S) as follows:
The permeate flux of each studied gas (Ji) was experimentally determined using Equation (2) and assuming an ideal gas behavior and a homogeneous membrane :where is the permeate volume, is the variation of downstream pressure, A is the effective membrane surface area, t is the experimental time, R is the gas constant, and T is the temperature. Equation (3) was then used to calculate the ideal gas permeability (Pi) from the pressure driving force () and membrane thickness ():
Gas diffusivity (Di) was determined according to Equation (4). The time-lag parameter (θ) was deduced by extrapolating the slope of the linear portion of the pd vs. t curve back to the time axis, where the intercept is equal to θ :
After defining both Pi and Di, the gas solubility (Si) was also calculated using Equation (1).
The ideal permeability selectivity (or permselectivity), , which can also be expressed as the product of the diffusivity selectivity and the solubility selectivity, was obtained by dividing the permeability of the more permeable species i to the permeability of the less permeable species j, as expressed in Equation (5):
3. Results and Discussion
3.1. CO2 and H2 Permeation Properties
3.1.1. Gas Permeability (P)
The CO2 and H2 permeabilities through the PIL–IL composite membranes that were studied are presented in Figure 2. The CO2 permeability was always higher than that of H2 and both permeabilities increased with increasing temperature, although the increment was not the same between the studied composites, varying from 15 to 50% for CO2 permeability values and from 39 to 77% for H2 permeabilities. The CO2 permeabilities at 293 K for all the membranes discussed here are in good agreement with those already reported [38,39,41], which emphasizes the high reproducibility of the method used. As expected, the incorporation of high amounts of IL led to enhanced CO2 and H2 permeabilities. Additionally, at 308 K, the temperature of bioH2 purification, the PIL NTf2–40 [C2mim][NTf2] membrane presented similar CO2 and H2 permeability values to those of PIL NTf2–60 [C4mpyr][NTf2]. This means that despite the higher structural compatibility of [C4mpyr][NTf2] with the pyrrolidinium-based PIL, the imidazolium-based cation of the IL is determinant in promoting increased gas permeabilities. However, and as already reported by our group , the use of [C2mim][NTf2] instead of [C4mpyr][NTf2] only allowed the incorporation of free IL up to 40 wt % so that a mechanically stable and homogeneous membrane could be obtained. Considering the PIL–IL membranes that comprise the [C(CN)3]− anion in both PIL and IL, the PIL C(CN)3–60 [C2mim][C(CN)3] composite showed the highest CO2 permeability (505 Barrer) at 308 K but not the highest H2 permeability (40.3 Barrer), which was obtained for the PIL NTf2–60 [C4mpyr][NTf2] composite membrane (46.0 Barrer). Moreover, CO2 permeability increased about 42% while H2 permeability increased approximately 57% when the IL content in the PIL C(CN)3–[C2mim][C(CN)3] composite varied from 40 to 60 wt %. A significant difference in CO2 permeability (76%) was obtained for the PIL–IL membranes that contained [C4mpyr][NTf2] IL when the IL amount increased from 40 to 60 wt %, while the increment in H2 permeability was only around 34%.
3.1.2. Gas Diffusivity (D)
The experimental gas diffusivity results at 293 K and 308 K through the prepared membranes are listed in Table 2. A high difference (one or, in some cases, two orders of magnitude) between CO2 and H2 diffusivity values, which corresponds to CO2/H2 diffusivity selectivities around 0.1, was observed. This difference in gas diffusivities was mainly due to the smaller size of H2 (2.89 Å) compared to CO2 kinetic diameter (3.30 Å) . Moreover, both CO2 and H2 diffusivity increased with increasing temperature and with increasing IL content in the PIL–IL composite (Table 2). The same behavior was also found for CO2 and H2 permeabilities (Figure 2). From Table 2, it can also be seen that CO2 and H2 diffusivities through the prepared membranes can be ordered as follows: PIL NTf2–40 [C4mpyr][NTf2] < PIL NTf2–60 [C4mpyr][NTf2] < PIL NTf2–40 [C2mim][NTf2] < PIL C(CN)3–40 [C2mim][C(CN)3] < PIL C(CN)3–60 [C2mim][C(CN)3], which means that the presence of the [C(CN)3]− anion in the composites, either in the PIL or IL’s structure, leads to higher CO2 and H2 diffusivities compared to the [NTf2]− anion. The same trend was also observed for N2 diffusivities [38,39,41]. Thus, and as expected, it can be concluded that gas diffusivities follow the order of the kinetic diameters CO2 < N2 < H2. It can also be noted that the presence of imidazolium-based cation ([C2mim]+) in the ILs led to superior gas diffusivities compared to the pyrrolidinium-based cation ([C4mpyr]+).
Another interesting point is the comparison between gas permeability and diffusivity behaviors. Regardless of the anion, although the composite that comprised 60 wt % of IL had the highest H2 diffusivities (>1200 m2 s−1 at 308 K), it did not present the highest H2 permeabilities (Figure 2). An equivalent behavior was also obtained for the PIL NTf2–40 [C4mpyr][NTf2] composite membrane, which displayed the lowest H2 diffusivities (546 m2 s−1 at 308 K) but not the lowest H2 permeabilities. In the case of CO2, it can be seen from Table 2 and Figure 2 that CO2 permeability followed the same trend as CO2 diffusivity, with the exception of the PIL NTf2–60 [C4mpyr][NTf2] and PIL C(CN)3–40 [C2mim][C(CN)3] membranes. This behavior led us to conclude that the very high difference (three or, in some cases, four orders of magnitude) among H2 diffusivities is somehow compensated by a reverse behavior in H2 solubilities (as will be discussed in the next section), which has a significant impact on the H2 permeability results.
3.1.3. Gas Solubility (S)
Gas solubility (S) values were calculated using Equation (1) at temperatures of 293 K and 308 K and are displayed in Figure 3. The CO2 solubility decreased with increasing temperature while H2 solubility increased with increasing temperature for all the PIL–IL membranes studied. Analogous reverse H2 solubility behavior with temperature was also found and discussed by Raeissi et al.  in imidazolium-based ILs, such as [C4mim][NTf2], which means that hydrogen dissolves better at higher than at lower temperatures. This trend seems to be the general rule for H2 solubility in ILs [49,50,51,52,53] and has been attributed to the extreme lightness and small intermolecular forces of hydrogen molecules .
It can also be observed that, as expected, both CO2 and H2 solubilities were enhanced with the incorporation of high amounts of IL in the composite. For instance, when the amount of [C2mim][C(CN)3] increased from 40 to 60 wt %, the CO2 and H2 solubilities at 293 K increased almost 50% and 15%, respectively, while at 308 K the increment in CO2 and H2 solubilities was around 39% and 5%, respectively. Similar behavior was found for the PIL–IL composites comprising the [C4mpyr][NTf2] IL. Moreover, the large differences between CO2 and H2 solubilities can be explained by the high CO2 critical temperature (CO2, 31 °C; H2, −240 °C), corresponding to the superior condensability of CO2 (Tε/k = 195.2 K) compared to H2 (Tε/k = 59.7 K) [48,54]. The fact that H2 can almost be considered an ideal gas due to its small kinetic diameter and non-interacting nature, while CO2 displays a higher kinetic diameter and a quadrupole moment, also plays a role in the difference in solubilities of the two gases. For the PIL–IL composites studied in this work at 308 K, the CO2 solubility ranged from 14 to 28.5 (×10−6) m3(STP)·m−3·Pa−1 whereas the H2 solubility values were two orders of magnitude lower, varying from 0.17 to 0.51 (×10−6) m3(STP)·m−3·Pa−1. Among all the tested membranes, the PIL NTf2–60 [C4mpyr][NTf2] composite presented the highest CO2 and H2 solubilities at both 293 and 308 K. Regarding the influence of the anion’s structure and considering the same amount of free IL in the composite, it can be concluded that the presence of the [NTf2]− anion in the PIL–IL membranes leads to higher CO2 and H2 solubilities compared to those membranes comprising the [C(CN)3]− anion. As mentioned before, this behavior masks the higher H2 diffusivities of composites with a cyano-functionalized anion, somehow explaining the low influence of H2 diffusivity on the H2 permeability results.
3.2. CO2/H2 Separation Performance
The CO2 and H2 permeabilities and the ideal CO2/H2 permselectivities determined at 293 K and 308 K are summarized in Table 3. Amongst the PIL−IL membranes studied, those bearing the [C(CN)3]− anion revealed slightly higher CO2/H2 permselectivities than those containing the [NTf2]− anion. This behavior was also observed in our previous works concerning the use of PIL–IL membranes for CO2/N2 and CO2/CH4 separation [38,39,41]. Moreover, from Table 3, it can be seen that CO2/H2 permselectivities decreased with increasing temperature. This result can be explained by the variations in CO2/H2 solubility selectivity with temperature, which leads to a decrease in CO2/H2 permselectivity as the temperature increases . In fact, CO2/H2 solubility selectivity through the studied composite membranes decreased from 78–145 at 293 K to 42–84 at 308 K. It can also be emphasized that CO2/H2 permselectivity seems to be controlled by a solubility mechanism, since CO2/H2 diffusivity selectivity (D CO2/H2) values were approximately equal to 0.1 at both temperatures while solubility selectivity (S CO2/H2) values ranged from 78–145 at 293 K and 42–84 at 308 K.
The gas separation performance of the studied PIL–IL membranes is shown in Figure 4, where the CO2/H2 permselectivity is plotted against the permeability of the more permeable gas species (CO2). This graph displays a tradeoff (black line) between gas permeability and permselectivity. These upper bound limits for several gas pairs were first developed by Robeson  who correlated data obtained from measurements carried out with polymeric membranes at low temperatures (298–308 K). Later, Rowe et al.  studied the influence of temperature on the tradeoff between gas permeability and permselectivity for different gas pairs. Thus, the upper bound at 300 K developed by Rowe et al.  for the CO2/H2 gas pair is represented in Figure 4 and was used to evaluate the performance of the studied PIL–IL membranes for biohydrogen purification (T = 308 K and 100 kPa).
Figure 4 clearly shows that all the PIL–IL membranes that were studied displayed CO2/H2 separation performances above the upper bound. The best CO2/H2 separation performance was obtained for the membrane composed of poly([Pyr11][C(CN)3]) and 60 wt % of [C2mim][C(CN)3] IL, which is in agreement with what has been observed in our recent works regarding the use of PIL–IL composites for CO2/N2 separation . Literature data points for other reported PIL–IL membranes are also plotted in Figure 4 for comparison. The gas permeation measurements reported by Carlisle et al.  were performed at room temperature with a transmembrane pressure differential of 200 kPa. Also, their PIL–IL membranes were not prepared by the solvent casting method but through UV polymerization by mixing different percentages of imidazolium-based IL monomers, a cross-linking monomer, and free IL . From Figure 4, it can be seen that the PIL–IL membranes reported in the literature also present CO2/H2 separation performances above the upper bound for the CO2/H2 gas pair at 300 K, but the PIL C(CN)3–60 [C2mim][C(CN)3] membrane studied in this work still revealed superior CO2/H2 separation performance.
In this work, dense composite membranes made of pyrrolidinium-based PILs with [C(CN)3]− or [NTf2]− anions and different amounts of free IL ([C2mim][C(CN)3], [C4mpyr][NTf2] or [C2mim][NTf2]) incorporated were prepared by the solvent casting method. Their CO2 and H2 permeation properties (permeability, diffusivity, and solubility) were determined at biohydrogen production conditions (T = 308 K and 100 kPa of feed pressure) and discussed. The CO2 and H2 permeation properties were measured at T = 293 K and the effect of temperature on gas separation performance was evaluated.
The PIL–IL membranes containing the [NTf2]− anion presented the highest H2 permeability and solubility values, while the PIL–IL composites having the [C(CN)3]− anion showed the highest H2 diffusivities and CO2/H2 permselectivities. As previously reported, increments in gas permeabilities, diffusivities, and solubilities were observed with increasing temperature and amounts of IL, with the exception of H2 solubility that showed the opposite behavior with temperature compared to what occurred in CO2 solubility. Overall, all the PIL–IL membranes studied revealed similar or superior CO2/H2 separation performance compared to the few PIL–IL composites reported so far in the literature. Particularly, at 308 K, the best result was obtained through the PIL C(CN)3–60 IL C(CN)3 composite membrane (CO2 permeability of 505 Barrer and CO2/H2 selectivity of 12.5), which, as shown in our previous work, also presented remarkable results for CO2/N2 separation.
Conceptualization, L.C.T. and I.M.M.; Methodology, A.S.L.G.; Gas Separation Measurements and Membrane Preparation, L.V. and A.S.L.G.; Writing-Original Draft Preparation, A.S.L.G.; Writing-Review & Editing, A.S.L.G., L.C.T. and I.M.M.
This work was supported by FCT through the project PTDC/CTM-POL/2676/2014 and R&D units UID/QUI/00100/2013 (CQE) and UID/Multi/04551/2013 (GreenIT). This project has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie Sklodowska-Curie grant agreement No 745734.
Andreia S. L. Gouveia and Liliana C. Tomé are grateful to FCT (Fundação para a Ciência e a Tecnologia) for their Doctoral (SFRH/BD/116600/2016) and Post-doctoral (SFRH/BPD/101793/2014) research grants, respectively.
Conflicts of Interest
The authors declare no conflict of interest.
|Δpd||Variation of downstream pressure|
|Δpi||Pressure driving force|
|A||Effective membrane surface area|
|Ji||Steady-state gas flux|
|R||Ideal gas law constant|
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Figure 1. Chemical structures of the poly(ionic liquid)s (PILs) and ionic liquids (ILs) used in this work to prepare the PIL–IL membranes.
Figure 2. Experimental CO2 and H2 permeabilities (P) through the prepared PIL–IL membranes. Error bars represent standard deviations based on three experimental replicas. In some cases, the standard deviations are very small leading to error bars that cannot be clearly represented.
Figure 3. Gas solubilities (S) for the studied PIL–IL membranes at 293 K and 308 K.
Figure 4. CO2/H2 separation performance of the PIL–IL membranes studied. The experimental error is within the data points. Data are plotted on a log–log scale and the upper bound at 300 K was adapted from Rowe et al. . Literature data points ( ) from other reported PIL–IL membranes are also displayed for comparison .
Table 1. Description of the poly(ionic liquid)–ionic liquid (PIL–IL) membrane’s composition and experimental preparation conditions of the solvent casting procedure.
|PIL–IL Membrane||Polymer (PIL)||wt % of IL||Solvent||T (K)||Evaporation Time (Days)|
|PIL C(CN)3–40 [C2mim][C(CN)3]||Poly([Pyr11][C(CN)3])||40||Acetonitrile||298||3|
|PIL C(CN)3–60 [C2mim][C(CN)3]||60|
|PIL NTf2–40 [C4mpyr][NTf2]||Poly([Pyr11][NTf2])||40||Acetone||298||2|
|PIL NTf2–60 [C4mpyr][NTf2]||60|
|PIL NTf2–40 [C2mim][NTf2]||Poly([Pyr11][NTf2])||40||Acetone||298||2|
Table 2. Experimental gas diffusivities (D) through the studied PIL–IL membranes at T = 293 K and T = 308 K.
|PIL–IL Membrane||Gas Diffusivity (×1012) (m2 s−1) (T = 293 K)||Gas Diffusivity (×1012) (m2 s−1) (T = 308 K)|
|D CO2 ± σ||D H2 ± σ||D CO2 ± σ||D H2 ± σ|
|PIL C(CN)3–40 [C2mim][C(CN)3]||64 ± 1.0||970 ± 36.2||112 ± 2.5||1146 ± 34.0|
|PIL C(CN)3–60 [C2mim][C(CN)3]||127 ± 1.1||1130 ± 5.70||181 ± 0.6||1211 ± 3.2|
|PIL NTf2–40 [C4mpyr][NTf2]||34 ± 0.1||484 ± 18.5||62 ± 1.8||546 ± 20.6|
|PIL NTf2–60 [C4mpyr][NTf2]||44 ± 0.7||610 ± 6.30||76 ± 0.5||673 ± 16.9|
|PIL NTf2–40 [C2mim][NTf2]||61 ± 0.4||722 ± 1.80||106 ± 1.5||792 ± 3.70|
Table 3. Single gas permeabilities (P) a and ideal permselectivities (α) of the PIL–IL membranes studied b.
|PIL–IL Membrane||Gas Permeability (Barrer)|
(T = 293 K)
|Gas Permeability (Barrer)|
(T = 308 K)
|P CO2 ± σ||P H2 ± σ||α CO2/H2||P CO2 ± σ||P H2 ± σ||α CO2/H2|
|PIL C(CN)3–40 [C2mim][C(CN)3]||139 ± 0.5||14.5 ± 0.2||9.6 ± 0.2||209 ± 0.9||25.7 ± 0.1||8.1 ± 0.1|
|PIL C(CN)3–60 [C2mim][C(CN)3]||438 ± 2.1||29.1 ± 0.4||15.1 ± 0.3||505 ± 0.3||40.3 ± 1.1||12.5 ± 0.3|
|PIL NTf2–40 [C4mpyr][NTf2]||119 ± 0.2||21.9 ± 0.1||5.4 ± 0.1||164 ± 1.6||34.4 ± 0.3||4.8 ± 0.1|
|PIL NTf2–60 [C4mpyr][NTf2]||232 ± 2.2||29.8 ± 0.1||7.8 ± 0.1||288 ± 1.6||46.0 ± 0.1||6.3 ± 0.1|
|PIL NTf2–40 [C2mim][NTf2]||214 ± 0.6||26.2 ± 0.1||8.2 ± 0.1||287 ± 2.4||43.8 ± 0.2||6.5 ± 0.1|
a Barrer (1 Barrer = 10−10 cm(STP)3·cm·cm−2·s−1·cm·Hg−1). b The listed uncertainties represent the standard deviations (σ) based on three experiments.
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