Structure–function study of tertiary amines as switchable polarity solvents

Aaron D. Wilson* and Frederick F. Stewart
Idaho National Laboratory, P.O. Box 1625 MS 2208, Idaho Falls, ID 83415-2208, USA. E-mail: aaron.wilson@inl.gov; Fax: +(208)-526-8511; Tel: +(208)-526-1103

Received 17th December 2013 , Accepted 31st January 2014

First published on 3rd February 2014


Abstract

A series of tertiary amines have been screened for their function as switchable polarity solvents (SPS). The relative ratios of tertiary amine and carbonate species as well as maximum possible concentration were determined through quantitative 1H and 13C NMR spectroscopy. The viscosities of the polar SPS solutions were measured and ranged from near water in dilute systems through to gel formation at high concentrations. The van't Hoff indices for SPS solutions were measured through freezing point depression studies as a proxy for osmotic pressures. A new form of SPS with an amine[thin space (1/6-em)]:[thin space (1/6-em)]carbonate ratio significantly greater than unity has been identified. Tertiary amines that function as SPS at ambient pressures appear to be limited to molecules with fewer than 12 carbons. The N,N-dimethyl-n-alkylamine structure has been identified as important to the function of an SPS.


Introduction

Developing safe, energy efficient, and environmentally friendly alternatives to traditional solvent systems is a primary goal of “green” and sustainable chemistry research.1 These goals can be achieved by reducing solvent volumes, changing processes to function with more benign solvents, or developing alternative solvents with new behaviors that allow better process lifecycle performance. Advances in alternative solvents are expected to improve conventional solvent process such as oil extraction from biomass, as well as non-standard uses of solvents. Novel “solvent” materials will allow the development of new processes in areas such as CO2 separations, water purification, and energy storage. Among the most well-known and promising alternative solvents are the various room-temperature ionic liquids, supercritical fluids, and switchable polarity solvents (SPSs) explored in this study.

SPSs can be divided into various subcategories based on composition and behavior.2–5 This study targeted water-compatible single-component SPSs which are immiscible with water in their basic form but when they are reacted with carbonic acid, derived from exposure to ∼1 atm carbon dioxide, the water miscible acid form [H+(base) HCO3] of the SPS is produced, reaction (1). Similar behavior can be obtained from dual component SPSs involving a nitrogen base (amidines and guanidines) and an alcohol or primary amine; but such systems require balanced stoichiometry to function correctly and tend to be water sensitive which makes them unattractive for many applications.2,6–8 Some single component SPS, such as secondary amines, also suffer water sensitivity in the form of material precipitation at relatively low water concentrations and thus are ignored in this study.9 Known water-compatible single-component SPSs include highly functionalized amidines and guanidines,4 tertiary amines,5 and pH sensitive ionic liquids;10 the scope of research was further focused to tertiary amines based on their potential cost effectiveness when produced at large scale.

 
NR3(org) + CO2(gas) + H2O ⇌ HNR3+(aq) + HCO3 (1)

Our laboratory became interested in SPS for their use as thermolytic draw solutes11 (versus more conventional non-thermolytic draw solutes12,13) in osmotically driven membrane processes (ODMPs). As thermolytic solutes, SPS can be used in water purification through forward osmosis (FO),14 solution concentration through direct osmotic concentration,15 and for osmotic heat engines through pressure retarded osmosis.16 Since its introduction in 2006, the ammonia–CO2 system has been considered one of the more viable next generation draw solute for FO.17 SPS draw solutes have a number of advantages over the ammonia–CO2 system; including negating the need to handle and store gaseous ammonia, lower permeability to properly selected membranes, lower energy requirements, and facile removal of SPS from water through liquid phase separation.

Tertiary amines, such as those screened in this publication, long have been considered unlikely candidates for carbon capture or natural gas sweetening. Primary and secondary amines react chemically with carbon dioxide rapidly to form carbamates.18 Tertiary amines, on the other hand, follow a second route in which carbon dioxide forms carbonic acid and then reacts via an acid–base reaction with the amine.18 The carbonic acid pathway is generally slower due to the rate of carbonic acid formation. However, tertiary amines and mixtures which include tertiary amines have recently been reported for carbon capture in conjunction with phase change processes.19–37 Amines included in our study have also been investigated by Zhang as carbon capture agents where he refers to them as biphasic or lipophilic amine solvents.19–22 A phase change carbon capture system, DMX™, has been developed by IFP Energies nouvelles; however the chemical composition of their formulation was not available to us.23,24 Heldebrant is exploring performance of single-component CO2-binding organic liquids (CO2BOLs).25–28 Hu of 3H Company has reported a two phase acid capture system involving a polarity switching amine.29–33 Eckert has worked with a switchable polarity ionic liquid.34–37

There have been various publications addressing the use of SPS for processing, extraction, and separation. This includes plastic recycling,5 extraction of oils from biomass and microbes,38–42 activation of recalcitrant biomass,43 and the use of SPS as a chemical synthesis solvent.2,44 The use of SPS in these applications has similarities to distillable room temperature ionic liquids (RTIL) which are often comprised of amines and carboxylic acids.45–48 There is also the well-established use of ammonium carbamate and carbonate salts as polyurethane polymerization catalysts.49

Each of the potential applications can benefit from achieving a higher concentration of the SPS polar form, [HNR3+ HCO3]; however, how the concentration is considered best depends on the application. In the case of FO, the osmotic strength of the draw solute is the thermodynamic driving force for the water transport process and is best measured by molality.50 In solvent extraction, the osmotic pressure is less important than the volume of non-aqueous amine contained within the SPS polar form. A solution with a high weight percent (wt%) of [HNR3+] allows the solution volumes used in the solvent extraction process to be minimized. In a carbon capture system, the SPS carbon capture agent would ideally have an extremely large capacity for carbon dioxide and the ideal unit is wt% of CO2. The most serious drawback of high concentration solutions is increased viscosity which may be problematic for many applications.

Theoretical treatments of high concentration solutions are usually modeled through activity, as. Activity (as = ysxs) is a product of the mole fraction, (xs, moles solute per total moles solvent and solute), and a dimensionless empirically based activity coefficient, ys. Thus, the mole fraction, xs, was also considered when looking for concentration trends.

Previous to this study, the information concerning the maximum concentration of amine based SPS in their polar form was limited to N,N-dimethylcyclohexylamine (5) and N,N,N′-tributylpentanamidine.4,5 Tertiary amines are among the most attractive SPS reported so far due to their simplicity and low cost. These advantages motivated the screening of tertiary amines 1–26 for a variety of physical properties similar to the study recently published by Eckert.36 This screening has identified a new form of SPS, as well as structural features and limitations of tertiary amines that are fundamental to their performance as SPS.

Results and discussion

Due to the fact that many SPS applications would benefit from higher SPS concentrations in the polar form, the maximum concentration was characterized for a series of tertiary amines, 1–26. This series was selected not because each amine was expected to be a top performer but rather they are representative of many small tertiary amines with features such as rings systems, different length carbon chains relative to the nitrogen, and alkyl chain branching. These representative amines were selected not only to set limits on the maximum and minimum number of carbons in a functional SPS but also to determine how structural features affect that function. The set of amines included the re-visitation of 12 tertiary amines that had been previously studied for SPS behavior, confirming that 8 amines transition from a water immiscible state to a water miscible state with the introduction of CO2 and thus “function” as SPS.5 In addition, 14 previously unreported amines were investigated for SPS behavior and, of these, 8 additional amines have been identified to function as SPS. The structures of the amines that functioned as SPS are illustrated in Fig. 1 and those that did not measurably function as SPS under our experimental conditions are illustrated in Fig. 2.
image file: c3ra47724j-f1.tif
Fig. 1 Structures of tertiary amines that functioned as SPS.

image file: c3ra47724j-f2.tif
Fig. 2 Structures of tertiary amines that did not function as SPS.

While a variety of properties were recorded including viscosity, density, and freezing point depression; it was the NMR spectroscopic studies that were of primary importance where it was used to measure both concentration and composition of SPS solutions. The procedure to identify the maximum concentration involved combining known quantities of water and tertiary amine and purging the solution with carbon dioxide at ambient pressure. The volume of the amine that did not react to form the polar water soluble SPS was measured and a tentative maximum solution concentration was calculated based on the initial masses and unreacted volume. This volume derived concentration measurement was used to corroborate the concentrations found through quantitative NMR studies of the polar SPS solutions.

The NMR studies also were used to identify composition characteristics of the polar SPS solutions. This compositional data indicated that the assumption featured in eqn (1) that all SPS form in a ratio of one tertiary amine to one carbonic acid is incorrect. There are two types of SPS whose primary compositional difference is in the amine[thin space (1/6-em)]:[thin space (1/6-em)]H2CO3 ratio.

Osmotic SPS

An SPS that can produce an osmotic driven flux across a semi-permeable membrane can be considered “osmotic”. Osmotic SPS amines are characterized by a maximum concentration of their polar SPS form, after which additional amine is rejected by the aqueous phase and remains separated in a nonpolar phase, even in the presence of excess ambient pressure carbon dioxide. Osmotic SPS systems remain fully liquid under all the experimental conditions and no precipitate is observed; although clouding is common during the switching process. Osmotic SPS can be diluted with water and display predictable decreases in osmotic pressure. Correlation between osmolality and molality produces representative van't Hoff indices. To accurately measure the maximum concentration of these SPS, quantitative NMR spectroscopy was conducted.

The quantitative 13C and 1H NMR spectra were conducted as neat solutions with a coaxial insert containing C6D6 as a reference. As examples, Fig. 3 and 4 feature the spectra for solution 5′. The 1H NMR spectrum contains chemical shifts, δ, which have been assigned to the exchangeable protons of water (H2O), carbonates (HCO3 and H2CO3), and ammonium (H+NR3) ions, Fig. 4. The analysis of this data can be simplified by ascribing two protons to carbonic acid and its salts. Based on 1H NMR spectrum integration, the ratio of water and carbonic acid to amine can be calculated. This ratio combined with the amine to carbonic acid ratio derived from the quantitative 13C NMR, Fig. 3, allow for the calculation of the relative mole ratio of amine[thin space (1/6-em)]:[thin space (1/6-em)]carbonic acid[thin space (1/6-em)]:[thin space (1/6-em)]water. With the molecular mass and solution density it is possible to calculate mole fractions, molarities, molalities, and weight percent (Table 1), all of which were considered in looking for trends associated with physical properties (Table 2).


image file: c3ra47724j-f3.tif
Fig. 3 The quantitative 13C NMR of dimethylcyclohexylamine bicarbonate solution 5′.

image file: c3ra47724j-f4.tif
Fig. 4 The quantitative 1H NMR of dimethylcyclohexylamine bicarbonate solution 5′.
Table 1 The relative integration of quantitative NMR select properties and concentrations of tertiary amine bicarbonate solutions
Amine Number Molecular mass (amine) Density (solution) Amine[thin space (1/6-em)]:[thin space (1/6-em)]H2CO3 (13C) (H2O + H2CO3)[thin space (1/6-em)]:[thin space (1/6-em)]amine (1H) wt% (amine + H2CO3) Mole fraction (amine) Molal (amine) Molarity (amine)
Dimethylbutylamine 1′ 101.2 1.05 1.06 5.13 67.9 0.163 13.3 4.47
Triethylamine 2′ 101.2 1.05 1.05 9.46 51.1 0.096 6.52 3.35
1-Ethylpiperidine 3′ 113.2 1.09 1.05 4.93 70.6 0.169 14.0 4.47
Methyldipropylamine 4′ 115.2 1.01 1.07 25.8 27.9 0.037 2.23 1.63
Dimethylcyclohexylamine 5′ 127.2 1.10 1.05 4.03 77.0 0.199 18.0 4.55
Dimethylhexylamine 6′ 129.2 0.98 1.23 6.40 64.1 0.135 9.94 3.50
1-Butylpyrrolidine 7′ 127.2 0.99 1.26 6.44 63.4 0.134 9.84 3.56
Diethylbutylamine 8′ 129.2 1.02 1.09 19.2 36.1 0.050 3.04 1.98
Dimethylbenzylamine 9′ 135.2 1.05 1.14 23.4 31.9 0.041 2.47 1.77
Methyldibutylamine 10′ 143.3 1.00 1.14 88.8 11.1 0.011 0.63 0.56
Dimethylphenethylamine 11′ 149.2 1.03 2.42 4.45 70.6 0.184 13.8 4.16
Dimethyloctylamine 12′ 157.3 0.92 1.91 5.97 65.9 0.143 10.2 3.20
Diethylcyclohexylamine 13′ 155.3 1.04 1.02 23.5 34.8 0.041 2.47 1.67
Dimethyl-2-ethylhexylamine 14′ 157.2 1.00 1.05 508 2.3 0.002 0.11 0.11
Dimethylnonylamine 15′ 171.3 0.88 2.70 5.73 66.8 0.149 10.4 3.03
Dimethyldecylamine 16′ 185.4 2.87 7.54 61.5 0.117 7.72 2.97


Table 2 The properties of tertiary amines bicarbonate solutions
Amine Number Carbon[thin space (1/6-em)]:[thin space (1/6-em)]nitrogen Density (amine) wt% (amine + H2CO3) Density (solution) Amine[thin space (1/6-em)]:[thin space (1/6-em)]H2CO3 (13C) van't Hoff index (amine) van't Hoff index (Σ ions) Max. osmotic pressure (atm) Viscosity (cP)
a Based on amine concentration <1.05 mol kg−1.
Dimethylbutylamine 1′ 6 0.721 67.9 1.05 1.06 1.81 0.93 616 25.0
Triethylamine 2′ 6 0.726 51.1 1.05 1.05 1.73 0.88 288 10.6
1-Ethylpiperidine 3′ 7 0.824 70.6 1.09 1.05 1.72 0.88 641 71
Methyldipropylamine 4′ 7 0.734 27.9 1.01 1.07 1.69 0.87 92.9 2.8
Dimethylcyclohexylamine 5′ 8 0.849 77.0 1.10 1.05 1.73 0.88 835 108
Dimethylhexylamine 6′ 8 0.744 64.1 0.98 1.23 1.37 0.76 328 25.5
1-Butylpyrrolidine 7′ 8 0.814 63.4 0.99 1.26 1.36a 0.76a 325a 29
Diethylbutylamine 8′ 8 0.748 36.1 1.02 1.09 1.79 0.93 135 11.3
Dimethylbenzylamine 9′ 9 0.900 31.9 1.05 1.14 1.37 0.73 87.1 2.8
Methyldibutylamine 10′ 9 0.745 11.1 1.00 1.14 1.77 0.94 27.3 1.6
Dimethylphenethylamine 11′ 10 0.89 70.6 1.03 2.42 15.0
Dimethyloctylamine 12′ 10 0.765 65.9 0.92 1.91 58
Diethylcyclohexylamine 13′ 10 0.845 34.8 1.04 1.02 1.82 0.92 114 4.8
Dimethyl-2-ethylhexylamine 14′ 10 0.768 2.3 1.00 1.05 1.1
Dimethylnonylamine 15′ 11 0.773 66.8 0.88 2.70 86
Dimethyldecylamine 16′ 12 0.778 61.5 2.87 Gel


The concentrations calculated from quantitative 13C and 1H NMR spectra studies allow the calculation of van't Hoff indices based on either the sum of tertiary amine/ammonium molality or the total species molality, which includes tertiary amines, tertiary ammonium, and carbonate species, Table 2. The total species molality is more informative as it removes the variation in the relative carbonate concentration and is more directly related to the ion dissociation. The degree of dissociation cannot be perfectly gauged because these indices are composites of various forms of “ion pairing”, which reduce the van't Hoff index, and the role of “bound” waters of hydration, which raise the indices.50,51 Freezing point depression studies were conducted to obtain experimental van't Hoff indices which allow estimation of osmotic pressure, Table 2.50 The van't Hoff indices were based on values measured generally between 0.10 and 2.0 Osm per kg, such as Fig. 5.


image file: c3ra47724j-f5.tif
Fig. 5 The van't Hoff plot for diethylcyclohexylamine, 13′. The diamonds are based on molality of tertiary amine and tertiary ammonium ions. The squares are based on the total species molality including tertiary amines, tertiary ammonium ions, and carbonate species.

The correlation over the 0.10 Osm per kg to 2.0 Osm per kg range, as measured by freezing point depression, was generally linear where total species van't Hoff indices ranged between 0.73 and 0.94 (Table 2) for osmotic SPS, indicating high degrees of dissociation for nearly all the solutions measured. One example that did not follow this trend is solution 7′, which deviated negatively from linearity when the amine concentration exceeded 1 mol kg−1, Fig. 6, suggesting higher order “ion pairing” equilibrium processes. No other solutions deviated from linearity, but solution 8′ would not freeze cleanly at or above 1.2 mol kg−1 of amine, which may be a result solution out gassing or exceeding a eutectic point.


image file: c3ra47724j-f6.tif
Fig. 6 The van't Hoff plot for diethylcyclohexylamine, 7′. The diamonds are based on molality of tertiary amine and tertiary ammonium ions. The squares are based on the total species molality including tertiary amines, tertiary ammonium ions, and carbonate species. Only the filled-marker data was used to calculate the trend lines. The higher concentration open-marker data feature a negative deviation from linearity.

It was previously reported that 5 forms a solution in a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 (v/v) ratio with water which our lab reported as a viable ODMP draw solute.11 The maximum concentration of 5′ was revisited and was found to have a maximum concentration of 77 wt%, which corresponds to 18 molal and 4.6 M by amine. This concentration is considerably higher than the value previously reported. The osmotic pressure of solution 5′ has been estimated at 836 atm based on previously described methods,50 which is considerable for an FO draw solute.

Non-osmotic SPS

Osmotic SPS were not the only SPS form encountered in this study; there were also “non-osmotic” SPS which differed in both composition and behavior. These SPS are coined “non-osmotic” because they did not produce the expected osmotic driven flux across a semi-permeable membrane when used as a FO draw solution in their “polar” form. The van 't Hoff indices of non-osmotic SPS could not be measured because the solutions do not dilute homogenously when water is added. All measured freezing points were much lower than expected given the concentration. For these reasons Table 2 does not contain a maximum osmotic pressure for non-osmotic SPS. This is an unexpected result for a solution made from the addition of carbon dioxide and tertiary amine to water. When water is added to a concentrated non-osmotic SPS, a portion of the solution dilutes, and is reflected in freezing point osmometry measurements, but another portion phase separates as the nonpolar tertiary amine. To understand this dilution phenomenon, the relative concentrations of the species in solution must be known. The solutions are comprised of amines species, both protonated and unprotonated, and carbonate species, which is mostly bicarbonate with equilibrium quantities of carbonate and carbonic acid. Because of the complexity involved with tracking the equilibrium concentration, it is useful to consider this acid–base system in its non-ionized form to compare the “amine” to “carbonic acid” ratios. The ratio of tertiary amine to carbonic acid for non-osmotic SPS varies between 1.82 and 2.87 based on the integration of the quantitative 13C NMR spectra. These values for non-osmotic SPS are significantly higher than polar SPS with all values listed in Tables 1 and 2 and plotted in Fig. 7.
image file: c3ra47724j-f7.tif
Fig. 7 The NR3[thin space (1/6-em)]:[thin space (1/6-em)]H2CO3 ratio represents the ratio between all forms of amine protonated and unprotonated and the sum of carbonate, bicarbonate, and carbonic acid; diamonds represent “osmotic” SPS, crosses represent “non-osmotic” SPS.

Modeling the maximum concentration equilibrium

Due to the discovery of non-osmotic SPS, the model SPS maximum concentration must be revisited. Since the organic amine is an immiscible material, its concentration does not change with the equilibria and thus can be taken as unity. Likewise the solvent, in this case water, is usually in a large excess such that its effective concentration does not change with the equilibrium and usually can also be treated as unity. Assuming the solvent as unity is not strictly proper for the SPS equilibria where the water concentration drops below 0.8 mole fraction and may also be involved in ionic hydration. Thus, the water concentration is included in this equilibrium. Because these are non-aqueous solutions of variable consistency, there are no known Henry's law constants for these systems. Thus, the CO2 concentration is not calculated based on the partial pressure. In addition, because CO2 partial pressure is the independent variable, it is preferred for the calculation of an equilibrium constant.52 These assumptions yield the equilibrium expression, eqn (3), from the reaction described by eqn (2).
 
NR3(org) + CO2(pressure) + H2O ⇌ HNR3+(aq) + HCO3 (2)
 
image file: c3ra47724j-t1.tif(3)
 
NR3(org) ⇌ NR3(aq) (4)
 
NR3(aq) + CO2(pressure) + H2O ⇌ HNR3+(aq) + HCO3 (5)
 
a[HNR3+(aq) + NR3(aq)] + NR3(org) ⇌ NR3(aq) + bH2O (6)
 
image file: c3ra47724j-t2.tif(7)

Non-osmotic SPS concentrations are not as simple as they can be modeled multiple ways. Because there are appreciable amounts of aqueous tertiary amine in non-osmotic SPS, the model needs to consider the conversion of organic tertiary amine to aqueous tertiary amine (eqn (4)). When aqueous tertiary amine is considered directly, eqn (2) is converted into eqn (5). As the aqueous tertiary amine and aqueous tertiary ammonium bicarbonate concentrations increase, the concentration of dissolved organic materials increases. This results in a solution polarity decrease, which shifts the solution towards something more like a water immiscible organic solvent. This shift in polarity allows the solution to accept more tertiary amine (eqn (6)). In this model, we assume HNR3+ and NR3 contribute equally to the polarity shift for the sake of simplicity. Presumably, the increase in aqueous amine when the products are favored in eqn (4) allows the further conversion of carbon dioxide into bicarbonate and protonated tertiary amine (eqn (5)) in a positive feedback loop. This feedback loop does two things: (1) increases the carbonate concentration relative to the osmotic SPS and (2) increases the absolute concentration of HNR3+(aq) and HCO3. The relative concentration of NR3(aq) also increases and the solution moves further away from a composition that is strictly aqueous. If water is added to a concentrated non-osmotic SPS solution, a portion of the NR3(aq) phase separates as the SPS solution polarity is driven to a more polar form. The ability of water to shift the polarity of the solution is featured in its role as a product dependent on the value “b” in eqn (6). The role of water is complex and it may be necessary to identify portions as “free” or “bound” in the SPS solution, but the treatment in eqn (5) and (6) is sufficient to model the current information yielding an equilibrium expression, eqn (7).

Limits of SPS function at ambient pressure and concerns with measurements

The number of carbons or the carbon[thin space (1/6-em)]:[thin space (1/6-em)]nitrogen (C[thin space (1/6-em)]:[thin space (1/6-em)]N) ratio of a tertiary amine is a useful proxy for both the mass and polarity of the tertiary amine; more carbons in the amine result in higher molecular mass, and thus lower overall polarity. Hansen solubility parameters and its components were explored to describe tertiary amine polarity without success; the calculated parameters varied little and were less intuitive than the simple C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio.

In this study, no tertiary amines with a C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio of less than 6 were explored. Tertiary amines with low C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio have many undesirable characteristics including low boiling points, high vapor pressures, higher water solubility, and a more difficult switch between the nonpolar and polar phases. Release of CO2 for these amines generally requires substantially higher temperatures or greater volumes of purge gas, followed by cryogenic amine capture, which complicates their utility. These factors serve to limit the use of these amines as SPS and motivates the efforts to define the proper upper thresholds of the C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio for tertiary amines that function as SPS.

When the total weight percent of both osmotic SPS (C[thin space (1/6-em)]:[thin space (1/6-em)]N 6–10) and non-osmotic SPS (C[thin space (1/6-em)]:[thin space (1/6-em)]N 10–12) are plotted against C[thin space (1/6-em)]:[thin space (1/6-em)]N their ratio, high weight percentages are found until C[thin space (1/6-em)]:[thin space (1/6-em)]N 12 after which no tertiary amines were found to form SPS, Fig. 8. The loss of SPS formation above C[thin space (1/6-em)]:[thin space (1/6-em)]N = 12 may be explained when the concentration is broken into the tertiary amine and the carbonate concentration. For example, focusing on the N,N-dimethyl-n-alkylamine series, Fig. 9, it is clear that the carbonate concentration steadily decreases from C[thin space (1/6-em)]:[thin space (1/6-em)]N 6 to 11. Solution 16′ is excluded from this analysis because it forms a gel distinct from the other liquid solutions. A trend line can be fitted to the carbonate concentrations of the N,N-dimethyl-n-alkylamine series, which includes osmotic SPS (1′ and 6′) and non-osmotic SPS (12′ and 15′) that indicates increasing the C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio results in a decline in the carbonate concentration. Because osmotic and non-osmotic systems are linear when the C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio is plotted against carbonate molarity, this is convenient trend for comparing all SPS systems. The linearity of the trend also could be taken to suggest that concentration phenomena influence the maximum concentrations of both osmotic and non-osmotic SPS in a similar way, rendering the previous equilibrium analysis (eqn (4)–(7)) unnecessary. Such a conclusion does acknowledge that while the C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio is a useful proxy for polarity and molecular mass, it is not a fundamental physical property commonly used to compare equilibrium states and thus, in many ways, an arbitrary unit, making the resulting trend similarly arbitrary.


image file: c3ra47724j-f8.tif
Fig. 8 Maximum acquired concentration as a function of the C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio.

image file: c3ra47724j-f9.tif
Fig. 9 Maximum acquired concentration as a function of the C[thin space (1/6-em)]:[thin space (1/6-em)]N at 1 atm CO2 for SPSs featuring the N,N-dimethyl-n-alkylamine structure plotted in molarity for both the amine (solid diamond) and carbonate components (open diamond).

The observed trend in Fig. 9 is a product of known theoretical and experimental influences. The slope of the regression might be steeper or fit a different mathematical/concentration model if not for three phenomena. First, as discussed earlier, there is a positive feedback loop associated with non-osmotic SPS and their elevated concentration of aqueous amine. This raises the concentration of carbonate in solution for 12′ and 15′ (and 16′) which define the low end of the trend. The second feature is the home-built experimental apparatus for this study pushed carbon dioxide through a column of solution which was then exhausted through a condenser open to the atmosphere through a needle, as shown in the experimental section. For lower viscosity amines, the CO2 pressure rapidly equilibrated with ambient pressure; however, the amines with viscosities greater than 50 cP (Table 2), namely 3′, 5′, 12′, and 15′ (and 16′) provide back pressure on the carbon dioxide flow slightly elevating the CO2 pressures directed at the solution.

The third phenomenon that affects the trend observed in Fig. 9 is the stability of the solutions. Not all solutions are stable for significant periods of time. Solutions 11′ and 15′ (and 16′) are prone to venting carbon dioxide when mild pressure or vacuum is applied or even mixing in the absence of a saturated carbon dioxide atmosphere. When conducting NMR experiments, approximately 20% of solutions 11′ and 15′ (and 16′) phase separated into the nonpolar amine form, suggesting they may be metastable supersaturated states.

Each of these three phenomena tend to inflate the observed concentration at high C[thin space (1/6-em)]:[thin space (1/6-em)]N ratios. Because two of these phenomena are related to the experimental process and design, the conclusions and performance trends regarding high C[thin space (1/6-em)]:[thin space (1/6-em)]N ratios and the upper threshold for tertiary amine function as SPS may be generous.

Structural features of SPS

Within the range of C[thin space (1/6-em)]:[thin space (1/6-em)]N ratios between 6 and 12 there are structural features that influences SPS performance. Better performing SPS are those that can reach the highest concentrations. Of the better performing SPS, it was noted that every example featured the core structure of N,N-dimethyl-R-amine (1′, 5′, 9′, 11′, and 15′), or 1-alkylpiperidine (3′). The N,N-dimethyl-R-amine grouping can be broken down into N,N-dimethyl-n-alkylamines (1′ and 15′), N,N-dimethylcyclohexylamine (5′), and N,N-dimethylphenealkylamines (9′ and 11′). Because the pKas of the studied tertiary amines are largely equivalent, it is assumed that an aspect of either or both polarity and intramolecular steric interaction are dictating the differences in the observed SPS performance.

There are many methods to model steric and polar interactions. Tolman cone angles have been used extensively to model the sterics influences of tertiary phosphines on their interactions with Lewis acid metal centers.53–55 While Tolman cone angles have not been used to describe amines, the phosphine values were used to conduct an evaluation that, while internally consistent, was ultimately unsuccessful. A functional group contribution model similar to the Hansen system, but dedicated to the tertiary amine SPS concentration model, is proposed below.

At the core of the functional group contribution treatment is the linear relationship between C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio and the maximum molarity of the HCO3 and HNR3+ concentrations in the N,N-dimethyl-n-alkylamine series, which holds for the alkyl = butyl (1′), hexyl (6′), octyl (12′), nonyl (15′) series. Amines which deviate from the N,N-dimethyl-n-alkylamine skeletal structure can be grouped into two overlapping groups. The first group of amine structures all contain carbons extending the core N,N-dimethyl-n-alkylamine structure but with no ring systems. For example, these carbons would include both carbons of dimethyl-2-ethylhexylamine’s, 14′, ethyl group or 1 carbon from each of the ethyl groups in diethylbutylamine, 8′, Fig. 10. The structures of these are amines and their pertinent carbons are labeled as (<) in Fig. 10 because their concentration are lower than predicted by the N,N-dimethyl-n-alkylamine trend.


image file: c3ra47724j-f10.tif
Fig. 10 The amines which deviate from the N,N-dimethyl-n-alkylamine core structure with β, γ, and δ carbons as well as α rings systems labeled and separated into groups according to whether their carbonate concentration are greater than (>), equal to (=), or less than (<) the trend line formed from the carbonate concentration of the N,N-dimethyl-n-alkylamine solutions (Fig. 9).

The concentrations of ring free systems in relation to N,N-dimethyl-n-alkylamine trend line are also plotted in Fig. 11. The second group is tertiary amines whose structures include a ring system such as a cyclohexyl group (5′ and 13′), phenyl group (9′ and 11′), piperidine (3′), and pyrrolidine (7′). The structure of ring containing systems are also included in Fig. 10 and are labeled as (<, =, and >) because their concentrations vary compared to what is predicted by the N,N-dimethyl-n-alkylamine trend. The maximum concentrations of ring containing systems in relation to N,N-dimethyl-n-alkylamine trend line are plotted in Fig. 12.


image file: c3ra47724j-f11.tif
Fig. 11 Maximum acquired concentration for SPSs featuring additional carbons functionality in addition to the N,N-dimethyl-n-alkylamine core structure. Trend line based on the N,N-dimethyl-n-alkylamine series from Fig. 9 included here for a reference. The conditions and labeling are the same as Fig. 9.

image file: c3ra47724j-f12.tif
Fig. 12 Maximum acquired concentration for SPSs featuring ring systems. Trend line based on the N,N-dimethyl-n-alkylamine series from Fig. 9 included here for a reference. The conditions and labeling are the same as Fig. 9.

Alkyl substituents in the absence of a ring system reduce a tertiary amine's effectiveness as an SPS. These carbons can be described as β, γ, and δ carbons, each with a different ability to influence steric crowding at nitrogen, Fig. 13. The β, γ, and δ carbons have the potential to sterically disrupt the space around the nitrogen's lone pair to differing degrees. Such steric hindrance does not inherently prevent the coordination of a proton, due to its small size. Most of the amines in this study readily form highly concentrated protic ionic liquids with strong acids. Carbonic acid, derived form carbon dioxide, is neither a strong acid nor a concentrated acid under ambient conditions. The steric hindrance around the nitrogen lone pair likely prevents formation of extended solvent and counter ion (bicarbonate) network necessary to stabilize the polar form of the SPS in the aqueous phase.


image file: c3ra47724j-f13.tif
Fig. 13 Position of β, γ, and δ carbons with respect to the nitrogen.

The potential for maximum steric interaction increases with the carbon's proximity from the nitrogen, δ > γ > β. In contrast rotational degrees of freedom have the opposite effect based on as the carbon's potential to relax away from the amine which also increases according to the carbon's proximity from the nitrogen, δ > γ > β.

The coefficients used in eqn (8) were produced by empirically adjusting the values to produce a one to one linear relationship between the experimental and calculated molar concentrations, Table 3 and Fig. 14. Based on the structures and concentrations observed in this study, the steric effect on the carbonate concentration of a γ (1.1) carbon is approximately double the effect of a β (0.55) or δ (0.5) carbon. It is expected that more distant carbons would have little effect on the nitrogen.

 
SPS(H2CO3(M)) = 7.86 − 0.62(Σ carbon) − 0.55β − 1.1γ − 0.5δ + 1.2(α ring) (8)

Table 3 Properties of tertiary amines that functioned as SPS
Amine Number Number of total carbon β carbons γ carbons δ carbons α ring systems Molar (exp.) Molar (calc.) Absolute difference
Dimethylbutylamine 1′ 6         4.21 4.15 0.06
Triethylamine 2′ 6 2       3.19 3.05 0.14
1-Ethylpiperidine 3′ 7 2     1 4.26 3.63 0.63
Methyldipropylamine 4′ 7 1 1     1.52 1.88 0.36
Dimethylcyclohexylamine 5′ 8 1     1 3.33 3.56 0.23
Dimethylhexylamine 6′ 8         2.84 2.91 0.07
1-Butylpyrrolidine 7′ 8 2     1 2.83 3.01 0.18
Diethylbutylamine 8′ 8 2       1.82 1.81 0.01
Dimethylbenzylamine 9′ 9   1     1.55 1.19 0.36
Methyldibutylamine 10′ 9 1 1 1   0.49 0.14 0.35
Dimethylphenethylamine 11′ 10         1.72 1.67 0.05
Dimethyloctylamine 12′ 10         1.67 1.67 0.00
Diethylcyclohexylamine 13′ 10 3     1 1.64 1.22 0.42
Dimethyl-2-ethylhexylamine 14′ 10   1 1   0.10 0.07 0.03
Dimethylnonylamine 15′ 11         1.12 1.05 0.07



image file: c3ra47724j-f14.tif
Fig. 14 The correlation between the observed maximum molarity of SPS and those calculated from eqn (8).

The effects of a ring system on tertiary amines SPS function is more ambiguous than the argument presented above. All of the systems containing carbons beyond N,N-dimethyl-n-alkylamine skeleton but no ring system performed more poorly than the N,N-dimethyl-n-alkylamine series. Of the systems that contained ring systems and additional carbons some performed better than the N,N-dimethyl-n-alkylamine series, including 3′ and 5′, but not all ring containing systems performed better. Solutions 7′ and 13′ have concentrations that are much higher than expected, lying on the line for the N,N-dimethyl-n-alkylamine series despite each containing two additional β carbons. Solution 11′ essentially lies on N,N-dimethyl-n-alkylamine trend line which suggests that the steric cost and benefit of ring system carbon γ to the nitrogen are roughly equal or are negligible. As for 9′, definitively resolving the subtle steric and electronic effects associated with the benzyl ring system is beyond the current scope of this paper but it models well as γ carbon sterics with no ring benefit. Based on these systems, an “α ring system” which includes the cyclohexyl groups (5′ and 13′), piperidine (3′), and pyrrolidine (7′) provides an enhancement to an amine's SPS function, which is not observed for more distant ring systems (9′ and 11′). The benefit of an α ring system (1.2) was incorporated into eqn (8), Table 3 and Fig. 14.

Aniline derivatives were not observed to function as SPS. The nonfunctionality of the aromatic aniline derivatives is not predicted by eqn (8), and is attributed to the pKa of 5–6 resulting from an amine directly bonded to an aromatic ring which is significantly lower than the alkyl substituted tertiary amines with pKa of 8–11.

Conclusion

In this study, a functional group contribution model has been developed for tertiary amine SPS. Also, structural limits for tertiary amines that function as SPS were identified, which suggested that a C[thin space (1/6-em)]:[thin space (1/6-em)]N ratio between 6 and 12 is necessary. Furthermore, a new form of non-osmotic SPS with an elevated amine to carbonate ratio in its polar form has been identified and characterized. This structure–function analysis and identification of a new form of SPS has implications on the design of SPS systems based on untested amine systems, as well as the selection of SPS for a variety of applications including solvent extraction systems, plastic recycling, synthetic media, acid gas capture, and osmotically driven membrane processes (ODMPs).

Experimental methods

General

Deionized water was used for these experiments. N,N-Dimethylbutylamine, triethylamine, 1-ethylpiperidine, N-methyldipropylamine N,N-dimethylcyclohexylamine 99% (N(Me)2Cy), 1-butylpyrrolidine, N,N-diethylbutylamine, N,N-dimethylbenzylamine, N-methyldibutylamine, N,N-dimethylphenethylamine, N,N-dimethyloctylamine, N,N-diethylcyclohexylamine, 2-ethylhexylamine, N,N-dimethylnonylamine, N,N-dimethyldecylamine, N,N-dimethyaniline, N-ethyldiisopropylamine, tripropylamine, triisopropylamine, 4-N,N-Trimethylaniline, N,N-dimethyl-o-toluidine, tributylamine, N,N-dicyclohexylmethylamine, N,N-dimethyldodecylamine, tripentylamine were obtained from Aldrich and used as received. All equipment was used in accordance with manufacturer specification unless stated otherwise. Freezing point depression osmometry was performed using an Advanced Instruments Inc. Model 3250 Osmometer. Viscosity measurements were made using the falling bob method with a Cambridge Applied systems VL4100 viscometer.

Nuclear magnetic resonance (NMR) spectra were acquired on a Bruker Avance III 600 MHz spectrometer with a magnetic field strength of 14.093 Tesla, corresponding to operating frequencies of 600.13 MHz (1H), and 150.90 MHz (13C). All NMR were captured with a co-axial insert containing C6D6 (Cambridge Isotopes Laboratories). 1H NMR spectra were collected with a 30° pulse and 10 s delays between scans, the T1 of every integrated shift was verified, most T1 relaxations well under 1 s and none above 2 s. The integration was set to a known peak in of the tertiary amine providing the relative concentration of (H2O + H2CO3)[thin space (1/6-em)]:[thin space (1/6-em)]tertiary amine. 13C NMR spectra with quantifiable integration were obtained with inverse gated decoupling spectra with a 30° pulse and 60 second delays between scans. The 13C T1 values were verified and found to range between 2.5 s and 10.5 s for the carbonate peak, all other peaks had shorter relaxation times. The integration of the carbonate peaks was set to unity providing the relative concentration of tertiary amine[thin space (1/6-em)]:[thin space (1/6-em)]carbonate.

Conversion of 1–16 to 1′–16′

As an example, deionized water (3.884 g) and dimethylhexylamine (6, 5.468 g, 7.35 ml, 0.0423 mol) are placed in home-built carbon dioxide addition cell, Fig. 15. The carbon dioxide addition cell was designed to measure the volume of nonpolar amine which remained phase separated from the aqueous volume. Knowing the original volume of the amine, it was possible to calculate the volume which had reacted with the known volume of water. The addition cell from bottom to top features a fine frit base with a ∼2.5 cm diameter, 5 ml reservoir bulb, 10 ml graduated cylinder (1.5 cm diameter 8 cm tall), 25 ml reservoir bulb, 30 cm condenser. A small stir bar is added and stirred rapidly, the condenser is operated at 2 °C, and CO2 is flowed through the cell at a steady rate of <3 ml s−1. After a 50 min purge, 1.0 ml of the amine is unreacted, after 2 h 0.9 ml of the amine unreacted. The solution was purged with carbon dioxide for a total of 5 h with 0.9 ml of the amine unreacted. The product, 6′ approximately [HN(Me)2Cy HCO3], and unreacted amine are removed with a syringe and long needle.
image file: c3ra47724j-f15.tif
Fig. 15 Carbon dioxide additional cell used to convert two phases of amine and water to a single phase polar SPS, 1′ through 16′.

Synthesis of N,N-dimethyl-2-ethylhexylamine (14)

2-Ethyl-1-hexylamine (304.55 g 2.36 mol) was slowly added to a solution of formaldehyde 37 wt% (575.17 g, 7.09 mol) and formic acid (328.53 g, 7.14 mol) and allowed to stir overnight. Slow addition of NaOH (162 g, 4.1 mol) caused the solution to split into organic and aqueous layers. The organic layer was isolated, washed with water (4 × 350 ml), and dried with sodium sulfate. The product (315.5 g) was then distilled at 150 mTorr and 25–30 °C giving a slightly yellow liquid (235.9 g, MW 157.4, 1.5 mol) with a density of 0.768 g ml−1 for a final yield of 64%. The product was confirmed as N,N-dimethyl-2-ethylhexylamine with a water content <1 wt% using 1H-NMR, 13C-NMR, COSY, HSQC, and HMBC.

Acknowledgements

This work was supported by the United States Department of Energy through contract DE-AC07-05ID14517. Funding was supplied by Idaho National Laboratory via the Laboratory Directed Research and Development Fund (LDRD) under project 14-079.

References

  1. M. Poliakoff and P. Licence, Nature, 2007, 450, 810–812 CrossRef CAS PubMed.
  2. P. G. Jessop, S. M. Mercer and D. J. Heldebrant, Energy Environ. Sci., 2012, 5, 7240–7253 CAS.
  3. P. G. Jessop, D. J. Heldebrant, X. Li, C. A. Eckert and C. L. Liotta, Nature, 2005, 436, 1102 CrossRef CAS PubMed.
  4. P. G. Jessop, L. Phan, A. Carrier, S. Robinson, C. J. Durr and J. R. Harjani, Green Chem., 2010, 12, 809–814 RSC.
  5. P. G. Jessop, L. Kozycz, Z. G. Rahami, D. Schoenmakers, A. R. Boyd, D. Wechsler and A. M. Holland, Green Chem., 2011, 13, 619–623 RSC.
  6. T. Yamada, P. J. Lukac, M. George and R. G. Weiss, Chem. Mater., 2007, 19, 967–969 CrossRef CAS.
  7. T. Yamada, P. J. Lukac, T. Yu and R. G. Weiss, Chem. Mater., 2007, 19, 4761–4768 CrossRef CAS.
  8. T. Yu, T. Yamada, G. C. Gaviola and R. G. Weiss, Chem. Mater., 2008, 20, 5337–5344 CrossRef CAS.
  9. L. Phan, J. R. Andreatta, L. K. Horvey, C. F. Edie, A.-L. Luco, A. Mirchandani, D. J. Darensbourg and P. G. Jessop, J. Org. Chem., 2008, 73, 127–132 CrossRef CAS PubMed.
  10. Y. Kohno, H. Arai and H. Ohno, Chem. Commun., 2011, 47, 4772–4774 RSC.
  11. M. L. Stone, C. Rae, F. F. Stewart and A. D. Wilson, Desalination, 2013, 312, 124–129 CrossRef CAS PubMed.
  12. M. L. Stone, A. D. Wilson, M. K. Harrup and F. F. Stewart, Desalination, 2013, 312, 130–136 CrossRef CAS PubMed.
  13. A. Achilli, T. Y. Cath and A. E. Childress, J. Membr. Sci., 2010, 364, 233–241 CrossRef CAS PubMed.
  14. T. Y. Cath, A. E. Childress and M. Elimelech, J. Membr. Sci., 2006, 281, 70–87 CrossRef CAS PubMed.
  15. B. Van der Bruggen, L. Lejon and C. Vandecasteele, Environ. Sci. Technol., 2003, 37, 3733–3738 CrossRef CAS.
  16. I. Alsvik and M.-B. Hägg, Polymers, 2013, 5, 303–327 CrossRef.
  17. J. R. McCutcheon, R. L. McGinnis and M. Elimelech, J. Membr. Sci., 2006, 278, 114–123 CrossRef CAS PubMed.
  18. G. Puxty, R. Rowland, A. Allport, Q. Yang, M. Bown, R. Burns, M. Maeder and M. Attalla, Environ. Sci. Technol., 2009, 43, 6427–6433 CrossRef CAS.
  19. J. Zhang, Y. Qiao and D. W. Agar, Energy Procedia, 2012, 23, 92–101 CrossRef CAS PubMed.
  20. J. Zhang, D. W. Agar, X. Zhang and F. Geuzebroek, Energy Procedia, 2011, 4, 67–74 CrossRef CAS PubMed.
  21. J. Zhang, J. Chen, R. Misch and D. W. Agar, Chemical Engineering Transaction, 2010, 21, 169–174 CrossRef PubMed.
  22. D. Agar; Y. Tan and Z. Hui, Separating CO2 from Gas Mixtures – PCT/EP2007/057907, February 8, 2008 Search PubMed.
  23. L. Raynal, P. Alix, P.-A. Bouillon, A. Gomez, M. le F. de Nailly, M. Jacquin, J. Kittel, A. di Lella, P. Mougin and J. Trapy, Energy Procedia, 2011, 4, 779–786 CrossRef CAS PubMed.
  24. M. Aleixo, M. Prigent, A. Gibert, F. Porcheron, I. Mokbel, J. Jose and M. Jacquin, Energy Procedia, 2011, 4, 148–155 CrossRef CAS PubMed.
  25. D. J. Heldebrant, C. R. Yonker, P. G. Jessop and L. Phan, Energy Environ. Sci., 2008, 1, 487–493 CAS.
  26. D. J. Heldebrant and C. R. Yonker, U.S. Pat., 7799299-Capture and Release of Mixed Acid Gasses with Binding Organic Liquids. 7799299, September 21, 2010.
  27. D. J. Heldebrant; C. R. Yonker; P. K. Koech, US 2009/0220397 A1-Capture and Release of Acid–Gasses with Acid–Gas Binding Organic Compounds.
  28. D. J. Heldebrant, P. K. Koech, J. E. Rainbolt and F. (Richard) Zheng, Energy Procedia, 2011, 4, 216–223 CrossRef CAS PubMed.
  29. L. Hu, U.S. Pat., 6969418-Phase Enhanced Gas-liquid Absorption Method. 6969418, November 29, 2005.
  30. L. Hu, U.S. Pat., 7541011-Phase Transitional Absorption Method. 7541011, June 2, 2009.
  31. L. Hu, U.S. Pat., 7718151-Methods and Systems for Deacidizing Gaseous Mixtures. 7718151, May 18, 2010.
  32. L. Hu, Grant: CO2 Capture from Flue Gas by Phase Transitional Absorption, Project no. NT42488.
  33. L. Hu, Grant: Post-Combustion CO2 Capture for Existing PC Boilers by Self-concentrating Amine Absorbent, Project no. FE0004274.
  34. V. Blasucci, R. Hart, V. L. Mestre, D. J. Hahne, M. Burlager, H. Huttenhower, B. J. R. Thio, P. Pollet, C. L. Liotta and C. A. Eckert, Fuel, 2010, 89, 1315–1319 CrossRef CAS PubMed.
  35. V. Blasucci, C. Dilek, H. Huttenhower, E. John, V. Llopis-Mestre, P. Pollet, C. A. Eckert and C. L. Liotta, Chem. Commun., 2009, 116 RSC.
  36. J. R. Switzer, A. L. Ethier, E. C. Hart, K. M. Flack, A. C. Rumple, J. C. Donaldson, A. T. Bembry, O. M. Scott, E. J. Biddinger, M. Talreja, M.-G. Song, P. Pollet, C. A. Eckert and C. L. Liotta, ChemSusChem, 2014, 7, 299–307 CrossRef CAS PubMed.
  37. C. A. Eckert, Grant: Reversible Liquids as Double-Action Solvents for Efficent CO2 Capture, Project no. NT0005287.
  38. L. Phan and P. G. Jessop, Green Chem., 2009, 11, 307 RSC.
  39. C. Samorì, C. Torri, G. Samorì, D. Fabbri, P. Galletti, F. Guerrini, R. Pistocchi and E. Tagliavini, Bioresour. Technol., 2010, 101, 3274–3279 CrossRef PubMed.
  40. C. Samorì, D. L. Barreiro, R. Vet, L. Pezzolesi, D. W. F. Brilman, P. Galletti and E. Tagliavini, Green Chem., 2013, 15, 353–356 RSC.
  41. A. R. Boyd, P. Champagne, P. J. McGinn, K. M. MacDougall, J. E. Melanson and P. G. Jessop, Bioresour. Technol., 2012, 118, 628–632 CrossRef CAS PubMed.
  42. Y. Du, B. Schuur, C. Samorì, E. Tagliavini and D. W. F. Brilman, Bioresour. Technol., 2013, 149, 253–260 CrossRef CAS PubMed.
  43. Q. Zhang, N. S. Oztekin, J. Barrault, K. De Oliveira Vigier and F. Jérôme, ChemSusChem, 2013, 6, 593–596 CrossRef CAS PubMed.
  44. A. D. Wilson, 2012, unpublished results.
  45. A. I. Bhatt, A. M. Bond, D. R. MacFarlane, J. Zhang, J. L. Scott, C. R. Strauss, P. I. Iotov and S. V. Kalcheva, Green Chem., 2006, 8, 161–171 RSC.
  46. A. E. Rosamilia, C. R. Strauss and J. L. Scott, Pure Appl. Chem., 2007, 79, 1869–1877 CrossRef CAS.
  47. S. A. Chowdhury, R. Vijayaraghavan and D. R. MacFarlane, Green Chem., 2010, 12, 1023–1028 RSC.
  48. A. W. T. King, J. Asikkala, I. Mutikainen, P. Järvi and I. Kilpeläinen, Angew. Chem., Int. Ed., 2011, 50, 6301–6305 CrossRef CAS PubMed.
  49. I. S. Bechara, Carbamate and Carbonate Salts of Tertiary Amines – USPTO 4,542,214. 4542214, September 17, 1985.
  50. A. D. Wilson and F. F. Stewart, J. Membr. Sci., 2013, 431, 205–211 CrossRef CAS PubMed.
  51. A. A. Zavitsas, J. Phys. Chem. B, 2001, 105, 7805–7817 CrossRef CAS.
  52. A. D. Wilson, K. Fraze, B. Twamley, S. M. Miller, D. L. DuBois and M. Rakowski DuBois, J. Am. Chem. Soc., 2008, 130, 1061–1068 CrossRef CAS PubMed.
  53. C. A. Tolman, Chem. Rev., 1977, 77, 313–348 CrossRef CAS.
  54. A. L. Seligson and W. C. Trogler, J. Am. Chem. Soc., 1991, 113, 2520–2527 CrossRef CAS.
  55. A. D. Wilson, A. J. M. Miller, D. L. DuBois, J. A. Labinger and J. E. Bercaw, Inorg. Chem., 2010, 49, 3918–3926 CrossRef CAS PubMed.

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