Abstract
Ionic liquids (ILs) have been used for carbon dioxide (CO2) capture, however, which have never been used as catalysts to accelerate CO2 capture. The record is broken by a uniquely designed IL, [EMmim][NTf2]. The IL can universally catalyze both CO2 sorption and desorption of all the chemisorption‐based technologies. As demonstrated in monoethanolamine (MEA) based CO2 capture, even with the addition of only 2000 ppm IL catalyst, the rate of CO2 desorption—the key to reducing the overall CO2 capture energy consumption or breaking the bottleneck of the state‐of‐the‐art technologies and Paris Agreement implementation—can be increased by 791% at 85 °C, which makes use of low‐temperature waste heat and avoids secondary pollution during CO2 capture feasible. Furthermore, the catalytic CO2 capture mechanism is experimentally and theoretically revealed.
Keywords: absorption and desorption, catalyst, CO2 capture, ionic liquid, monoethanolamine
A uniquely designed and synthesized ionic liquid (IL) is first used as a homogeneous catalyst for monoethanolamine (MEA) based CO2 capture. Only 2000 ppm IL catalyst can universally catalyze both CO2 sorption and desorption of all the chemisorption‐based technologies. Furthermore, the catalytic CO2 capture mechanism is experimentally and theoretically revealed.

1. Introduction
Carbon dioxide (CO2) capture is critical not only because of its close connection with climate change according to Paris Climate Accord [ 1 , 2 , 3 ] but also because of its increasing importance as a material and fuel synthesis resource.[ 4 , 5 , 6 ] Thus, CO2 capture is very important.[ 7 , 8 ] Chemisorption is one of the most important methods for CO2 capture.[ 9 , 10 , 11 ] The fundamental challenge of chemisorption‐based technologies is the slow absorption and desorption reaction kinetics, especially the latter one, which leads to the need for CO2 desorption at >100 °C.[ 12 ] Consequently, excessive energies are needed to vaporize a large amount of liquid water during CO2 desorption operation and condense the same amount of water vapor prior to CO2 sorption during cyclic CO2 sorption and desorption. Also, severe corrosion and sorbent degradations could result in secondary environmental and health issues, especially when organic amines are used as sorbents.
Thus, is there a way to overcome the fundamental and the associated challenges by desorbing CO2 or regenerating spent sorbents at temperatures less than 100 °C? This is the pivotal to making use of abundant low quality or waste heats for CO2 desorption feasible, while desired CO2 desorption rates are achievable. Fan et al.[ 13 ] reported that 20 000 ppm nanostructured TiO(OH)2 as a heterogeneous catalyst can increase CO2 desorption rate of MEA‐based CO2 capture over 4000% at 88 °C . However, to date, homogeneous catalysis has not been utilized for CO2 capture.
After a long time of study, a homogeneous CO2 capture catalyst—a new ionic liquid (IL), [CH3COOCH2mim][NTf2], denoted as [EMmim][NTf2]—was discovered. The IL, used as a CO2 capture catalyst instead of a sorbent, is not only very effective for catalyzing CO2 desorption but also CO2 sorption. It should be emphasized that [EMmim][NTf2] is used as a transformative catalyst instead of a sorbent for CO2 capture [ 14 ] in this work.
2. Results and Discussion
2.1. Effect of the Synthesized IL Catalyst
Detailed procedure for preparing [EMmim][NTf2], the first IL and homogeneous catalyst for CO2 capture, is provided in the Materials and Methods part. A schematic drawing of this CO2 absorption and desorption experimental setup is shown in Figure S1 (Supporting Information). Schematic diagram for synthesizing the IL and its characteristic results are provided in Figure S2 (Supporting Information). The optimal dosage of this catalyst for accelerating CO2 desorption, the key step for reducing overall CO2 capture energy consumption, is 2000 ppm according to Figure S3 (Supporting Information).
Figure 1 exhibits the CO2 absorption and desorption performances of 20 wt% monoethanolamine (MEA) solution catalyzed by 2000 ppm [EMmim][NTf2]. [EMmin][NTf2] can promote both CO2 absorption and desorption. Capturing 90% CO2 is targeted by the U.S. Department of Energy, and thus the period with 90% CO2 capture efficiency is defined as effective absorption time. According to Figure 1A, 20 wt% MEA sorbent without catalyst can absorb only 144.34 mmol CO2 within the shorter effective absorption time of 4446 s, while the sorbent with 2000 ppm IL catalyst can absorb 210.09 mmol CO2, and extend effective absorption time to 6350 s, which are 45.55% and 42.83% absorption improvements, respectively, compared to the sorbent without catalyst.
Figure 1.

Catalytic effects of [EMmim][NTf2] on CO2 absorption and desorption. A) Uncatalyzed and catalyzed CO2 absorption profiles of 20% MEA sorbent; B) effects of CO2 desorption rates with and without uses of the catalyst; C) the percentage increases in CO2 desorption rate and desorption amount with the use of catalyst; D) effect of catalyst on the quantities of desorbed CO2.
Variations of desorption with time with and without uses of catalyst are illustrated in Figure 1B. The time needed for reaching the maximum desorption rate with the use of [EMmim][NTf2] is shortened by 150 s in comparison to the time required for CO2 desorption without the use of the IL catalyst. Meanwhile, the peak desorption rate improvement is 175%. The increases in desorption rate and the desorbed CO2 amount obtained with [EMmim][NTf2] can reach as high as 791% at 507 s and 534% at 551 s (Figure 1B–D), respectively. The quantities of CO2 desorbed from uncatalytic and catalytic solutions are 18.7 and 28.2 mmol, respectively. When the absorption time is 7000 s or the outlet CO2 concentrations of both uncatalyzed and catalyzed CO2 absorption are 3.2 vol% (Figure S4, Supporting Information), use of [EMmim][NTf2] can increase the total desorbed CO2 amount by 88.90%. It should be noted that dosage of [EMmim][NTf2] is only 2000 ppm—the lowest dosage for achieving such significant CO2 capture catalysis effect. To the best knowledge, such a low catalyst dosage has not been reported for achieving such a significant CO2 capture. Also, as a homogeneous catalyst, [EMmim][NTf2] is easy to use. Therefore, [EMmim][NTf2] is quite effective for catalyzing both the CO2 absorption and desorption processes.
2.2. Stabilities of the Catalytic CO2 Capture System
Stability characteristic of [EMmim][NTf2] for CO2 capture was studied with 50 cyclic tests, and the results are shown in Figure 2 and Figure S5 (Supporting Information). There is no apparent change in both quantities of absorbed and desorbed CO2. The average CO2 capture working capacities within the 50 cyclic tests are 31.94 and 32.77 mmol for absorption and desorption amounts, respectively. As shown in Figure S5C (Supporting Information), FT‐IR spectra of the regenerated MEA solution confirm that no change in the structure of MEA molecules was observed after 50 cycles of the tests. Thus, both MEA and the [EMmim][NTf2] are stable. Moreover, [EMmim][NTf2] can thermally be stable at as high as 300 °C as shown in Figure S2F (Supporting Information).
Figure 2.

Evaluation of stability of [EMmim][NTf2] as a catalyst for MEA based CO2 capture.
2.3. Mechanism
2.3.1. Experimental Study of the Reaction Mechanisms
The molecular structure of the IL, [EMmim][NTf2] is shown in Figure S2A (Supporting Information). After CO2 absorption, the pH of the capture system decreased from 12.01 to 8.52 (Table 1 ), indicating the increase of H+ concentration and promotion of the hydrolysis of the ‐COOCH3 in [EMmim][NTf2] into —COOH, which is need for catalyzing CO2 desorption. Thus, the activation of [EMmim][NTf2] is accompanied with the enhancement of the acidity of [EMmim][NTf2] after CO2 absorption, as illustrated in Figure 3A. The FT‐IR spectra of water, and the 2000 ppm [EMmim][NTf2] aqueous solution with or without CO2 shown in Figure 3B further confirm this mechanism. Anhydrous CH3OH and CH3COOCH3 as well as CH3COOH and 50% CH3COOH solutions were used to identify the functional groups in the catalytic solutions with or without additions of CO2. The bands around 1381–1339 cm−1 in the catalytic solutions [Figure 3B (1)] are assigned to the —CH3 group in the IL catalyst (—COOCH3), observed in anhydrous CH3OH, CH3COOCH3 and CH3COOH and 50% CH3COOH solutions. With the increase in the introduced CO2 in the solution, hydrolysis of ‐COOCH3 is enhanced, leading to increasing the concentration of —CH3 or CH3OH in the catalytic solution as illustrated in Figure 3A. Bands with wavenumbers between 1221–1190 cm−1 [Figure 3B (2)], detected in anhydrous CH3OH as well, confirm the formation of CH3OH with an enhanced hydrolysis process with CO2. As concentration of —COOCH3 decreases, the —C—O—C peak [1160–1128 cm−1, Figure 3B (3)] in the catalytic solution with the addition of CO2 was weaker than that of the solution without addition of CO2 according to the reference peaks of anhydrous CH3COOCH3. Consequently, more —COO— or —COOH formation or more —COOCH3 hydrolysis, was detected within 1079–1050 cm−1 [Figure 3B (4)], which are concluded from the observations of peaks of anhydrous CH3COOCH3 and CH3COOH, and 50% CH3COOH solution. Also, the acidity of the [EMmim][NTf2] was verified via the measurement of the pH (6.19) of the solution resulting from the addition of 0.2 g [EMmim][NTf2] to 80 g H2O (Table 1). The FT‐IR spectra of fresh catalytic solution, catalytic solutions after the 1st absorption and the 1st absorption–desorption runs are displayed in Figure S6 (Supporting Information). The differences in the changes of the quantities of CO2 absorbed and desorbed, and pH values of the uncatalytic and catalytic solutions with absorption and desorption times as shown in Figure 4 result from the use of the catalyst. The uncatalytic solution and catalytic solution both absorbed 232 mmol CO2 at 130 and 120 min, respectively. However, the pH value (8.65) of the catalytic solution is lower than that (8.79) of the uncatalytic solution, which is another direct evidence of hydrolysis of ‐COOCH3 in the IL into —COOH, a key functional group in catalyzing the subsequent CO2 desorption.
Table 1.
pH values of aqueous IL solutions and mMEA solutions
| Sample | pH values |
|---|---|
| 80 g H2O | 6.37 |
| 80 g H2O + 0.2 g [EMmim][NTf2] | 6.19 |
| 20 g MEA + (80 g H2O + 0.2 g [EMmim][NTf2]) | 12.01 |
| 20 g MEA + 80 g H2O | 12.04 |
| MEA without catalyst after the 1st abs1. | 8.79 |
| MEA with [EMmim][NTf2] catalyst after the 1st abs2. | 8.52 |
| MEA without catalyst after the 1st cyclic abs.‐des3. | 9.47 |
| MEA with [EMmim][NTf2] catalyst after the 1st cyclic abs.‐des4. | 9.46 |
| MEA with [EMmim][NTf2] catalyst after 50 cycles of abs.‐des. | 9.34 |
Note:1, 2 1st abs.: solution received after the 2 h 10 min sorption. 3,4 1st cyclic abs.‐des.: solution obtained after the first cyclic test.
Figure 3.

The [EMmim][NTf2] catalyst activation process via hydrolysis in CO2 absorbing system. A) The schematic representation of the [EMmim][NTf2] catalyst and the hydrolysis activation process. B) FT‐IR spectra of water, water +2000 ppm catalyst with or without additions of CO2, anhydrous CH3OH and CH3COOH as well as CH3COOCH3, and 50% CH3COOH aqueous solution. 5.18 mmol CO2 was bubbled into the water + 2000 ppm Catalyst + CO2 system with a simulated flue gas containing 10 vol% CO2, 10 vol% O2, and 80 vol% N2 with a total flow rate of 500 mL min−1 in 20 min.
Figure 4.

Changes of the quantities of CO2 absorbed and desorbed, and pH values of the uncatalytic and catalytic solutions with A) absorption times and B) desorption times.
The catalytic effect of [EMmim][NTf2] at different absorption and desorption times is observed through FT‐IR spectra, as shown in Figure 5 . The bands at 1324 cm−1 (stretching of N—COO−), 1488 cm−1 (symmetric stretching of COO−) and 1559 cm−1 (asymmetric stretching of COO−) are ascribed to the MEACOO−,[ 15 ] while peaks at 1385 and 1635 cm−1 are assigned to CO3 2− and HCO3 −, respectively.[ 15 , 16 ] Intensities of peaks of HCO3 − in the catalytic MEA solution during CO2 absorption (Figure 5B) increase faster than those of the uncatalytic ones (Figure 5A). Moreover, peak intensities of MEACOO− and CO3 2− for the catalytic MEA solutions at the end of CO2 absorption (7800 s or 130 min) are stronger than those of the uncatalytic one. Differences are more obvious for the desorption tests, as shown in Figure 5C,D. Peak intensities of HCO3 − in the uncatalytic MEA solutions decrease slowly with the continuous CO2 desorption, and the intensities of CO3 2− and MEACOO− peaks and thus the concentrations of CO3 2− and MEACOO− barely change, in spite of the subsequent slightly noticeable variations. However, peak intensities of HCO3 −, CO3 2−and MEACOO− of the catalytic MEA solutions decrease considerably fast with time during CO2 desorption, especially in the initial 10 min. The experimental observations of the changes in concentrations of intermediates with FT‐IR spectra confirm the significant catalytic effect of the [EMmim][NTf2].
Figure 5.

FT‐IR spectra of the catalytic and uncatalytic solutions during CO2 absorption and desorption at different times. A) Uncatalyzed CO2 absorption; B) catalyzed CO2 absorption; C) uncatalyzed CO2 desorption; D) catalyzed CO2 desorption.
2.3.2. Uncatalyzed and Catalyzed CO2 Sorption and Desorption Pathways as well as Their Essential Differences
The density functional theory (DFT) calculations in this research have been performed by using the Gaussian09 package.[ 17 ] The reaction processes with and without uses of the catalyst are shown vertically and horizontally in Figure 6A, respectively, while the corresponding energy changes for each step are provided in Figure 6B. Also, the calculation results reveal the highest energy barriers in CO2 absorption and desorption processes (especially CO2 sorption) and how they can be lowered with the catalyst [EMmim][NTf2].
Figure 6.

DFT based noncatalytic and catalytic CO2 capture reaction pathways and energy profiles. A) Pathways. B) Energy profiles.
When catalyst is not used, there are two possible CO2 capture pathways, P1‐WOcat‐MEA‐CO2 (pathway without presences of the catalyst and H2O) and P2‐WOcat‐MEA‐CO2‐H2O (pathway without presence of the catalyst but with the presence of H2O) according to zwitterion (ZW) and bicarbonate (HCO3 −) formation mechanisms.[ 18 , 19 ] The step reactions in P1‐WOcat‐MEA‐CO2 shown in Figure 6A include
| (P1‐R1) |
| (P1‐R2) |
The ring configuration of MEA shown in Figure S7 (Supporting Information) is the most stable structure. As shown in Figure 6B, the Gibbs free energy of reaction for the CO2 absorption process consisting of P1‐R1 and P1‐R2 in P1‐WOcat‐MEA‐CO2 is exothermic by 5.3 kcal mol−1. Furthermore, as shown in Figure S8 (Supporting Information), the calculated Gibbs free energy of reaction and activation energies in the forward reaction or CO2 absorption and reverse reaction or CO2 desorption of P1‐WOcat‐MEA‐CO2, P1‐R1 and P1‐R2, as well as P1‐R‐1 and P1‐R‐2, respectively, are very close to those in the literatures.[ 20 , 21 , 22 , 23 , 24 , 25 , 26 ] Thus, the computational methods are effective. Special attention should be paid to P1‐R‐1 because it is identified as the rate‐determining step of CO2 desorption for P1‐WOcat‐MEA‐CO2 due to its high Gibbs free energy of reaction (6.5 kcal mol−1). According to the energetic span model of Kozuch and Shaik,[ 27 ] the apparent activation energy for CO2 absorption and desorption are 13.8 and 19.6 kcal mol−1, respectively.
For the HCO3 − formation mechanisms,[ 18 , 19 ] P2‐WOcat‐MEA‐CO2‐H2O, the HCO3 − generation reactions probably are [ 28 , 29 , 30 ]
| (P2‐R1) |
| (P2‐R2‐1) |
| (P2‐R2‐2) |
The reaction energy values of P2‐R1 and P2‐R2 were calculated and compared in Figure S9 (Supporting Information). P2‐R1 is the preferred pathway because of its lower Gibbs free energy (7.1 kcal mol−1) for activation among all the steps of P2‐R1 and P2‐R2. Thus, Figure 6 only shows P2‐R1, denoted as P2‐R1‐WOcat‐MEA‐CO2‐H2O, and its step reactions as well as the associated energy data.
Then, the assured computational methods were applied to explain how the catalyst [EMmim][NTf2] can overcome the challenge of chemisorption‐based CO2 capture via significant acceleration of both CO2 absorption and CO2 desorption with catalyst in P1‐WHcat‐MEA‐CO2 (pathway with the catalyst but without H2O) and P2‐WHcat‐MEA‐CO2‐H2O (pathway with both catalyst and H2O). [mimCH2COOH]+ as a Brønsted acid is the core of the catalytic CO2 capture technology, thus, [mimCH2COOH]+ instead of [EMmim][NTf2] is used for modeling the catalyst. In Figure 6, it clearly shows that [mimCH2COOH]+ in [EMmim][NTf2] readily transfers the carboxyl group proton to MEA to form the complex of [mimCH2COO−]+ and MEAH+, denoted as MEA‐cat Complex, which is barrierless and exothermic by 2.6 kcal mol−1. And it is found that the individual [mimCH2COOH]+ is effective than the whole MEA‐cat Complex in P1‐WHcat‐MEA‐CO2, as shown in Figure S10 (Supporting Information). Reactions in the catalyzed desorption pathway are in way of:
| (P1‐R‐2‐WHcat) |
| (P1‐R‐1‐WHcat) |
In the catalysis pathway, P1‐WHcat‐MEA‐CO2, in presence of [mimCH2COOH]+, MEACOO− decomposes into MEA and CO2 in one step without ZW formation. Its Gibbs free energies of activation are 4.7 kcal mol−1, much lower than that in P1‐WOcat‐MEA‐CO2 (12.7 kcal mol−1). And then, to put into the next catalytic cycle, the other absorption product MEAH+ would provide the proton to [mimCH2COO−]+ to regenerate the catalyst. The apparent activation energy for CO2 absorption and desorption in P1‐WHcat‐MEA‐CO2 are 13.8 and 11.6 kcal mol−1, respectively, which are 13.8 and 19.6 kcal mol−1 in the pathway without catalyst P1‐WOcat‐MEA‐CO2. Thus, [mimCH2COOH]+ can clearly facilitate P1‐WOcat‐MEA‐CO2 based CO2 capture pathway, with the P1‐WHcat‐MEA‐CO2 more preferable.
Also, energy profiles for CO2 absorption and desorption in P2‐R1 and P2‐R2, with and without the presences of [mimCH2COOH]+, were calculated and presented in Figure S11 (Supporting Information). The Gibbs free energy of activation for the catalytic CO2 absorption in P2‐R1‐WHcat‐MEA‐CO2‐H2O is 2.6 kcal mol−1, lower than 7.1 kcal mol−1 in the noncatalytic P2‐R1‐WOcat‐MEA‐CO2‐H2O. While the Gibbs free energy of activation for the other catalytic CO2 absorption, P2‐R2‐WHcat‐MEA‐CO2‐H2O, are 12.7 and 3.5 kcal mol−1, respectively, which is very close to 12.7 and 3.9 kcal mol−1 in the noncatalytic P2‐R2‐WOcat‐MEA‐CO2‐H2O. Thus, both noncatalytic P2‐R1‐WOcat‐MEA‐CO2‐H2O and the catalyzed P2‐R1‐WHcat‐MEA‐CO2‐H2O appear to be easier for CO2 capture with H2O pathway.
As shown in Figure S10 (Supporting Information), [mimCH2COOH]+ is more effective than MEA‐cat Complex in accelerating not only HCO3 − formation during CO2 absorption, but also HCO3 − decomposition into CO2 during CO2 desorption in P2‐R1‐WHcat‐MEA‐CO2‐H2O. In noncatalytic P2‐R1‐WOcat‐MEA‐CO2‐H2O, the Gibbs free energy of activation for CO2 desorption is 12.6 kcal mol−1, and with [mimCH2COOH]+ that for CO2 catalytic desorption in P2‐R1‐WHcat‐MEA‐CO2‐H2O slightly decrease to 11.5 kcal mol−1, as shown in Figure 6B. The participation of [mimCH2COOH]+ does not change the reaction pathway, however the apparent activation energy for catalytic CO2 absorption and desorption in P2‐R1‐WHcat‐MEA‐CO2 are 12.4 and 14.6 kcal mol−1, which are 15.7 and 17.9 for noncatalytic CO2 absorption and desorption in P2‐R1‐WOcat‐MEA‐CO2, respectively. Then, after MEAH+ transfer proton to [mimCH2COO−]+ and produce [mimCH2COOH]+ and MEA, the catalyst regenerates. Also, the regenerated MEA can be used for CO2 absorption in the subsequent cyclic CO2 capture.
The reactions in the desorption pathway with the use of [mimCH2COOH]+ are
| (P2‐R‐1,2‐WHcat) |
| (P2‐R‐1,1‐WHcat) |
Obviously, [mimCH2COOH]+ as a Brønsted acid or the core of the novel catalytic CO2 capture process, is necessary for initiating and driving P2‐R1‐WHcat, which further confirms the significant function of hydrolysis of [EMmim][NTf2] during CO2 absorption. The electrophilic characteristic of mim+ in [mimCH2COOH]+ can enhance the acidity of the —COOH in [mimCH2COOH]+ via inductive effect, which is desired for P2‐R‐1,2‐WHcat or formation of CO2 and H2O as well as [mimCH2COO−]+. The stable intermediate ([mimCH2COO−]+) resulting from the inherent resonance effect existing in —COO− is a conjugate base of [mimCH2COOH]+, which can quickly react with Brønsted acid, MEAH+ in P2‐R‐1,1‐WHcat for realization of MEA regeneration. Furthermore, the essential part of P2‐R‐1,2‐WHcat is to convert HCO3 − into CO2 and H2O, which is a well‐known rate limiting step in all the chemisorption‐based capture CO2 technologies. Thus, [EMmim][NTf2] with the desired Brønsted acidity is shown to be a highly effective homogenous organocatalyst for chemisorption‐based capture CO2 technologies.
3. Conclusions
The much quicker CO2 desorption kinetics at low temperature enabled with the use of the IL catalyst can significantly advance the development of a new generation of CO2 capture technology, from the perspectives of decreasing the parasitic penalty of these systems, capital investment, and environmental protection. The catalyst can make CO2 capture much less demanding for high quality energy, and thus widely available low‐temperature heat (e.g., those from solar collectors or waste heat) can be effectively used for CO2 capture, which will not only leads to a significant decrease in parasitic energy penalty, capital and operating costs, but also is beneficial to the elimination of the secondary environmental pollutant resulting from MEA degradation during high‐temperature CO2 desorption of conventional CO2 capture technologies. Therefore, [EMmim][NTf2] is a transcendent catalyst for CO2 capture technology.
4. Experimental Section
Experimental Design—Synthesis of IL
The detailed synthesis information of the [EMmim][NTf2] catalyst is presented as follows, and the schematic diagram of the synthetic route is displayed in Figure S2 (Supporting Information). First, [EMmim][Br] was synthesized with the reaction between 1‐methylimidazole and methyl bromoacetate. In a typical experiment, methyl bromoacetate (0.155 mol) was added dropwise to a solution of 1‐methylimidazole (0.15 mol) in acetonitrile (150 mL) under nitrogen atmosphere. The mixture was continuously stirred at room temperature until it was thoroughly homogeneous, following by heating the mixture at 55 °C for 12 h. The resulting solution was evaporated under vacuum and washed with ethyl acetate repeatedly to remove excess methyl bromoacetate. [EMmim][Br] was obtained after evaporating the above solution under vacuum condition. The produced IL was dried under vacuum for at least 24 h before use (31.6 g, yield 89.6%). [EMmim][NTf2] was prepared from the metathesis reaction between [EMmim][Br] and [Li][NTf2]. In a typical procedure, [EMmim][Br] (0.06 mol) was mixed with equimolar amount of [Li][NTf2] in 20 mL water. Then the mixture was vigorously stirred for 4 h at room temperature. After that, the bottom phase was washed with deionized water repeatedly to remove the excess salt. The resulting solution was rotary evaporated under vacuum to obtain the final product [EMmim][NTf2]. The prepared IL was dried under vacuum for at least 24 h before use (23.1 g, yield 88.3%).
Experimental Design—CO2 absorption–desorption Test
100 mL of 20 wt% MEA (99+%, product number: 11016‐7‐4L, Aldrich chemical company, Inc.) aqueous solution with the desired quantity of IL catalyst was employed for each test. The first run of CO2 absorption process was conducted at 30 °C and atmospheric pressure (0.78 bar at Laramie, Wyoming, USA, where the experiment was conducted), while the cyclic tests were conducted at 22 °C (room temperature). The simulated flue gas containing 10 vol% CO2, 10 vol% O2 and 80 vol% N2 with a total flow rate of 500 mL min−1 was bubbled into the 20 wt% amine solution. The outlet gas concentration was monitored with an inline gas analyzer (NDIR ZRE, California Analytical Instruments), and then recorded using a data recording unit. Absorption time for the first run test was 7800 s and that for each cyclic test was 1800 s. Upon the completion of the CO2 absorption experiment, the temperatures of the uncatalytic and catalytic MEA solutions were gradually heated to 85 °C. During the desorption process, N2 with a flow rate of 500 mL min−1 was used as the carrier gas. Desorption times were 1800 s for both first‐run and cyclic tests. The uncatalytic and catalytic solutions for Fourier‐transform infrared (FT‐IR) spectroscopy characterizations were collected under similar conditions except for different absorption or desorption times.
Statistical Analysis—Characterizations
1H NMR and 13C NMR spectra were recorded on a Bruker spectrometer (400 MHz) in the solvent of DMSO. ESI‐MS spectrum was obtained by ultra‐high‐resolution electro‐spray time‐of‐flight mass spectrometry (Bruker microTOF II, Germany). FT‐IR spectra were collected using a Thermo Nicolet Magna‐IR 760 spectrometer with a resolution of 4 cm−1 by scanning 32 times from 4000 to 400 cm−1. Thermogravimetric analysis (TGA) of IL was obtained using a TA Instruments SDT Q600 apparatus with a heating ramp of 10 °C min−1 at the temperature of 20–600 °C with a nitrogen flow rate of 100 mL min−1.
Statistical Analysis—Theoretical Studies
All of the calculations were performed with Gaussian09 package. Geometry optimization of all the minima and transition states involved was carried out at the B3LYP [ 31 , 32 ] level with the 6–31G(d) basis set for C, H, O, N. Default convergence criteria were used. The vibrational frequency calculations were conducted at the same level of theory as geometry optimization to confirm whether each optimized structure is an energy minimum or a saddle point. For transition state, intrinsic reaction coordinate (IRC) analysis [ 33 ] was performed to verify that it connects the right reactants and products. The solvent effects were considered using the PCM model [ 34 , 35 ] with the as‐phase‐optimized structures as the initial geometries.
Conflict of Interest
The authors declare no conflict of interest.
Supporting information
Supporting Information
Acknowledgements
X.H. and Y.G. contributed equally to this work. The authors thank support from the National Science Foundation (NSF 1604630) and the National Natural Science Foundation of China (Grant No. 21707083). [Correction added after publication January 25, 2023: F.C.'s affiliation was corrected]
He X., Gao Y., Shi Y., Zhang X., Liang Z., Zhang R., Song X., Lai Q., Adidharma H., Russell A. G., Eddings E. G., Fei W., Cheng F., Tsang S. C. E., Wang J., Fan M., [EMmim][NTf2]—a Novel Ionic Liquid (IL) in Catalytic CO2 Capture and ILs’ Applications. Adv. Sci. 2023, 10, 2205352. 10.1002/advs.202205352
Contributor Information
Fangqin Cheng, Email: cfangqin@sxu.edu.cn.
Shik Chi Edman Tsang, Email: edman.tsang@chem.ox.ac.uk.
Jianji Wang, Email: jwang@htu.cn.
Maohong Fan, Email: mfan@uwyo.edu, Email: mfan3@mail.gatech.edu.
Data Availability Statement
The data that support the findings of this study are available in the supplementary material of this article.
References
- 1. Rosenzweig C., Karoly D., Vicarelli M., Neofotis P., Wu Q., Casassa G., Menzel A., Root T. L., Estrella N., Seguin B., Tryjanowski P., Liu C., Rawlins S., Imeson A., Nature 2008, 453, 353. [DOI] [PubMed] [Google Scholar]
- 2. Sanna A., Uibu M., Caramanna G., Kuusik R., Maroto‐Valer M. M., Chem. Soc. Rev. 2014, 43, 8049. [DOI] [PubMed] [Google Scholar]
- 3. Kompas T., Pham V. H., Che T. N., Earths Future 2018, 6, 1153. [Google Scholar]
- 4. Nugent P., Giannopoulou E. G., Burd S. D., Elemento O., Giannopoulou E. G., Forrest K., Pham T., Ma S., Space B., Wojtas L., Eddaoudi M., Zaworotko M. J., Nature 2013, 495, 80. [DOI] [PubMed] [Google Scholar]
- 5. Saeidi S., Najari S., Fazlollahi F., Nikoo M. K., Sefidkon F., Klemeš J. J., Baxter L. L., Renewable Sustainable Energy Rev. 2017, 80, 1292. [Google Scholar]
- 6. Xia Y., Tian Z., Heil T., Meng A., Cheng B., Cao S., Yu J., Antonietti M., Joule 2019, 3, 2792. [Google Scholar]
- 7. Singh S. P., Hao P., Liu X., Wei C., Xu W. Q., Wei N., Li X., Lu H., Ku A. Y., Joule 2019, 3, 2154. [Google Scholar]
- 8. Zhang J., Sewell C. D., Huang H., Lin Z., Adv. Energy Mater. 2021, 11, 2102767. [Google Scholar]
- 9. Rochelle G. T., Science 2009, 325, 1652. [DOI] [PubMed] [Google Scholar]
- 10. Borhani T. N., Wang M., Renewable Sustainable Energy Rev. 2019, 114, 109299. [Google Scholar]
- 11. Yang Z., He L., Gao J., Liu A., Yu B., Energy Environ. Sci. 2012, 5, 6602. [Google Scholar]
- 12. Raganati F., Chirone R., Ammendola P., Ind. Eng. Chem. Res. 2020, 59, 3593. [Google Scholar]
- 13. Lai Q., Toan S., Assiri M. A., Cheng H., Russell A. G., Adidharma H., Radosz M., Fan M., Nat. Commun. 2018, 9, 2672. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 14. Aghaie M., Rezaei N., Zendehboudi S., Renewable Sustainable Energy Rev. 2018, 96, 502. [Google Scholar]
- 15. Richner G., Puxty G., Ind. Eng. Chem. Res. 2012, 51, 14317. [Google Scholar]
- 16. Köck E. M., Kogler M., Bielz T., Klötzer B., Penner S., J. Phys. Chem. C 2013, 117, 17666. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 17. Delley B., J. Chem. Phys. 2000, 113, 7756. [Google Scholar]
- 18. Yamada H., Shimizu S., Okabe H., Matsuzaki Y., Chowdhury F. A., Fujioka Y., Ind. Eng. Chem. Res. 2010, 49, 2449. [Google Scholar]
- 19. Chakraborty A. K., Astarita G., Bischoff K. B., Chem. Eng. Sci. 1986, 41, 997. [Google Scholar]
- 20. Bin Xie H., Zhou Y., Zhang Y., Johnson J. K., J. Phys. Chem. A 2010, 114, 11844. [DOI] [PubMed] [Google Scholar]
- 21. Li H. C., Da Chai J., Tsai M. K., Int. J. Quantum Chem. 2014, 114, 805. [Google Scholar]
- 22. Narimani M., Amjad‐Iranagh S., Modarress H., J. Mol. Liq. 2017, 233, 173. [Google Scholar]
- 23. Zhang T., Yu Y., Zhang Z., Mol. Simul. 2018, 44, 815. [Google Scholar]
- 24. Davran‐Candan T., J. Phys. Chem. A 2014, 118, 4582. [DOI] [PubMed] [Google Scholar]
- 25. Vassilev‐Galindo V., Matus M. H., Morales‐Cabrera M. A., Int. J. Greenhouse Gas Control 2016, 50, 198. [Google Scholar]
- 26. Kubota Y., Ohnuma T., Bučko T., J. Chem. Phys. 2017, 146, 094303. [Google Scholar]
- 27. Kozuch S., Shaik S., Acc. Chem. Res. 2011, 44, 101. [DOI] [PubMed] [Google Scholar]
- 28. Matsuzaki Y., Yamada H., Chowdhury F. A., Higashii T., Kazama S., Onoda M., Energy Procedia 2013, 37, 400. [Google Scholar]
- 29. Stowe H. M., Vilčiauskas L., Paek E., Hwang G. S., Phys. Chem. Chem. Phys. 2015, 17, 29184. [DOI] [PubMed] [Google Scholar]
- 30. Lv B., Guo B., Zhou Z., Jing G., Environ. Sci. Technol. 2015, 49, 10728. [DOI] [PubMed] [Google Scholar]
- 31. Hu W., Smith J. M., Doǧu T., Doǧu G., AIChE J. 1986, 32, 1483. [Google Scholar]
- 32. Becke A. D., J. Chem. Phys. 1993, 98, 5648. [Google Scholar]
- 33. Lee C., Yang E., Parr R. G., Phys. Rev. B. 1988, 37, 785. [DOI] [PubMed] [Google Scholar]
- 34. Gonzalez C., Schlegel H. B., J. Phys. Chem. 1990, 94, 5523. [Google Scholar]
- 35. Barone V., Cossi M., Tomasi J., J. Chem. Phys. 1997, 107, 3210. [Google Scholar]
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Supplementary Materials
Supporting Information
Data Availability Statement
The data that support the findings of this study are available in the supplementary material of this article.
