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Article

CO2 Sorption and Regeneration Properties of K2CO3/Al2O3-Based Sorbent at High Pressure and Moderate Temperature

1
Department of Chemical Engineering, Kyungpook National University, Daegu 41566, Korea
2
JnK Co., Ltd., Daegu 41566, Korea
3
Department of Chemical and Environmental Engineering, University of California-Riverside, Riverside, CA 92521, USA
4
Research Institute of Advanced Energy Technology, Kyungpook National University, Daegu 41566, Korea
*
Authors to whom correspondence should be addressed.
These authors contributed equally to this work.
Appl. Sci. 2022, 12(6), 2989; https://doi.org/10.3390/app12062989
Submission received: 14 February 2022 / Revised: 3 March 2022 / Accepted: 13 March 2022 / Published: 15 March 2022

Abstract

:
In this study, the CO2 sorption mechanisms and regeneration properties of alumina-based sorbent using K2CO3 loading under high-pressure and moderate temperature conditions were examined. To investigate the mechanism of CO2 sorption, a zirconium-based sorbent was compared with an alumina-based sorbent. The CO2 capture capacities of the PAI10, 20, 30, and 40 were 32.3, 63.0, 95.4, and 124.5 mg CO2/g sorbent, respectively. To investigate the CO2 sorption mechanism of an alumina-based sorbent, we performed XRD, TG/DTG, and FTIR analyses after CO2 sorption in the presence of 10 vol% CO2 and H2O each at 200 °C and 20 atm. For PAI10–40 sorbents, KHCO3 and KAl(CO3)(OH)2 phases were observed by TG/DTG and FTIR analysis. For PAI-x sorbents, it was confirmed that the captured CO2 is desorbed completely at a temperature below 400 °C at 20 atm.

1. Introduction

Fossil fuels, coal, petroleum, and natural gas account for about 86 percent of the world’s primary energy. Greenhouse gas emissions are associated with human activities [1]; in particular, carbon dioxide (CO2) is a major greenhouse gas emitted into the atmosphere by coal-fired power plants. Improved power generation technology can help prevent global warming and climate change by reducing carbon dioxide emissions from coal-fired power plants. Currently, several technological processes for CO2 capture have been widely investigated: pre-combustion, post-combustion, and oxyfuel technology. In the case of pre-combustion process, CO2 capture occurs before combustion from the synthesis gas of an integrated gasification combined cycle (IGCC). The total pressure in the pre-combustion process is 20–70 atm, and the CO2 content is between 15 and 60%. In addition, the separation of CO2 is significantly easier because of the high CO2 partial pressure when compared with the post-combustion process [2,3,4]. The capture of CO2 using dry CO2 sorbent is one of the most efficient techniques in an IGCC plant. The ideal dry solid CO2 sorbent for applying the pre-combustion process must have a high CO2 capture capacity, a fast sorption rate, high selectivity for carbon dioxide, a stable CO2 capture capacity for multiple cycles, and excellent physical properties, due to the high pressure and moderate temperature [5,6]. Many researchers use inorganic materials such as magnesium oxide, aluminum oxide, hydrotalcite, calcium oxide, and lithium-containing material to develop a dry CO2 sorbent, applicable in the pre-combustion process in IGCC plants [7,8,9,10,11,12,13,14,15,16,17]. K2CO3-promoted alumina-based CO2 sorbents have several advantages over these materials, including a lower cost, high physical strength, and a relatively high CO2 capture capacity [18,19,20,21,22,23,24,25,26,27,28,29,30]. As a result, many researchers have been studying the interaction between carbon dioxide and alumina-based CO2 sorbents loaded with K2CO3 at relatively low temperatures of below 150 °C and low atmospheric pressure.
To understand the interaction between CO2 and K2CO3 loaded alumina-based CO2 sorbent under high-pressure and moderate temperature conditions, we investigated the CO2 capture capacity and sorption mechanism of a K2CO3 loading at 200 °C and 20 atm.
This article reports the CO2 capture capacities and absorption mechanism of PAI10–40 sorbents prepared by the impregnation method. X-ray diffraction (XRD), thermogravimetric analysis/differential thermal gravimetry (TGA/DTG), and temperature-programmed desorption (TPD) experiments were also carried out to investigate the CO2 sorption mechanism, physical change, and regeneration properties of an alumina-based sorbent, respectively after CO2 sorption at 20 atm.

2. Materials and Methods

2.1. Preparation of the CO2 Sorbent and Analysis

The aluminum oxide (Sigma Aldrich) and zirconium oxide (Sigma Aldrich) sorbent impregnated with K2CO3 (Sigma Aldrich) in this study was prepared by the impregnation method. The preparation procedure was as follows: Al2O3 and ZrO2 supports were added to aqueous solutions of K2CO3 from 10 to 40 weight % in de-ionized water. Then, the solutions were mixed with a magnetic stirrer for 24 h at room temperature. After stirring, the mixed samples were dried in a vacuum rotary evaporator [5,19,20,21,22]. These samples were calcined in an air furnace for 5 h at 500 °C. The calcination temperature was raised to 500 °C at a rate of 5 °C/min and then ground and sieved to produce a particle size range of 150–250 µm in diameter. These CO2 sorbents are denoted as PAI-x and PZIx, where P, A, Z, I, x represent potassium carbonate, aluminum oxide, zirconium oxide, the impregnation method, and the potassium carbonate loading amount, respectively.
The changes in the crystalline phase before and after CO2 sorption were examined by XRD (Philips X’PERT) using Cu Kα radiation at the Korea Basic Science Institute. TGA and DTG (SDT Q600, TA instrument) were conducted to investigate the thermal characteristics after CO2 sorption. Nitrogen gas was used as the carrier gas, and the CO2 sorbent was heated from 30 °C to 500 °C at a ramping rate of 5 °C/min. The N2 adsorption-desorption isotherms at −196 °C were recorded using a Micrometrics ASAP 2020 instrument to evaluate textural properties such as the BET surface area, pore volume, and pore size. The changes in the properties of the sorbents after CO2 sorption were investigated by Fourier transform infrared (FTIR, PerkinElmer Inc., Waltham, MA, USA). The TPD experiment was conducted in a nitrogen atmosphere, and the sample was heated from 100 °C to 450 °C at a heating rate of 2 °C/min.

2.2. Apparatus and Procedure

The CO2 capture capacity of the aluminum and zirconium oxide sorbents were conducted using a stainless steel fix-bed reactor with an outside diameter of 1 inch. The CO2 sorbent was dried for 12 h at 350 °C in a nitrogen atmosphere to remove moisture and impurities from the sorbent surface. The CO2 capture capacity of the CO2 sorbent was investigated by packing 10 g of the sorbent into a stainless steel reactor and maintaining the CO2 sorption pressure at 20 atm with a back pressure regulator. An analog pressure gauges and two digital pressure gauges were used to check pressures during CO2 sorption. The composition of feed gases was 10 vol% CO2, 10 vol% H2O and the remainder was N2. The GC column used in the analysis was a 1/8 inch stainless tube packed with Porapak Q. The outlet gas was automatically analyzed every 2 min with a thermal conductivity detector (Agilent, Santa Clara, CA, USA, 6890) equipped with an autosampler (Valco, Houston, TX, USA). The CO2 capture capacity was calculated from the CO2 breakthrough curve, which indicates the amount of CO2 absorbed until the output concentration of CO2 reaches 10 vol%, which is the same as the inlet concentration. The CO2 capture capacity is determined by the amount of CO2 absorbed per 1 g of sorbent (mg CO2/g sorbent). The CO2 capture capacity was calculated according to Equation (1) as follows:
CO 2   capture   capacity   =   ( P × V CO 2 R × T × M CO 2 × t ,   m i l l i g r a m ) / ( gram per sorbent )

3. Results

3.1. CO2 Capture Capacity of a CO2 Sorbent

Table 1 provides information on the surface area, pore volume, and pore size of ɣ-Al2O3, ZrO2, PZI30 sorbent, and PAI-x sorbents. The bare ZrO2 had a surface area of 8.05 m2/g, a pore volume of 0.02 cm3/g, and a pore size of 3.83 nm. The ɣ-Al2O3 had a surface area of 157.65 m2/g, a pore volume of 0.31 cm3/g, and a pore size of 4.91 nm. Compared with the ZrO2 support material, the surface area and pore volume of the PZI30 sorbent decreased; it might be expected that the very low surface area and pore volume of PZI30 sorbent results in poor CO2 capture capacity. When K2CO3 is loaded on the support materials, surface area decreases, whereas a significant change in pore size is not observed regardless of the K2CO3 loading amount. When the K2CO3 loading is 40 wt% (PAI40 sorbent), the surface area is reduced to about 17.3% compared with the Al2O3 support material, and the pore volume is also significantly reduced. The decrease in surface area and pore volume is caused by filling the pores or blocking the pore openings with K2CO3.
Figure 1 presents the breakthrough curves (a) and the CO2 capture capacity (b) per 1 g of sorbent for PAI10 to 40 and PZI30 sorbents in the presence of 10 vol% CO2, 10 vol% H2O, N2 balance at 200 °C and 20 atm. Figure 1b shows the CO2 capture capacities of PAI10 to 40 and PZI30 sorbents calculated from the CO2 sorption breakthrough curves shown in Figure 1a. Under high-pressure conditions (20 atm), PZI30 sorbent was used to investigate the reaction mechanism of alumina-based sorbent. PZI30 and PAI10–40 sorbents had CO2 capture capacities of 19.7 and 32.3, 63.0, 95.4, and 124.5 mg CO2/g sorbent, respectively. CO2 capture capacities of PAI-x sorbents increased with increasing K2CO3 loading. Compared with the PZI30 sorbent, the PAI30 sorbent showed a higher CO2 capture capacity.
Figure 2 shows the amount of CO2 sorption per 1 g K2CO3 as a function of the K2CO3 loading. The CO2 sorption per 1 g K2CO3 was calculated from the CO2 capture capacities of PZI30 and PAI10–40 sorbents, as shown in Figure 1. The CO2 capture capacities of PAI10–40 sorbents were maintained at approximately 311.2–323.1 mg CO2/g K2CO3. These calculated values corresponded to approximately 98–101% of the K2CO3 theoretical value of 318.4 mg CO2/g K2CO3. However, the CO2 capture capacity of PZI30 sorbent was approximately 65.7 mg CO2/g K2CO3, which is equivalent to approximately 26% of the K2CO3 theoretical value. The differences in the CO2 capture capacities of PZI30 and PAI10–40 sorbents mean that the CO2 sorbents can be absorbed through different reaction mechanisms.

3.2. Physical Characteristic Analysis after CO2 Sorption

The results of the XRD analysis of PZI30 and PAI10–40 sorbents conducted to identify the structural changes before and after CO2 sorption are shown in Figure 3. The XRD patterns of PZI30 in the fresh state show the sharp peaks of ZrO2 (JCPDS No. 83-0940) and small peaks of K2CO3 (JCPDS No. 16-0820). For PAI10–40 sorbents before CO2 sorption, only K2CO3, and ɣ-Al2O3 (JCPDS No. 10-0425) phases were observed. In the case of PAI10–40 sorbents, the peak intensity of K2CO3 increased with increasing K2CO3 loading. For PZI30 sorbent, the KHCO3 phase could not be detected after CO2 sorption in the presence of water vapor at 200 °C and 20 atm, as shown in Figure 3II. After CO2 sorption, on the other hand, the XRD patterns of PAI10–40 sorbents showed two phases: Al2O3, and KAl(CO3)(OH)2 (JCPDS No. 15-3303). XRD patterns of PAI10–40 sorbents showed no KHCO3 phase after CO2 sorption regardless of the K2CO3 loading. Based on the XRD results, the KAl(CO3)(OH)2 phase formed from K2CO3 and ɣ-Al2O3 over PAIx sorbents during CO2 sorption in the presence of 10 vol% CO2 and 10 vol% H2O at 200 °C and 20 atm.
FTIR analysis of PZI30, PAI10–40 sorbents, and pure KHCO3 reagent (Sigma-Aldrich, CAS No. 298-14-6) was conducted to confirm the formation of the KHCO3 structure after CO2 sorption in the range of 400 to 4000 cm−1. These results are shown in Figure 4. In all PZI30 and PAI10-40 sorbents, the broad peaks at a wavenumber of 3400 cm−1 (the expected bond is O-H) are attributed to H2O on the surface. In the case of PAI-x and PZI30 sorbents after CO2 sorption, the weak peaks at wavenumber 662 cm−1 (the expected bond is O1CO2), and 840 cm−1 (the expected bond is CO3) are attributed to carbonate. In addition, the strong peaks at wavenumber 1007 cm−1 (the expected bond is C-O+C∙∙∙O), 1402 cm−1 (the expected bond is O-H∙∙∙O), and 1630 cm−1 (the expected bond is C=O) are attributed to bicarbonate species [17,24,27,31]. These results are in agreement with pure KHCO3 analysis. The weak peaks at 1100 cm−1 of PAI10-40 sorbents are due to Al-O stretching and Al-O-H bending vibration, and the broad peaks at 1500 cm−1 of PAI10-40 sorbents are attributed to the H-O-H bend of absorbed H2O [32]. The FTIR results show that for the K2CO3 loaded alumina-based CO2 sorbent, the KHCO3 structure was formed during CO2 sorption in the presence of 10 vol% CO2 and 10 vol% H2O at 200 °C and 20 atm. We suggest that the KHCO3 structure is formed during CO2 sorption in the presence of water vapor at 200 °C and 20 atm [24,25,26]. According to the XRD and FTIR results, the alumina-based CO2 sorbent could form the KHCO3 phase and KAl(CO3)(OH)2 phase after CO2 sorption in the presence of water vapor at high pressure and 200 °C.
The results of TGA/DTG of PZI30 and PAI10–40 sorbents conducted to investigate the thermal properties after CO2 sorption are shown in Figure 5. PZI30 and PAI10–40 sorbents showed weight loss at temperatures between 30 °C and 100 °C. This is due to the desorption of adsorbed water on the sorbent surface. The weight loss of PZI30 sorbent after CO2 sorption at 20 atm was 5% at temperatures from 140 °C to 200 °C. The DTG peak of PZI30 sorbent showed one peak at the same temperature range as the weight loss range of TGA. Figure 3II shows that the PZI30 sorbent did not change structure after CO2 sorption at 20 atm, but the TGA/DTG confirmed that the PZI30 sorbent showed weight loss at temperatures ranging from 140 °C to 200 °C, which is attributed to CO2 desorption from the KHCO3 phase. At temperatures ranging from 140 °C to 350 °C, the weight loss of the PAI10–40 sorbents was 5.73%, 7.28%, 10.63%, and 11.61%, respectively. The DTG peak of PAI10 and 20 sorbents showed one peak between 200 °C and 350 °C due to the decomposition of the KAl(CO3)(OH)2 structure. The DTG peak of PAI30 and 40 sorbents showed two peaks at 140 °C to 200 °C and 200 °C to 350 °C, respectively. In the case of 140 °C to 200 °C, it was confirmed that the temperature range of the DTG peak was the same as for the PZI30 sorbent. In the XRD analysis for PAI30 and 40 sorbents, no KHCO3 structures were found after CO2 sorption, but we confirmed a weight loss in the temperature range from 140 °C to 200 °C. The TGA/DTG results confirmed that for the PAI10–40 sorbents, there are two CO2 sorption mechanisms involving KHCO3 and KAl(CO3)(OH)2 structures formed with increasing K2CO3 loading under water vapor at high pressure [28].
From these analysis results, it was concluded that unlike for the PZI30 sorbent, the CO2 absorption mechanism of the PAI-x sorbent was due to the formation of KHCO3 and KAl(CO3)(OH)2 structures in the presence of water vapor in the conditions of 200 °C and 20 atm.

3.3. TPD at 20 atm of PZI30 and PAI10–40 Sorbents

TPD experiments of PAI10–40 sorbents were conducted to examine the regeneration properties under 20 atm, as shown in Figure 6. In addition, a test of PZI30 sorbent was conducted to identify the decomposition temperature of the KHCO3 structure at 20 atm. The CO2 desorption of PAI-x sorbents started at 150 °C, and the desorbed CO2 peak was observed in the temperature range from 150 °C to 400 °C. The TPD results of PAI10 and 20 sorbents showed one peak between 250 °C and 350 °C, and the TPD results of PAI30 and 40 sorbents showed two peaks between 150 °C and 400 °C. In the case of low K2CO3 loading such as PAI10 and 20, the CO2 peak was produced by the decomposition of the KAl(CO3)(OH)2 structure. In the case of high K2CO3 loadings such as PAI30 and 40 sorbents, the CO2 peak was produced by the decomposition of the KHCO3 and KAl(CO3)(OH)2 structures. Particularly, the KHCO3 decomposition of PAI30 and 40 sorbents appeared at the same temperature range as the PZI30 sorbent, and the CO2 peak caused by the decomposition of KAl(CO3)(OH)2 increased with increasing K2CO3 loading. The CO2 peak caused by KHCO3 decomposition also increased due to increased K2CO3 loading. Based on the TPD results, the alumina-based CO2 sorbent was confirmed to be capable of regeneration at temperatures below 400 °C at 20 atm. This study concluded that the potassium-loaded alumina-based sorbent had a higher CO2 capture capacity than the zirconium-based sorbent due to the high surface area of alumina and the KHCO3 and KAl(CO3)(OH)2 conversion. This means that these sorbents could be used as a support and additive to prepare a sorbent with the potential for CO2 capture and regeneration under high and moderate temperature conditions.

4. Conclusions

This study examined the CO2 absorption mechanisms and regeneration properties of alumina-based sorbents according to K2CO3 loading in the presence of 10 vol% CO2, 10 vol% H2O, N2 balance at 200 °C and 20 atm. For the alumina-based sorbent loaded with K2CO3, such as PAI10–40, the CO2 capture capacities were found to be 32.3, 63.0, 95.4, 124.5 mg CO2/g sorbent, respectively, which was about 98% to 101% of the K2CO3 theoretical value. However, the CO2 capture capacity of PZI30 sorbent was 19.7 mg CO2/g sorbent, corresponding to 26% of the K2CO3 theoretical value. The higher CO2 capture capacity of PAI-x sorbent relative to the PZI30 sorbent was confirmed by an XRD, FTIR analysis, and TPD experiment. This was attributed to KHCO3 and KAl(CO3)(OH)2 structures. As for the regeneration properties measured in the TPD experiment, the PAI10 and 20 sorbents showed one peak due to the decomposition of KAl(CO3)(OH)2 at temperatures of 250 °C and 350 °C. The PAI30 and 40 sorbents showed two peaks due to the decomposition of KHCO3 and KAl(CO3)(OH)2 at temperatures of 150 °C and 400 °C. In the case of PAI-x sorbent, the KHCO3 structure generated during CO2 sorption was confirmed to have the same decomposition temperature as the KHCO3 structure generated after CO2 sorption of PZI30 sorbent. This study demonstrated that the regeneration of an alumina-based sorbent is possible at temperatures lower than 400 °C. This low regeneration energy is advantageous because the CO2 capture cost can be reduced under high pressure and moderate temperature conditions.

Author Contributions

Conceptualization, D.-Y.R., S.-C.L.; formal analysis, D.-Y.R., S.J., T.-Y.K.; investigation, J.-H.W., S.-Y.I., J.-H.L., H.-J.C., J.-K.K., J.-E.H.; supervision, S.-C.L., and J.-C.K.; writing—original draft, D.-Y.R., S.J.; writing—review and editing, S.J. and S.-C.L. All authors have read and agreed to the published version of the manuscript.

Funding

This work was supported by the Technology Innovation Program (No. 20015460) funded By the Ministry of Trade, Industry & Energy (MOTIE, Korea). This research was also supported by National R&D Program through the National Research Foundation of Korea (NRF) funded by Ministry of Science and ICT (No.2021M3I3A1084502).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. CO2 breakthrough curves (a) and CO2 capture capacities (b) of PZI30 and PAI10–40 sorbents according to K2CO3 loading at 20 atm.
Figure 1. CO2 breakthrough curves (a) and CO2 capture capacities (b) of PZI30 and PAI10–40 sorbents according to K2CO3 loading at 20 atm.
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Figure 2. CO2 capture capacities per 1 g of K2CO3 as a function of the amount of K2CO3 for PZI30 and PAI10–40 sorbents after CO2 sorption in the presence of 10 vol% CO2, 10 vol% H2O, N2 balance at 200 °C and 20 atm.
Figure 2. CO2 capture capacities per 1 g of K2CO3 as a function of the amount of K2CO3 for PZI30 and PAI10–40 sorbents after CO2 sorption in the presence of 10 vol% CO2, 10 vol% H2O, N2 balance at 200 °C and 20 atm.
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Figure 3. XRD patterns of the PZI30 and PAI10–40 sorbents before (I) and after (II) CO2 sorption according to K2CO3 loading; (△) K2CO3, (▼) ZrO2, (■) ɣ-Al2O3, (+) KAl(CO3)(OH)2.
Figure 3. XRD patterns of the PZI30 and PAI10–40 sorbents before (I) and after (II) CO2 sorption according to K2CO3 loading; (△) K2CO3, (▼) ZrO2, (■) ɣ-Al2O3, (+) KAl(CO3)(OH)2.
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Figure 4. FTIR results of PZI30 and PAI10–40 sorbents after CO2 sorption: (a) KHCO3, (b) KZI30, (c) PAI10, (d) PAI20, (e) PAI30, (f) PAI40.
Figure 4. FTIR results of PZI30 and PAI10–40 sorbents after CO2 sorption: (a) KHCO3, (b) KZI30, (c) PAI10, (d) PAI20, (e) PAI30, (f) PAI40.
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Figure 5. TG (a) and DTG (b) curves of PZI30 and PAI10–40 sorbents after CO2 sorption according to K2CO3 loading.
Figure 5. TG (a) and DTG (b) curves of PZI30 and PAI10–40 sorbents after CO2 sorption according to K2CO3 loading.
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Figure 6. TPD results at 20 atm of PZI30 and PAI10–40 sorbents after CO2 sorption at 20 atm.
Figure 6. TPD results at 20 atm of PZI30 and PAI10–40 sorbents after CO2 sorption at 20 atm.
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Table 1. Textural properties of ɣ-Al2O3, PZI30, and potassium-based alumina sorbents.
Table 1. Textural properties of ɣ-Al2O3, PZI30, and potassium-based alumina sorbents.
SampleSurface Area
(m2/g)
Pore Volume
(cm3/g)
Pore Size
(nm)
ɣ-Al2O3157.650.314.91
ZrO28.040.033.83
PZI303.920.023.82
PAI10134.980.224.32
PAI2069.670.174.32
PAI3044.260.174.32
PAI4027.370.094.31
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Ryu, D.-Y.; Jo, S.; Kim, T.-Y.; In, S.-Y.; Woo, J.-H.; Lee, J.-H.; Chae, H.-J.; Kim, J.-K.; Hwang, J.-E.; Kim, J.-C.; et al. CO2 Sorption and Regeneration Properties of K2CO3/Al2O3-Based Sorbent at High Pressure and Moderate Temperature. Appl. Sci. 2022, 12, 2989. https://doi.org/10.3390/app12062989

AMA Style

Ryu D-Y, Jo S, Kim T-Y, In S-Y, Woo J-H, Lee J-H, Chae H-J, Kim J-K, Hwang J-E, Kim J-C, et al. CO2 Sorption and Regeneration Properties of K2CO3/Al2O3-Based Sorbent at High Pressure and Moderate Temperature. Applied Sciences. 2022; 12(6):2989. https://doi.org/10.3390/app12062989

Chicago/Turabian Style

Ryu, Do-Yeong, Seongbin Jo, Tae-Young Kim, Soo-Yeong In, Jin-Hyeok Woo, Jong-Heon Lee, Ho-Jin Chae, Jae-Kuk Kim, Jae-Eun Hwang, Jae-Chang Kim, and et al. 2022. "CO2 Sorption and Regeneration Properties of K2CO3/Al2O3-Based Sorbent at High Pressure and Moderate Temperature" Applied Sciences 12, no. 6: 2989. https://doi.org/10.3390/app12062989

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