(48a) Computational Modeling of Mixture Solids for CO2 Capture Sorbents | AIChE

(48a) Computational Modeling of Mixture Solids for CO2 Capture Sorbents

Nowadays, the burning of fossil fuels is still the main energy source for the world’s economy. One consequence of the use of these fuels is the emission of huge quantities of CO2 into the atmosphere creating environmental problems such as global climate warming.1-3 In order to solve such problems, there is a need to reduce CO2 emissions into atmosphere by capturing and sequestrating CO2.4-6

For a given CO2 capture process, its optimal working conditions (CO2 pressures of pre- and after-capture, absorption/desorption temperature range (ΔTo), etc.) were fixed. However, at a given CO2 pressure, the turnover temperature (Tt) of an individual solid capture CO2 reaction is fixed. Such Tt may be outside the operating temperature range ΔTo for a particularly capture technology. In order to adjust Tt to fit the practical working through reversible chemical transformations ΔTo, we have demonstrated that by mixing different types of solids it’s possible to shift Tt to the practical operating ΔTo range.7-9 Generally, when we mix two solids A and B to form a new sorbent C, the turnover temperature of the newly resulted system (TC) is located between those of A and B (TA, TB). Here it was assumed that A is a strong CO2 sorbent while B is a weak CO2 sorbent and TA>TB. Also, we assumed that the desired operating temperature TO is between TA and TB (TA>TO>TB). Depending on the properties of A and B, we have typically three scenarios to synthesize the mixing sorbent C:

(1) TA>>TB and the A component is the key part to capture CO2. In this case since TA is higher than TO, by mixing B into A will decrease the turnover TC of the C solid to values closer to To. For example, Li2O is a very strong CO2 sorbent which forms Li2CO3. However, its regeneration from Li2CO3 only can occur at very high temperature (TA). In order to move its TA to lower temperatures, one can mix some weak CO2 sorbents (such as SiO2, ZrO2). Our results showed that in this way, the turnover T and the CO2 capture capacity of mixtures decrease with decreasing the ratio of Li2O/SiO2 or Li2O/ZrO2.7-13

(2) TA>>TB and B component is the key part to capture CO2. In this case, since TB is lower than TO, by mixing A into B will increase the turnover temperature TC of the C solid to values closer to To. For example, pure MgO (as B component) has a very high theoretical CO2 capture capacity.14 However, its turnover temperature (250 °C) is lower than the required temperature range of 300-470 °C used in warm gas clean up technology and its practical CO2 capacity is very low, and therefore, it cannot be used directly as a CO2 sorbent in this technology. Our experimental and theoretical results showed that by mixing alkali metal oxides M2O (M=Na, K, Cs, Ca) or carbonates (M2CO3) into MgO, the calculated results showed that the corresponding newly formed mixing systems have higher turnover temperatures making them useful as CO2 sorbents through the reaction MgO + CO2 + M2CO3 = M2Mg(CO3)2.15-17

(3) Both A and B components are active to capture CO2. In this case, the CO2 capacity of the mixture is the summation of those of A and B. Li2MSiO4 (M=Mg, Ca, etc.) and M2-aNaZrO3 (M, N=Li, Na, K) belong to this category. Obviously, those doped systems can be treated as mixing of three solids (Li2O:MO:SiO2, M2O:N2O:ZrO2). In this study, we focus on this type of mixing sorbents: Na2-¨»M¨»ZrO3 (M=Li, Na, K, ¨»=0, 0.5, 1.0, 1.5, 2.0).18

Our obtained results showed that by changing the mixing ratio of solid A and solid B to form mixed solid C it’s possible to shift the turnover Tt of the newly formed solid C to fit the practical CO2 capture technologies. When mixing SiO2 or ZrO2 into the strong Li2O sorbent, one can obtain a series of lithium silicates (or zirconates) with Tt lower than that of pure Li2O. By mixing oxides (Na2O, K2O, CaO) or their corresponding carbonates into MgO, the obtained mixtures exhibit different thermodynamic behaviors and their Tt are higher than that of pure MgO. Such results can be used to provide insights for designing new CO2 sorbents. Therefore, although one single material taken in isolation might not be an optimal CO2 sorbent to fit the particular needs to operate at specific temperature and pressure conditions, by mixing or doping two or more materials to form a new material, our results showed that it is possible to synthesize new CO2 sorbent formulations which can fit the industrial needs. Our results also show that computational modeling can play a decisive role for identifying materials with optimal performance.

The author thanks Drs. D. C. Sorescu, B. Zhang, K. Zhang, S. X. Li, J. K. Johnson, H. Pennline, B. Li, D. King and X. F. Wang for their help and collaborations.

 

References:

1.         D. Aaron and C. Tsouris, Separation Science and Technology, 2005, 40, 321-348.

2.         C. M. White, B. R. Strazisar, E. J. Granite, J. S. Hoffman and H. W. Pennline, J Air Waste Manag Assoc, 2003, 53, 645-715.

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4.         H. Pfeiffer and P. Bosch, Chemistry of Materials, 2005, 17, 1704-1710.

5.         E. Ochoa-Fernandez, H. K. Rusten, H. A. Jakobsen, M. Ronning, A. Holmen and D. Chen, Catalysis Today, 2005, 106, 41-46.

6.         B. Y. Li, Y. Duan, D. Luebke and B. Morreale, Applied Energy, 2013, 102, 1439-1447.

7.         Y. Duan, Physical Chemistry Chemical Physics, 2013, 15, 9752-9760.

8.         Y. Duan, D. Luebke and H. W. Pennline, International Journal of Clean Coal and Energy, 2012, 1, 1-11.

9.         Y. Duan, H. Pfeiffer, B. Li, I. C. Romero-Ibarra, D. C. Sorescu, D. R. Luebke and J. W. Halley, Physical Chemistry Chemical Physics, 2013, 15, 13538-13558.

10.       Y. Duan, J Renew Sustain Ener, 2011, 3, 013102.

11.       Y. Duan, J Renew Sustain Ener, 2012, 4, 013109.

12.       Y. Duan and K. Parlinski, Phys Rev B, 2011, 84, 104113.

13.       Y. Duan and D. C. Sorescu, Phys Rev B, 2009, 79, 014301.

14.       Y. Duan and D. C. Sorescu, J Chem Phys, 2010, 133, 074508.

15.       K. L. Zhang, X. H. S. Li, Y. Duan, D. L. King, P. Singh and L. Y. Li, International Journal of Greenhouse Gas Control, 2013, 12, 351-358.

16.       J. L. Chi, L. F. Zhao, B. Wang, Z. Li, Y. H. Xiao and Y. Duan, International Journal of Hydrogen Energy, 2014, 39, 6479-6491.

17.       K. L. Zhang, X. H. S. Li, W. Z. Li, A. Rohatgi, Y. Duan, P. Singh, L. Y. Li and D. L. King, Advanced Materials Interfaces, 2014, 1, 1400030.

18.       Y. Duan, et al,  Physical Review Applied, 2014, to be submitted.

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