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Frontiers in Energy

ISSN 2095-1701

ISSN 2095-1698(Online)

CN 11-6017/TK

Postal Subscription Code 80-972

2018 Impact Factor: 1.701

Front. Energy    2023, Vol. 17 Issue (4) : 545-554    https://doi.org/10.1007/s11708-023-0867-7
RESEARCH ARTICLE
Enhanced performance of oxygen vacancies on CO2 adsorption and activation over different phases of ZrO2
Juntian NIU1(), Cunxin ZHANG1, Haiyu LIU1, Yan JIN1, Riguang ZHANG2
1. College of Electrical and Power Engineering, Taiyuan University of Technology, Taiyuan 030024, China
2. State Key Laboratory of Clean and Efficient Coal Utilization, Taiyuan University of Technology, Taiyuan 030024, China
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Abstract

The effect of oxygen vacancies on the adsorption and activation of CO2 on the surface of different phases of ZrO2 is investigated by density functional theory (DFT) calculations. The calculations show that the oxygen vacancies contribute greatly to both the adsorption and activation of CO2. The adsorption energy of CO2 on the c-ZrO2, t-ZrO2 and, m-ZrO2 surfaces is enhanced to 5, 4, and 3 folds with the help of oxygen vacancies, respectively. Moreover, the energy barrier of CO2 dissociation on the defective surfaces of c-ZrO2, t-ZrO2, and m-ZrO2 is reduced to 1/2, 1/4, and 1/5 of the perfect surface with the assistance of oxygen vacancies. Furthermore, the activation of CO2 on the ZrO2 surface where oxygen vacancies are present, and changes from an endothermic reaction to an exothermic reaction. This finding demonstrates that the presence of oxygen vacancies promotes the activation of CO2 both kinetically and thermodynamically. These results could provide guidance for the high-efficient utilization of CO2 at an atomic scale.

Keywords CO2 activation      oxygen vacancies      ZrO2      different phases     
Corresponding Author(s): Juntian NIU   
About author:

* These authors contributed equally to this work.

Online First Date: 03 March 2023    Issue Date: 29 August 2023
 Cite this article:   
Juntian NIU,Cunxin ZHANG,Haiyu LIU, et al. Enhanced performance of oxygen vacancies on CO2 adsorption and activation over different phases of ZrO2[J]. Front. Energy, 2023, 17(4): 545-554.
 URL:  
https://academic.hep.com.cn/fie/EN/10.1007/s11708-023-0867-7
https://academic.hep.com.cn/fie/EN/Y2023/V17/I4/545
Crystals and surface Space group DFTa (In this study) X-rayb (Experimental measurement)
a b c β a b c β
c-ZrO2 (111) Fm3m 5.14 5.14 5.14 5.09 5.09 5.09
t-ZrO2 (101) P42/nmc 3.64 3.64 5.31 3.64 3.64 5.27
m-ZrO2 (−111) P21/c 5.23 5.27 5.42 100.05 5.17 5.23 5.34 99.2
Tab.1  Lattice parameters of c-ZrO2, t-ZrO2, and m-ZrO2 from X-ray crystallographic and their DFT optimized structures
Phase Defective sites Adsorption energy /eV
C O
c −3.38 −3.81
t −2.29 −3.82
m VO1 −2.33 −3.31
VO2 −2.68 −3.61
VO3 −2.45 −3.43
Tab.2  Comparison of adsorption energy of C atoms and O atoms on defective surfaces
Fig.1  Adsorption configurations of CO2 on perfect and defective surfaces.
Phase Defective sites Adsorption energy/eV
Defective surface Perfect surface
c −0.996 −0.198
t −1.028 −0.226
m VO1 −0.999 −0.306
VO2 −1.003
VO3 −0.728
Tab.3  Adsorption energy of CO2 adsorbed on perfect and defective surfaces of ZrO2, respectively
Fig.2  CO2 adsorption energy.
Fig.3  Transition state model for activation process of CO2 on perfect and defective surfaces (Oxygen atoms adsorbed on the surface are labeled O2 and O atoms retained in CO are labeled O1.).
Phase Defective sites Energy barrier/eV Reaction heat/eV Mulliken charge/e
Perfect surface Defective Perfect surface Defective surface Perfect surface Defective surface
c 1.671 0.463 1.511 −0.592 −0.230 −0.653
t 1.713 0.352 1.347 −0.663 −0.247 −0.667
m VO1 1.593 0.758 1.171 −0.306 −0.188 −0.464
VO2 0.312 −0.499 −0.701
VO3 0.436 −0.619 −0.585
Tab.4  Energy barrier, reaction heat, and Mulliken atomic charge of CO2 activation on perfect and defective surfaces
Fig.4  Electron density of CO2 binding on surface of different phases of ZrO2.
Fig.5  CO2 dissociation energy barrier.
Fig.6  Energy change curve (a value of Max means that the presence of oxygen vacancies can reduce the energy barrier to a maximum of 1/5 of the initial, and a value of Min means that the reduction is a factor of 1/2 similarly.).
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