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Synthesis of n-butanol-rich C3+ alcohols by direct CO2 hydrogenation over a stable Cu–Co tandem catalystoa mark
  • Irshad, Muhammad ;
  • Chun, Hee Joon ;
  • Khan, Muhammad Kashif ;
  • Jo, Heuntae ;
  • Kim, Seok Ki ;
  • Kim, Jaehoon
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30

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Publication Year
2024-01-01
Publisher
Elsevier B.V.
Citation
Applied Catalysis B: Environmental, Vol.340
Keyword
ButanolC3 +alcoholsCatalyst stabilityCO2 conversionCobaltCopper
Mesh Keyword
A-stableBimetallicsC3 +alcoholCatalyst stabilityCO2 conversionCu-co catalystsDirect conversionHeterogeneous catalystN-butanol]+ catalyst
All Science Classification Codes (ASJC)
CatalysisEnvironmental Science (all)Process Chemistry and Technology
Abstract
The direct conversion of CO2 into liquid fuels and chemical heterogeneous catalysts is considered a promising route to mitigate global warming issues. However, the production of n-butanol-rich C3+ alcohol from CO2 remains a significant challenge. Herein, we demonstrate that a Cu-rich bimetallic Cu–Co catalyst can achieve an unprecedentedly high space-time yield (STYC3+OH) of 80.8 mg g−1 h−1. The decoration of Co nanoparticles onto the dendritic Cu substrate established a crucial balance between CHx and CH3O* and regulated C–C coupling, which is a prerequisite for C3+ alcohol synthesis. We provide new mechanistic insights into n-butanol synthesis involving the C–O bond dissociation of an acetaldehyde intermediate on the interfacial Cu–Co site and subsequent C–C bond formation on the Cu site. Furthermore, the Cu–Co catalyst exhibited exceptional stability up to 1000 h by effectively suppressing re-oxidation and carbon deposition. The Cu–Co catalyst has great potential for large-scale CO2 hydrogenation to C3+ alcohol owing to its high selectivity and remarkable stability.
ISSN
0926-3373
Language
eng
URI
https://dspace.ajou.ac.kr/dev/handle/2018.oak/33639
DOI
https://doi.org/10.1016/j.apcatb.2023.123201
Fulltext

Type
Article
Funding
This study received funding from the Korea Institute of Energy Technology Evaluation and Planning (KETEP) under the Ministry of Trade, Industry & Energy, Republic of Korea (No. 20224C10300010 ) and a National Research Council of Science & Technology (NST) grant from the Korean government ( MSIT ) (No. CAP21012–100 ). Some experiments were performed at the 8 C and 8A2 synchrotron beamlines of the Pohang Accelerator Laboratory (PAL, Republic of Korea) under Contract Nos. 2023–1st-8 C-032 and 2021–3rd-8A2–002, respectively.This study received funding from the Korea Institute of Energy Technology Evaluation and Planning (KETEP) under the Ministry of Trade, Industry & Energy, Republic of Korea (No. 20224C10300010) and a National Research Council of Science & Technology (NST) grant from the Korean government (MSIT) (No. CAP21012–100). Some experiments were performed at the 8 C and 8A2 synchrotron beamlines of the Pohang Accelerator Laboratory (PAL, Republic of Korea) under Contract Nos. 2023–1st-8 C-032 and 2021–3rd-8A2–002, respectively.
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