Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure

Spectroscopic analysis was conducted on microwave (MW) argon (Ar) plasma, promoted by a charcoal bed, during the dry reforming of methane at atmospheric pressure. High-resolution spectroscopic analysis revealed five prominent peaks near the CH (B2Σ− → X2П) region when methane dissociation occurred i...

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Main Authors: Xiuqiang Zhang, Nobusuke Kobayashi, Yoshinori Itaya
Format: Article
Language:English
Published: Taylor & Francis Group 2024-12-01
Series:Journal of Chemical Engineering of Japan
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Online Access:https://www.tandfonline.com/doi/10.1080/00219592.2024.2401003
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author Xiuqiang Zhang
Nobusuke Kobayashi
Yoshinori Itaya
author_facet Xiuqiang Zhang
Nobusuke Kobayashi
Yoshinori Itaya
author_sort Xiuqiang Zhang
collection DOAJ
description Spectroscopic analysis was conducted on microwave (MW) argon (Ar) plasma, promoted by a charcoal bed, during the dry reforming of methane at atmospheric pressure. High-resolution spectroscopic analysis revealed five prominent peaks near the CH (B2Σ− → X2П) region when methane dissociation occurred in Ar plasma. The most prominent peak corresponded to the energy excitation of Ar (II) ions at 388.03 nm, and the atomic transition process was 3s23p4(3P)4d4D1/2 → 3s23p4(3P)4p4D°1/2. This process might be enhanced by interactions with intermediates or free radicals produced during the methane dissociation reaction. The ion temperature of the Ar (II) in MW plasma was calculated from the intensity of any two of the five characteristic peaks. Due to different transition processes, the temperature of ions also exhibited significant variation, consistent with the characteristics of a non-equilibrium plasma. The Ar (II) ion temperature reached as high as 18,000 K. According to the Boltzmann plot, the relative error of the ion temperature in this study was less than 0.02 when the ion temperature was lower than 10,000 K, and the error corresponding to the highest ion temperature was also less than 0.05, indicating that the temperature of the Ar (II) ion describing a particular energy state can be determined with reasonable accuracy. Furthermore, activated Ar (II) ions inducing methane dissociation through collisions are considered to be the primary cause of methane dissociation.
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spelling doaj-art-8b15b17fa40a4f8c834974c44d23ab4a2024-12-19T15:13:29ZengTaylor & Francis GroupJournal of Chemical Engineering of Japan0021-95921881-12992024-12-0157110.1080/00219592.2024.2401003Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric PressureXiuqiang Zhang0Nobusuke Kobayashi1Yoshinori Itaya2Environmental and Renewable Energy Systems, Gifu University, 1-1 Yanagido, Gifu City 501-1193, JapanEnvironmental and Renewable Energy Systems, Gifu University, 1-1 Yanagido, Gifu City 501-1193, JapanEnvironmental and Renewable Energy Systems, Gifu University, 1-1 Yanagido, Gifu City 501-1193, JapanSpectroscopic analysis was conducted on microwave (MW) argon (Ar) plasma, promoted by a charcoal bed, during the dry reforming of methane at atmospheric pressure. High-resolution spectroscopic analysis revealed five prominent peaks near the CH (B2Σ− → X2П) region when methane dissociation occurred in Ar plasma. The most prominent peak corresponded to the energy excitation of Ar (II) ions at 388.03 nm, and the atomic transition process was 3s23p4(3P)4d4D1/2 → 3s23p4(3P)4p4D°1/2. This process might be enhanced by interactions with intermediates or free radicals produced during the methane dissociation reaction. The ion temperature of the Ar (II) in MW plasma was calculated from the intensity of any two of the five characteristic peaks. Due to different transition processes, the temperature of ions also exhibited significant variation, consistent with the characteristics of a non-equilibrium plasma. The Ar (II) ion temperature reached as high as 18,000 K. According to the Boltzmann plot, the relative error of the ion temperature in this study was less than 0.02 when the ion temperature was lower than 10,000 K, and the error corresponding to the highest ion temperature was also less than 0.05, indicating that the temperature of the Ar (II) ion describing a particular energy state can be determined with reasonable accuracy. Furthermore, activated Ar (II) ions inducing methane dissociation through collisions are considered to be the primary cause of methane dissociation.https://www.tandfonline.com/doi/10.1080/00219592.2024.2401003Microwave plasmaCH4 dissociationIon temperatureSpectroscopic measurementInteractions
spellingShingle Xiuqiang Zhang
Nobusuke Kobayashi
Yoshinori Itaya
Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
Journal of Chemical Engineering of Japan
Microwave plasma
CH4 dissociation
Ion temperature
Spectroscopic measurement
Interactions
title Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
title_full Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
title_fullStr Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
title_full_unstemmed Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
title_short Optical Analysis of Dry Reforming of Methane in Microwave-Induced Plasma at Atmospheric Pressure
title_sort optical analysis of dry reforming of methane in microwave induced plasma at atmospheric pressure
topic Microwave plasma
CH4 dissociation
Ion temperature
Spectroscopic measurement
Interactions
url https://www.tandfonline.com/doi/10.1080/00219592.2024.2401003
work_keys_str_mv AT xiuqiangzhang opticalanalysisofdryreformingofmethaneinmicrowaveinducedplasmaatatmosphericpressure
AT nobusukekobayashi opticalanalysisofdryreformingofmethaneinmicrowaveinducedplasmaatatmosphericpressure
AT yoshinoriitaya opticalanalysisofdryreformingofmethaneinmicrowaveinducedplasmaatatmosphericpressure