CO2 reforming of CH4 in single and double dielectric barrier discharge reactors: Comparison of discharge characteristics and product distribution
Introduction
The unprecedented development of human society has consumed enormous amount of carbon-based fossil fuels (e.g., coal, nature gas and petroleum) with the demand for energy sources continuously growing. However, the consumption of fossil fuels not only results in the depletion of these limited non-renewable sources, but also leads to the huge volumetric emissions of greenhouse gases into the atmosphere, such as CO2, CH4, N2O and SF6, which contributes to the global warming and climate change [1]. Carbon conversion and utilization (CCU) can transform CO2 into useful chemicals, bringing dual benefits for the environment and energy supply [[2], [3], [4], [5], [6]]. Among the viable solutions for CCU, CO2 reforming of CH4 has attracted significant attention [[7], [8], [9]], as it can simultaneously reduce the emission of the two main greenhouse gases (CO2 and CH4) and transform them into syngas, which can be used as a raw material to produce an array of chemicals.
However, due to the high stability of both CO2 and CH4, high temperatures (> 700 °C) are required for thermal catalytic routes to achieve a reasonable reaction rate for CO2 reforming of CH4, resulting in a highly energy-intensive process. Moreover, catalysts are found to readily deactivate due to carbon deposition and the sintering of active metals under the high-temperatures, which limits the commercial development of this process [10,11].
In this regard, non-thermal plasma (NTP) can be a promising alternative to the conventional thermal reforming process. NTP contains energetic electrons, which have an average energy of 1−10 eV. Gas molecules can be activated in NTP through ionization, dissociation and excitation processes to generate various chemically reactive species for the initiation and propagation of the chemical reactions, while the bulk gas temperature remains close to room temperature [9]. Therefore, the thermodynamically unfavorable reactions can occur at ambient conditions with the aid of NTP [[12], [13], [14], [15]]. In addition, NTP has the property of rapid start-up and shutdown, which makes it more efficient compared with the traditional thermal processes. It also has the flexibility to be combined with renewable energy sources (e.g., solar, wind or hydraulic power) for energy storage and transportation in the form of chemical energy, especially when the renewable energy is produced during peak periods, leading to a significant decrease in the overall energy cost [9,16].
Various investigations have been performed on CO2 reforming of CH4 using different NTPs, such as corona discharge [17], atmospheric pressure glow discharge (APGD) [18], microwave discharge (MW) [19], gilding arc (GlidArc) discharge [20,21] and dielectric barrier discharge (DBD) [7,12,22]. Among these NTPs, DBD has received the most attention due to its mild operating conditions, simplicity of design, suitability for scaling and its successful experience for gas cleaning and ozone generation at commercial scale [23,24]. Currently, the energy efficiency for CO2 reforming of CH4 using DBD is typically low [9]. But on the other hand, valuable liquid chemicals can be directly synthesized from the one-step process for CO2 reforming of CH4 in DBDs, especially when appropriate catalysts are employed, which is more challenging in other plasmas (e.g., MW and GAD) and thermal-catalytic processes [9,[25], [26], [27], [28], [29]]. The performance of CO2 reforming of CH4 (e.g., reactant conversion, product yield and selectivity, energy efficiency) is found to be dependent on the reactor design [[30], [31], [32]], operating parameters [7,33,34], external conditions [35,36], catalysts and plasma-catalytic configurations [27,[37], [38], [39]].
A DBD is made up of metal electrodes and at least one dielectric layer [40]. For cylindrical DBDs, the structure of the dielectric tube is also a factor influencing the physical properties and reaction performance of plasma processing. In the DBD reactor with single dielectric tube (DBD-SD), the inner metal electrode is exposed to the plasma and reactant environment, which may result in the electrode corrosion and/or erosion and influence the performance of the plasma reactor [41]. To deal with this issue, DBD with double dielectric tube (DBD-DD) have been proposed by inserting another dielectric tube to protect the metal electrode from the chemically reactive discharge region [41]. However, the energy consumption will be higher, which will lower the electrical efficiency due to the increased stray capacitance by introducing the extra dielectric layer [42,43]. Comparisons between DBD-SD and DBD-DD have been widely investigated in the plasma treatment of waste gas and water, with DBD-DDs showing better performance in most cases [44]. Limited attention has been paid to investigating CO2 reforming of CH4 using DBDs with different dielectric structures. It remains unclear how the dielectric structure affects the plasma reforming process in DBD-SD and DBD-DD. Therefore, it is important to understand the roles of the dielectric structure on the physical properties and reforming performance to gain new insights into reactor design and process optimization for plasma CO2 reforming of CH4.
In this work, we investigated the plasma CO2 reforming of CH4 in coaxial DBD-SD and DBD-DD reactors. The role of the dielectric structure was evaluated from different perspectives, including electrical characterization, optical and temperature measurements, quantified reactant conversions and product distributions, and energy efficiency for both reactant conversion and product formation. Moreover, the energy efficiencies are compared with the results in the literature.
Section snippets
Experimental system
Fig. 1 presents the experimental system for the plasma-assisted CO2 reforming of CH4, which contains a power source, a DBD reactor, an electrical diagnosis system and a product collecting and analysis system. Fig. 2 displays the structure of the DBD-SD and DBD-DD reactors. The DBD-SD was comprised of a quartz tube (20 mm i.d. × 23 mm o.d.), a stainless steel rod (diameter: 15 mm) and a stainless steel mesh (mesh opening size: 120 meshes; wire diameter: 0.07 mm; length: 10 cm), which served as
Physical properties of CO2/CH4 discharge
The physical properties of a CO2/CH4 discharge are believed to significantly affect the plasma process for CO2 reforming of CH4. Therefore, the physical properties of the discharge in the DBD-SD and DBD-DD reactors were firstly investigated in terms of electrical characteristics, discharge images and operating temperature. Fig. 3 presents the voltage and current waveforms (including the applied voltage, the measured total current and the gap voltage) in both cases at different discharge powers.
Conclusions
Plasma CO2 reforming of CH4 has been performed in both DBD-SD and DBD-DD reactors. The physical properties of the CO2/CH4 discharge in both cases are studied in term of electrical characterization, optical and temperature measurement. The plasma reforming performance is then compared according to the reactant conversion, product distribution and energy efficiency. In both reactors, typical filamentary microdischarges are observed, but the discharge strength is intensified in the DBD-SD,
Author statement
Danhua Mei: Conceptualization, Methodology, Investigation, Formal analysis, Writing - Original Draft.
Gehui Duan: Investigation, Formal analysis, Data curation, Validation.
Junhui Fu: Methodology, Formal analysis, Visualization.
Shiyun Liu: Methodology, Formal analysis, Validation
Renwu Zhou: Formal analysis, Visualization
Rusen Zhou: Formal analysis, Visualization
Zhi Fang: Conceptualization, Supervision, Resources, Writing- Reviewing and Editing, Project administration.
Patrick J. Cullen:
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
The authors would like to thank for the financial support from the National Natural Science Foundation of China (Grant No. 51807087), the Natural Science Foundation of Jiangsu Province of China (Grant No. BK20180705), the Project of Six Talent Peak High-Level Talent Team of Jiangsu Province (Grant No. TD-JNHB-006), the Postgraduate Research & Practice Innovation Program of Jiangsu Province of China (Grant No. KYCX20_1078), and the State Key Laboratory of Electrical Insulation and Power Equipment
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