Mechanism of CO2 Cracking by Gliding Arc
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摘要: 建立了一维滑动弧裂解CO2的反应机理模型. 利用对流冷却的特征频率计算横向气流对流引起的等离子体组分损失. 将等离子体密度和温度的数值模拟结果与文献中滑动电弧等离子体反应器的实验数据进行了对比,吻合较好. 模拟结果表明,滑动弧裂解CO2会产生大量O和O2等活性助燃粒子以及可燃的CO. 随着对流冷却特征频率的增加,放电过程中最大电子数密度和电子温度减小,CO2转化率下降. 在整个CO2裂解机制中e+CO2→e+CO+O的贡献最大,准稳态中贡献率为90.63%,瞬态中贡献率为98.43%. 反应CO+O+M→CO2+M对CO2生成的贡献率最大. 在实际应用中,为提高CO2转化率,可以通过增大放电电流,增大e+CO2→e+CO+O的反应速率,同时选择合适的气体流量,避免过大的速度引起CO2转化率下降.Abstract: In this paper, a one-dimensional gliding arc model and the detailed mechanism of CO2 cracking reaction were established. The characteristic frequency of convection cooling was used to calculate the plasma component loss caused by cross flow convection. The calculated plasma density and plasma temperature were compared with the experimental data of gliding arc plasma reactor in the literature. The calculation results show that a large number of active combustion supporting particles such as O and O2 and combustible CO gas will be produced during CO2 cracking by gliding arc. With the increase of the characteristic frequency of convection cooling, the maximum electron number density and electron temperature decrease, and the CO2 conversion rate decreases. The contribution rate of e+CO2→e+CO+O is the largest in the whole mechanism of CO2 cracking, which is 90.63% in quasi steady state and 98.43% in transient state. The contribution rate of CO+O+M→CO2+M to CO2 generation is the largest. In practical application, in order to improve the conversion rate of CO2, the discharge current and the reaction rate of e+CO2→e+CO+O should be appropriately increased. The gas flow rate should be appropriately selected to avoid the decline of CO2 conversion rate caused by excessive speed.
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Key words:
- CO2 cracking /
- gliding arc /
- non-equilibrium plasma /
- reaction mechanism
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表 1 模型中包含的粒子
Table 1. Particles contained in the model
neutral species and radicals charged particles CO2, CO, O, C, O2 CO2+, e 表 2 模型中电子碰撞反应
Table 2. Electron collision reactions
表 3 模型中中性粒子反应
Table 3. Neutral particle reactions
reaction reaction rate reference No. M+CO2→M+CO+O 4.39×10-7exp
(-65 000/Tg)[6] R11 O+CO2→O2+CO 7.77×10-12exp
(-16 600/Tg)[6] R12 CO+O+M→CO2+M 8.2×10-34exp
(-1 560/Tg)[27] R13 O2+CO→CO2+O 1.28×10-12exp
(-12 800/Tg)[6] R14 C+CO2→CO+CO 1.0×10-15 [28] R15 O2+C→CO+O 3.0×10-11 [27] R16 CO+M→C+O+M 1.52×10-4exp
(-12 800/Tg)[29] R17 C+O+M→CO+M 2.14×10-29exp
(-2 114/Tg)[26] R18 O+O+M→O2+M 1.27×10-32exp
(-170/Tg)[30] R19 表 4 各反应对CO2裂解贡献率
Table 4. Contribution rate of each reaction to CO2 cracking
No. reaction relative contribution rate R7 e+CO2→e+CO+O 90.63% R11 M+CO2→M+CO+O < 0.01% R12 O+CO2→O2+CO 0.11% R15 C+CO2→CO+CO 9.26% 表 5 各反应对CO2裂解贡献率
Table 5. Contribution rate of each reaction to CO2 cracking
No. reaction relative contribution rate R7 e+CO2→e+CO+O 98.43% R11 M+CO2→M+CO+O < 0.01% R12 O+CO2→O2+CO < 0.01% R15 C+CO2→CO+CO 1.57% -
[1] 赵黛青, 夏亮, 何立波. 低热值燃料稳定燃烧的研究现状与进展[J]. 世界科技研究与发展, 2005, 27(5): 33-39. doi: 10.3969/j.issn.1006-6055.2005.05.006Zhao D Q, Xia L, He L B. Research and development of stable combustion using low heat value fuel[J]. World Sci-Tech R&D, 2005, 27(5): 33-39(in Chinese). doi: 10.3969/j.issn.1006-6055.2005.05.006 [2] 刘日新, 刘七新, 饶文涛. 高炉煤气在连续加热炉上的应用[J]. 工业加热, 2003, 32(5): 57-58. doi: 10.3969/j.issn.1002-1639.2003.05.018Liu R X, Liu Q X, Rao W T. The applications of blast furnace gas to continuous-heating furnaces[J]. Industrial Heating, 2003, 32(5): 57-58(in Chinese). doi: 10.3969/j.issn.1002-1639.2003.05.018 [3] 王松岭, 董君, 陈海平, 等. 高炉煤气燃气轮机联合循环的发展现状与前景[J]. 燃气轮机技术, 2005, 18(4): 22-24, 38. doi: 10.3969/j.issn.1009-2889.2005.04.005Wang S L, Dong J, Chen H P, et al. The development situation and prospects of blast-furnace-gas-fired gas turbine combined cycle[J]. Gas Turbine Technology, 2005, 18(4): 22-24, 38(in Chinese). doi: 10.3969/j.issn.1009-2889.2005.04.005 [4] 李沛泽. 低热值燃料点火与助燃方法研究[D]. 哈尔滨: 哈尔滨工程大学, 2019.Li P Z. Research on low heat value fuel ignition and combustion enhancement[D]. Harbin: Harbin Engineering University, 2019(in Chinese). [5] Czernichowski A. Gliding arc: applications to engineering and environment control[J]. Pure and Applied Chemi-stry, 1994, 66(6): 1301-1310. doi: 10.1351/pac199466061301 [6] Fridman A, Nester S, Kennedy L A, et al. Gliding arc gas discharge[J]. Progress in Energy and Combustion Science, 1999, 25(2): 211-231. doi: 10.1016/S0360-1285(98)00021-5 [7] Richard F, Cormier J M, Pellerin S, et al. Gliding arcs fluctuations and arc root displacement[J]. High Tempe-rature Material Processes: An International Quarterly of High-Technology Plasma Processes, 1997, 1(2): 239-248. doi: 10.1615/HighTempMatProc.v1.i2.80 [8] Du C M, Mo J M, Tang J, et al. Plasma reforming of bio-ethanol for hydrogen rich gas production[J]. Applied Energy, 2014, 133: 70-79. doi: 10.1016/j.apenergy.2014.07.088 [9] Tu X, Whitehead J C. Plasma dry reforming of methane in an atmospheric pressure AC gliding arc discharge: co-generation of syngas and carbon nanomaterials[J]. International Journal of Hydrogen Energy, 2014, 39(18): 9658-9669. doi: 10.1016/j.ijhydene.2014.04.073 [10] Czernichowski A, Nassar H, Ranaivosoloarimanana A, et al. Spectral and electrical diagnostics of gliding arc[J]. Acta Physica Polonica A, 1996, 89(5/6): 595-603. [11] Mutaf-Yardimci O, Saveliev A V, Fridman A A, et al. Thermal and nonthermal regimes of gliding arc discharge in air flow[J]. Journal of Applied Physics, 2000, 87(4): 1632-1641. doi: 10.1063/1.372071 [12] Tu X, Gallon H J, Whitehead J C. Dynamic behavior of an atmospheric argon gliding arc plasma[J]. IEEE Transactions on Plasma Science, 2011, 39(11): 2900-2901. doi: 10.1109/TPS.2011.2150247 [13] Kustova E V, Nagnibeda E A. Transport properties of a reacting gas mixture with strong vibrational and chemical nonequilibrium[J]. Chemical Physics, 1998, 233(1): 57-75. doi: 10.1016/S0301-0104(98)00092-5 [14] Kustova E V, Nagnibeda E A, Chauvin A H, et al. State-to-state nonequilibrium reaction rates[J]. Chemical Physics, 1999, 248(2/3): 221-232. [15] Rusanov V D, Fridman A A, Sholin G V. The physics of a chemically active plasma with nonequilibrium vibrational excitation of molecules[J]. Soviet Physics Uspekhi, 1981, 24(6): 447-474. doi: 10.1070/PU1981v024n06ABEH004884 [16] Hokazono H, Obara M, Midorikawa K, et al. Theoretical operational life study of the closed-cycle transversely excited atmospheric CO2 laser[J]. Journal of Applied Physics, 1991, 69(10): 6850-6868. doi: 10.1063/1.347675 [17] Aerts R, Martens T, Bogaerts A. Influence of vibrational states on CO2 splitting by dielectric barrier discharges[J]. The Journal of Physical Chemistry C, 2012, 116(44): 23257-23273. doi: 10.1021/jp307525t [18] 吴帆. 等离子体法分解CO2的反应动力学研究[D]. 大连: 大连理工大学, 2017.Wu F. The reaction kinetics study of CO2 decomposition in plasma[D]. Dalian: Dalian University of Technology, 2017(in Chinese). [19] Pietanza L D, Colonna G, D'Ammando G, et al. Time-dependent coupling of electron energy distribution function, vibrational kinetics of the asymmetric mode of CO2 and dissociation, ionization and electronic excitation kinetics under discharge and post-discharge conditions[J]. Plasma Physics and Controlled Fusion, 2016, 59(1): 014035. [20] Wang W Z, Berthelot A, Kolev S, et al. CO2 conversion in a gliding arc plasma: 1D cylindrical discharge model[J]. Plasma Sources Science and Technology, 2016, 25(6): 065012. doi: 10.1088/0963-0252/25/6/065012 [21] Pellerin S, Richard F, Chapelle J, et al. Heat string model of bi-dimensional DC Glidarc[J]. Journal of Physics D: Applied Physics, 2000, 33(19): 2407-2419. doi: 10.1088/0022-3727/33/19/311 [22] Richard F, Cormier J M, Pellerin S, et al. Physical study of a gliding arc discharge[J]. Journal of Applied Physics, 1996, 79(5): 2245-2250. doi: 10.1063/1.361188 [23] Lowke J J, Phelps A V, Irwin B W. Predicted electron transport coefficients and operating characteristics of CO2-N2-He laser mixtures[J]. Journal of Applied Physics, 1973, 44(10): 4664-4671. doi: 10.1063/1.1662017 [24] Lawton S A, Phelps A V. Excitation of the b1Σg+ state of O2 by low energy electrons[J]. Chemical Physic, 1978, 69(3): 1055-1068. [25] Land J E. Electron scattering cross sections for momentum transfer and inelastic excitation in carbon mo-noxide[J]. Journal of Applied Physics, 1978, 49(12): 5716-5721. doi: 10.1063/1.324589 [26] Beuthe T G, Chang J S. Chemical kinetic modelling of non-equilibrium Ar-CO2 thermal plasmas[J]. Japanese Journal of Applied Physics, 1997, 36: 4997. doi: 10.1143/JJAP.36.4997 [27] Cenian A, Chernukho A, Borodin V, et al. Modeling of plasma-chemical reactions in gas mixture of CO2 lasers I. gas decomposition in pure CO2 glow discharge[J]. Contributions To Plasma Physics, 1994, 34(1): 25-37. doi: 10.1002/ctpp.2150340105 [28] Cenian A, Chernukho A, Borodin V. Modeling of plasma-chemical reactions in gas mixture of CO2 lasers. Ⅱ. theoretical model and its verification[J]. Contributions To Plasma Physics, 1995, 35(3): 273-296. doi: 10.1002/ctpp.2150350309 [29] Mick H J, Burmeister M, Roth P. Atomic resonance absorption spectroscopy measurements on high-temperature CO dissociation kinetics[J]. AIAA Journal, 1993, 31(4): 671-676. doi: 10.2514/3.11602 [30] Hadj-Ziane S, Held B, Pignolet P, et al. Ozone generation in an oxygen-fed wire-to-cylinder ozonizer at atmospheric pressure[J]. Journal of Physics D: Hadj-Ziane, 1992, 25(4): 677-685. doi: 10.1088/0022-3727/25/4/014 [31] Wu A J, Yan J H, Zhang H, et al. Study of the dry methane reforming process using a rotating gliding arc reactor[J]. International Journal of Hydrogen Energy, 2014, 39(31): 17656-17670. doi: 10.1016/j.ijhydene.2014.08.036 [32] Zhao T L, Xu Y, Song Y H, et al. Determination of vibrational and rotational temperatures in a gliding arc discharge by using overlapped molecular emission spectra[J]. Journal of Physics D: Applied Physics, 2013, 46(34): 345201. doi: 10.1088/0022-3727/46/34/345201 [33] Gangoli S P, Gutsol A F, Fridman A A. A non-equilibrium plasma source: magnetically stabilized gliding arc discharge: Ⅰ. Design and diagnostics[J]. Plasma Sources Science and Technology, 2010, 19(6): 065003. doi: 10.1088/0963-0252/19/6/065003