Acta Physica Sinica, Volume. 69, Issue 16, 165202-1(2020)

Two-dimensional simulation of dynamic characteristics of N2–O2 corona discharge at micro scale

Yu Chai1... Ni Zhang1, Jie Liu1, Ning Yin1, Shu-Lin Liu1, and Jing-Yuan Zhang1,23,* |Show fewer author(s)
Author Affiliations
  • 1College of Electrical and Control Engineering, Xi'an University of Science and Technology, Xi'an 710054, China
  • 2Postdoctoral Station of Mechanical Engineering, Xi’an University of Science and Technology, Xi’an 710054, China
  • 3Jiangsu Province Laboratory of Mining Electric and Automation, China University of Mining and Technology, Xuzhou 221008, China
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    Figures & Tables(12)
    Discharge schematic diagram.
    Electron density maps at different times: (a) t1 = 0.1 ns; (b) t2 = 0.3 ns; (c) t3 = 1 ns; (d) t4 = 100 ns; (e) t5 = 150 ns; (f) t6 = 200 ns.
    Curves of electric field strength with time at different positions on the central axis.
    Time-varying curve of applied voltage on the negative plate.
    Axial distributions of positive and negative ion density at different times: (a) t1 = 100 ns; (b) t2 = 140 ns; (c) t3 = 150 ns; (d) t4 = 200 ns
    Curve of discharge current density with time.
    Curve of the electric field strength at the tip with time.
    Variation curve of electric field strength with time at the tip under different pole spacing.
    The intensity of the electric field at the different poles: (a) All the time; (b) stable time.
    The increment of field strength at the tips of different pole spaces.
    • Table 1.

      N2-O2 plasma chemical reactions.

      N2-O2等离子体化学反应

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      Table 1.

      N2-O2 plasma chemical reactions.

      N2-O2等离子体化学反应

      类型序号反应式反应速率参考文献
      电子碰撞反应R1${\rm{e}} + {{\rm{N}}_{\rm{2}}} \to {\rm{e}} +{\rm{ e}} +{\rm{ N}}_{\rm{2}}^{{ + }} $f (ε) [29]
      R2${\rm{e}} + {{\rm{O}}_2} \to {\rm{e}} + {\rm{e}} + {\rm{O}}_2^ + $f (ε) [29]
      R3${\rm{e}} + {\rm{O}}_4^ + \to 2{{\rm{O}}_2}$1.4 × 10–42(300/Te)0.5 mol·s–1[29]
      R4${\rm{e}} + {\rm{O}}_2^ + \to 2{\rm{O}}$2.0 × 10–13(300/Te) mol·s–1[29]
      R5${\rm{e}} + 2{{\rm{O}}_2} \to {{\rm{O}}_2} + {\rm{O}}_2^ - $2.0 × 10–41(300/Te) mol·s–1·m–6[29]
      重粒子反应R6${\rm{O}}_{\rm{2}}^{{ + }}{{ + }}{{\rm{O}}_{\rm{2}}}{{ + }}{{\rm{N}}_{\rm{2}}} \to {\rm{O}}_{\rm{4}}^{{ + }}{{ + }}{{\rm{N}}_2}$2.4 × 10–42 mol·s–1·m–6[29]
      R7${{\rm{N}}_{\rm{2}}}{\rm{O}}_{\rm{2}}^{{ + }}{{ + }}{{\rm{O}}_{\rm{2}}} \to {\rm{O}}_{\rm{4}}^{{ + }}{{ + }}{{\rm{N}}_2}$1.0 × 10–15 mol·s–1·m–3[29]
      R8${{\rm{N}}_{\rm{2}}}{\rm{O}}_{\rm{2}}^{{ + }}{{ + }}{{\rm{N}}_{\rm{2}}} \to {\rm{O}}_2^{{ + }}{{ + 2}}{{\rm{N}}_{\rm{2}}}$4.3 × 10–10 mol·s–1·m–3[29]
      R9${\rm{O}}_{\rm{2}}^{{ + }}{{ + 2}}{{\rm{N}}_{\rm{2}}} \to {{\rm{N}}_{\rm{2}}}{\rm{O}}_{\rm{2}}^{{ + }}{{ + }}{{\rm{N}}_{\rm{2}}}$9.0 × 10–43 mol·s–1·m–6[29]
      R10${{\rm{O}}_{\rm{2}}} +{\rm{ N}}_{\rm{2}}^{{ + }} \to {{\rm{N}}_{\rm{2}}} +{\rm{ O}}_{\rm{2}}^{{ + }}$6.0 × 10–17 mol·s–1·m–3[29]
      R11${\rm{N}}_{\rm{2}}^{{ + }}{{ + }}{{\rm{N}}_{\rm{2}}}{{ + }}{{\rm{O}}_{\rm{2}}} \to {{\rm{O}}_{\rm{2}}} + {\rm{N}}_{\rm{4}}^{{ + }}$5.0 × 10–41 mol·s–1·m–6[29]
      R12${{\rm{O}}_{\rm{2}}}+ {\rm{ N}}_{\rm{4}}^{{ + }} \to {\rm{2}}{{\rm{N}}_{\rm{2}}}+ {\rm{ O}}_{\rm{2}}^{{ + }}$2.5 × 10–16 mol·s–1·m–3[29]
      R13${\rm{2}}{{\rm{N}}_{\rm{2}}}+ {\rm{ N}}_{\rm{2}}^{{ + }} \to {{\rm{N}}_{\rm{2}}}+ {\rm{ N}}_{\rm{4}}^{{ + }}$5.0 × 10–41 mol·s–1·m–6[29]
      R14${\rm{O}}_{\rm{2}}^{{ + }}+ {\rm{ 2}}{{\rm{O}}_{\rm{2}}} \to {\rm{O}}_{\rm{4}}^{{ + }}{{ + }}{{\rm{O}}_{\rm{2}}}$2.4 × 10–42 mol·s–1·m–6[29]
      R15${\rm{O}}_{\rm{4}}^{{ + }}+ {\rm{ O}}_{\rm{2}}^ - \to {\rm{3}}{{\rm{O}}_{\rm{2}}}$1.0 × 10–13 mol·s–1·m–3[29]
      R16${\rm{O}}_{\rm{4}}^{{ + }}+ {\rm{ O}}_{\rm{2}}^ - {{ + }}{{\rm{N}}_2} \to {\rm{3}}{{\rm{O}}_{\rm{2}}} + {{\rm{N}}_{\rm{2}}}$2.0 × 10–17 mol·s–1·m–6[29]
      R17${\rm{O}}_{\rm{4}}^{{ + }}+ {\rm{ O}}_{\rm{2}}^ - {{ + }}{{\rm{O}}_{\rm{2}}} \to {\rm{3}}{{\rm{O}}_{\rm{2}}}{{ + }}{{\rm{O}}_{\rm{2}}}$2.0 × 10–17 mol·s–1·m–6[29]
      R18${\rm{O}}_{\rm{2}}^{{ + }}+ {\rm{ O}}_{\rm{2}}^ - {{ + }}{{\rm{O}}_{\rm{2}}} \to {\rm{2}}{{\rm{O}}_{\rm{2}}}{{ + }}{{\rm{O}}_{\rm{2}}}$22.0 × 10–17 mol·s–1·m–6[29]
      R19${\rm{O}}_{\rm{2}}^{{ + }}+ {\rm{ O}}_{\rm{2}}^ - {{ + }}{{\rm{N}}_{\rm{2}}} \to {\rm{2}}{{\rm{O}}_{\rm{2}}}{{ + }}{{\rm{N}}_{\rm{2}}}$2.0 × 10–17 mol·s–1·m–6[29]
    • Table 2.

      Surface reactions.

      表面反应

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      Table 2.

      Surface reactions.

      表面反应

      序号反应式针电极(阴极)板电极(阳极)
      γεi/eV γεi/eV
      R20${\rm{e}} + {\rm{N}}_{\rm{2}}^{{ + }} \to {{\rm{N}}_{\rm{2}}}$0.05400
      R21${\rm{e }}+{{\rm{N}}_{\rm{2}}}{\rm{O}}_{\rm{2}}^{{ + }} \to {{\rm{N}}_{\rm{2}}}{{ + }}{{\rm{O}}_{\rm{2}}}$0.05400
      R22${\rm{e}} + {\rm{N}}_{\rm{4}}^{{ + }} \to {\rm{2}}{{\rm{N}}_{\rm{2}}}$0.05400
      R23${\rm{e}} + {\rm{O}}_{\rm{2}}^{{ + }} \to {{\rm{O}}_{\rm{2}}}$0.05400
      R24${\rm{e}} +{\rm{ O}}_{\rm{4}}^{{ + }} \to 2{{\rm{O}}_{\rm{2}}}$0.05400
      R25${\rm{e}} +{\rm{ O}}_{\rm{2}}^{{ - }} \to {{\rm{O}}_{\rm{2}}}$0000
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    Yu Chai, Ni Zhang, Jie Liu, Ning Yin, Shu-Lin Liu, Jing-Yuan Zhang. Two-dimensional simulation of dynamic characteristics of N2–O2 corona discharge at micro scale [J]. Acta Physica Sinica, 2020, 69(16): 165202-1

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    Paper Information

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    Received: Jan. 14, 2020

    Accepted: --

    Published Online: Jan. 4, 2021

    The Author Email:

    DOI:10.7498/aps.69.20200095

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