• High Power Laser and Particle Beams
  • Vol. 33, Issue 6, 065011 (2021)
Yuanyuan Jiang, Yanhui Wang, Caihui Gao, and Dezhen Wang
Author Affiliations
  • Key Laboratory of Materials Modification by Laser, Ion and Electron Beams (Ministry of Education), School of Physics, Dalian University of Technology, Dalian 116024, China
  • show less
    DOI: 10.11884/HPLPB202133.210148 Cite this Article
    Yuanyuan Jiang, Yanhui Wang, Caihui Gao, Dezhen Wang. Numerical study of atmospheric pressure Ar plasma jets under different electrode structures[J]. High Power Laser and Particle Beams, 2021, 33(6): 065011 Copy Citation Text show less
    Discharge device and simulation domain used in our calculation
    Fig. 1. Discharge device and simulation domain used in our calculation
    Calculation results of the neutral gas flow
    Fig. 2. Calculation results of the neutral gas flow
    Temporal and spatial evolution of electron density for the first and the second electrode device
    Fig. 3. Temporal and spatial evolution of electron density for the first and the second electrode device
    Radial and axial electron density evolutions for different electrode device
    Fig. 4. Radial and axial electron density evolutions for different electrode device
    Evolution of the axial and radial electric field in the ionization head when the ionization wave propagates inside the tube for different electrode device
    Fig. 5. Evolution of the axial and radial electric field in the ionization head when the ionization wave propagates inside the tube for different electrode device
    Evolution of the axial and radial electric field in the ionization head when the ionization wave propagates outside the tube for different electrode device
    Fig. 6. Evolution of the axial and radial electric field in the ionization head when the ionization wave propagates outside the tube for different electrode device
    Spatial distribution of reactive species density at 50 ns for two electrode devices
    Fig. 7. Spatial distribution of reactive species density at 50 ns for two electrode devices
    Evolution reactive species density on the axis for two electrode devices
    Fig. 8. Evolution reactive species density on the axis for two electrode devices
    Temporal-spatial evolution of electron density for bare needle electrode device
    Fig. 9. Temporal-spatial evolution of electron density for bare needle electrode device
    Axial electron density evolution for the bare needle electrode device
    Fig. 10. Axial electron density evolution for the bare needle electrode device
    Evolution of the electric field during the propagation of the ionization wave under the bare needle electrode device
    Fig. 11. Evolution of the electric field during the propagation of the ionization wave under the bare needle electrode device
    Axial plasma potential distribution at different moments for the bare needle electrode (solid line) and needle electrode with insulation dielectric (dashed line)
    Fig. 12. Axial plasma potential distribution at different moments for the bare needle electrode (solid line) and needle electrode with insulation dielectric (dashed line)
    boundaryvelocity conditionbackground species condition
    Note: ${u_{{r}}}$ and ${u_{ {\textit{z}} } }$ are the velocity in the axial and radial directions, respectively. ${{n}}$ is the unit vector pointing toward the boundary.
    BC
    BJ,CI,IH,HD,GF
    DE
    KG
    EF0.1 MPa
    Table 1. [in Chinese]
    boundaryelectrostatic conditionspecies condition
    Note: “ring” is the high voltage electrode.
    BC
    BJ, CIHDEq.(13)Eq.(8), (9), (10), (11)
    KG
    AKV
    GF0——
    EF0
    ring0——
    Table 2. [in Chinese]
    indexreactionrate coefficientsthreshold energy/eVreference
    1e+Ar→e+ArBOLSIG+/[17]
    2e+Ar→e+Ar*BOLSIG+11.5[17]
    3e+Ar→2e+Ar+BOLSIG+15.8[17]
    4e+N2→2e+N2+BOLSIG+15.58[17]
    5e+N2→e+2N BOLSIG+13[17]
    6e+N2→e+N2(C3π) BOLSIG+11.03[17]
    7e+O2→2e+O2+BOLSIG+12.06[17]
    8e+O2→e+2O BOLSIG+5.58[17]
    9e+O2→O2BOLSIG+/[17]
    10Ar*+Ar*→e+Ar+Ar+6.4×10−16 (m−3/s) /[17]
    11Ar*+Ar→Ar+Ar 2.09×10−21 (m−3/s) /[17]
    12Ar*+N2→Ar+2N 3.6×10−17 (m−3/s) /[17]
    13Ar*+O2→Ar+2O 2.1×10−16 (m−3/s) /[17]
    Table 3. [in Chinese]
    Yuanyuan Jiang, Yanhui Wang, Caihui Gao, Dezhen Wang. Numerical study of atmospheric pressure Ar plasma jets under different electrode structures[J]. High Power Laser and Particle Beams, 2021, 33(6): 065011
    Download Citation