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Suresh BASNET, Atit DEUJA, Raju KHANAL. Kinetic-theory-based investigation of electronegative plasma–wall transition with two populations of electrons[J]. Plasma Science and Technology, 2021, 23(3): 35002-035002. DOI: 10.1088/2058-6272/abde1d
Citation: Suresh BASNET, Atit DEUJA, Raju KHANAL. Kinetic-theory-based investigation of electronegative plasma–wall transition with two populations of electrons[J]. Plasma Science and Technology, 2021, 23(3): 35002-035002. DOI: 10.1088/2058-6272/abde1d

Kinetic-theory-based investigation of electronegative plasma–wall transition with two populations of electrons

  • Kinetic theory has been employed to investigate the magnetized plasma-sheath structure and its
    characteristics in the presence of more than one species of negatively charged particles: hot electrons,
    cold electrons, and negative ions. The cold electrons and negative ions are considered to obey a
    Maxwellian distribution, whereas the hot electrons follow a truncated Maxwellian distribution. The
    Bohm sheath condition has been extended for the case of more than one species of negatively
    charged particles, in which the concentration of hot electrons has a crucial role in achieving the
    Bohm velocity. The thermal motion of hot electrons is much higher compared to cold electrons and
    negative ions, such that the variation of hot electron concentrations and the temperature ratio of hot to
    cold electrons play a key role in the determination of the plasma-sheath parameters: particle densities,
    electrostatic potential, the flow of positive ions towards the wall, and sheath thickness. We have
    estimated the deviation of the resultant drift velocity of positive ions on the plane perpendicular to the
    wall from the parallel component at the presheath–sheath interface. It is found that the deviation
    between the two velocity components increases with an increase in the obliqueness of the magnetic
    field. Furthermore, the results obtained from the kinetic trajectory simulation model are compared
    with the results obtained using a fluid model; the results are qualitatively similar, although the
    potential varies by less than 4% in terms of the magnitude at the wall.
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