“…R is the active resistance of the plasma, C = S/(4πL) is the capacity of the space between the DEL filled with plasma, where S is the characteristic cross-sectional area of the plasma arc, L is the characteristic dimension of the plasma, = −ω pe 2 /ν 2 en is the dielectric constant of the plasma), R1 is the active resistance resulting in the heating of the electrodes, connected with the flow of thermoelectrons and electrons that have passed from the plasma through the DEL to the electrodes, C1 = S1/(4πd) is the capacity of the DEL, where S1 is the area of the electrodes, d = 3r D (the radius of the Debye) is the characteristic longitudinal size of DEL. The value of R is determined by the formula R = L/σS, where L is the characteristic dimension of the plasma, S is the characteristic crosssectional area of the plasma arc, and σ = ω pe 2 /4πν en is the conductivity of the plasma [12]. The resistance and impedances of this circuit are calculated according to this formula and are equal to R = 6 Ω, Z C = 10 Ω, Z C1 = 400 Ω, where Z C = 1/iωC is the impedance capacitance C. Since R is comparable with Z C , there are two components of the electric current in the plasma: the conduction current and the bias current.…”