Abstract:A method of resonant near field microwave probing is developed for contactless diagnostics of a high pressure plasma. The efficiency of this method in measuring the parameters of the plasma of an rf capac itive discharge in argon under atmospheric pressure is demonstrated. The experimental results are compared with the data obtained using the independent method, the microwave radiation "cutoff," and with theoretical estimates.
“…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.…”
The report discusses the use of a new type of plasma source of hydrogen plasma based on a RF (13.56 MHz) arc discharge of atmospheric pressure between two electrodes. This discharge was used for hydrogen reduction of the tetrafluorides of silicon, boron and molybdenum. As a result of the studies, the main regularities of the hydrogen reduction process were established and the main synthesized products were determined. Samples of carbides of silicon, boron and molybdenum were prepared.
“…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.…”
The report discusses the use of a new type of plasma source of hydrogen plasma based on a RF (13.56 MHz) arc discharge of atmospheric pressure between two electrodes. This discharge was used for hydrogen reduction of the tetrafluorides of silicon, boron and molybdenum. As a result of the studies, the main regularities of the hydrogen reduction process were established and the main synthesized products were determined. Samples of carbides of silicon, boron and molybdenum were prepared.
“…The most frequently used techniques for determining the electron density are optical diagnostics, including Thomson scattering method, continuum radiation, atomic line Stark broadening, and so on [12,14,15]. Microwave diagnostic [16][17][18][19][20][21] is an effective method to measure various plasmas with plasma density below 10 13 cm −3 , however, it is invalid to measure the plasma of higher density due to the limited frequency of microwave [22].…”
The diagnostic of high-density hot plasma is a challenging task due to its high temperature and electron density. Arc plasma is one of the typical hot density plasmas, and its diagnosis is the key to develop its new applications. In this paper, the temperature and density distributions of welding plasmas with different discharge currents are numerically simulated based on a Tungsten Inert Gas Arc Welding model, and the electron density distributions are calculated. Then propagation properties of broadband terahertz (THz) waves in the modeling arc jets are calculated by the finite difference time domain method. These results not only provide a preliminary theoretical guidance for in-depth understanding the problems of blackout in re-entry communication, but also develop a new idea for the terahertz diagnostic of plasma with high density.
“…The method of resonance near-field sounding [1][2][3] is used successfully to study electrodynamic properties of various substances in the microwave range. Depending on the operating frequency, either oscillatory circuits with lumped parameters or distributed resonance systems can be used as measurement sensors.…”
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