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The dependence of the plasma plume current on the object condition is investigated by atmospheric pressure non-thermal equilibrium argon plasma. When processing with plasma, the flow of plasma current changes depending on the condition of the object. In the case of metal object with grounded condition, the plasma current was independent of the surface area and electrical conductivity of the metal object. While, in the case of metal object with floating condition, the plasma current was dependent on the surface area of the metal object, but not on the electrical conductivity of the metal object. When an object is grounded, the closed circuit is fixed with plasma, object, and ground-line, and then the current flow follows Ohm’s law. Because the ground-line is longer than the plasma plume length and the scale length of the object, the plasma current is independent of the characteristics of the metal object. When the object is in a floating condition, the divergence of the charge stored in the object to the atmosphere depends on the surface area of the object because it follows Gauss’s law.
The dependence of the plasma plume current on the object condition is investigated by atmospheric pressure non-thermal equilibrium argon plasma. When processing with plasma, the flow of plasma current changes depending on the condition of the object. In the case of metal object with grounded condition, the plasma current was independent of the surface area and electrical conductivity of the metal object. While, in the case of metal object with floating condition, the plasma current was dependent on the surface area of the metal object, but not on the electrical conductivity of the metal object. When an object is grounded, the closed circuit is fixed with plasma, object, and ground-line, and then the current flow follows Ohm’s law. Because the ground-line is longer than the plasma plume length and the scale length of the object, the plasma current is independent of the characteristics of the metal object. When the object is in a floating condition, the divergence of the charge stored in the object to the atmosphere depends on the surface area of the object because it follows Gauss’s law.
The main findings of this study are that the plasma propagation state changes with the force equilibrium relationship between the driving force due to the electromagnetic field and neutral gas flow. The plasma propagation transitions from a continuous state to a discontinuous state when plasma emission light intensity changes. The plasma emission light intensity changes suddenly as the applied voltage frequency varies. The frequency at which plasma emission light changes is inversely proportional to the dynamic pressure with the flow velocity of neutral gas. The plasma with strong light emission at high frequency propagates continuously, while that with weak light emission at low frequency propagates discontinuously. Because the plasma current with strong light emission is larger than that with weak light emission, the plasma charge quantity—the amount of plasma generated—increases. Consequently, when the plasma quantity is enough to exist continuously as a group, the plasma group propagates in space with time variations like a stationary wave. However, when the plasma quantity is inadequate to exist continuously, the plasma group propagates through the space discontinuously like a bullet state.
In many plasma applications, the plasma current, which is determined by the plasma density and drift velocity, is an important parameter when investigating the induced phenomenon and its effects. However, it is unclear which physical parameters are responsible for regulating the current. Plasma is generated by a balance between the driving and restricting forces. The driving force originates from the electric and magnetic fields, and the restricting force originates from collisions between different species (electrons, ions, and neutral particles). When the electric field fluctuates over time, the pressure of the driving force is generated. The pressure of the driving force depends on the square of the electric field and the reciprocal of the repetition frequency. The pressure of the restricting force depends on the gas flow velocity and the collision frequency. When electrons and/or ions flow with the flowing neutral gas, a plasma current is generated from flowing charged particles. The magnitude of the plasma current is linearly proportional to the pressure caused by the driving force, and the variation in the plasma current depends on the pressure caused by the restricting force. In addition, the plasma current varies with the applied period of the voltage. Consequently, the plasma charge, which is the time integral of the plasma current, shows a linear relationship with the driving force and is thus regulated by the force balance between the driving and restricting forces. Therefore, the plasma current value and its generation time are regulated by the strength, applied period, and repetition frequency of the applied voltage and the neutral gas flow velocity.
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