Investigation of the AC Plasma Torch Working Conditions for the Plasma Chemical Applications

14th High-Tech Plasma Processes Conference

Safronov, A.A.^1 ; Vasilieva, O.B.^1 ; Dudnik, J.D.^1 ; Kuznetsov, V.E.^1 ; Shiryaev, V.N.^1 ; Subbotin, D.I.^1 ; Pavlov, A.V.^1

Institute for Electrophysics and Electric Power of Russian Academy of Sciences (IEE RAS), Dvortsovaya emb. 18, St.-Petersburg

191186, Russia^1

关键词: Alternating current;    Chemical applications;    Chemical technologies;    Continuous operation;    Dispersed materials;    Electrodynamic forces;    Nano-scale materials;    Plasma-chemical process;   

Others  :  https://iopscience.iop.org/article/10.1088/1742-6596/825/1/012013/pdf
DOI  :  10.1088/1742-6596/825/1/012013

来源: IOP

【 摘 要 】

The presented design and parameters of a three-phase AC plasma torch with the power up to 500 kW, flow rate of air 30-50 g/s (temperature up to 5000 K) could be used in different plasma chemical processes. Range of measured plasma temperature is 3500-5000 K. The paper presents investigations of the plasma torch operation modes for its application in plasma chemical technologies. Plasma chemical technologies for various purposes (processing, destruction of various wastes, including technological and hazardous waste, conversion or production of chemicals to obtain nanoscale materials, etc.) are very promising in terms of the process efficiency. Their industrial use is difficult due to the lack of inexpensive and reliable plasma torches providing the desired level of temperature, enthalpy of the working gas and other necessary conditions for the process. This problem can be solved using a considered design of a three-phase alternating current plasma torch with power of 150-500 kW with working gas flow rate of 30-50 g/s with mass average temperature up to 5000K on the basis of which an industrial plasma chemical plant can be created. The basis of the plasma torch operation is a railgun effect that is the principle of arc movement in the field of its own current field. Thanks to single supply of power to the arc, arcs forming in the discharge chamber of the plasma torch move along the electrodes under the action of electrodynamic forces resulting from the interaction of the arc current with its own magnetic field. Under the condition of the three-phase supply voltage, arc transits from the electrode to the electrode with change in the anodic and cathodic phases with frequency of 300 Hz. A special feature of this design is the ability to organize the movement of the arc attachment along the electrode, thus ensuring an even distribution of the thermal load and thus achieve long time of continuous operation of the plasma torch. The parameters of the plasma jet of the plasma torch and the single-phase three-phase plasma injector for use in a plasma-chemical unit for production of nano-dispersed materials are described in the paper.