1. Mode transition induced by back‐breakdown of the gliding arc and its influence factors
- Author
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Haochen Huang, Ruobing Zhang, and Tianshu Yang
- Subjects
arcs (electric) ,Work (thermodynamics) ,Materials science ,arc speed ,lcsh:QC501-721 ,Energy Engineering and Power Technology ,electric field strength ,arc velocity ,Arc (geometry) ,nonequilibrium plasma generation method ,mode transition ,Electric field ,lcsh:Electricity ,Electrical and Electronic Engineering ,minimum gap breakdown ,electrode opening angle ,back-breakdown phenomenon ,plasma sources ,electrode parameters ,Mode (statistics) ,Plasma ,Mechanics ,applied voltage ,electrodes ,Volumetric flow rate ,gliding arc ,gas flow rate ,plasma flow ,Electrode ,lcsh:Electrical engineering. Electronics. Nuclear engineering ,lcsh:TK1-9971 ,Voltage - Abstract
Gliding arc is a mostly used non-equilibrium plasma generation method whose characteristic is affected by the back-breakdown phenomenon. Mode transition induced by back-breakdown of the gliding arc is studied in this work and effects of gas flow rate, applied voltage, electrode parameters on mode transition were studied. Experimental results show that there are two typical modes during the development of the gliding arc. Mode A comprises periodicitical development of the arc from the minimum gap breakdown to the longest extinguishment, while the arc in mode B continues to produce a back-breakdown at the ends of the electrodes. As the flow rate descends, the gliding arc gradually changes from mode A to B. It is the decrease of the arc velocity caused by lower flow rate leads to the occurrence of back-breakdown, which generates mode B. Smaller electrode opening angle, shorter length and wider minimum gap reduce the gliding speed, so that arc is more likely to enter mode B. As the applied voltage is increased, enhancing of the electric field strength on the breakdown path of the back-breakdown and thickening of the arc's diameter allow the gliding arc to enter mode B at a higher arc speed.
- Published
- 2020
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