2005IEEE Conference Record - Abstracts. PPPS-2001 Pulsed Power Plasma Science 2001. 28th IEEE International Conference on Plasma Science and 13th IEEE International Pulsed Power Conference (Cat. No.01CH37255)Requires access

Distinction Between Streamer to Glow Transition in Atmospheric Discharge using Optical Emission Spectroscopy

Jai Hyuk Choi, Hong Koo Baik, Kie Moon Song, Yong Sik Lim

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Abstract

Summary form only given. Generally to generate glow discharge in air, sufficient numbers of seed electrons or metastables are needed. But by electronegative gases such as oxygen and water vapor etc, atmospheric discharge exists as streamer, non-uniform microdischarges. As mentioned by other references, the parameter Ptimesd in dielectric barrier discharge (DBD) controls electrical breakdown. At high gas pressure, two types of breakdown mechanisms can occur. One is called Townsend breakdown at low Ptimesd and the other breakdown is termed streamer breakdown at high Ptimesd. Therefore, we investigated optimum streamer-to-glow transition Ptimesd by controlling pressure. And to find transition Ptimesd condition, we compared the relative intensities of generated species at each discharge mode during discharge by optical emission spectroscopy analysis. Experimental results show that in case of DBD using alumina with 1 mm thickness streamer-to-glow transition occurred at the 1 torrmiddotcm condition.

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Summary form only given. Generally to generate glow discharge in air, sufficient numbers of seed electrons or metastables are needed. But by electronegative gases such as oxygen and water vapor etc, atmospheric discharge exists as streamer, non-uniform microdischarges. As mentioned by other references, the parameter Ptimesd in dielectric barrier discharge (DBD) controls electrical breakdown. At high gas pressure, two types of breakdown mechanisms can occur. One is called Townsend breakdown at low Ptimesd and the other breakdown is termed streamer breakdown at high Ptimesd. Therefore, we investigated optimum streamer-to-glow transition Ptimesd by controlling pressure. And to find transition Ptimesd condition, we compared the relative intensities of generated species at each discharge mode during discharge by optical emission spectroscopy analysis. Experimental results show that in case of DBD using alumina with 1 mm thickness streamer-to-glow transition occurred at the 1 torrmiddotcm condition.

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Available abstract

Summary form only given. Generally to generate glow discharge in air, sufficient numbers of seed electrons or metastables are needed. But by electronegative gases such as oxygen and water vapor etc, atmospheric discharge exists as streamer, non-uniform microdischarges. As mentioned by other references, the parameter Ptimesd in dielectric barrier discharge (DBD) controls electrical breakdown. At high gas pressure, two types of breakdown mechanisms can occur. One is called Townsend breakdown at low Ptimesd and the other breakdown is termed streamer breakdown at high Ptimesd. Therefore, we investigated optimum streamer-to-glow transition Ptimesd by controlling pressure. And to find transition Ptimesd condition, we compared the relative intensities of generated species at each discharge mode during discharge by optical emission spectroscopy analysis. Experimental results show that in case of DBD using alumina with 1 mm thickness streamer-to-glow transition occurred at the 1 torrmiddotcm condition.

Key concepts: Townsend discharge, Streamer discharge, Atmospheric pressure, Glow discharge, Atomic physics, Dielectric barrier discharge, Materials science, Spectroscopy

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