Features of the Structure of Spark Channels in a Near-Cathode Region

Features of the generation of a highly ionized plasma from a tip cathode after the electrical breakdown of a millimeter air discharge gap at atmospheric pressure have been studied using picosecond laser probing at a wavelength of 532 nm. It has been found that the transformation of a micron-sized cathode spot to a growing spark channel is accompanied by the formation of a spherical plasma region in the base of the spark channel in the near-cathode region. The electron density in this region, which is about 100 μm in diameter, decreases to 3 × 1019 cm–3 in the center and increases to (5–6) × 1019 cm–3 in its shell with a thickness of about 20 μm. It has been shown that the growth of the subsequent spark channel is governed by a strong ionization front formed at the boundary of the expanding spherical plasma region in 1 ns after the gap breakdown. It has been assumed that the formation of the spherical plasma region in the near-cathode region affects the subsequent development of the microstructure of the electric spark.

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Publication Details

Journal
Journal of Experimental and Theoretical Physics Letters
Published
2024-10-01
DOI
https://doi.org/10.1134/s0021364024602951
Citations
3
Primary Topic
Plasma Applications and Diagnostics
Type
article
Field-Weighted Citation Impact
1.21
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article

Features of the Structure of Spark Channels in a Near-Cathode Region

E. V. Parkevich
3 citations
Journal of Experimental and Theoretical Physics Letters
Plasma Applications and Diagnostics
1.21
article

Features of the Structure of Spark Channels in a Near-Cathode Region

E. V. Parkevich
article en
3 citations

Abstract

Features of the generation of a highly ionized plasma from a tip cathode after the electrical breakdown of a millimeter air discharge gap at atmospheric pressure have been studied using picosecond laser probing at a wavelength of 532 nm. It has been found that the transformation of a micron-sized cathode spot to a growing spark channel is accompanied by the formation of a spherical plasma region in the base of the spark channel in the near-cathode region. The electron density in this region, which is about 100 μm in diameter, decreases to 3 × 1019 cm–3 in the center and increases to (5–6) × 1019 cm–3 in its shell with a thickness of about 20 μm. It has been shown that the growth of the subsequent spark channel is governed by a strong ionization front formed at the boundary of the expanding spherical plasma region in 1 ns after the gap breakdown. It has been assumed that the formation of the spherical plasma region in the near-cathode region affects the subsequent development of the microstructure of the electric spark.

Journal of Experimental and Theoretical Physics LettersVol. 120(7)
P.N. Lebedev Physical Institute of the Russian Academy of Sciences (RU)
Openalex Percentile: Top 19%
Plasma Applications and Diagnostics
1.21
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