Shock discontinuity in high-current vacuum arcs

Evgeny Gidalevich*, Samuel Goldsmith, Raymond L. Boxman

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

Abstract

The deceleration of a cathode plasma jet caused by interaction with a secondary ion cushion at the anode is analyzed. Copper electrodes are considered. The secondary ions are assumed to be sputtered and/or reflected from the anode. The sputtering coefficient was found by integrating the energy distribution of the cathode spot plasma jet, weighed by the copper-copper self-sputtering yield. The system of equations of motion and continuity for the primary plasma jet and the secondary ions was solved numerically for arc current densities in the range of (3 × 10 4-5 × 10 5) A/m 2. It was found that for an interelectrode gap of 2 cm, and a secondary ion velocity of 10 3 m/s, there is no upper limit for the current density for continuous jet motion. For secondary ion velocities < 0.25 × 10 3 m/s, the upper limit is 10 5 A/m 2, above which a shock front forms between the primary and secondary plasma.

Original languageEnglish
Pages (from-to)700-703
Number of pages4
JournalIEEE Transactions on Plasma Science
Volume29
Issue number5 I
DOIs
StatePublished - Oct 2001

Funding

FundersFunder number
Israel Ministry of Absorption
Israel Science Foundation

    Keywords

    • Hydrodynamicity of plasma
    • Shock waves
    • Vacuum arc

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