9 research outputs found

    INTERACTION OF HELIUM AND ARGON PLASMA JETS ARRAYS

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    We discuss results from computational investigations of the properties of jets arrays operated in He and Ar. He or Ar is flowing through the tubes of the jets into ambient humid air. We show that jet-jet interactions primarily depend on the properties of plasma forming gas through the tubes. For the helium array, the jets at edges of the array tend to divert while for Ar array plasma propagates more directionally.223-22

    DYNAMICS OF SUBNANOSECOND BREAKDOWN OF HIGH-PRESSURE GASES

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    Recent results on computational study of subnanosecond discharge formation are presented. Their comparison with available experimental data is given. The effects of various factors governing the discharge characteristics are discussed.130-13

    DYNAMICS OF SUBNANOSECOND BREAKDOWN OF HIGH-PRESSURE GASES

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    130-130Recent results on computational study of subnanosecond discharge formation are presented. Their comparison with available experimental data is given. The effects of various factors governing the discharge characteristics are discussed

    INTERACTION OF HELIUM AND ARGON PLASMA JETS ARRAYS

    No full text
    223-223We discuss results from computational investigations of the properties of jets arrays operated in He and Ar. He or Ar is flowing through the tubes of the jets into ambient humid air. We show that jet-jet interactions primarily depend on the properties of plasma forming gas through the tubes. For the helium array, the jets at edges of the array tend to divert while for Ar array plasma propagates more directionally

    Wafer edge uniformity considering ion inertia in single- and dual-frequency capacitively coupled discharges

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    Streamer properties of pulsed corona discharge in water

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    Pulsed discharges in water are investigated to obtain knowledge of fundamental aspects of their behavior. The electrical energy dissipated in one pulse is measured with a calorimetric method to be 80 mJ. From photographs detailed information on streamer structure is obtained. In a gap of 20 mm at a pulse voltage of 20 kV the average length of the streamer in tap water is 5 mm, in deionized water it is 11 mm. The number of streamers is higher in tap water. The propagation velocity of the streamers is determined using photomultipliers and is in the order of 106 mis
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