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October 9, 2025Plasma Sources Science and Technology0 citations

Repetitively nanosecond pulsed discharge along dielectric surfaces: discharge and surface charge dynamics and local streamer-to-filament transition

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XZXinlei ZhengHZHaotian ZhengZSZongxiao Sun

Key Points

  • The study reveals distinct phases in a three-electrode surface discharge, including streamer and reverse breakdown.
  • Simulation results align qualitatively with experimental data on discharge current waveforms and electric field features.
  • A 2D fluid model combined with kinetic modeling effectively characterizes surface charge accumulation and transition mechanisms.
  • The local streamer-to-filament transition is driven by the accumulation of active species in regions of high electric fields.

Abstract

Abstract The discharge and surface charge dynamics, as well as the local streamer-to-filament transition of a three-electrode surface discharge under repetitive nanosecond pulses with a frequency of 1 kHz at atmospheric pressure, are studied through experiments and simulations. Evolutions of plasma morphology and electric field vector, as obtained by an ICCD camera and an improved E-FISH method, respectively, are utilized to analyze discharge dynamics. A 2D fluid model combined with a 0D kinetic model is established to study the accumulation behavior of surface charge and mechanism of the local streamer-to-filament transition. The simulation results demonstrate a qualitative agreement with the experimental measurements on the discharge evolution, waveforms of discharge current and key features of the electric field. The results show that a three-electrode surface discharge includes three discharge phases: the primary streamer, local enhanced discharge and reverse breakdown. The local enhanced discharge occurs near the high-voltage (HV) electrode, characterized by a local streamer-to-filament transition and subsequent emission belt parallel to the edge of HV electrode, after the primary streamer bridges the two electrodes. The local streamer-to-filament transition is attributed to the local accumulation of active species with a lower threshold energy in the high field region (~ 25 kV/cm) similar to that of the secondary streamer in pin-plane discharges. The emission belt is formed by the high-density charge spot at the filament head, a phenomenon attributable to charge migration under the influence of an applied electric field. The spatial non-uniformity of plasma channel is a general feature in non-uniform field discharges and is a key process that induces the discharge mode transition.

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Cite This Study

Zheng et al. (2025) studied this question.

synapsesocial.com/papers/68e70da790569dd607ee5a38https://doi.org/10.1088/1361-6595/ae105a
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