Abstract

Propagation of positive streamers in dielectric liquids, modeled by the electron avalanche mechanism, is simulated in a needle–plane gap. The streamer is modeled as an RC-circuit where the channel is a resistor and the extremities of the streamer have a capacitance towards the plane. The addition of the RC-model introduces a time constant to the propagation model. Increase in capacitance as a streamer branch propagates reduces its potential, while conduction through the streamer channel increases its potential, as a function of the time constant of the RC-system. Streamer branching also increases the capacitance and decreases the potential of the branches. If the electric field within the streamer channel exceeds a threshold, a breakdown occurs in the channel, and the potential of the streamer is equalized with the needle electrode. This is interpreted as a re-illumination. According to this model, a low conductive streamer branch can propagate some distance before its potential is reduced to below the propagation threshold, and then the RC time constant controls the streamer propagation speed. Channel breakdowns, or re-illuminations, are less frequent when the channels are conductive and more frequent for more branched streamers.

Highlights

  • When dielectric liquids are exposed to a sufficiently strong electric field, partial discharges occur and a gaseous channel called a streamer is formed

  • Propagation of positive streamers in dielectric liquids, modeled by the electron avalanche mechanism, attribution to the is simulated in a needle–plane gap

  • Electron avalanches can be important for streamer propagation, but the results showed a relatively low propagation speed and a low degree of branching

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Summary

Introduction

When dielectric liquids are exposed to a sufficiently strong electric field, partial discharges occur and a gaseous channel called a streamer is formed. The first simulations of streamer breakdown in liquids applied Monte Carlo methods on a lattice [12], and have since been expanded, for instance by including conductivity [13]. Another model use the electric network model to calculate the electric field in front of the streamer, which is used to evaluate the possibility for streamer growth or branching [14]. Our previous work describes a model for propagation of 2nd mode positive streamers in dielectric liquids governed by electron avalanches [16, 17]. The channel is included by considering its conductivity as well as capacitance between the streamer and the plane

Electron avalanche model
Single channel streamer at constant speed
Numerical simulation results
Findings
Discussion
Conclusion
Full Text
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