Abstract

This paper proposes an arc propagation model based on electric and thermal field coupling to investigate the arc propagation mechanism around composite insulators. The charge simulation method reduces the computational complexity of the electric field calculation and simulates the leakage current density and charge motion during the arc propagation. The finite difference time domain method describes the continuous variation in the thermal field generated by the leakage current density and the arc close to the insulator. Different types of heat transfer are analyzed to evaluate the arc injection and dissipation energies. The stochastic arc trajectory property is modeled by the Markov process based on electric and thermal field coupling instead of the conventional deterministic flashover model. The modified model simulates three typical arc trajectories from ignition to extinction to analyze the mutual effects of arc trajectory and arc energy. The results show that the arc trajectories that travel away from the insulator and along the leakage distance are more likely to be extinguished during propagation than the arc trajectory bridging most sheds. The consecutively rising leakage current and relatively low energy dissipation during the arc propagation process are two dominant factors that cause flashover. The model explains the mechanism of the phenomena in which the probability of arc jumping between sheds increases when the insulator surface pollution level becomes severe, which leads to a decrease in the average flashover voltage.

Highlights

  • IntroductionInsulators are used to provide electrical insulation and mechanical support for transmission lines [1]

  • The electric and thermal fields are coupled by the instantaneous field calculation and heat transfer simulation

  • ELECTRIC AND THERMAL FIELD DISTRIBUTIONS Instantaneous electric and thermal fields are calculated to create the arc trajectory and obtain the arc energy during propagation

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Summary

Introduction

Insulators are used to provide electrical insulation and mechanical support for transmission lines [1]. Arcs are likely to ignite close to high-voltage (HV) electrodes and propagate in the air close to the insulator surface [2]–[4]. Arcs initiate when the instantaneous electric field exceeds the threshold value and ionizes air [5]–[7]. Consecutive arcs are inclined to formalize a conductive path from an insulator HV electrode to a ground electrode and lead to flashover. Many researchers have studied arc propagation models on the insulator surface. Obenaus and Neumarker introduced the classic static arc propagation and flashover model in 1958 [8]. Sundararajan et al modified the static model by considering leakage current variation instantaneously during arc propa-

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