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Flashover voltage of porcelain insulator under various pollution distributions: Experiment and modeling

Salem, Ali Ahmed and Lau, Kwan Yiew and Abdul Malek, Zulkurnain and Al-Gailani, Samir A. and Tan, Chee Wei (2022) Flashover voltage of porcelain insulator under various pollution distributions: Experiment and modeling. Electric Power Systems Research, 208 (NA). pp. 1-13. ISSN 0378-7796

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Official URL: http://dx.doi.org/10.1016/j.epsr.2022.107867

Abstract

The current work investigates the flashover voltage of an 11 kV porcelain insulator against changes in the location of the dry band, salt deposit density, humidity, non-uniform pollution degree, and polluted surface area. Generally, the flashover voltage of the polluted insulator dropped sharply compared to that of the clean insulator. Specifically, under salt deposit density (SDD) of 0.03 mg/cm2, the flashover voltages of scenarios A (full pollution), B (dry band 1), C (dry band 2), and D (dry band 3) decrease by 26%, 19%, 10%, and 2%, respectively, compared to 43.70 kV flashover voltage of the clean insulator. With an increase in SDD, the flashover voltage under all scenarios decreases steadily, with the median flashover voltage of scenario A being the lowest at 17.52 kV. The flashover voltage under all scenarios also varies with changes in the humidity level, non-uniform pollution degree and polluted surface area. Subsequently, an artificial neural network (ANN) and fuzzy logic (FL) hybrid model is proposed to predict the flashover voltage and condition of the insulator, where the model successfully yields the insulator condition index between 0 and 100% to indicate the pollution severity of the insulator.

Item Type:Article
Uncontrolled Keywords:Artificial neural network, Flashover voltage, Fuzzy logic, Pollution distribution, Porcelain insulator
Subjects:T Technology > TK Electrical engineering. Electronics Nuclear engineering
Divisions:Electrical Engineering
ID Code:103539
Deposited By: Widya Wahid
Deposited On:14 Nov 2023 06:40
Last Modified:14 Nov 2023 06:40

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