高电压技术2024，Vol.50Issue(5)：1997-2008,中插13,13.DOI:10.13336/j.1003-6520.hve.20232342
低频交流电压下低密度聚乙烯的空间电荷特性
Space Charge Characteristics of Low-density Polyethylene at Low-frequency AC Voltages
摘要
Abstract
Fractional frequency transmission technology has gradually become one of the mainstream solutions for real-izing carbon neutrality and long-distance transmission of offshore wind power.However,the research on electrical equipment in the context of high-voltage FFTS is rarely available,and the effects of frequency change on the characteris-tics of cable insulation materials need to be studied in depth.To this end,a pulsed electroacoustic test system capable of rapid detection was used to investigate the space charge characteristics of low-density polyethylene materials at crossover voltages with different field strengths and temperatures as well as the effect of frequency change on the charge build-up behavior.The results show that the charge accumulation is obvious when the field strength and temperature conditions are more severe;while the charge accumulation becomes more remarkable with the decrease of frequency,and the charge growth rate increases significantly when the frequency decreases below 20 Hz.Based on this,a bipolar carrier model ap-plied under alternating electric field was developed,and the experimental observations were rationalized by simulation calculations to reveal the mechanism of the influence of electric field,temperature and frequency on the space charge be-havior.The research methodology and results can provide theoretical supports for the frequency choice and optimal design of cable insulation in frequency-divided transmission systems.关键词
碳中和/海上风电/分频输电/低密度聚乙烯/空间电荷/电场分布Key words
carbon neutrality/offshore wind power/fractional frequency transmission/low-density polyethylene/space charge/electric field distribution引用本文复制引用
魏鼎欣,刘鹏,谢宗良,庞曦,许天蕾,彭宗仁..低频交流电压下低密度聚乙烯的空间电荷特性[J].高电压技术,2024,50(5):1997-2008,中插13,13.基金项目
国家自然科学基金(U23B20132).Project supported by National Natural Science Foundation of China(U23B20132). （U23B20132）
