胡玉耀, 迟明辰, 蒋兴良, 咸日常, 刘晓阳, 耿凯. 不同电压类型作用下过冷却水滴运动特性及绝缘子雾凇覆冰试验[J]. 高电压技术, 2025, 51(4): 1663-1673. DOI: 10.13336/j.1003-6520.hve.20240954
引用本文: 胡玉耀, 迟明辰, 蒋兴良, 咸日常, 刘晓阳, 耿凯. 不同电压类型作用下过冷却水滴运动特性及绝缘子雾凇覆冰试验[J]. 高电压技术, 2025, 51(4): 1663-1673. DOI: 10.13336/j.1003-6520.hve.20240954
HU Yuyao, CHI Mingchen, JIANG Xingliang, XIAN Richang, LIU Xiaoyang, GENG Kai. Movement Characteristics of Supercooled Water Droplets Under AC and DC Electric Fields and Its Effect on Rime Ice Accretion on the Insulator[J]. High Voltage Engineering, 2025, 51(4): 1663-1673. DOI: 10.13336/j.1003-6520.hve.20240954
Citation: HU Yuyao, CHI Mingchen, JIANG Xingliang, XIAN Richang, LIU Xiaoyang, GENG Kai. Movement Characteristics of Supercooled Water Droplets Under AC and DC Electric Fields and Its Effect on Rime Ice Accretion on the Insulator[J]. High Voltage Engineering, 2025, 51(4): 1663-1673. DOI: 10.13336/j.1003-6520.hve.20240954

不同电压类型作用下过冷却水滴运动特性及绝缘子雾凇覆冰试验

Movement Characteristics of Supercooled Water Droplets Under AC and DC Electric Fields and Its Effect on Rime Ice Accretion on the Insulator

  • 摘要: 覆冰严重威胁输电线路的安全稳定运行。已有试验研究表明电场对绝缘子覆冰确有影响,但是不同电压类型作用下,水滴的微观运动过程及其对冰树枝生长的影响机理尚未厘清。文中以3片串LXY-160绝缘子为研究对象,基于电磁学、流体力学和场致荷电理论,首次对比分析了在交流电场和负极性直流电场作用下水滴的受力特性和运动偏移特性。在此基础上,通过自然环境下的人工雾凇覆冰试验解释了不同类型电场对覆冰增长过程的影响。结果表明:荷电水滴的运动特性与电场类型密切相关,交流电场下荷电水滴的运动轨迹出现振荡,且水滴捕获时间是直流的1.15倍。直流作用下绝缘子伞裙边缘的法向电场最大,绝缘子雾凇覆冰冰树枝集中分布于此。由于交流情况下荷电水滴受到的电场力在一个周期内有抵消效应,因此单位时间内捕获的水滴数量较直流少,且直流电场作用下的绝缘子覆冰质量和覆冰长度分别较交流提高了13.7%和8.75%。

     

    Abstract: Experimental studies have been conducted to show the effect of electric field on insulator icing. However, the motion process of droplets and its influence mechanism on the growth of ice dendrites under different types of voltages have not been understood. In the research, based on electromagnetism, hydrodynamics and field charging theory, the force characteristics and motion deviation features of the droplets under different electric fields were compared and analyzed by numerical simulations. On this basis, the impact of electric field on icing growth process was explained combined with icing tests. The results indicate that the trajectory of charged droplet presents oscillating in AC electric field, and the capture time of the droplet is 1.15 times that of DC. The normal electric field at the edge of the shed is the largest under DC, and ice branches are concentrated in this area. Since the electric force on the charged droplet has a counteracting effect in one cycle in the case of AC, the number of the droplets captured by the insulator per unit time is less than that of DC. Consequently, ice amount and length of icing insulator under DC are 13.7% and 8.75% higher than those under AC, respectively.

     

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