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浙江大学学报(工学版)  2019, Vol. 53 Issue (8): 1563-1571    DOI: 10.3785/j.issn.1008-973X.2019.08.015
电气工程、机械工程     
超大伞裙腕臂复合绝缘子积污分布的风洞模拟
董海燕1(),张友鹏1,*(),李少远2,董海龙3
1. 兰州交通大学 自动化与电气工程学院,甘肃 兰州 730070
2. 上海交通大学 电子信息与电气工程学院,上海 200240
3. 国家电网临夏供电公司,甘肃 临夏 731100
Wind tunnel simulation on contamination distribution of cantilever composite insulator with booster sheds
Hai-yan DONG1(),You-peng ZHANG1,*(),Shao-yuan LI2,Hai-long DONG3
1. School of Automation and Electrical Engineering, Lanzhou Jiao Tong University, Lanzhou 730070, China
2. School of Electronic Information and Electrical Engineering, Shanghai Jiao Tong University, Shanghai 200240, China
3. State Grid Linxia Electric Power Company, Linxia 731100, China
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摘要:

为了提高盐湖重污区接触网腕臂复合绝缘子的防污效果,降低污闪事故率,在清洁复合绝缘子的电场转折点处加装超大伞裙,以提高绝缘子防污能力和增大绝缘子的爬电距离,从源头改善绝缘子的外绝缘性能. 以工频电磁场理论和气固两相流理论为基础,采用COMSOL Multiphysics电场、流场及粒子追踪场等建立多场单相耦合的绝缘子风洞积污有限元模型. 将碰撞系数和分布系数作为绝缘子积污量的表征参数,利用数值模拟分析布置方式和环境因素对积污特性的影响. 结果表明, 在平、斜安装下,碰撞系数随风速的增大而增大,随粒径的增大呈现先增大后减小的趋势;当风向为0°时,碰撞系数最小;当风速越大或粒径越大或风向为[0°, ±30°]时,布置方式对碰撞系数的影响越明显;当风速为30 m/s、粒径为15 μm时,伞裙表面的分布系数与风向的关系符合“γ”型分布. 通过加装超大伞裙,两超大伞裙间的碰撞系数及与超大伞裙相邻的单个伞裙表面的碰撞质量大大减小.

关键词: 腕臂复合绝缘子超大伞裙布置方式积污特性数值分析    
Abstract:

The booster sheds were installed at the electric field turning point of the clean composite insulator to improve the anti-contamination ability of insulator and increase the creeping distance, thereby improving the external insulation property from the source. The purpose was to improve the anti-contamination effect of cantilever composite insulator for overhead contact system in the heavy contaminated area of the salt-lake, and further reduce pollution flashover accidents. A multi-field and single-phase coupling finite element model of contamination insulator in wind tunnel was established by using COMSOL Multiphysics electric field, flow field and particle tracking field, based on the theories of power frequency electromagnetic field and gas-particle two-phase flow. The effects of suspension mode and environmental factors on the contamination characteristics were analyzed numerically, taking the collision coefficient and the distribution coefficient as the characterization parameters of insulator contamination. Results showed that the collision coefficient increased with the increase of wind speed and increased first and then decreased with the increase of particle size, when the insulator was installed horizontally or obliquely. The collision coefficient reached minimum when the wind direction was 0°. The effect of suspension mode on the collision coefficient was greater when the wind speed or particle size was larger or the change range of wind direction was between negative thirty degree and thirty degree. The relationship between the distribution coefficient of the sheds and the wind direction was in line with the " γ” type when the wind speed was 30 m/s and the particle size was 15 μm. The collision coefficient between the two booster sheds and the collision quality of the single shed adjacent to the booster sheds greatly reduced with the installation of the booster sheds.

Key words: cantilever composite insulator    booster shed    suspension mode    contamination characteristics    numerical analysis
收稿日期: 2019-01-08 出版日期: 2019-08-13
CLC:  TM 852  
通讯作者: 张友鹏     E-mail: donghaiyancool@126.com;zhangyp@mail.lzjtu.cn
作者简介: 董海燕(1987—),女,博士生,从事高电压绝缘研究. orcid.org/0000-0002-5523-6649. E-mail: donghaiyancool@126.com
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引用本文:

董海燕,张友鹏,李少远,董海龙. 超大伞裙腕臂复合绝缘子积污分布的风洞模拟[J]. 浙江大学学报(工学版), 2019, 53(8): 1563-1571.

Hai-yan DONG,You-peng ZHANG,Shao-yuan LI,Hai-long DONG. Wind tunnel simulation on contamination distribution of cantilever composite insulator with booster sheds. Journal of ZheJiang University (Engineering Science), 2019, 53(8): 1563-1571.

链接本文:

http://www.zjujournals.com/eng/CN/10.3785/j.issn.1008-973X.2019.08.015        http://www.zjujournals.com/eng/CN/Y2019/V53/I8/1563

图 1  FQB 25型接触网腕臂复合绝缘子
图 2  绝缘子各伞裙平均电场分布特性
图 3  超大伞裙腕臂复合绝缘子
参数 取值 参数 取值
H/mm 895 D2/mm 181
s/mm 620 D1/mm 141
l/mm 2 050 αu/(°) 9
D3/mm 229 αd/(°) 6
表 1  超大伞裙复合绝缘子结构参数
图 4  绝缘子风洞积污模型
图 5  绝缘子风洞计算域网格划分截面
图 6  绝缘子表面颗粒碰撞系数与风速的关系
图 7  绝缘子表面颗粒碰撞系数与风向的关系
图 8  绝缘子表面颗粒碰撞系数与粒径的关系
图 9  伞裙护套局部结构图
图 10  绝缘子表面颗粒分布系数与风向关系
图 11  伞裙表面颗粒物分布系数与风向关系
图 12  平安装绝缘子伞裙表面颗粒的碰撞特性
图 13  斜安装绝缘子伞裙表面颗粒的碰撞特性
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