周超, 陈朋. 低风压导线覆冰特性与关键因素研究[J]. 电网技术, 2025, 49(5): 2176-2185. DOI: 10.13335/j.1000-3673.pst.2024.0378
引用本文: 周超, 陈朋. 低风压导线覆冰特性与关键因素研究[J]. 电网技术, 2025, 49(5): 2176-2185. DOI: 10.13335/j.1000-3673.pst.2024.0378
ZHOU Chao, CHEN Peng. Research on Ice Accretion Characteristics and Key Factors of Low Wind Pressure Conductor[J]. Power System Technology, 2025, 49(5): 2176-2185. DOI: 10.13335/j.1000-3673.pst.2024.0378
Citation: ZHOU Chao, CHEN Peng. Research on Ice Accretion Characteristics and Key Factors of Low Wind Pressure Conductor[J]. Power System Technology, 2025, 49(5): 2176-2185. DOI: 10.13335/j.1000-3673.pst.2024.0378

低风压导线覆冰特性与关键因素研究

Research on Ice Accretion Characteristics and Key Factors of Low Wind Pressure Conductor

  • 摘要: 低风压导线通过改变外层线股形状来降低风阻系数,但较少考虑外层线股形状改变可能对导线覆冰特性的影响。为揭示低风压导线覆冰特性和关键影响因素,该研究建立低风压导线精细化几何模型,利用ANSYS Fluent模块划分网格、定义边界并在ANSYS Icing模块开展了覆冰过程模拟计算。讨论了外层线股开口角(30°、45°、60°和90°)、开口处小圆弧半径(0.8、1.7、2.8和3.5mm)、凹弧面半径(7.09、9.15、12.09和16.9mm)对低风压导线碰撞系数、积冰形状的影响,并与同直径钢芯铝绞线进行了对比。研究发现,外层线股开口角45°时,覆冰质量最大;小圆弧半径增加,覆冰质量逐渐减小;另外,随凹弧面半径增加,覆冰质量及范围都逐渐增大;与钢芯铝绞线相比,低风压导线积冰量在短时间覆冰条件下明显减小(当覆冰30 min时,覆冰质量减少50.1%),但在长时间覆冰条件下积冰量差别很小(当覆冰24h时,覆冰质量增加1.65%)。

     

    Abstract: Low wind pressure conductor could reduce the wind resistance coefficient by designing the outer strand shape. However, very few researchers relate to the effects of the outer strand shape of the low wind pressure on ice accretion. To reveal the ice accretion characteristics and key influencing factors, a refined geometrical model of low wind pressure conductors is established. By using the ANSYS Fluent module to delimit the mesh and define the boundary, the ice accretion process is computed with the ANSYS Icing module. The effects of the opening angle of the outer strand (30°, 45°, 60°and 90°), the radius of the small arc at the opening (0.8 mm, 1.7 mm, 2.8 mm, and 3.5 mm), and the radius of the concave arc (7.09 mm, 9.15 mm, 12.09 mm, and 16.9 mm) on the collision coefficient of the low wind pressure conductors and the shape of the ice accretion are discussed and then, compared with steel core aluminum stranded conductor. It is found that the maximum ice accretion mass that occurs at the opening angle of the outer strand is 45°. Moreover, increasing the small arc radius gradually decreases the ice accretion mass. Additionally, with the increase in the concave arc radius, the ice accretion mass and region increase gradually. Compared with steel core aluminum stranded conductor, the ice accretion of the low wind pressure conductor is significantly reduced under short ice accretion (ice mass is reduced by 50.1% when ice is covered for 30 min). Still, the difference is small under long ice accretion (ice mass is increased by 1.65% when ice is covered for 24h).

     

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