气压–风速耦合下的低压交流串联故障电弧特性和热传导机制研究

Characteristics and heat transfer mechanism of low-voltage AC series arc fault under coupled pressure–wind speed conditions

  • 摘要: 大气压与风速是影响低压交流串联故障电弧行为的关键环境因素,但目前对二者耦合作用机理的认识尚不清晰. 本文基于COMSOL Multiphysics建立二维轴对称磁流体动力学模型,采用正交试验设计,设置60795、81060、101325 Pa三种大气压与2、4 m·s−1两种风速,系统研究耦合条件下故障电弧的温度场、电气特性及能量演化规律. 结果表明:风速主要通过增强弧柱外围区域的对流换热,显著降低边缘区域温度,而对核心区域影响有限;在101325 Pa下,风速由2 m·s−1增至4 m·s−1时,电压有效值由63.997 V降至59.461 V,降幅达7.1%,电流有效值则始终稳定在34.370~34.724 A之间;在60795 Pa、4 m·s−1工况下,电弧峰值温度由无风时的30752.78 K降至22986.32 K,外围观测点温度降幅高达85.78%,然而核心温度降幅仅为0.56%,表明电弧核心区域以焦耳热为主导,对外部气流扰动具有较强的热惯性. 低气压叠加高风速会拉伸电弧形态,加剧温度场的空间偏移,降低电弧稳定性;在风速与大气压的耦合作用中,风速对电弧温度场分布及能量释放的调控作用更为显著. 本文的研究成果可为故障电弧检测系统优化及建筑火灾防控提供理论依据.

     

    Abstract: Alternating current (AC) series arc faults are a major cause of electrical fires. Atmospheric pressure and wind speed are two key factors that affect low-voltage AC series arc faults. However, their coupled effect is not well understood. In this study, a two-dimensional axisymmetric magnetohydrodynamic model is built using COMSOL Multiphysics. An orthogonal experimental design is adopted with three pressure levels (60795, 81060 and 101325 Pa) and two wind speeds (2 and 4 m·s−1) to investigate the temperature field, electrical characteristics, and energy evolution of arc faults under coupled conditions. The results are evaluated in terms of the average temperature, temperature integral, root mean square values of the current and voltage, and arc energy. The simulated arc voltage matches the zero-current characteristics and the overall trend observed in the experiment. The results show that wind primarily lowers the temperature of the peripheral region by improving the convective heat transfer near the arc column. Its effect on the core region is limited. At 101325 Pa, increasing the wind speed from 2 m·s−1 to 4 m·s−1 reduces the root mean square voltage by 7.1% from 63.997 V to 59.461 V. In contrast, the root mean square current stays within the narrow range of 34.370–34.724 A across all test conditions. This confirms that airflow has little effect on the current magnitude. Low pressure combined with high wind stretches the arc, changes the arc shape, increases the spatial shift of the temperature field, and reduces arc stability. At 60795 Pa and 4 m·s−1, the peak arc temperature drops from 30752.78 K (with no wind) to 22986.32 K, while peripheral points decrease by up to 85.78%. The core temperature drops by only 0.56%, showing that the arc core is dominated by Joule heating and resists airflow disturbances. Further analysis shows that wind plays a larger role than pressure in shaping the temperature field and energy release. At 101325 Pa, arc energy decreases by approximately 0.34% from 58751 J at 2 m·s−1 to 58549 J at 4 m·s−1. This suggests that stronger airflow cools the arc and weakens its sustainability. Pressure has a smaller, stabilizing effect. Higher pressure slightly improves the spatial shift and compactness of the temperature field. The temperature integral, which measures cumulative heat over time, follows the same trend as the average temperature. This supports the idea that wind effects vary across different spatial regions. The peripheral region cools the most: at 60795 Pa, the temperature integral there drops by approximately 44% when wind speed increases from 2 m·s−1 to 4 m·s−1. These results provide a better understanding of series arc faults under complex environments. They also form a basis for improving arc fault detection systems and preventing building electrical fires. The numbers we report, such as the 7.1% and 85.78% voltage and temperature drop at the periphery, respectively, can serve as useful benchmarks for model validation. They also show why airflow should be a key consideration when designing detection algorithms for ventilated or outdoor settings.

     

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