“高电压技术”课程线上线下混合式教学

本文采用超星学习通线上教学平台，以 “高电压技术”课程为对象，实施了规模为120余人的线上线下混合式教学。基于线上教学和传统教学的优势互补，设计了“高电压技术”多个教学环节。归纳分析了混合式教学在各个教学环节取得的效果和问题，并根据学生反馈提出了持续性的改进措施。     

一种电弧引燃电缆的电气火源模拟方法

模拟故障电弧引燃电缆的火源对电缆火灾模拟试验和防火性能评估十分重要,现有的电气火源大多基于化学燃烧,较难反映故障电弧引燃特点,为了模拟故障电弧引燃电缆,本文开发了一种基于电弧的火源。首先,本文分析了110 kV电缆发生接地线被盗或两侧交叉互联线被盗等故障时金属铠装层上的感应电压,其可高达数千伏。其次,对比研究了工频交流电压和20 kHz交流电压条件下金属护套对地电弧和雅各布天梯电弧的击穿前电压与维持电压,发现两者电弧击穿与维持特性接近。进一步提出了基于雅各布天梯电弧引燃电缆的电气火源模拟方法,并实验验证了该火源能够使110 kV电缆引燃和火焰蔓延。所得结论为：高频雅各布天梯电弧能够模拟故障电弧特点并有效引燃110 kV电缆。     

Influence of high-voltage pulse parameters on the propagation of a plasma synthetic jet

In this work, a typical pin-to-pin plasma synthetic jet in static air is excited by a pulsed DC power supply. The influences of the pulse rising time, the amplitude and the repetition frequency of the pulse voltage on the jet flow have been investigated. First, using a high-speed Schlieren imaging technique, the induced shock waves and the fast jet flow generated by the plasma synthetic jet are characterized. With a deposited energy of 44 mJ per pulse, the velocity of the shock wave and the maximum velocity of the jet flow reach 320 m s⁻¹ and 100 m s⁻¹, respectively. Second, when the applied voltage increases from 12.8 kV to 16 kV, the maximum jet velocity increases from 66 m s⁻¹ to 93 m s⁻¹. On the other hand, as the pulse rising time varies from 50 ns to 500 ns, or the pulse repetition frequency increases from 5 Hz to 40 Hz, the jet velocity induced by the plasma synthetic jet is weakly dependent. In addition, a comparative study of the plasma synthetic jets using three commercial pulsed power supplies (XJ-15, NPG- 18, and PG-30) is implemented. It reveals that the maximum jet velocity of 120 m s⁻¹ is obtained in the case of PG-30, with the longest pulse rising time and the lowest breakdown voltage, while the maximum velocity of 33 m s⁻¹ is detected in the case of NPG-18, even though it has the shortest pulse rising time and the highest breakdown voltage.     

电缆燃烧典型火源模拟方法综述

针对电缆火灾问题,综述了国内外电缆火灾模拟试验及电缆燃烧测试中使用的火源模拟方法,并对比探讨了多种火源模拟方法的点火时间、火源温度、火源面积、火源功率、可扩展性、可移动性以及可持续使用性等方面的差异：燃气喷灯法和辐射加热法（锥形量热计）所需点火时间短;电加热法火源温度高,操作简便易移动;燃油点火法的点火面积大,可扩展性强;电弧引燃法的温度最高、可控性强。以期为电缆火灾模拟及防火提供参考。     

宽频高压脉冲参数对聚酰亚胺薄膜局部放电特性的影响

为了探索脉冲电应力作用下高压绝缘栅双极型晶体管(IGBT)器件绝缘材料的局部放电特性,建立高频高压脉冲作用下的局部放电测量平台,系统研究了电压幅值、脉冲重复频率、上升沿时间和脉宽对聚酰亚胺薄膜局部放电特性的影响规律。结果表明:随着电压幅值从3 kV增加至11 kV,脉冲上升沿处的局部放电信号幅值逐渐增大,而放电时延逐渐减小;随着脉冲重复频率从50 Hz增大至100 kHz,上升沿的放电时延逐渐增大但局部放电信号幅值几乎不变;随着上升沿时间从136 ns增大至300 ns,放电时延逐渐增大且更加分散,局部放电信号幅值逐渐减小且更加紧密;与脉宽为1μs的情况相比,脉宽为500 ns时局部放电信号幅值更大且放电时延更小。该结果可为高压大功率电力电子装置中固态开关的绝缘老化和状态监测提供重要科学依据。     

"高电压技术"课程线上线下混合式教学

本文采用"超星学习通"线上教学平台,以"高电压技术"课程为对象,实施了规模为120余人的线上线下混合式教学.基于线上教学和传统教学的优势互补,设计了"高电压技术"多个教学环节.归纳分析了混合式教学在各个教学环节取得的效果和问题,并根据学生反馈提出了持续性的改进措施.     

高电压技术中流注放电的科研反哺教学研究

针对《高电压技术》课程中流注放电的教学难点，本文从科研反哺教学的角度出发，介绍了一种具有高重复性的新流注放电形式-大气压等离子体射流，并采用ICCD相机拍摄它的高速传播过程，实现了流注放电教学直观形象化和定量化。从教学内容更新、教学手段丰富、课程设置优化、教学考核与反馈等多个教学环节落实流注放电的科研反哺教学方法，并取得了较好的教学效果，为该课程其他知识点的教学质量提升提供参考。     

Numerical study on the modulation of THz wave propagation by collisional microplasma photonic crystal

In order to demonstrate the modulation of terahertz wave propagation in atmospheric pressure microplasmas, in this work, the band structure and the transmission characteristics of a onedimensional collisional microplasma photonic crystal are investigated, using the transfer matrix method. For a lattice constant of 150 μm and a plasma width of 100 μm, three stopbands of microplasma photonic crystal are observed, in a frequency range of 0.1–5 THz. Firstly, an increase in gas pressure leads to a decrease in the central frequency of the stopband. When the gas pressure increases from 50.5 kPa to 202 kPa, the transmission coefficient of the THz wave first increases and then decreases at high frequency, where the wave frequency is much greater than both the plasma frequency and the collision frequency. Secondly, it is interesting to find that the central frequency and the bandwidth of the first THz stopband remain almost unchanged for electron densities of less than 10¹⁵ cm^–3, increasing significantly when the electron density increases up to 10¹⁶ cm^–3. A central frequency shift of 110 GHz, and a bandgap broadening of 200 GHz in the first stopband are observed. In addition, an atmospheric pressure microplasma with the electron density of 1 × 10¹⁵–6 × 10¹⁵ cm^–3 is recommended for the modulation of THz wave propagation by plasma photonic crystals.     

Investigation on the characteristics of an atmospheric-pressure microplasma plume confined inside a long capillary tube

An atmospheric-pressure microplasma plume of diameter 10 μm is generated inside a long tube. The length of the microplasma plume reaches as much as 2 cm. First, with the assistance of an air dielectric barrier discharge (DBD), the ignition voltage of the microplasma decreases from 40 kV to 23.6 kV. Second, although the current density reaches as high as (1.2−7.6)×10⁴ A cm ⁻² , comparable to the current density in transient spark discharge, the microplasma plume is non- thermal. Third, it is interesting to observe that the amplitude of the discharge current in a positive cycle of applied voltage is much lower than that in a negative cycle of applied voltage. Fourth, the electron density measured by the Stark broadening of Ar spectral line 696.5nm reaches as high as 3×10¹⁶ cm⁻³ , which yields a conductivity of the microplasma column of around 48 S m⁻¹ . In addition, the propagation velocity of the microplasma plume, obtained from light signals at different axial positions, ranges from 1×10⁵ m s ⁻¹ to 5×10 ⁵ m s⁻¹ . A detailed analysis reveals that the surface charges deposited on the inner wall exert significant influence on the discharge behavior of the microplasma.     

Characteristics of the plasma sheath in helium discharge within dielectric tubes

To understand the characteristics of the plasma sheath within small tubes, a 2D numerical model of He discharge within dielectric tubes is developed. During plasma propagation for a tube diameter of 0.05 mm, the sheath thickness in the plasma head is almost equal to the tube radius.It decreases rapidly to several micrometers at an axial distance of 0.05 mm behind the plasma head, and then slightly increases and saturates at the axial position far behind the plasma head. A plasma-gas sheath surro...