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国家自然科学基金(51177131)

作品数:5 被引量:16H指数:2
相关作者:姚学玲陈景亮杨志豪杜志航胡上茂更多>>
相关机构:西安交通大学福建省电力有限公司更多>>
发文基金:国家自然科学基金教育部“新世纪优秀人才支持计划”更多>>
相关领域:电气工程电子电信更多>>

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Emission Current Characteristics of Triggered Device of Vacuum Switch
2014年
The characteristics of the triggered vacuum switch (TVS) are obviously influenced by the emission current ie and emission charge of the trigger device. In this paper, an RC charge collector is designed, and the characteristics of emission current ie and collecting charge Qc of the trigger device are studied. The experimental results indicate that the emission current ie which is produced by the initial plasma has both positive and negative components, and the polarity of the emission current ie depends mainly on the polarity of the bias voltage UBias. The emission current ie and collecting charge Qe increase with the increase of the trigger voltage Utr and the bias voltage UBias. The emission efficient r] increases linearly with the increase of the bias voltage UBias. When the gap distance is 15 mm and bias voltage UBias is 160 V and trigger voltage Utr is 2.6 kV, the emission efficiency r/reaches 6%
姚学玲陈景亮胡上茂
Experimental Research of ZnO Surface Flashover Trigger Device of Pseudo-Spark Switch
2014年
Pseudo-spark switch(PSS) is one of the most widely used discharge switches for pulse power technology.It has many special characteristics such as reliability in a wide voltage range,small delay time,as well as small delay jitter.In this paper,the measuring method for the initial plasma of ZnO surface flashover triggering device of PSS is studied and the results of the measurement show that the electron emission charge is mainly influenced by trigger voltage,gas pressure and DC bias voltage.When the bias voltage increases from 2 kV to 6 kV with the gap distancc fixed at 3 mm,the electron emission charge changes from 2 μC to about 6μC.When the gap distance changes from 3 mm to 5 mm with the bias voltage fixed at 2 kV,the electron emission charge increases from 1.5 μC to 2.5μC.When the gap distance is 4 mm,the hold-off voltage of PSS is 45 kV at gas pressure of 2 Pa,the minimum operating voltage is less than 1 kV.So,the operating scope is from 2.22%to 99%of its self-breakdown voltage.The discharging delay time decreases from 450 ns to 150 ns when the trigger pulse voltage is 1 kV and the discharging voltage is changed from 1 kV to 12 kV.When the trigger pulse voltage is 6 kV,the discharging delay time is less than 100 ns and changes from 100 ns to 50 ns,and the delay jitters are less than30 ns.
黄忠德姚学玲陈景亮邱爱慈
气体放电管直流击穿电压测量技术的研究被引量:9
2012年
为了寻找一个能有效表征气体放电管(GDT)从高阻状态转变为低阻状态的判据,在分析和实验对比现有技术的基础上,提出了利用电磁感应原理设计判据提取的方法.该方法设计了一个耦合线圈,将初级线圈串入主回路采集GDT击穿瞬间产生的微电流脉冲,将该脉冲整形后作为判据信号.对GDT击穿瞬间的电路状态进行了建模分析,首次从电路角度分析了GDT击穿瞬间出现的脉冲电流的形成原因,并指出不同的脉冲电流是由电流中脉冲分量和线性分量相互作用的结果.实验结果表明:在宽电压范围(50~5 000V)测量系统中,稳态击穿电流小于5mA,且在上升速率为100V/s直流电压作用下,从GDT击穿到系统响应最小时间为2.06μs,最大为3.34μs,平均为2.81μs.
姚学玲杜志航杨志豪陈景亮
关键词:气体放电管击穿电流电磁感应
沿面闪络触发真空开关初始等离子体特性实验被引量:6
2012年
提出了一种RC阻容式电荷收集器,并对触发真空开关触发初始等离子体特征进行了实验研究。实验结果表明,在触发真空开关初始等离子体的起始阶段有一个尖峰脉冲,而且初始等离子体电流波形呈振荡衰减的过程。初始等离子体电流波形的第一个振荡峰的极性取决于触发脉冲的极性。触发初始等离子体的电子电荷略大于离子电荷;触发初始等离子体的电荷随触发电压、触发电流、触发电荷的增加呈线性增加;触发初始等离子体在TVS真空间隙中的扩散时间受触发电压、触发电流、触发电荷以及TVS真空间隙距离的影响,在触发电压小于8kV时,初始等离子体的扩散时间随触发电压的增加呈线性减小,而后基本稳定在66~69ns;初始等离子体的扩散时间随TVS真空间隙距离的增加而增加,当真空间隙距离从0.5mm增加至8mm,初始等离子体的扩散时间从50ns增大至70ns。
胡上茂姚学玲陈景亮
关键词:电荷收集触发真空开关沿面闪络触发
An Active Triggered Surge Protective Gap被引量:1
2012年
A triggered surge protective device is designed and its discharge characteristics axe studied. The experimental results show that the triggered surge protective device has excellent surge protective characteristics. When the gap distance is 5 mm, p. d is 90 Pa.mm and without an active energy trigger circuit, the DC breakdown voltage of the triggered surge protective device is 2.32 kV and the pulse breakdown voltage is 5.75 kV. Therefore, the pulse voltage ratio, which is defined as the specific value of pulse breakdown voltage and DC breakdown voltage, is 2.48. With a semiconductor ZnO flashover trigger device and an active energy coupling trigger circuit, the pulse breakdown voltage can be reduced to 3.32 kV, the pulse voltage ratio is 1.43 and the response time is less than 100 ns. These results are helpful in laying a theoretical foundation for further studies on triggered surge protective devices.
姚学玲陈景亮
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