金属化聚丙烯膜脉冲电容器过载特性

脉冲电容器作为爆磁压缩激励电流源的储能元件之一,通常要求单次可靠运行。正是由于单次运行,为脉冲电容器的过载工作提供了极大的可能。过载工作的电容器与额定电容器相比具有体积小、重量轻的优点,可实现爆磁压缩激励电流源的紧凑化。研究了不同温度下国产金属化聚丙烯膜脉冲电容器的过载特性,如过载运行的储能密度,放电电流及可靠度等。实验表明:在-45℃~60℃范围内过载运行这种电容器,其储能密度可达额定储能密度的1.8倍,同时在0.95的置信水平下,其过载运行的可靠度单侧置信下限为0.9,可以实现稳定可靠运行。     

电晕放电辐射信号分析的小波基函数选取

研究电晕放电辐射信号既有利于消除其危害又有助于加强对其利用。针对小波变换提出在不同情况下对不同类型的电晕放电进行分析时,选取小波基函数的方法,理论上可以通过信号与小波波形的匹配或者通过计算信号与小波相关系数的方法来确定,而在不确定放电类型时可进行实际分析。     

对空气静电放电的频域研究

利用辐射电磁场的推迟势方程对空气静电放电的电磁场频谱进行了理论推导,对放电电流峰值和金属小环上的耦合电压峰-峰值进行了测量,使用数字存储示波器记录了放电电流和耦合电压的波形。利用测量结果对静电放电的电磁场频谱进行了理论计算,比较了不同放电电压下耦合电压的幅度谱和功率谱,结果表明:空气静电放电的能量主要集中在直流到2.0 GHz的频段内。     

电晕放电辐射场若干特性分析

为了研究电晕放电辐射场若干特性,首先进行了电晕放电时电晕电流的理论分析,研究了电晕电流的波形随电压变化情况。然后在采用针-板电极物理实验模型的基础上进行了电晕放电实验研究,分析了放电针上的充电电压对脉冲电流的影响,并确定了辐射场随传播距离的变化规律以及放电重复率随电压的变化情况。实验结果发现,当针为负极性时先发生放电,但正极性下先发生火花放电;电晕放电辐射场与距离成反比关系;放电重复率随着电压的增大而增大。     

航天服静电放电点燃能力实验研究

人—航天服系统产生的静电放电能否引燃航天服关系到载人航天飞机的安全性。通过实验研究了在纯氧和普通大气条件下 ,静电放电对各种航天服的引燃能力。实验表明 ,在普通大气条件下 ,静电放电不能引燃航天服材料。在纯氧条件下 ,点燃航天服材料所需的静电能量与静电放电的模型有关 ,机器模型的引燃能力最强。静电放电航天服点燃航天服材料所需的最小能量为 4 8mJ。     

战术电磁导轨炮用电源初探

本文提出战术电磁导轨炮对电源的要求,依此分析了四种高功率脉冲电源特性。评述了它们在战术上的可用性.     

实现任意全极点有界实函数的低灵敏度SCF的状态空间法

1 引言 Leapfrog sCF具有低灵敏度特性。但在低通情况下,由于开关电容模拟输人电阻的近似性,使得Lcapfrog scF的灵敏度特性变差二。文献[2贻出了设计低灵敏度scF的状态空间法,描述了满足低灵敏度和零灵敏度的矩阵条件,·但未给出寻求满足一定条件的变换矩阵的系统方法。本文在文献口汹基础上,导出了具     

混纺导电纤维及其织物电晕放电实验研究

本文报导了混纺导电纤维及其织物的电晕放电实验研究结果,指出导电纤维的电晕放电对人体静电荷的消散不起主要作用,而只有人体静电接地,才能较好地消除静电隐患,进而明确了防静电工作服的作用机理。     

A reusable planar triggered spark-gap switch batched-fabricated with PCB technology for medium-and low-voltage pulse power systems

Triggered spark-gap switch is a popular discharge switch for pulse power systems. Previous studies have focused on planarizing this switch using thin film techniques in order to meet the requirements of compact size in the systems. Such switches are one-shot due to electrodes being too thin to sufficiently resist spark-erosion. Additionally, these switches did not employ any structures in securing internal gas composition, resulting in inconsistent performance under harsh atmospheres. In this work, a novel planar triggered spark-gap switch (PTS) with a hermetically sealed cavity was batched-prepared with printed circuit board (PCB) technology, to achieve reusability with low cost. The proposed PTS was inspected by micro-computed tomography to ensure PCB techniques meet the requirements of machining precision. The results from electrical experiments demonstrated that PCB PTS were consistent and reusable with lifespan over 20 times. The calculated switch voltage and circuit current were consistent with those derived from real-world measurements. Finally, PCB PTS was used to introduce hexanitrostilbene (HNS) pellets in a pulse power system to verify its performance.     

Research on fuze microswitch based on corona discharge effect

Abnormal voltages such as electrostatic, constant current, and strong electromagnetic signals can erro-neously trigger operation of MEMS pyrotechnics and control systems in a fuze, which may result in casualties. This study designs a solid-state micro-scale switch by combining the corona gas discharge theory of asymmetric electric fields and Peek's Law. The MEMS switch can be transferred from "off" to"on" through the gas breakdown between the corona electrodes. In the model, one of the two electrodes is spherical and the other flat, so a non-uniform electric field is formed around the electrodes. The theoretical work is as follows. First, the relation among the radius of curvature of the spherical electrode, the discharge gap, and the air breakdown voltage is obtained; to meet the low voltage (30-60 V) required to drive the MEMS switch, the radius of curvature of the spherical electrode needs to be 10-50 μm and the discharge gap between the two electrodes needs to be 9-11 μm. Second, the optimal ratio ε is introduced to parameterize the model. Finally, the corona discharge structural parameters are determined by comparing the theoretical and electric field simulation results. The switch is then fabricated via MEMS processing. A hardware test platform is built and the performing chip tested. It is found that when the electrode gap is 9 μm, the electrostatic voltage is at least 37.3 V, with an error of 2.6% between the actual and theoretical air breakdown voltages. When the electrode gap is 11 μm, the electrostatic voltage is at least 42.3 V, with an error of 10.5% between the actual and theoretical air breakdown voltages. Both cases meet the design requirements.