Mode transition in homogenous dielectric barrier discharge in argon at atmospheric pressure

The influence of driving frequency on the discharge regime of a homogenous dielectric barrier discharge in argon at atmospheric pressure is studied through a one-dimensional self-consistent fluid model. The simulation results show that the discharge exhibits five notable discharge modes, namely the Townsend mode, stable glow mode, chaotic mode, asymmetric glow, and multiple period glow mode in a broad frequency range. The transition mechanisms of these modes should be attributed to the competition between the applied voltage and the memory voltage induced by the surface charges.     

The influence of dielectric surface charge distribution upon thepartial discharge behavior in short air gaps

A two-dimensional breakdown model based upon the continuity equations for electrons and ions and the Poisson equation is employed to examine the influence of surface charges upon the partial discharge behavior of a short metallic-dielectric plane-parallel electrode gap of 0.05 cm in an air-like mixture at atmospheric pressure. The form of charge distribution at the dielectric electrode surface is found to significantly affect a number of important discharge parameters, such as the uniformity of the electric field, the charge density and its radial distribution within the gap, as well as the discharge propagation time     

介质窗口材料对高功率微波传输特性的影响

运用光学方法,分析平面波通过无限大介质平板的传输特性,进而分析单层介质窗口的引入对微波传输性能的影响。在S波段微波源上对聚四氟乙烯材料进行了真空环境下的微波放电击穿实验,通过长时间的表面放电,在聚四氟乙烯材料表面出现电痕和电树枝。在100 ns脉冲宽度下,未发生大面积表面放电前,通过光学照相,在介质表面观测到局部放电现象,认为局部放电仍能导致材料表面破坏。作为对比,进行了聚苯乙烯材料的电老化实验,实验结果表明聚苯乙烯材料具有良好的耐电痕、耐电树枝老化特性。     

氩气介质阻挡放电不同放电模式的电学特性研究

采用水电极介质阻挡放电装置，在气压为40kPa的氩气中实现了弥散、流光和斑图三种不同 模式的放电，并对其光电特性进行测量.通过测量测试电容上的电压，从而将气隙电压计算 出来，发现随外加电压增加，放电起始时刻不断提前，放电占空比增加；对应放电时刻，气 隙电压减小、输运电荷突增，使得气隙电压和电量波形都远远偏离正弦.气隙电压与输运电 荷成非线性关系.给出了外加电压零点对应的气隙电压随外加电压峰值的变化关系.讨论了壁 电荷在放电中的作用及对气隙电压和电量波形的影响. 关键词： 介质阻挡放电 气隙电压 自组织斑图 输运电荷     

介质窗口材料对高功率微波传输特性的影响

运用光学方法,分析平面波通过无限大介质平板的传输特性,进而分析单层介质窗口的引入对微波传输性能的影响。在S波段微波源上对聚四氟乙烯材料进行了真空环境下的微波放电击穿实验,通过长时间的表面放电,在聚四氟乙烯材料表面出现电痕和电树枝。在100 ns脉冲宽度下,未发生大面积表面放电前,通过光学照相,在介质表面观测到局部放电现象,认为局部放电仍能导致材料表面破坏。作为对比,进行了聚苯乙烯材料的电老化实验,实验结果表明聚苯乙烯材料具有良好的耐电痕、耐电树枝老化特性。     

Improved piezoelectric properties of cellular polypropylene ferroelectrets by chemical modification

To improve the thermal stability of piezoelectricity of polypropylene (PP) ferroelectrets, chemical modification of the cellular PP film was performed via chromic acid oxidation and then hydrofluoric acid treatment. Deep chemical modification is achieved as indicated by the energy-dispersive X-ray analyses on the cross-section of the modified cellular PP film. The results of the isothermal decay for piezoelectric d ₃₃-coefficient at 70°C indicate the improved thermal stability of piezoelectricity and the enhanced piezoelectric activity of the modified PP ferroelectrets. The former is attributed to the improvement of thermal stability of the charges trapped in the internal void surface layers as indicated by the thermally stimulated discharge measurements, while the latter results not only from the improved thermal stability of the charges but also from the reduction in Young’s modulus of the PP ferroelectrets due to the chemical modification as revealed by the dielectric resonance analyses.     

低气压氙气介质阻挡放电的一维仿真研究

通过建立一个自洽耦合的一维流体模型来描述低气压氙气介质阻挡放电(DBD),并采用有限元法对模型进行数值仿真研究,得到了不同外加电压幅值和频率下的气体间隙压降、放电电流、介质表面电荷随时间的变化关系以及电子、离子、中性粒子和空间电场的时域分布.仿真结果表明:介质表面电荷对放电的点燃与熄灭起着关键的作用;在一个放电周期内,根据气体间隙压降的变化情况,介质表面电荷可按六个阶段进行分析;随着外施电压幅值的增加,间隙击穿逐渐提前至外施电压过零点之前发生,放电更为剧烈;随着外施电压频率的提高,气体间隙压降减小,间隙容易击穿,放电也更加均匀.粒子及空间电场的时域分布表明氙气DBD为典型的辉光放电.     

大气压氩气介质阻挡辉光放电的一维仿真研究

为了研究氩气(Ar)中介质阻挡大气压辉光放电(APGD)的放电机理, 通过建立一个一维的多粒子自洽耦合流体模型, 采用有限元方法进行数值计算, 得到了气体间隙压降、介质表面电荷密度、放电电流密度随时间的周期变化波形, 以及电子、离子、亚稳态粒子密度和空间电场强度的时空分布. 仿真计算结果表明：介质表面积聚的电荷对于放电的过程的起始及熄灭具有重要作用;当增大外施电压时, 放电击穿时刻提前, 放电电流密度和介质表面电荷密度峰值增大, 表明放电过程更加剧烈;随着阻挡介质相对介电常数的增大, 放电电流密度也随之增大. 各粒子密度及电场的时空分布表明放电过程在外施电压半个周期中只有一次放电, 且存在明显的阴极位降区、负辉区、等离子体正柱区等辉光放电的典型区域, 为大气压辉光放电(APGD).     

Neutralization of charged dielectric materials using a dielectric barrier discharge

Safety and efficiency are two characteristics that must be satisfied by an electric charge neutralizer. The dielectric barrier discharge (DBD), which has the advantage of preventing arc transition, is an interesting tool to safely neutralize unwanted charge. This paper is aimed at studying the efficiency of neutralizing charged polyethylene (PE) granules by using a dielectric barrier discharge. During this study, several factors were considered such as the amplitude and the frequency of the AC voltage, the polarity and the charging mode of the samples, as well as the electrode configuration. Two DBD electrode configurations were considered: simple DBD and a DBD with installed metallic grid. The obtained results show that using the DBD can lead to excellent neutralization results when the grid is installed. With the appropriate voltage amplitude and frequency and with grid installed, the elimination of nearly 99% of the initial surface charges can be achieved. The metallic grid placed between the DBD electrode and the target enhances significantly the neutralization efficiency.     

恒流电晕充电对聚四氟乙烯多孔薄膜驻极体驻极态的影响

利用常温下恒流和恒压电晕充电、充电后的等温表面电位衰减、热刺激放电和扫描电镜等实 验手段研究了恒流和恒压电晕充电技术对聚四氟乙烯多孔薄膜驻极体驻极态的影响.与恒压电晕充电相比较，恒流电晕充电时由于流过薄膜的电流恒定，增加了注入电荷在多孔结构厚度方向界面处的俘获概率，使沉积电荷密度上升，改善了驻极体的储电能力.然而，这些位于不同层深多孔界面处的俘获电荷在这类功能膜储存或使用过程中，经外激发从脱阱位置 以跳动（hopping）模式输运至背电极的路径相对缩短将导致脱阱电荷衰减较快. 关键词： 恒流电晕充电 聚四氟乙烯多孔膜 驻极体 电荷稳定性     

The nature of emitting microdischarges in barrier-discharge lamps

The nature of the microdischarges of the barrier discharge is studied. The distribution of the fields generated in the discharge gap by charges on the dielectric surface is determined, the microdischarge parameters are estimated, and the results obtained are compared with the experimental data.     

大气压氩气放电中的斑图形成

采用双水电极的介质阻挡放电装置，在混有0.5％空气的大气压氩气放电中观察到了六边形及正方网格斑图；测量了正方网格中的微放电的时间行为，发现相邻两次放电的时间间隔是长短交替的；分析了壁电荷对放电丝自组织成斑图过程的影响. 关键词： 自组织斑图 微放电     

实验研究大气压多脉冲辉光放电的模式和机理

采用稍不平行电极进行大气压He气介质阻挡多脉冲辉光放电实验,通过增强电子耦合器件相机短时曝光照片,研究大气压多脉冲辉光放电在不同时刻的放电模式.通过气隙放电电流、表面电荷计算,理论分析了表面电荷、空间电荷、外加电压与气隙电场强度的关系,研究大气压辉光放电形成多脉冲的机理.实验结果表明,放电首先在间隙稍窄的电极左端开始;在第一个脉冲电流峰值,电极右端也开始放电;第一个电流脉冲经历了Townsend放电到辉光放电的过程;电流脉冲之间的时间内,间隙一直维持着微弱的辉光放电;随后的每个电流脉冲均是辉光放电.理论分析表明,大气压辉光放电的多个电流脉冲是表面电荷、空间电荷与外加电压共同演化的结果;除放电伊始出现Townsend放电外,同一半周期内的放电电流脉冲中不会再出现Townsend放电. 关键词： 介质阻挡放电 增强电子耦合器件 大气压辉光放电 多脉冲     

实验研究大气压多脉冲辉光放电的模式和机理

采用稍不平行电极进行大气压He气介质阻挡多脉冲辉光放电实验,通过增强电子耦合器件相机短时曝光照片,研究大气压多脉冲辉光放电在不同时刻的放电模式.通过气隙放电电流、表面电荷计算,理论分析了表面电荷、空间电荷、外加电压与气隙电场强度的关系,研究大气压辉光放电形成多脉冲的机理.实验结果表明,放电首先在间隙稍窄的电极左端开始;在第一个脉冲电流峰值,电极右端也开始放电;第一个电流脉冲经历了Townsend放电到辉光放电的过程;电流脉冲之间的时间内,间隙一直维持着微弱的辉光放电;随后的每个电流脉冲均是辉光放电.理论分析表明,大气压辉光放电的多个电流脉冲是表面电荷、空间电荷与外加电压共同演化的结果;除放电伊始出现Townsend放电外,同一半周期内的放电电流脉冲中不会再出现Townsend放电.     

介质阻挡放电中微放电的映射方程

利用双水电极介质阻挡放电装置，采用光学方法测量了大气压空气和氩气中介质阻挡放电的微放电时间特性.实验发现微放电通道相邻两次放电时间间隔是长短交替的.根据壁电荷对相邻两次微放电的不同影响，建立了介质阻挡放电时间序列的映射方程.不同放电参量取值情况下的计算结果表明，介质阻挡放电中，壁电荷电场的衰减时间常数远大于100μs量级.由方程所得的结果，解释了相邻两次放电时间间隔长短交替的实验现象，确定了壁电荷衰减时间常数的范围. 关键词： 介质阻挡放电 时间特性 壁电荷 映射方程     

宏观电偶极子对聚丙烯铁电驻极体膜电荷储存及其动态特性的影响

利用栅控恒压电晕充电组合反极性电晕补偿充电法，研究了孔洞(单元电畴)内分布的空间电荷型宏观电偶极子的形成，及其增长对聚丙烯孔洞膜电极化期间的电流特性及电导率的影响. 借助等温表面电位衰减测量、开路和短路热刺激放电电流谱分析等，讨论了宏观电偶极子及其密度变化时的聚丙烯孔洞驻极体膜电荷储存稳定性及电荷动态特性. 实验结果说明：由电极化形成的宏观电偶极子的自身电场提高了聚丙烯孔洞驻极体膜的电导率，从而降低了驻极体膜电荷储存的稳定性. 对呈现弱极化强度的孔洞驻极体膜，以孔洞为畴结构基本单元内的宏观电偶极子，其两性空间电荷的大部分仅仅分别沉积在透镜状孔洞上下两壁的两端. 外激发脱阱电荷从脱阱位置的输运路径，主要是绕孔洞两边沿介质层迁移；而极化强度较高的样品，其两性电荷则分别分布在上下两壁的宽广区域内，脱阱电荷的大部分在驻极体电场驱动下从脱阱位置通过孔洞层间的介质层迁移并衰减.     

An investigation into the effects of oxygen plasma discharge on tin-doped indium oxide thin films

The surfaces of tin-doped indium oxide (ITO) thin films for polymer light-emitting electrochemical cells (LECs) were modified by oxygen plasma discharge. The properties of the ITO surfaces were evaluated by means of the measurements of X-ray photoelectron spectroscopy (XPS), contact angle, surface free energy and polarity. The influence of surface properties of the ITO thin films on the performance of polymer LECs was investigated in terms of the turn-on voltage, injection current and luminance. When oxygen plasma discharge was employed to modify the ITO surfaces, the surface properties of ITO are optimized due to the improvement of surface stoichiometry and the enhancement of wettability. And the improved surface properties benefited from the oxygen plasma discharge is observed to decay with the time after the plasma discharge. The difference in chemical composition, surface free energy and polarity between the non-treated and treated ITO surfaces appears to become smaller with the increase of the time after plasma discharge. In addition, the electrical and optical performance of the devices is found to become worse with the increasing time after plasma discharge on ITO substrates. The results demonstrate that the device performance strongly depends on the ITO surface properties and the ITO/organic interface characteristics.     

Si基Si3N4/SiO2双层膜驻极体的电荷储存与输运

利用等温表面电位衰减及热刺激放电(thermally stimulated discharge,TSD)方法探讨了恒栅压电晕充电经常压化学气相沉积(APCVD)的Si基Si3N4和热生长SiO₂双层薄膜驻极体电荷的存储特性.结果表明:在常温环境中,300℃高温下,以及95%相对湿度时的60℃条件下,所有试样表现出极好的电荷储存稳定性.对于负电晕充电试样,其电荷输运受慢再捕获效应(slow retrapping effect)控制;用热离子发射模型来描述了正电晕充电Si₃N₄/SiO₂驻极体的正电荷输运特性. 关键词： 驻极体 薄膜 电荷储存 热离子发射     

中等pd值介质阻挡放电的空间均匀性

使用双液体电极介质阻挡放电装置，在中等pd值下获得了具有高空间均匀性的等离子体。采用时空分辨测量方法研究了放电的光电特性。结果表明，具有高空间均匀性的等离子体能在很大的电压范围内维持，相应的输入功率也在一个很大范围内变化。讨论了壁电荷对放电功率和空间均匀性的影响。     

Analysis on surface charging of insulator prior to flashover in vacuum

Prior to the flashover across an insulator in vacuum, the insulator surface is usually charged. It is of great importance to investigate the charging phenomena for better understanding the flashover characteristics. It is considered that there are two kinds of mechanisms closely related to the surface charging of insulator i.e., the secondary electron emission occurred over an insulator, and while employing a perfect electrode contact ahead of electron emission into vacuum, the charge injection and accumulation occurred inside the surface layer of an insulator. Based on the rigorous analysis of the kinetic processes of both primary and secondary electrons, the related surface charges were theoretically deduced. Involving the detrapping of charges trapped and the recombination of charges injected, the charging process due to charge injection and accumulation was analyzed. Some formulas were given to express the density of surface charges.