显示屏表面空气式静电放电实验特性

显示屏是人机交互的重要部件,当人体静电放电发生在显示屏表面时,有可能导致软硬故障。为了研究显示屏空气式静电放电实验特性,通过一个自制的装置对显示屏空气式静电放电电流和通过显示屏的位移电流进行了实验测量。研究发现:放电电流峰值随接近速度的增加而增加,上升时间随接近速度的增加而减小。在±10~±12 kV电压范围,受电弧长度的影响,上升时间增大,电流峰值变小。随着测量点与放电点之间距离的增大,位移电流波形峰值减小、上升时间增大,正极性放电峰值更大且扩散范围更广,而负极性放电上升时间增大更加明显。由位移电流波形及其分布可以计算出电荷密度。电荷密度随距离放电位置距离的增大而减小。与正极性相比,尽管负极性放电电流峰值较低,但电荷密度较高,说明负极性放电具有造成更高等级损伤风险的危害。     

On Various Kinds of Dielectric Barrier Discharges

Dielectric barrier discharges in Xe and Ne/Xe, He/Xe mixtures are investigated with regard to the ranges of existence of various discharge types over a wide range of parameters (total gas pressure p, electrode distance d, frequency f and mixture ratio X). The discharges were explained in more detail because of the bistable behaviour and the transfered charges, partly of the peak current and the maximum of the visible radiation pulse. The time behaviour of the discharge was observed, too. In this paper a distinction of various discharge types could be achieved by the similarity parameters f/p and pd. The charge carriers remaining in the volume and long-living plasma species could be identified as essential mechanisms for the development of various types of discharges. The influence of space charges on the bistable behaviour could be shown indirectly.     

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.     

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     

纳秒脉冲下真空中绝缘子表面带电特性

 实验研究了前沿50 ns、脉宽350 ns和3 μs正负极性的4种脉冲电压作用下,真空中绝缘材料的各种局部放电现象以及由此引起的表面带电。结果表明:在脉冲电压作用下,绝缘材料沿面闪络发生前会发生各种局部放电现象,局部放电是纳秒脉冲下绝缘材料表面带电的根本原因。只要发生局部放电,绝缘材料表面就会出现正极性的电荷,并且在阴极附近的电荷密度略大于阳极附近的电荷密度,但由于材料陷阱的分布,也会有局部突变。有机玻璃比聚乙烯容易发生局部放电和积聚电荷,沿面闪络电压值更低。局部放电引起表面带电的物理机制是二次电子发射形成过程中的电子碰撞电离和材料陷阱捕获电荷共同作用。     

Positive discharge from a grounded electrode toward negatively charged particles cloud

In order to understand electrostatic discharges occurring between a grounded electrode and a space charge cloud, the positive discharges were experimentally caused by negatively charged particles cloud. The discharges were initiated by locating a grounded sphere electrode at the inside or outside of the charged powder particles blown by an air flow. The luminous aspect and the discharge current were observed for the grounded sphere electrode with various diameters. Positive streamer corona discharges extended from it. The luminous aspect, peak value of the discharge current and the interval of the discharge significantly depend on the diameter of the grounded sphere electrode as well as its position.     

Surface charge measurement in surface dielectric barrier discharge by laser polarimetry

Measurements of surface charge in a surface dielectric barrier discharge driven in atmospheric air were successfully demonstrated by a laser polarimetry. AC voltage at a frequency of 2 kHz generated the discharge between an exposed electrode and the dielectric barrier over a buried electrode. Although the discharge behaviors varied depending on the polarity of the exposed electrode, there were no differences in the tendency and amplitude of the surface charge accumulation except the polarity. With higher applied voltage, the amount of surface charge became larger and the charge was distributed farther from the exposed electrode.     

Factors that influence the corona charging of fibrous dielectric materials

Corona discharge has a wide range of industry applications, such as charging the photosensitive layer and the toner particles in photocopying machines, modifying the wet-ability of plastic films, and conditioning the electrets for air filters. In all these situations, it is important to evaluate the surface charge density and compare it to the dielectric rigidity of atmospheric air. Experiments were carried out on 0.3 mm and 0.8 mm thick non-woven polypropylene fibrous media (average diameter of the fibres: 20 μm) that were exposed to positive corona discharges from a wire–grid–plate electrode system. The electrode system was powered from a continuously-adjustable DC high-voltage supply, employed as constant current generator. The monitored variable was the surface potential detected by the probe of an electrostatic voltmeter. The controlled variables were the potential of the grid electrode and the pre-conditioning temperature of the samples. The results of the experiments enabled a crude evaluation of each factor effect. Research should continue, using the experimental design methodology, in order to establish the optimum operating conditions.     

Investigation of a single barrier discharge in submillimeter air gaps. Nonuniform field

Pulse characteristics of single barrier discharges as well as parameters of charges accumulated on the surface of a dielectric under the atmospheric pressure in the “needle-(0.1–2.0)-mm air gap-polymer barrier-plane” system are investigated. It is found experimentally that for the positive polarity of the needle, the voltage for the discharge initiation is higher than in the case of the negative polarity by ～25–35%. The reversal of the needle polarity from negative to positive increases the amplitude of the discharge current and the accumulated surface charge by ～1.5–3 times. For the positive polarity of the needle, the discharge is governed by a streamer mechanism, while for the negative polarity, the discharge is initiated by the formation of a single Trichel pulse. The single pulse regime is observed for the discharge current up to a certain electrode gap d _CR. For the positive needle and for air gap width d _air > d _CR ≈ 1.5 mm, a multipulse burst corona is formed, while for the negative needle and d _air > d _CR ≈ 0.9 mm, a damped sequence of Trichel pulses evolves in the system.     

Sheet sticking caused by charge flow in a buried conducting layer

Electrostatic charge causes sheets to misfeed from the input stacks in inkjet and laser printers. Conductive layers within sheets that suppress discharges and reduce particulate contamination also aggravate sheet sticking. The surface potential of sheet media is a direct measure of the charge in the buried conducting layer. Our experiments find that the times characterizing the voltage transients range from 10 to 1000 s for conductive layers with sheet resistivities in the range from 10⁺⁹ to 10⁺¹¹ Ω/□. Our models predict that charge flowing in the conducting layer increases the electrostatic sticking force. Model predictions are in agreement with our experimental measurements.     

Triggered discharges with high arc voltages in a vacuum interrupter

Studies of nonsustained disruptive discharges (NSDDs), isolated cases of which can occur in vacuum interrupters, indicate lateral discharges between the cathode and shield, which can initiate a brief discharge between the contacts. To facilitate the study of such discharges, the sample discharges were triggered by a surface discharge induced by a spark gap, built into the side of the cathode, and observed with a high-speed film camera and image-converter camera. The tests showed a cathode spot after igniting. The emitted electrons first charge the shield negatively and then are directed toward the anode. The discharge burns at a high voltage, with current ranging from 10 to 100 A. After a period of up to 400 μs, the current demand increases abruptly; an arc discharge occurs between the contacts and discharges the capacitances near the switch. The contact gap undergoes a rapid dielectric recovery, and the restored voltage is maintained. These types of discharge were also observed with NSDDs; thus it can be assumed that the triggered discharges studied correspond to the NSDD type     

X-ray radiation due to nanosecond volume discharges in air under atmospheric pressure

The formation of nanosecond discharges in atmospheric-pressure air versus the applied pulse polarity and discharge gap geometry is studied. It is shown that the polarity of high-voltage nanosecond pulses and the electrode configuration have a minor effect on the volume discharges under a variety of experimental conditions. When the spacing between needle-like electrodes is large, the discharge is asymmetric and its glow is weakly dependent on the sign of the potential applied to the electrode. Negative voltage pulses applied to the potential electrode generate X-ray radiation from both the surface and volume. For a subnanosecond rise time of the voltage pulse and diffusion character of the discharge, the X-ray radiation comes from the brightly glowing region of a corona discharge. The average values of the fast electron velocity and energy in nitrogen are calculated. At field strengths E/p < 170 kV/cm atm, the average velocity of a fast electron bunch is constant because of central collisions. At field strengths E/p > 170 kV/cm atm, fast electrons run away. Central collisions are the reason for X-ray radiation from the volume.     

Characteristics of the discharge of a charged dielectric in low-pressure air

A charged dielectric generates a series of discharges in the surrounding air when the pressure is steadily reduced from near atmospheric to fractions of a torr. The dielectrics here employed were Mylar and Teflon. With positive polarity different discharge regimes were observed as the pressure varied: spark and long streamers at relatively high pressure; diffuse cloud-like discharges below 266 Pa (2 torr). With negative polarity it is difficult to induce a discharge, due to the absence of an electron-emitting surface. Similarities between our results and some of the features of mesospheric and stratospheric discharges are discussed.     

Relationship between surface potential and d33 constant in cellular piezoelectric polymers

The development of cellular piezoelectric polymers has shown very promising results thanks to their high d₃₃ piezoelectric constants which make them candidates for many applications. Cellular piezoelectric polymers, known as ferroelectrets, are obtained by means of an activation process which consists in generating an internal dipole with electrostatic charges produced by internal electric discharges. The most common system for this activation process is the application of a corona discharge on the surface of the sample in order to produce a high internal electric field. The theoretical electrostatic model of the process which is widely used is the Sessler model which relates the internal surface charge density, the air and polymer layers thickness, the dielectric permittivity of the polymer and the Young's Modulus of the cellular material to the d₃₃ piezoelectric constant. In our work, we relate the internal charges of the material with the d₃₃ piezoelectric constant by means of a surface potential scanning of cellular polypropylene biaxially stretched samples. Samples were charged by a corona discharge controlled with a triode electrode. Surface potentials were high enough to generate internal discharges and obtain measurable d₃₃ piezoelectric constants but low enough to be measured with spatial resolution by means of a 3 kV electrostatic probe. Surface potential profiles showed some deviations from the expected bell-shape profile due to the internal electric field generated by the internal static charge. These deviations can be numerically related to the measured d₃₃ piezoelectric constant with the electrostatic Sessler model.     

Study of electret effect of rat skin by thermally stimulated discharge analysis

The thermally stimulated discharge (TSD) spectra of three types of rat skin treated and untreated by negative polypropylene (PP) electret were measured. The natural rat skin shows an excellent electret effect due to the lamellar lipid structure, reticular structure of collagen and protein space structure related hydrogen bond network and non-covalent bond system. Hydration intensifies the skin electret effect. Electret could change the lamellar lipid structure and charge state of skin surface by alteration of dipolar orientation, intermolecular non-covalent action and protein transformation from α helix to β sheet. The regulation of skin electret effect depends on tightly bound water.     

Underwater current distribution induced by spark discharge on a water surface

Discharge current distributions generated underwater by spark discharges from the atmosphere to free water surfaces with conductivities in the range 0.07–10.0 S/m were investigated using a laboratory-scale electrode system consists of a discharge electrode and nine underwater grounding electrodes. Discharge emission on the water surface, which shows significant change with slight increase in conductivity, affects the current distribution in the water. The electric potential of the water surface also changes significantly with slight increase in conductivity. Results of numerical calculations of the underwater discharge current based on the water surface potential agree with the experimental results.     

Investigation of the Directional Velocities of Ions in a Vacuum Arc Discharge by Emission Methods

This paper is devoted to an investigation of the directional velocities of the ions generated in cathode spots of vacuum arc discharges. By using emission methods of studying the processes in a vacuum arc discharge, which involve the determination of the parameters and characteristics of the discharge plasma by analyzing the ion current extracted from the plasma and the ion charge states, the velocities of ions have been determined for the majority of cathode materials available in the periodic table. Is has been shown that at a low pressure of the residual gas in the discharge gap the directional velocities of the ions do not depend on the ion charge state. Comparison of the data obtained with calculated values allows the conclusion that the acceleration of ions in a vacuum arc occurs by the magnetohydrodynamic mechanism.     

Teilprozesse bei der Ozonerzeugung mittels stiller elektrischer Entladungen. I. Die elektrische Entladung im Ozonisator

The properties of the silent gas discharge in Siemens ozonizers are studied. The charge and potential distributions at the dielectric, the time variation of the current of partial discharges, the statistical distribution of the quantity of charge due to the partial discharges, the space and time dependence of the temperature and the heat sources in the air gap are studied in details.     

Measurements of air discharges from insulating,electrostatic dissipative and conductive materials with different ESD probes

In this work, we have compared the performance of three different kinds of passive resistor-transmission line ESD probes: an unshielded ball probe, a shielded ball probe with the ESD current collected on a coaxial wire tip, and a needle-like probe. We have measured discharges from ESD sources having different surface resistivities including charged insulator surfaces, electrostatic dissipative materials and metal plates. In compliance with the results, there is no single probe type that is ideal for all kinds of situations—there are significant differences between the probe responses comprising sensitivity, charge transferred and peak ESD current. As expected, the initiation of air discharges was suppressed in accordance with increasing surface resistivity of the ESD source.     

Effective method for measuring the energy of propagating brush discharges

Due to their very high energy propagating brush discharges are the most dangerous electrostatic discharges. As it is known, they usually occur on thick insulating layers on which significant charge can be accumulated. Discharge energy is a function of several parameters, like the surface charge density (influenced by the thickness of the layer and its relative permittivity), the size of the charged surface, etc. This paper represents a laboratory model to examine the energy of propagating brush discharges. Based on these measurements list of results were evaluated to estimate the energy of the generated propagating brush discharges. This energy is especially important to determine how incentive these discharges are. By the help of the model the effect of the polarity of the original charging, the surface charge density of the sample and the geometry of the sample have been examined.