μs振荡脉冲电源激励下同轴电极介质阻挡放电特性

采用μs振荡脉冲电源激励同轴电极结构产生空气中介质阻挡放电(DBD),通过电压-电流波形的测量及发光图像拍摄研究了放电特性,计算得到了放电功率及传输电荷量等重要放电参量,研究了电压幅值、气隙距离对放电特性及放电参量的影响,在分析放电机理的基础上对实验结果进行了解释。结果表明:μs振荡脉冲电源激励下,DBD平均放电功率可达上百W,传输电荷量可达几千nC;增大电压幅值和减小放电气隙距离能获得更剧烈的放电,平均放电功率和传输电荷量均增加。     

μs振荡脉冲电源激励下同轴电极介质阻挡放电特性

 采用μs振荡脉冲电源激励同轴电极结构产生空气中介质阻挡放电(DBD),通过电压-电流波形的测量及发光图像拍摄研究了放电特性,计算得到了放电功率及传输电荷量等重要放电参量,研究了电压幅值、气隙距离对放电特性及放电参量的影响,在分析放电机理的基础上对实验结果进行了解释。结果表明:μs振荡脉冲电源激励下,DBD平均放电功率可达上百W,传输电荷量可达几千nC;增大电压幅值和减小放电气隙距离能获得更剧烈的放电,平均放电功率和传输电荷量均增加。     

Study of basic characteristics of radiation of flashlamps with microsecond discharge lengths

Spectral and temporal characteristics of xenon flashlamps are studied theoretically for the case of high-power nonstationary discharges of microsecond lengths. It is shown that several factors affect them simultaneously under these conditions: parameters of electric discharge pulse, thermal inertia of a heated gas, and the region of transparency of a lamp envelope.     

共面介质阻挡放电特性研究

对共面介质阻挡放电(DBD)的放电过程进行了实验和理论研究. 在实验中设计了分段电极方法来获取放电过程中不同位置上的局域电流和光辐射特性，得到了阴极上等离子体的扩展速度，并与二维流体数值模拟结果进行了比较. 结果表明，在共面DBD的暂态放电过程中，电极上空等离子体区域始终存在有不均匀电场，导致了不同位置上放电电流和光辐射分布的不一致. 同时研究还表明，在DBD放电过程中应当考虑表面光致二次电子发射. 关键词： 介质阻挡放电 分段电极 放电特性     

UAV flight test of plasma slats and ailerons with microsecond dielectric barrier discharge

Plasma flow control(PFC) is a promising active flow control method with its unique advantages including the absence of moving components, fast response, easy implementation, and stable operation. The effectiveness of plasma flow control by microsecond dielectric barrier discharge(μs-DBD), and by nanosecond dielectric barrier discharge(NS-DBD) are compared through the wind tunnel tests, showing a similar performance between μs-DBD and NS-DBD. Furthermore, theμs-DBD is implemented on an unmanned aerial vehicle(UAV), which is a scaled model of a newly developed amphibious plane. The wingspan of the model is 2.87 m, and the airspeed is no less than 30 m/s. The flight data, static pressure data,and Tufts images are recorded and analyzed in detail. Results of the flight test show that the μs-DBD works well on board without affecting the normal operation of the UAV model. When the actuators are turned on, the stall angle and maximum lift coefficient can be improved by 1.3° and 10.4%, and the static pressure at the leading edge of the wing can be reduced effectively in a proper range of angle of attack, which shows the ability of μs-DBD to act as plasma slats. The rolling moment produced by left-side μs-DBD actuation is greater than that produced by the maximum deflection of ailerons,which indicates the potential of μs-DBD to act as plasma ailerons. The results verify the feasibility and efficacy of μs-DBD plasma flow control in a real flight and lay the foundation for the full-sized airplane application.     

Spectral characteristics of a barrier discharge in cadmium dihalide vapor-inert gas mixtures

Spectral characteristics of a barrier-discharge plasma produced in atmospheric-pressure mixtures of cadmium diiodide and cadmium dibromide vapors with neon, krypton, and xenon at a repetition rate of sine voltage pulses up to 130 kHz are studied. The emission from the discharge is studied within the spectral range 200–900 nm with a resolution of 0.05 nm. Emission of exciplex molecules CdI(B → X) and CdBr(C, B → X), and cadmium and inert gas atoms is revealed, as well as emission of exciplex molecules XeI(B → X, A) and XeBr(B → X, A) in xenon-containing mixtures. The emission of xenon halides prevails in the spectra at a mixture temperature up to 200°C. With a further temperature increase, the emission of cadmium halides becomes dominating. It is ascertained that the most intense emissions of CdI(B → X) and CdI₂/CdBr₂/Xe/Kr and CdBr(B → X) molecules are observed, respectively, in CdI₂/CdBr₂/Xe/Kr and CdI₂/CdBr₂/Xe mixtures. The cadmium dihalide-inert gas mixtures are of interest for the use as a radiating gas in a multiwavelength and broadband excilamp emitting in the UV and visible spectral ranges.     

Emission characteristics of a barrier discharge in an Ar-H2O mixture

We have experimentally studied the UV radiation of a low-temperature barrier discharge plasma in an Ar-H₂O mixture. The spectral interval 300–400 nm has been examined in detail. Addition of argon with a pressure of 24 kPa to a barrier discharge in water vapor at a pressure of ～0.1 kPa leads to a ninefold increase in the UV radiation power of excited hydroxyl molecules. An increase in the duration of the UV radiation pulse of the mixture in the longitudinal discharge decay has been achieved for the first time, which may be direct evidence of energy transfer from metastable argon atoms to water molecules. An estimate of the upper boundary of the dissociative excitation rate constant of hydroxyl molecules OH*(A ²Σ⁺) upon interaction of metastable argon atoms with water molecules has been obtained.     

圆筒状DBD放电特性模拟研究

用XOOPIC软件对同轴圆筒状反应装置DBD放电特性进行了二维模拟研究。在频率为20kHz、正弦电压幅值为5kV的大气压氩气放电中,再现了微放电通道形成和发展过程,其微放电的寿命约为4ns。获得了电子、离子、介质表面电荷密度和电场强度随空间和时间的分布,发现在高压线圈的位置附近电子、离子和介质表面电荷密度存在极值。与典型平板介质阻挡放电相比,微放电中的电子密度、场强增加2~3个数量级。     

Electrical characterization of dielectric barrier discharge driven by repetitive nanosecond pulses in atmospheric air

Dielectric barrier discharge (DBD) is an important method to produce non-thermal plasma, which has been widely used in many fields. In the paper, a repetitive nanosecond-pulse generator is used for the excitation of DBD. Output positive pulse of the generator has a rise time of about 15 ns and a full width at half maximum of 30–40 ns, and pulse repetition frequency varies from single shot to 2 kHz. The purpose of this paper is to experiment the electrical characteristics of DBD driven by repetitive nanosecond pulses. The variables affecting discharge conditions, including air gap spacing, dielectric thickness, barrier fashion, and applied pulse repetition frequency, are investigated. The relationship between electric field, discharge current, instantaneous discharge power across air gap, and estimated electron density with the length of air gap, dielectric thickness, barrier fashion, and pulse repetition frequency is obtained respectively, and the experimental results are also discussed. In addition, two typical images exhibiting homogeneous and filamentary discharges are given with different experimental conditions.     

Study on the transition from filamentary discharge to diffuse discharge by using a dielectric barrier surface discharge device

Discharge characteristics have been investigated in different gases under different pressures using a dielectric barrier surface discharge device. Electrical measurements and optical emission spectroscopy are used to study the discharge, and the results obtained show that the discharges in atmospheric pressure helium and in low-pressure air are diffuse, while that in high-pressure air is filamentary. With decreasing pressure, the discharge in air can transit from filamentary to diffuse one. The results also indicate that corona discharge around the stripe electrode is important for the diffuse discharge. The spectral intensity of N电介质 表面放电 扩散放电 发射光谱学dielectric barrier surface discharge, diffuse discharge, optical emission spectroscopyProject supported by the National Natural Science Foundation of China (Grant Nos 10575027 and 10647123), the National Science Foundation of Hebei Province, China (Grant No A2007000134), the Education Department of Hebei Province, China (Grant No 2006106),2006-10-24Discharge characteristics have been investigated in different gases under different pressures using a dielectric barrier surface discharge device. Electrical measurements and optical emission spectroscopy are used to study the discharge, and the results obtained show that the discharges in atmospheric pressure helium and in low-pressure air are diffuse, while that in high-pressure air is filamentary. With decreasing pressure, the discharge in air can transit from filamentary to diffuse one. The results also indicate that corona discharge around the stripe electrode is important for the diffuse discharge. The spectral intensity of N＋ （391.4nm） relative to N2 （337.1 nm） is measured during the transition from diffuse to filamentary discharge. It is shown that relative spectral intensity increases during the discharge transition. This phenomenon implies that the averaged electron energy in diffuse discharge is higher than that in the filamentary discharge.     

NaOH对苯胺气液两相介质阻挡放电特性的影响

研究气液两相介质阻挡放电(DBD)的特性,对于深入理解其放电机理、促进其在环保等工业领域中应用具有重要意义。通过电压电流波形和Lissajous图形等电气特性诊断及发射光谱和发光图像等光学特性诊断,研究了液体成分对大气压气液两相DBD放电特性的影响。比较了苯胺和苯胺加NaOH溶液中气液两相DBD放电特性,利用实验结果计算得到放电功率和传输电荷,并结合放电理论对放电机制进行了分析。结果表明,苯胺加NaOH溶液中气液两相DBD,其放电特性与纯苯胺溶液有明显不同,相同电压下其放电电流约为纯苯胺溶液的两倍,其发光强度更强,放电功率和传输电荷更大,且在光谱特性图波长589nm处出现Na原子谱线,NaOH的加入增加了溶液的电导率,同时促进了气相放电强度,使得放电增强。     

NaOH对苯胺气液两相介质阻挡放电特性的影响

研究气液两相介质阻挡放电(DBD)的特性,对于深入理解其放电机理、促进其在环保等工业领域中应用具有重要意义。通过电压电流波形和Lissajous图形等电气特性诊断及发射光谱和发光图像等光学特性诊断,研究了液体成分对大气压气液两相DBD放电特性的影响。比较了苯胺和苯胺加NaOH溶液中气液两相DBD放电特性,利用实验结果计算得到放电功率和传输电荷,并结合放电理论对放电机制进行了分析。结果表明,苯胺加NaOH溶液中气液两相DBD,其放电特性与纯苯胺溶液有明显不同,相同电压下其放电电流约为纯苯胺溶液的两倍,其发光强度更强,放电功率和传输电荷更大,且在光谱特性图波长589 nm处出现Na原子谱线,NaOH的加入增加了溶液的电导率,同时促进了气相放电强度,使得放电增强。     

重复频率纳秒脉冲介质阻挡放电对聚对苯二甲酸乙二酯表面改性

介绍了0.1 MPa下的纳秒脉冲介质阻挡放电(DBD)对聚对苯二甲酸乙二酯(PET)材料表面进行的亲水性改善。分别采用均匀和丝状放电模式对PET表面改性处理,并采用水接触角测量、原子力显微镜观察、X射线光电子能谱分析对改性材料进行表面分析。实验发现介质阻挡放电处理后PET表面水接触角明显减小,接触角从78°下降到25°,但随处理时间的增加有饱和效应;PET表面粗糙程度增加,亲水性含氧基团被引入,从而改善了材料表面亲水性;纳秒脉冲下的均匀DBD比丝状DBD处理效果更为显著。     

重复频率纳秒脉冲介质阻挡放电对聚对苯二甲酸乙二酯表面改性

介绍了0.1 MPa下的纳秒脉冲介质阻挡放电(DBD)对聚对苯二甲酸乙二酯(PET)材料表面进行的亲水性改善。分别采用均匀和丝状放电模式对PET表面改性处理,并采用水接触角测量、原子力显微镜观察、X射线光电子能谱分析对改性材料进行表面分析。实验发现介质阻挡放电处理后PET表面水接触角明显减小,接触角从78°下降到25°,但随处理时间的增加有饱和效应;PET表面粗糙程度增加,亲水性含氧基团被引入,从而改善了材料表面亲水性;纳秒脉冲下的均匀DBD比丝状DBD处理效果更为显著。     

纳秒脉冲表面介质阻挡放电特性实验研究

在常规大气环境条件下,基于单极性纳秒脉冲电源对表面介质阻挡放电特性进行了实验研究。结果表明:纳秒脉冲表面介质阻挡放电的本质是丝状放电,放电集中在电压脉冲的上升沿;激励电压和脉冲重复频率越大,放电越强烈,越接近均匀放电,但电压的作用更侧重于均匀性,而频率的作用则侧重于放电的强度;电极间隙的优化可以使表面介质阻挡放电特性最好;玻璃作为阻挡介质时容易发生沿面闪络。     

Experimental study on characteristics of nanosecond-pulse surface dielectric barrier discharge

在常规大气环境条件下,基于单极性纳秒脉冲电源对表面介质阻挡放电特性进行了实验研究.结果表明:纳秒脉冲表而介质阻挡放电的本质是丝状放电,放电集中在电压脉冲的上升沿;激励电压和脉冲重复频率越大,放电越强烈,越接近均匀放电,但电压的作用更侧重于均匀性,而频率的作用则侧重于放电的强度;电极间隙的优化可以使表面介质阻挡放电特性最好;玻璃作为阻挡介质时容易发生沿面闪络.     

介质阻挡放电丝模式和均匀模式转化的特性

利用水电极介质阻挡放电装置,采用电学方法和发射光谱,研究了空气中介质阻挡放电从微放电丝模式向均匀放电模式转化的过程. 结果表明,大气压下增大外加电压或者电压一定减小气压,放电都能够从微放电丝模式过渡到均匀模式. 高气压下放电为流光击穿而低气压下为辉光放电. 利用放电发射光谱,研究了高能电子比例随实验参数的变化. 结果表明气压减小时高能电子比例增大,电压增加时高能电子减少. 利用壁电荷理论对以上实验结果进行了定性分析. 结果对介质阻挡均匀放电的深入研究具有重要价值. 关键词： 介质阻挡放电 光学发射谱 微放电丝 均匀放电模式     

介质阻挡放电丝模式和均匀模式转化的特性

利用水电极介质阻挡放电装置，采用电学方法和发射光谱，研究了空气中介质阻挡放电从微放电丝模式向均匀放电模式转化的过程. 结果表明，大气压下增大外加电压或者电压一定减小气压，放电都能够从微放电丝模式过渡到均匀模式. 高气压下放电为流光击穿而低气压下为辉光放电. 利用放电发射光谱，研究了高能电子比例随实验参数的变化. 结果表明气压减小时高能电子比例增大，电压增加时高能电子减少. 利用壁电荷理论对以上实验结果进行了定性分析. 结果对介质阻挡均匀放电的深入研究具有重要价值.     

级联型高压重复频率微秒脉冲源的研制

针对等离子体的应用,基于级联型电压叠加技术研制了一种最高输出电压为20 kV的高压微秒脉冲源,该电源由40个相同的电源模块组成,其单个模块电压等级为500 V,降低了对器件的绝缘耐压要求。电源的输出电压值在0~20 kV之间可调;重复频率在0~10 kHz之间、脉宽在0~30 μs之间可调;该电源的上升沿和下降沿均在1 μs以内。模块化的设计提高了电源的冗余容错能力。将该电源作为产生等离子体的激励源时,其输出的高压脉冲波形稳定,且根据负载对输出高压波形的要求不同,该电源可以方便地进行调节。