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Square grid pattern with direction-selective surface discharges in dielectric barrier discharge
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作者 张建华 潘宇扬 +3 位作者 冯建宇 贺玉楠 褚佳惠 董丽芳 《Plasma Science and Technology》 SCIE EI CAS CSCD 2023年第2期146-154,共9页
A new phenomenon that a filament discharged only once instead of twice in a cycle of the applied voltage is observed in a square grid pattern in a dielectric barrier discharge(DBD)with a larger gas gap,which is named ... A new phenomenon that a filament discharged only once instead of twice in a cycle of the applied voltage is observed in a square grid pattern in a dielectric barrier discharge(DBD)with a larger gas gap,which is named intermittent discharge.Its spatiotemporal dynamics and the formation mechanism are studied by the multiple photomultiplier tubes and an intensified charge-coupled device.Corresponding to the positions of spots in the picture with an exposure time of 40 ms,there are some bright spots(discharge spots)and black spots(non-discharged spots)in the instantaneous image with an exposure time of 10μs(a half cycle of the applied voltage).There are at least two bright spots around one black spot and vice versa.The surface discharges(SDS)can be observed between any two adjacent spots.The intensity of the SDSbetween the bright spot and the black spot is 2.5 times greater than that between two adjacent bright spots,which indicates that the SDSare directional-selective.The intermittent discharge with positive(negative)current polarity changes to that with negative(positive)current polarity,after it sustains up to 14 voltage cycles at the longest.The spatial distribution of the electric field component is calculated through COMSOL software to solve the Poisson equation numerically.It is found that the inhomogeneous distribution of surface electric field is caused by the inhomogeneous distribution of wall charges,which leads to direction-selective SDS.The intermittent discharge is formed by the competition between the direction-selective SDSand volume discharges(VDS)in DBD.This is the reason why the intermittent discharge is generated. 展开更多
关键词 dielectric barrier discharge PATTERN direction-selective surface discharges intermittent discharge
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非对称条纹电极介质阻挡放电中放电特性的空间分布
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作者 褚佳惠 董丽芳 +4 位作者 田淼 李耀华 贺玉楠 张建华 潘宇扬 《中国科学:物理学、力学、天文学》 CSCD 北大核心 2024年第4期172-184,共13页
本工作设计了由横条纹水电极和竖条纹水电极组成的非对称介质阻挡放电装置,所产生的电场强度在放电气隙各个截面的分布不同,具有S4点群对称性.实验采用光电倍增管(PMT)和高速照相机(ICCD)对放电时空特性进行了测量,研究了上述电场对放... 本工作设计了由横条纹水电极和竖条纹水电极组成的非对称介质阻挡放电装置,所产生的电场强度在放电气隙各个截面的分布不同,具有S4点群对称性.实验采用光电倍增管(PMT)和高速照相机(ICCD)对放电时空特性进行了测量,研究了上述电场对放电特性的影响.结果表明:在放电气隙中部,由光信号积分估计的电荷产生量ΔQ最少,放电通道也最细.结果表明:在放电气隙中部,光信号时间积分值最小,放电通道最细.采用ICCD对单个放电丝在多个外加电压周期的空间分布进行了研究,发现其在靠近电极处的空间位置分布与电场分布一致.数值求解拉普拉斯方程模拟了该装置产生的外加电场,发现外加电场强度在气隙中各个截面的分布呈现如下连续变化:自一侧电极横向条纹分布演变至中部四边形阵列分布,最后至另一侧电极竖向条纹分布,具有S4点群对称性.综合上述实验及电场模拟结果,发现非对称介质阻挡放电中放电的空间特性与电场强度的空间分布有关. 展开更多
关键词 介质阻挡放电 非均匀电场 放电时空特性
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