针板电极结构中纳秒脉冲介质阻挡放电的时空分辨光谱演化过程

Li Zhang, Dezheng Yang, Jing Feng, Tao Shao, Shuang Zhang
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摘要

作为一种优化电离效率的有效方法,[1]高压纳秒脉冲放电(NPD)已成为一种新兴的常压非热等离子体生产技术。NPD中的气体快速击穿机理、放电模式转换、物理化学过程等,除了在应用中具有独特的优势外,对快速脉冲电压也具有非常重要的意义。本文利用高分辨率时空光谱和图像研究了大气中针板电极结构下高压纳秒脉冲介质阻挡放电的快速击穿机理和动态演化过程。用单次ICCD图像观察了放电脉冲的演化动态过程。NPD过程主要分为三个阶段,即从针尖到极板电极的流光击穿阶段、从流光到扩散的状态转变阶段和表面放电在极板电极表面的传播阶段。研究了N2 (C3∏u→B3∏g)和N2+ (B2∑u+→X2∑g+)发射强度的时空分布,并通过氮离子第一负体系和氮分子第二正体系的强度比计算出约简电场(E/N)。发现在击穿初期,N2+ (B2∑u+→X2∑g+)的光谱主要从针尖附近区域发射。初始时刻,电场在针电极边缘处最大,随着离针距离的增加而减小。体积放电在35 ~ 40 ns时熄灭后,介质板表面附近的电场出现明显的增大,促使表面放电沿介质板向周边传播。
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Evolution Processes of Nanosecond Pulsed Dielectric Barrier Discharge by Spatiotemporal Resolved Spectra in Needle-Plate Electrode Configuration
As an effective method to optimize the ionization efficiency, [1] high voltage nanosecond pulsed discharge (NPD) has become an emerging technology for the production of nonthermal plasma at atmospheric pressure. Besides the unique advantages in the applications, the gas rapid breakdown mechanism, the discharge mode transition, and the physicochemical processes in NPD are also very significance for the fast pulse voltage. In our work, high resolution temporal-spatial spectra and images are employed to investigate the rapid breakdown mechanism and dynamical evolution process of high-voltage nanosecond pulsed dielectric barrier discharge under needle-plate electrode configuration at atmospheric air. Evolution dynamic processes in a discharge pulse are observed by one-shot ICCD images. There are three main stages in NPD are distinguished, which are the streamer breakdown from needle tip to plate electrode, the regime transition from streamer to diffuse, and the propagation of surface discharge on the plate electrode surface. The temporal-spatial distributions of the emission intensities of N2 (C3u→ B3g) and N2+ (B2u+→ X2g+) are investigated and the reduced electric field (E/N) can be calculated by the intensity ratio from the first negative systems of nitrogen ion and second positive systems of nitrogen molecular. It is found the spectra of N2+ (B2u+→ X2g+) are mainly emitted from the region near the needle tip in the initial period of the breakdown process. The electrical field is maximum on the edge of the needle electrode at the initial time, and decreases with the increase of distance from the needle. After the volume discharge is extinguished at 35–40 ns, an obvious increase of the electrical field near the surface of the dielectric plate appears, which drives the surface discharge propagating to the periphery along the dielectric plate.
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