纳秒脉冲多空心针板填料床介质阻挡层放电的时间分辨特性

Liang Qin, Yao Li, Hao Guo, Nan Jiang, Ying Song, Rui Jia, Xiongfeng Zhou, Hao Yuan, Dezheng Yang
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摘要

本文采用自行设计的多空心针状电极作为填料床介质阻挡放电反应器中的高压电极,以促进气体快速流过活性放电区,实现大体积稳定放电。利用快速曝光 ICCD 图像和时间分辨光发射光谱研究了正放电(PD)和负放电(ND)中等离子体的动态特性、生成的活性物种以及能量传递机制。实验结果表明,用多空心针电极取代多针电极后,放电强度、放电通道数和放电量都明显增加。在单个电压脉冲周期内,PD 主要以流线模式发展,与 ND 中观察到的扩散模式相比,流线模式会产生更强的放电电流、发光强度和 E/N。在 PD 中,当电介质珠之间的间隙从 0 微米变为 250 微米时,电介质珠间隙的放电从局部放电变为静止的丝状微放电,这使得等离子体不会停留在局部区域,有利于表面流的传播。在 ND 中,无论是否存在放电间隙,放电都只以介质珠间隙的扩散状模式出现。此外,激发态 N2 +(B2Σu +) 和 N2(C3Πu)的生成主要是在 PD 中观察到的,这是因为 PD 的 E/N 比 ND 高。然而,ND 中自由基 OH(A2Σ+) 的生成量高于 PD。这并不是由 E/N 直接主导的,而主要是由可逸散的 N2(A3Σu +) 和 OH(X2Π) 之间的共振能量转移过程主导的。此外,PD 和 ND 都表现出明显的电子到振动和振动到振动的能量弛豫过程,没有观察到振动到旋转的能量弛豫过程。
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Time-resolved characteristics of nanosecond pulsed multi-hollow needle plate packed bed dielectric barrier discharge
In this paper, self-designed multi-hollow needle electrodes are used as a high-voltage electrode in the packed bed dielectric barrier discharge reactor to facilitate fast gas flow through the active discharge area and achieve large volume stable discharge. The dynamic characteristics of the plasma, the generated active species, and the energy transfer mechanisms in both positive discharge (PD) and negative discharge (ND) are investigated by using fast exposure ICCD images and time-resolved optical emission spectra. The experimental results show that the discharge intensity, number of discharge channels, and discharge volume are obviously enhanced when the multi-needle electrode is replaced by a multi-hollow needle electrode. During a single voltage pulse period, PD mainly develops in a streamer mode, which results in stronger discharge current, luminous intensity, and E/N compared to the diffuse mode observed in ND. In PD, as the gap between dielectric beads changes from 0 to 250 μm, the discharge between the gap of dielectric beads changes from the partial discharge to the standing filamentary micro-discharge, which makes the plasma not stay in the local area and is conducive to the propagation of surface streamer. In ND, the discharge only appears as a diffusion-like mode between the gap of dielectric beads, regardless of whether there is a discharge gap. Moreover, the generation of excited states N2 +(B2Σu +) and N2(C3Πu) is mainly observed in PD, which is attributed to the higher E/N in PD than that in ND. However, the generation of radical OH(A2Σ+) in ND is higher than that in PD. It is not directly dominated by E/N, but mainly by the resonant energy transfer process between metastable N2(A3Σu +) and OH(X2Π). Furthermore, both PD and ND demonstrate obvious energy relaxation processes of electron-to-vibration and vibration-to-vibration, and no vibration-to-rotation energy relaxation process is observed.
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