冲击微通道阵列表面的大气等离子体射流中的时空电场分布

S. Raskar, I. V. Adamovich, K. Konina, M. Kushner
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引用次数: 1

摘要

在微通道阵列介质表面传播的电离波中的电场分布是通过ps电场诱导二次谐波(EFISH)产生来测量的,微通道阵列介质表面要么是空的,要么充满了蒸馏水。表面电离波由垂直冲击表面的大气压 N2-Ar 等离子体射流引发,并由 ns 脉冲放电爆发提供动力。结果表明,微通道内的电场,特别是其水平分量,最多可增强 2 倍。通道内的垂直电场在时间上滞后于在脊上测量到的电场,这表明电离波在通道内的传播方向发生了瞬时逆转(朝向喷流)。这与锁相等离子体发射图像一致,并得到动力学建模预测的证实,动力学建模预测显示电离波 "跳跃 "过空通道,在相邻脊间跳跃后才传播到通道内。当通道中充满水时,由于表面的有效介电常数较高,波速最多可增加 50%。在本诊断仪的空间分辨率(约 100 微米)范围内,没有发现电介质表面(陶瓷或水)附近有明显的电场增强迹象。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spatio-temporal electric field distributions in an atmospheric plasma jet impinging on a microchannel array surface
The electric field distribution in the ionization waves propagating over a microchannel array dielectric surface, with the channels either empty or filled with distilled water, is measured by ps Electric Field Induced Second Harmonic (EFISH) generation. The surface ionization wave is initiated by the atmospheric pressure N2-Ar plasma jet impinging on the surface vertically and powered by ns pulse discharge bursts. The results show that the electric field inside the microchannels, specifically its horizontal component, is enhanced by up to a factor of 2. The field enhancement region is localized within the channels. The vertical electric field inside the channels lags in time compared to the field measured at the ridges, indicating the transient reversal of the ionization wave propagation direction across the channels (toward the jet). This is consistent with the phase-locked plasma emission images and confirmed by the kinetic modeling predictions, which show that the ionization wave “jumps” over the empty channels and propagates into the channels only after the jump between the adjacent ridges. When the channels are filled with water, the wave speed increases by up to 50%, due to the higher effective dielectric constant of the surface. No evidence of a significant electric field enhancement near the dielectric surface (ceramic or water) has been detected, within the spatial resolution of the present diagnostic, ~100 μm.
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