Properties and characteristics of the nanosecond discharge developing at the water-air interface: tracking evolution from a diffused streamer to a spark filament

G. Arora, P. Hoffer, V. Prukner, Petr Bílek, Milan Šimek
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Abstract

The characteristics of nanosecond discharge propagating along the water-air interface in a unique DBD-like configuration with coplanar electrodes submerged in deionized/tap water are studied by combining ultrafast imaging and emission spectra with electrical characteristics. Time-resolved images provide a clear signature of diffusive plasma excited on the water surface at either side of the blade (insulated plastic separating the anode/cathode) called streamer phase and propagating perpendicularly away from it towards the anode /cathode with different velocities. Later on, the diffusive plasma converts into a few discrete and bright plasma filaments due to ionization instability (spark phase). There is no distinctive dependence in the streamer phase on water conductivity, but in the spark phase, more numerous, brighter, and thicker filaments form in tap water. The time-resolved emission spectra reveal the dominance of the first and second positive system of $\mathrm{N_2}$ molecular bands in the streamer phase, followed by the appearance of atomic lines of hydrogen, nitrogen, and oxygen in the spark phase. The emission spectra are utilized to estimate plasma parameters (gas temperature ($T_d$), electric field ($E/N$), and electron density ($n_e$)) where a more dominant spark phase is formed in tap water with $T_d\sim1100$ K, $E/N$ $\sim800$ Td, and $n_e\sim10^{18}$ /$\rm cm^{-3}$.
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在水气界面形成的纳秒放电的性质和特征:跟踪从扩散流到火花丝的演变过程
通过将超快成像和发射光谱与电特性相结合,研究了浸没在去离子水/自来水中的共面电极的独特 DBD 样式配置中沿水气界面传播的纳秒放电特性。时间分辨图像提供了在叶片(分隔阳极/阴极的绝缘塑料)两侧的水面上激发的扩散等离子体(称为流相)的清晰特征,这些等离子体以不同的速度垂直于叶片向阳极/阴极传播。随后,由于电离不稳定性(火花阶段),扩散等离子体转换成一些离散的明亮等离子体丝。流线阶段与水的电导率没有明显的关系,但在火花阶段,自来水中会形成更多、更亮、更粗的等离子体丝。时间分辨发射光谱显示,在流线阶段,$\mathrm{N_2}$ 分子带的第一和第二正系占主导地位,随后在火花阶段出现了氢、氮和氧的原子线。发射光谱被用来估算等离子体参数(气体温度($T_d$)、电场($E/N$)和电子密度($n_e$)),其中在自来水中形成的火花相更为主要,其温度为 $T_d\sim1100$ K,电场为 $E/N$ $\sim800$ Td,电子密度为 $n_e\sim10^{18}$ /$\rm cm^{-3}$。
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