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Electrical and spectroscopical characterization of pulsed single bubble discharge in water with a pin-to-plate electrode configuration

机译:使用针对板电极配置的水中脉冲单气泡放电的电学和光谱表征

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摘要

Plasma discharges inside gas or vapour bubbles in water have been proposed in the last decade as a new and effective method of water treatment. However, the fundamental nature of bubble discharge is still poorly understood. In the present paper, the mechanism and properties of bubble discharge are investigated by application of a high voltage pulse to a single free gas bubble in between a pin-to-plate electrode configuration submerged in de-ionised water. A spark gap pulse generator is used to create triggered negative voltage pulses with rise times below 10 ns. The peak voltage is varied from 12 kV up to 18 kV. In the present research, the metal pin electrode is consequently chosen as the cathode. The low conductivity of the de-ionised water is maintained on the order of 10 µS/m for all experiments. The gas bubbles are formed on the tip of a capillary positioned underneath the electrodes such that every bubble passes in between the pin and plate electrode. The He gas flow rate through the capillary is kept as low as 30 sccm in order to avoid discharge in successive bubbles by a single voltage pulse. In our first setup, voltage pulses are not triggered according to the bubble flow rate. Therefore, vertical bubble position at the moment of discharge is not made reproducible in successive measurements. The bubbles are estimated to be slightly smaller than the distance between the electrodes, i.e. 2 mm.Time dependence of voltage and current during discharge are measured in both cases with and without gas bubbling. Comparison shows that two types of bubble discharge are observed. One is spark discharge in a bubble and the other one is a delayed bubble discharge that starts the same way as discharge without bubbles. Spectra of the different types of discharge are measured in a wavelength range from 200 nm up to 900 nm. Electron temperature and density are determined from emission lines. Plasma parameters are determined for peak voltages of -12 kV, -15 kV and -18 kV respectively. Influence of the bubbling gas is discussed by comparison of measurements with helium and argon.
机译:在过去的十年中,血浆中的气体或蒸气气泡内部的放电已被提出作为一种新的有效的水处理方法。但是,气泡排放的基本性质仍知之甚少。在本文中,通过将高压脉冲施加到浸没在去离子水中的针对板电极结构之间的单个自由气泡中,研究了气泡放电的机理和性能。火花隙脉冲发生器用于产生触发的负电压脉冲,其上升时间低于10 ns。峰值电压从12 kV到18 kV不等。因此,在本研究中,金属针状电极因此被选作阴极。对于所有实验,去离子水的低电导率保持在10 µS / m的数量级。气泡在位于电极下方的毛细管尖端上形成,以使每个气泡都在销和板电极之间通过。通过毛细管的氦气流量应保持在30 sccm的低水平,以避免通过单个电压脉冲在连续的气泡中放电。在我们的第一个设置中,不会根据气泡流速触发电压脉冲。因此,在连续的测量中,放电时的垂直气泡位置无法再现。气泡估计略小于电极之间的距离,即2 mm。在有气泡和无气泡的两种情况下,都测量放电期间电压和电流的时间依赖性。比较显示观察到两种类型的气泡排放。一种是气泡中的火花放电,另一种是延迟气泡放电,其开始时间与无气泡放电相同。在200 nm至900 nm的波长范围内测量不同类型放电的光谱。电子温度和密度由发射线确定。确定分别针对-12 kV,-15 kV和-18 kV峰值电压的等离子体参数。通过比较氦气和氩气的测量值来讨论起泡气体的影响。

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