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Dynamics of Nonequilibrium Liquid Plasma Generation

机译:非喹硫纤维等离子体产生的动态

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In most cases, the electric breakdown of liquids is initiated by the application of high electric field on the electrode, followed by rapid propagation and branching of plasma channels. Typically plasmas are only considered to exist through the ionization of gases and typical production of plasmas in liquids has generated bubbles through heating or via cavitation and sustains the plasmas within those bubbles. The question appears: Is it possible to ionize the liquid without cracking and voids formation? To answer this question we used a pulsed power system with 32-220 kV pulse amplitude, 0.5-12 ns pulse duration, 150 ps rise time. Discharge cell had point-to-plate geometry with a tip diameter of 100 μm. These parameters allow us to observe the non-equilibrium plasma generation. The measurements were performed with the help of 4Picos ICCD camera. It was found that discharge in liquid water forms in picosecond time scale. Emission intensity increase and plasma formation took 200-300 ps. Diameter of excited region near the tip of the high-voltage electrode was ~ 1 mm. After this initial stage emission rapidly decreased and plasma region becomes almost invisible in 500 ps. The absence of the emission during the rest of the pulse is explained by electrical field decrease on the boundary of conductive zone. Thus we have demonstrated possibility of formation of nonequilibrium plasma in liquid phase and investigated the dynamics of excitation and quenching of nonequilibrium plasma in liquid water.
机译:在大多数情况下,通过在电极上施加高电场来启动液体的电击,然后快速传播和等离子体通道的分支。通常,通过气体的电离而仅被认为存在等离子体,并且液体中的等离子体的典型生产通过加热或通过空化产生气泡并维持在那些气泡内的等离子体。出现问题:是否可以在不破裂和空隙形成的情况下电离液体?为了回答这个问题,我们使用了32-220 kV脉冲幅度的脉冲电力系统,0.5-12 ns脉冲持续时间,150 ps上升时间。放电电池具有尖端直径为100μm的点对板几何形状。这些参数允许我们观察非平衡等离子体生成。在4Picos ICCD相机的帮助下进行测量。发现在Pic秒时尺度中液体水形式排出。发射强度增加和血浆形成需要200-300 ps。高压电极尖端附近激发区域的直径为约1mm。在该初始阶段发射迅速下降和血浆区域在500 ps中变得几乎是看不见的。通过导电区边界的电场减小来解释在脉冲其余部分期间的发射。因此,我们已经证明了在液相中形成非纤维血浆的可能性,并研究了液态水中非纤维血浆的激发和淬火动态。

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