单极亚微秒方波驱动He/N2混合物的均匀介质阻挡放电

X. Lu, M. Laroussi
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引用次数: 5

摘要

为了使电子能量分布函数在非平衡等离子体中向高值移动,使用了亚微秒高压脉冲。较高的电子能量导致电离和激发程度的增强。在本文中,使用纳秒级高压脉冲驱动介质阻挡放电,这是产生非平衡大气压等离子体的广泛方法之一。为了研究放电的点火过程及其结构,采用了高速ICCD相机。使用5ns的曝光时间,照片显示有两个单独的放电,本文称为一次放电和二次放电。第一次放电从间隙体开始,整个间隙在20ns内达到最大发射强度。在二次放电开始之前,在两个电极附近都有微弱的发射层。二次放电从阳极发展并向阴极扩展,在弱发光阴极层附近明显存在黑暗空间。由于等离子体的有效反应是由紫外光子和化学反应物质引起的,因此本文还研究了紫外辐射和化学反应物质的产生效率。发射光谱显示,大部分紫外线是由激发的NO自由基发射的,其中氧原子来自残留的微量空气。除NO和NO2外,血浆中还存在活化的N2、N2 +、OH和He
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Homogeneous Dielectric Barrier Discharge in He/N2 Mixtures Driven by Unipolar Sub-microsecond Square Pulses
To shift the electron energy distribution function to high values in non-equilibrium plasmas, sub-microsecond high-voltage pulses have been used. Higher electron energies lead to an enhanced degree of ionization and excitation. In this paper, nanoseconds high-voltage pulses are used to drive a dielectric barrier discharge, one of the widely used methods to generate non-equilibrium, atmospheric pressure plasmas. To study the ignition process of the discharge and its structure, a high-speed ICCD camera was used. Using a 5 ns exposure time, photos showed that there are two separate discharges, referred to in this paper as the primary discharge and the secondary discharge. The first discharge starts from the bulk of the gap and the whole gap reaches its maximum emission intensity within 20 ns. Before the secondary discharge starts, there are weak emission layers next to both electrodes. The secondary discharge develops from the anode and expands towards the cathode, with the marked presence of a dark space adjacent to a weakly luminous cathode layer. Since the agents responsible for the efficient plasma reactivity are the ultraviolet (UV) photons and the chemically reactive species, the UV radiation and reactive species generation efficiency are also studied. The emission spectra shows that most of the UV is emitted by excited NO radicals, where the oxygen atoms come from residual trace amounts of air. In addition to NO and NO2 , excited N2, N2 +, OH, and He are also present in the plasma
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