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A New Approach to High-Power Pulsed Glow Plasma Generation: Shunting Glow Plasma

机译:高功率脉冲辉光等离子体产生的新方法:分流辉光等离子体

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Shunting discharge plasmas are metal plasmas that can be generated around a conductive rod at a reduced pressure on the order of 0.1–100 Pa. Even at atmospheric pressure, a plasma can be generated because the rod is heated to emit metal vapor so as to generate gas breakdown around the rod. When the temporally increasing voltage across the rod matches the plasma ignition voltage, a shunting plasma is ignited. The plasma ignition is triggerless and, thus, does not require an external signal. There are two types of shunting plasmas: glow and arc discharges, with sustenance voltages of approximately 100 and 60 V, respectively. The plasma results in an arc discharge via a glow state. When a pulsed-power source with a controlled pulse duration is used to obtain a glow plasma only, a stable steady-state glow can be obtained under a suppressed current with a duration of over 10 $muhbox{s}$ and a consumed power of several tens of kilowatts. A shunting glow plasma can be realized by controlling the pulse duration. In this paper, optical emission spectra from the shunting glow and shunting arc are observed. Singly charged carbon ions were found to be produced by the glow plasma. Carbon emission was significant in a nitrogen gas environment, as compared with an argon environment. In the case of a shunting arc, the optical emission is broad in wavelength, and doubly ionized carbon species also arise. A preliminary test of diamond-like carbon (DLC) film deposition was carried out, where the DLC was deposited on a substrate set near a plasma source. The DLC state was determined using Raman spectroscopy, and no macroparticles were found on the deposited film, which had a clean surface. The rod holder used as an electrode showed no damage. In contrast, in the case of a shunting arc, many macroparticles were found on the deposited films, and serious damage to the electrode also occurred.
机译:分流放电等离子体是金属等离子体,它可以在导电棒周围约0.1–100 Pa的减压下产生。即使在大气压下,由于加热棒发射出金属蒸气而产生等离子体,也会产生等离子体。杆周围发生气体击穿。当杆上的暂时增加的电压与等离子点火电压匹配时,分流的等离子被点燃。等离子点火是无触发的,因此不需要外部信号。分流等离子体有两种类型:辉光放电和电弧放电,维持电压分别约为100 V和60V。等离子体通过辉光状态导致电弧放电。当使用具有受控脉冲持续时间的脉冲电源仅获得辉光等离子体时,可以在持续时间超过10 muh和消耗功率为255的抑制电流下获得稳定的稳态辉光。几十千瓦。分流辉光等离子体可以通过控制脉冲持续时间来实现。在本文中,观察了来自分流辉光和分流电弧的光发射光谱。发现辉光等离子体产生单电荷的碳离子。与氩气环境相比,在氮气环境中碳排放量显着。在分流电弧的情况下,光发射的波长很宽,并且还会产生双电离的碳物质。进行了类金刚石碳(DLC)膜沉积的初步测试,其中DLC沉积在靠近等离子体源的基板上。使用拉曼光谱法确定DLC状态,并且在沉积的膜上没有发现大颗粒,该沉积的膜具有清洁的表面。用作电极的棒固定器未显示损坏。相反,在分流电弧的情况下,在沉积的膜上发现许多大颗粒,并且还严重损坏了电极。

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