Microhollow cathode discharge （MHCD） plasmas were generated in gas mixtures containing water vapor at pressures of up to 100 kPa of He or 20 kPa of air. The cathode diameter was 1.0 mm with a length of 2.0 ram. The ...Microhollow cathode discharge （MHCD） plasmas were generated in gas mixtures containing water vapor at pressures of up to 100 kPa of He or 20 kPa of air. The cathode diameter was 1.0 mm with a length of 2.0 ram. The electricM characteristics showed an abnormal glow mode. Spectroscopic measurements were carried out to examine the plasma and radicals. An analysis of the spectral profile of Ha at 656.3 nm enabled a derivation of the electron densities, namely 2× 1014 cm-3 （at 10 kPa） and 6× 1014 cm-3 （at 4 kPa） for the helium and air atmospheres, respectively, in the negative glow region. By comparing the observed OH radical spectra with those calculated by the simulation code L[FBASE, the gas temperature was deduced to be 900 K for 4 kPa of He at a discharge current of 50 mA.展开更多
Considering the feature of distributions of parameters within the micro-hollow cathode discharge, we use a simple method to separate the sheath region characterized by drastic changes of plasma parameters and the bulk...Considering the feature of distributions of parameters within the micro-hollow cathode discharge, we use a simple method to separate the sheath region characterized by drastic changes of plasma parameters and the bulk plasma region characterized by smooth changes of plasma parameters. A zero-dimensional chemical kinetic model is used to analyze the dissociation mechanism of CO2 in the bulk plasma region of a micro-hollow cathode discharge and is validated by comparisons with previous modeling and experimental results. The analysis of the chemical kinetic processes has shown that the electron impact dissociation and heavy species impact dissociation are dominant in different stages of the rnicro-hollow cathode discharge process for a given applied voltage. The analysis of energy consumption distributions under different applied voltages reveals that the main reason of the conversion improvement with the increase of the applied voltage is that more input energy is distributed to the heavy species impact dissociation.展开更多
为了描述微空心阴极内等离子体放电特性,采用二维流体模型对氩气微空心阴极放电进行了数值模拟。在工作气压4 42×10~4×10 Pa,放电电流1.0~2.5 m A范围内,微空心阴极内氩气放电处于正常辉光放电区域,计算获得的微空心阴极伏安...为了描述微空心阴极内等离子体放电特性,采用二维流体模型对氩气微空心阴极放电进行了数值模拟。在工作气压4 42×10~4×10 Pa,放电电流1.0~2.5 m A范围内,微空心阴极内氩气放电处于正常辉光放电区域,计算获得的微空心阴极伏安特性及各种组分数密度与文献报道结果符合良好。数值模拟结果表明,在典型计算工况条件下,微空心阴极环形鞘层内电子温度可达20 e V;气体温度可高出室温几百K,说明微空心阴极内等离子体放电具有明显的气体加热效应。通过对体系内的化学动力学过程分析发现,在不同的区域内,Ar＋的产生机理不同。在阴极孔鞘层区内,高能电子直接电离基态原子占主导;在阴极孔中心处,电子冲击激发态电离占主导;在阴极孔外的放电区域中心轴线上,Ar＋的产生来自电子冲击激发态电离、Penning电离和电子直接冲击基态原子电离共同贡献。展开更多
根据微空心阴极放电(m icrohollow cathode d ischarge,简称MHCD)的基本结构,设计了一种新颖的放电结构,它利用MHCD与第三电极(金属针)之间构成新的放电方式,产生大体积高电流密度的辉光放电等离子体,利用等离子体中强烈的准分子辐射制...根据微空心阴极放电(m icrohollow cathode d ischarge,简称MHCD)的基本结构,设计了一种新颖的放电结构,它利用MHCD与第三电极(金属针)之间构成新的放电方式,产生大体积高电流密度的辉光放电等离子体,利用等离子体中强烈的准分子辐射制作紫外准分子灯。利用该放电结构进行了Xe气的放电实验,实验测到了波长为172nm的强烈准分子辐射;在400Torr气压下放电,大约有15%的内部效率;当21个这样的放电并联运行时,获得了功率密度为15mW/cm2的真空紫外光输出。实验结果表明:利用这种结构能够制作出高功率的紫外准分子灯。展开更多
文摘Microhollow cathode discharge （MHCD） plasmas were generated in gas mixtures containing water vapor at pressures of up to 100 kPa of He or 20 kPa of air. The cathode diameter was 1.0 mm with a length of 2.0 ram. The electricM characteristics showed an abnormal glow mode. Spectroscopic measurements were carried out to examine the plasma and radicals. An analysis of the spectral profile of Ha at 656.3 nm enabled a derivation of the electron densities, namely 2× 1014 cm-3 （at 10 kPa） and 6× 1014 cm-3 （at 4 kPa） for the helium and air atmospheres, respectively, in the negative glow region. By comparing the observed OH radical spectra with those calculated by the simulation code L[FBASE, the gas temperature was deduced to be 900 K for 4 kPa of He at a discharge current of 50 mA.
基金Supported by the National Natural Science Foundation of China under Grant Nos 11575019 and 11275021
文摘Considering the feature of distributions of parameters within the micro-hollow cathode discharge, we use a simple method to separate the sheath region characterized by drastic changes of plasma parameters and the bulk plasma region characterized by smooth changes of plasma parameters. A zero-dimensional chemical kinetic model is used to analyze the dissociation mechanism of CO2 in the bulk plasma region of a micro-hollow cathode discharge and is validated by comparisons with previous modeling and experimental results. The analysis of the chemical kinetic processes has shown that the electron impact dissociation and heavy species impact dissociation are dominant in different stages of the rnicro-hollow cathode discharge process for a given applied voltage. The analysis of energy consumption distributions under different applied voltages reveals that the main reason of the conversion improvement with the increase of the applied voltage is that more input energy is distributed to the heavy species impact dissociation.
基金The subject was financed by the state studing abroad scholarship fund of Doctoral College of France-China to pursue the microdischarge study in the Joseph Fourier University.
文摘为了描述微空心阴极内等离子体放电特性,采用二维流体模型对氩气微空心阴极放电进行了数值模拟。在工作气压4 42×10~4×10 Pa,放电电流1.0~2.5 m A范围内,微空心阴极内氩气放电处于正常辉光放电区域,计算获得的微空心阴极伏安特性及各种组分数密度与文献报道结果符合良好。数值模拟结果表明,在典型计算工况条件下,微空心阴极环形鞘层内电子温度可达20 e V;气体温度可高出室温几百K,说明微空心阴极内等离子体放电具有明显的气体加热效应。通过对体系内的化学动力学过程分析发现,在不同的区域内,Ar＋的产生机理不同。在阴极孔鞘层区内,高能电子直接电离基态原子占主导;在阴极孔中心处,电子冲击激发态电离占主导;在阴极孔外的放电区域中心轴线上,Ar＋的产生来自电子冲击激发态电离、Penning电离和电子直接冲击基态原子电离共同贡献。
文摘根据微空心阴极放电(m icrohollow cathode d ischarge,简称MHCD)的基本结构,设计了一种新颖的放电结构,它利用MHCD与第三电极(金属针)之间构成新的放电方式,产生大体积高电流密度的辉光放电等离子体,利用等离子体中强烈的准分子辐射制作紫外准分子灯。利用该放电结构进行了Xe气的放电实验,实验测到了波长为172nm的强烈准分子辐射;在400Torr气压下放电,大约有15%的内部效率;当21个这样的放电并联运行时,获得了功率密度为15mW/cm2的真空紫外光输出。实验结果表明:利用这种结构能够制作出高功率的紫外准分子灯。
