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大气压等离子体炬电子密度的光谱诊断
引用本文:董丽芳,刘为远,杨玉杰,王帅,嵇亚飞.大气压等离子体炬电子密度的光谱诊断[J].物理学报,2011,60(4):45202-045202.
作者姓名:董丽芳  刘为远  杨玉杰  王帅  嵇亚飞
作者单位:河北大学物理科学与技术学院,保定 071002
基金项目:国家自然科学基金(批准号:10975043,10775037),河北省自然科学基金(批准号:A2010000185)资助的课题.
摘    要:利用空心针-板放电装置产生了大气压等离子体炬,采用光谱法测量了其内部及表面的电子密度. 向空心针中通入氩气,在大气环境中产生了长度为1cm的等离子体炬.实验分别测量了Hα谱线和ArⅠ(696.54nm)谱线,通过反卷积方法分离出其相应的Stark展宽,并由此计算了电子密度.结果发现,采用Hα谱线和ArⅠ(696.54nm)谱线Stark展宽计算得到的等离子体的电子密度分别为1.0×1015cm-3和3.78×1015关键词: 等离子体炬 电子密度 气体温度 Stark展宽

关 键 词:等离子体炬  电子密度  气体温度  Stark展宽
收稿时间:2010-05-13
修稿时间:6/4/2010 12:00:00 AM

Spectral diagnostics of electron density of plasma torch at atmospheric pressure
Dong Li-Fang,Liu Wei-Yuan,Yang Yu-Jie,Wang Shuai,Ji Ya-Fei.Spectral diagnostics of electron density of plasma torch at atmospheric pressure[J].Acta Physica Sinica,2011,60(4):45202-045202.
Authors:Dong Li-Fang  Liu Wei-Yuan  Yang Yu-Jie  Wang Shuai  Ji Ya-Fei
Institution:College of Physics Science and Technology, Hebei University, Baoding 071002, China;College of Physics Science and Technology, Hebei University, Baoding 071002, China;College of Physics Science and Technology, Hebei University, Baoding 071002, China;College of Physics Science and Technology, Hebei University, Baoding 071002, China;College of Physics Science and Technology, Hebei University, Baoding 071002, China
Abstract:An atmospheric pressure plasma torch is generated with a hollowneedle-to-plate dielectric barrier discharge and the electron densities in the inside and at the surface of the plasma torch are measured by optical emission spectroscopy (OES). A plasma torch with 1cm long is generated in atmospheric ambient when argon gas is introduced through the hollwneedle. The Stark broadenings of Hα and ArⅠ(696.54 nm) lines, which are decomposed from the experimental profiles by using deconvolution method, are used to estimate the corresponding electron densities. The electron densities are 1.0×1015 cm-3 and 3.78×1015 cm-3 corresponding to the Stark broadening of Hα and ArⅠ(696.54 nm) lines, respectively. The electron density calculated from the Stark broadening of Hα is the same as that at the surface of the plasma because Hα line originates from the dissociation and the excitation of H\-2O at the plasma torch surface where argon can meet with atmosphere. While the electron density calculated from the Stark broadening of ArⅠ(696.54 nm)line is the same as that in the insid of plasma.
Keywords:plasma torch  electron density  gas temperature  Stark broadening
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