摘要
在前期对常压下多针对板负电晕放电伏安特性研究的基础上,利用光学发射光谱(OES)法检测放电产生的N2发射光谱,研究其电离区形貌。根据N2发射光谱中峰值最大的第二正态激发谱峰强度ISPB在高压针电极周围的空间分布,较精确地确定了电离区形貌;在电离区内体积分ISPB,获知ISPB与放电电流I之间的关系。实验结果表明,电离区大小随着外加电压U升高而增大;电子雪崩始于距离针尖半径约1mm处的球面上,并且只在mm量级范围内发展,即电离区的大小为mm量级;电子雪崩沿针尖轴向比沿径向发展范围大,电离区形貌为"子弹"状;ISPB的积分值与I成二次相系数很小的二阶线性关系,故放电中受激物质主要是N2;高能电子主要存在于电离区,迁移区中形成电流的带电粒子为离子。
Based on the former work on the current-voltage characteristics of a multi-needle-to-plate negative corona discharge at atmospheric pressure, the present work uses the method of OES （optical emission spectrum） for measuring N2 emission spectrum, and the morphology determination of the ionization region has been investigated. According to the distribution of N2 second positive hand＇s intensity ISPB, the highest of all bands, the outline of the ionization region was drawn fairly accurately. The relationship between ISPB and discharge current I can he obtained through the volume integral of the ISPB. The experimental results show that the size of the ionization region enhances with the rise of the applied voltage U, and the electron avalanche begins at about 1 mm off the tips of needle electrode and multiplies only in the range of several millimeters, indicating that, the range of the ionization region is at the magnitude of ram. The electron avalanche along the axis of the needle develops farther than that along the radial direction of needle, and the shape of the ionization region looks like a bullet. The integral of ISPB is second-order linear to I, with a very second order coefficient, meaning that the main excited substance is N2. Energetic electrons mainly exist in ionization region while ions are the main charged particles to form discharge current in the transfer region.
出处
《光谱学与光谱分析》
SCIE
EI
CAS
CSCD
北大核心
2007年第11期2171-2174,共4页
Spectroscopy and Spectral Analysis
基金
国家自然科学基金项目(50276006
50208005)
辽宁省高等学校优秀人才资助计划(RC-05-08)资助
关键词
发射光谱
电晕放电
电离区
电子雪崩
高能电子
N2第二正态谱峰
Emission spectrum
Corona discharge
Ionization region
Electron avalanche
Energetic electron
N2 second positive band＇s intensity
