...
首页> 外文期刊>Physical Science International Journal >Measurements of Absolute Atomic Oxygen Density by Two-photon Absorption Laserinduced Fluorescence Spectroscopy in Hot Air Plasma Generated by Microwave Resonant Cavity
【24h】

Measurements of Absolute Atomic Oxygen Density by Two-photon Absorption Laserinduced Fluorescence Spectroscopy in Hot Air Plasma Generated by Microwave Resonant Cavity

机译:微波谐振腔产生的热空气等离子体中双光子吸收激光诱导的荧光光谱法测量绝对原子氧密度

获取原文

摘要

Hot air plasma is generated inside a 2.45GHz microwave resonant cavity and is ejected towards a gas conditioning cell at 600 mbar. A flow of 12 liter/min of dry air with a small amount of H2, in order to better detect OH (A-X) spectra for gas temperature measurements, is injected at the entrance of the resonant cavity using an input power of 1 kW. The measurement of absolute density of atomic ground state oxygen is determined using two-photon absorption laser-induced fluorescence (TALIF) spectroscopy for several radial and axial positions of the hot air plasma column which is a post discharge propagating inside the cell. The gas temperature corresponding to the radial and axial positions, where atomic oxygen density is measured, varies between about 3500K in the column axis down to about 2500K in the plasma border. The measured absolute oxygen density using xenon for calibration varies between about 2.1x1017cm-3 in the axis down to 0.05x1017cm-3. This leads to a dissociation degree of oxygen inside the post discharge air plasma column lower than the case where only local thermodynamic equilibrium is assumed. This deviation is due to non-thermal equilibrium effects that can be associated to the not yet achieved relaxation of the long-lived excited species during such post discharge stage.
机译:热空气等离子体在2.45GHz微波谐振腔内生成,并在600 mbar处朝气体调节池喷射。为了更好地检测用于气体温度测量的OH(AX)光谱,在共振腔的入口处注入12 L / min的干燥空气和少量H 2 输入功率为1 kW。原子基态氧的绝对密度的测量是使用双光子吸收激光诱导荧光(TALIF)光谱仪对热空气等离子体柱的几个径向和轴向位置进行确定的,该位置是在单元内部传播的后放电。对应于径向和轴向位置(测量原子氧密度)的气体温度在柱轴方向大约3500K到等离子边界大约2500K之间变化。使用氙气校准的测得的绝对氧密度在大约2.1x10 17 cm -3 的轴上变化至0.05x10 17 cm -3 。因此,与仅假设局部热力学平衡的情况相比,放电后空气等离子体塔内的氧的解离度低。该偏差是由于非热平衡效应引起的,该非热平衡效应可能与在这种后放电阶段中长寿命激发物质尚未实现的松弛有关。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号