首页> 外文期刊>Plasma Sources Science & Technology >How dielectric, metallic and liquid targets influence the evolution of electron properties in a pulsed He jet measured by Thomson and Raman scattering
【24h】

How dielectric, metallic and liquid targets influence the evolution of electron properties in a pulsed He jet measured by Thomson and Raman scattering

机译:电介质,金属和液体目标如何影响通过汤姆森和拉曼散射测量的脉冲HE喷射中电子特性的演变

获取原文
获取原文并翻译 | 示例
           

摘要

Thomson scattering using a Bragg grating notch filter is used to determine the electron properties of a pulsed, kHz-driven, non-thermal atmospheric pressure plasma jet in helium expanding in air. The plasma jet is allowed to freely expand or interact with targets with different electrical properties, i.e. glass, copper and water. With the same setup, Raman scattering is used to determine spatially- and time-resolved the densities and rotational temperatures of oxygen and nitrogen molecules entrained into the jet. Fast imaging is used to determine the development of the discharge in the plasma jet as well as its behavior in the plasma-target interaction zone. As the discharge approaches the target, the rise of electron density was followed by the fall of electron temperature. The discharge is influenced only over a few millimeters before it hits the target. The electron density and temperature during the spreading of the discharge on the lowpermittivity target are measured to be resp. 2 × 1019 m~(?3) and ≈1 eV. During the return stroke on the high-permittivity and the metallic target the densities rise with a factor 1.5 resp. 2.2, and the temperature with a factor 2.5 for both cases. The discharges on the high- and low-permittivity targets extinguished soon after the initial impact of the ionization front, while the diffuse discharge on the metallic target extinguished only after the end of the voltage pulse (with a duration of 1 μs). In the diffuse discharge the electron temperature reaches 3.4 eV, the gas temperature increases by approximately 100 K and the electron density increases by approximately a factor three with respect to before its formation.
机译:使用布拉格光栅缺口滤波器的汤姆森散射用于确定空气中氦气膨胀的脉冲,KHz驱动的非热大气压等离子体射流的电子性质。允许等离子体射流自由地扩展或与具有不同电性能的靶的靶,即玻璃,铜和水。利用相同的设置,拉曼散射用于确定空间和时间分辨氧气和氮素分子的密度和旋转温度。快速成像用于确定等离子体射流中的放电的发展以及其在等离子体靶相互作用区中的行为。当放电接近目标时,电子密度的升高之后是电子温度下降。在击中目标之前,放电仅在几毫米上受到影响。测量在低分析靶的放电扩散过程中的电子密度和温度是REAC。 2×1019 m〜(?3)和≈1ev。在高介电常数和金属靶的回程中风期间,密度升高为1.5倍。 2.2,以及两种情况的温度为2.5。在电离前沿的初始冲击之后熄灭的高介电常数目标上的放电,而仅在电压脉冲结束后熄灭的金属靶上的漫射放电(持续1μs)。在漫反射放电中,电子温度达到3.4eV,气体温度升高约为100 k,并且电子密度相对于其形成之前增加了大约倍数三。

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