...
首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Net emission coefficients of argon iron plasmas with electron Stark widths scaled to experiments
【24h】

Net emission coefficients of argon iron plasmas with electron Stark widths scaled to experiments

机译:电子斯塔克宽度的氩铁等离子体的净发射系数按实验缩放

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

The net emission coefficient of plasmas containing argon and iron at atmospheric pressure is calculated and analysed for the case of cylindrical geometry. Its values are obtained by integrating the monochromatic net emission coefficient taking into account continuous and line radiation. The width of the spectral lines is determined by Doppler broadening, natural, resonance, van der Waals, electron and ion Stark broadening. As Stark broadening is the most important broadening mechanism in the considered pressure and temperature range, the electron Stark widths are calculated following the semi-empirical Stark broadening theory. Additionally, the electron Stark widths of Ar, Ar ~+, Fe and Fe~+ are multiplied by scaling factors in order to reproduce experimental electron Stark widths. The scaling factor is determined for each species separately. For small plasma radii the net emission coefficient determined here shows good agreement with literature values where spherical geometry is considered while they decrease faster with increasing plasma radius. This behaviour is caused by the increase of the irradiation of the symmetry axis when cylindrical instead of spherical geometry is considered. For radii and temperatures typical of the metal filled core of arcs occurring in gas metal arc welding processes, i.e. radii between 1 and 2 × 10 ~(-3) m and temperatures between 5000 and 10 000 K, the scaling of the Stark widths increases the net emission coefficient of iron plasmas by between 2% and 23%. In this parameter range the net emission coefficient of iron plasmas for cylindrical geometry is between 30% and 37% smaller than values calculated for spherical geometry.
机译:计算并分析了在大气压下含有氩和铁的等离子体的净发射系数。它的值是通过综合考虑连续辐射和线辐射的单色净发射系数而获得的。谱线的宽度由多普勒展宽,自然,共振,范德华,电子和离子斯塔克展宽确定。由于斯塔克展宽是在考虑的压力和温度范围内最重要的展宽机制,因此电子斯塔克宽度是根据半经验斯塔克展宽理论计算得出的。此外,将Ar,Ar〜+,Fe和Fe〜+的电子Stark宽度乘以比例因子,以重现实验电子Stark宽度。分别为每个物种确定比例因子。对于较小的等离子体半径,此处确定的净发射系数与文献值具有很好的一致性,其中考虑了球形几何形状,而随着等离子体半径的增加,球形几何形状的减小速度更快。当考虑圆柱而不是球形几何形状时,此行为是由于对称轴的辐射增加而引起的。对于在气体金属电弧焊过程中发生的典型的金属填充电弧芯的半径和温度,即半径在1和2×10〜(-3)m之间并且温度在5000和10000 K之间,斯塔克宽度的比例会增加铁等离子体的净发射系数在2%到23%之间。在此参数范围内,圆柱几何形状的铁等离子体的净发射系数比球形几何形状的计算值小30%至37%。

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