...
首页> 外文期刊>Physics of plasmas >Measurements and code comparison of wave dispersion and antenna radiation resistance for helicon waves in a high density cylindrical plasma source
【24h】

Measurements and code comparison of wave dispersion and antenna radiation resistance for helicon waves in a high density cylindrical plasma source

机译:高密度圆柱形等离子体源中螺旋波的波分散和天线辐射电阻的测量和代码比较

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

Helicon wave dispersion and radiation resistance measurements in a high density (n(e) approximate to 10(19) -10(20) m(-3)) and magnetic field (B < 0.2 T) cylindrical plasma source are compared to the results of a recently developed numerical plasma wave code [I. V. Kamenski and G. G. Borg, Phys. Plasmas 3, 4396 (1996)]. Results are compared for plasmas formed by a double saddle coil antenna and a helical antenna. In both cases, measurements reveal a dominance of the m = +1 azimuthal mode to the exclusion of most other modes; in particular, no significant m = -1 mode was observed. The helical antenna, designed to launch m<0 and m>0 modes in opposite directions along the field, resulted in an axially asymmetric discharge with very little plasma on the m<0 side of the antenna. For both antennas, good agreement of the antenna radiation resistance and wave dispersion with the model was obtained. It is concluded that unshielded antennas formed from current loops with an important m = 1 component for the conditions of our experiment, couple most of their power to the m = +1 helicon mode and thus have negligible parasitic, nonhelicon plasma loading. This result greatly simplifies calculations of power balance in these sources by identifying the helicon as the mode by which energy is transferred to the plasma. (C) 1999 American Institute of Physics. [S1070-664X(99)02902-X]. [References: 28]
机译:比较了高密度(n(e)近似于10(19)-10(20)m(-3))和磁场(B <0.2 T)圆柱等离子体源的螺旋波色散和辐射电阻测量结果最近开发的数字等离子波代码[I. V. Kamenski和G. G. Borg,物理学。 Plasmas 3,4396(1996)]。比较了由双鞍形线圈天线和螺旋天线形成的等离子体的结果。在这两种情况下,测量结果都显示出m = +1方位角模式比其他大多数模式都占优势。特别是,没有观察到明显的m = -1模式。螺旋形天线设计为沿磁场沿相反方向发射m <0和m> 0模式,导致轴向不对称放电,并且在天线的m <0侧上只有很少的等离子体。对于这两种天线,天线辐射阻抗和波色散均与模型良好吻合。结论是,在我们的实验条件下,由具有重要 m = 1分量的电流环路形成的非屏蔽天线会将其大部分功率耦合到m = +1螺旋模式,因此寄生的非螺旋等离子体负载可忽略不计。通过将螺线管识别为能量转移到等离子体的方式,此结果大大简化了这些源中功率平衡的计算。 (C)1999美国物理研究所。 [S1070-664X(99)02902-X]。 [参考:28]

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