首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Three-fluid simulation of a cathode spot jet in vacuum arc discharge with a metal deuteride cathode
【24h】

Three-fluid simulation of a cathode spot jet in vacuum arc discharge with a metal deuteride cathode

机译:用金属氘代孔真空电弧放电中阴极点射流的三种流体模拟

获取原文
获取原文并翻译 | 示例
           

摘要

To study the physical process of a cathode spot jet in vacuum arc discharge with a metal deuteride cathode (TiD), a two-dimensional hydrodynamic model based on three-fluid theory is established in this paper. The ionization and recombination of the plasma are considered in this model. The total current of the cathode spot is set to 2-4 A. The simulation shows that: (1) for Ti ions, there are huge pressure gradients and D-Ti ion collisions (10(13)-10(14)Pa m(-1)) in both the axial and radial direction near the cathode spot region, therefore the plasma jet will expand rapidly in all directions. For D ions, the ion collisions (D-Ti) play an important role in the whole region of the cathode spot jet, resulting in the velocity of a deuterium ion (m(i)n(i)(u(i) . del)u(i) = -del p(i) + del . (tau) over bar (i) + Z(i)en(i)(E+ u(i) x B) + R-i) being limited to a level close to the velocity of a titanium ion (u(i)). (2) Due to the expansion of the cathode spot jet, the ion density decreased rapidly from 10(26) m(-3) to 10(22) m(-3). Meanwhile, ion speed quickly reached a level of 10(4) m s(-1) at a distance of 2 mu m from the cathode spot. (3) When the current of the cathode spot is small (I = 2 A), deuterium ions obtained by the reaction path are significantly less than that obtained by the reaction path. However, with an increase in the cathode spot current, deuterium ions obtained by the two reaction paths are almost the same. (4) Finally, the plasma parameters of the cathode spot jet predicted by our numerical model are in good agreement with the experimental results.
机译:为了研究真空电弧放电的阴极点射流的物理过程,用金属氘代(TID),本文建立了基于三流体理论的二维流体动力学模型。在该模型中考虑了等离子体的电离和重组。阴极点的总电流设定为2-4A。模拟表明:(1)对于Ti离子,存在巨大的压力梯度和D-Ti离子碰撞(10(13)-10(14)PA M. (-1))在阴极点区域附近的轴向和径向方向上,因此等离子体射流将在所有方向上迅速膨胀。对于D离子,离子碰撞(D-Ti)在阴极点射流的整个区域中起重要作用,导致氘离子的速度(m(i)n(i)(u(i)。del )U(i)= -del p(i)+ del。(tau)在酒吧(i)+ z(i)en(i)(e + u(i)x b)+ ri)被限制为关闭水平钛离子的速度(U(I))。 (2)由于阴极点射流的膨胀,离子密度从10(26)m(-3)至10(22)m(-3)迅速下降。同时,离子速度快速达到10(4)升(-1)的距离,距离阴极点2μm。 (3)当阴极点的电流小时(I = 2 A)时,通过反应路径获得的氘离子显着小于通过反应路径获得的氘离子。然而,随着阴极点电流的增加,通过两个反应路径获得的氘离子几乎是相同的。 (4)最后,我们数值模型预测的阴极点射流的等离子体参数与实验结果吻合良好。

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