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Transition from the anodic arc phase to the cathodic metallic arc phase in vacuum at low DC electrical level

机译:在低直流电水平下,在真空中从阳极电弧相过渡到阴极金属电弧相

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Contact material transfer during arcing in relays has been described in several papers. Transfer from the anode to the cathode has been attributed to the anodic arc phase, and opposite transfer from the cathode to the anode has been attributed to the cathodic arc phase. In a previous paper we showed that the transition from the anodic to the cathodic arc occurs when a break arc becomes longer than a critical arc length, independently from electrical and mechanical parameters. In this paper, we completed our work by using the same breaking apparatus (14 VDC, 40 A) equipped with an arc length control device. We showed that the transition from the anodic to the cathodic arc occurs always at the same critical arc length, independently from the opening speed and the ambient pressure. Through measurements of material transfer in vacuum, we have shown that a cathodic arc in the metallic phase can occur, i.e., that material transfer direction is independent of metallic and gaseous phases. Finally, we showed that it was possible to distinguish the transition from the anodic to the cathodic arc by observing the evolution of the arc spots on the rivets.
机译:在几篇论文中已经描述了继电器电弧放电过程中的接触材料转移。从阳极到阴极的转移已归因于阳极电弧相,而从阴极到阳极的相反转移已归因于阴极电弧相。在先前的论文中,我们表明,当中断电弧的长度超过临界电弧长度时,便会发生从阳极电弧到阴极电弧的过渡,而与电气和机械参数无关。在本文中,我们使用配备了电弧长度控制装置的同一个断路设备(14 VDC,40 A)完成了工作。我们表明,从阳极电弧到阴极电弧的过渡总是在相同的临界电弧长度下发生,与打开速度和环境压力无关。通过在真空中测量材料的转移,我们已经表明在金属相中会发生阴极电弧,即,材料的转移方向与金属和气相无关。最后,我们表明可以通过观察铆钉上弧斑的变化来区分从阳极弧到阴极弧的过渡。

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