I. Introduction
Vacuum arc (VA) essentially is metal vapor arc in vacuum environment. Metal vapor generated by electrodes determines the characteristics of VA. When the current does not exceed the interruption limit, the cathodes spots are the main sources of VA plasmas. Cathode spots can be clearly seen in many experiments with the aid of a high-speed digital camera [1]. Under this kind of arc model, the arc plasma has the characteristics of cathode material. For instance, in the modeling and simulation of VA in [2], many parameters (as average charge, ion temperature, electron temperature, and so on) in the arc plasma takes the value of copper. When the current reaches a certain level, the anode will become active due to the intense heat flux density from arc column. Herberlin and Gorman [3] observed detailed VA modes: diffuse arc, diffuse column, constricted column, jet column, and anode jet. For jet column and anode jet modes, the interaction between anode jet and cathode jet becomes more significant. Toya et al. [4] thought that the anode discharge mode will influence not only current distribution in arc column but also the bunch of cathode spots. Therefore, electrode material has a serious influence on VA. In gas switches (such as trigatrons, low-voltage air circuit breakers, high-voltage SF6 circuit breakers, and so on), electrode material is also very important.