I. Introduction
IT IS WELL known that inside the vacuum interrupters, the vacuum arc is in diffuse state and the arc plasma mainly comes from cathode spots when arc current is not very high and a moderate axial magnetic field (AMF) is applied. At the diffuse state, homogeneous heat flux to anode could avoid overheating at single locations, only cathode erosion can be found and the anode is still in passive state [1]–[6]. However, when arc current exceeds a critical value, anode becomes active due to large and inhomogeneous heat flux from arc column to anode, it becomes to be a new source of metal vapor and arc plasma [7]–[9]. The anode evaporation can influence the high-current vacuum arc (HCVA) characteristics [10], [11], such as arc appearance and current distribution in arc column. Meanwhile, anode activities have great influence on the interruption performance of vacuum interrupters as excessive metal vapor at current zero may lead to failure of interruption [12]–[14].