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Transition to the diffuse mode for high-current drawn arcs in vacuum with an axial magnetic field

机译:在轴向磁场下真空中大电流引弧过渡到扩散模式

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The opening of electrical contacts while passing current generates a drawn arc. In vacuum, the arc begins as a bridge of molten metal connecting the contacts, which then ruptures to form a bridge column arc. For butt contacts without an AMF at currents up to 16 kA peak, the bridge evolves into a transition mode before switching to a diffuse or diffuse column mode. Previous work observing the development of high-current drawn arcs in vacuum with an axial magnetic field (AMF) measured the time period required for the bridge column to evolve into the diffuse mode. Arc visualization experiments on Cu-Cr contacts with an AMF have now determined that the transition to the fully diffuse mode has a more complicated structure. The opening sequence begins with the rupturing of the molten metal bridge, forming the bridge column. This column evolves into the transition mode, and then into the fully diffuse mode. The transition mode consists of a region of concentrated cathode spots, similar to the transition mode for butt contacts. Over a period of a few milliseconds, individual cathode spots begin to appear outside the concentrated region until a diffuse arc forms. Increasing the axial field strength reduces the lifetime of the transition mode. This reduction correlates with changes in the arc voltage. In addition, the transition mode appearance also agrees with previous studies of contact melting in an AMF.
机译:当电流通过时,电触头的断开会产生拉弧。在真空中,电弧从连接触点的熔融金属桥开始,然后破裂形成桥柱电弧。对于没有AMF且峰值电流高达16 kA的对接触点,在切换到扩散或扩散列模式之前,电桥会演变为过渡模式。先前的工作是在轴向磁场(AMF)的作用下观察真空中大电流引弧的发展,从而测量了桥柱演化为扩散模式所需的时间。现在,在带有AMF的Cu-Cr触点上进行电弧可视化实验已经确定,过渡到完全扩散模式的结构更加复杂。打开顺序从熔融金属桥的断裂开始,形成桥塔。此列演变为过渡模式,然后演变为完全扩散模式。过渡模式包括一个集中的阴极斑点区域,类似于对接触点的过渡模式。在几毫秒的时间内,各个阴极斑点开始出现在集中区域之外,直到形成扩散电弧。增加轴向磁场强度会缩短过渡模式的寿命。这种减少与电弧电压的变化相关。此外,过渡模式的出现也与以前在AMF中接触熔化的研究相吻合。

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