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首页> 外文期刊>IEEE Transactions on Plasma Science >Transition to the Diffuse Mode for High-Current Drawn Arcs in Vacuum With an Axial Magnetic Field
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Transition to the Diffuse Mode for High-Current Drawn Arcs in Vacuum With an Axial Magnetic Field

机译:轴向磁场在真空中过渡到大电流绘制电弧的扩散模式

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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. Previous work observing the development of drawn arcs in vacuum with an imposed axial magnetic field (AMF) measured the time required for the bridge column to evolve into the high-current 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 development. With high-speed photography, we characterized the appearance of the arc modes over half-cycles of power frequency short-circuit current. 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. This transition mode in an AMF consists of a region of concentrated cathode spots, similar to the transition mode for butt contacts at lower currents and no AMF. Over a few milliseconds, an increasing number of individual cathode spots begin to appear outside the concentrated region, until a diffuse arc forms. The transition mode produces a transient peak in the arc voltage. Increasing the AMF strength at a particular current can shorten the duration of the transition mode and reduces the arc voltage peak. Single or multiple half-cycle operations have been performed on Cu-Cr contacts to investigate the effect of the transition mode on contact melting. The melting patterns after a single half-cycle of high current are correlated with the behavior observed in the arc movies. Anode melting is confined to one or two regions of shallow melting, while individual cathode spot tracks covered most of the cathode surface. The combination of arc visualization and post-arcing contact examinations demonstrated that the transition arc mode was a significant source of contact melting.
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。先前的工作是在真空中用施加的轴向磁场(AMF)观察引弧的发展,该过程测量了桥柱发展为大电流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,向全扩散模式的过渡具有更为复杂的发展。通过高速摄影,我们在工频短路电流的半个周期内表征了电弧模式的出现。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。 AMF中的这种过渡模式包含一个集中的阴极斑点区域,类似于在较低电流且无AMF时对接触点的过渡模式。在几毫秒内,越来越多的单个阴极斑点开始出现在集中区域之外,直到形成扩散电弧。过渡模式会在电弧电压中产生一个瞬态峰值。在特定电流下增加AMF强度可以缩短过渡模式的持续时间,并减小电弧电压峰值。已经对Cu-Cr触点执行了一个或多个半周期操作,以研究过渡模式对触点熔化的影响。单个大电流半个周期后的熔化模式与电弧电影中观察到的行为相关。阳极熔化被限制在一个或两个浅熔化区域,而单个阴极斑点轨道覆盖了大部分阴极表面。电弧可视化和电弧后接触检查的结合表明,过渡电弧模式是接触熔化的重要来源。

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