屏蔽容量对真空管击穿电压的影响

U. Schumann, M. Budde, M. Kurrat
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引用次数: 1

摘要

使用普通真空开关,在系统中内置屏蔽电极来控制电场分布。因此,屏蔽电极代表了与接触电极平行的额外容量。这种电极在真空中的高压强度预测是复杂的。电极材料、表面光洁度、表面积、表面调理状态和电极排列的几何形状等一系列参数都对电极性能有影响。众所周知,电极的面积会影响真空中的介电强度。随着面积的增加,介电强度减小,相反,电极布置的容量增大。这项工作表明,在真空管中代表并联容量的屏蔽不会改变触点系统在雷击电压下的击穿行为。由于屏蔽的间隙距离明显大于接触系统的间隙距离,因此不能指望通过“面积效应”从增加的总表面中降低击穿电压。击穿电压与电极表面面积之间的经验关系也可以描述为容量影响。但是,不断增加的运力并不是造成这种现象的原因。为此目的。共面电极在雷电冲击电压(1.2/50μs)条件下受力。测试容器能够拾取一对以上的电极。这使得通过第二对甚至第三对并联电极来改变总电容成为可能。对测量结果进行了讨论,并与面积效应进行了比较。
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Influence of shield capacity on the breakdown voltade of vacuum tubes
With a normal vacuum switch, shield electrodes are built into the system to control the electric field distribution. The shield electrodes thus represent an additional capacity, which is in parallel to the contact electrodes. The prediction of the high-voltage strength of such electrode arrangements in vacuum is complex. Effects of a wide range of parameters like electrode material_ surface finish: surface area, conditioning state of the surface and the geometry of the electrode arrangement exist. It is well known that the electrode's area influences the dielectric strength in vacuum. With increasing area the dielectric strength decreases, in the opposite direction the capacity of the electrode arrangement rises. This work shows that shields in a vacuum tube which represent a parallel capacity, do not alter the breakdown behaviour during lightning impulse voltage of the contact system. Since the gap distance of the shields lies clearly over that of the contact system, a reduction of the breakdown voltage is not to be expected from the increasing total surface by the ¿area effect¿. The empirical relation between the breakdown voltage and the area of the electrodes surface can also be described as a capacity influence. But the increasing capacity is not causal for the phenomenon. For this purpose. coplanar electrodes are stressed and conditioned with lightning impulse voltage (1.2/50μs). The test vessel is enabled to pick up more than one pair of electrodes. That makes possible to vary the total capacitance by a second or even third parallel connected pair of electrodes. The results of the measurements are discussed and compared to the area effect.
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