Swarm parameters along gas-solid dielectric interfaces

S. Mahajan, T. Sudarshan, R. Dougal
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引用次数: 1

Abstract

In order to understand the surface flashover mechanisms in a spacer-bridged, compressed-gas-insulated system, it is essential to have a detailed knowledge of the associated physical parameters, these being dominantly the first Townsend ionization coefficient (α) and the electron drift velocity (Ve). As the addition of a solid spacer to a compressed gas insulated system inevitably reduces the breakdown strength it is important to know how α and Ve are modified or if these are modified at all. These parameters can be determinated through the measurement of electron avalanches using the pulsed Townsend technique [1,2]. Jaksts and Cross attempted such measurements, however, the relatively long pulse width (∼10ns) of the laser used for photo-initiation of the electron avalanche and the poor bandwidth of the electron current amplifier, coupled with noise from the laser, prevented accurate measurements [3].
沿气固介质界面的群参数
为了了解间隔桥接压缩气体绝缘系统中的表面闪络机制,有必要详细了解相关的物理参数,这些参数主要是第一汤森电离系数(α)和电子漂移速度(Ve)。由于在压缩气体绝缘系统中添加固体隔离剂不可避免地会降低击穿强度,因此了解α和Ve是如何修改的,或者是否对它们进行了修改,是很重要的。这些参数可以通过使用脉冲Townsend技术测量电子雪崩来确定[1,2]。Jaksts和Cross尝试了这样的测量,然而,用于电子雪崩光引发的激光的相对较长的脉冲宽度(~ 10ns)和电子电流放大器的差带宽,再加上激光的噪声,阻碍了精确的测量[3]。
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