首页> 外文会议>Industry Applications Society Annual Meeting, 1992., Conference Record of the 1992 IEEE >High speed electrostatic surface discharge between a charged thinfilm and a sphere electrode with or without a thin dielectric film onthat
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High speed electrostatic surface discharge between a charged thinfilm and a sphere electrode with or without a thin dielectric film onthat

机译:薄带电之间的高速静电表面放电膜和带或不带电介质薄膜的球形电极那

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The electrostatic surface discharge (ESD) between a charged thindielectric film on a conductive flat plate electrode and a sphereelectrode that is connected to the plate, and is either covered with anuncharged thin dielectric film or fare, was observed. Discharge currentwaveform, discharge gap length, current risetime, discharge photographs,current peak value, etc. were recorded. The initial charge generation byirradiation with beta-rays or ultraviolet light was not readilyapparent, so that the reproducibility of ESD experiments was not muchimproved. The charging polarity dependence of such a surface ESD betweentwo dielectric films becomes small with increasing film thickness. Thedischarge gap length of an ESD with an 12.5 μm uncharged film on theelectrode reduces to 50 or 70% of that between a charged film and asphere metal electrode. Peak current and transferred charge value ofsuch an ESD also decreases to roughly one-third of that between the filmand the electrode
机译:带电薄层之间的静电表面放电(ESD) 导电平板电极和球体上的介电膜 连接到板上的电极,或者覆盖有 观察到不带电的薄介电薄膜或票价。放电电流 波形,放电间隙长度,电流上升时间,放电照片, 记录当前峰值等。初始电荷的产生 用β射线或紫外线照射并不容易 很明显,因此ESD实验的可重复性不高 改善。这种表面ESD之间的充电极性依赖性 随着膜厚度的增加,两个电介质膜变小。这 静电放电(ESD)的放电间隙长度,其上有12.5μm的不带电薄膜 电极减少到带电膜和带电膜之间的50%或70% 球形金属电极。的峰值电流和转移的电荷值 这样的ESD也减少到薄膜之间的ESD的三分之一左右 和电极

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