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Balanced static elimination in variable ion mobility environments

机译:在可变离子迁移率环境中平衡消除静电

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Electrical ionizers with point-to-point and point-to-plane electrode arramgements were evaluated for use in static elimination systems. Elevated-temperature tests to 433 K were done in air, while reduced-temperature tests to 213 K were done in the vapors from liquid nitrogen. Balanced static elimination was obtained throughout the temperature range by controlling the ratio of the potentials on the positive and negative emitters, and allowing large free-electron currents from the negative meitters in the nitrogen environment. The charge-decay times were continuous through the nitrogen-to-air transition and dependent upon temperature as exp(const./kT). Under balanced conditions, the ratio of charge-decay times for negative-charged and positive-charged targets increased from about 1.1 at 213 K to 1.4 at 323 K, and returned to about 1.0 at 433 K. In air, the charge-decay times at constant negative meitter current decreased and their ratio approached unity with incresing superificial flow in the chamber. Nitrogen injection about the emitters primarily influenced static elimination when gas circulation in the chamber was otherwise small. Separate control of positive and negative carrier generation is essential to achieve balanced static elimination in industrial applications.
机译:对具有点对点和点对平面电极布置的电离器进行了评估,以用于静电消除系统。在空气中进行了433 K的高温测试,而在液氮中的蒸气中进行了213 K的低温测试。在整个温度范围内,通过控制正负发射极上的电势比,并在氮环境中允许来自负发射极的大自由电子电流,可以实现平衡的静电消除。电荷衰减时间在氮到空气的过渡过程中是连续的,并且取决于温度,为exp(const./kT)。在平衡条件下,负电荷和正电荷目标的电荷衰减时间比例从213 K时的约1.1增加到323 K时的1.4,然后在433 K时返回到约1.0。当恒定负负金属离子流减小时,随着室中表观流量的增加,它们的比率趋于一致。当室内的气体循环较小时,围绕发射器注入的氮气主要影响静电消除。正负载流子产生的单独控制对于实现工业应用中的平衡静电消除至关重要。

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