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首页> 外文期刊>Journal of Applied Physics >Dynamic and stationary charging of heavy metallic and dielectric particles against a conducting wall in the presence of a dc applied electric field
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Dynamic and stationary charging of heavy metallic and dielectric particles against a conducting wall in the presence of a dc applied electric field

机译:在直流施加电场的作用下,重金属和介电粒子在导电壁上的动态和静态充电

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摘要

Dielectric and metallic paricles (both spherical and irregular in shape) in the range 29-4760 μm in diameter are electrically charged while in dynamic or stationary contact with either wall of a charged parallel‐plate capacitor. The charge distribution received tends to remove any particle from the wall. Particles larger than 127 μm are studied individually with dc electric field strengths of 2-15 kV/cm. Smaller particles are studied mainly in the form of clouds. In the presence of gravity and standard atmosphereic air, the particle motion, once initiated, is continuous between the parallel plates both dynamic and stationary charging and the resulting particle motion are experimentally and theoretically studied considering the particles as capacitors in themselves. For copper particles a single formula of the form Q= (πϵ) a2EK applies 2EK applies with K=1.64 whether or not charging is dynamically or statically acquired. The presence of an oxide film does not alter K. Dielectric particles followed a similar equation (K≪1.64) when contact (triboelectric) charging was assumed small and surface electrical conductivity was sufficiently large. K for dielectrics is dependent on surface conductivity, permittivity, diameter, and contact time. Induced average particle velocities in atmospheric air were tested from 40 to 105 cm/s. Inelastic particle‐wall collisions and a conservative body force such as gravity resulted in a critical lower limit electric field strength for sustained particle motion. Gaseous discharge from a particle to a wall of opposite sign can occur with sufficient particle size and electric field strength.
机译:直径在29-4760μm范围内的介电和金属粒子(球形和不规则形状)会带电,同时与带电的平行板电容器的任一壁动态或静态接触。接收到的电荷分布趋于从壁上去除任何颗粒。单独研究大于127μm的粒子,其直流电场强度为2-15 kV / cm。较小的粒子主要以云的形式研究。在存在重力和标准大气的情况下,粒子运动一旦开始,便在平行板之间是连续的,无论是动态充电还是静止充电,并且通过将粒子本身视为电容器的实验和理论研究所得的粒子运动。对于铜粒子,无论是动态还是静态获取电荷,均采用Q =(πϵ)形式的单个公式a2EK适用2EK,K = 1.64。氧化膜的存在不会改变K。当假定接触(摩擦带电)较小且表面电导率足够大时,介电粒子遵循类似的方程(K≪1.64)。电介质的K取决于表面电导率,介电常数,直径和接触时间。在大气中诱导的平均粒子速度测试为40至105 cm / s。非弹性的粒子壁碰撞和保守的体力(例如重力)导致了持续的粒子运动的临界下限电场强度。从颗粒到相反符号的壁的气体放电可以在具有足够的颗粒大小和电场强度的情况下发生。

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    《Journal of Applied Physics》 |1976年第11期|P.4839-4849|共11页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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