In the initial charge phase the high voltage setting is used. When charging is nearly complete and the charge voltage has risen to a specified value (with the charge current decreased), the charger switches the voltage to the lower setting. This method allows rapid charging in cycle or float service without the possibility of overcharging, even ...
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Get PriceAbstract: In vacuum, the surface of insulators becomes electrically charged when subjected to high-voltage stresses. The charging mechanism is described. A model simulating the charging shows that the surface charge densities are proportional to the applied voltage and depend on the secondary electron emission of the dielectric surface.
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Get PriceIn vacuum, the surface of insulators becomes electrically charged when subjected to high-voltage stresses. The charging mechanism is described. A model simulating the charging shows that the surface charge densities are proportional to the applied voltage and depend on the secondary electron emission of the dielectric surface. It is also time dependent.
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Get PriceIn the initial charge phase the high voltage setting is used. When charging is nearly complete and the charge voltage has risen to a specified value (with the charge current decreased), the charger switches the voltage to the lower setting. This method allows rapid charging in cycle or float service without the possibility of overcharging, even
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Get Price360 Zouache et al.: Electrical Breakdown of Small Gaps in Vacuum 0 10 20 d(lO.m) 30 Figure 4. Breakdown gradient vs. electrode separation (0 < d < 30 pm Eloc = PE,, where p is the field multiplication factor.When the interelectrode gap d is low in comparison to microprotrusion height H, the values of p are low.This requires a high macroscopic field to initiate
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