Particles are
charged by negative gas ions moving toward the collection plate by one of these
two mechanisms: field charging or diffusion charging. In field charging (the mechanism
described above), particles capture negatively charged gas ions as the ions move
toward the grounded collection plate. Diffusion charging, as its name implies, depends
on the random motion of the gas ions to charge particles.
In field charging (Figure 1), as
particles enter the electric field, they cause a local dislocation of the
field. Negative gas ions traveling along the electric field lines collide with
the suspended particles and impart a charge to them. The ions will continue to
bombard a particle until the charge on that particle is sufficient to divert
the electric lines away from it. This prevents new ions from colliding with the
charged dust particle. When a particle no longer receives an ion charge, it is
said to be saturated. Saturated charged particles then migrate to the
collection electrode and are collected.
Diffusion charging is
associated with the random Brownian motion of the negative gas ions. The random
motion is related to the velocity of the gas ions due to thermal effects: the
higher the temperature, the more movement. Negative gas ions collide with the
particles because of their random thermal motion and impart a charge on the particles.
Because the particles are very small (submicrometer), they do not cause the electric
field to be dislocated, as in field charging. Thus, diffusion charging is the
only mechanism by which these very small particles become charged. The charged
particles then migrate to the collection electrode. Each of these two charging
mechanisms occurs to some extent, with one dominating depending on particle
size. Field charging dominates for particles with a diameter >1.0 micrometer
because particles must be large enough to capture gas ions. Diffusion charging
dominates for particles with a diameter less than 0.1 micrometer. A combination
of these two charging mechanisms occurs for particles ranging between 0.2 and 1.0
micrometer in diameter. A third type of charging mechanism, which is
responsible for very little particle charging is electron charging. With this type of charging, fast-moving free
electrons that have not combined with gas ions hit the particle and impart a
charge.
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