Electrostatic Precipitator Dust Capture

2D twin of the 3D precipitator digital twin: dust is charged near the wires, then pushed to the plates by the electric field.

Presets

Playback

Operating point

Higher voltage and slower gas raise the efficiency; moisture and very high fields push the device toward sparking.

Maintenance

Model checks

The science

What is modelled

Dust in a gas stream is charged by corona ions (field charging, saturating at qs = 3πε0 d2E), then migrates toward the collector plates at the electrical terminal velocity w = q E C / (3πμ d) with a Cunningham slip correction C.

Equations

  • Mean field E = V / (pitch / 2).
  • Deutsch-Anderson efficiency η = 1 - exp(-w A / Q), where A/Q is the collecting area per unit gas flow.
  • A dust layer reduces the effective field until rapping shakes it off.

Honest limits

The particle simulation is a teaching model: it uses a stronger field near the wire and weights by particle mass, so it reads higher than the uniform-field Deutsch law; it has no re-entrainment, back corona or turbulence. Not a design tool.

What to try
  • Choose Low voltage: the efficiency drops sharply, since drift velocity grows with the square of the field.
  • Choose Fast gas flow: particles have less time to cross the channel and more escape.
  • Choose Humid gas near sparking and watch the sparking risk rise as the field approaches breakdown.
Collection efficiency: simulation against the Deutsch law
Ideal efficiency against plate voltage
Drift velocity against particle size
Dust layer on the plates
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