Electrostatic Precipitator Design Calculator

Collection efficiency equals 1 minus e to the power of negative A times drift velocity over Q

Solution

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How It Works

An electrostatic precipitator (ESP) charges airborne particles with a high-voltage electrode, then collects them on grounded plates. The Deutsch-Anderson equation predicts collection efficiency based on the ratio of collecting-plate area and gas flow rate, scaled by the particle drift velocity toward the plates.

Increasing electrode area or reducing gas flow improves efficiency. Drift velocity depends on particle size, charge, and gas properties -- typical values range from 0.03 to 0.2 m/s.

Example Problem

An ESP has 5,000 m² of collecting area, handles 50 m³/s of gas, and the drift velocity is 0.05 m/s. What is the collection efficiency?

  1. R = 1 − e−(5000 × 0.05 / 50)
  2. R = 1 − e−5 = 1 − 0.0067
  3. R ≈ 99.3%

Frequently Asked Questions

What efficiency can an electrostatic precipitator achieve?

Modern ESPs routinely achieve 99–99.9% collection efficiency for particulate matter. Large power plants may use ESPs with collecting areas exceeding 10,000 m² to meet emissions standards.

What is drift velocity in ESP design?

Drift velocity is the speed at which charged particles migrate toward the collecting electrode. It depends on particle size, electric field strength, and gas viscosity. Common values are 0.03–0.2 m/s for fly ash applications.

How does the Deutsch-Anderson equation work?

The equation R = 1 − e−AVd/Q models collection as an exponential approach to 100%. Doubling the electrode area or halving the gas flow rate both raise the exponent, sharply increasing efficiency at high values.

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