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The power supply system is designed to provide voltage to the electrical field (or bus section) at the highest possible level. The voltage must be controlled to avoid causing sustained arcing or sparking between the electrodes and the collecting plates.
Electrically, a precipitator is divided into a grid, with electrical fields in series (in the direction of the gas flow) and one or more bus sections in parallel (cross-wise to the gas flow). When electrical fields are in series, the power supply for each field can be adjusted to optimize operation of that field. Likewise, having more than one electrical bus section in parallel allows adjustments to compensate for their differences, so that power input can be optimized. The power supply system has four basic components:
Automatic voltage control varies the power to the transformer-rectifier in response to signals received from sensors in the precipitator and the transformer-rectifier itself. It monitors the electrical conditions inside the precipitator, protects the internal components from arc-over damages, and protects the transformer-rectifier and other components in the primary circuit.
The ideal automatic voltage control would produce the maximum collecting efficiency by holding the operating voltage of the precipitator at a level just below the spark-over voltage. However, this level cannot be achieved given that conditions change from moment to moment. Instead, the automatic voltage control increases output from the transformer-rectifier until a spark occurs. Then the control resets to a lower power level, and the power increases again until the next spark occurs.
To maximize electrostatic precipitator efficiency, a voltage controller usually attempts to increase the electrical power delivered to the field. However in some conditions a voltage controller must just maintain power at a constant level. Increased electrical power into the electrostatic precipitator directly correlates with better precipitator performance, but there is a limit. If too much voltage is applied for a given condition (as mentioned in the spark reaction section), a spark over will occur. During a spark over precipitator performance in that field will drop to zero, rendering that field temporarily ineffective.
To overcome the crippling effect that spark over has to increasing the electrical power in the precipitator field, spark response algorithms have been developed that will interrupt power upon detection of a spark, then ramp power back up to a high level. These response algorithms can greatly influence overall precipitator performance.
Transformer/Rectifiers – The T/R set rating should be matched to the load imposed by the electrical field or bus section. The power supply will perform best when the T/R set operates at 70 – 90% of the rated capacity, without excessive sparking. This reduces the maximum continuous-load voltage and corona power inputs. Practical operating voltages for T/R sets depend on:
At secondary current levels over 1500 mA, internal impedance of a T/R set is low, which makes stable automatic voltage control more difficult to achieve. The design of the T/R set should call for the highest possible impedance that is commensurate with the application and performance requirements. Often, this limits the size of the electrical field or bus section. ¨It is general practice to add additional impedance in the form of a current-limiting reactor in the primary circuit. This reactor will limit the primary current during arcing and also improve the wave shape of the voltage/current fed into the T/R set.
Corona current density should be in the range of 10 – 100 mA/1000 ft2 of plate area. (Calculate this using secondary current divided by collecting area of the electrical field or bus section.) The actual level depends upon:
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