We undertake all types of works for Dry ESP  under Overhauling, Performance Enhancement, Technical troubleshooting and Erection Works. Visit our site for details.
Causes of poor performance of ESP & discussions
There are many causes of poor
performance of ESP (Electrostatic Precipitators). Some of the reasons are:
·       Excess gas volume
·      
Poor gas distribution
·      
Tracking and air inleakage
·      
Electrode breakage
 
·      
Ash resistivity
·      
Particle size
 
·      
Electrical conditions
·      
Over-full 
hoppers
 
·      
Defective collector plates
Excess gas volume
If the gas volume is high, the gas
velocity through the precipitator will be high so that the time available for
the charged particles to migrate to the collector plates is reduced, possibly
to the extent that the particles pass out of the working zone before they can
be captured. The normal gas velocity is about 2 m/s, but this may be increased
by:
Poor gas distribution
It could be that the total gas flow is satisfactory but the spatial distribution is poor, causing good performance where the gas velocity is low and for it to be poor where the velocity is high. To be completely acceptable, all the traverse point velocities should be within 25% of the average for the duct.
Tracking and air in leakage
This is a common cause of trouble
because precipitator structures are physically large and have numerous access doors,
etc, at which leakage can occur. If the in leakage is sufficiently high, a draft
of cool and possibly moist air will pass over the insulators, steady bars, etc.
As the voltage inside a precipitator is very high (40-50 k V), tracking paths
may result. Therefore, it is important that access -door seals, rapping rod
covers, expansion joints and other ingress points are kept in good condition
and are airtight.
Poor rapping
In the usual precipitator arrangement
the wires are negatively charged and the collector plates are earthed. In the
immediate vicinity of the wires the electrostatic field is so strong that
corona discharge occurs. The corona ionizes the flue gases and the entrained
solid particles acquire negative ions, causing them to migrate towards the
relatively –positive collecting plates. A few particles acquire positive ions
and theses migrate towards the discharge electrodes.
Electrode 
breakage
The discharge electrodes consist of
relatively thin wires which may be of flat, circular, star or square
cross-section. In addition, they may be barbed or plain, twisted or straight
and rigidly or loosely fastened, besides being made from a range of materials. Whichever
arrangement is adopted, the essential requirement is that the wires should have
excellent reliability. Out of the huge number in a zone, it only needs one to
break to cause short-circuiting and electrical instability generally, which may
seriously affect the performance of the plant.
Ash resistivity
An important factor in precipitator
performance is the electrical conductivity of the ash itself. Poor combustion
can result in a higher than normal carbon content in the ash. This causes the
particles to have a lower resistivity which may cause them to be difficult to
collect. This means that they can be readily re-entrained by the gas,
particularly during rapping. On the other hand, if the resistivity is too high,
the dust will accumulate on the collector plates and form an insulating layer,
so preventing subsequent particles from surrendering their charge.
Consequently, the charge on the surface layer will repel incoming dust, causing
re-entrainment. In addition, a very high voltage- gradient will be built up
across the dust layer which could result in flashover. Dust with high
resistivity will suppress the corona discharge, seriously lowering the
performance of the plant.
Particle size
Particle sizing has an important
bearing upon the efficiency of precipitations. Up to approximately 20 µm, the
electrical and the drag forces combine to give a deposition velocity which
increases in roughly efficient for sizes over 20 µm, the only problem being
that of slight re-entrainment. Dust less than 20 µm is more difficult to
capture, so the stack emission will contain a preponderance of fine particles.
Electrical conditions
Figure below shows the relationship
between electrical power input and   precipitator efficiency. As one would expect,
increased power results in improved performance, provided the power is useful.
For example, flashover and tracking
will give high power consumption, but much of it is wasted. To find the
demarcation between useful and wasted power, a simple graph is determined from
tests on the plant. Starting at a low value the current is increased by
suitable increments, noting the corresponding voltage. A typical diagram is
shown below:
Notice that the current and voltage
both increase until the voltage is about 45 k V. Thereafter increasing current
is accompanied by reducing voltage. The knee of the curve determines the
demarcation between stable and unstable operation, the highest stable current
here being a little over 200 m A.
The automatic voltage control always tries to operate the plant with the
highest stable power input which can be maintained.
·      
Tracking , possibly due to air ingress
Defective collector plates
The plates are mechanically strong,
but can become defective if the gas temperature falls below the dew point,
allowing deposition of dilute acid. This can occur in discrete areas if cold
air inleakage takes place. Alternatively, general corrosion can occur if the
flue gas itself has a low temperature, possibly due to massive air ingress at
defective seals on the ducts between the air heater and the precipitator, or if
the ducting is corroded and holed. Frequent cold-starting of the boiler can
also lead to low- temperature gas at the precipitator.
We undertake all types of works for Dry ESP  under Overhauling, Performance Enhancement, Technical troubleshooting and Erection Works. Visit our site for details.
·      
Electrode breakage
·      
Particle size
·      
Over-full 
hoppers
Excess gas volume
If the gas volume is high, the gas
velocity through the precipitator will be high so that the time available for
the charged particles to migrate to the collector plates is reduced, possibly
to the extent that the particles pass out of the working zone before they can
be captured. The normal gas velocity is about 2 m/s, but this may be increased
by:
·      
Tramp air in leakage at the boiler.
·      
High air heater gas outlet temperature
causing increased volume flow.
·      
Poor condition of rotary air heater seals.
·      
Operating the boiler with too much excess
air.


 
 
