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Improving
Air
System
Efficiency
by: R. Scot Foss, Plant Air
Technology
Part 10: There are a number of ways to deal with omnipresent water vapor
in compressed-air systems to avoid the problems of its evil companion,
liquid water.
In compressed-air systems, water is an
insidious contaminant. It enters a system invisibly. It causes
problems – corrosion, clogging, washing away lubricants – internally,
while still unseen. When water finally shows up at an exhaust port, its
damage already may be done.
Water can be damaging to pneumatic
production equipment on its own, but water also is a carrier. Many
other contaminants depend on water to distribute them around the system
or require liquid water to initiate a destructive reaction. One of the
most problematic is acid gas, a common airborne constituent in most
industrial atmospheres. When mixed with water in the cooling stages
after compression, this gas can form hydrochloric and sulfuric acids.
Without water, acid gas and many other contaminants could not do their
dirty work.
Almost all water enters a compressed-air
system in the form of vapor as part of the ambient air drawn in by the
compressor. Water vapor causes no problems. Only when it condenses
does it become a contaminant.
Terminology:
Special terminology has evolved to explain
the interrelationship of water vapor, temperature, pressure, and liquid
water. Misunderstanding and misuse of this terminology has led to a
great deal of confusion about the behavior of water vapor in
compressed-air systems and how to avoid the damage liquid water can
cause.
There is a well-defined, maximum amount of
water vapor that any gas can hold at any given temperature and
pressure. Compressed air under these conditions is said to be
saturated. If its temperature is increased, the air can hold more
water vapor. If the pressure of saturated air is increased or the
temperature decreased, some of the water vapor will condense. If
compressed air containing an arbitrary amount of water vapor is cooled
at constant pressure, some water eventually condenses. The temperature
at which condensation begins is called the saturation temperature.
Any statement about saturation temperature
must always include the system’s pressure. For the special case where
the air pressure is equal to atmospheric pressure, the saturation
temperature is called the dew point. However, some people use
the terms dew point and saturation temperature
synonymously. Hence, it always is good practice to include a statement
of pressure when mentioning dew point temperatures as well. This
precision avoids confusion. (When a pressure does not accompany dew
point information, atmospheric dew point is assumed.)
In systems that operate below 0o
F, the user may measure dew point from an air sample that expanded from
system pressure to atmospheric pressure. That resulting dew point is
significantly lower than that which would have been measured at
pressure. The user then thinks that he has achieved an adequate dew
point, when the dryer on line may be operating at 30o to 40o
F above the rated performance.
For engineering calculations, humidity
usually is written as the weight of water per unit weight of
moisture-free compressed air (e.g., 0.001 pounds of water per pound of
dry air). Frequently, these numbers are very small decimal fractions,
so it is more convenient to express them as parts of water vapor per
million parts of dry air. The conversion to ppm by weight merely
involves moving the decimal point six places. But again, care must be
exercised. Most constituents of an air sample are analyzed on a
volumetric basis; hence, chemists often report water and contaminants as
ppm by volume.
The percentage relative humidity (%RH)
is 100 x the ratio of partial pressure of water vapor to the vapor
pressure of water at the stated temperature. Many people confuse
percentage relative humidity with percentage saturation
(which sometimes is called percentage humidity). Percentage
saturation is 100 x the ratio of the existing weight of water vapor per
unit weight of dry air to the weight of water vapor that would exist per
unit weight of dry air if the air were saturated at the existing
temperature and pressure. Another way to express water or water vapor
content is as weight (grains or pounds) of water per unit volume
(standard cubic foot) of compressed air.
Removing Water Vapor:
There are many methods that will remove
water and water vapor from compressed air. Mechanical methods, such as
centrifugal separation or porous-media filtration, usually will take out
liquid water, mist, and droplets only; vapor remains. Note that these
methods are very velocity sensitive. Too high or too low an air steam
velocity will degrade performance.
Refrigeration drying is limited to the
saturation moisture content of the air at the refrigerant temperature.
All of the moisture will condense down to the airside heat-exchanger
temperature in the refrigerant-to-air heat exchanger. The balance of
moisture present will exist saturated at the discharge temperature from
the dryer. You must also provide a mechanical separator to remove the
liquid condensate, which results from this process. The efficiency of
the dryer is dependent on the efficiency of the separator. Many
separators in dryers are 80 to 95% efficient in moisture removal. The
liquid water not removed in the separator will be absorbed into a vapor
state in the air stream in the reheat cycle of the refrigerant dryer.
This will result in higher than intended pressure dew points. The
efficiency of the separator is largely dependent on its ability to
isolate the separated liquid from the air stream so that it cannot be
re-entrained. This is why most 35oF dew point refrigerated
dryers perform much better than those rated for 40o to 42oF.
Chemical Drying:
Deliquescent drying involves chemicals –
usually in tablet form – made up primarily of salt and desiccated urea.
The compressed-air stream is usually directed through a bed of
deliquescent tablets, which adsorbs the water vapor. A chemical phase
conversion produces a liquid brine solution that runs down into a
holding tank (A timer or solenoid-operated drain valve arrangement
typically removes the brine.) This type of dryer can reduce pressure
dew points by 20o to 40o F.
One of the potential problems associated
with deliquescent drying is the highly corrosive nature of the tablets
and the brine. Another is the bed geometry. Optimum dew-point
reduction depends on the bed geometry as well as saturation temperature
and mass flow of the compressed air. As the bed dissolves during its
normal functioning, its geometry changes and the dew-point reduction
performance can degrade.
Obviously, maintaining the bed geometry or
desiccant level is important to the operation of the dryer. Maintenance
involves topping off the bed with fresh tablets. While this sounds
simple, remember that this dryer is a pressure vessel. To add
desiccant, the dryer first must be isolated from the system and
depressurized. If a bypass valve is installed to provide isolation,
gross water may drop out downstream when the valve closes. If there is
no valve, the whole air system has to be shut down – if possible. What
happens in the real world is that the bed is seldom serviced until the
moisture content of the plant air gets so high that there are complaints
form the production people.
Another factor in desiccant-dryer operation
is that the chemicals will absorb lubricants and liquid water from the
air stream. Both of these liquids interfere with the tablets’
performance. So for desiccant dryers to function at their best, it is
very important to provide pre-filtration that removes all liquids and
aerosols prior to drying.
Adsorption Drying:
In the adsorption process, vapors are
attracted to and condense on the interior surfaces of certain solid
materials or tablets, which contain literally millions of submicroscopic
pores and cavities. There is no chemical reaction, so adsorption is
generally superior to absorption because it is not corrosive an does not
require the frequent material refills. When the chemical bed becomes
saturated, it can be regenerated by driving out the collected moisture
with heat of flowing dry air through it.
The adsorption process can easily produce
consistent pressure dew points of –20oF and lower. (When
necessary, a properly engineered and applied adsorption dryer can
produce pressure dew points below –100oF.)
Adsorption dryers typically are constructed
as twin towers. While one active tower is drying air, the other tower
is regenerating. Once the first tower’s desiccant bed is saturated, a
valve shifts to divert the raw air stream to the second dry tower. If
the regeneration is performed by dry air – which reabsorbs the moisture
from the bed – the technique is identified as heatless. This
heatless technique uses a portion of the dry air exiting from the drying
tower to regenerate the wet tower.
In a typical heatless dryer rated at –20o
to –40oF Pressure dew point, the quantity of air
consumed for regeneration is about 15% of the rated flow capacity of the
dryer at pressure. If the pressure is higher, the purge flow will be
higher. If the pressure is lower, the dryer may be unable to produce
the desired pressure dew point. Dew points lower than –40oF
will require higher flows, sometime approaching 25 to 30% of the dryer’s
rated performance. The drying cycle for tower changes usually is about
five minutes.
The other approach towards regeneration is
with heat. The heat source can be internal or external. Calrod heaters
can be installed right in the bed, or electric heater elements can be
mounted on the towers’ exteriors. (An alternate internal heat source is
steam, if available.) Note that drying temperatures can approach 450oF.
This can be a problem if a lubricated compressor supplies the system;
most compressor lubricants have flash points well below 450oF.
The initial cost of externally heated dryers
is significantly more than internally heater or heatless dryers. The
operating cost of heated dryers doesn’t vary much from type to type, but
they do require so purge air in order to function. Generally to purge
flow consumes about 6% of the dryer capacity. It is important to
understand that when we say a percentage of dryer capacity, we do not
refer to the mass being processed. If a dryer is rated at 1,000 scfm,
it will use the same amount of purge flow whether it is operating at 10%
or 100% of capacity.
Another type of dryer uses the heat of
compression to regenerate the bed. The hot air flow exiting the
compressor is channeled directly to the tower to be regenerated, then
through the aftercooler where some moisture is condensed, and finally to
the active tower for more drying. This arrangement is by far the most
economical of all forms of regeneration. Its drawback is that
maintaining the proper bed temperatures may be difficult. If the
airflow is too high or the temperature is too low, the dryer will not
work correctly. Too many heat-of-compression dryers have not performed
properly because flow and temperature were not considered.
Although there are other methods for drying
compressed air – such as microwaves and membranes – the systems just
described represent the large majority of those used commercially in
industry for water and vapor removal.
Temperature
Considerations:
Like everything in life, good ideas poorly
applied do not work. One drawback of all heat-regenerated dryers is the
high bed temperature. The temperature of air discharging into the
system immediately following tower switching can be 200oF or
higher. The air temperature will reduce to 100oF in time for
the towers to switch again. It is possible that this cyclical
temperature swing will adversely affect some downstream production
processes. Remember: the weight flow of the air at 200oF and
100 psig is 0.470 lb/cf, while the same cubic foot of air weighs 0.551
lb/cf at 100oF and 100 psig. The 15% lower density at the
elevated temperature may be a problem.
Other Water-Ingression
Points:
In addition to the well-documented point
that most water vapor comes into a system with the air in the
compression inlet, there are other less-commonly understood ways for
water to enter. Leaks – even pinhole types – can be a source of water
contamination. The assumption that nothing can get into a pressurized
system because pressure inside is greater than pressure on the outside
is not always valid. There are a least three effects that allow this
intrusion: jet pump, shortened diffusion path, and molecular flow.
The jet pump effect siphons stagnant
external contaminants into a system when a high-velocity pressurized gas
steam passes over a leak point. The entry opening can be as small as
0.00001 in. It only needs to be larger than the molecule of moisture or
contaminant that is drawn into the system in what is called a direct
hit.
The shortened diffusion path effect occurs
when a leak or leaks allow outflow from a pressurized system. The hole
in the pipe acts as an orifice, and the cross-sectional area of the jet
formed by leaking compressed air may decrease over a finite distance
downstream from the inner edge of the hole where the leak originates.
Eddy currents then form near the hole. The refrigeration effect from
the expansion of the leaking air may be sufficient to cause water vapor
to condense both in the vicinity of and around the edges and sides of
the hole. The actual path length a water molecule must travel to enter
the system may not be the metal thickness but rather a shorter distance
near the leak’s inner edge.
Molecular flow can occur if the partial
pressure of the vapor inside the system is sufficiently lower than the
partial pressure of the vapor in the ambient air. Water vapor will
diffuse through a solid pipe wall and enter the system. This phenomenon
occurs where compressed air systems are operating at pressure dew points
of –40oF or less and the outside-saturated temperature is
high.
The proper selection of the piping material
can significantly reduce the potential for contaminant ingression via
this effect. Systems that have pressure dew points of -75oF
to -100oF or lower should use copper or pickled-and-lined
pipe to prevent this diffusion path problem from downstream
contaminants. An extreme application error would be to use very dry
compressed air for open blowing where the atmosphere is quite humid.
In fact, the most ludicrous method of
contaminating a system with water is to drive the dew point of the air
down to the point where it is hydroscopic, and then expose the gas to a
liquid downstream of the drying process. Vapor seeks the lowest vapor
pressure. A condensation problem can occur after regeneratively drying
compressed air at the source to a low dew point and then using the air
for one of these applications downstream:
-
Sparging or agitating any liquid with
compressed air,
-
Dripping or atomizing oil via
point-of-use lubricators into the air steam,
-
Agitating sludge or chemicals with air,
-
Aspirating oil or other liquids with
compressed air,
-
Transporting slurries or powdered
solids through a pipeline using compressed air, and
-
Spilling high-pressure, wet compressed
air into a drier compressed-air source.
In most systems, this effect can occur when
the air is extremely dry and the atmosphere is very wet, or when very
dry air comes in contact with liquid. The greater the dryness extremes
between the air and the contaminant, the greater the problem. When
molecular diffusion brings water into a system where water contamination
is unacceptable to production, the uneducated solution may be to make
the air even dryer. This, of course, exacerbates the problem rather
than solving it.
Conclusion:
Compressed air needs only to be dry enough
to suit its application. Excessive drying may fix one problem, but it
creates new ones in the process – and more drying costs more.
Reprinted with
permission from R. Scot Foss, president of Plant Air Technology,
Charlotte, N.C., a company specializing in system auditing and design.
This article is based on his book, "Compressed Air System Solution." A
portion of the proceeds from sales of the book is donated to children’s
charities. To order a copy of the book, please contact Southern
Corporation. |