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Are You Worried Your Particle Counter May Be Reporting
Inaccurately?
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Are you performing filter testing?
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Is your cleanroom ISO class 8 or ISO class 9?
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Are you using a cleanroom particle counter to perform sampling in an
IAQ or
non-cleanroom environment?
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Do you think you may be exceeding the concentration limit of your
particle counter?
If you answered YES to ANY of these questions,
you are at high risk of recording bad data due to coincidence
counting! Consult with an expert to find out if you
need an aerosol diluter for your application. Call
1-800-531-4889.
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Aerodynamic Particle Sizer,
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Proper Filter Integrity Testing
Requires Aerosol Dilution
During the 1980’s, miniaturization in the semiconductor industry
required very clean, particle free cleanrooms to be
developed. It was critical the HEPA filters and
ULPA filters in the cleanrooms be free of pinhole defects
that would allow contamination into the process. The traditional
method to determine filter integrity required challenging the
filters with a high... [More Information]
Aerosol Diluter by Milholland and Associates
|
Product |
Pros |
Cons |
Features |
Application |
MSRP |
Aerosol Diluter
Model 450 AD
Model 1000 AD
 |
• Simple to operate
• Portable
• No Power Source Needed
• Comes with all necessary tubing |
• Unattractive Casing |
• Particle Dilution of 450:1 for Model
450AD
• Particle Dilution of 1000:1 for
Model 1000AD
• NIST Traceable Calibration |
Filter testing
Aerosol Research
Cleanroom
Pharmaceutical
Aerospace
Semiconductor |
Call for Price
Call to learn more about the Aersosol
Dilutor |
concentration of DOP (oil) droplets and then
scanning the downstream filter face (surface) with an aerosol
photometer. Leaks were
determined to be any defect resulting in a reading greater than
0.01% of the challenge concentration.
As the semiconductor geometries
decreased, airborne molecular compounds (AMC’s) became a
contaminant. One source of AMC’s was the oil used as a challenge
aerosol for filter integrity testing. In the late 1980’s a new
process was developed that used polystyrene latex spheres (PSL) as a
challenge aerosol and the particle counter as a detection device.
This process used considerably less total aerosol challenge than the
photometer method. With only 1x10-3 of the mass of the DOP aerosol
and a more stable latex sphere, AMC’s from filter integrity testing
were no longer a problem.
Need for Aerosol Dilution Device
A major obstacle that had to be overcome was measuring the
PSL aerosol challenge concentration. Aerosol particle counters are
designed to measure individual particles and are limited to
approximately 5x104
to 1x105 particles per minute, depending on the counter
design. Thus, direct sampling is limited to a maximum of up to
100,000 particles per cubic foot for a counter with a 1.0 cfm sample
rate or 1,000,000 per cubic foot for a counter with a 0.1 cfm
sample. Coincidence counting occurs when concentrations exceed these
limits. The counting errors can be due to both optical and
electronic coincidence. Simply stated, coincidence occurs when two
or more small particles pass through the laser beam at the same
instant and the counter counts them as only one larger particle. As
a result, the true concentration of the challenge aerosol is always
greater than that reported by a counter exhibiting coincidence
counting.
Filter integrity testing requires aerosol challenge concentrations
from two million (2 x106) to thirty million (3x107)
Particles per cubic foot. This is 20 to 3,000 times the upper limit
of the aerosol particle counter with a 1.0 cfm sample rate. The
challenge concentration must be known to determine the maximum scan
speed and to quantify the size of a defect. Therefore, it is
necessary to have a simple reliable means to accurately dilute the
aerosol to a concentration that can be measured accurately with the
particle counter.
The dilutor mixes a known quantity of clean air with the aerosol
sample. By knowing this ratio of clean air, a “dilution factor” is
calculated. The actual particle counter display is multiplied by
this factor to determine the actual aerosol concentration.
Dilution devices with factors of 500:1 are typically used to allow
the particle counter to accurately measure concentrations up to 50
million (5x107) Particles per cubic foot. (100,000 x 500
= 50,000,000).
Evolution of the Dilutor
Biocon, Inc. of Raleigh, NC began using simple dilutors in the
late 1980’s. Revisions of the early dilutors lead to the basis of
the current capillary tube technology. The capillary is simply
placed in the sample line between the particle counter and the
aerosol to be measured. ULPA filtered air is used as a carrier for
the particles passing through the capillary. These units have proven
to be very durable and rugged for field use. The dilutors do not
require compressed air or electrical power.
Principle of Operation
The volumetric flow through a capillary tube is a function of
the pressure differential across the tube. Thus any changes in
pressure will result in a change in the aerosol sample volume
passing through the capillary. The plenum pressure has a direct
effect on the capillary pressure and thus
aerosol flow and thus the
dilution factor. The pressure across the capillary is measured via a
Dwyer Magnehelic gauge. The resulting dilution factor for the
corresponding capillary pressure for each specific application is
referenced on a dilution factor chart.
Particle Counter Airflow
It is not necessary for the particle counter to sample exactly 1.0
cfm of air through the dilutor. The counter is only counting
particles that have passed through the capillary or about 0.002 cfm.
The remainder of the sample air is clean filtered air and has no
effect on determining the final concentration. Thus, the particle
sample flow rate can be adjusted to obtain a wide range of pressure
across the capillary and thus a variable dilution factor range.
However for maximum particle counter accuracy, you should adjust the
flow on the particle counter to 1.0 cfm with the dilutor attached to
then sample tubing. The counter was calibrated at this flow. If
adjusted for the resistance of the dilutor, one must reset
the counter to 1.0 cfm sample flow rate once the dilutor is removed
from the inlet sample line of the counter.
Diffusion Loss
It should be noted that particles in the size range of 0.1 um to 2
um are easily sampled with virtually no sample line losses. Smaller
particles will be lost to diffusion and larger particles will be
lost to sedimentation in the sample tubing. It is always best to
keep the inlet sample line to the dilutor (1/4” OD tube) to the same
length it was at the time of calibration of the dilutor. The tubing
should be as short as possible with a small internal diameter to
minimize losses. Large diameter and / or longer inlet tubes would
result in significant particle loss.
Very little particle losses occur in the 0.1 um to 2 um particles
once the sample is diluted with clean air. The 3/8” OD sample tube
from the dilutor to the particle counter can be up to 30 meters
long, provided it is made of a conductive polymer such as Tygothane.
Density Correction
As with any laminar flow device, airflow is affected by the density
and viscosity of the air. The dilutors are calibrated to sccm flow
(29.92 “ Hg and 70 degrees F). To correct the dilution factor for
your local conditions, use the following formula:

As a general rule, there is an estimated 3% correction for every
1,000 ft above sea level, and a 1% correction for every 5.3 degrees
F from 70 degrees.
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