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The Precision, Accuracy, and Reproducibility of IRGASTM Systems
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PDF Version

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Problem Statement
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What is the precision, accuracy, and reproducibility of an FTIR
instrument? A seemingly relatively easy question with a not so relatively easy answer.
Unfortunately, there is no straight-forward answer to this question, and the
answers that there are can get complicated and confusing. Hopefully this
application note will give some insight into signal/noise ratio, standard
error, precision, accuracy, and reproducibility and will explain why there is
no straight-forward, definitive answer to this question.
The data and information presented are based on an IRGAS-EPI/Hx
system* and a KIN-TEK moisture generator.
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Explanation
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Before being able to understand the precision, accuracy, and
reproducibility of a FTIR instrument, one must first have a grasp on how these
terms are used. The following are definitions of some of the important terms
that will be used in this application note:
- Signal/noise (s/n) ratio - difference between the signal
strength of a system compared to the amplitude of the systems undesirable background
noise
- Standard Error (s.e.) - measure of the sampling variability,
s.e. = standard deviation
- Precision - measurement of how consistent repeated measures are
to one another. Precision = s.e./concentration
- Accuracy - amount by which a measured value adheres to a
standard or true value
- Reproducibility - the variation arising using the same measurement
process among different instruments and operators
Keeping these terms in mind will help to better understand how
these concepts are all interrelated. Precision can not be discussed without discussing
s/n ratios, s.e., and concentration. The reason for this is a result of the
relationship each concept has with one another. Precision is a ratio between
s.e. and concentration, and s.e. is a function of the s/n ratio and the
absorption coefficient of individual species. With this being said, let’s start
with a single beam spectrum.

Figure 1: Single beam background spectra
As can be seen in figure 1, the single beam spectra somewhat
resembles a bell curve; this is the response of the detector throughout the IR spectrum.
In a system the noise level will remain relatively constant; however, the s/n
ratio will not. Therefore, the closer to the center of the bell curve the more
the s/n increases. As the s/n level increases, the s.e. decreases; so when the
s/n is at it’s maximum at the center of the curve the s.e. is at it’s minimum.
The s.e. will also increase the higher the concentration of a
species. This is because the absorption peak grows and as it grows there is
less available light at that wavelength for the system to see. With less light
the energy level decreases and so does the s/n ratio.
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Figure
2: Data calculated and used to create the precision graph (figure 3) below.

Figure
3: IRGAS systems precision as responding to moisture generator set points
Using figure 2, let’s discuss a little more the relationshipamong s.e. and concentration. From the table in figure 2, it can be deduced
that the data will plot as an exponential decay graph, and in fact it does as
is seen in figure 3; however this may not always be the case. In general it can
be said that the s.e. grows as the concentration increases, but it doesn’t grow
as fast as the concentration. So generally speaking the precision of the
instrument increases as the concentration increases. It can not be emphasized enough
that these statements are generalizations and truly speaking the precision of
an instrument changes along a concentration range based on a value of s.e. at
each point of a concentration range. Now that precision has been explained, accuracy
can be addressed. Accuracy is basically precision that correctly reads a true
value over repeated measurements. Therefore, without precision there would be
no accuracy. With that said, accuracy brings a new level of complexity to precision.
The accuracy of a system does not just depend on the particular
system, but it also depends on any auxiliary equipment being used with said
system. For example, the data presented in this application note is based on an
IRGAS-EPI/Hx, but it is also based on a KIN-TEK moisture generator. So the precision
and accuracy of the system can only be as good as the lowest precision and
accuracy, whether that be from the IRGAS system or the moisture generator.
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Figure 4: Concentration Step Ladder showing the IRGAS systems Accuracy
The expected accuracy of the KIN-TEK moisture generator is
approximately +/- 3%. To test the accuracy of the IRGAS-EPI/Hx system, the
KIN-TEK moisture generator was set at moisture concentrations (ppb) of 1000,
750, 500, 250, 125, 100, 75, 50, and 27. Figure 4 depicts the IRGAS’s system
ability to accurately read the moisture generator’s set points. Please note
that like precision, accuracy is case dependent and there is no one definitive
accuracy level that can be applied to every instrument.
Thus far, every concept that has been explained has focused on
one instrument, but what about the reproducibility from one instrument to
another? The reproducibility from one system to another depends on the quality
of the system components. In the case of an IRGAS system, it will depend on the
FTIR spectrometer used and the integrated gas cell. The IRGAS systems use an
ABB FTIR spectrometer meant for production environments and a CIC Photonics
stainless steel gas cell.
According to an ABB specification sheet:
- -The
wavenumber reproducibility is 0.1 cm at -1
1918 cm
- 100% line repeatability is within 0.1% over the -1
4000 to
550 cm range for MIR models.
- 100% line long term stability does not exceed 2% deviation over 16 hrs. over the 4000 to 550 -1
cm range
in the MIR models
These specifications will not only ensure that the collected
spectra will have minimal variations from spectral record to spectral record,
but from system to system as well. This, in addition to CIC Photonics gas cell,
which have a minimum throughput acceptance of 36%-48% depending on pathlength, creates
a quality system with high reproducibility.
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Copyright (c) 1994 to 2008 CIC Photonics, Inc. All rights reserved.
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