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8/22/2019 Conductivity Sensor Calibrations to Meet Industry Requirement Braga 2
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Conductivity Sensor Calibrations to Meet Water
Industry Requirements
Victor M. Braga
Technical Service/Training Manager
Mettler-Toledo Thornton Inc.
36 Middlesex Turnpike
Bedford, Massachusetts 01730Phone (781) 301-8600
Phone (800) 642-4418
FAX (781) 271-0675
Web: www.mt.com/thornton
Abstract
As water purification technologies improve and the need for reliable, repeatable, and
accurate conductivity measurements grows, instrument manufacturers are constantly
challenged by water system manufacturers and end-users to continuously improve
measurement accuracies and to provide dependable, accurate readings. The challenge to
instrument manufacturers is not only to press forward with new more accurate
technologies, but to also reexamine existing processes and identify new and reliable
methods of improving them. By improving existing processes, instrument manufacturers
can achieve higher levels of accuracy with existing technologies.
One area that has recently been reevaluated is the calibration process, particularly the
conductivity sensors calibration. It is well documented that a significant percentage of
the error associated with a conductivity-measurement-system is attributed to the
conductivity sensor1. It is therefore crucial that, to produce accurate conductivity
measurements, the conductivity sensor undergo a well-defined calibration process that
enhances or improves accuracy.
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Introduction
In response to the demand for better and more accurate conductivity measurements,
instrument manufacturers have responded by not only evaluating new and improved
technologies, but by also reevaluating existing calibration processes and examining waysto improve or minimize errors.
One area that has recently experienced such a reexamination is the calibration process of
the conductivity sensor. By reevaluating this process, instrument manufacturers have
devised new and innovated methods to calibrated the sensor and achieve higher levels of
accuracy without significant changes in technology. Each phase of the sensors
calibration process has been reevaluated and analyzed to improve overall accuracy.
The conductivity sensors calibration process produces two calibration factors, the
conductivity multiplier (also know as the cell constant) and the temperature multiplier.
These factors are determined by placing the sensor in known conductivity samples at a
controlled and known temperature. This paper will examine ways of conducting and
computing these factors to minimize overall system error.
National Standards and Traceability
In the United States, we have two national standards to which most conductivity and
temperature calibrations are traceable, the American Society for Testing and Materials
(ASTM) and the National Institution of Standards and Technology (NIST).
The National Institute of Standards and Technology is an agency of the U.S. Department
of Commerces Technology Administration. It was established in 1901 to strengthen the
U.S. economy and improve the quality of life by working with industry to develop and
apply technology, measurements, and standards. It operates primarily in two locations;
Gaithersburg, MD and Boulder, CO. NIST laboratories provide calibration services and
calibrations standards to industries.
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The American Society for Testing and Materials was organized in 1898; it is one of the
largest voluntary standards development organizations in the world. It is a not-for-profit
organization that provides a forum for the development and publication of voluntary
consensus standards. It publishes more than 10,000 standards each year in the 73 volumes
of theAnnual Book of ASTM Standards.ASTM does not provide calibration services. It
publishes standard calibration methods and procedures to which calibrations may be
performed.
These are standards that are used by laboratories and industries that could be responsible
for forensics, environmental, density, chemical and other analytical analysis.
Measuring Systems
A complete measuring system consists of three basic components: measuring instrument
(or analyzer), sensor or cell, and the cable linking the sensor and analyzer. Each of these
components contributes to overall system accuracy.
Analyzer Calibration
Todays analyzers are highly sophisticated technological measuring instruments. The
more advanced instruments have several measurement circuits which optimize overall
accuracy (see Figure 1). The analyzer is capable of evaluating the input signal from the
conductivity sensor and selecting the most accurate gain circuitry for optimal accuracy.
This automated analysis and selection process happens instantly and the operator is never
aware of its occurrence. It is therefore imperative that each circuit be fully calibrated each
time the analyzer is recalibrated.
In addition to measuring the conductivity of the solution, todays modern analyzers must
also accurately measure the solutions temperature. This measurement is generally
performed by yet another circuit and must also be fully calibrated during the analyzers
calibration.
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It could take an operator several hours to perform a multiple point calibration on all the
measuring circuits. Some modern analyzers measure several parameters and require up to
72 calibration points. Fortunately, analyzer manufacturers have developed automated
calibration systems that can perform a full calibration in minutes.
Sensor Calibration
Conductivity is measured by placing two electrodes of known area (a) in a solution at a
fixed distance apart ( ). The ability of solution to conduct (conductivity) is measured by
applying an alternating current (AC) to the electrodes and measuring how difficult
(resistance) it is for the electrons to flow from one electrode to the other (current flow).
The closer the electrodes are to each other, and the more surface area they have, the
easier it is for current flow. Therefore, a fixed area of 1 square centimeter and a distance
of 1 centimeter were established to standardize conductivity measurements worldwide
(see figure 2). This makes conductivity measurements a volumetric measurement of 1
cubic centimeter and defines the cell constant as:
1
2
=
= cm
cm
cm
aK
It not imperative that the electrodes be exactly 1cm apart or have exactly 1 square cm of
surface area as long as the exact ratio is known. As a matter of fact, instrument
manufacturers routinely alter these dimensions to facilitate current flow from one
electrode to the other. Cell constants of 0.1 cm-1
and even 0.01 cm-1
are frequently used
G1
G2
ConductivityCell
Figure 1
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to measure ultrapure water (UPW) because they produce lower resistance to current flow
in very high resistivity water.
Figure 2
The electrode design illustrated in Figure 2 is impractical for general use due to
mechanical instability; any small change in distance would compromise the cell constant.
The concentric design (see Figure 3), which is far more robust, was developed to meet
industry needs.
Figure 3
The calibration process for a conductivity sensor not only computes cell constant, but
also must calibrate the temperature sensor located inside the conductivity sensor. Most
modern sensors use 1000 ohm platinum (Pt1000) resistance temperature devices (RTD)
to accurately measure the temperature.
Standard Calibrations
Four parameters must be fully calibrated to produce a calibrated system. They are:
1. The analyzers resistance circuit2. The analyzers temperature circuit
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3. The sensors cell constant4. The sensors RTD
Standard calibrations consist of calibrating the analyzer and conductivity sensor
individually. The analyzer and sensor will each have its own tolerance and accuracy
limits, for both resistance and temperature.
The analyzer resistance and temperature circuits are calibrated by placing precise
resistance values on the analyzers inputs and adjusting the analyzers gain circuitry until
the input value equals the displayed value. This can be performed with resistors traceable
to national standards (NIST) or with automated fixtures whose internal resistors are also
traceable to national standards.
Since it would be very difficult and impractical to physically measure the area and
distance of a concentric sensors electrodes, the sensor is calibrated by placing it in a
known conductivity solution, traceable to national standards (ASTM) and computing the
cell constant. However, low level conductivity standards for UPW applications are not
commercially available, nor can they be easily produced. Thus, the sensor is calibrated in
a sealed, circulating ultrapure water loop against a standard sensor whose cell constant
has been computed by placing it in ASTM D1125 solution D and in ultrapure water at
various temperatures1. The water loop circulates until the water quality reaches 18.18
M-cm (0.055S/cm) and the temperature is stabilized at 25C. At this point, the
unknown sensors cell constant and temperature factors are computed.
Calibration at Elevated Temperatures for Ultrapure Water
Applications
The need for accurate temperature measurements have been well documented2. Accurate
temperature compensated resistivity measurements depend not only on the measuring
systems ability to read the raw uncompensated resistivity but also on the sensors ability
to deliver an accurate temperature measurement. Relatively small temperature errors at
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or near ambient temperature can greatly impacted compensated resistivity measurements
at elevated temperatures. Figure 4 illustrates how a small temperature error of just -0.2C
can have dramatic effects at elevated temperatures.
Many factors can impact the sensors ability to measure an accurate temperate, such as
location of the RTD, the ability of the sensors material to conduct heat and temperature
gradients. Temperature gradients occur when a portion of the sensor is at ambient
temperature (outside the pipe) and another part of it is at an elevated temperature (inside
the pipe). As the difference between the internal and external temperature increases, the
temperature errors also increases and the greater the impact on compensated readings.
To minimize the impact of temperature gradients, sensors can be calibrated at elevated
temperatures. With knowledge of the end-user applications, especially temperature
requirements, improved accuracy can be achieved by calibrating under similar conditions.
This can significantly reduce the temperature error and optimize overall accuracy.
17.4
17.5
17.6
17.7
17.8
17.9
18.0
18.1
18.2
18.3
18.4
0 10 20 30 40 50 60 70 80 90 100
Temperature (C)
CompensatedResistivity(M-cm)
No temperature or resistivity error
-0.2C temperature error
Figure 4
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Calibration to Meet and Exceed USP Requirements
Water quality standards for pharmaceutical and biotech industries in the United States, or
for any manufacturer who wishes to sell pharmaceuticals in the United States, are set by
the United States Pharmacopeia (USP) and enforced by the Food and DrugAdministration (FDA). These standards require that Water for Injection (WFI) and
Purified Water (PW) meet certain conductivity limits before it can be used to
manufacture product. The water quality limits range from 0.6S/cm at 0.0C to 3.1S/cm
at 100C, as illustrated in Table 1.
Stage 1 USP Conductivity Limits
as a Function of Temperature
Temperature
(C)
Conductivity
Limit (S/cm)
Temperature
(C)
Conductivity
Limit (S/cm)
0 0.6 50 1.9
5 0.8 55 2.1
10 0.9 60 2.2
15 1.0 65 2.4
20 1.1 70 2.5
25 1.3 75 2.7
30 1.4 80 2.7
35 1.5 90 2.7
40 1.7 95 2.9
45 1.8 100 3.1
Table 1
Standard sensor calibrations compute the cell constant at a single conductivity level.
Although this is adequate, and meets USP requirements, many pharmaceutical and
biotech companys Standard Operating Procedures (SOP) require that the sensor be
verified at a different conductivity level and demand before calibration or as foundreadings be provide to assure that product produced with the sensor met all the
requirements.
To meet the water system manufacturers and end-usersneeds, instrument manufacturers
are providing calibration options that calibrate or compute the cell constant in ultrapure
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water (0.0550 S/cm) and verify it in ASTM D1125 Solution D (146.93 S/cm), as
illustrated in figure 5. By calibrating at a point below the requirement and verifying at a
point above the requirement, the user is assured of accurate and linear performance
throughout the dynamic range. Additionally, as found readings with the sensors
previous or original cell constant are provide for historical data and to assure that all
product produced with the sensor meets USP requirements.
Figure 5
System Calibration
As the need for more accurate and precise conductivity measurements increases,
instrument and sensor manufacturers have looked for new innovative ways to reduce the
overall system accuracy. One method of reducing overall system accuracy is to calibrate
the entire measuring system (analyzer and sensor) as a single unit.
As discussed earlier, a measuring system consists of four basic measurements:
1. The analyzers resistance circuit2. The analyzers temperature circuit3. The sensors cell constant4. The sensors RTD
Table 2 shows typical inaccuracies associated with each measurement. If all the
inaccuracies are added in a negative or positive direction, errors greater than 3% could be
expected. However, it is highly unlikely that all errors add in the same direction. A more
0.011.0100.01,000.0
S/cm S/cm10.0 0.1
25C
UPW
Solution DUSP waters
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typical analytical method is to take the square root of the sum of all errors. Using this
method, a typical system accuracy of about 2% is more reasonable. Still, more precise
accuracies are desirable.
Instrument manufacturers have improved system accuracy by first calibrating the
analyzers resistance and temperature circuits with known traceable standards. Then, the
sensor is placed in known and traceable conductivity standards at a known and fixed
temperature. Using the previously calibrated analyzer, the sensors cell and temperature
constant are computed. By computing the sensors constants with its own analyzer, the
only unknown inaccuracy is the conductivity solution. Thus, only the sensors
inaccuracies, and the conductivity standard solution, contribute to the overall system
accuracy. In most cases, even the cable which connects the sensor to analyzer is used
during the calibration process to further reduce inaccuracies.
Using this method, system inaccuracy can be reduced to about 1% over the dynamic
range of sensor and analyzer, and to less than 0.5% at the calibration point, usually
ultrapure water.
TYPICAL MEASURING SYSTEM ERRORSAnalyzers Resistivity Error 0.5%
Analyzers Temperature Error 1.0%
Sensors Cell Constant 1.0%
Sensors RTD 0.8%
Worst Case Error 3.3%
Square root of the sum of the squares 1.7%
Table 2
Conclusion
The need for more accurate conductivity measurements is well documented. By using
existing technologies and unique innovative calibration methods, the technology offered
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in todays instrumentation provides more precise and accurate conductivity
measurements.
Biography
Mettler Toledo Thornton Inc. has been a leading innovator and manufacturer of sensors
and instrumentation to monitor water purity and other fluid-based parameters since 1964,
specializing in Ultrapure Water for the semiconductor, pharmaceutical, and power
generation industries. Thornton instrumentation includes measurements for Resistivity,
Conductivity, TOC, Temperature, % Acid/Base, pH, ORP, Flow, Pressure, Level and
more. Thornton is a leader and technological innovator in the design and development of
multi-parameter instrumentation, accurate temperature compensation algorithms, accurate
UPW and hot UPW resistivity measurements, patented Smart Sensor calibration
technology, rapid TOC measurements for UPW and reclaim/recycle, high resistivity
applications such as ethylene glycol coolant and isopropyl alcohol cleaning, and high
conductivity applications such as regenerant acid/caustic and wastewater.
References
1. A.C. Bevilacqua, "Ultrapure Water The Standard for Resistivity Measurements ofUltrapure Water, 1998 Semiconductor Pure Water and Chemicals Conference,
March 2-5, 1998.
2. K.R. Morash, R.D. Thornton, C.H. Saunders, A.C. Bevilacqua, and T.S. Light,"Measurement of the Resistivity of High-Purity Water at Elevated Temperatures",
Ultrapure Water, 11(9), pp. 18-26, December, 1994.