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In-Situ Calibration 
Methods & Pitfalls of Thermal Mass Flow 
Meter Sensor Field Validation 
By Matthew J. Olin, President & CEO, Sierra Instruments, Inc. 
A S I E R R A W H I T E P A P E R 
www.sierrainstruments.com 
N O R T H A M E R I C A 
5 Harris Court, Building L / Monterey, CA 93940 / USA 
800.866.0200 / 831.373.0200 / fx 831.373.4402 
E U R O P E 
Bijlmansweid 2 / 1934 RE Egmond aan den hoef / The Netherlands 
+31 72 5071400 / fx +31 72 5071401 
A S I A - P A C I F I C 
Second Floor Building 5 / Senpu Industrial Park 
25 Hangdu Road Hangtou Town / Pu Dong New District 
Shanghai, P.R. China Post Code 201316 
+8621 5879 8521 / fx +8621 5879 8586
INTRODUCTION 
Mid-to-large size facilities and campuses inevitably have 
hundreds of  ow instruments to monitor, maintain, and repair. 
For a reliability engineer, ensuring that all instrumentation 
meets ISO 9000 or similar standards is a time-consuming 
responsibility. These standards mandate that precision 
instrumentation needs to be checked (validated) or 
recalibrated as often as once a year. Sensor elements can 
become dirty, plugged, or drift over time. The resistance and 
capacitance of electronic components also degrades, leading 
to changes in sensitivity or drift. 
Once an instrument drifts out of speci cation, it must be 
recalibrated to maintain its original accuracy. Thermal mass 
 ow meters are not immune to these factors. As a precision 
instrument designed to measure the molecular mass  ow 
rate of gases in ducts and pipes, these types of instruments 
can require cleaning, veri cation, and recalibration. Many 
 ow meter manufacturers falsely claim that in-situ (or in-place) 
calibration is an easy and inexpensive method for both 
verifying the meter’s original factory-calibrated accuracy and 
verifying the meter is in calibration. However, when evaluating 
thermal mass  ow meters for in-situ calibration or validation 
capability, be aware that sensor drift will create false positives 
that reduce the reliability of the validation. 
2
This white paper not only explores the role of stable no-drift 
sensor design, but examines  ve methods of  eld calibration 
validation to help end users choose the most accurate, stable, 
and cost-effective in-situ calibration solution. 
Background: Wet Sensor Design 
The stability of all thermal mass  ow meter sensors starts with mechanical design. The basic physics of 
thermal mass  ow meters is attributed to Louie V. King, who published his famous King’s Law in 1914, 
mathematically describing heat transfer between a heated wire and the  uid  ow it is immersed into. King 
called his original instrument a “hot-wire anemometer,” which measured the mass velocity at a point in 
the  ow. The usage of hot wire anemometers grew, in particular, in research environments. This technology 
was not widely used in industry because of the fragile nature of the hot wires. 
To solve this fragility problem, Sierra Instruments pioneered the development of an industrial-strength 
sensor in the ‘80s that could be used in a broad spectrum of industrial process control applications. 
The solution was to coil the platinum wire around a ceramic mandrel and mold the wire in place with a 
glass coating. This assembly was then placed inside of a thermo-well. However, the gap or boundary layer 
between the thermo-well and the platinum-wound mandrel needed to be  lled with something other than 
air to assure heat transfer from the sensor to the  ow. This was the key to assuring an accurate and stable 
thermal mass  ow meter. The air gap was  lled with a potting compound—a conductive epoxy called 
thermal grease or cement. This type of sensor is known today as a wet sensor and is used by virtually all 
manufacturers of thermal meters (See Figure 1). 
The Problem: Wet Sensor Drift 
This wet sensor design proved workable, but it had an inherent weakness. The sensor would drift over time 
affecting the accuracy of  ow measurement readings. As a function of its very principal of operation, the 
sensor is heated and cooled over time, expanding and contracting the cement inside the sensor, making it 
crack, settle, and shift from its original state. This phenomenon is analogous to freshly poured cement on a 
sidewalk. Eventually, the cement hardens and often cracks, shifts, and settles as it is repeatedly heated by 
the sun and cooled at night. 
3
Since thermal sensors are precisely calibrated to determine the heat transfer versus  ow characteristics, 
any change in the physical makeup of the sensor layers will invalidate this calibration, resulting in drift or 
outright failure. Excessive drift means users must send the meter back to the factory for recalibration. 
Dry Sensor: No Drift Thermal Dispersion Sensor 
The best way to minimize drift in a thermal sensor is to remove the root cause—the epoxies, cements, 
and thermal greases that make up the wet sensor. In March of 1999, Sierra Instruments introduced a 
new patented sensor design. Through a proprietary, highly-controlled manufacturing process, the metal 
thermowell sheath is tightly formed on the mandrel and platinum-wire assembly. The sensor is designed to 
form such close contact that little or no air gap exists and no organic  ller cements are needed 
(See Figure 2). 
4 
Figure 1. A Typical Wet Thermal Dispersion Sensor 
Sensor Wall 
Organic Filler 
Sensor Windings
5 
Patented Swage 
Sensor Wall 
Design 
Hard Glass 
Coating 
NO Organic Filler / 
NO Air Gaps 
Sensor Windings 
Figure 2. Patented Dry Thermal Dispersion Sensor 
Velocity Sensor 
(cutaway) 
Temperature Sensor 
This innovative new cement-free sensor, known as a dry sensor, was patented by Sierra as DrySense™ 
Sensor Technology. All materials used to make the sensor are selected to assure that the coef cients 
of thermal expansion are approximately the same. As a result, they expand and contract at the same 
rate, limiting the stress and cracking. Sierra determined that using a dry sensor was the only way a 
manufacturer could claim stability over the sensor’s lifetime. 
In-Situ Calibration Veri cation 
Despite wet sensor design weaknesses, to this day, all manufacturers of thermal mass  ow meters, except 
for Sierra, use the wet sensor design because they are easy and economical to build. In addition, all 
thermal meter manufacturers have generally the same method of using in-situ validation. 
As expected, in-situ calibration veri cation of thermal  ow meters is a highly marketed feature that claims 
to validate the sensor’s accuracy on location. In-situ veri cation does not replace calibration. If substantial 
drift is found, the  ow meter must be sent back to the factory for recalibration.
The following section details  ve principles of thermal mass  ow meter sensor validation to assess which 
in-situ veri cation method will result in the most accurate results, thereby saving time and lowering costs. 
These  ve approaches are: Resistance, Zero-Flow, K-factor, Full-Flow, and Flow-Audit. 
Validation Using Resistance 
The simplest method measures the resistance across the velocity sensor. Since the velocity sensor is 
normally a platinum resistance temperature detector (PRTD), the measured resistance is directly related 
to the temperature of the sensor. This temperature should be equal to the space surrounding the velocity 
sensor once everything has come to equilibrium (See Figure 3). 
6 
Velocity Sensor 
Platinum Windings 
Figure 3. Validation Using Resistance 
Resistance of 
Windings 
(20  typical) 
Multimeter 
This method only measures the resistance of the platinum wire that is wrapped around the platinum 
mandrel. As the dry versus wet sensor discussion illustrates, there is much more to a thermal dispersion 
sensor. Resistance measurement makes this a good troubleshooting tool in determining whether the wire 
has an open or short circuit and thus the sensor has totally failed. 
Power must be removed from the velocity sensor, and it must be allowed to come into thermal equilibrium 
with its surroundings. Further, these surroundings must be at a constant temperature. In some cases, the 
meter can take as long as 30 minutes to reach thermal equilibrium and, for that period of time, it is not 
capable of measuring  ow. If the temperature of the process  uid is  uctuating, this check cannot be done 
in-situ. 
However, this method does nothing to measure drift since the test doesn’t measure factors related to heat 
transfer from the wire through the epoxies and sheath into the  owing  uid. Therefore, this method can 
only be con dently used with dry sensor design which doesn’t drift.
Validation Using Zero Flow 
Most manufacturers have realized the limitations of validation using resistance and have various methods 
of checking the sensor’s electrical output (either power or raw sensor output voltage) at a zero- ow 
condition (See Figure 4). Zero  ow is the only truly reproducible point between the factory calibration and 
the site where the meter is being used. 
To understand how this process works, it is necessary to review the factors that in uence a thermal 
dispersion  ow meter’s calibration: 
n Gas being measured 
n Temperature and pressure of the gas 
n The pipe the gas is  owing inside and the maximum  ow rate the meter is expected to measure 
If a meter is in the same gas at the same temperature and pressure as factory calibration and the  ow is 
zero, it should read the same sensor output voltage or dissipate the same power as it did at the factory. If 
it does not, it is because the sensor, or the electronics that drive the sensor, have drifted over time. 
There are a variety of reasons why this measurement can be problematic: 
n As stated, this measurement is only valid at zero  ow, meaning the  ow in the pipe must be either 
shut off or the  ow meter partially removed from the pipe with a hot-tap. 
n Even if the meter is at zero  ow, it still must be in the same gas at the same temperature and 
pressure as factory calibration. 
7 
Velocity Heater 
Coil 
Power to 
Heater Coil 
(500mW typical) 
Multimeter 
Figure 4. Validation Using Zero Flow Calibration 
For these reasons, many manufacturers provide data for checking zero at another set of more reproducible 
conditions: zero  ow at atmospheric pressure and temperature. This requires the meter to be completely 
removed from the process and allowed to come to equilibrium at ambient conditions. At best, this 
stretches the de nition of in-situ veri cation, as it is not “in place.” 
The key drawback of validation using zero  ow is that it is only valid at a single  ow point. While this is a 
good indicator of the type of offset that can be caused by drift, it does nothing to validate the accuracy of 
the  ow meter through its calibrated range.
Field Adjustment Using K-Factors 
As an interim step, many manufactures enable the application of a global K-factor that works as a 
multiplier to the observed  ow value. This is simply a linear offset most often employed to make the meter 
reading agree with another device. The problem with K-factors is that the inherent response curve of a 
thermal sensor to  ow is non-linear and is best represented by a complex polynomial function, typically at 
least to the  fth order (See Figure 5). 
8 
60 
50 
40 
30 
20 
10 
0 
0 0.5 1 1.5 2 2.5 3 
Electrical power, Watts (W) 
Mass velocity, Standard m/s (Vs ) 
Figure 5. Sensor Output Versus Increasing Flow Rate 
In other cases, the manufacturer may allow several points on the calibration curve to be adjusted. This is 
typically done for large ducts and pipes as part of a  ow transit. This is sometimes erroneously called an 
in-situ calibration. 
In this procedure, the  ow pro le inside a large duct or pipe is characterized by measuring the velocities at 
various points, generally along horizontal and vertical lines. Since an thermal  ow meter is a point velocity 
device, it can only measure the velocity at a single point in the total  ow and is affected by  ow pro le 
disturbances. A  ow traverse can determine the best placement of the  ow meter, and may suggest that 
multiple points are needed. Some manufacturers offer multipoint thermal  ow meter averaging systems for 
this purpose (See Figure 6). A  ow traverse is not an in-situ calibration. It simply re nes the placement of 
the meter, or determines a gross correction K-factor to bring the existing calibration in line with observed 
results. 
Figure 6. Multipoint Flow Meter System
Validation Using Full-Flow 
One complex and expensive technique that validates beyond a zero  ow condition checks the full- ow 
range by generating a series of known  ow rates, from zero to full scale (See Figure 7). The system uses a 
small sonic nozzle opening that directs a known  ow past the velocity sensor. The diameter of the nozzle is 
 xed, and by applying a known differential pressure across the nozzle, the  ow through the nozzle can be 
calculated. 
Pressure 
Regulator 
Test Valve 
Internal Flow 
Tube 
Calibrated 
Nozzle 
Known Flow 
Rate 
As with the other techniques discussed, this method has its drawbacks: 
n It depends on the nozzle not becoming plugged or dirty (and thus changing the size of the nozzle 
from when it was calibrated) and requires precision pressure gages, which themselves need periodic 
recalibration. 
n The meter must be removed from the process (although not necessarily the pipe), so a hot tap 
system is required. 
n This is a rather complex and expensive technique, requiring a source of pressurized air or nitrogen, 
a variable pressure regulator, tubing, and the nozzle. Such a system cannot be back- tted, and the 
nozzle is a permanent  xture of the probe assembly. 
9 
Figure 7. Validation Using Sonic Nozzles 
Temperature 
Sensor 
Velocity Sensor
Validation Using Actual Flow-Audit Method 
The  ow-audit method is perhaps the very best in-situ calibration veri cation. This method uses a 
high-accuracy  ow standard to prove the accuracy of the  ow device under test (DUT). A  ow-audit is 
performed with a similarly calibrated meter that is installed into the pipe via hot-tap near the DUT, or 
even at the same measurement point if the meter under test can be removed. The key words above are 
“similarly calibrated;” a meter calibrated for natural gas cannot be used to check a meter on compressed 
air for instance. Likewise, the temperature and pressure as well as pipe size must be matched. 
The ideal meter for the  ow audit method has the application  exibility to work on different gases and 
pipe sizes and dynamically compensate for temperature and pressure differences. Many companies buy 
thermal insertion mass  ow meters as audit meters because of their ability to insert the sensor into the 
 ow via hot tap. This adds convenience and avoids costly process shutdowns. However, traditionally, a 
thermal meter needs to be purchased for each speci c application at the facility. For the majority of users, 
this is cost prohibitive. 
For gas  ow auditing, a solution now exists that allows a single thermal  ow meter to be used across 
multiple pipe sizes and gases. Released to market in 2011, Sierra’s QuadraTherm® 640i insertion thermal 
mass  ow meter has been rapidly adopted as a  ow-audit meter to check other thermal meters at a 
facility. Due to its high accuracy of 0.75% of reading, it is also commonly used to check many different gas 
mass and volumetric  ow technologies. 
Coupled with a hot-tap insertion point located near the DUT, the 640i is a “universal”  ow meter that 
can be recon gured in the  eld to match nearly any  ow measurement point in a facility. The 640i has 
Sierra’s patented no-drift dry sensor as discussed earlier in this whitepaper. The result is a stable reliable 
measurement. As seen in Figure 8, the user programs the instrument to the exact gas and pipe size of the 
device under test and inserts the 3/4” (19mm) sensor probe into the pipe near the DUT. Engineering units 
can even be programmed to match the DUT. 
The 640i  ow-audit meter will immediately start reading  ow. Compare this  ow to the DUT. If the two 
units read close to each other, the DUT can be signed off as validated and reading properly. 
10 
Figure 8. Audit-Meter with Hot-Tap 
Device Under 
Test 
Flow 
Flow Audit 
Meter 
Low Pressure 
Hot Tap
In-Situ Validation Isn’t Calibration 
For four of the calibration validation methods, if the meter does not pass the validation, it generally must 
be returned to the factory for recalibration. However, using the  ow–audit method does allow the end user 
to adjust a DUT using the K-factor method discussed earlier in the whitepaper to adjust the DUT to match 
the exact  ow reading of the audit meter. 
Precise thermal  ow meter calibration occurs under tightly controlled temperature and pressure conditions 
using the same gas and the same size pipe section or  ow body that the meter will be used in. 
As you can imagine, such a facility is a large and expensive asset and certainly not portable. Consequently, 
if you  nd your meter is out of calibration, it is highly recommended to send it back to the factory or 
accredited  ow calibration service center for recalibration. 
Validate, Don’t Calibrate 
How can you validate a sensor that will drift out of spec due to the very nature of its mechanical design? 
You can’t. All validation methods assume that there is no drift. As described earlier in this white paper, 
wet sensors are prone to drift and dry sensors do not drift. 
Dry no-drift sensors have a big advantage during in-situ calibration validation. The allmetal, epoxy-free 
mechanical design provides the con dence that the in-situ calibration validation is actually valid. Dry 
sensors are validated in the same way as a wet sensor, although in this case, it is not drift that is expected, 
but rather dirt or mechanical damage. For this reason, Sierra offers a lifetime warranty on its patented dry 
sensor and guarantees that there will be no drift. 
As a result, there is no need to buy expensive in-situ calibration instruments. Sierra offers a free in-situ 
calibration validation software package called ValidCal™ Diagnostics. Unlike other validation methods, the 
ValidCal™ Diagnostics program provides a complete check of all meter components including the velocity 
and temperature sensors, the sensor drive circuitry, the accuracy of the pressure transducer (if applicable), 
and all digital and analog outputs and alarm relays. This capability is included free with each meter and 
provides a printed calibration certi cate and diagnostics report. All of this can be accomplished without 
removing the meter from the process piping. This capability can be found in all Sierra thermal meters, 
including the latest high-accuracy QuadraTherm meter (See Figure 9, which is multivariable and has 0.5% 
of reading accuracy). 
When evaluating thermal mass  ow meters for in-situ calibration validation capability, be aware that 
sensor drift will create false positives that reduce the reliability of the validation resulting in reduced 
measurement quality. Assure that the instrument has a dry sensor and that the manufacturer backs up 
their sensor with a no-drift guarantee before you run an in-situ calibration validation procedure. 
11
Summary and Conclusion 
In-situ calibration validation is one of the great bene ts of thermal mass  ow technology. This whitepaper 
reviews  ve in-situ calibration validation approaches. These are: Resistance, Zero-Flow, K-factor, Full-Flow, 
and Flow-Audit. Each method has varying cost and complexity, but does offer the end user the advantage 
of proving some aspect of  ow meter performance in the  eld to ful ll quality requirements. 
When evaluating thermal mass  ow meters for in-situ calibration validation capability, beware that 
sensor drift will create false positives that reduce the reliability of the validation. The assumption by all 
manufacturers, including Sierra, is that their sensor does not drift. Only with sensor stability can users truly 
validate a sensor’s factory-calibrated accuracy in the  eld. Assure that your thermal mass  ow meter has a 
drift-free, dry sensor, which has no organics and cements that drift over time. 
Finally, it is highly recommended to use the  ow–audit method for the highest quality calibration 
validation. All forms of in-situ calibration validation discussed in this whitepaper give the end user 
information about the thermal meter’s operating performance, but only the  ow-audit method actually 
validates the calibration at actual  owing conditions. 
Acknowledgements 
I would like to thank Scott Rouse, Erica Giannini and Charlotte Chapman for their contributions to the 
white paper. 
12 
Figure 9. Sierra’s QuadraTherm® Mass Flow Meter Featuring DrySense™ Sensor Technology

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In-Situ Calibration: Methods & Pitfalls of Thermal Mass Flow Meter Sensor Field Validation

  • 1. In-Situ Calibration Methods & Pitfalls of Thermal Mass Flow Meter Sensor Field Validation By Matthew J. Olin, President & CEO, Sierra Instruments, Inc. A S I E R R A W H I T E P A P E R www.sierrainstruments.com N O R T H A M E R I C A 5 Harris Court, Building L / Monterey, CA 93940 / USA 800.866.0200 / 831.373.0200 / fx 831.373.4402 E U R O P E Bijlmansweid 2 / 1934 RE Egmond aan den hoef / The Netherlands +31 72 5071400 / fx +31 72 5071401 A S I A - P A C I F I C Second Floor Building 5 / Senpu Industrial Park 25 Hangdu Road Hangtou Town / Pu Dong New District Shanghai, P.R. China Post Code 201316 +8621 5879 8521 / fx +8621 5879 8586
  • 2. INTRODUCTION Mid-to-large size facilities and campuses inevitably have hundreds of ow instruments to monitor, maintain, and repair. For a reliability engineer, ensuring that all instrumentation meets ISO 9000 or similar standards is a time-consuming responsibility. These standards mandate that precision instrumentation needs to be checked (validated) or recalibrated as often as once a year. Sensor elements can become dirty, plugged, or drift over time. The resistance and capacitance of electronic components also degrades, leading to changes in sensitivity or drift. Once an instrument drifts out of speci cation, it must be recalibrated to maintain its original accuracy. Thermal mass ow meters are not immune to these factors. As a precision instrument designed to measure the molecular mass ow rate of gases in ducts and pipes, these types of instruments can require cleaning, veri cation, and recalibration. Many ow meter manufacturers falsely claim that in-situ (or in-place) calibration is an easy and inexpensive method for both verifying the meter’s original factory-calibrated accuracy and verifying the meter is in calibration. However, when evaluating thermal mass ow meters for in-situ calibration or validation capability, be aware that sensor drift will create false positives that reduce the reliability of the validation. 2
  • 3. This white paper not only explores the role of stable no-drift sensor design, but examines ve methods of eld calibration validation to help end users choose the most accurate, stable, and cost-effective in-situ calibration solution. Background: Wet Sensor Design The stability of all thermal mass ow meter sensors starts with mechanical design. The basic physics of thermal mass ow meters is attributed to Louie V. King, who published his famous King’s Law in 1914, mathematically describing heat transfer between a heated wire and the uid ow it is immersed into. King called his original instrument a “hot-wire anemometer,” which measured the mass velocity at a point in the ow. The usage of hot wire anemometers grew, in particular, in research environments. This technology was not widely used in industry because of the fragile nature of the hot wires. To solve this fragility problem, Sierra Instruments pioneered the development of an industrial-strength sensor in the ‘80s that could be used in a broad spectrum of industrial process control applications. The solution was to coil the platinum wire around a ceramic mandrel and mold the wire in place with a glass coating. This assembly was then placed inside of a thermo-well. However, the gap or boundary layer between the thermo-well and the platinum-wound mandrel needed to be lled with something other than air to assure heat transfer from the sensor to the ow. This was the key to assuring an accurate and stable thermal mass ow meter. The air gap was lled with a potting compound—a conductive epoxy called thermal grease or cement. This type of sensor is known today as a wet sensor and is used by virtually all manufacturers of thermal meters (See Figure 1). The Problem: Wet Sensor Drift This wet sensor design proved workable, but it had an inherent weakness. The sensor would drift over time affecting the accuracy of ow measurement readings. As a function of its very principal of operation, the sensor is heated and cooled over time, expanding and contracting the cement inside the sensor, making it crack, settle, and shift from its original state. This phenomenon is analogous to freshly poured cement on a sidewalk. Eventually, the cement hardens and often cracks, shifts, and settles as it is repeatedly heated by the sun and cooled at night. 3
  • 4. Since thermal sensors are precisely calibrated to determine the heat transfer versus ow characteristics, any change in the physical makeup of the sensor layers will invalidate this calibration, resulting in drift or outright failure. Excessive drift means users must send the meter back to the factory for recalibration. Dry Sensor: No Drift Thermal Dispersion Sensor The best way to minimize drift in a thermal sensor is to remove the root cause—the epoxies, cements, and thermal greases that make up the wet sensor. In March of 1999, Sierra Instruments introduced a new patented sensor design. Through a proprietary, highly-controlled manufacturing process, the metal thermowell sheath is tightly formed on the mandrel and platinum-wire assembly. The sensor is designed to form such close contact that little or no air gap exists and no organic ller cements are needed (See Figure 2). 4 Figure 1. A Typical Wet Thermal Dispersion Sensor Sensor Wall Organic Filler Sensor Windings
  • 5. 5 Patented Swage Sensor Wall Design Hard Glass Coating NO Organic Filler / NO Air Gaps Sensor Windings Figure 2. Patented Dry Thermal Dispersion Sensor Velocity Sensor (cutaway) Temperature Sensor This innovative new cement-free sensor, known as a dry sensor, was patented by Sierra as DrySense™ Sensor Technology. All materials used to make the sensor are selected to assure that the coef cients of thermal expansion are approximately the same. As a result, they expand and contract at the same rate, limiting the stress and cracking. Sierra determined that using a dry sensor was the only way a manufacturer could claim stability over the sensor’s lifetime. In-Situ Calibration Veri cation Despite wet sensor design weaknesses, to this day, all manufacturers of thermal mass ow meters, except for Sierra, use the wet sensor design because they are easy and economical to build. In addition, all thermal meter manufacturers have generally the same method of using in-situ validation. As expected, in-situ calibration veri cation of thermal ow meters is a highly marketed feature that claims to validate the sensor’s accuracy on location. In-situ veri cation does not replace calibration. If substantial drift is found, the ow meter must be sent back to the factory for recalibration.
  • 6. The following section details ve principles of thermal mass ow meter sensor validation to assess which in-situ veri cation method will result in the most accurate results, thereby saving time and lowering costs. These ve approaches are: Resistance, Zero-Flow, K-factor, Full-Flow, and Flow-Audit. Validation Using Resistance The simplest method measures the resistance across the velocity sensor. Since the velocity sensor is normally a platinum resistance temperature detector (PRTD), the measured resistance is directly related to the temperature of the sensor. This temperature should be equal to the space surrounding the velocity sensor once everything has come to equilibrium (See Figure 3). 6 Velocity Sensor Platinum Windings Figure 3. Validation Using Resistance Resistance of Windings (20 typical) Multimeter This method only measures the resistance of the platinum wire that is wrapped around the platinum mandrel. As the dry versus wet sensor discussion illustrates, there is much more to a thermal dispersion sensor. Resistance measurement makes this a good troubleshooting tool in determining whether the wire has an open or short circuit and thus the sensor has totally failed. Power must be removed from the velocity sensor, and it must be allowed to come into thermal equilibrium with its surroundings. Further, these surroundings must be at a constant temperature. In some cases, the meter can take as long as 30 minutes to reach thermal equilibrium and, for that period of time, it is not capable of measuring ow. If the temperature of the process uid is uctuating, this check cannot be done in-situ. However, this method does nothing to measure drift since the test doesn’t measure factors related to heat transfer from the wire through the epoxies and sheath into the owing uid. Therefore, this method can only be con dently used with dry sensor design which doesn’t drift.
  • 7. Validation Using Zero Flow Most manufacturers have realized the limitations of validation using resistance and have various methods of checking the sensor’s electrical output (either power or raw sensor output voltage) at a zero- ow condition (See Figure 4). Zero ow is the only truly reproducible point between the factory calibration and the site where the meter is being used. To understand how this process works, it is necessary to review the factors that in uence a thermal dispersion ow meter’s calibration: n Gas being measured n Temperature and pressure of the gas n The pipe the gas is owing inside and the maximum ow rate the meter is expected to measure If a meter is in the same gas at the same temperature and pressure as factory calibration and the ow is zero, it should read the same sensor output voltage or dissipate the same power as it did at the factory. If it does not, it is because the sensor, or the electronics that drive the sensor, have drifted over time. There are a variety of reasons why this measurement can be problematic: n As stated, this measurement is only valid at zero ow, meaning the ow in the pipe must be either shut off or the ow meter partially removed from the pipe with a hot-tap. n Even if the meter is at zero ow, it still must be in the same gas at the same temperature and pressure as factory calibration. 7 Velocity Heater Coil Power to Heater Coil (500mW typical) Multimeter Figure 4. Validation Using Zero Flow Calibration For these reasons, many manufacturers provide data for checking zero at another set of more reproducible conditions: zero ow at atmospheric pressure and temperature. This requires the meter to be completely removed from the process and allowed to come to equilibrium at ambient conditions. At best, this stretches the de nition of in-situ veri cation, as it is not “in place.” The key drawback of validation using zero ow is that it is only valid at a single ow point. While this is a good indicator of the type of offset that can be caused by drift, it does nothing to validate the accuracy of the ow meter through its calibrated range.
  • 8. Field Adjustment Using K-Factors As an interim step, many manufactures enable the application of a global K-factor that works as a multiplier to the observed ow value. This is simply a linear offset most often employed to make the meter reading agree with another device. The problem with K-factors is that the inherent response curve of a thermal sensor to ow is non-linear and is best represented by a complex polynomial function, typically at least to the fth order (See Figure 5). 8 60 50 40 30 20 10 0 0 0.5 1 1.5 2 2.5 3 Electrical power, Watts (W) Mass velocity, Standard m/s (Vs ) Figure 5. Sensor Output Versus Increasing Flow Rate In other cases, the manufacturer may allow several points on the calibration curve to be adjusted. This is typically done for large ducts and pipes as part of a ow transit. This is sometimes erroneously called an in-situ calibration. In this procedure, the ow pro le inside a large duct or pipe is characterized by measuring the velocities at various points, generally along horizontal and vertical lines. Since an thermal ow meter is a point velocity device, it can only measure the velocity at a single point in the total ow and is affected by ow pro le disturbances. A ow traverse can determine the best placement of the ow meter, and may suggest that multiple points are needed. Some manufacturers offer multipoint thermal ow meter averaging systems for this purpose (See Figure 6). A ow traverse is not an in-situ calibration. It simply re nes the placement of the meter, or determines a gross correction K-factor to bring the existing calibration in line with observed results. Figure 6. Multipoint Flow Meter System
  • 9. Validation Using Full-Flow One complex and expensive technique that validates beyond a zero ow condition checks the full- ow range by generating a series of known ow rates, from zero to full scale (See Figure 7). The system uses a small sonic nozzle opening that directs a known ow past the velocity sensor. The diameter of the nozzle is xed, and by applying a known differential pressure across the nozzle, the ow through the nozzle can be calculated. Pressure Regulator Test Valve Internal Flow Tube Calibrated Nozzle Known Flow Rate As with the other techniques discussed, this method has its drawbacks: n It depends on the nozzle not becoming plugged or dirty (and thus changing the size of the nozzle from when it was calibrated) and requires precision pressure gages, which themselves need periodic recalibration. n The meter must be removed from the process (although not necessarily the pipe), so a hot tap system is required. n This is a rather complex and expensive technique, requiring a source of pressurized air or nitrogen, a variable pressure regulator, tubing, and the nozzle. Such a system cannot be back- tted, and the nozzle is a permanent xture of the probe assembly. 9 Figure 7. Validation Using Sonic Nozzles Temperature Sensor Velocity Sensor
  • 10. Validation Using Actual Flow-Audit Method The ow-audit method is perhaps the very best in-situ calibration veri cation. This method uses a high-accuracy ow standard to prove the accuracy of the ow device under test (DUT). A ow-audit is performed with a similarly calibrated meter that is installed into the pipe via hot-tap near the DUT, or even at the same measurement point if the meter under test can be removed. The key words above are “similarly calibrated;” a meter calibrated for natural gas cannot be used to check a meter on compressed air for instance. Likewise, the temperature and pressure as well as pipe size must be matched. The ideal meter for the ow audit method has the application exibility to work on different gases and pipe sizes and dynamically compensate for temperature and pressure differences. Many companies buy thermal insertion mass ow meters as audit meters because of their ability to insert the sensor into the ow via hot tap. This adds convenience and avoids costly process shutdowns. However, traditionally, a thermal meter needs to be purchased for each speci c application at the facility. For the majority of users, this is cost prohibitive. For gas ow auditing, a solution now exists that allows a single thermal ow meter to be used across multiple pipe sizes and gases. Released to market in 2011, Sierra’s QuadraTherm® 640i insertion thermal mass ow meter has been rapidly adopted as a ow-audit meter to check other thermal meters at a facility. Due to its high accuracy of 0.75% of reading, it is also commonly used to check many different gas mass and volumetric ow technologies. Coupled with a hot-tap insertion point located near the DUT, the 640i is a “universal” ow meter that can be recon gured in the eld to match nearly any ow measurement point in a facility. The 640i has Sierra’s patented no-drift dry sensor as discussed earlier in this whitepaper. The result is a stable reliable measurement. As seen in Figure 8, the user programs the instrument to the exact gas and pipe size of the device under test and inserts the 3/4” (19mm) sensor probe into the pipe near the DUT. Engineering units can even be programmed to match the DUT. The 640i ow-audit meter will immediately start reading ow. Compare this ow to the DUT. If the two units read close to each other, the DUT can be signed off as validated and reading properly. 10 Figure 8. Audit-Meter with Hot-Tap Device Under Test Flow Flow Audit Meter Low Pressure Hot Tap
  • 11. In-Situ Validation Isn’t Calibration For four of the calibration validation methods, if the meter does not pass the validation, it generally must be returned to the factory for recalibration. However, using the ow–audit method does allow the end user to adjust a DUT using the K-factor method discussed earlier in the whitepaper to adjust the DUT to match the exact ow reading of the audit meter. Precise thermal ow meter calibration occurs under tightly controlled temperature and pressure conditions using the same gas and the same size pipe section or ow body that the meter will be used in. As you can imagine, such a facility is a large and expensive asset and certainly not portable. Consequently, if you nd your meter is out of calibration, it is highly recommended to send it back to the factory or accredited ow calibration service center for recalibration. Validate, Don’t Calibrate How can you validate a sensor that will drift out of spec due to the very nature of its mechanical design? You can’t. All validation methods assume that there is no drift. As described earlier in this white paper, wet sensors are prone to drift and dry sensors do not drift. Dry no-drift sensors have a big advantage during in-situ calibration validation. The allmetal, epoxy-free mechanical design provides the con dence that the in-situ calibration validation is actually valid. Dry sensors are validated in the same way as a wet sensor, although in this case, it is not drift that is expected, but rather dirt or mechanical damage. For this reason, Sierra offers a lifetime warranty on its patented dry sensor and guarantees that there will be no drift. As a result, there is no need to buy expensive in-situ calibration instruments. Sierra offers a free in-situ calibration validation software package called ValidCal™ Diagnostics. Unlike other validation methods, the ValidCal™ Diagnostics program provides a complete check of all meter components including the velocity and temperature sensors, the sensor drive circuitry, the accuracy of the pressure transducer (if applicable), and all digital and analog outputs and alarm relays. This capability is included free with each meter and provides a printed calibration certi cate and diagnostics report. All of this can be accomplished without removing the meter from the process piping. This capability can be found in all Sierra thermal meters, including the latest high-accuracy QuadraTherm meter (See Figure 9, which is multivariable and has 0.5% of reading accuracy). When evaluating thermal mass ow meters for in-situ calibration validation capability, be aware that sensor drift will create false positives that reduce the reliability of the validation resulting in reduced measurement quality. Assure that the instrument has a dry sensor and that the manufacturer backs up their sensor with a no-drift guarantee before you run an in-situ calibration validation procedure. 11
  • 12. Summary and Conclusion In-situ calibration validation is one of the great bene ts of thermal mass ow technology. This whitepaper reviews ve in-situ calibration validation approaches. These are: Resistance, Zero-Flow, K-factor, Full-Flow, and Flow-Audit. Each method has varying cost and complexity, but does offer the end user the advantage of proving some aspect of ow meter performance in the eld to ful ll quality requirements. When evaluating thermal mass ow meters for in-situ calibration validation capability, beware that sensor drift will create false positives that reduce the reliability of the validation. The assumption by all manufacturers, including Sierra, is that their sensor does not drift. Only with sensor stability can users truly validate a sensor’s factory-calibrated accuracy in the eld. Assure that your thermal mass ow meter has a drift-free, dry sensor, which has no organics and cements that drift over time. Finally, it is highly recommended to use the ow–audit method for the highest quality calibration validation. All forms of in-situ calibration validation discussed in this whitepaper give the end user information about the thermal meter’s operating performance, but only the ow-audit method actually validates the calibration at actual owing conditions. Acknowledgements I would like to thank Scott Rouse, Erica Giannini and Charlotte Chapman for their contributions to the white paper. 12 Figure 9. Sierra’s QuadraTherm® Mass Flow Meter Featuring DrySense™ Sensor Technology