Self-Validating ThermocouplesClosing presentation
NPL: Claire Elliott, Jonathan Pearce, Graham Machin
ESA-estec: Christian Schwarz, Robert Lindner
13th July 2012
The UK’s national standards laboratory
Develop & disseminate UK’s measurement
standards, ensure they are internationally
accepted
� Founded in 1900
� 450+ specialists in Measurement Science
� State-of-the-art laboratory facilities
� World leading National Measurement Institute
About NPL
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Overview
� Introduction
• Novel high temperature fixed points
• Self-validating concept
� Measurement
• Test arrangement
• Software
� Performance of self-validating thermocouples, up to 2300 ˚C
• Thermal cycling & extended exposure
• Benefits & current limitations
� Multi-cell design & initial results
� Future & applications
� Summary & conclusions
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Availability & Range
� Thermocouples provide the best uncertainties at high temperatures (for contact thermometry)
� Standardised types for high temperatures:
Type Max exposure
Pt-Rh types (B, R, S) 1600 ˚C (1800 ˚C)
Lower temp (K, N) 1150 ˚C (1350 ˚C)
Pt/Pd 1500 ˚C
W-Re (C, D, G) 2300 ˚C (2600 ˚C)
� W-Re thermocouples in particular degrade very quickly
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Embrittlement & Drift
� W-Re thermocouples are commonly used
above 1500 ˚C
• Suffer from embrittlement
• Quickly exhibit thermoelectric drift –
typically 10 ˚C within 10 h of operation
• Recalibration often impossible
� To address this issue, NPL, in
cooperation with ESA-estec, have developed an innovative method of validating the performance of high
temperature thermocouples in-situ
Further information: Brixy et al. High Temperatures – High Pressures 12, 625-631 (1994)
[After Brixy]
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Concept of Self-validation
� The user is enabled to perform a suitable adjustment to the reference function, if required – increasing measurement confidence
� This could be automated with a suitable algorithm
� Position of thermocouple measuring junction crucial
• Customised design from Omega Engineering
• What reliable materials could we use?
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Position the HTFP onto the thermocouple in-situ
Observe thermocouple output through the transition temperature
Apply suitable correction algorithm to the output reference function
Choose a HTFP – with a transition temperature to match process
Fixed-points for Calibration
� The international temperature scale of 1990 ( ITS-90 ) defines temperature above 0.65 K, through a series of temperature fixed-points
from…
The lowest vapour pressure point of helium (-270.15 ˚C)
to…
The freezing point of copper (1084.62 ˚C)
� How to calibrate thermocouples at higher temperatures?
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Innovative Fixed-Points
� Novel high-temperature fixed points (HTFPs)
� Many eutectic metal-carbon alloys have been shown to be suitably stable as HTFPs, for example:
• MP Fe-C 1153 ˚C
• MP Co-C 1324 ˚C
• MP Pd-C 1492 ˚C
• MP Rh-C 1657 ˚C
• MP Pt-C 1738 ˚C
• MP Ru-C 1953 ˚C
• MP Ir-C 2292 ˚C
• MP Re-C 2474 ˚C
• …
� MP determined by radiation thermometry
� Repeatability of the MP, known to be better than ±0.05 ˚C (k = 2)
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Self-validating Thermocouple
� The design consists of two parts:
• Miniature HTFP (containing a eutectic
M-C ingot)
• High temperature thermocouple
(Type C, W5%Re-W26%Re)
� Self-validation is a technique to check the calibration of a thermocouple in-situ
� The thermovoltage can be verified each time the thermal environment passes the fixed-point transition temperature
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Measurement set-up
Test Arrangement (1)
� High temperature graphite furnace (RD Webb Co., Model: RD-G)
� Argon atmosphere
Delivered Breadboard
� Five self-validating thermocouples have been provided
• Five W-Re thermocouples (from Omega Engineering)
• Five HTFP cells
� … with the equipment necessary to measure them:
• W-Re extension cable
• Zero point block calibrator
• Keithley 2182A digital nanovoltmeter
• GPIB-USB connector
• Laptop with software
• “TC Scanner”
• “Best Fit”
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Test Arrangement (2)
� Open up the furnace…
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Test Arrangement (3)
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� Open up the furnace…
� … remove the felt insulation stack…
Test Arrangement (4)
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� … remove the lid of the hot zone…
� … load the HTFP cell into a graphite shield…
� This ensures the temperature gradient over the cell is as uniform as possible
Test Arrangement (5)
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Test Arrangement (6)
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� … position the HTFP cell on the Type C thermocouple…
Test Arrangement (7)
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� … move the control thermocouple into position…
� Note, the furnace is controlled by:
• Type C thermocouple (below 1500 ˚C)
• Pyrometer (above 1500 ˚C)
Test Arrangement (8)
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� … replace the lid, felt insulation and seal the furnace…
Test Arrangement (9)
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� … connect up the thermocouples…
Test Arrangement (10)
� … ensure the reference junction is ready…
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Software (1) – “TC scanner”
� … start measuring...
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Software (2) – “Best fit”
� … and fit a curve to the melt plateau.
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Results
Results (1) - Example
� Thermal cycling
• Ramp rate of 1 ˚C/min through melt and freeze
• Held at maximum temperature for 1 hour
• Presence of cell does not impede sensor function (under these conditions) 15/26
Temperature Assignment
1720
1730
1740
1750
Tem
pera
ture
/ °
C
Time
5 min
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� Melting temperature assigned by radiation thermometry
ISO17025
traceable to ITS-90
HTFP alloy Melting temperature, °C
Uncertainty (k = 2), °C
Co-C 1323.28 0.64
Pt-C 1737.52 0.94
Ru-C 1952.98 1.00
Ir-C 2289.70 1.56
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1323.28 ± 0.64 ˚C
Results (2)
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1737.52 ± 0.94 ˚C
Results (3)
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1952.98 ± 1.00 ˚C
Results (4)
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Results (5)
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1323.28 ± 0.64 ˚C 1737.52 ± 0.94 ˚C
1952.98 ± 1.00 ˚C 2289.70 ± 1.56 ˚C
Results (6) - Thermal Cycling
� At high temperatures, the thermocouple is clearly unreliable
� Ru-C drift between 1st and 2nd melt is: 20.9 µV (~1.7 ˚C)
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Results (7) - Endurance
� Extended exposure
• Maximum temperature maintained for 10 hours
• Thermovoltage drift over 5 h (at Ir-C) is 347 µV, equivalent to ~43 ˚C
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Benefits
� By correcting for every step in drift, the user gains confidence in the temperature reading
� The thermocouple is kept within calibration: extending its useful life
� The process eliminates the uncertainty due to changing thermoelectric homogeneity
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Current limitations
� Current limitations:
• One ingot (fixed point temperature) and therefore,
• Limited temperature range of correction validity
• Ingot size
• Thermocouple and HTFP cell are separate items, at present
• Powder filling takes many steps
� All of the above can be overcome with development
� Design and use can be tailored for specific requirements
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Multi-cell (1) - Design
� Multi-cells to allow dual validation (design also
developed during the ESA/ESTEC project)
� Multi-cell containing both:
• Pt-C
• Ru-C
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Multi-cell (2) - Results
� Each ingot is clearly observed, showing good thermal contact
� Also tried Co-C and Pt-C, but found that the Co-C compartment leaked 30000
31000
32000
33000
34000
Ru-C:
1953 °C
Pt-C and Ru-C multicell
em
f /
µV
Time
1 h
Pt-C: 1737 °C
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Future & Applications
� Looking to develop into a commercial device
• User requirements
• Develop correction algorithm
� Benefits to industry are clear
• Interest in the improved temperature measurement and reliability
• Casting / manufacturing – reduced costs and enhanced quality
� Nuclear industry – self-validation with low neutron capture cross-section materials e.g. Fe-C and Cu
• EMRP project “MetroFission”
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Summary
� Introduced novel eutectic M-C fixed-points & the principle of self-validation
� Test arrangement and results
• Clear melting and freezing plateaus for all four HTFPs – up to 2300 ˚C
• The need for such validation is shown (particularly at Ir-C point)
� Benefits and current limitations
� Multi-cell design and results
� Future and applications
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Conclusions
� The concept of self-validation has been shown to be viable
• Cell size provides suitable immersion
• The presence of the cell does not impede on the function of the sensor, under these conditions
� Application of in-situ self-validation will achieve:
• Assured temperature measurement confidence
• Extended useful life of the sensor
� Which opens up the possibility for:
• Improved temperature measurement /reliability
• Reduced costs and enhanced quality
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