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Resistance Thermometr
Transcript of Resistance Thermometr
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Resistance thermometer
Resistance thermometers, also called resistancetemperature detectors (RTDs), are temperaturesensors
that exploit the predictable change in electricalresistance of some materials with changing temperature.As they are almost invariably made ofplatinum, they areoften called platinum resistance thermometers (PRTs).They are slowly replacing the use of thermocouples in
many industrial applications below 600 C.General description
There are two broad categories, "film" and "wire-wound"types.
Film thermometers have a layer of platinum on asubstrate; the layer may be extremely thin, perhaps 1micrometer. Advantages of this type are relatively lowcost and fast response. Such devices have improved inperformance although the different expansion rates of
the substrate and platinum give "strain gauge" effectsand stability problems.
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How do resistance thermometers work?
Resistance thermometers are constructed in a number offorms and offer greater stability, accuracy and repeatability
in some cases than thermocouples. While thermocouplesuse the Seebeck effect to generate a voltage, resistancethermometers use electrical resistance and require a smallpower source to operate. The resistance ideally varieslinearly with temperature.
Resistance thermometers are usually made using platinum,because of its linear resistance-temperature relationshipand its chemical inertness. The platinum detecting wire
needs to be kept free of contamination to remain stable. Aplatinum wire or film is supported on a former in such a waythat it gets minimal differential expansion or other strainsfrom its former, yet is reasonably resistant to vibration.
Commercial platinum grades are produced which exhibit a
change of resistance of 0.385 ohms/C (European
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Advantages and limitations
Advantages of platinum resistance thermometers:
High accuracy
Low drift Wide operating range
Suitability for precision applications
Limitations:
RTDs in industrial applications are rarely used above 660C. At temperatures above 660 C it becomes increasinglydifficult to prevent the platinum from becomingcontaminated by impurities from the metal sheath of thethermometer. This is why laboratory standard
thermometers replace the metal sheath with a glassconstruction. At very low temperatures, say below -270 C(or 3 K), due to the fact that there are very few phonons,the resistance of a RTD is mainly determined by impuritiesand boundary scattering and thus basically independent
of temperature. As a result, the sensitivity of the RTD is
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Resistance thermometer elements
Resistance thermometer elements are available in a
number of forms. The most common are:
Wire wound in a ceramic insulator - wire spiral within
sealed ceramic cylinder, works with temperatures to 850
C
Wire encapsulated in glass - wire around glass core with
glass fused homogenously around, resists vibration, more
protection to the detecting wire but smaller usable range
Thin film - platinum film on ceramic substrate, small and
inexpensive to mass produce, fast response totemperature change
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Resistance thermometer construction
These elements nearly always require insulated leads attached. At low
temperatures PVC, silicon rubber or PTFE insulators are common to 250C.Above this, glass fibre or ceramic are used. The measuring point and usually most
of the leads require a housing or protection sleeve. This is often a metal alloy
which is inert to a particular process. Often more consideration goes in to
selecting and designing protection sheaths than sensors as this is the layer that
must withstand chemical or physical attack and offer convenient process
attachment points.
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Resistance thermometer wiring configurations
Two-wire configuration The simplest resistance thermometer configuration
uses two wires. It is only used when high accuracyis not required as the resistance of the connecting
wires is always included with that of the sensor
leading to errors in the signal. Using this
configuration you will be able to use 100 metres of
cable. This applies equally to balanced bridge and
fixed bridge system.
Three-wire configuration In order to minimize the effects of the leadresistances a three wire configuration can be
used. Using this method the two leads to the
sensor are on adjoining arms, there is a lead
resistance in each arm of the bridge and
therefore the lead resistance is cancelled out.
High quality connection cables should be used
for this type of configuration because an
assumption is made that the two lead
resistances are the same. This configuration
allows for up to 600 meters of cable.
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Resistance thermometer wiring configurations
Four-wire configuration The four wire resistance thermometerconfiguration even further increases
the accuracy and reliability of the
resistance being measured. In the
diagram above a standard two terminal
RTD is used with another pair of wires
to form an additional loop that cancels
out the lead resistance. The aboveWheatstone bridge method uses a little
more copper wire and is not a perfect
solution. Below is a better alternative
configuration four-wire Kelvin
connection that should be used in all
RTDs. It provides full cancellation ofspurious effects and cable resistance of
up to 15 can be handled. Actually in
four wire measurement the resistance
error due to lead wire resistance is
zero.
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History
The application of the tendency ofelectrical conductors to
increase their electrical resistance with rising temperature
was first described by Sir William Siemens at the BakerianLecture of 1871 before the Royal Society ofGreat Britain.
The necessary methods of construction were established
by Callendar, Griffiths, Holborn and Wein between 1885
and 1900.
Standard resistance thermometer data
Temperature sensors are usually supplied with thin-film
elements. These are rated in accordance with BS EN
60751:1996 as:
Tolerance class Valid range
Tolerance class B 70 to +500C
Tolerance class A
(1/2B
30 to +350 C
Tolerance class 1/3B 0 to +100 C
Resistance thermometer elements can be supplied which function up to 850C. Sensor
tolerances are calculated as:
Tolerance Class Temperature DeviationClass B t= (0.3+0.005|t|)
Class A t= (0.15+0.0025|t|)
1/3 DIN t= 13 (0.3+0.005|t|)
1/3 DIN t= 15 (0.3+0.005|t|)
1/10 DIN t= 110
(0.3+0.005|t|)
where |t| = absolute value of temperature inC. Where elements have a resistance ofn x
100 then the basic values and tolerances
also have to be multiplied by n.
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Temperature to resistance equation
The relation between temperature and resistance is given
by the Callendar-Van Dusen equation, Here, R
Tis the resistance at temperature T, R0 is the
resistance at 0 C, and the constants (for an
alpha=0.00385 platinum RTD) are
Since the B and Ccoefficients are relatively small, theresistance changes almost linearly with the temperature.
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