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.

    http://en.wikipedia.org/wiki/Temperaturehttp://en.wikipedia.org/wiki/Sensorhttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Platinumhttp://en.wikipedia.org/wiki/Thermocouplehttp://en.wikipedia.org/wiki/Celsiushttp://en.wikipedia.org/wiki/Platinghttp://en.wikipedia.org/wiki/Metrehttp://en.wikipedia.org/wiki/Strain_gaugehttp://en.wikipedia.org/wiki/Strain_gaugehttp://en.wikipedia.org/wiki/Strain_gaugehttp://en.wikipedia.org/wiki/Strain_gaugehttp://en.wikipedia.org/wiki/Metrehttp://en.wikipedia.org/wiki/Platinghttp://en.wikipedia.org/wiki/Celsiushttp://en.wikipedia.org/wiki/Thermocouplehttp://en.wikipedia.org/wiki/Platinumhttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Sensorhttp://en.wikipedia.org/wiki/Temperature
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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

    http://en.wikipedia.org/wiki/Seebeck_effecthttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Linearhttp://en.wikipedia.org/wiki/Platinumhttp://en.wikipedia.org/wiki/Ohm_(unit)http://en.wikipedia.org/wiki/Ohm_(unit)http://en.wikipedia.org/wiki/Platinumhttp://en.wikipedia.org/wiki/Linearhttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Seebeck_effect
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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

    http://en.wikipedia.org/wiki/Phononhttp://en.wikipedia.org/wiki/Impuritieshttp://en.wikipedia.org/w/index.php?title=Boundary_scattering&action=edithttp://en.wikipedia.org/wiki/Sensitivityhttp://en.wikipedia.org/wiki/Sensitivityhttp://en.wikipedia.org/w/index.php?title=Boundary_scattering&action=edithttp://en.wikipedia.org/w/index.php?title=Boundary_scattering&action=edithttp://en.wikipedia.org/w/index.php?title=Boundary_scattering&action=edithttp://en.wikipedia.org/wiki/Impuritieshttp://en.wikipedia.org/wiki/Phonon
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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.

    http://en.wikipedia.org/wiki/Image:Threewire.gif
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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.

    http://en.wikipedia.org/wiki/Electrical_conductorhttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Carl_Wilhelm_Siemenshttp://en.wikipedia.org/wiki/Bakerian_Lecturehttp://en.wikipedia.org/wiki/Bakerian_Lecturehttp://en.wikipedia.org/wiki/Royal_Societyhttp://en.wikipedia.org/wiki/Great_Britainhttp://en.wikipedia.org/wiki/Absolute_valuehttp://en.wikipedia.org/wiki/Absolute_valuehttp://en.wikipedia.org/wiki/Great_Britainhttp://en.wikipedia.org/wiki/Great_Britainhttp://en.wikipedia.org/wiki/Great_Britainhttp://en.wikipedia.org/wiki/Royal_Societyhttp://en.wikipedia.org/wiki/Royal_Societyhttp://en.wikipedia.org/wiki/Royal_Societyhttp://en.wikipedia.org/wiki/Bakerian_Lecturehttp://en.wikipedia.org/wiki/Bakerian_Lecturehttp://en.wikipedia.org/wiki/Bakerian_Lecturehttp://en.wikipedia.org/wiki/Carl_Wilhelm_Siemenshttp://en.wikipedia.org/wiki/Carl_Wilhelm_Siemenshttp://en.wikipedia.org/wiki/Carl_Wilhelm_Siemenshttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_resistancehttp://en.wikipedia.org/wiki/Electrical_conductorhttp://en.wikipedia.org/wiki/Electrical_conductorhttp://en.wikipedia.org/wiki/Electrical_conductor
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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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