winsem2012 13 cp0401 28 mar 2013 rm01 temperature transducers

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    Thermocouples

    Resistance-Temperature Detectors (RTD)

    Thermistors

    Temperature Sensors

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    In 1821, T.J.Seebeck discovered that an electric potentialoccurs when two different metals are joined into a loop and thetwo junctions are held at different temperatures.

    Seebeck e.m.f

    a voltage difference between the two ends ofthe conductor that depends on the temperature difference ofthe ends and a material property.

    If the ends of the wire has the same temperature, no e.m.f

    occurs, even if the middle of the wire is hotter or colder.

    Thermocouple

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    Thermocouple - Principle

    Twisting or welding of 2 wires

    http://en.wikipedia.org/wiki/Image:Tc-dia.jpg
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    In normal operation, cold junction is

    placed in an ice bath

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    In normal operation, cold junction is

    placed in an ice bath

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    Type K : Chromel-Alumel

    Type J : Iron-Constantan

    Type E : Chromel-Constantan

    Type N : Nicros-Nisil

    Type T : Copper-Constantan

    It is important to note that thermocouplesmeasure the temperature difference betweentwo points, not absolute temperature.

    Thermocouples

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    Thermocouples Characteristics

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    where

    c andk = constants of the thermocouple materials

    T1= the temperature of the hot junction

    T2= the temperature of the cold or reference junction

    Magnitude of thermal EMF

    )()( 222

    121 TTkTTcE

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    A thermocouple was found to have linear calibrationbetween 0oC and 400oC with emf at maximumtemperature (reference junction temperature 0oC) equalto 20.68 mV.

    a) Determine the correction which must be made to the indicated e.m.f if the cold

    junction temperature is 25oC.

    b) If the indicated e.m.f is 8.92 mV in the thermocouple circuit, determine thetemperature of the hot junction.

    Problem

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    (a) Sensitivity of the thermocouple

    = 20.68/(400o-0o)

    = 0.0517 mV/C

    Since the thermocouple is calibrated at thereference junction of 0C and is being used at25C, then the correction which must be made,E

    corr

    between 0C and 25C

    Ecorr= 0.0517 x 25

    Ecorr= 1.293 mV

    Solution

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    Thermocouples are most suitable for measuring

    over a large temperature range, up to 1800 K.

    Example:

    Type K: Chromel-Alumel (-190C to 260C)

    Type J: Iron-Constantan (-190C to 760C)

    Type E: Chromel-Constantan(-100C to 1260C)

    Thermocouple - applications

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    Thermocouples are most suitable for measuring

    over a large temperature range, up to 1800 K.

    They are less suitable for applications wheresmaller temperature differences need to be

    measured with high accuracy, for example the

    range 0100C with 0.1C accuracy. For suchapplications, Thermistors and RTDs are more

    suitable.

    Thermocouple - applications

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    Resistance temperature detectors (RTDs), alsocalled resistance thermometers, are temperaturesensors that exploit the predictable change inelectrical resistance of some materials with

    changing temperature.

    Temperature Metal Resistance

    The resistance ideally varies linearly withtemperature.

    Resistance temperature detector (RTD)

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    RTD/Resistance Theromometer/PRT100 Circuit

    Connection:

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    Resistance Vs Temperature

    Approximations

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    A straight line has been drawn between the

    points of the curve that represent temperature,

    T1 and T2, and T0 represent the midpoint

    temperature.

    Resistance vs Temperature

    Approximations

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    Linear Approximation

    R(T) = approximation of resistance at

    temperature T

    R(T0) = resistance at temperature T0o = fractional change in resistance per

    degree of temperature at T0

    T = T - T0

    Resistance Vs Temperature

    Approximations

    21]1)[()( TTTTTRTR oo

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    Linear Approximation

    R2 = resistance at T2R1 = resistance at T1

    Resistance Vs Temperature Linear

    Approximations

    )()(

    1

    12

    12

    0 TT

    RR

    TRo

    E l

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    Example

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    More accurate representation of R-T curve

    over some span of temperatures.

    RTD quadratic approximation

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    R(T) = quadratic approximation of

    resistance at temperature T

    R(T0) = resistance at temperature T01 = linear fractional change in resistance

    with temperature2 = quadratic fractional change in

    resistance with temperature

    T = T - T0

    RTD quadratic approximation

    21

    2

    21 ])(1)[()( TTTTTTRTR o

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    Example - Solution

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    Platinum

    Copper

    TungstenNickel

    Platinum: very repeatable, sensitive,expensive

    Nickel: not quite repeatable, moresensitive, less expensive

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    Sensitivity is shown by the value o

    Platinum 0.004/ C

    Nickel 0.005/ C

    Thus, for a 100 platinum RTD, a change of

    only 0.4 would be expected if the

    temperature is changed by 1C

    RTD - sensitivity

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    Generally 0.5 to 5 seconds or more

    The slowness of response is due principally to

    the slowness of thermal conductivity in

    bringing the device into thermal equilibrium

    with its environment.

    RTD response time

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    Construction of a platinum resistance

    thermometer

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    Construction of a platinum resistance

    thermometer

    Wire is in a coil to achieve small size and improve thermalconductivity to decrease response time.

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    Construction of a platinum resistance

    thermometer

    Protect from the environment

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    Semiconductor resistance sensors

    Unlike metals, thermistors respond negatively totemperature and their coefficient of resistance is

    of the order of 10 times higher than that ofplatinum or copper.

    Temperature semiconductor resistance

    Symbol

    Thermistors

    http://en.wikipedia.org/wiki/Image:Thermistor_symbol.png
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    Thermistor: resistance vs temperature

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    Thermistor

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    Scan example 6.3 module page 109