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Capgo datalogger, data logger, datalogging and data logging. Home | About Us | Contact Us | Employment Products News Resources Support Subscribe search RTDs Home > Resources > Temperature > Sensors > RTDs Introduction to RTDs Resistance Temperature Detectors (RTDs) rely on the predictable and repeatable phenomena of the electrical resistance of metals changing with temperature. The temperature coefficient for all pure metals is of the same order 0.003 to 0.007 ohms/ohm/°C. The most common metals used for temperature sensing are platinum, nickel, copper and molybdenum. While the resistance temperature characteristics of certain semiconductor and ceramic materials are used for temperature sensing (see sections on Semiconductor and Thermistor ), such sensors are generally not classified as RTDs. A precision RTD Temperature Calculator supporting four RTD types can provide a "handson" understanding of RTD characteristics. How are RTDs constructed? RTDs are manufactured in two ways: using wire or film. Wire RTDs are a stretched coil of fine wire placed in a ceramic tube that supports and protects the wire. The wire may be bonded to the ceramic using a glaze. The wire types are generally the more accurate, due to the tighter control over metal purity and less strain related errors. They are also more expensive. Film RTDs consist of a thin metal film that is silkscreened or vacuum spluttered onto a ceramic or glassy substrate. A laser trimmer then trims the RTD to its correct resistance value. Film sensors are less accurate than wire types, but they are relatively inexpensive, they are available in small sizes and they are more robust. Film RTDs can also function as a strain gauge so don't strain them! The alumina element should be supported by grease or a light elastomer, but never embedded in epoxy or mechanically clamped between hard surfaces. RTDs cannot generally be used in their basic sensing element form, as they are too delicate. They are usually built into some type of assembly, which will enable them to withstand the various environmental conditions to which they will be exposed when used. Most commonly this is a stainless steel tube with a heat conducting grease (that also dampens vibration). Standard tube diameters include 3, 4.5, 6, 8, 10, 12 and 15 mm and standard tube lengths include 250, 300, 500, 750 and 1000 mm. Characteristics of RTDs Metal RTDs have a response defined by a polynomial: R(t) = R 0 ( 1 + a.t + b.t 2 + c.t 3 ) Where R 0 is the resistance at 0°C, "t" in the temperature in Celsius, and "a", "b" and "c" are constants dependent on the characteristics of the metal. In practice this equation is a close but not perfect fit for most RTDs, so slight modifications are often be made. Commonly, the temperature characteristics of an RTD are specified as a single number (the "alpha"), representing the average temperature coefficient over the 0 to 100°C temperature range as calculated by: alpha = ( R 100 R 0 ) / 100 . R 0 in ohms/ohm/°C Note: RTDs cover a sufficient temperature range that their response needs to be calibrated in terms of the latest temperature scale ITS90. For assistance with such calculations, see the RTD temperature calculator. It is also of interest to note that the temperature coefficient of an alloy is frequently very different from that of the

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  • Capgodatalogger,datalogger,datalogginganddatalogging.

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    IntroductiontoRTDsResistanceTemperatureDetectors(RTDs)relyonthepredictableandrepeatablephenomenaoftheelectricalresistanceofmetalschangingwithtemperature.Thetemperaturecoefficientforallpuremetalsisofthesameorder0.003to0.007ohms/ohm/C.Themostcommonmetalsusedfortemperaturesensingareplatinum,nickel,copperandmolybdenum.Whiletheresistancetemperaturecharacteristicsofcertainsemiconductorandceramicmaterialsareusedfortemperaturesensing(seesectionsonSemiconductorandThermistor),suchsensorsaregenerallynotclassifiedasRTDs.AprecisionRTDTemperatureCalculatorsupportingfourRTDtypescanprovidea"handson"understandingofRTDcharacteristics.

    HowareRTDsconstructed?RTDsaremanufacturedintwoways:usingwireorfilm.WireRTDsareastretchedcoiloffinewireplacedinaceramictubethatsupportsandprotectsthewire.Thewiremaybebondedtotheceramicusingaglaze.Thewiretypesaregenerallythemoreaccurate,duetothetightercontrolovermetalpurityandlessstrainrelatederrors.Theyarealsomoreexpensive.

    FilmRTDsconsistofathinmetalfilmthatissilkscreenedorvacuumsplutteredontoaceramicorglassysubstrate.AlasertrimmerthentrimstheRTDtoitscorrectresistancevalue.Filmsensorsarelessaccuratethanwiretypes,buttheyarerelativelyinexpensive,theyareavailableinsmallsizesandtheyaremorerobust.FilmRTDscanalsofunctionasastraingaugesodon'tstrainthem!Thealuminaelementshouldbesupportedbygreaseoralightelastomer,butneverembeddedinepoxyormechanicallyclampedbetweenhardsurfaces.

    RTDscannotgenerallybeusedintheirbasicsensingelementform,astheyaretoodelicate.Theyareusuallybuiltintosometypeofassembly,whichwillenablethemtowithstandthevariousenvironmentalconditionstowhichtheywillbeexposedwhenused.Mostcommonlythisisastainlesssteeltubewithaheatconductinggrease(thatalsodampensvibration).Standardtubediametersinclude3,4.5,6,8,10,12and15mmandstandardtubelengthsinclude250,300,500,750and1000mm.

    CharacteristicsofRTDsMetalRTDshavearesponsedefinedbyapolynomial:

    R(t)=R0(1+a.t+b.t2+c.t3)

    WhereR0istheresistanceat0C,"t"inthetemperatureinCelsius,and"a","b"and"c"areconstantsdependentonthecharacteristicsofthemetal.InpracticethisequationisaclosebutnotperfectfitformostRTDs,soslightmodificationsareoftenbemade.Commonly,thetemperaturecharacteristicsofanRTDarespecifiedasasinglenumber(the"alpha"),representingtheaveragetemperaturecoefficientoverthe0to100Ctemperaturerangeascalculatedby:

    alpha=(R100R0)/100.R0inohms/ohm/C

    Note:RTDscoverasufficienttemperaturerangethattheirresponseneedstobecalibratedintermsofthelatesttemperaturescaleITS90.Forassistancewithsuchcalculations,seetheRTDtemperaturecalculator.Itisalsoofinteresttonotethatthetemperaturecoefficientofanalloyisfrequentlyverydifferentfromthatofthe

  • constituentmetals.Smalltracesofimpuritiescangreatlychangethetemperaturecoefficients.Sometimestrace"impurities"aredeliberatelyaddedsoastoswamptheeffectsofundesiredimpuritieswhichareuneconomictoremove.Otheralloyscanbetailoredforparticulartemperaturecharacteristics.Forexample,analloyof84%copper,12%Manganeseand4%Nickelhasthepropertyofhavinganalmostzeroresponsetotemperature.Thealloyisusedforthemanufactureofprecisionresistors.

    TypesofRTDsWhilealmostanymetalmaybeusedforRTDmanufacture,inpracticethenumberusedislimited.

    Metal TemperatureRange Alpha Comments

    Copper Pt 200Cto260C 0.00427 Lowcost

    Molybdenum Mo 200Cto200C 0.003000.00385Lowercostalternativetoplatinuminthelowertemperatureranges

    Nickel Ni 80Cto260C 0.00672 Lowcost,limitedtemperaturerangeNickelIron NiFe 200Cto200C 0.00518 Lowcost

    Platinum Pt 240Cto660C0.003850.003920.00377

    Goodprecision.Extendtemperaturerangeto1000Cavailable

    Othermaterialsareusedforspecialistapplications.Forexample,cryogenictemperaturesensors.

    PlatinumRTDsPlatinumisbyfarthemostcommonRTDmaterial,primarilybecauseofitslongtermstabilityinair.TherearetwostandardPlatinumsensortypes,eachwithadifferentdopinglevelof'impurities'.ToalargeextenttherehasbeenaconvergenceinplatinumRTDstandards,withmostnationalstandardsbodiesadoptingtheinternationalIEC7511983,withamendment1in1986andamendment2in1995.TheUSAcontinuestomaintainitsownstandard.AlltheplatinumstandardsuseamodifiedpolynomialknownastheCallendarVanDusenequation:

    R(t)=R0(1+a.t+b.t2+c.(t100).t3)

    PlatinumRTDsareavailablewithtwotemperaturecoefficientsoralphasthechoiceislargelybasedonthenationalpreferenceinyoucountry,asindicatedinthefollowingtable:

    Standard Alphaohms/ohm/CR0

    ohmsPolynomialCoefficients Countries

    IEC751(Pt100) 0.00385055 100

    200C

  • thermoelectriceffect,vibrationtolerance,leadmarkingandsensormarking.Someofthesearediscussedbelow:ThermoelectricEffect:AplatinumRTDgenerallyemploystwometalstheplatinumsensingelementandcopperleadwires,makingitagoodcandidateforathermocouple.Ifatemperaturegradientisallowstodevelopalongthesensingelement,athermoelectricvoltagewithamagnitudeofabout7V/Cwillbegenerated.Thisisonlylikelytobeaproblemwithveryhighprecisionmeasurementsoperatingatlowexcitationcurrents.WiringConfigurationsandLeadMarking:Therearethreewiringconfigurationsthatcanbeusedformeasuringresistance2,3and4wireconnections.

    IEC751requiresthatwiresconnectedtothesameendoftheresistorbethesamecoloureitherredorwhite,andthatthewiresateachendbedifferent.Seethemeasurementsectionforthemeritsofeachofthesewiringschemes.SensorMarking:IEC751stipulatesthatasensorshouldbemarkedwithitsnominalR0value,toleranceclass,thewiringconfigurationandtheallowabletemperaturerange.Anexamplemarkingis:

    Pt100/A/3/100/+200

    correspondingto100Ohmplatinum,classA,3wireconfigurationandwithatemperaturerangefrom100Cto+200C.MeasurementCurrent:Preferredmeasurementcurrentsarespecifiedas1,2and5mA,although5mAisnotallowedwithclassAsensorsduetopotentialselfheatingerrors.

    NickelRTDsNickelsensorsarepreferredincostsensitiveapplicationssuchasairconditioningandconsumergoods.Becausecostisanissue,theyaregenerallymanufacturedinhigherresistancevaluesof1kor2kohmssothatasimpletwowireconnectioncanbeused(ratherthanthe3or4wireconnectionscommonwithplatinumtypes).ThereappearstobenointernationalstandardcoveringthenickelRTD,althoughmostmanufacturersappeartofollowIEC751(whichonlydealswithplatinumdevices)whereappropriate.AresultingproblemisthatthereappearstobenowidelyacceptedcalibrationforthenickelRTD.OnemanufacturerofnickelRTDsrecommendsthefollowingpolynomial:

    R(t)=R0(1+a.t+b.t2+d.t4+f.t6)

    wherea=5.485x103b=6.650x106d=2.805x1011andf=2.000x1017.Thealphaforthispartis0.00672ohms/ohm/CMorecommonforlowtomediumprecisionmeasurementthesimplificationoftheequationisusedwitha=alpha:

    R(t)=R0(1+a.t)

    whichiseasilyinvertedfortemperature:

    t=(Rt/R01)/a=(Rt/R01)/0.00672

    where"a"issubstitutedforthealphavalue.Nickelislesschemicallyinertthatplatinumandsoislessstableathighertemperatures.Glasspassivationcanextendtheusefultemperaturerangeto200C,butthenickelRTDisnormallyusedforsensingintheenvironmentaltemperaturerangeandinclearair.

    NickelIronRTDsLowerincostthanthepureNickelRTD,theNickelIronRTDfindsapplicationinHVACandothercostsensitiveapplications.Thealpha=0.00518

    CopperRTDsCopperisrarelyusedspecificallyasasensingelement,butisoftenemployedwhenacoppercoilexistsforotherpurposes.Forexampleinavibratingwirestaingaugeacoilisrequiredto"pluck"thewireandsenseitsvibrationfrequency.Thesamecoilcanbeusedtosensethetemperatureofthesensorsothatitsreadingsmaybecompensatedfortemperatureinduceddrifts.Anotherapplicationisinmeasuringthetemperatureofelectricmotorandtransformerwindings.Inthesetypesofapplications,wheretemperaturesensingisasecondaryfunction,careshouldbetakeninwindingthecoilsothatthermalexpansionofthesystemdoesnotinducesignificantstraingaugeeffectsinthecopperwirewhichmayaddtotheuncertaintyofthemeasurement.ThereappearstobenointernationalstandardforcopperRTDs,howeveranalpha=0.00427ohms/ohm/Ciscommonlyused.Whenthetemperaturerangeissmall(say0Cto180C)andtheaccuracyneedsarenotgreat,asimplelinearfunctioncanbeused:

  • t=(Rt/R01)/0.00427

    MolybdenumRTDsMolybdenumhasatemperaturecoefficientofexpansionwhichalmostperfectlymatchesthatofalumina,makingitanidealmaterialforfilmtypeofconstruction.Theusefultemperaturerangeistypically200Cto+200Candthematerial'salpha=0.00300ohms/ohm/C.MolybdenumRTDsarealsoavailablewithanalpha=0.00385ohms/ohm/C(achievedbydopingwithothermetals)whichmakesitcompatiblewiththestandardPt100devicesoverareducedtemperaturerangeandatareducedcost.

    ProprietarytypesAnumberofcompaniesmanufactureproprietaryRTDsensortypesanddonotnecessarilypublishdetailsaboutthesensingmaterialused.OnesuchdeviceistheTDSeriesoftemperaturesensorsfromHoneywell.Theseappeartobeconstructedbydepositingathinmetalfilmonasiliconsubstrateandtrimmingbylaser.Thebenefitsarearelativelylowcost,simplicityand0.7Cinterchangeabilityat20C.TheresponseoftheHoneywellpartsissimilartoaplatinumRTD:

    R(t)=R0(1+3.84x103.t+4.94x106.t2)

    ThefollowingtablerepresentssomeoftheproprietaryRTDsensortypesmanufacturedbyavarietyofcompanies:

    Sensor Manuf. Output Tolerance(range) Package Comments

    TD4ATD5A Honeywell

    8ohms/C(1854ohmsat

    0C)2.5C

    (40Cto150C)TO92orthreaded

    tubeMetalfilmonsiliconsubstrate

    KTY81KTY82KTY83KTY84KTY85

    Philips1Kor2Kat

    25C,+0.8%/CSeebelow

    6Cto12C(55Cto+150Csometo300C)

    SOD70,SOT23SOD68SOD80

    Bulkresistanceofsilicon.Keepexcitationcurrent>0.1mAand