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Instrument Model for Narrow Angle Radiometers KAITLYN SCHEIB, JENNIFER SPINTI, ANDREW FRY, STAN HARDING, IGNACIO PRECIADO DEPARTMENT OF CHEMICAL ENGINEERING THE UNIVERSITY OF UTAH

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  • InstrumentModelforNarrowAngleRadiometersKAITLYNSCHEIB, JENNIFERSPINTI, ANDREWFRY, STANHARDING,IGNACIOPRECIADODEPARTMENTOFCHEMICALENGINEERINGTHEUNIVERSITYOFUTAH

  • L15001.5MWFurnace

    FDandRecycleFan

    ConvectiveSection

    BaghouseAir/FGR/O2Control

    RadiativeSection

    Burner

    SamplePorts(Radiometers)

  • OverviewofanInstrumentModel

    MeasuredSignal(mV)

    QuantityofInterest(Incidentheatflux)

    SourcesofUncertainty

  • NarrowAngleRadiometerDesign◦ Thechangeintemperatureofthethermistorcausesachangeinresistance◦ DesignbasedonIFRFandusedbyPRAXAIR◦ Wehaveidentifieduncertaintiesinconstruction,operationandcalibration

    𝛼"#

  • NarrowAngleRadiometerDesign:WheatstoneBridge

    𝑉%&'( = 𝑉'**𝑅,-,

    𝑅,-, + 𝑅/−

    𝑅122𝑅122 + 𝑅3 𝑅122 =

    𝑉-45𝑅/𝑉'** − 𝑉-45

    𝛼"#

  • NarrowAngleRadiometerDesign:LensFocallength(17-25mm):𝑓 = 7

    ,8/

    Reflectivity(0.022-0.041):𝜌 = ,:8,;,:

  • DesignUncertainty

    𝛼"#

    • Transienttemperature

    • Irradiatedthermistortemperature

    • Non-irradiatedthermistorplacement

    • Measuredvoltage

    • Refractiveindex• Imagesize• Focalpoint• Lensmounting

    • Viewangle• Reflectivity

  • DesignUncertainty:WheatstoneBridge◦ Resistors◦ Two250ΩresistorswereusedintheWheatstonebridge

    ◦ Operatingtemperaturerange:-55˚Cto150˚C◦ Resistorscandriftupto1%overlifetime

    ◦ Thermistors◦ Thetemperatureofthethermistorsisrelatedtotheresistance

    ◦ Theoperatingtemperaturerangeofthethermistorsis-40˚Cto125˚C

    ◦ Thethermistorresistancecandriftupto1%◦ ±5%uncertaintybetweenthermistors

    𝑇 = 𝐴 + 𝐵𝑙𝑛𝑅𝑅2&"

    + 𝐶𝑙𝑛3𝑅𝑅2&"

    + 𝐷𝑙𝑛D𝑅𝑅2&"

    8/

  • DesignUncertainty:TransientTemperatureEffectsonWheatstoneBridge

  • DesignUncertainty:ViewAngleRadiometer 1 1 3 3

    Percentofmax 2% 0% 2% 0%

    Viewangle 5.67˚ 6.7˚ 3.7˚ 4.16˚

    Correction2D(⍺) 0.286 0.244 0.356 0.318

    Correction 3D(⍺) 0.303 0.238 0.552 0.474

    𝑞F'G” = 𝑞1” 1 − 𝜌 𝛼

    Camperchioli, William. “Narrow Angle Wide Spectral Range Radiometer Design.” NASA, 2005.

  • Calibration:MuffleFurnace

    01002003004005006007008009001000110012001300

    0 10 20 30 40 50 60 70

    Flux(W

    /m2)

    mV

    Radiometer3

    12/01- 10cm- midrange

    12/02- 5cm- midrange

    11/28- 7.6cm- midrange

  • Calibration:LowRangeBlackbody

    https://www.landinst.com/products/landcal-r1200p-high-temperature-portable

    0

    100

    200

    300

    400

    500

    25 27 29 31 33 35 37 39

    Flux(W

    /m2)

    mV

    Radiometer3

    10/28- lowrange

    8/8- lowrange

    7/12- lowrange

  • CalibrationUncertaintyMid-rangeuncertainties◦ Targettemperature◦ Graphitesheet◦ Non-uniformtemperature◦ Targetsize◦ Calibrationalignment

    Low-rangeuncertainties:◦ Non-uniformtemperature◦ Targetsize◦ Targettemperature◦ Oxidelayerformation◦ Calibrationalignment

  • CalibrationResults

  • InstrumentUncertainty:AnalysisWHEATSTONEANALYSIS

    Voltagedividerequation:

    𝑅122 =Z[\] 7±/%

    Z̀ aa±D%Z 8Z[\]

    Wheatstonebridgeequation:

    𝑉%&'( = 𝑉'** ± 3𝑚𝑉7h[h±/%

    (7h[h±/%)

  • InstrumentUncertainty:Results

    Tbb (˚C) mVmin mVmax ±%

    600 -21.591 71.374 186.74%

    800 -15.393 78.089 149.10%

    1000 -4.570 89.815 110.722%

    1200 11.699 107.441 80.361%

  • ConclusionsandRecommendationsManysourcesofuncertaintyhavebeenidentifiedandaccountedfor

    Therearestillsourcesofuncertaintynotaccountedforasseeninthecalibrationcurves

    ThelargestsourceofuncertaintycomesfromtheuseoftheWheatstonebridge◦ ±130% with1%thermistoruncertaintyvs.±72% withnothermistoruncertainty

    Weneedmoreaccurateheatfluxmeasurementsinthefuture

    Recommendations◦ EliminateWheatstonebridge:usethermopileinstead◦ Smallerviewangleandeliminatereflectivityinsidetube◦ Higherpurgegasflowrate

  • THANKYOU