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Temperature Temperature measurementsmeasurements
OutlineOutline1. Liquid-in-glass thermometres1. Liquid-in-glass thermometres
2. Bimaterial thermometres2. Bimaterial thermometres
3. Electrical thermometres3. Electrical thermometres
4. IR-thermometres4. IR-thermometres
5. Pyrometres5. Pyrometres
6. Summary6. Summary
7. Other measurement methods7. Other measurement methods
Liquid-in-glass Liquid-in-glass thermometresthermometres
Liquid-in-glass Liquid-in-glass thermometresthermometres
The “traditional” thermometresThe “traditional” thermometresMeasurement scale from -190 Measurement scale from -190 °C to °C to +600 °C+600 °C
Used mainly in calibrationUsed mainly in calibrationMercury: -39 °C … +357 °CMercury: -39 °C … +357 °CSpirit: -14 °C … +78 °CSpirit: -14 °C … +78 °C
Functionning methodFunctionning method
Method is based on the expansion of Method is based on the expansion of a liquid with temperaturea liquid with temperature
The liquid in the bulb is forced up the The liquid in the bulb is forced up the capillary stemcapillary stem
Thermal expansion:Thermal expansion:
)1(0 TVV
StructureStructure
Causes of inaccuratiesCauses of inaccuraties Temperature Temperature
differences in the differences in the liquidliquid
Glass temperature Glass temperature also affectsalso affects
The amount of The amount of immersion (vs. immersion (vs. calibration)calibration)
Bimaterial thermometresBimaterial thermometres
Method based on different thermal Method based on different thermal expansions of different metalsexpansions of different metals– Other metal expands more than other: Other metal expands more than other:
twistingtwisting– Inaccurary Inaccurary ± 1 ° C± 1 ° C– Industry, sauna thermometresIndustry, sauna thermometres
Bimaterial thermometresBimaterial thermometres
Electrical thermometresElectrical thermometres
Electrical thermometresElectrical thermometres
Resistive thermometresResistive thermometres– Resistivity is temperature dependentResistivity is temperature dependent
– Materials: Platinum, nickelMaterials: Platinum, nickel
)1()( 0 TRTR
Characteristic resistancesCharacteristic resistances
Thermistor thermometresThermistor thermometres
Semiconductor materialsSemiconductor materials Based on the temperature Based on the temperature
dependence of resistancedependence of resistance Thermal coefficient non-linear, 10 Thermal coefficient non-linear, 10
times bigger than for metal resistortimes bigger than for metal resistor NTC, (PTC): temperature coefficient’s NTC, (PTC): temperature coefficient’s
signsign
Example of a characteristic Example of a characteristic curvecurve
Limitations of electrical Limitations of electrical thermometresthermometres
Sensor cable’s resistance and its Sensor cable’s resistance and its temperature dependencytemperature dependency
Junction resistancesJunction resistances Thermal voltagesThermal voltages Thermal noise in resistorsThermal noise in resistors Measurement currentMeasurement current Non-linear temperature dependenciesNon-linear temperature dependencies Electrical perturbationsElectrical perturbations Inaccuracy at least Inaccuracy at least ± 0.1 °C± 0.1 °C
Infrared thermometresInfrared thermometres
Thermal radiationThermal radiation
Every atom and molecule exists in Every atom and molecule exists in perpetual motionperpetual motion
A moving charge is associated with an A moving charge is associated with an electric field and thus becomes a electric field and thus becomes a radiatorradiator
This radiation can be used to This radiation can be used to determine object's temperaturedetermine object's temperature
Thermal radiationThermal radiation
Waves can be characterized by their Waves can be characterized by their intensities and wavelengthsintensities and wavelengths– The hotter the object:The hotter the object:
the shorter the wavelengththe shorter the wavelength the more emitted lightthe more emitted light
Wien's law:Wien's law:
cmKT 2896.0max
Planck's lawPlanck's law
1
21)(
2
5
kT
hc
e
hcF
Magnitude of radiation at particular wavelength (λ) and particular temperature (T).h is Planck’s constant and c speed of light.
BlackbodyBlackbody
An ideal emitter of electromagnetic An ideal emitter of electromagnetic radiationradiation– opaqueopaque– non-reflectivenon-reflective– for practical blackbodies for practical blackbodies εε = 0.9 = 0.9
Cavity effectCavity effect– em-radiation measured from a cavity of em-radiation measured from a cavity of
an objectan object
Cavity effectCavity effect
Emissivity of the cavity increases and Emissivity of the cavity increases and approaches unityapproaches unity
According to Stefan-Boltzmann’s law, According to Stefan-Boltzmann’s law, the ideal emitter’s photon flux from the ideal emitter’s photon flux from area a isarea a is
In practice:In practice:
40 Ta
0 r
Cavity effectCavity effect
For a single reflection, effective For a single reflection, effective emissivity isemissivity is
Every reflection increases the Every reflection increases the emyssivity by a factor (1-emyssivity by a factor (1-εε))
bbr )1(0
Cavity effectCavity effect
Practical blackbodiesPractical blackbodies
Copper most common materialCopper most common material The shape of the cavity defines the The shape of the cavity defines the
number of reflectionsnumber of reflections– Emissivity can be increasedEmissivity can be increased
DetectorsDetectors
Quantum detectorsQuantum detectors– interaction of individual photons and interaction of individual photons and
crystalline latticecrystalline lattice– photon striking the surface can result to photon striking the surface can result to
the generation of free electronthe generation of free electron– free electron is pushed from valency to free electron is pushed from valency to
conduction band conduction band
DetectorsDetectors
– hole in a valence band serves as a hole in a valence band serves as a current carriercurrent carrier
– Reduction of resistanceReduction of resistance
Photon’s energyPhoton’s energy
hE
DetectorsDetectors
Thermal detectorsThermal detectors– Response to heat resulting from Response to heat resulting from
absorption of the sensing surfaceabsorption of the sensing surface– The radiation to opposite direction (from The radiation to opposite direction (from
cold detector to measured object) must cold detector to measured object) must be taken into accountbe taken into account
Thermal radiation from Thermal radiation from detectordetector
PyrometresPyrometres
Disappearing filament pyrometerDisappearing filament pyrometer– Radiation from and object in known Radiation from and object in known
temperature is balanced against an temperature is balanced against an unknown targetunknown target
– The image of the known object The image of the known object (=filament) is superimposed on the (=filament) is superimposed on the image of targetimage of target
PyrometresPyrometres
– The measurer adjusts the current of the The measurer adjusts the current of the filament to make it glow and then filament to make it glow and then disappeardisappear
– Disappearing means the filament and Disappearing means the filament and object having the same temperatureobject having the same temperature
Disapperaring filament Disapperaring filament pyrometerpyrometer
PyrometresPyrometres
Two-color pyrometerTwo-color pyrometer– Since emissivities are not usually known, Since emissivities are not usually known,
the measurement with disappearing the measurement with disappearing filament pyrometer becomes impracticalfilament pyrometer becomes impractical
– In two-color pyrometers, radiation is In two-color pyrometers, radiation is detected at two separate wavelengths, detected at two separate wavelengths, for which the emissivity is approximately for which the emissivity is approximately equalequal
Two-colour pyromererTwo-colour pyromerer
PyrometersPyrometers
– The corresponding optical transmission The corresponding optical transmission coefficients are coefficients are γγxx and and γγy y
Displayed temperatureDisplayed temperature
1
5
5
ln11
yx
xy
xyc CT
MeasurementsMeasurements
– Stefan-Boltzmann’s law with manipulation:Stefan-Boltzmann’s law with manipulation:
– Magnitude of thermal radiation flux, sensor Magnitude of thermal radiation flux, sensor surface’s temperature and emissivity must surface’s temperature and emissivity must be known before calculationbe known before calculation
– Other variables can be considered as Other variables can be considered as constants in calibrationconstants in calibration
44
sc A
TT
Error sourcesError sources
Errors in detection of the radiant flux Errors in detection of the radiant flux or reference temperatureor reference temperature
Spurious heat sourcesSpurious heat sources– Heat directly of by reflaction into the Heat directly of by reflaction into the
optical system optical system Reflectance of the object (e.g. 0.1)Reflectance of the object (e.g. 0.1)
But does not require contact to surface But does not require contact to surface measured!measured!
Pyroelectric thermometresPyroelectric thermometres
Generate electric charce in response Generate electric charce in response to heat fluxto heat flux– Crystal materialsCrystal materials– Comparable to piezoelectric effect: the Comparable to piezoelectric effect: the
polarity of crystals is re-orientedpolarity of crystals is re-oriented
SummarySummary
Only some temperature Only some temperature measurement methods presentedmeasurement methods presented
Examples of phenomenons used: Examples of phenomenons used: thermal expansion, resistance’s thermal expansion, resistance’s thermal dependency, radiationthermal dependency, radiation
The type of meter depends onThe type of meter depends on– Measurement object’s propertiesMeasurement object’s properties– TemperatureTemperature
More temperature More temperature measurement possibilitiesmeasurement possibilities
ThermocouplesThermocouples Semiconductor thermometresSemiconductor thermometres Temperature indicatorsTemperature indicators
– Crayons etc.Crayons etc. Manometric (gas pressure) sensors Manometric (gas pressure) sensors
Questions?Questions?