cryogenic thermometry (2)
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AN OVERVIEW OF CRYOGENIC THERMOMETRY
Karthikeyan SubbuM.Tech (Cryogenic Engineering)
Roll No. 10CR60R11Autumn Semester Seminar-I
Indian Institute Of Technology Kharagpur 1Karthikeyan Subbu
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INTERNATIONAL TE MP ERATURE SCALE S
Temperature is defined asa thermodynamic statevariable.
T-1dQ =0Lord Kelvin 1854:absolute zero point existsfor systems in
thermodynamicequilibrium.T0= -273 .15C
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OVERVIEW OF THERMOMETER TYPES
P rimary ThermometerTemperature measurement is possible
without any prior calibration based on
fundamental law of P hysics.Secondary Thermometer
Temperature measurement is calibrated
via other available thermometer.
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P RIMARY THERMOMETER
Gas Thermometry
Vapor-Pressure Thermometry N oise ThermometersSuperconducting Fixed -P oint ThermometersN uclear -O rientation Thermometers
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S ECONDARY THERMOMETER
Resistance ThermometryCapacitance Thermometry
ThermocouplesR TDs (Resistive Temperature Devices)Thermistors
Integrated CircuitsOptical pyrometersInfrared thermometers
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GA S THERMOMETRY
Ideal gas law
PV = nRT
T (K) =f( P ) / T (K) =f(V)
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THE TWO TY P E S OF GA S THERMOMETER S
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U seful In calibration of secondary thermometer
It is one of the device used to establish the ITS-90
High precision Gas Thermometry is very tediousthus it is used mostly by National laboratories
Good up to the range of 4.2k
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NOI S E THERMOMETER
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Noise spectra taken in the region from 1 K to300 K.
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Temperatures obtained from the current sensing noise thermometer vs. temperatures from a 3He melting pressure thermometer ( ) and a
platinum NMR thermometer ( )
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NOI S E THERMOMETER
H as a very high resolution of the order of nKThe typical dimensions of the CS N T isapproximately 2X3 mm 2
R and L are chosen to fit the bandwidthrequirement it is usually L & R of the order of 2 nH and 1m
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RE S I S TANCE THERMOMETER S
Basic TheoryThe electrical conductivity of a metal
depends on the movement of electrons throughits crystal lattice. Due to thermal excitation , theelectrical resistance of a conductor variesaccording to its temperature and this forms the
basic principals of resistance thermometry.1. P ositive temperature coefficient2 . N egative temperature coefficient
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TEMP ERATURE DE P ENDENCE OF FEW MATERIAL S
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From the graph wecan see that most
of the metal areP TC e.g. P latinumSimilarly thesemiconductors
like germaniumshows a N TC
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S IMP LE S CHEMATIC DIAGRAM FOR THE MEA S UREMENT OF RE S I S TANCE
THERMOMETER
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Wheatstone Bridge
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TY P E S OF RE S I S TANCE THERMOMETER S
M etals
Semiconductors(doped)Carbon ResistorsThermoelectric
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CAP ACITANCE THERMOMETRY
Capacitance thermometry works on theprinciple of variation in the dielectricsusceptibility of the material filled inside thecapacitor .
Depending on the material property thedielectric constant varies i.e. either increases ordecreases which can be measured and theoutput is displayed.
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CAP ACITANCE V/ S TEMP ERATURE GRA P H
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CAP ACITANCE V/ S TEMP ERATURE GRA P H
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CAP ACITANCE THERMOMETRY
Capacitance thermometry has a numerousadvantage over the resistance thermometryCapacitance thermometry gives a good resolutionover the resistance thermometryComparatively capacitance thermometer are fieldindependent i.e. its is not affected by the magneticor electric field in the surrounding of themeasurement.
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REFERENCE S
Springerlink.comScience directonline.com
IEEE manuals.comWikipedia
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S UMMARY
Outline of thermometryFour important thermometer of cryogenicimportanceQuestions
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