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CHAPTER VII

Thermometry

1. Introduction

Temperature is a measure of the degree of warmth or cold in a material. We can

perceive through touch that one bath of water is warmer than another. To make such a

concept precise we need to define a quantity called temperature in such a way that the

higher the value of the temperature of a body, the hotter it is. We also have to devise

practical and convenient methods of measuring temperature. The definition and methods

must be such as to lead to the same value of the temperature of a body measured by

different observers, using different methods.

A thermometer is a device to measure temperature. It uses a property of a material that

changes as it is heated or cooled. This property can be the volume of the material, or the

pressure of a gas at constant volume or some electrical property such as the resistance.

We have to choose two different baths and arbitrarily set a value for the temperature T1

for the cold bath and a value T2 , higher than T1 , for the temperature of the warmer bath.

We bring the thermometric device in contact with the bath, wait till thermal equilibrium

is achieved, and measure the value P of the property. Let P(T1) be the property value

when the material is kept in the cold standard bath and P(T2) be its property value when

the material is kept in the warm standard bath. If we now have a bath, the temperature T

of which is to be measured, the thermometer is brought to thermal equilibrium with this

bath and the property value P is measured. The temperature T of this bath is then defined

by the relation

T = T1 +{[P −P(T1)]/ [ P(T2) − P(T1)]} (T2 – T1) (VII.1.1)

The temperature of a bath defined in this way will depend both on the property that is

measured and the material of the thermometer. For example, if we take the property to be

the resistance of a metallic wire which forms the thermometer, there is no justifiable

reason to expect that the way the resistance changes with temperature will be the same for

wires of different material. This implies that temperature defined in this fashion will not

be absolute in the sense that measurements made with different material and using

different properties will generally give different values for the temperature of the same

bath. This will create chaos.

To define an absolute temperature, we have to look for a device and a property such that

the variation of the property with temperature will be independent of the working

substance used. The device may only be a theoretical one that will not be possible to be

realized in practice. Still, such an absolute temperature scale will be useful since it

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provides a benchmark against which the actual performance of practical thermometers

can be tested.

2. Absolute temperature

The Carnot engine is a heat engine in which the working substance undergoes a cycle of

changes in its thermodynamic state. In each cycle it absorbs a quantity, Q1, of heat from a

warm reservoir and delivers a smaller quantity, Q2, of heat to a cold reservoir. The

difference W = (Q1 − Q2) is available as work. The important feature of the Carnot cycle

is that its efficiency, η, defined by the relation

η = W/Q1 = (1 − Q2 / Q1) (VII.2..1)

is independent of the working substance in the heat engine or the nature of the property

used in converting heat to work in the heat engine . This is a consequence of the second

law of thermodynamics. So the efficiency of a Carnot engine can be used to define an

absolute temperature scale. If we take the temperature of the standard cold reservoir as

T2, and the warm reservoir has a temperature T, we may define the efficiency by

η = (1 − T2 /T) (VII.2.2)

The coldest reservoir that one can use must have a temperature T2 = 0 since the

efficiency of any engine cannot be greater than 1. This is called the Absolute Zero of

Temperature and all bodies must have a positive temperature on this scale. A scale of

temperature defined thus is called the absolute or Kelvin scale.

2. 1. Ideal Gas Scale

While it is nice to be able to define such an absolute scale, is there any practical way of

realizing the Kelvin scale? Here the ideal gas laws come to our help. Boyle and Charles

performed experiments on the pressure, P, of a given volume, v, of a gas in different

warm baths. They found that if the gas is at low pressure, the product of the pressure and

volume, Pv, remains constant in a given bath. This quantity increases as the bath

becomes warmer. One can therefore take a mole of a gas at low pressure and determine

the product PV (here V is the volume of 1 mole of the gas) in different baths. One can

define a practical temperature scale using this product PV. If we take the temperature of

a bath of melting ice as 0 and temperature of water boiling under atmospheric pressure as

100,1 we may define a gas scale of temperature by

T = {[PV(T) − PV(0) ] / [PV(100) −PV(0)]} 100 (VII.2.3)

This relation implies that on this scale

PV = C + RT (VII.2.4)

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The above constant, C, can be written as RT0. In such a case,

PV = R (T+T0) (VII..2.5)

Experiments show that (a) in the limit of low pressure all gases show the same behaviour

and (b) the constants R and T0 have the same values for all gases. The constant R has a

value 8.316 Joules/K and T0 has a value 273.15. We may now define a new scale of

temperature, called the Ideal Gas Temperature Scale, in which the ice point temperature

T2 ig = 273.15 and the temperature of boiling point water under atmospheric pressure T1 ig

= 373.15. This is also called the Celsius Scale. We may use any gas as our thermometric

substance and measure the pressure at a constant volume of the gas. The temperature of a

bath deduced from such a measurement, in the limit of pressure of the gas tending to zero,

will be the same. Also it will be independent of the gas. The relation

PV = RTig (VII.2.6)

is called the Charles law. At high pressures, the density of the gas becomes high and

interatomic interactions play a role in causing deviations from Charles law.

2. 3. Relation of ideal gas scale to the absolute scale

How does the ideal gas scale of temperature relate to the absolute temperature scale

based on Carnot cycle? If we use an ideal gas as the working substance in the Carnot

engine and calculate from Charles law the heat, Q1, absorbed at the warm temperature Tig

and the heat, Q2 , rejected at the cold temperature T2 ig we find

Q2ig/Q1ig = T2ig/Tig (VII.2.7)

And hence,

η = (1 − T2ig/Tig) (VII.2.8)

Comparing the equations (VII.2.2) and (VII.2.8), we find that the ideal gas temperature

Tig should be proportional to the absolute temperature TK. It is convenient to choose the

constant of proportionality to be unity. Hence we see that the ideal gas temperature scale

coincides with the absolute temperature scale. So the absolute temperature scale is

realizable in practice using a gas thermometer filled at very low pressure (i. e. in the limit

P tending to zero).

The ideal gas thermometer is called a primary thermometer. In actual practice a

gas thermometer can be filled only at a finite pressure and there will be small deviations

from Charles law. But one can apply corrections for temperatures measured by the gas

thermometer and obtain the temperature on the absolute scale. These corrections will

depend on the nature of the gas used.

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In practice one cannot use the gas thermometer in experiments. One will have to use

secondary thermometers that are small in size and weight and that are more convenient

for measurement and control. There are a variety of such thermometers available. These

are calibrated at a few fixed points using certain interpolation formulae as agreed upon by

International convention. We shall describe the International Temperature Scale currently

in use.

3. International temperature scale (ITS90)

The ITS90 was adopted by the International Commission on Weights and Measures in

1989. This scale supercedes the practical temperature scale of 1968 and the provisional

0.5 to 30 K Temperature Scale of 1976. The temperature measured on the ITS90 scale is

written as T90. The ITS 90 is defined in different temperature ranges as follows:

Between 0.65 to 5 K, T90 is defined in terms of vapour pressure of 3He and

4He. The

temperature T90 is represented in terms of the vapour pressure by the following equation:

9

T90 = A0 + Σ Ai{ [ln(P) − B]/C}i (VII.3.1)

i = 1

The vapour pressure P is in Pascals. Table VII.1 gives the constants for 3He and

4He and

the temperature range in which the constants are valid is indicated.

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Between 4.2 K to triple point of Ne, a 4He gas thermometer calibrated at three fixed

points (at the triple point of Ne, triple point of e-Hydrogen, and one other temperature

between 3 and 5 K as determined by vapour pressure thermometer) is used. The equation

to be used to obtain T90 is

T90 = a + bP +cP2

(VII.3.2)

Here P is the pressure of the Helium gas. The constants a, b and c are determined from

the calibration at the above three temperatures.

Between the triple point of e- hydrogen and melting point of silver, a platinum

resistance thermometer calibrated at specified sets of defined fixed points using specific

interpolations defines T90. We define W(T90) by the ratio R(T90)/R(273.16) where R(T) is

the resistance of the Pt thermometer at temperature T. The thermometer should be made

of pure strain-free Platinum wire satisfying at least one of the following two conditions:

W (MP of Ga) ≥ 1.11807 (VII.3.3)

and W (TP of Hg) ≥ 0.844235 (VII.3.4)

If it is to be used till the freezing point of Ag it must also satisfy the condition

W (FP of Ag) ≥ 4.2844 (VII.3.5)

From 13.8033 to 273.16 K the temperature can be calculated from W (T) by the relation

15

T90 = B0 + Σi Bi[{W1/6

(T) − 0.65)/0.35]i

(VII.3.6)

i=1

The constants Bi are listed in Table VII.2. Table VII.3 gives the temperature of a few

fixed points.

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4. Secondary thermometers

A secondary thermometer is a device of low thermal capacity having a property, which

changes with temperature. It should have a well-characterized and reproducible response

to variations in temperature. It will be useful if the response can be fitted to a well-

defined equation containing a few parameters that can be obtained by calibrating the

thermometer at a few fixed points. The sensitivity of the thermometer (i.e. the change in

signal for one degree change in temperature) should be high. At the same time the

thermometer should respond quickly to changes in temperature. This is achieved by

making the thermal capacity of the thermometer small and having a good thermal contact

with the object, the temperature of which is to be measured.

For cryogenic thermometry it is necessary to have long leads connecting the sensor at

low temperature to electrical leads at room temperature. One must take adequate

precautions to see that the heat leaking through the leads is small. Otherwise the

temperature indicated by the thermometer will be higher than the actual temperature of

the object. One should use as thin and as long leads as possible to increase the thermal

resistance of the leads. It will be good to anchor the leads to a point that is at the

temperature of the object at low temperature. Then all the heat from room temperature

will go to the cold object and ultimately to the refrigerating medium used to cool the

object. Heat leak to the thermometer will become small. This is indicated in Figure

VII.1.

The thermometer leads from the feed through (FT) at the room temperature flange is

wrapped round the specimen chamber and fixed to it with a thin layer of GE varnish

before being connected to the thermometer. Such anchoring is necessary in all

thermometric measurements at low temperature.

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5. Resistance thermometers

One of the most widely used techniques for measurement of temperature is resistance

thermometry. In this technique the resistance of a material is measured and the

temperature is deduced from the value of resistance. One can have materials with a

positive temperature coefficient (PTC) of resistance. In these materials the resistance

increases with increase in temperature. This is usually the behaviour of metals and

metallic alloys. The semi-conducting materials, on the other hand, have a negative

temperature coefficient (NTC) of resistance. In these materials, the resistance increases

(often by a few orders of magnitude) as the sensor is cooled. In the case of PTC sensors

one uses a constant current source to drive a constant current through the material. The

voltage across the sensor is measured with a digital voltmeter. As the temperature falls

the power dissipated in the sensor will decrease. With NTC materials, it is usual to use a

constant voltage across the resistor and measure the current. The power dissipated is

inversely proportional to the resistance. So, with this method of measurement, the power

dissipated will decrease in NTC sensors as the sensor cools.

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5. 1. Self Heating

Why are we worried about the power dissipated in the sensor? This power will have to

be conducted away to the cold object, the temperature of which is being measured. If the

thermal resistance of the contact between the thermometer and the object is ρcontact and P

is the power dissipated in the sensor during measurement, there will be a temperature

difference ∆T between the thermometer and the object given by

∆T = ρcontact P (VII.5.1)

If the object temperature is T, the temperature recorded by the thermometer will be T+∆T.

This is called the self-heating effect. The contact resistance increases as the temperature

falls and varies as T−3

below 1 K. It is therefore necessary to keep P small enough so that

∆T is a small fraction of T. The lower the temperature the smaller should be the value of

P. That is the reason for using a constant current mode of measurement with PTC sensors

and a constant voltage mode of measurement with NTC sensors. The power dissipated

depends on the square of the current while the measuring signal will be proportional to

the current. It is therefore possible to choose a current value that will give a large enough

signal to measure the temperature accurately and that, at the same time, will keep the

power dissipated small enough to make the error ∆T smaller than a pre-assigned value.

5. 2. Two Wire and Four-Wire Measurement:

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Figures VII..2(a) and 2(b) show the connections for a two-wire and a four-wire

measurement of the resistance of the sensor. In the two-wire measurement the DVM

measures the voltage across the resistance thermometer and the current leads. So the

resistance measured includes the resistance of the current leads, which will vary with

temperature in a manner different from the behaviour of the resistance thermometer.

Unless the resistance of the current leads is negligibly small compared to the resistance of

the thermometer, the measured temperature will be in error.

In the four-wire measurement the current and voltage leads are connected to the

terminals of RT. So the DVM measures only the voltage across RT and the resistance of

the current leads does not enter into the measurement.

5. 3. AC Measurement:

One can also measure the resistance of RT by AC methods using either a bridge

circuit or a lock in amplifier. This involves expensive instrumentation and is justified

only if one requires a very high sensitivity in measurement.

5. 4. Platinum resistance thermometer (PRT)

The platinum resistance thermometer is widely used in the temperature range 20K to

room temperature and above. The thermometer is made of a thin, high purity wire of

platinum mounted strain-free and encapsulated in a ceramic tube or a glass tube. It comes

with two leads. The PRT has a diameter of about 2 mm and a length varying between 5

to 20 mm. For four-wire measurement the voltage and current leads will have to be

soldered to the two leads of the PRT. The resistance thermometer usually has a nominal

resistance of 100 Ohms at 273.15 K. For such a thermometer the sensitivity is roughly

about 0.4 Ohm/K from 40 K to 500 K. Below 30 K the sensitivity falls off steeply. The

temperature variation of resistance is shown in Figure VII. 3.

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If the thermometer is calibrated, its accuracy in measuring temperature is around 5 to 10

mK and reproducibility is also of the same magnitude. The response time of the

thermometer depends on (a) its mass and (b) the temperature. The response time is a few

seconds at low temperature and increases as the temperature increases. The excitation

current is usually 1 mA, which will give a self-heating power of 100 microwatts at 273 K.

The Platinum thermometer can be used above 50 K in magnetic fields as the magneto-

resistance of platinum causes only an error of a few per cent in the measurement of

temperature.

5. 5. Rhodium-Iron resistance thermometer

The temperature variation of resistance of Rhodium-iron alloy depends on its

composition. It is possible to choose a composition for which the resistance increases

monotonically in the range 1.4 to 300 K as the temperature increases. Thermometers are

made either with a thin film of Rh-Fe alloy or with a thin wire. Because of the small

thermal capacity in the former case, the response time is much shorter (of the order of a

few milliseconds at 4.2 K to about twenty milliseconds at 300 K) than the response time

(a few seconds) with the wire wound thermometer. The sensitivity is high from 100-300

K. Below 100 K the sensitivity drops till 30 K. The sensitivity rises again to a high value

below 10 K. This thermometer is unsuitable for measurement in magnetic fields below

77 K.

5. 6. NTC Resistance Thermometers

5. 6. 1. Doped Germanium resistance thermometer

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Germanium (Ge) is a semi-conductor and appropriate doping can alter its electrical

conductivity. The resistance increases sharply as the temperature is reduced. Various

models are available with different suppliers, for use in the temperature range 0.05 K to

30 K. The rapid increase in sensitivity below 4.2 K makes it well suited for sub-milli

Kelvin control of temperature. A typical resistance temperature curve for a GRT is shown

in Figure VII.4.

It is seen that above 30 K the sensitivity of the thermometer becomes poor. It has to be

used with a constant voltage excitation. At 0.5 K the excitation voltage will be a few tens

of microvolts and this is increased to 10 mV at 100 K. This excitation voltage is chosen

so that the self-heating power at 4.2 K is about 0.1 µW and at 0.5 K is about 0.1 pico-

Watt. Typical thermal response time is a few hundred milliseconds at 4.2 K and a few

seconds at 77K.

5. 6. 2. Cernox Thermometers

These are ceramic oxides with a negative temperature coefficient of resistance. They

are useful in the temperature range 1.4 to 300 K. These thermometers are characterised

by a very low magneto-resistance and so are useful to measure temperature in the

presence of high magnetic fields. These are used with constant voltage excitation of a

few millivolts such that the self-heating power is about 10 µWatt at 300 K and 0.1 µW at

4.2 K. The thermal response time is a few milliseconds in the range 0.3 to 4.2 K. Figure

VII.5 shows the resistance temperature graph of commercial Cernox thermometers.

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5. 6. 3. Other NTC resistance thermometers

Carbon glass sensors, which consist of carbon fibres trapped in a glass matrix, can be

used from 1.4 to 300 K. They have a negative temperature coefficient of resistance.

Below 10 K they have a high sensitivity. However above 100 K their sensitivity falls

below 1Ohm/K. Above 100 K they can only provide rough temperature measurement to

an accuracy of 0.1 K. They have a low magneto-resistance, this being negative below

20K. They can be used in magnetic fields as high as 19T and the correction for the

temperature amounts only to a few per cent.

Ruthenium oxide sensors are thick film thermometers. They are useful in the range 50

mK to 30 K. The magnetic field dependence of resistance is small. Allen-Bradley carbon

resistors have been used for thermometry. They are inexpensive. But they need frequent

calibration.

6. Diode thermometers

At a constant current, the voltage across a forward biased p-n junction diode changes

with temperature. This property is used in diode thermometry. The advantage of diode

thermometers is their sensitivity (change in forward bias voltage for unit change in

temperature) is large and nearly constant from 300 K down to about 25 K in the case of Si

diodes and 40 K in the case of GaAs diodes. Below 25 K in Si diodes and 40 K in GaAs

diodes, the forward voltage increases rapidly as the temperature decreases.

Figure VII.6 Forward voltage of a Si diode and a Ga-As diode as a function of

temperature at constant current.

The forward voltage as a function of temperature at a constant current is shown in

Figure VII.6 for both Si and GaAs diodes. Si diodes are relatively inexpensive. Though

they are less sensitive than GaAs diodes they are more stable. Above 1 K one can

achieve an accuracy of about ± 25 mK in temperature measurement. The excitation

current is 10 µA. Problems can arise if there is an AC component of current from the DC

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source. One should take precautions like proper electrical shielding and grounding to get

precise measurements. The GaAs diodes can be used in moderate magnetic fields.

7. Thermocouples

Thermocouples have been used often in the past for the measurement of cryogenic

temperatures. They are inexpensive. When two dissimilar metals A and B are joined

together and the two junctions are maintained at different temperatures T1 and T2 an

electromotive force is generated which can be measured on a digital voltmeter. The

typical measurement arrangement is shown in Figure VII.7.

Figure VII.7: A and B are wires of two dissimilar metals joined together to form two

junctions maintained at temperatures T1 and T2.

The open ends of A are connected to the terminals of a DVM.

If T1 is different from T2 the DVM indicates an emf in millivolts. This is called the

thermo-emf. The thermo-emf is a function of temperature difference (T1 − T2) provided

the junctions of leads A and A’ to the terminals of the DVM are at the same temperature.

If T2 is a temperature of a reference bath such as melting ice then one can measure the

unknown temperature T1. Usually the reference bath is dispensed with. The open ends of

A and B are connected to the DVM. But at the junction to the DVM a resistance

thermometer measures the temperature and produces an appropriate voltage by a bridge

circuit.

Figure VII. 8: Thermo-emf of standard thermocouples with

the reference junction at 273.15 K

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There are three standard thermocouples used in the range of cryogenic temperature.

These are type E (chromel-constantan), type K (chromel-alumel) and type T (copper-

constantan). In Figure VII.8 the thermoelectric emf of these standard junctions are

plotted in millivolts against temperature T1, taking the reference temperature to be that of

melting ice (273.15 K). The slope of the curve gives the sensitivity. We see that the

curves flatten out at the low temperature end. The sensitivity falls at low temperature and

so these thermocouples are not usable below 30 K. For example the thermoelectric power

at 20 K for E, K and T type thermocouples are 8.5, 4.1, and 4.5 µV/K.

Since the wires find themselves in a region where temperature gradient exists, it is

essential that the wires A and B must be homogeneous. Otherwise the temperature

gradient along the length of the thermocouple wires will produce an emf of its own. The

Gold- (0.7 at %) Fe – Chromel thermocouple is suited for temperatures below 30 K as its

thermo-electric power remains high at 15 µV/K above 10 K.

One can measure the temperature to an accuracy of about 1 K. Relative changes in

temperature can however be measured more accurately. The advantage of thermocouple

thermometry is the low response time of the thermometer.

8. Capacitance thermometers

The dielectric constant of strontium titanate shows an appreciable variation with

temperature. A capacitance of a few nano-farads made with this material as the dielectric

medium can be used as a thermometer below 100 K. The capacitance will have to be

measured by an AC bridge with about a few volts of excitation. The disadvantage of

these thermometers is that the calibration changes after thermal cycling. They have to be

re-calibrated frequently. The advantage of the capacitance thermometer is that it is totally

insensitive to magnetic fields. The capacitance thermometer is useful for controlling

temperature in the presence of magnetic fields. Their thermal response time is high, of

the order of minutes.

9. Magnetic susceptibility thermometer

Temperatures of a few tens of a milliKelvin can be obtained either by adiabatic

demagnetization of a paramagnetic salt or with the help of the dilution refrigerator.. For

the measurement of such low temperatures the magnetic susceptibility thermometer can

be used. The paramagnetic susceptibility of a dilute system of of magnetic atoms varies

with temperature as

χ = C / T (VII..9.1)

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This is known as the Curie law. In a solid, two effects cause a change in the behaviour

of the susceptibility represented by Curie’s law. One is the exchange interaction between

neighbouring magnetic atoms, which cause the magnetic moments of the atoms to

become ordered below a certain temperature leading to ferro-, antiferro- or ferri-

magnetism. This interaction drops off rapidly as the distance between the neighbouring

magnetic atoms increases. Secondly the degenerate levels of the ground state of the free

atom are split by crystal field effect.

The paramagnetic salt should be in good thermal contact with the object the

temperature of which is to be measured. The magnetic susceptibility is measured by

using a Hartshorne bridge or a ratio transformer system. Cerium magnesium nitrate is the

thermometric substance commonly used below 1 K since its magnetic ordering

temperature is 4 mK. The other material is Pd containing a few parts per million of iron

atoms. The spin freezing temperature of this material is 0.1 mK and it has a giant atomic

magnetic moment of 10 Bohr magnetons.

10 . Vapour pressure thermometry

The pressure exerted by the saturated vapour over the liquid surface is a definite

function of temperature and hence can be used to measure the temperature of the liquid.

In fact, in the International Scale of Temperature (ITS90), the vapour pressure of 3He and

4He are used for defining the temperature scale between 0.65K and 5K. With a good

pressure measuring arrangement, the vapour pressure thermometer is an excellent

secondary standard, since the temperature response depends on the physical property of a

pure element. The vapour pressure is expressed by semi-empirical formulae with fit

coefficients. The vapour pressure equations for many common cryogenic fluids are

given in Table VII.4 and the constants in Table VII.5.

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The different fixed points of common vapour pressure thermometers are given in Table

VII.6.

The vapour pressure thermometer is useful for temperature measurement in the range

from the triple point to the critical point of the liquid. One of the important advantages of

vapour pressure thermometer is the extreme sensitivity in the range over which they can

be used. The disadvantage is that it is useful only over a limited temperature range. The

thermometers are most accurate in the range of the normal boiling point of the liquid

chosen. The constants for the vapour pressure equations are given in Tables VII.5 and

VII.6.

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The apparatus for vapour pressure determination is quite simple. There are many

variations of vapour pressure thermometers, but one described by Scott is shown in

Figure VII.9. The copper bulb having the liquid is connected to an accurate mercury

manometer through a thin walled vacuum jacketed stainless steel tube and a coiled copper

tubing. It should be obvious that the tubing between the bulb and manometer should

nowhere be colder than the bulb since this can cause refluxing and the pressure readings

will be low.

Also, the gas purity is quite important. With Hydrogen, the ortho / para ratio is an

important parameter due to the strong dependence of the vapour pressure on this

composition. In the case of helium, hydrogen is the possible source of impurity, since all

the other impurities will be solidified. As mentioned earlier, the vapour pressure

thermometry is quite sensitive. It also has good response and is not affected by magnetic

fields and does not need calibration.

11. Conclusion

There are other thermometric techniques like noise thermometry and nuclear orientation

thermometry which are outside the purview of the book. Since temperature measurement

is an important component of any low temperature measurement one must pay special

attention to thermometry.

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REFERENCES

1. Thomas M. Flynn, “Cryogenic Engineering”, Mercel Dekker Inc., N.Y 1997.

2. Randall F Barron, “Cryogenic Systems”, 2nd

edition, Oxford University Press,

New York, 1985.

3. Scott, R. B., “Cryogenic Engineering”, D. Van Nostrand Co., Inc., Princeton, New

Jersy, 1959.

4. McClintock, M., “Cryogenics”, Reinhold Publishing Corp., New York, 1964.

5. Guy K. White, “Experimental Techniques in low temperature Physics”, 3rd

edition, Oxford University Press, New York, 1979.

6. A. C. Rose-Innes, “Low Temperature Technique”, The English Universities Press

Ltd., London, 1974.

7. S I Data sheets.

8. Lab Facility, U. K.

9. Lakeshore Cryotronics.