ENGINEERING METALORGY AND MEASUREMENT

338  ENGINEERING METROLOGY AND MEASUREMENTS

of inertia of the coil is most important. Further, sensitivity of the oscillograph is a function of
the number of turns in the coil. It is essential to keep the mass moment of inertia at a minimum
level; thus, the actual design is a compromise.

13.8.5  XY Plotters

The XY plotters generate Cartesian graphs, which are obtained by two DC inputs, one in X and
the other in Y axis. It basically consists of two self-balancing potentiometers, one to control the
position of the paper and the other to control the position of the pen. In some XY plotters, the
paper does not move while two self-balancing potentiometers are used to obtain the movement
of the pen in the X and Y directions.

In XY plotters, the output is generated by plotting one emf as a function of the other emf.
Further, the emf, which is the output signal of transducers, may be a value of displacement,
force, pressure, strain, or any other parameter. Thus, by transducing appropriate parameters,
plots for any combination of parameters may be obtained. A pair of servo systems enables the
movement of the recording pen in both the axes. The paper chart remains stationary.

A QUICK OVERVIEW

• Depending on the information sensed and • A null-type device works on the principle of

delivered by the sensor, transfer efficiency is maintaining a zero deflection by applying an

defined as follows: appropriate known effect that opposes the one

Transfer efficie ncy = IIsd eenl generated by the measured quantity. This type
of transducer requires a detector capable of
detecting an imbalance and a means to restore

Here, Idel is the information delivered by the a balance either manually or automatically. A
pickup device and Isen is information sensed by deflection-type transducer works based on the
the pickup device. principle that the measured quantity produces

• Active transducers are of a self-generating type a physical effect that stimulates an analogous

wherein they develop their own voltage or current effect in the opposite direction in some parts of

output. They do not need any auxiliary power the measuring instrument. There is an increase

source to produce output. Passive transducers in the opposing effect until a balance is restored,

derive power required for transduction from an at which stage the measurement of deflection is

auxiliary source of power. A part of the power carried out.

required for generating the output is derived • Reflected frictional amplification, reflected

from the physical quantity being measured. inertial amplification, amplification of backlash

• When a measuring device measures and and elastic deformation, tolerance, and

transforms a non-electrical variable into an temperature problems are the major problems

electrical variable, it is called a transducer. associated with the mechanical systems.

A thermocouple, which is used to measure • Telemetry is measurement made at a distance,

temperature, radiation, and heat flow, is an as suggested by its name. Distant measurement

example of a transducer. If an electrical quantity is usually performed using radio, hypersonic,

is transformed into a non-electrical quantity, it is or infrared systems and hence referred to as

termed an inverse transducer. wireless data communications. Data can also be

TRANSDUCERS  339

communicated via telephone, computer network, deflection plates in order to use them extensively
optical link, etc. for measurement applications.
• In most of the instruments, the permanent- • Synchronization is a must in order to ensure a
magnet moving-coil meter movement, which stationary image, since the input voltage is a
is known as D’Arsonval movement, is the basic time-dependent function irrespective of the type
movement. It is a current-sensitive device and of sweep employed. Synchronization is essential
hence current will flow, regardless of whether it to avoid drifting of the image across the screen.
is used as a voltmeter or a current meter. • In order to obtain bright and dark shades in the
• A cathode ray oscilloscope (CRO) is probably fluorescent image generated by electron beams,
the most popular terminating device, which positive and negative voltage can be applied
finds various applications in mechanical correspondingly to the grid of the cathode
measurements. A CRO is a voltage-sensitive ray tube. In order to modulate the brightness
device that is used to view, measure, and analyse further, voltage from an external source can be
waveforms. used. This is achieved by providing a terminal
• Due to poor sensitivity of the CROs, it is essential in the front panel or a connection at the back
to provide amplification of the signal (using an of the instrument. This is termed intensity or
oscillation amplifier) before it is applied to the Z-modulation.

MULTIPLE-CHOICE QUESTIONS (d) tolerance problems
6. Temperature problems can be limited by
1. Which of the following transducers is a passive
transducer? (a) selection of proper materials
(a) Photovoltaic cell (b) providing temperature compensation
(b) Piezoelectric (c) proper control of temperature
(c) Thermocouple (d) all of these
(d) Thermistor 7. The function of a multiplexer is
(a) mixing and transferring of information
2. Which of the following is an inverse transducer? (b) performing multiple functions
(a) Piezoelectric crystal (c) calibrating telemetry system
(b) Thermocouple (d) attenuation of signals
(c) Capacitive transducer 8. PCM stands for
(d) LVDT (a) pulse code multiplexer
(b) pulse code modulation
3. Thermocouple is (c) pulse character multiplexer
(a) a passive transducer (d) pulse course modulation
(b) an inverse transducer 9. VTVM has
(c) an active transducer (a) high impedance (c) zero impedance
(d) both active and passive transducers (b) low impedance (d) negative impedance
10. Synchronization is required
4. A consequence of backlash is (a) for obtaining a moving image
(a) gain in amplification (b) for amplifying the image
(b) lost motion (c) for not obtaining any image
(c) conditioned signal (d) for obtaining a stationary image
(d) attenuation of signal

5. Zero shift is the result of
(a) temperature variations
(b) backlash
(c) hysteresis

340  ENGINEERING METROLOGY AND MEASUREMENTS

REVIEW QUESTIONS 12. Explain a single-stage electronic amplifier with
a neat circuit.
1. Define transfer efficiency.
2. Classify transducers. 13. What is telemetry? With the help of a neat block
3. Distinguish between the following: diagram, explain the working of a telemetry
system.
(a) Active and passive transducers
(b) Transducers and inverse transducers 14. With the help of a sketch, explain a simple
4. With an example, explain a primary detector D’Arsonval type to measure current or voltage.
transducer stage.
5. Explain null- and deflection-type transducers. 15. Explain the working of a VTVM.
6. List the quality attributes of transducers. 16. With a neat diagram, explain the working of
7. Explain the inherent problems associated with
mechanical systems. mechanical counters.
8. With a chart explain the typical operation of 17. Explain the working of a CRT with a neat figure.
transduction in electrical, electronic, and self- 18. With a block diagram, explain the working of a
generating transducers.
9. List the advantages of electrical transducers. general-purpose CRO.
10. Explain a simple current-sensitive circuit. 19. Explain the unique features of a CRO.
11. With a neat circuit diagram, explain the working 20. Write short notes on the following:
of a ballast circuit. In addition, derive an express-
ion for the same. (a) Direct writing-type oscillographs
(b) Light beam oscillographs
(c) XY plotters

Answers to Multiple-choice Questions

1. (d)  2. (a)  3. (c)  4. (b)  5. (a)  6. (d)  7. (a)  8. (b)
9. (a)  10. (d) 

14CHAPTER Measurement of Force,
Torque, and Strain

After studying this chapter, the reader will be able to

• understand the basics and describe methods of force, torque,
and strain measurements

• explain the direct method of force measurement
• differentiate between the different types of elastic members

for force measurements
• discuss the different electrical pressure transducers
• elucidate the various types of dynamometers used for torque

measurements
• appreciate the different aspects of strain measurement

systems
• explain gauge factor measurement
• describe temperature compensation

14.1 INTRODUCTION

We all know that force is defined as the product of mass and acceleration, as per Newton’s
second law of motion. Force is a vector quantity whose unit of measurement is Newton (N);
1 N is equivalent to the force required to accelerate a mass of 1 kg at a rate of 1 m/s2, that is, 1
N = 1 kg × 1 m/s2. The standards of mass and acceleration determine the standard of force. It
is a well-known fact that the fundamental unit of mass is kilogram, which is traceable to the
international prototype of mass. The international standard for mass is international kilogram,
which is equivalent to the mass of a cylinder of platinum–iridium maintained at Sevres, France.
Although acceleration is not a fundamental unit, it is derived from two other well-defined
and internationally accepted fundamental quantities: length and time. The acceleration due to
gravity g can be adopted as a suitable standard and is approximately equal to 9.81 m/s2.

Torque is defined as the force, which, besides exerting effects along its line of action, may
also exert a rotating force relative to any axis excepting those intersecting the line of action.
It can also be termed as a couple or twisting force. It is determined by measuring the force at
a known radius r and is expressed as T = F × r. The metric unit of measurement of torque is
Newton metre (N m), which is a force multiplied by the distance of this force from an axis of
rotation. Torque is closely related to the measurement of force, and since force and length that
define torque conform to international standards, separate standards are not required for torque.

342  ENGINEERING METROLOGY AND MEASUREMENTS

14.2  MEASUREMENT OF FORCE

The methods for measuring force can be classified into two basic categories: direct and
indirect. In case of direct methods, a direct comparison is made between an unknown force
and the known gravitational force on a standard mass. For this purpose, a beam balance may be
employed wherein masses are compared. In this case, the beam neither attenuates nor amplifies.
Indirect comparison is made by a calibrated transducer that senses gravitational attraction or
weight. Sometimes, the deformation due to a force applied on an elastic member is measured.

14.2.1  Direct Methods

Direct methods involve the comparison of an unknown force with a known gravitational force
on the standard mass. A force is exerted on a body of mass m due to the earth’s gravitational
field, which can be represented by the following equation:

W = mg
Here m is the standard mass, g is the acceleration due to gravity, and W is the weight of the
body.
It is imperative to know the values of mass and acceleration due to gravity accurately in
order to determine the force acting on the body. With the help of an analytical balance, a direct
comparison can be drawn between an unknown force and the gravitational force. The following
section describes the working of an analytical balance.

Analytical Balance

An analytical balance, also known as an equal arm balance, is probably the simplest force-

measuring system. As discussed in Section 14.2, an unknown force is directly compared with a

known gravitational force. Comparison of masses is carried out by attaining some kind of beam

balance by employing a null balance method. It is sufficient to only find out the magnitude

since the unknown force and the

l gravitational force act in directions
Fulcrum parallel to each other. The working
l principle is illustrated schematically

q O dB Line joining in Fig. 14.1.
dG CG knife edge The rotation of the balance arm

is about the knife edge point or

fulcrum O. Figure 14.1 shows the

q W2 balance in an unbalanced condition.
The distance between the fulcrum

W1 WB and the centre of gravity point CG
is dG. Let WB denote the weight of
Pointer and scale the balance arms and pointer; W1 and
arrangement W2 are two weights acting on either

side of the balance. When the two

weights W1 and W2 are equal, angle
q will be zero, and hence the weight

Fig. 14.1  Analytical balance of the balance arms and pointer will

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  343

not influence the measurements.

Deflection per unit unbalance gives a measure of the sensitivity of the balance. The difference

between the two weights, that is, W1 − W2, gives the unbalance. Let this difference be ∆W.

Hence, sensitivity S = (W1 q W2) = q (14.1)
− DW

When the balance is at equilibrium, the following equation is realized:

W1(l cos q − dB sin q) = W2 (l cos q + dB sin q) + WB dG sin q (14.2)

When the angle of deflection is small, sin q = q and cos q = 1. For such small angles of

deflection, Eq. (14.1) can be modified as follows:

W1 (l − dBq) = W2 (l + dBq) + WB dG q

Therefore, q = l (W1 − W2) (14.3)
(W1 + W2) dB + WB dG

Hence, sensitivity S = q W2) = (W1 l WB dG (14.4)
(W1 − + W2) dB +

When in equilibrium, W1 = W2 = W.
l

S = 2W dB + WB dG (14.5)
If balances are constructed such that dB, the distance between the fulcrum and the line joining
the knife edges, is zero, then equation (14.5) becomes as follows:

l (14.6)
S = WB dG

Hence, it can clearly be seen from Eq. (14.6) that the sensitivity is independent of the applied
weights W1 and W2. There may be errors in measurement due to the buoyancy effects of air
exerted on the weights, which can be eliminated through proper care. In addition, to enhance
sensitivity, it is necessary to increase l and decrease WB and dG, which again affect the stability.
Hence, a trade-off needs to be made between the stability and sensitivity of the balance. It is
pertinent to mention here that for optimal performance, the design and operation of the balance
is crucial. The disadvantage associated with an analytical balance is that it necessitates the use
of a set of weights that are at least equal to the maximum weight to be measured. However, it
can be mentioned here that an equal-arm balance system is not appropriate for the measurement
of large weights.

Platform Balance

For applications involving measurement of large weights, a platform balance or multiple-lever
system is preferred. A platform balance is schematically represented in Fig. 14.2.

In a platform balance, two smaller weights, poise weight Wx and pan weight Wy, are used
for the measurement of a large weight W. The initial zero balance can be set by an adjustable

344  ENGINEERING METROLOGY AND MEASUREMENTS

Poise
weight

Beam scale

Adjustable b a
counterpoise W1 W
Tension T
Platform W2

f Pan
weight

Wy

h

Main lever d e
c

Fig. 14.2  Platform balance

counterpoise. The poise weight Wx is set to zero of the beam scale, and then the counterpoise
is adjusted for obtaining the initial balance before applying the unknown weight W on the

platform. For ease of analysis, it can be assumed here that the two weights W1 and W2 are
substituted by W. Since Wx has already been adjusted to zero, the entire unknown weight W is
balanced by the pan weight Wy.
It can be seen that T × b = Wy × a (14.7)

and T × c = W1(f/d)e + W2 × h (14.8)

The linkage proportion can be arranged such that h/e = f/d.

Hence, we have T × c = (W1 + W2)h = Wh (14.9)

It is clear from these discussions that weight W can be placed anywhere on the platform and

its position with respect to the knife edges of the platform is not significant.

From Eqs (14.7) and (14.9), we obtain the following equation:

Wy a Wh (14.10)
b = c

This gives a new equation. (14.11)
ac

W = b h Wy = S Wy

where S is known as the scale multiplication ratio, which is given by another equation:

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  345

ac
S = b h (14.12)

The multiplication ratio gives an indication of the weight that should be applied to the pan
in order to balance the weight on the platform. This means that if the multiplication factor is
100, then a weight of 1 kg applied on the pan can balance a weight of 100 kg placed on the
platform. Let us assume that the beam is divided with a scale of m kg per scale division, then a
poise movement on the y scale division has to produce the same result as a weight Wx placed on
the pan at the end of the beam; hence, Wxy = mya. Therefore, we obtain the following equation:

m = Wx/a (14.13)
The required scale divisions on the beam for any poise weight Wx is determined by this
relationship. The length of the beam scale a is expressed in terms of scale divisions. The beam
is balanced by appropriate combinations of pan weights and an adjustment of the poise weight
along the calibrated beam scale.

14.3  ELASTIC MEMBERS

For determining the applied force, many force-measuring transducers employ various
mechanical elastic members or their combinations. Application of a load or force on these
members causes an analogous deflection. This deflection, which is usually linear, is measured
either directly or indirectly by employing secondary transducers. This displacement is then
converted into an electrical signal by the secondary transducers. The strain gauge is the most
popular secondary transducer employed for the measurement of force. Figure 14.3 depicts the
use of a strain gauge for the determination of applied force.

Load/Force Elastic member Strain gauge Electrical signals

Fig. 14.3  Use of a strain gauge for force determination

The strain gauge operates on a simple principle. When force is applied on an elastic member,
a steel cylindrical rod in this case, the dimensions undergo a change. If the strain gauge is
bonded to the cylinder, the gauge is stretched or compressed, resulting in a change in its length
and diameter. The dimension of the strain gauge changes due to a change in resistance. This
change in resistance or output voltage of the strain gauge gives a measure of the applied force.
Load cells and proving rings that employ strain gauges are the two most common instruments
used for force measurement.

14.3.1  Load Cells

Elastic members are generally used for the measurement of force through displacement
measurement. When an elastic member is combined with a strain gauge and used for the
measurement of force, it is termed as a load cell. In load cells, elastic members act as primary
transducers and strain gauges as secondary transducers. A load cell is used in an indirect method
of force measurement where force or weight is converted into an electrical signal. Load cells
are used extensively for the measurement of force.

346  ENGINEERING METROLOGY AND MEASUREMENTS

F
B

R1 R2

A CV

Strain F R3 R4
gauge R1 D

R2 R3 ei

R4
Fig. 14.4  Strain gauge arrangement for a load cell

A load cell comprises four strain gauges; two of these are used for measuring the longitudinal
strain while the other two for measuring the transverse strain. The four strain gauges are
mounted at 90° to each other, as shown in Fig. 14.4.

Two gauges experience tensile stresses while the other two are subjected to compressive
stresses. At the no-load condition, resistance in all the four gauges will be same. The potential
across the two terminals B and D are same. The Wheatstone bridge is now balanced and hence
output voltage is zero When the specimen is stressed due to the applied force, the strain induced
is measured by the gauges. Gauges R1 and R4 measure the longitudinal (compressive) strain,
while gauges R2 and R3 measure the transverse (tensile) strain. In this case, voltages across
the terminals B and D will be different, causing the output voltage to vary, which becomes a
measure of the applied force upon calibration.

The longitudinal strain developed in the load cell is compressive in nature and given by the
following relation:

F
e1 = − AE

Here, F is the force applied, A is the cross-sectional area, and E is the Young’s modulus of
elasticity.

Gauges 1 and 4 experience this strain. Strain gauges 2 and 3 would experience a strain given
by the following relation:

e2 = − gF
AE

Here, g is the Poisson’s ratio.
This arrangement of mounting of gauges compensates the influence of bending and

temperature. In fact, a complete compensation is obtained if the gauges are mounted

symmetrically.

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  347

L F F V R1 R2
A

1 Pt e0
3
2
4
A R4 R3

l yb

Fig. 14.5  Cantilever beam for force measurement Fig. 14.6  Strain gauge
arrangement for force measurement

14.3.2  Cantilever Beams

A cantilever beam is one of the simple devices used for the measurement of force. One end of
the cantilever is fixed and a force F is applied on the free end, as shown in Fig. 14.5. Four strain
gauges are bonded near the fixed end to measure the strain induced by the application of force.
Two strain gauges are fixed on the top for measuring tensile strain +e and two at the bottom
side for measuring compressive strain −e. The strain developed at the fixed end is determined
using the following equation:

6Fl
e = Ebt2

Here, l is the length of the beam, E is the Young’s modulus of the material, b is the width of
the beam, and t is the thickness of the cantilever.

In Fig. 14.6, strain gauges R1 and R3 measure tensile strain, whereas compressive strain
is measured by R2 and R4. Strains measured by all the four gauges are of equal magnitude.
Apart from the measurement of force, a load cell finds application in vehicle weighbridges and
cutting tool force dynamometers.

14.3.3  Proving Rings

One of the most popular devices used for force measurement is the proving ring. In order
to measure the displacement caused by the applied pressure, a displacement transducer is
connected between the top and bottom of the ring. Measurement of the relative displacement
gives a measure of the applied force. A proving ring can be employed for measuring the applied
load/force, with deflection being measured using a precise micrometer, a linear variable
differential transformer (LVDT), or a strain gauge. When compared to other devices, a proving
ring develops more strain owing to its construction. A proving ring, which is made up of steel,
can be used for measuring static loads, and is hence employed in the calibration of tensile
testing machines. It can be employed over a wide range of loads (1.5 kN to 2 MN).

A proving ring comprises a circular ring having a rectangular cross-section, as shown in Fig.
14.7. It has a radius R, thickness t, and an axial width b. The proving ring may be subjected
to either tensile or compressive forces across its diameters. The two ends between which
force is measured are attached with structures. Four strain gauges are mounted on the walls of
the proving ring, two on the inner walls, and two other on the outer walls. The applied force
induces a strain (compressive) −e in gauges 2 and 4, while gauges 1 and 3 undergo tension

348  ENGINEERING METROLOGY AND MEASUREMENTS

Strain Applied force F +e. The four strain gauges are connected to the bridge circuit,
gauges and the unbalanced voltage caused by the applied force can
t be measured. This voltage is calibrated in terms of force. The
R2 R4 magnitude of the strain is given by the following expression:
R1
R3 1.08FR
e = Ebt2
Applied force F
b The relationship between the applied force and the deflection
caused by the applied force is given by

( )p 4 Fd3

dy = 2 − p 16EI

Here, E is the Young’s modulus, I is the moment of inertia,
F is the force, d is the outside diameter of the ring, and dy is the
deflection.

14.3.4  Differential Transformers

Fig. 14.7  Proving ring An LVDT can be employed in a load cell to measure the applied
force. The working of an LVDT has been discussed in detail

in Chapter 16 (refer to Section 16.7.3). An LVDT can be used in conjunction with a primary

transducer to measure force, pressure, weight, etc. It can generate an AC output voltage as a

function of the displacement of the magnetic core caused by the applied force. The frictionless

movement and low mass of the core provide advantages such as high resolution and low

hysteresis, making the LVDT an obvious choice for dynamic measurement. LVDTs can be

employed as alternatives to strain gauges or micrometers.

14.4  MEASUREMENT OF TORQUE

Measurement of torque is important for the following reasons:
1. It is necessary to obtain load information for the analysis of stress or deflection. In this case,

torque T is determined by the measurement force F at a known radius r using the following
relationship:

T = Fr (in N m)
2. Measurement of torque is essential in the determination of mechanical power. Mechanical

power is nothing but the power required to operate a machine or the power developed by the
machine, and is computed using the following relation:

P = 2πNT
Here, N is the angular speed in resolution per second.
Torque-measuring devices employed for this purpose are popularly known as dynamom-

eters. Dynamometers are used to measure torque in internal combustion machines, small
steam turbines, pumps, compressors, etc.
3. Measurement of torque is important for evaluating the performance characteristics of ma-
chines.
The nature of the machine to be tested determines the kind of dynamometer to be used
for torque measurement. If the machine generates power, the dynamometer employed must

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  349

Observer have the capability of absorbing that power.
These dynamometers are called absorption

Mirror Light source dynamometers, which are particularly useful
for measuring the power or torque developed by

T power sources such as engines or electric motors.

In case the machine is a power absorber, the

T Torque bar dynamometer must have the capacity to drive
it; such a dynamometer is known as a driving

dynamometer. Driving dynamometers are the-

1 refore useful in determining performance

2 characteristics of devices such as pumps and

3 Transparent scale compressors. The third type is the transmission

Transparent index dynamometer. These are passive devices placed

mark and vernier at an appropriate location within the machine or

Slot for stroboscopic effect between machines. They are used to sense torque

Fig. 14.8  Torsion-bar dynamometer at that particular location. These are sometimes
known as torque meters.

14.4.1  Torsion-bar Dynamometer

Elastic deflection of the transmitting element may be used for the measurement of torque,
which can be achieved by measuring either a gross motion or a unit strain. The main problem
associated with either case is the difficulty in reading the deflection of the rotating shaft. A
torsion-bar dynamometer is also known as a torsion-bar torque meter, which employs optical
methods for deflection measurement, as shown in Fig. 14.8.

Calibrated scales are used to read the relative angular displacement of the two sections of
the torsion bar. This is possible because of the stroboscopic effect of intermittent viewing and
persistence of vision. Transmission dynamometers, which employ this principle, are available
in ranges up to 60,000 m kgf and 50,000 r/min, having an error of ±0.25%.

Replacing the scales on disks 1 and 2 with sectored disks, which are alternately transparent
and opaque sectors, and the human eye with an electro-optical transducer, a version having an
electrical output is obtained. When there is no torque, the sectored disks are positioned to give
a 50% light transmission area. The area of proportionality increases with positive torque and
decreases with negative torque, thus giving a linear and direction-sensitive electric output.

14.4.2  Servo-controlled Dynamometer

Torque and speed are measured under actual driving conditions of an automobile engine; tape
recordings of such an exercise of an engine are obtained and then simulated under laboratory
conditions. Engine speed and torque are controlled by two feedback systems. A servo-controlled
dynamometer is schematically represented in Fig. 14.9.

The actual speed signal generated by the tachometer generator, from the dynamometer,
is compared with the preferred speed that is set in the tape recorder. If the actual and the
preferred speeds are not the same, the dynamometer control is automatically adjusted until
they are equal. The load cell on the dynamometer measures the actual torque from the engine,
and is compared with the preferred torque that is set in the tape recorder. If these two values

350  ENGINEERING METROLOGY AND MEASUREMENTS

Speed control differ, then the error signal generated
actuates the engine throttle control in

the appropriate direction. Both torque

Engine control and speed control operate
simultaneously and continuously such
Dynamometer Throttle that they conform to the desired value
control

Tachometer set in the tape recorder.
generator
14.4.3  Absorption Dynamometer
Load cell Actual torque
The Prony brake dynamometer was
Preferred torque + – Error in invented by Gaspard de Prony, a
torque French engineer inventor, in 1821
to measure engine power. A Prony
Recording + brake dynamometer is one of the

Preferred speed – Error in
speed
Actual speed

Fig. 14.9  Schematic representation of a servo-controlled dynamometer simplest, inexpensive, and the most
Arrangement popular absorption dynamometers.
It is a mechanical type of device
L for tightening that depends on dry friction wherein

mechanical energy is converted into
Arm heat.

Torque T = FL As illustrated in Fig. 14.10, a

Prony brake dynamometer comprises

F two wooden blocks that are mounted

Flywheel on either side of the fly wheel in

Wooden blocks diagrammatically opposite directions.
Fig. 14.10  Prony brake dynamometer The fly wheel is attached to the shaft
whose power needs to be determined.

A lever arm is fixed to one block and

the other arm is connected to an arrangement provided to tighten the rope. Tightening of the

rope is performed in order to enhance the frictional resistance between the blocks and the

flywheel.

The torque exerted by the Prony brake is given by the following equation:

T = FL

Here, force F is measured by conventional force-measuring instruments such as load cells

or balances.

The power dissipated in the brake is then calculated by the following equation:

2pNT
P = 60

2pNFL
or P = 60 W

Here, P is the dissipated power in watts, L is the length of the lever arm in metres, N is the
angular speed in revolution per minute, and F is the force in Newton.

Although a Prony brake is inexpensive, it is inherently unstable. It is difficult to adjust or

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  351

maintain a specific load. The following are certain limitations associated with a Prony brake
dynamometer:
1. Due to wear of the wooden blocks, there will be variations in the coefficients of friction

between the blocks and the flywheel. This necessitates tightening of the clamp. This makes
the system unstable, and large powers cannot be measured particularly when used for longer
periods.
2. The coefficients of friction decrease due to excessive rise in temperature, which may result
in brake failure. Therefore, cooling is required in order to limit the temperature rise. Water is
supplied into the hollow channel of the flywheel to provide cooling.
3. Due to variations in coefficients of friction, there may be some difficulty in taking readings
of force F. The measuring arrangement may be subjected to oscillations, especially when the
machine torque is not constant.

14.5  MEASUREMENT OF STRAIN

The problem of determining stresses acting on a body has been an important and interesting
aspect of materials engineering. Prior to the invention of electrical resistance, strain gauge
extensometers were extensively employed for the determination of strain. These were associated
with a number of problems. One of the most important problems was their bulk, which was a
major constraint in its use. Due to lack of precise knowledge of stress conditions of the material
or structure, many engineering problems were solved on a theoretical basis, by employing trial
and error methods and by assuming a large factor of safety.

In 1856, Lord Kelvin established the principle of electrical resistance strain gauges when he
demonstrated that when stress is applied to a metal wire, apart from undergoing changes in both
length and diameter, there will be some changes in the electrical resistance of the wire.

When external forces act on a body, the body is in a condition of stress and strain. Since
direct measurement of stress is not possible, its effects, such as change of shape of the body
or change in length, are measureable, thus providing a known relationship between stress and
strain. If adequate information is available, stresses acting on a body can be computed.

When a force or load is applied to a body, it undergoes some deformation. This deformation
per unit length is known as unit strain or simply strain, denoted by e, and is given by the
following equation:

δl
e= l

Here, dl is the change in the length of the body and l is the original length of the body.
Strain gauges are essentially employed for two different purposes:
1. To determine the state of strain existing at a point on a loaded member for carrying out strain
analysis
2. To act as a strain-sensitive transducer element in the measurement of quantities such as
force, pressure, displacement, and acceleration

Normally, measurements are made over the shortest gauge lengths. The change in length
measured over a finite length does not give the value of strain at a fixed point but rather gives
the average strain over the entire length. A magnification system is essential since the change in

352  ENGINEERING METROLOGY AND MEASUREMENTS

length is over a small gauge length. Two types of strain gauges are employed:
1. Mechanical strain gauges
2. Electrical strain gauges

14.5.1  Mechanical Strain Gauges

The Berry strain gauge extensometer, shown in Fig. 14.11, is used in civil engineering for
structural applications. This gauge was designed by Professor Herman C. Berry of the University
of Pennsylvania in 1910. It is employed for measuring small deformations under linear strain
conditions over gauge lengths up to 200 mm.

The strain obtained is magnified by employing mechanical means. Lever systems are
employed for amplifying the displacements measured over the gauge lengths. Mechanical
strain gauges comprise two gauge points: one is a fixed point and the other is connected to
the magnifying lever. Both points are placed on the specimen. The displacement caused is
magnified by the lever and is indicated in the dial indicator. Strain is determined by dividing
the measured displacements over the gauge length.

Earlier extensometers used a single mechanical lever for obtaining a magnification of 10 to
1. This was sufficient to work on a long gauge length. Recent extensometers, which are used
for short gauge length, employ compound levers (dial gauges) having a higher magnification
of 2000 to 1.

One of the main advantages of a mechanical strain gauge is that it contains a self-contained
magnification system. There is no need to use auxiliary equipment in a mechanical strain gauge.
It is best suited for conducting static tests. The following are some obvious disadvantages
associated with a mechanical strain gauge:
1. Its response is slow due to high inertia, and friction is more.
2. Automatic recording of the readings is not possible.
3. It cannot be used for dynamic strain measurements and varying strains.

14.5.2  Electrical Strain Gauges

In electrical strain gauges, a change in strain produces a change in some electrical characteristic

Dial gauge

Lever Fixed point
F
Pivot

Gauge point
connected lever

F Specimen
Gauge length

Fig. 14.11  Berry strain gauge extensometer

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  353

such as capacitance, inductance, or resistance. Magnification of the measured strain can be
attained by employing an auxiliary equipment. The main advantages of measurement of strain
using electrical methods are their high sensitivity and ability to respond to dynamic strains. The
following are the advantages of these strain gauges:
1. They are simple in construction.
2. Strain gauges can be calibrated in terms of quantities such as force, displacement, pressure,

and acceleration.
3. They are very sensitive.
4. Linear measurement is accomplished.
5. They provide good output for indicating and recording purposes.
6. Strain gauges are inexpensive and reliable.

There are two types of resistance strain gauges: unbonded and bonded.

Unbonded Resistance Strain Gauges

In case of unbonded resistance strain gauges, the electrical resistance element or the grid is not
supported. A fine wire is stretched out between two or three points, which may become part of
a rigid base that itself is strained, as shown in Fig. 14.12.

Fixed base

R4 R1 F R1 R2
Pins R3 e0 R3

R2 R4

Fig. 14.12  Unbonded resistance strain gauge

The resistance strain gauge shown in Fig. Insulating
14.12 can be used to measure compressive material
strain as it is preloaded. The four resistance
wires are connected in such a manner that Wire grid
they act as a full bridge. Unbonded strain
gauges are used more often as elements of X Assembled gauge
force and pressure transducers, and also in Y
accelerometers. They are seldom used for
strain measurement. Y
X
Bonded Resistance Strain Gauges Fig. 14.13  Exploded view of a bonded resistance

When a strain gauge, which is an appropriately strain gauge
shaped piece of resistance material, is bonded
to the surface of the material to be tested, it
is known as a bonded strain gauge. As shown
in Fig. 14.13, a thin wire in the form of a grid
pattern is cemented in between thin sheets of

354  ENGINEERING METROLOGY AND MEASUREMENTS

insulating materials such as paper or plastic. The strain gauge may also be a thin metal foil. The
gauges are bonded to the surface under study using a thin layer of adhesive, and waterproofing
is provided by applying a layer of wax or lacquer on the gauge. The strain experienced by the
grid and the surface under study to which the grid is bonded will be the same. The gauge is
highly sensitive in the axial direction, and in the transverse direction strain occurs due to the
Poisson’s ratio effect; hence, some small error may be present in the measurement of strain.
However, cross-sensitivity can be completely eliminated by making the ends of the foil gauges
thick. A cluster of three or more strain gauges, known as rosette gauges, can be employed if the
direction of the principal strain is unknown.

Rosette gauges are normally used in the measurement of strain in complex parts. These
gauges comprise three or four separate grids having different orientations and can be cemented
to the surface of the part. The resultant strain can then be gathered and recorded. From the data
gathered, the true magnitudes and directions of the significant surface strains can be computed.

The resistance type of electric strain gauges is the most popular device used for measuring
strain. In this case, electrical resistance of the gauge proportionately changes with the strain it
is subjected to. These gauges exist in the following forms:
1. Wire-type strain gauge
2. Foil-type strain gauge
3. Semiconductor or piezoresistive strain gauge

Wire-type strain gauge  It is made up of a very thin wire having a diameter
of 0.025 mm wound into a grid shape, as illustrated in Fig. 14.14. The grid is
cemented in between two pieces of thin paper with ceramic or plastic backing.
This will facilitate easy handling of the strain gauge. This gauge is further bonded
securely to the surface of the member on which the strain is to be measured using
a suitable cement.

Fig. 14.14  Wire-type Foil-type resistance strain gauge  A foil-type resistance strain gauge has
strain gauge a thickness of about 0.005 mm. It comprises a metal foil grid element on an
epoxy support. For high-temperature applications, epoxy filled with fibre glass
is employed. These gauges are manufactured by printing them on a thin sheet of
metal alloy with an acid-resistant ink and the unprinted portion is etched away.
They offer advantages such as improved hysteresis, better fatigue life, and lateral
strain sensitivity. They can be fixed on fillets and sharply curved surfaces because
they are thin and have higher flexibility. These are also known as metallic gauges.
A foil-type resistance strain gauge is shown in Fig. 14.15.

Fig. 14.15  Foil-type Semiconductor or piezoresistive strain gauge  Semiconductor gauges are cut
resistance strain gauge from single crystals of silicon or germanium. This type of gauge contains precise
amounts of impurities like boron, which impart certain desirable characteristics.
The backing, bonding materials, and mounting techniques used for metallic
gauges are also employed here. When the material onto which semiconductor
gauges are bonded is strained, the current in the semiconductor material changes
correspondingly. When the electrical resistance of the gauge increases due to the
tensile strain, it is known as a positive or p-type semiconductor gauge. When

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  355

the electrical resistance of the gauge

Semiconductor element Copper decreases in response to tensile strain, it is
lead called a negative or n-type semiconductor

gauge. A semiconductor gauge is shown

in Fig. 14.16.

Backing A semiconductor gauge comprises a
rectangular filament having a dimension

Fig. 14.16  Semiconductor gauge of 10 × 0.25 × 0.05 mm. It is essential to
make them as thin as possible because

breaking stresses of the material increase as its cross-sectional area decreases. Without

fracturing the gauge, it can be bent to a much smaller radius of curvature. These have certain

advantages: they show high strain sensitivity and can measure small strain variations accurately.

Semiconductor gauges also possess certain disadvantages:

1. The output obtained in a semiconductor gauge is non-linear in nature.

2. The strain sensitivity of the gauge is temperature dependent.

3. It is more fragile when compared to a wire or foil element.

4. It is more expensive than an ordinary metallic gauge.

14.6  STRAIN GAUGE MATERIALS

Strain gauge sensing materials can be divided into two categories: metallic and semiconductor
materials. The following are the five most popular metals used in the manufacture of strain
gauges:

Constantan It is an alloy of copper and nickel having a low and controllable temperature
coefficient. It finds applications in static and dynamic measurements.

Nichrome  It is a nickel–chrome alloy that finds applications in static and dynamic
measurements.

Dynaloy  It is made up of nickel and iron, which has a high gauge factor, and exhibits high
resistance to fatigue. It can be used for dynamic strain measurements.

Stabiloy  It is a modified nickel–chrome alloy. It has a wide compensation range, from
cryogenic to elevated temperatures, and good fatigue life.

Platinum alloy  It is an alloy of platinum and tungsten and displays unusual stability and
fatigue life at elevated temperatures. It is used for dynamic and static tests up to a temperature
of 800 and 650 °C, respectively.

A specially processed silicon crystal, which is cut into filaments, is used for manufacturing
semiconductor gauges. The filaments exhibit either p (positive) or n (negative) characteristics.
When compared to metallic sensing elements, the gauge factor is much higher in semiconductor
materials. Semiconductor materials are highly sensitive and provide a high output.

Resistances of commercially available strain gauges vary from 60 to 5000 Ω. However, the strain
gauge of 120 Ω is considered to be a standard because most of the commercially available strain-
measuring equipment are designed for 120 Ω. The safe current carrying range is between 25 and
50 mA. If stress distribution of the specimen is reasonably uniform, then a narrow gauge of 10–

356  ENGINEERING METROLOGY AND MEASUREMENTS

30 mm length can be used. For high strain applications, gauges of shorter length can be employed.
Selection of grid materials is important and is based on a compromise of the following

desirable characteristics. The grid materials should have all or many of the following
characteristics:
1. High gauge factor
2. High resistivity
3. Low temperature sensitivity
4. High electrical stability
5. High yield point
6. High endurance limit
7. Good workability
8. Good solderability or weldability
9. Low hysteresis
10. Low thermal emf when joined with other materials
11. Good corrosion resistances

14.7  BACKING OR CARRIER MATERIALS

Backing materials provide support, dimensional stability, and some mechanical protection for
fragile and delicate strain-sensing elements. Basically, two types of carrier materials are used.

Permanent carriers  In addition to supporting the gauge, permanent carriers provide
electrical insulation between the grid and the surface of the part under study. These carriers are
manufactured from organic materials. They are thin and flexible enough to sustain mechanical
contact with the specimen irrespective of the surface contour, temperature gradient, or transient
conditions.

Temporary carriers  Organic carriers may not be appropriate for certain environmental
conditions. In such cases, temporary carriers are employed. Gauges that are used for high-
temperature applications employ temporary carriers, which provide temporary backing. The
backing is removed once the grid is mounted. The advantage of using temporary carriers is that
even though there is an increase in specimen stiffness, there is an improvement in mechanical
and thermal contacts. The following are the desirable characteristics of a backing material:

1. The backing material should be very thin.
2. It should have high mechanical strength so that it is strong enough to transmit force from the

structure under study to the sensing resistance wire.
3. It should have high dielectric strength, that is, it should be an insulator of electricity.
4. The backing material should not absorb humidity, that is, it should be non-hygroscopic.
5. It should be compatible with the adhesive material used to bond it to the structure under

study.
6. It should have minimum temperature restriction, that is, temperature changes should not af-

fect it.

The most commonly used backing materials are thin papers, phenolic-impregnated papers,
epoxy-type plastic films, and epoxy-impregnated fibre glass. Most foil gauges intended for a
moderate range of temperature (−100 to 200 °F) employ an epoxy film backing.

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  357

14.8 ADHESIVES

Adhesives or bonding materials are the most commonly employed agents to bond the strain
gauge to the specimen or the test area in order to transmit strain to the gauge carrier and later
on to the strain-sensing element with true fidelity. They provide some additional insulation.
The strain gauge is fixed on the structure under consideration using an adhesive or a paste. The
adhesives are also called cements. Installation of a strain gauge is probably the most critical
aspect of strain measurement, which is least emphasized. If not properly installed, it may give
erroneous readings, thus degrading the validity of the test. The following are the desirable
characteristics of a strain gauge adhesive:
1. It should have high mechanical strength so that it would have good shear strength to transmit

force from the structure under study to the sensing resistive wire.
2. It should possess high creep resistance.
3. It should have high dielectric strength.
4. It should possess minimum temperature restrictions, that is, temperature changes should not

affect it.
5. It should spread easily and provide good bonding adhesion. It should be easy to apply.
6. It should be non-hygroscopic, which means that the bonding material should not absorb

moisture. If moisture is absorbed, the cement swells and causes large zero shifts.
7. It should go along with the backing material so that the latter is bonded rigidly to the struc-

ture under study.
8. It should have the capacity to be set up fast.
9. It should be economically viable and easily available.

Epoxy and polyamide adhesives are commonly used. Table 14.1 gives the recommended
adhesives with temperature ranges.

14.9  PROTECTIVE COATINGS

In order to prevent damage that may be caused to the relatively delicate gauge installation,
it is essential to use protective coatings. There are chances of mechanical damage, chemical
damage, or damage by other environmental conditions. The following factors may influence
the selection of coatings:
1. Test environment
2. Test duration
3. Accuracy requirements

Table 14.1  Recommended adhesives with The different materials employed for coating strain
temperature ranges gauges are as follows:
1. Micro-crystalline wax from −75 to 70 °C
Adhesive Temperature range (ºF) 2. Silicones up to 420 °C
3. Synthetic rubber coatings, −75 to 220 °C
Nitro cellulose −300 to 180 4. Plastic coatings, which are of two types: vinyl coatings

Cyanoacrylate −100 to 200 (used at the cryogenic temperature range) and epoxy
coatings (used at a higher operating range)
Phenolic −400 to 400 5. Metal foil type

Ceramic −400 to 1000

358  ENGINEERING METROLOGY AND MEASUREMENTS

14.10  BONDING OF GAUGES

The following are the steps to be followed while bonding the gauge to the specimen:
1. Wash hands with soap and water. The working desk area should be kept clean and all related

tools should be washed with a solvent or degreasing agent.
2. The folder containing the gauge should be opened carefully. Bare hands should not be used

to grasp the gauge. Tweezers can be used to hold the gauge. Do not touch the grid.
3. Place the gauge on a clean working area with the bonding side down.
4. Use a proper length, say, about 15 cm, of cellophane tape to pick up the strain gauge and

transfer it to the gauging area of the specimen. Align the gauge with the layout lines. Press
one end of the tape to the specimen, and then smoothly and gently apply the whole tape and
gauge into position.
5. Lift one end of the tape such that the gauge does not contact the gauging area and the bond-
ing site is exposed. Apply the catalyst evenly and gently on the gauge.
6. Apply enough adhesive to provide sufficient coverage under the gauge for proper adhesion.
Some iteration may be required in determining ‘sufficient’ coverage. Place the tape and
gauge back onto the specimen smoothly and gently. Immediately place the thumb over the
gauge and apply firm and steady pressure on it for at least one minute.

14.11  GAUGE FACTOR

The gauge factor is the most important parameter of strain gauges. It is a measure of the amount
of resistance change for a given strain and therefore serves as an index of the strain sensitivity
of the gauge. Mathematically, it is expressed as follows:

DR / R
F = DL / L

Here, F is the gauge factor, ∆R is the change in resistance, and ∆L is the change in length.
Both ∆R and ∆L are due to straining of the gauge along the surface to which it is bonded
by the application of force. R and L are the initial resistance and length of the strain gauge,
respectively.

A higher gauge factor makes the gauge more sensitive, and the electrical output obtained
for indication and recording purposes will be greater. The gauge factor is normally supplied by
the manufacturer and may range from 1.7 to 4, depending on the length of the gauge. Thus, a
means is available for measuring the change of resistance, and hence strain can be determined.
Although a higher gauge factor increases sensitivity, in case of metallic gauges it is limited
owing to the relatively low resistivity of the metals. This limitation can be overcome by using
semiconductor strain gauges, which have gauge factors of the order of ±100 or more.

14.12  THEORY OF STRAIN GAUGES

The change in the resistance value obtained by straining the gauge is attributed to the elastic
behaviour of the material. If an elastic material is strained by applying a tensile load in the axial
direction, its longitudinal dimension increases and the lateral dimension reduces as a function
of the Poisson’s ratio. The resistance of the elastic material is given by the following equation:

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  359

R= rL (14.14)
A

Here, L is the length of the wire, A is the cross-sectional area, and r is the resistivity of the
material.

Assume that the initial length is L having a cross-sectional area of CD2, where C is the

proportionality constant and D is a sectional dimension; C = 1 for a square cross-section and C

= π/4 for a circular cross-section. In order to determine the effect of change in resistance ∆R,

which depends upon the physical quantities of the material, Eq. (14.14) must be differentiated.

dR = CD2(Ldr + rdL) – 2CrDLdD
(CD2)2

[( ) ]1 dD

dR = CD2 Ldr + rdL – 2rL D (14.15)

Dividing Eq. (14.15) by Eq. (14.14), we get the following equation:

dR = dL – 2dD + dr (14.16)
R L D r

Dividing throughout by dL/L, equation (14.16) becomes as follows:

dR/R = 1 – 2dD/D + dr/r (14.17)
dL/L dL/L dL/L

We now conclude the following:

Axial strain = dL/L = ea
Lateral strain = dD/D = eL

dD/D
Poisson’s ratio u = − dL/L

Substituting these values, we get the basic relation for the gauge factor F:

F= dR/R = dR/R =1 + 2u + dr/r
dL/L ea dL/L

This is the basis for a resistance strain gauge.

Here, 1 indicates the change in resistance due to change in length, 2u indicates the change
in resistance due to change in area, and (ddLr//rL)specifies the change in resistance due to the
piezoresistance effect. The piezoresistance effect signifies the dependency of resistivity r on

the mechanical strain.

14.13  METHODS OF STRAIN MEASUREMENT

An electrical resistance-type strain gauge predominantly employs a highly sensitive resistance
bridge arrangement for strain measurement. As can be seen from Fig. 14.17, it comprises four
resistance arms, an energy source, and a detector. The two methods used for strain measurement
are null method and deflection method.

360  ENGINEERING METROLOGY AND MEASUREMENTS

It can be assumed that in order to balance the bridge, the resistances have been balanced,

that is, eBD = 0. To attain this, it is necessary that the ratio of the resistances of any two adjacent
arms and the ratio of the resistance of the remaining arms taken in the same sense are equal;

R1 = R2
R4 R3

In case any one of the resistances change, the meter across BD will indicate a change in the

voltage, which unbalances the bridge. This change in the meter reading can be made use of to

compute the change in resistance. Since the change in resistance is indicated by the deflection

of the meter, this method is known as the deflection method. In this method, readings of the

change in strain can be noted down continuously without any rebalancing. This method is not

accurate because of the tendency of the bridge output to become non-linear with the change in

strain.

In the null method, after each successive change in resistance, the bridge is balanced so that

the meter is brought back to zero, thus nullifying the effect of any change in resistance. The null
method is superior to the deflection method because the strain indicators calibrated under null
balance conditions exhibit linearity and high accuracy.

14.14  STRAIN GAUGE BRIDGE ARRANGEMENT

The arrangement of the resistance bridge shown in Fig. 14.18 is suitable for use with strain
gauges, as the adjustment to null position for zero strain is very easy. In addition, it provides a
means for effectively minimizing or eliminating the temperature effects. Arm 1, shown in Fig.
14.18, includes a strain-sensitive gauge mounted on the test item. Arm 2 contains an identical
gauge mounted on a piece of unstrained material, which is almost a replica of the test material,
placed near the test location in order to maintain the same temperature. The arrangement also
consists of arms 3 and 4, which act as fixed resistors for providing good stability. For balancing
the resistance of the bridge, the arrangement has portions of slide wire resistance D.

B F

R1 R2 G
2
A i1 i2 C V 1 34

i4 i3 D
F
R4 R3 Fig. 14.18  Arrangement of a resistance bridge for strain measurement

D

ei
Fig. 14.17  Basic Wheatstone bridge

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  361

14.15  TEMPERATURE COMPENSATION IN STRAIN GAUGES

One of the most important and critical factors in the use of resistance strain gauges is
temperature sensitivity. Although compensation is provided in the electrical circuitry, for a
majority of the applications, the problem is not eliminated completely. The following three
factors are involved:
1. The gauge is unable to differentiate the strain resulting from the differential expansion exist-

ing between the grid support and the proper grid from the load strain.
2. The resistivity r changes with the change in temperature.
3. The strong magnetic field has an influence on the gauge performance.

Temperature changes affect the sensitivity of resistance-type strain gauges. These strain
gauges are influenced by variations in temperature in the following ways:
1. Temperature variation due to creep affects the gauge factor of the strain gauge.
2. Due to temperature variation, the resistance of the strain gauge element varies.
3. Owing to the differential expansion between the test member and the strain gauge bonding

material, strains may be induced in the gauge.

Compensation may be provided for eliminating the effects of temperature in the following
ways:
1. By the use of an adjacent-arm balancing or compensating gauge
2. By means of self-temperature compensation

14.15.1  Adjacent-arm Compensating Gauge

In Fig. 14.17, arms 1 and 2 are in similar conditions. The initial arm balance is given by the

following relation:

R1 = R3
R2 R4

If the gauges contained in arms 1 and 2 are similar and mounted on identical materials, and

if their shift in resistance ∆Rt due to temperature effect is the same, then the following equation
is obtained:

R1 + DRt = R3
R2 + DRt R4

It can be observed here that the change in temperature has not affected the output, and the

bridge remains in balance. The compensating gauge that is used to only complete the bridge

circuit and to balance the output temperature component is called a dummy gauge.

14.15.2  Self-temperature Compensation

In some situations, the adjacent-arm compensating or dummy gauge may not provide complete
compensation. Sometimes, due to the presence of large temperature gradients in the test
specimens, it may not be possible to maintain identical conditions between two gauges. In such
instances, self-temperature compensation may be employed. A completely self-temperature-
compensated gauge displays zero change of resistance with changes in temperature when
bonded to a specified material. Gauges made from selected melt alloys are the most widely used
self-temperature-compensated gauges. During manufacture, it is essential that the coefficient of

362  ENGINEERING METROLOGY AND MEASUREMENTS

linear expansion of both the gauge and the test material is matched by a suitable heat treatment
process. The matching can only be carried out over a limited range of temperatures. In order
to overcome this limitation, it is essential to calibrate some selected gauges from each batch
produced. Another method is that, during the formation of the grid, two different wires, having
a positive and a negative gauge factor, are connected in series. The advantage is that due to
temperature variation, an increase in resistance in one wire is almost compensated by a decrease
in resistance in the other wire. However, the problem of matching still persists, especially for
use in the case of some specified materials.

A QUICK OVERVIEW

• Force is defined as the product of mass and • Torque and speed are measured under actual
acceleration, as per Newton’s second law of driving conditions of an automobile engine; tape
motion. Force is a vector quantity whose unit of recordings of such an exercise of an engine are
measurement is Newton (N), which is equivalent obtained and then simulated under laboratory
to the force required to accelerate a mass of 1 kg conditions. Engine speed and torque are con-
at a rate of 1 m/s2, that is, 1 N = 1 kg × 1 m/s2. trolled by two feedback systems.

• The acceleration due to gravity g can be adopted • A Prony brake dynamometer is one of the
as a suitable standard and is approximately equal simplest, inexpensive, and the most popular
to 9.81 m/s2. absorption dynamometer. It is a mechanical type
of device that depends on dry friction wherein
• Torque is defined as the force, which, besides mechanical energy is converted into heat.
exerting effects along its line of action, may
also exert a rotating force relative to any axis • In 1856, Lord Kelvin established the principle
excepting those intersecting the line of action. of electrical resistance strain gauges when he
Torque can also be termed as a couple or twisting demonstrated that when stress is applied to a
force. It is determined by measuring the force at metal wire, apart from undergoing changes in
a known radius r and is expressed as T = F × r. both length and diameter, there will be some
changes in the electrical resistance of the wire.
• Direct methods involve the comparison of an
unknown force with a known gravitational force • In electrical strain gauges, a change in strain
on the standard mass. A force is exerted on a produces a change in some electrical characteristic
body of mass m due to the earth’s gravitational such as capacitance, inductance, or resistance.
field, which can be represented by the following Magnification of the measured strain can be
equation: attained by employing auxiliary equipment. The
W = mg main advantages of measurement of strain using
Here, m is the standard mass, g is the acceleration electrical methods are their high sensitivity and
due to gravity, and W is the weight of the body. ability to respond to dynamic strains.

• Elastic members are generally used for the • When a strain gauge, which is an appropriately
measurement of force through displacement shaped piece of resistance material, is bonded
measurement. When an elastic member is to the surface of the material to be tested, it is
combined with a strain gauge and used for the known as a bonded strain gauge.
measurement of force, it is termed a load cell.
In load cells, elastic members act as primary • A cluster of three or more strain gauges, known
transducers and strain gauges as secondary as rosette gauges, can be employed if the
transducers. direction of principal strain is unknown. Rosette
gauges are normally used in the measurement of

MEASUREMENT OF FORCE, TORQUE, AND STRAIN  363

strain in complex parts. Here F is the gauge factor, ∆R is the change in
• A gauge factor is a measure of the amount of the resistance, and ∆L is the change in length.
Both ∆R and ∆L are due to straining of the
resistance change for a given strain and therefore gauge along the surface to which it is bonded
serves as an index of the strain sensitivity of the by the application of force. R and L are the
initial resistance and length of the strain gauge,
gauge. Mathematically, it is expressed as follows: respectively.

DR / R
F = DL / L

MULTIPLE-CHOICE QUESTIONS

1. Strain gauge rosettes are used when the direction (d) a corner only
6. Buoyancy effects are found in
of the
(a) platform balance
(a) principal stress is unknown (b) analytical balance
(c) electromagnetic-type balance
(b) hoop stress is known (d) pendulum-type balance
7. Which of the following balances is not appro-
(c) principal stress is known priate for large weights?
(a) Analytical balance
(d) hoop stress is unknown (b) Platform balance
(c) Electromagnetic-type balance
2. Dummy strain gauge are used for (d) Pendulum-type balance
8. When an elastic member is used in conjunction
(a) bridge sensitivity enhancement with a strain gauge, it is called a
(a) proving ring
(b) temperature compensation (b) absorption dynamometer
(c) Prony brake
(c) determining gauge factor (d) load cell
9. Tape recordings are used in
(d) calibration of strain gauges (a) servo-controlled dynamometers
(b) torsion-bar dynamometer
3. Strain gauges cannot be used at high temperatures (c) Prony brake dynamometer
(d) piezoelectric transducers
because of 10. In servo-controlled dynamometers,
(a) speed is controlled
(a) inferior strain gauge materials (b) torque is controlled
(c) both speed and torque are controlled
(b) gauge not being properly welded (d) strain is controlled
11. In a Prony brake dynamometer,
(c) a problem with gauge factor (a) mechanical energy is converted into heat
(b) mechanical energy is converted into electri-
(d) decomposition of cement and carrier
cal energy
materials (c) electrical energy is converted into torque
(d) there is no need for energy conversion
4. Which of the following equations is correct?

(a) dR/R = dR/R =1 – 2u + dr/r
dL/L ea dL/L

(b) dL/L dR/R dr/r
= =1 – 2u + dL/L
dR/R ea

(c) dL/L = dR/R =1 + 2u + dr/r
dR/R ea dL/L

dR/R dR/R dr/r
(d) = =1 + 2u + dL/L
dL/L ea

5. In a platform balance, the unknown weight is

placed at

(a) a specified position only

(b) any position with certain conditions

(c) any position without any conditions

364  ENGINEERING METROLOGY AND MEASUREMENTS

12. In a p-type semiconductor gauge, as tensile (b) electrical methods
strain increases (c) electronic methods
(a) gauge resistance decreases (d) optical methods
(b) gauge resistance increases 14. In torsion-bar dynamometers, to read the de-
(c) gauge resistance increases and then decreas- flection of the rotating shaft
es (a) hygroscopic effect is used
(d) there is no effect on gauge resistance (b) telescopic effect is used
(c) stroboscopic effect is used
13. In torsion-bar dynamometers, deflection mea- (d) microscopic effect is used
surement is carried out by
(a) mechanical methods

REVIEW QUESTIONS 11. Write a note on strain gauge materials.
12. Enlist the desirable characteristics of grid
1. With the help of a neat sketch, explain the
working of an analytical balance. materials.
13. Explain the different types of carrier materials.
2. Describe a platform balance with a neat diagram. 14. Mention the desirable characteristics of backing
3. Explain, with a neat sketch, determination of
materials.
force using a load cell. 15. Why are adhesives required? What are the
4. Explain the working of a proving ring with a
desirable characteristics of adhesives?
neat sketch. 16. Write short notes on the following:
5. Explain the working of a torsion-bar dy-
(a) Protective coatings on strain gauges
namometer. (b) Bonding of strain gauges
6. Discuss a servo-controlled dynamometer with a 17. What is a gauge factor? Explain its importance.
18. Deduce an expression for the gauge factor.
neat schematic diagram. 19. Explain the different methods of strain
7. Explain the working of the Berry strain gauge measurement.
20. Explain how the strain gauge is influenced by
extensometer. temperature variations.
8. Explain the following: 21. Explain the different methods of strain gauge
compensation.
(a) Unbonded strain gauge
(b) Bonded strain gauge
9. Explain the three types of bonded strain gauges
with a neat sketch.
10. What are rosette gauges? Explain briefly.

Answers to Multiple-choice Questions

1. (a)  2. (b)  3. (d)  4. (d)  5. (c)  6. (b)  7. (a)  8. (d)
9.  (a)   10.  (c)  11.  (a)  12.  (b)  13.  (d)  14.  (c) 

15CHAPTER Measurement of
Temperature

After studying this chapter, the reader will be able to

• understand the basics of temperature measurement
• describe the methods of temperature measurements
• explain thermocouples and the different laws of

thermocouples
• elucidate the different resistance temperature detectors
• comprehend calibration of liquids in glass thermometers
• discuss bimetallic strip thermometers
• throw light on pyrometers

15.1 INTRODUCTION

We know that temperature is a physical property of a material that gives a measure of the average
kinetic energy of the molecular movement in an object or a system. Temperature can be defined
as a condition of a body by virtue of which heat is transferred from one system to another. It is
pertinent to mention here that both temperature and heat are different. Temperature is a measure
of the internal energy of a system, whereas heat is a measure of the transfer of energy from one
system to another. Heat transfer takes place from a body at a higher temperature to one at a
lower temperature. The two bodies are said to be in thermal equilibrium when both of them are
at the same temperature and no heat transfer takes place between them. The rise in temperature
of a body is due to greater absorption of heat, which increases the movement of the molecules
within the body.

The first thermometer was developed by Galileo Galilei in the 17th century, which has
undergone significant improvement with the advancement of science and technology; present-
day thermometers are capable of measuring temperatures more accurately and precisely. In
1724, D.G. Fahrenheit, a German physicist, contributed significantly to the development of
thermometry. He proposed his own scale, in which 32° and 212° were considered the freezing
point and boiling point of water, respectively. The Swedish physicist Anders Celsius, in 1742,
developed the mercury-in-glass thermometer. He identified two points, namely the melting
point of ice and the boiling point of water, and assigned 0° and 100°, respectively, to them.
He made 100 divisions between these two points. In 1859, William John Macquorn Rankine,
a Scottish physicist, proposed an absolute or thermodynamic scale, known as Rankine scale

366  ENGINEERING METROLOGY AND MEASUREMENTS

when, after investigating the changes in thermal energy with changes in temperature, he came
to a conclusion that the theoretical temperature of each of the substances was the same at zero
thermal energy level. According to him, this temperature was approximately equal to −460 °F.

William Thomson, first Baron Kelvin, popularly known as Lord Kelvin, a British physicist,
introduced a new concept, known as the Kelvin scale, in the mid-1800s. He suggested 0 K
as the absolute temperature of gas and 273 K as the freezing point of water. A comparison
between Kelvin, Celsius, and Fahrenheit scales with respect to absolute zero, and boiling and
freezing points of water is shown in Table 15.1. Although human beings generally perceive
temperature as hot, warm (neutral), or cold, from an engineering perspective, a precise and
accurate measurement of temperature is essential.

Table 15.1  Comparison of temperature scales

Scales Water boils Water freezes Absolute zero
Kelvin 373.16 K 273.16 K 0K
Celsius 100 °C 0 °C −273.16°C
Fahrenheit 212 °F 32 °F −459.7 °F

The scales used to measure temperature can be divided into relative scales [Fahrenheit (°F)
and Celsius (°C)] and absolute scales [Rankine (°R) and Kelvin (K)]. The various temperature
scales are related as follows:

F = 1.8C + 32
C = (F − 32)/1.8
R = F + 460
K = C + 273

15.2  METHODS OF MEASURING TEMPERATURE

Measurement of temperature cannot be accomplished by direct comparison with basic
standards such as length and mass. A standardized calibrated device or system is necessary
to determine temperature. In order to measure temperature, various primary effects that cause
changes in temperature can be used. The temperature may change due to changes in physical or
chemical states, electrical property, radiation ability, or physical dimensions. The response of
the temperature-sensing device is influenced by any of the following factors:
1. Thermal conductivity and heat capacity of an element
2. Surface area per unit mass of the element
3. Film coefficient of heat transfer
4. Mass velocity of a fluid surrounding the element
5. Thermal conductivity and heat capacity of the fluid surrounding the element

Temperature can be sensed using many devices, which can broadly be classified into two
categories: contact- and non-contact-type sensors. In case of contact-type sensors, the object
whose temperature is to be measured remains in contact with the sensor. Inference is then
drawn on the assessment of temperature either by knowing or by assuming that the object and

MEASUREMENT OF TEMPERATURE  367

the sensor are in thermal equilibrium. Contact-type sensors are classified as follows:

1. Thermocouples 4. Liquid-in-glass thermometers

2. Resistance temperature detectors (RTDs) 5. Pressure thermometers

3. Thermistors 6. Bimetallic strip thermometers

In case of non-contact-type sensors, the radiant power of the infrared or optical radiation

received by the object or system is measured. Temperature is determined using instruments

such as radiation or optical pyrometers. Non-contact-type sensors are categorized as follows:

1. Radiation pyrometers

2. Optical pyrometers

3. Fibre-optic thermometers

15.3 THERMOCOUPLES

Thermocouples are active sensors employed for the measurement of temperature. The

thermoelectric effect is the direct conversion of temperature differences to an electric voltage.

In 1821, Thomas Johan Seebeck discovered that when two dissimilar metals are joined together

to form two junctions such that one junction (known as the hot junction or the measured

junction) is at a higher temperature than the other junction (known as the cold junction or the

reference junction), a net emf is generated. This emf, which also establishes the flow of current,

can be measured using an instrument connected as shown in Fig. 15.1. The magnitude of emf

generated is a function of the junction temperature. It is also dependent on the materials used to

form the two junctions. The thermoelectric emf is a result of the combination of two different

effects—the Peltier effect and the Thomson effect.

The French physicist Jean Charles Athanase Peltier discovered that if two dissimilar metals

are connected to an external circuit in a way such that a current is drawn, the emf may be slightly

altered owing to a phenomenon called Peltier effect. A potential difference always exists between

two dissimilar metals in contact with each other. This is known as the Peltier effect.

Thomson found out that the emf at a junction undergoes an additional change due to the

existence of a temperature gradient along either or both the metals. The Thomson effect states

that even in a single metal a potential gradient exists, provided there is a temperature gradient.

Both these effects form the basis of a thermocouple, which finds application in temperature

measurement. The flow of current through the circuit is spontaneous when two dissimilar metals

are joined together to form a closed circuit, that is, a thermocouple, provided one junction is

maintained at a temperature different from the other. This effect is termed the Seebeck effect.

In Fig. 15.1, if temperatures at the hot junction (T1) and the cold junction (T2) are equal
and at the same time opposite, then there will not be any flow of current. However, if they are

unequal, then the emfs will not balance and hence current will flow. It is to be mentioned here

that the voltage signal is a function of the junction temperature at the measured end and the

Voltmeter voltage increases as the temperature
rises. Variations in emf are

calibrated in terms of temperatures;

Hot junction Dissimilar metals Cold junction the devices employed to record
these observations are termed

Fig. 15.1  Basic thermocouple circuit thermocouple pyrometers.

368  ENGINEERING METROLOGY AND MEASUREMENTS

15.3.1  Laws of Thermocouples

Apart from the Peltier and Thomson effects, which form the basis of thermoelectric emf
generation, three laws of thermocouples that govern this phenomenon are required to be studied
in order to understand their theory and applicability. They also provide some useful information
on the measurement of temperature.

Law of Homogeneous Circuit

This law states that a thermoelectric current cannot be sustained in a circuit of a single
homogenous material, regardless of the variation in its cross section and by the application of
heat alone. This law suggests that two dissimilar materials are required for the formation of any
thermocouple circuit.

Law of Intermediate Metals

If an intermediate metal is inserted into a thermocouple circuit at any point, the net emf will not
be affected provided the two junctions introduced by the third metal are at identical temperatures.
This law allows the measurement of the thermoelectric emf by introducing a device into the
circuit at any point without affecting the net emf, provided that additional junctions introduced
are all at the same temperature.

T1 M1 T2 T1 M1 M3 M1 T2
P Q P R T3 S Q

M2 e M2 M2 e M2

Fig. 15.2  Law of intermediate metals

It is clear from Fig. 15.2 that when a third metal, M3, is introduced into the system, two more
junctions, R and S, are formed. If these two additional junctions are maintained at the same
temperature, say T3, the net emf of the thermocouple circuit remains unaltered.

Law of Intermediate Temperatures

If a thermocouple circuit generates an emf e1 when its two junctions are at temperatures T1
and T2, and e2 when the two junctions are at temperatures T2 and T3, then the thermocouple
will generate an emf of e1 + e2 when its junction temperatures are maintained at T1 andT3
(Fig. 15.3).

This law pertains to the calibration of the thermocouple and is important for providing
reference junction compensation. This law allows us to make corrections to the thermocouple
readings when the reference junction temperature is different from the temperature at which the
thermocouple was calibrated. Usually while preparing the calibration chart of a thermocouple,
the reference or cold junction temperature is taken to be equal to 0 °C. However, in practice, the
reference junction is seldom maintained at 0 °C; it is usually maintained at ambient conditions.
Thus, with the help of the third law, the actual temperature can be determined by means of the
calibration chart.

MEASUREMENT OF TEMPERATURE  369

T1 M1 T2 T2 M1 T3
P QP Q

M2 e1 M2 M2 e2 M2

T1 M1 T3
PQ

M2 e1+e2 M2

Fig. 15.3  Law of intermediate temperatures

15.3.2 Thermocouple Materials

Theoretically, any two different materials can be used to form a thermocouple. However,
only a few are suitable for temperature measurement applications. Combinations of different
thermocouple materials and their temperature range are given in Table 15.2. Base metal-type
thermocouples like copper–constantan pose high resistance to condensed moisture corrosion.
The iron–constantan type is essentially an inexpensive thermocouple capable of enduring
oxidizing and reducing atmospheres. The chromel–alumel thermocouple can resist an oxidizing
atmosphere.

Table 15.2  Temperature range of various thermocouple materials

Type Thermocouple materials Temperature range (ºC)

Base metal type

T Copper (40%)–constantan (60%) −200 to 350

J Iron–constantan −150 to 750

E Chromel–constantan (57% Cu, 43% Ni) −200 to 1000

K Chromel (90% Ni, 10% Cr)–Alumel (94% −200 to 1300
Ni, 2% Al, 3% Mn, 1% Si)

Rare metal type

S Platinum (90%)–rhodium–platinum (10%) 0–1500

R Platinum–rhodium (87% Pt, 13% Rh)– 0–1500
platinum

Thermocouple materials are divided into base metal type and rare, noble, or precious metal
type. Platinum (platinum–rhodium) thermocouples are called noble thermocouples, and all other
thermocouples belong to the base metal type. In a reducing atmosphere, these thermocouples

370  ENGINEERING METROLOGY AND MEASUREMENTS

are used with protection. Material combinations such as tungsten–tungsten–rhenium, iridium–
tungsten, and iridium–iridium–rhodium are called special types of thermocouples and are
used for a high temperature range of 1500–2300 °C. For high-temperature measurements, the
thermocouple wire should be thicker. However, an increase in the thickness of the wire lowers
the time of response of the thermocouple to temperature variations. Depending on the range of
temperature that thermocouples can measure, they are designated by a single letter and grouped
accordingly. Base metals, which can measure up to 1000 °C, are designated as Type K, Type
E, Type T, and Type J. Noble metals, which can measure up to a temperature of 2000 °C, is
classified as Type R, Type S, or Type B. Refractory metals are designated as Type C, Type D,
or Type G.

The choice of the thermocouple materials is influenced by several factors. Different
combinations of thermocouple materials should possess the following characteristics in order
to be used for temperature measurement:
1. Capable of producing a reasonable linear temperature–emf relationship
2. Able to generate sufficient thermo-emf per degree temperature change to facilitate detection

and measurement
3. Capable of withstanding persistent high temperatures, rapid temperature variations, and the

effects of corrosive environments
4. Good sensitivity to record even small temperature variations
5. Very good reproducibility, which enables easy replacement of the thermocouple by a similar

one without any need for recalibration
6. Good calibration stability
7. Economical

15.3.3  Advantages and Disadvantages of Thermocouple Materials

The following are some distinct advantages that merit the use of thermocouples:
1. Temperature can be measured over a wide range.
2. Thermocouples are self-powered and do not require any auxiliary power source.
3. A quick and good response can be obtained.
4. The readings obtained are consistent and hence are consistently repeatable.
5. Thermocouples are rugged, and can be employed in harsh and corrosive conditions
6. They are inexpensive.
7. They can be installed easily.

However, thermocouples also have certain disadvantages, which are listed as follows:
1. They have low sensitivity when compared to other temperature-measuring devices such as

thermistors and RTDs.
2. Calibration is required because of the presence of some non-linearity.
3. Temperature measurement may be inaccurate due to changes in the reference junction tem-

perature; hence thermocouples cannot be employed for precise measurements.
4. For enhancing the life of thermocouples, they should be protected against contamination and

have to be chemically inert.

15.3.4  Thermopiles

An extension of thermocouples is known as a thermopile. A thermopile comprises a number

MEASUREMENT OF TEMPERATURE  371

of thermocouples connected in series, wherein the hot junctions are arranged side by side or
in a star formation. In such cases, the total output is given by the sum of individual emfs. The
advantage of combining thermocouples to form a thermopile is that a much more sensitive
element is obtained. For example, a sensitivity of 0.002 °C at 1 mV/°C can be achieved with a
chromel–constantan thermopile consisting of 14 thermocouples. If n identical thermocouples
are combined to form a thermopile, then the total emf will be n times the output of the single
thermocouple.

For special-purpose applications such as measurement of temperature of sheet glass,
thermopiles are constructed using a series of semiconductors. For average temperature
measurement, thermocouples can be connected in parallel. During the formation of a thermopile,
one has to ensure that the hot junctions of the individual thermocouples are properly insulated
from one another.

Figures 15.4(a) and 15.4(b) illustrate, respectively, a thermopile having a series connection
and one having a star connection.

Intermediate Voltmeter
cold junctions

T1

T2 T2

Hot junctions Cold junction

(a) (b)

Fig. 15.4  Thermopiles (a) Series connection (b) Star connection

15.4  RESISTANCE TEMPERATURE DETECTORS

Thomas Johan Seebeck, in 1821, discovered thermoelectric emf. In the same year, Sir
Humphrey Davy showed that the resistivity of metals is highly dependent on temperature. In
1871, Sir William Siemens proposed the use of platinum as the primary element in resistance
thermometers. Platinum is extensively used in high-accuracy resistance thermometers because
it is capable of withstanding high temperatures and, at the same time, can sustain excellent
stability and exhibit good linearity. The first classical RTD was constructed by C.H. Meyers
in 1932, using platinum. A helical coil of platinum was wound on a crossed mica web, and the
entire assembly was mounted inside a glass tube. The advantage of this type of construction is
that the strain on the wire can be minimized and its resistance can be maximized. Slow thermal
response time and fragility of the structure limited its application due to poor thermal contact
between platinum and the measured point. Technological advancement led to the development
of more rugged RTDs later. The International Practical Temperature Scale was developed in
1968, and pure platinum RTDs have been used as the standard instruments for interpolating
between fixed points of the scale. The triple point of water (0.01 °C), boiling point of water
(100 °C), triple point of hydrogen (13.81 K), and freezing point of zinc (419.505 °C) are some
of the fixed points.

RTDs are also known as resistance thermometers. The American Society for Testing and

372  ENGINEERING METROLOGY AND MEASUREMENTS

Materials has defined the term resistance thermometer as follows: RTD is ‘a temperature-
measuring device composed of a resistance thermometer element, internal connecting wires, a
protective shell with or without means for mounting a connection head, or connecting wire or
other fittings, or both’.

We know that the electrical conductivity of a metal is dependent on the movement of electrons
through its crystal lattice. An RTD is a temperature sensor that works on the principle that the
resistance of electrically conductive materials is proportional to the temperature to which they
are exposed. Resistance of a metal increases with an increase in temperature. Hence, metals can
be classified as per their positive temperature coefficient (PTC).

When temperature measurement is performed by a resistance thermometer using
metallic conductors, it is called a resistance temperature detector (RTD); on the other hand,
semiconductors used for temperature measurement are called thermistors.

We know that an RTD measures temperature using the principle that the resistance of a metal
changes with temperature. In practice, the RTD element or resistor that is located in proximity
to the area where the temperature is to be measured transmits an electrical current. Then, using
an instrument, the value of the resistance of the RTD element is measured. Further, on the basis
of known resistance characteristics of the RTD element, the value of the resistance is correlated
to temperature. RTDs are more rugged and have more or less linear characteristics over a wide
temperature range. The range of RTDs is between 200 and 650 °C.

Many materials are commonly used for making resistance thermometers, such as platinum,
nickel, and copper, which are contained in a bulb. However, platinum is the most popular and
internationally preferred material. When platinum is employed in RTD elements, they are
sometimes termed platinum resistance thermometers. The popularity of platinum is due to the
following factors:
1. Chemical inertness
2. Almost linear relationship between temperature and resistance
3. Large temperature coefficient of resistance, resulting in readily measurable values of resis-

tance changes due to variations in temperature
4. Greater stability because the temperature resistance remains constant over a long period of

time
Selection of a suitable material for RTD elements depends on the following criteria:
1. The material should be ductile so that it can be formed into small wires.
2. It should have a linear temperature-versus-resistance graph.
3. It must resist corrosion.
4. It should be inexpensive.
5. It should possess greater stability and sensitivity.
6. It must have good reproducibility.
RTDs essentially have the following three configurations:
1. A partially supported wound element: A small coil of wire inserted into a hole in a ceramic
insulator and attached along one side of that hole
2. Wire-wound RTD: Prepared by winding a platinum or metal wire on a glass or ceramic bob-
bin and sealed with a coating on molten glass known as wire-wound RTD elements (Fig.
15.5)
3. Thin film RTD: Prepared by depositing or screening a platinum or metal glass slurry film
onto a small flat ceramic substrate called thin film RTD elements

MEASUREMENT OF TEMPERATURE  373

The general construction of a resistance thermometer is shown in Fig. 15.6. It comprises a

number of turns of resistance wire wrapped around a solid silver core. Transmission of heat

takes place quickly from the end flange through the core to the winding.

The thin film element used for temperature sensing is manufactured by depositing a very thin

(around 10–100 Å) layer of platinum on a ceramic substrate. The platinum layer is coated with

epoxy or glass, which protects the deposited platinum film and also acts as a strain reliever for

external lead wires. During the early stages of development, thin film sensors were unreliable

due to their instability and susceptibility to mechanical failure resulting in the breakage of lead

wires. Thin film RTD is the most rugged of the three RTD elements and is preferred for its

increased accuracy over time and improved reliability. A thin film responds faster due to its low

thermal mass and ease of assembly into smaller packages. Figure 15.7 shows a thin film RTD.

Compared to other types of temperature sensors, RTDs have the following advantages:

1. The resistance versus temperature linearity characteristics of RTDs are higher.

2. They possess greater accuracy (as high as ±0.1 °C). Standard platinum resistance thermom-

eters have ultra-high accuracy of around ±0.0001 °C.

3. They have excellent stability over time.

Resistance elements 4. Resistance elements can be used for
the measurement of differential tem-

perature.

Platinum Ceramic 5. Temperature-sensitive resistance ele-
leads bobbin ments can be replaced easily.

6. RTDs show high flexibility with re-

spect to the choice of measuring

Protective coating equipment, interchangeability of ele-
Fig. 15.5  Wire-wound RTD ments, and assembly of components.
7. Multiple resistance elements can be

Sensitive Platinum used in an instrument.
capsule leads 8. RTDs have a wide working range

without any loss of accuracy and, at

the same time, can be employed for

Resistance Ceramic Extension small ranges also.
windings insulator tube 9. They are best suited for remote indi-

Silver core cation applications.
1 0. It is possible to operate indicators, re-

Fig. 15.6  General construction of an RTD corders, or controllers.

Platinum lead wires RTDs are also associated with some
Fig. 15.7  Thin film RTD disadvantages. They are as follows:
1. The use of platinum in RTDs makes

them more expensive than other tem-
perature sensors.
2. The nominal resistance is low for a
given size, and the change in resis-
tance is much smaller than other tem-
perature sensors.

374  ENGINEERING METROLOGY AND MEASUREMENTS

3. Although its temperature sensitivity is high, it is less than that of thermistors.

15.5  THERMISTORS

Semiconductors that are used to measure temperature are called thermistors. When a thermistor

is employed for temperature measurement, its resistance decreases with increase in temperature.

The valence electrons, which are mutually shared by the metal atoms, move continuously and

freely through the metal during their movement from atom to atom. The vibration in the crystal

lattice of atoms increases with the increase in temperature. The free movement of electrons

becomes restricted due to an increase in the volume of space occupied by the atoms. In case

of thermistors, the valence electrons are attached more firmly to the atoms; some of the

electrons are detached and flow due to the increase in temperature, which decreases electrical

resistance facilitating the easy flow of electrons. Materials used in thermistors for temperature

measurements have very high temperature coefficients (8–10 times higher than platinum and

copper) and high resistivity (higher than any pure metal). Thus, they are very sensitive to small

variations in temperature and respond very quickly. The relationship between temperature and

resistance is given by the following equation:

( )1 – 1

R = RR eβ T TR

Here, R is the resistance at temperature T, RR is the resistance at the reference temperature
TR, e is the base of the Napierian logarithm, and β is a constant, which lies in the range of
3000–4600 K depending on the composition.

The temperature coefficient of resistance is given by the following equation:

dR/dT = b
R T2

The temperature coefficient of platinum at 25 °C is +0.0036/K and, for thermistors, it is
generally around −0.045/K, which is more than 10 times sensitive when compared to platinum.
A variety of ceramic semiconductor materials qualify as thermistor materials. Among them,
germanium containing precise proportions of arsenic, gallium, or antimony is most preferred.
The temperature measurement range of thermistors is −250 to 650 °C.

Thermistors are also produced using oxides of manganese, nickel cobalt, nickel copper, iron,
zinc, titanium, and tin. In order to attain better reproducibility and stability of the thermistor
characteristics, some chemically stabilizing oxides are added. The oxides are milled into powder
form and mixed with a plastic binder, which are then compressed into desired forms such as
disks or wafers. Disks are formed by compressing the mixtures using pelleting machines, and
the wafers are compression moulded. They are then sintered at high temperatures to produce
thermistor bodies. Depending on their intended application, leads are then added to these
thermistors and coated if necessary. To achieve the required stability, the thermistors so formed
are subjected to a special ageing process. Figure 15.8 illustrates the different forms in which
thermistors can be made.

The variation of temperature with voltage and resistance is shown in Fig. 15.9. The use of
thermistors as temperature sensors has several advantages:
1. Thermistors possess very high sensitivity, which is much higher than that of RTDs and ther-

mocouples, and hence have the capability to detect very small changes in temperature.

MEASUREMENT OF TEMPERATURE  375

(a) (b) (c) (d) (e) Thermistors

RTD

(f) (g) (h) (i) V or R Thermocouple

(j) (k) T
Fig. 15.9  Comparison of temperature characteristics
Fig. 15.8  Different forms of thermistors (a, b) Wafers
(c–e) Rods (f–i) Beads (j, k) Disks

2. Their response is very fast, and hence, they are employed for precise control of temperature.
3. They are inexpensive.

Thermistors also have certain disadvantages:
1. They have highly non-linear resistance temperature characteristics.
2. The temperature range is narrow.
3. Low fragility is often a problem.
4. High-temperature performance of thermistors is not good and they exhibit instability with

time.
5. They are prone to self-heating errors.

15.6  LIQUID-IN-GLASS THERMOMETERS

The liquid-in-glass thermometer is the most popular and is widely used for temperature

measurement. It comprises a bulb that contains a temperature-sensing liquid, preferably

mercury. Alcohol and pentane, which have lower freezing points than mercury and do not

contaminate if the bulb is broken, are also used. Since alcohol has a better expansion coefficient

than mercury, it is also used. A graduated capillary tube is connected to the bulb. At the top

of the capillary, a safety or expansion bulb is provided. Figure 15.10 shows a liquid-in-glass

thermometer. A range cavity is provided just above the

Capillary tube Expansion bulb bulb to accommodate the range variation. The walls of the
Scale Stem bulb should be thin in order to facilitate quick transfer of
heat. Further, for the response to be quick, the volume of
liquid should be small. However, the larger the volume of

Range cavity Liquid column the liquid, the higher the sensitivity. Since speed of response
depends on the volume of the liquid, a compromise needs to
be made between sensitivity and response.

Bulb The entire assembly is enclosed in a casing to provide
protection from breakage. An extra-long stem may

Fig. 15.10  Liquid-in-glass thermometer be provided to facilitate easy dipping into hot liquids.
Calibration of thermometers has to be carried out for better

376  ENGINEERING METROLOGY AND MEASUREMENTS

results. Liquid-in-glass thermometers are simple, portable, and inexpensive. However, they are
fragile and not suitable for remote applications and sensing surface temperature. Under optimal
conditions, the accuracy of this type of thermometers is around 0.1 °C.

15.7  PRESSURE THERMOMETERS

The change in temperature can be measured using pressure thermometers. These thermometers
work on the principle of thermal expansion of the matter wherein the change in temperature is
to be measured. Temperature change can be determined using these thermometers, which rely
on pressure measurement. Depending on the filling medium, pressure thermometers can be
classified as liquid, gas, or a combination of liquid and its vapour.

Pressure thermometers comprise the following components: a bulb filled with a liquid,
vapour, or gas; a flexible capillary tube; and a bourdon tube. Due to variation in temperature, the
pressure and volume of the system change and the fluid either expands or contracts. This causes
the bourdon tube to move or uncoil, which actuates the needle on the scale, thus providing a
measure of the temperature. A typical pressure thermometer is shown in Fig. 15.11.

Pressure thermometers are extensively preferred because of the following advantages:
1. Direct reading or recording is possible since pressure thermometers give adequate force

output.
2. Pressure thermometers are less expensive than other systems.

Pointer and scale
arrangement

Bourdon tube Free end
Capillary tube
Linkage
and gearing
mechanism

Bulb

Liquid
Fig. 15.11  Pressure thermometer

MEASUREMENT OF TEMPERATURE  377

3. They show a superior dynamic response when compared to liquid-in-metal thermometers.
4. They deliver a high-speed response.
5. Their maintenance is easy.

However, they suffer from limited linearity and are prone to output errors. In case of liquid-
or gas-filled thermometers, the tube and the filling are temperature sensitive, and if calibration
conditions differ along the tube, an error is induced. This error can be minimized by increasing
the ratio of volumes of the bulb and the tube. Increasing the bulb size reduces the time response
of the system but does not degrade the response. The presence of a pressure gradient resulting
from the elevation difference between the bulb and the bourdon tube also contributes to errors.

15.8  BIMETALLIC STRIP THERMOMETERS

John Harrison, who invented bimetallic thermometers, made the first bimetallic strip in 1759
to compensate for changes in the balance spring induced by temperature. A bimetallic strip
thermometer works on the well-known principle that different metals expand and contract
to different degrees, depending on the coefficient of expansion of the individual metals. For
example, if two strips of two different metals (steel and copper) are firmly welded, riveted, or
brazed together and subjected to temperature changes, either cooling or heating, the degree of
contraction or expansion of the metals differ depending on their coefficient of expansion. The
metal strips tend to bend owing to their different coefficients of expansion; the contraction or
expansion of one strip will be greater than that of the other. The difference in the expansion of
two metals, which makes the strip bend, is a measure of temperature, and since two different
metal strips are employed it is called a bimetallic strip thermometer. Figure 15.12 shows the
principle of a bimetallic strip.

Bimetallic strips are manufactured in different shapes: cantilever type, flat form, U form,
and helical and spiral shapes. In bimetallic strips, the lateral displacement in both the metals
is much larger than the small longitudinal expansion. This effect is made use of in mechanical
and electrical devices. For industrial use, the strips are wrapped around a spindle into a helical
coil. Due to its coil form, the length of the bimetallic strip increases, which in turn increases its
sensitivity. Bimetallic strip thermometers are preferred for their ruggedness and availability in

Metal strip 1 Metal strip 2

(a) (b) (c)
Fig. 15.12  Deflection of a bimetallic strip (a) Normal condition (b) Cold condition (c) Hot condition

378  ENGINEERING METROLOGY AND MEASUREMENTS

suitable forms. These thermometers are used for sensing temperature of hot water pipes, steam
chambers, etc. They are also used in temperature compensation clocks and circuit breakers.

15.9 PYROMETRY

In the preceding sections, contact-type temperature measurement devices have been discussed.
If the temperature of a very hot body has to be measured, contact-type temperature-measuring
devices will not be suitable, because they are liable to be damaged when they come in contact
with the hot body. Hence, the use of non-contact-type temperature-measuring devices becomes
imperative. When such devices are employed for high-temperature measurement, the distance
between the source of the temperature and the instrument has no effect on the measurement.
These non-contact-type devices are called pyrometers. The term pyrometer is of Greek origin,
wherein pyro stands for ‘fire’ and metron means ‘to measure’. Pyrometer was first invented
by the great English potter Josiah Wedgwood in the early 1780s, for which he received the
Fellowship of the Royal Society in 1783. Measurements of temperature are carried out either
by measuring energy radiated by a hot body or by colour comparison. Pyrometers are classified
into two distinct categories: total radiation pyrometers and optical pyrometers.

It is very well known that conduction, convection, and radiation are the three modes of
heat transfer. It is also a fact that all bodies above absolute zero radiate energy, and radiation
does not require any medium. When heat is radiated by a body at a given intensity, radiation
is emitted across a spectrum of wavelengths. Radiation intensity is directly proportional to
temperature. When radiation intensity falls, there is a corresponding increase in the wavelength
of radiation. On the other hand, the wavelength decreases when there is an increase in the
intensity of radiation.

A body that is capable of absorbing all the radiations that fall on it and does not reflect or
transmit any radiation is called a black body. A black body is an ideal thermal radiator. The
capacity of radiation absorption of a body depends on its surface condition. Under similar
conditions, a black body absorbs and loses heat more quickly than a non-black body. The
radiation absorption of a body is much superior when its colour is black and when it has a matt
or rough surface finish. The heat radiated by a black body is a function of temperature.

When a body radiates less heat than a black body, the ratio of this radiation to the black
body radiation is known as the total emissivity of the surface. If the emissivity of a black body
radiation is 1, then other bodies that transmit some of the incoming radiation is said to have an
emissivity of less than 1.

If E is the radiation impinging on a body (W/m2), a is the fraction of radiation power
absorbed by the body, and e is the total emissivity, then

e = aE = Radiation emitted from a body
E Radiation falling upon the body

The Stefan–Boltzmann law states that the total energy radiated by a black body is a function
of its absolute temperature only and is proportional to the fourth power of that temperature.

If E is the total energy radiated per unit area per unit time, then

E a Ta4 or E = σ Ta4

MEASUREMENT OF TEMPERATURE  379

Here, σ is the Stefan’s constant, which is equal to 50 × 10−8 W K4/m2 and Ta is the absolute
temperature in K.

According to the Stefan–Boltzmann law, if two ideal radiators are considered, the pyrometer
not only receives heat from the source, but also radiates heat to the source. Therefore, the net
rate of exchange of energy between them is given by

E = σ (Tp4 − Ts4)

whFeruertThpera,nTdp4Tissasrme tahlle temperatures of the pyrometer and the radiating source, respectively.
when compared to Ts and can be neglected.

If e is the emissivity of the body at a given temperature, then

E = eσTa4

If the emissivity of the surface is known, then the temperature of the body can be determined
provided it is kept in the open. If Tt is the true temperature and T is the apparent temperature
taken with a radiation pyrometer positioned in such a way that the body is in full view, then

E = σT4

The pyrometer receives energy that is equivalent to the energy emitted by a perfect black
body radiating at a temperature T. This temperature is lower than the temperature of the body
under consideration. We know that the energy emitted by a non-black body is given by the
equation E = eσTa4.

Hence, eTa4 = T4

With the help of this equation, the value of Ta can be determined.

15.9.1  TOTAL RADIATION PYROMETER

A total radiation pyrometer gives a measure of temperature by evaluating the heat radiation
emitted by a body. All the radiations emitted by a hot body or furnace are measured and
calibrated for black-body conditions. A total radiation pyrometer (shown in Fig. 15.13) basically
comprises an optical system that includes a lens, a mirror, and an adjustable eyepiece. The heat
energy emitted from the hot body is focused by an optical system onto the detector. The heat
energy sensed by the detector, which may be a thermocouple or a thermopile, is converted to its
analogous electrical signal and can be read on a temperature display device.

The pyrometer has to be aligned properly such that it is in line with the furnace or hot
body and is placed as close to it as possible. This is essential to minimize the absorption of
radiation by the atmosphere. Radiation pyrometers find applications in the measurement of
temperature in corrosive environments and in situations where physical contact is impossible.
In addition, radiations of moving targets and invisible rays can also be measured. It is also
used for temperature measurement when sources under consideration have near-black body
conditions.

The following are the advantages of radiation pyrometers:
1. It is a non-contact-type device.
2. It gives a very quick response.
3. High-temperature measurement can be accomplished.

380  ENGINEERING METROLOGY AND MEASUREMENTS

Radiation pyrometers also have certain disadvantages. They are as follows:
1. Errors in temperature measurement are possible due to emission of radiations to the atmo-

sphere.
2. Emissivity errors affect measurements.

Incoming
radiation

Mirror Eyepiece
Lens
Furnace or
hot body

Thermopile Temperature
display

Fig. 15.13  Total radiation pyrometer

15.9.2  Optical Pyrometer

Optical pyrometers work on the disappearing filament principle. In order to measure
temperature, the brightness generated by the radiation of the unknown source or hot body whose
temperature is to be determined is compared with that of the reference lamp. The brightness of
the reference lamp can be adjusted so that its intensity is equal to the brightness of the hot body
under consideration. The light intensity of the object depends on its temperature, irrespective
of its wavelength. A battery supplies the current required for heating the filament. The current
flowing through the filament is adjusted by means of a rheostat and an ammeter is used to
measure it. The current passing through the circuit is proportional to the temperature of the
unknown source. An optical pyrometer is schematically represented in Fig. 15.14.

An optical pyrometer essentially consists of an eyepiece, by means of which the filament and
the source are focused so that they appear superimposed, enabling a clear view for the observer.
Between the eyepiece and the reference lamp, a red filter is positioned, which helps narrow

Lamp Absorption filter

Eyepiece

Observer Hot source

Red filter Rheostat Objective
Battery Ammeter

Fig. 15.14  Optical pyrometer

MEASUREMENT OF TEMPERATURE  381

down the wavelength band and attain monochromatic

conditions. An absorption filter helps operate the lamp at

reduced intensity, thereby enhancing the life of the lamp.

The current in the reference lamp can be varied by operating

the rheostat and can be measured using the ammeter. Thus, (a) (b) (c)
the intensity of the lamp can be altered. The following three
situations (represented in Fig. 15.15) arise depending on Fig. 15.15  Disappearing filament
the current passing through the filament or lamp: principle (a) Current passing though
1. When the current passing through the filament is very the filament is low (b) Current passing

low, the radiation emitted by the filament is of a lesser though the filament is exact

(c) Current passing though the

intensity than that of the source, and the filament ap- filament is high

pears dark against a bright backdrop, as shown in Fig.

15.15(a).

2. When the current passing through the filament is exact, the intensity of the radiation emit-

ted by the filament is equal to that of the source and hence the filament disappears into the

background, as shown in Fig. 15.15(b).

3. When the current passing through the filament is very high, the radiation emitted by the fila-

ment is of higher intensity than that of the source and the filament appears brighter than the

background, as shown in Fig. 15.15(c).

When the filament disappears, the current that flows in the circuit is measured. The value

at which the filament disappears is a measure of the temperature of the radiated light in the

temperature source, when calibrated.

In another form of optical pyrometer, the red wavelength from the hot body is compared

with the radiation of a similar wavelength emitted by an electric lamp after calibration. The

advantages associated with optical pyrometers are as follows:

1. They are simple in construction and portable.

2. Optical pyrometers are flexible and easy to operate.

3. They provide very high accuracy of up to ±5 °C.

4. Since they are non-contact-type sensors, they are used for a variety of applications.

5. They can be used for remote-sensing applications, since the distance between the source and

the pyrometer does not affect the temperature measurement.

6. Optical pyrometers can be employed for both temperature measurement and for viewing and

measuring wavelengths that are less than 0.65 µm.

The following are the disadvantages of optical pyrometers:

1. Optical pyrometers can be employed for measurement only if the minimum temperature is

around 700 °C, since it is based on intensity of light.

2. Temperature measurement at short intervals is not possible.

3. Emissivity errors may affect measurement.

4. Optical pyrometers are used for the measurement of clean gases only.

Optical pyrometers can be employed to measure temperatures of liquid metals and materials

that are heated to a high temperature. This method is useful in situations where physical contact

is impossible, for example, for determining the temperature of molten metals and materials that

are heated to a high temperature. Temperature of furnaces can be measured easily.

382  ENGINEERING METROLOGY AND MEASUREMENTS

15.9.3  Fibre-optic Pyrometers

At the tip of the fibre optics’ free end, a temperature-sensing component is placed. The desired
radiation is collected by connecting a measuring system to the other end. The information
collected is then processed into a temperature value. The fibre-optic pyrometer essentially
comprises a fibre-optic cable and an array of components such as probes, sensors or receivers,
terminals, lenses, couplers, and connectors. A fibre-optic cable  is used to transmit radiation
from the black box cavity to a spectrometric device that computes the temperature. The
operating temperature of the fibre optics can be raised as they do not possess any electronic
components and hence do not require any cooling effort. Fibre optics can be used up to a
temperature of 300 °C and are available for wavelengths of 1 and 1.6 µm. With the advent of
technology, replacement of fibre-optic cables and optic systems can be carried out without any
recalibration. These find applications in procedures such as induction heating and welding.
Fibre-optic pyrometers are basically employed in applications where strong electrical and
magnetic interference fields act.

The following are the advantages of fibre optics:
1. These can be employed when the path of sight to the target is unclear.
2. When accuracy is a critical parameter, these can be used for measurement.
3. These can be used when the target whose temperature is to be determined is subjected to a

physical or chemical change.
4. Temperature as low as 100 °C can be measured.
5. Fibre-optic pyrometers do not carry any electrical current and can hence be safely employed

in explosive and hazardous locations.

15.9.4  Infrared Thermometers

It is a well-known fact that every material or matter whose temperature is above absolute zero

emits infrared radiations depending on the temperature. Infrared radiations are invisible to the

human eye and can be sensed as heat. An infrared thermometer is a non-contact-type sensor

that can detect infrared radiation from a heated body. We know that the radiation emitted by an

object or a heated body has different wavelengths. Radiations that have longer wavelengths than

visible light are known as infrared radiations; these radiations possess less energy and are less

harmful. A part of the infrared energy radiated by an object is detected by an infrared sensor. It

essentially measures the amount of radiation emitted by an object. Infrared thermometers are

Display IR filter ideally suited for high-temperature measurement. The
device surface of the object begins to radiate when it attains
a temperature of around 500–600 °C. The infrared

Very hot energy increases with increase in temperature. The

target practical wavelength range of infrared radiations is

between 0.7 and 20 μm, but normally radiations in

Detector Lens the wavelength range 0.7–14 μm are employed for
measurement. 

Field of view An infrared thermometer comprises a lens through

Fig. 15.16  Principle of infrared measurement which the infrared wave is focused on the detector.

MEASUREMENT OF TEMPERATURE  383

The infrared energy is absorbed and converted into an electrical signal by the detector. The
amount of radiation striking the detector determines the electrical output signal. The amplified
electrical output signal is then displayed on the screen in terms of temperature units. Variation
due to ambient temperature is adequately compensated before display. The principle of infrared
measurement is schematically represented in Fig. 15.16.

In order to assess the temperature of the target accurately, care needs to be taken to place the
heated body or target in such a way that it is in the complete field of view of the instrument.
The field of view can be defined as the angle of vision at which the instrument functions.
The infrared instrument determines the average temperature of all the surfaces exposed within
the field of vision. Temperature measurement may not be accurate if the temperature of the
background surfaces is different from that of the surfaces of the target under consideration. The
infrared thermometer provides better accuracy if emissivity of the material is known. Higher the
emissivity of the material, higher the accuracy of measurement. Reflection from other surfaces
also contributes to measurement errors.

An infrared thermometer facilitates the measurement of temperatures of moving objects. In
situations where objects are placed in vacuum or in a controlled atmosphere, or the distance
between the source of the temperature and the instrument of measurement is large, an infrared
device is most useful. It is particularly helpful when the objects are in inaccessible areas/
hazardous conditions, wherein non-contact measurement is the only option available for
determining temperature. Ambient conditions such as temperature variations and percentage
of CO2 (since it absorbs infrared radiations) in the atmosphere also affect accuracy. However,
infrared thermometers have limited accuracy.

A QUICK OVERVIEW

• Temperature can be defined as a condition of a external circuit in a way such that a current is
body by virtue of which heat is transferred from drawn, the emf may be slightly altered owing to
one system to another. Temperature is a measure a phenomenon called Peltier effect. A potential
of the internal energy of a system, whereas heat difference always exists between two dissimilar
is a measure of the transfer of energy from one metals in contact with each other. This is known
system to another. as the Peltier effect.
• Thomson found out that the emf at a junction
• Temperature can be sensed using many devices, undergoes an additional change due to the
which can broadly be classified into two existence of temperature gradient along either
categories: contact- and non-contact-type sensors. or both the metals. The Thomson effect states
that even in a single metal, a potential gradient
• Thomas Johan Seebeck discovered that when exists, provided there is a temperature gradient.
two dissimilar metals are joined together to form • Law of homogeneous circuit states that a
two junctions such that one junction (called thermoelectric current cannot be sustained
the hot junction or the measured junction) is in a circuit of a single homogenous material,
at a higher temperature than the other junction regardless of the variation in its cross-section
(known as the cold junction or the reference and by the application of heat alone. This law
junction), a net emf is generated. suggests that two dissimilar materials are

• Jean Charles Athanase Peltier discovered that
if two dissimilar metals are connected to an

384  ENGINEERING METROLOGY AND MEASUREMENTS

required for the formation of any thermocouple • A bimetallic strip thermometer works on the

circuit. well-known principle that different metals

• Law of intermediate metals states that if expand and contract to different degrees,

an intermediate metal is inserted into a depending on the coefficient of expansion of

thermocouple circuit at any point, there will not individual metals.

be any effect on the net emf, provided the new • Radiation thermometers (pyrometers) measure

two junctions formed by the insertion of the third temperature from the amount of thermal

metal are at identical temperatures. This law electromagnetic radiation received from a spot

allows the measurement of the thermoelectric on the object of measurement.

emf by introducing a device into the circuit at • Optical pyrometers measure temperature using

any point without affecting the net emf, provided the human eye to match the brightness of a hot

that additional junctions introduced are all at the object to the brightness of a calibrated lamp

same temperature. filament inside the instrument.

• Law of intermediate temperatures states that • A body that is capable of absorbing all the

if a thermocouple circuit generates an emf e1 radiations that fall on it and does not reflect or

when its two junctions are at temperatures T1 transmit any radiation is called a black body. A

and T2, and e2 when the two junctions are at black body is an ideal thermal radiator.

temperatures T2 and T3, then the thermocouple • If E is the radiation impinging on a body (W/m2),

will generate an emf e1 + e2 when its junction α is the fraction of radiation power absorbed by
temperatures are maintained at T1 and T3.
• An extension of thermocouples is known the body, and e is the total emissivity, then

as a e = aE = Radiation emitted from a body
E Radiation falling upon the body
thermopile. A thermopile comprises a number of

thermocouples connected in series, wherein the • The Stefan–Boltzmann law states that the total

hot junctions are arranged side by side or in star energy radiated by a black body is a function of

formation. its absolute temperature only and is proportional

• The American Society for Testing and Materials to the fourth power of that temperature.

has defined the term resistance thermometer • If E is the total energy radiated per unit area per

as follows: RTD is ‘a temperature-measuring unit time, then

device composed of a resistance thermometer E a Ta4 or E = σTa4
where σ is the Stefan’s constant, which is equal
element, internal connecting wires, a protective to 50 × 10−8 W K4/m2 and Ta is the absolute
temperature in K.
shell with or without the means for mounting

a connection head, or connecting wire or other

fittings, or both’. • At the tip of the fibre optics’ free end, a

• Semiconductors that are used to measure temperature-sensing component is placed. The

temperature are called thermistors. When desired radiation is collected by connecting

a thermistor is employed for temperature a measuring system to the other end. The

measurement, its resistance decreases with information collected is then processed into a

increase in temperature. temperature value.

• The change in temperature can be measured using • Every material or matter whose temperature is

pressure thermometers. These thermometers above absolute zero emits infrared radiations

work on the principle of thermal expansion depending on the temperature. Infrared

of matter wherein change in temperature is radiations are invisible to the human eye and can

to be measured. Temperature change can be be sensed as heat. An infrared thermometer is a

determined using these thermometers, which non-contact-type sensor that detects the infrared

rely on pressure measurement. radiation of a heated body.

MEASUREMENT OF TEMPERATURE  385

MULTIPLE-CHOICE QUESTIONS

1. Temperature gives a measure of 9. Semiconductors used for temperature meas-

(a) internal energy of the system urement are called

(b) external energy of the system (a) thermistors

(c) total energy of the system (b) thermopiles

(d) no relationship with energy (c) resistance temperature detectors

2. The first thermometer was developed by (d) pyrometers

(a) Rankine (c) Kelvin 10. The metal extensively used in high-accuracy

(b) Celsius (d) Galileo Galilei resistance thermometers is

3. If two bodies that are at different temperatures (a) rhodium (c) iridium

are so positioned that they are in contact with (b) nickel (d) platinum

one another, then 11. When a thermistor is employed for temperature

(a) heat will flow from the colder to the hotter measurement, its

body until they are at the same temperature (a) resistance increases with the increase in

(b) heat will flow from the hotter to the colder temperature

body until they are at the same temperature (b) resistance decreases with the increase in

(c) heat will not flow temperature

(d) heat will continue to flow from the hotter to (c) resistance increases with the decrease in

the colder body until you move them apart temperature

4. The measurable property that varies with (d) resistance decreases with the decrease in

temperature in a thermocouple is temperature

(a) expansion (c) voltage 12. The Stefan–Boltzmann law states that the total

(b) thermal radiation (d) electrical resistance energy radiated by a black body is given by

5. Which of the following temperatures is correct? (a) E = σσTTaa53 (c) EE2==σσTTa4a2
(b) E = (d)
(a) F = 1.6C + 32 (c) F = 1.8C + 273

(b) F = 1.8C + 32 (d) F = 1.8C + 212 13. Which of the following statements is true?

6. When there is no heat exchange between two (a) When radiation intensity falls, the

bodies that are at the same temperature, they are wavelength increases.

said to be in (b) When radiation intensity falls, the

(a) thermal equilibrium wavelength decreases.

(b) energy equilibrium (c) When radiation intensity falls, the

(c) heat equilibrium wavelength remains the same.

(d) electrical equilibrium (d) No relationship exists between the

7. Iron–constantan is a wavelength and radiation intensity.

(a) K-type thermocouple 14. Current flows through a circuit spontaneously

(b) J-type thermocouple when two dissimilar metals are joined to form

(c) S-type thermocouple a thermocouple, provided the two junctions

(d) R-type thermocouple formed are maintained at different temperatures.

8. Peltier effect states that when two dissimilar This effect is termed as

metals are in contact with each other, there (a) Thomson effect (c) Rankine effect

exists a (b) Seebeck effect (d) Stefan effect

(a) current difference 15. To reduce the band width of a wavelength, an

(b) energy difference optical pyrometer is provided with a

(c) potential difference (a) radiation filter (c) absorption filter

(d) temperature difference (b) blue filter (d) red filter

386  ENGINEERING METROLOGY AND MEASUREMENTS

REVIEW QUESTIONS 13. Explain the working principle of a bimetallic
strip with neat sketches.
1. Define temperature. How is it different from
heat? 14. What is pyrometry? Briefly explain the theory
of pyrometry.
2. Compare the different temperature scales.
3. List the factors that influence the response of a 15. With a neat sketch, explain a total radiation
pyrometer.
temperature-sensing device.
4. Explain Seebeck, Thomson, and Peltier effects. 16. Explain the construction and working of an
5. State and explain the different laws of optical pyrometer with the help of a schematic
diagram.
thermocouples.
6. Explain the different thermocouple materials 17. Mention the advantages and disadvantages of an
optical pyrometer.
and their designation.
7. Explain thermistors with a neat sketch. 18. List the different applications of a total radiation
8. With sketches, describe the different forms of pyrometer.

thermistors. 19. Write a note on the measurement of temperature
9. Write a short note on thermopiles. using a fibre-optic pyrometer.
10. With the help of a neat diagram, explain the
20. With a neat sketch, explain the working of an
construction and working of an RTD. infrared thermometer. In addition, state its
11. With a neat sketch, explain a liquid-in-glass application areas.

thermometer. 21. List the factors that contribute to inaccuracy
12. With a schematic diagram, explain the working in temperature measurement using infrared
systems.
of a pressure thermometer.

Answers to Multiple-choice Questions

1. (a)  2. (d)  3. (d)  4. (c)  5. (b)  6. (a)  7. (b)  8. (c)
9.  (a)   10.  (d)  11.  (b)  12.  (c)  13.  (a)  14.  (b)  15.  (d)

CHAPTER

16 Pressure Measurements

After studying this chapter, the reader will be able to

• understand the basics and elucidate the methods of pressure
measurement

• discuss manometers
• explain the different types of elastic transducers
• describe the different electrical pressure transducers
• explain the calibration of pressure gauges
• elucidate vacuum measurement systems
• explain high-pressure measurement

16.1 INTRODUCTION

Pressure is an essential component of everyday life of human beings. We talk about atmospheric
pressure, blood pressure, gauge pressure, vacuum, etc. Hence, it becomes imperative to know
the elementary details about pressure and its measurement. Pressure can be defined in many
ways.

Pressure is the force exerted by a medium, usually a fluid, on a unit area. Measuring devices
usually register a differential pressure—gauge pressure. Pressure is also defined as the force
exerted over a unit area. Force may be exerted by liquids, gases, and solids.

Pressure (P) = Force (F)
Area (A)

Pressure may be measured in atmospheres, bars, or in terms of the height of a liquid column.
Standard atmospheric pressure is usually referred to as 760 mmHg. The standard atmospheric
level is always measured at the sea level. It is to be noted that atmospheric pressure decreases
with increasing altitude. The units of pressure normally depend on the context in which pressure
is measured.

Measurement of pressure becomes an important aspect due to the following reasons:
1. It is a quantity that describes a system.
2. It is invariably a significant process parameter.
3. Many a time, pressure difference is used as a means of measuring the flow rate of a fluid.
4. From the lowest to the highest pressures usually encountered in practice, the level of pres-

sure has a range of nearly 18 orders of magnitude.