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Electric Motors and Generators 
 Introduction 
 A Simple AC Generator 
 A Simple DC Generator 
 DC Generators or Dynamos 
 AC Generators or Alternators 
 DC Motors 
 AC Motors 
 Universal Motors 
 Electrical Machines – A Summary 
Chapter 23 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.1
Introduction 
 In this lecture we consider various forms of rotating 
electrical machines 
 These can be divided into: 
23.1 
– generators – which convert mechanical energy into 
electrical energy 
– motors – which convert electrical energy into 
mechanical energy 
 Both types operate through the interaction between a 
magnetic field and a set of windings 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.2
A Simple AC Generator 
 We noted earlier that Faraday’s law dictates that if a 
coil of N turns experiences a change in magnetic 
flux, then the induced voltage V is given by 
23.2 
= d 
V N Φ 
t 
d 
 If a coil of area A rotates with respect to a field B, 
and if at a particular time it is at an angle q to the 
field, then the flux linking the coil is BAcosq, and the 
rate of change of flux is given by 
( ) q q cosq wcosq 
= d sin = d 
= 
d 
d 
t t 
BA 
dΦ 
dt 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.3
 Thus for the arrangement shown below 
( ) q w cosq 
d 
d d sin 
NBA 
V = N Φ = NBA 
= 
= d 
t 
V N Φ 
t 
d 
d 
t 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.4
 Therefore this arrangement produces a sinusoidal 
output as shown below 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.5
 Wires connected to 
the rotating coil 
would get twisted 
 Therefore we use 
circular slip rings 
with sliding 
contacts called 
brushes 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.6
A Simple DC Generator 
 The alternating signal from the earlier AC generator 
could be converted to DC using a rectifier 
 A more efficient approach is to replace the two slip 
rings with a single split slip ring called a commutator 
23.3 
– this is arranged so that connections to the coil are 
reversed as the voltage from the coil changes polarity 
– hence the voltage across the brushes is of a single 
polarity 
– adding additional coils produces a more constant output 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.7
 Use of a commutator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.8
 A simple generator with two coils 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.9
 The ripple can be further reduced by the use of a 
cylindrical iron core and by shaping the pole pieces 
– this produces an 
approximately 
uniform field in the 
narrow air gap 
– the arrangement 
of coils and core 
is known as the 
armature 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.10
DC Generators or Dynamos 
 Practical DC generators or dynamos can take a 
number of forms depending on how the magnetic 
field is produced 
23.4 
– can use a permanent magnet 
– more often it is generated electrically using field coils 
 current in the field coils can come from an external supply 
– this is known as a separately excited generator 
 but usually the field coils are driven from the generator output 
– this is called a self-excited generator 
– often use multiple poles held in place by a steel tube 
called the stator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.11
 A four-pole DC generator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.12
 Field coil excitation 
– sometimes the field coils are connected in series with 
the armature, sometimes in parallel (shunt) and 
sometimes a combination of the two (compound) 
– these different forms 
produce slightly 
different 
characteristics 
– diagram here 
shows a 
shunt-wound 
generator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.13
 DC generator characteristics 
– vary slightly between forms 
– examples shown here are for a shunt-wound generator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.14
AC Generators or Alternators 
 Alternators do not require commutation 
– this allows a simpler construction 
– the field coils are made to rotate while the armature 
windings are stationary 
23.5 
 Note: the armature windings are those that produce the output 
– thus the large heavy armature windings are in the 
stator 
– the lighter field coils are mounted on the rotor and 
direct current is fed to these by a set of slip rings 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.15
 A four-pole alternator 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.16
 As with DC generators multiple poles and sets of 
windings are used to improve efficiency 
– sometimes three sets of armature windings 
are spaced 120° apart around the stator to form 
a three-phase generator 
 The e.m.f. produced is in sync with rotation of the 
rotor so this is a synchronous generator 
– if the generator has a single set of poles the output 
frequency is equal to the rotation frequency 
– if additional pole-pairs are used the frequency is 
increased accordingly 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.17
Example – see Example 23.2 from course text 
A four-pole alternator is required to operate at 60 Hz. 
What is the required rotation speed? 
A four-pole alternator has two pole pairs. Therefore 
the output frequency is twice the rotation speed. 
Therefore to operate at 60Hz, the required speed 
must be 60/2 = 30Hz. This is equivalent to 30 ´ 60 = 
1800 rpm. 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.18
DC Motors 
 When current flows in a conductor it produces a 
magnetic field about it - as shown in (a) below 
23.6 
– when the current-carrying conductor is within an 
externally generated magnetic field, the fields interact 
and a force is exerted on the conductor - as in (b) 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.19
 Therefore if a conductor lies within a magnetic field: 
– motion of the conductor produces an electric current 
– an electric current in the conductor will generate motion 
 The reciprocal nature of this relationship means that, 
for example, the DC generator above will function as a 
DC motor 
– although machines designed as motors are more 
efficient in this role 
 Thus the four-pole DC generator shown earlier could 
equally well be a four-pole DC motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.20
 DC motor characteristics 
– many forms – each with slightly different characteristics 
– again can be permanent magnet, or series-wound, 
shunt-wound or compound wound 
– figure below shows a shunt-wound DC motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.21
AC Motors 
 AC motors can be divided into two main forms: 
– synchronous motors 
– induction motors 
23.7 
 High-power versions of either type invariably operate 
from a three-phase supply, but single-phase 
versions of each are also widely used – particularly 
in a domestic setting 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.22
 Synchronous motors 
– just as a DC generator can be used as a DC motor, so 
AC generators (or alternators) can be used as 
synchronous AC motors 
– three phase motors use three sets of stator coils 
 the rotating magnetic field drags the rotor around with it 
– single phase motors require some starting mechanism 
– torque is only produced when the rotor is in sync with 
the rotating magnetic field 
 not self-starting – may be configured as an induction motor 
until its gets up to speed, then becomes a synchronous motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.23
 Induction motors 
– these are perhaps the most important form of AC motor 
– rather than use slip rings to pass current to the field 
coils in the rotor, current is induced in the rotor by 
transformer action 
– the stator is similar to that in a synchronous motor 
– the rotor is simply a set of parallel conductors shorted 
together at either end by two conducting rings 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.24
 A squirrel-cage induction motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.25
 In a three-phase induction motor the three phases 
produce a rotating magnetic field (as in a three-phase 
synchronous motor) 
– a stationary conductor will see a varying magnetic field 
and this will induce a current 
– current is induced in the field coils in the same way 
that current is induced in the secondary of a 
transformer 
– this current turns the rotor into an electromagnet which 
is dragged around by the rotating magnetic field 
– the rotor always goes slightly slower than the magnetic 
field – this is the slip of the motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.26
 In single-phase induction motors other techniques 
must be used to produce the rotating magnetic field 
– various techniques are used leading to various forms 
of motor such as 
 capacitor motors 
 shaded-pole motors 
– such motors are inexpensive and are widely used in 
domestic applications 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.27
Universal Motors 
 While most motors operate from either AC or DC, 
some can operate from either 
 These are universal motors and resemble series-wound 
23.8 
DC motors, but are designed for both AC and 
DC operation 
– typically operate at high speed (usually > 10,000 rpm) 
– offer high power-to-weight ratio 
– ideal for portable equipment such as hand drills and 
vacuum cleaners 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.28
Electrical Machines – A Summary 
 Power generation is dominated by AC machines 
23.9 
– range from automotive alternators to the synchronous 
generators used in power stations 
– efficiency increases with size (up to 98%) 
 Both DC and AC motors are used 
– high-power motors are usually AC, three-phase 
– domestic applications often use single-phase induction 
motors 
– DC motors are useful in control applications 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.29
Key Points 
 Electrical machines include both generators and motors 
 Motors can usually function as generators, and vice versa 
 Electrical machines can be divided into AC and DC forms 
 The rotation of a coil in a uniform magnetic field produces a 
sinusoidal e.m.f. This is the basis of an AC generator 
 A commutator can be used to produce a DC generator 
 The magnetic field in an electrical machine is normally 
produced electrically using field coils 
 DC motors are often similar in form to DC generators 
 Some forms of AC generator can also be used as motors 
 The most widely used form of AC motor is the induction 
motor 
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.30

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Electric motors and generators

  • 1. Electric Motors and Generators  Introduction  A Simple AC Generator  A Simple DC Generator  DC Generators or Dynamos  AC Generators or Alternators  DC Motors  AC Motors  Universal Motors  Electrical Machines – A Summary Chapter 23 Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.1
  • 2. Introduction  In this lecture we consider various forms of rotating electrical machines  These can be divided into: 23.1 – generators – which convert mechanical energy into electrical energy – motors – which convert electrical energy into mechanical energy  Both types operate through the interaction between a magnetic field and a set of windings Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.2
  • 3. A Simple AC Generator  We noted earlier that Faraday’s law dictates that if a coil of N turns experiences a change in magnetic flux, then the induced voltage V is given by 23.2 = d V N Φ t d  If a coil of area A rotates with respect to a field B, and if at a particular time it is at an angle q to the field, then the flux linking the coil is BAcosq, and the rate of change of flux is given by ( ) q q cosq wcosq = d sin = d = d d t t BA dΦ dt Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.3
  • 4.  Thus for the arrangement shown below ( ) q w cosq d d d sin NBA V = N Φ = NBA = = d t V N Φ t d d t Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.4
  • 5.  Therefore this arrangement produces a sinusoidal output as shown below Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.5
  • 6.  Wires connected to the rotating coil would get twisted  Therefore we use circular slip rings with sliding contacts called brushes Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.6
  • 7. A Simple DC Generator  The alternating signal from the earlier AC generator could be converted to DC using a rectifier  A more efficient approach is to replace the two slip rings with a single split slip ring called a commutator 23.3 – this is arranged so that connections to the coil are reversed as the voltage from the coil changes polarity – hence the voltage across the brushes is of a single polarity – adding additional coils produces a more constant output Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.7
  • 8.  Use of a commutator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.8
  • 9.  A simple generator with two coils Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.9
  • 10.  The ripple can be further reduced by the use of a cylindrical iron core and by shaping the pole pieces – this produces an approximately uniform field in the narrow air gap – the arrangement of coils and core is known as the armature Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.10
  • 11. DC Generators or Dynamos  Practical DC generators or dynamos can take a number of forms depending on how the magnetic field is produced 23.4 – can use a permanent magnet – more often it is generated electrically using field coils  current in the field coils can come from an external supply – this is known as a separately excited generator  but usually the field coils are driven from the generator output – this is called a self-excited generator – often use multiple poles held in place by a steel tube called the stator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.11
  • 12.  A four-pole DC generator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.12
  • 13.  Field coil excitation – sometimes the field coils are connected in series with the armature, sometimes in parallel (shunt) and sometimes a combination of the two (compound) – these different forms produce slightly different characteristics – diagram here shows a shunt-wound generator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.13
  • 14.  DC generator characteristics – vary slightly between forms – examples shown here are for a shunt-wound generator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.14
  • 15. AC Generators or Alternators  Alternators do not require commutation – this allows a simpler construction – the field coils are made to rotate while the armature windings are stationary 23.5  Note: the armature windings are those that produce the output – thus the large heavy armature windings are in the stator – the lighter field coils are mounted on the rotor and direct current is fed to these by a set of slip rings Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.15
  • 16.  A four-pole alternator Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.16
  • 17.  As with DC generators multiple poles and sets of windings are used to improve efficiency – sometimes three sets of armature windings are spaced 120° apart around the stator to form a three-phase generator  The e.m.f. produced is in sync with rotation of the rotor so this is a synchronous generator – if the generator has a single set of poles the output frequency is equal to the rotation frequency – if additional pole-pairs are used the frequency is increased accordingly Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.17
  • 18. Example – see Example 23.2 from course text A four-pole alternator is required to operate at 60 Hz. What is the required rotation speed? A four-pole alternator has two pole pairs. Therefore the output frequency is twice the rotation speed. Therefore to operate at 60Hz, the required speed must be 60/2 = 30Hz. This is equivalent to 30 ´ 60 = 1800 rpm. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.18
  • 19. DC Motors  When current flows in a conductor it produces a magnetic field about it - as shown in (a) below 23.6 – when the current-carrying conductor is within an externally generated magnetic field, the fields interact and a force is exerted on the conductor - as in (b) Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.19
  • 20.  Therefore if a conductor lies within a magnetic field: – motion of the conductor produces an electric current – an electric current in the conductor will generate motion  The reciprocal nature of this relationship means that, for example, the DC generator above will function as a DC motor – although machines designed as motors are more efficient in this role  Thus the four-pole DC generator shown earlier could equally well be a four-pole DC motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.20
  • 21.  DC motor characteristics – many forms – each with slightly different characteristics – again can be permanent magnet, or series-wound, shunt-wound or compound wound – figure below shows a shunt-wound DC motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.21
  • 22. AC Motors  AC motors can be divided into two main forms: – synchronous motors – induction motors 23.7  High-power versions of either type invariably operate from a three-phase supply, but single-phase versions of each are also widely used – particularly in a domestic setting Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.22
  • 23.  Synchronous motors – just as a DC generator can be used as a DC motor, so AC generators (or alternators) can be used as synchronous AC motors – three phase motors use three sets of stator coils  the rotating magnetic field drags the rotor around with it – single phase motors require some starting mechanism – torque is only produced when the rotor is in sync with the rotating magnetic field  not self-starting – may be configured as an induction motor until its gets up to speed, then becomes a synchronous motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.23
  • 24.  Induction motors – these are perhaps the most important form of AC motor – rather than use slip rings to pass current to the field coils in the rotor, current is induced in the rotor by transformer action – the stator is similar to that in a synchronous motor – the rotor is simply a set of parallel conductors shorted together at either end by two conducting rings Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.24
  • 25.  A squirrel-cage induction motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.25
  • 26.  In a three-phase induction motor the three phases produce a rotating magnetic field (as in a three-phase synchronous motor) – a stationary conductor will see a varying magnetic field and this will induce a current – current is induced in the field coils in the same way that current is induced in the secondary of a transformer – this current turns the rotor into an electromagnet which is dragged around by the rotating magnetic field – the rotor always goes slightly slower than the magnetic field – this is the slip of the motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.26
  • 27.  In single-phase induction motors other techniques must be used to produce the rotating magnetic field – various techniques are used leading to various forms of motor such as  capacitor motors  shaded-pole motors – such motors are inexpensive and are widely used in domestic applications Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.27
  • 28. Universal Motors  While most motors operate from either AC or DC, some can operate from either  These are universal motors and resemble series-wound 23.8 DC motors, but are designed for both AC and DC operation – typically operate at high speed (usually > 10,000 rpm) – offer high power-to-weight ratio – ideal for portable equipment such as hand drills and vacuum cleaners Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.28
  • 29. Electrical Machines – A Summary  Power generation is dominated by AC machines 23.9 – range from automotive alternators to the synchronous generators used in power stations – efficiency increases with size (up to 98%)  Both DC and AC motors are used – high-power motors are usually AC, three-phase – domestic applications often use single-phase induction motors – DC motors are useful in control applications Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.29
  • 30. Key Points  Electrical machines include both generators and motors  Motors can usually function as generators, and vice versa  Electrical machines can be divided into AC and DC forms  The rotation of a coil in a uniform magnetic field produces a sinusoidal e.m.f. This is the basis of an AC generator  A commutator can be used to produce a DC generator  The magnetic field in an electrical machine is normally produced electrically using field coils  DC motors are often similar in form to DC generators  Some forms of AC generator can also be used as motors  The most widely used form of AC motor is the induction motor Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.30