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Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.1
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 23.2
Introduction
 In this lecture we consider various forms of rotating
electrical machines
 These can be divided into:
– 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
23.1
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.3
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
 If a coil of area A rotates with respect to a field B,
and if at a particular time it is at an angle θ to the
field, then the flux linking the coil is BAcosθ, and the
rate of change of flux is given by
23.2
t
Φ
NV
d
d
=
( ) θωθ
θθ
coscos
d
d
d
sind
===
tt
BA
dt
dΦ
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.4
 Thus for the arrangement shown below
t
Φ
NV
d
d
=
( ) θω
θ
cos
d
sind
d
d
NBA
t
NBA
t
Φ
NV ===
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.5
 Therefore this arrangement produces a sinusoidal
output as shown below
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.6
 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 23.7
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
– 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
23.3
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.8
 Use of a commutator
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.9
 A simple generator with two coils
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.10
 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 23.11
DC Generators or Dynamos
 Practical DC generators or dynamos can take a
number of forms depending on how the magnetic
field is produced
– 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
23.4
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.12
 A four-pole DC generator
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.13
 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 23.14
 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 23.15
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
 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
23.5
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.16
 A four-pole alternator
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.17
 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 23.18
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 Ă— 60 =
1800 rpm.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.19
DC Motors
 When current flows in a conductor it produces a
magnetic field about it - as shown in (a) below
– 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)
23.6
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.20
 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 23.21
 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 23.22
AC Motors
 AC motors can be divided into two main forms:
– synchronous motors
– induction motors
 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
23.7
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.23
 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 23.24
 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 23.25
 A squirrel-cage induction motor
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.26
 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 23.27
 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 23.28
Universal Motors
 While most motors operate from either AC or DC,
some can operate from either
 These are universal motors and resemble series-
wound 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
23.8
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.29
Electrical Machines – A Summary
 Power generation is dominated by AC machines
– 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
23.9
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.30
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

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Dcgenerator

  • 1. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.1 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
  • 2. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.2 Introduction  In this lecture we consider various forms of rotating electrical machines  These can be divided into: – 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 23.1
  • 3. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.3 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  If a coil of area A rotates with respect to a field B, and if at a particular time it is at an angle θ to the field, then the flux linking the coil is BAcosθ, and the rate of change of flux is given by 23.2 t Φ NV d d = ( ) θωθ θθ coscos d d d sind === tt BA dt dΦ
  • 4. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.4  Thus for the arrangement shown below t Φ NV d d = ( ) θω θ cos d sind d d NBA t NBA t Φ NV ===
  • 5. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.5  Therefore this arrangement produces a sinusoidal output as shown below
  • 6. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.6  Wires connected to the rotating coil would get twisted  Therefore we use circular slip rings with sliding contacts called brushes
  • 7. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.7 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 – 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 23.3
  • 8. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.8  Use of a commutator
  • 9. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.9  A simple generator with two coils
  • 10. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.10  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
  • 11. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.11 DC Generators or Dynamos  Practical DC generators or dynamos can take a number of forms depending on how the magnetic field is produced – 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 23.4
  • 12. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.12  A four-pole DC generator
  • 13. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.13  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
  • 14. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.14  DC generator characteristics – vary slightly between forms – examples shown here are for a shunt-wound generator
  • 15. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.15 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  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 23.5
  • 16. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.16  A four-pole alternator
  • 17. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.17  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
  • 18. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.18 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 Ă— 60 = 1800 rpm.
  • 19. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.19 DC Motors  When current flows in a conductor it produces a magnetic field about it - as shown in (a) below – 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) 23.6
  • 20. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.20  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
  • 21. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.21  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
  • 22. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.22 AC Motors  AC motors can be divided into two main forms: – synchronous motors – induction motors  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 23.7
  • 23. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.23  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
  • 24. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 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
  • 25. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.25  A squirrel-cage induction motor
  • 26. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.26  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
  • 27. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.27  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
  • 28. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.28 Universal Motors  While most motors operate from either AC or DC, some can operate from either  These are universal motors and resemble series- wound 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 23.8
  • 29. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.29 Electrical Machines – A Summary  Power generation is dominated by AC machines – 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 23.9
  • 30. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.30 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