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Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
JCT College of Engineering & Technology,
Pichanur, Coimbatore - 641105.
Electrical Machines-I
Faculty Name : D.Nagarajan
Designation : Assistant Professor
Year/Sem : II/III
Dept : EEE
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
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
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
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
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
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  to the
field, then the flux linking the coil is BAcos, and
the rate of change of flux is given by
t
Φ
N
V
d
d

  




cos
cos
d
d
d
sin
d



t
t
BA
dt
dΦ
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
• Thus for the arrangement shown below
t
Φ
N
V
d
d

  


cos
d
sin
d
d
d
NBA
t
NBA
t
Φ
N
V 


Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
• Therefore this arrangement produces a
sinusoidal output as shown below
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
• 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.‹#›
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
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
• Use of a commutator
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#›
• A simple generator with two coils

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111electrical-machines-i-ppt.pptx

  • 1. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› JCT College of Engineering & Technology, Pichanur, Coimbatore - 641105. Electrical Machines-I Faculty Name : D.Nagarajan Designation : Assistant Professor Year/Sem : II/III Dept : EEE
  • 2. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› 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
  • 3. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› 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
  • 4. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› 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  to the field, then the flux linking the coil is BAcos, and the rate of change of flux is given by t Φ N V d d         cos cos d d d sin d    t t BA dt dΦ
  • 5. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› • Thus for the arrangement shown below t Φ N V d d       cos d sin d d d NBA t NBA t Φ N V   
  • 6. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› • Therefore this arrangement produces a sinusoidal output as shown below
  • 7. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› • Wires connected to the rotating coil would get twisted • Therefore we use circular slip rings with sliding contacts called brushes
  • 8. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› 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
  • 9. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› • Use of a commutator
  • 10. Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 23.‹#› • A simple generator with two coils