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Electrical Machines Module 2'27

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... wire coil, called a stator winding. It is built into the motor. ... most common is the squirrel-cage winding. This entire winding is made up of heavy copper bars ... – PowerPoint PPT presentation

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Title: Electrical Machines Module 2'27


1
Electrical MachinesModule 2.27
  • Lecturer
  • Dr Vesna Brujic-Okretic
  • Ext 9676 and 9681
  • Email mes1vb_at_surrey.ac.uk

2
Induction motor
  • The induction motor derives its name from the
    fact that ac voltages are induced in the rotor
    circuit by the rotating magnetic field of the
    stator
  • An Induction motor operates on the principle of
    induction
  • The rotor receives power from the stator due to
    Induction The rotor is not connected to an
    external source of voltage.
  • It is important to understand the principle of
    rotating magnetic field in order to understand
    the operation of an Induction motor.
  • The induction motor is the most commonly used
    type of AC motor. Its simple, rugged construction
    costs relatively little to manufacture.
  • induction motors are often large motors and
    permanently mounted motors that drive loads at
    fairly constant speed.
  • Examples washing machines, refrigerator
    compressors, bench grinders, table saws etc.

3
Induction motor
  • The stator in an AC motor is a wire coil, called
    a stator winding. It is built into the motor.
    When this coil is energized by AC power, a
    rotating magnetic field is produced.
  • When a magnetic field comes close to a wire, it
    produces an electric current in that wire. This
    is called induction - as you remember (Faraday's
    law)
  • In induction motors, the induced magnetic field
    of the stator winding induces a current in the
    rotor. This induced rotor current produces a
    second magnetic field necessary for the rotor to
    turn.

4
Induction motor
  • When a three-phase voltage is applied to the
    stator winding , a rotating magnetic field of
    constant magnitude is produced.
  • This rotating field is produced by the
    contributions of space-displaced phase windings
    carrying appropriate time displaced currents
  • These currents, which are time displaced by 120
    electrical degrees, are shown in the following
    slide

5
Induction motor - rotating field
  • iaImcos wt
  • ibImcos (wt - 1200)
  • icImcos (wt - 2400)

6
Induction motor Rotor
  • The induction rotor is made of a laminated
    cylinder with slots in its surface.
  • The most common is the squirrel-cage winding.
    This entire winding is made up of heavy copper
    bars connected together at each end by a metal
    ring made of copper or brass. No insulation is
    required between the core and the bars. This is
    because of the very low voltages generated in the
    rotor bars.

7
Induction motors Rotor
  • squirrel cage rotors resemble the exercise wheels
  • Configuration Several metal bars are placed
    within end rings in a cylindrical pattern.
    Because the bars are connected to one another by
    these end rings, a complete circuit is formed
    within the rotor.
  • Another possible type is a wound rotor induction
    motor

8
Induction motor Rotor and stator
9
Induction motor Cut away view
10
How does it work?
  • Alternating current flowing in the stator causes
    the poles to change rapidly, from north to south
    and back again, thus generating a changing
    magnetic field.
  • The rotating magnetic field generated in the
    stator induces a magnetic field in the rotor. The
    two fields interact and cause the rotor to turn.
    To obtain maximum interaction between the fields,
    the air gap between the rotor and stator should
    be very small.
  • As you know from Lenz's law, any induced emf
    tries to oppose the changing field that induces
    it.
  • In the case of an induction motor, the changing
    field is the motion of the resultant stator
    field. A force is exerted on the rotor by the
    induced emf and the resultant magnetic field.
    This force tends to cancel the relative motion
    between the rotor and the stator field. The
    rotor, as a result, moves in the same direction
    as the rotating stator field.

11
How does it work?
  • The lines of force of the rotor magnetic field
    are moving in the same direction as those of the
    stator, thus adding to the magnetic field, which
    keeps the rotor turning.
  • It is, however, impossible for the rotor of an
    induction motor to turn at the same speed as the
    rotating magnetic field.
  • If the speeds were the same, there would be no
    relative motion between the stator and rotor
    fields without relative motion there would be no
    induced voltage in the rotor.
  • In order for relative motion to exist between the
    two, the rotor must rotate at a speed slower than
    that of the rotating magnetic field.
  • The difference between the speed of the rotating
    stator field and the rotor speed is called slip.
    The smaller the slip, the closer the rotor speed
    approaches the stator field speed.

12
Rotating field velocity
  • The velocity of the rotating magnetic field of
    the stator can be calculated with the formula
    below (we shall not go into details of how it is
    derived, but it is simple, and follows from the
    equations for poly-phase machines)
  • Ns120fs / p
  • where p is the number of poles and fs is the
    applied frequency of the stator magnetic field
  • When the stator is supplied by a balanced
    three-phase source, it will produce a magnetic
    field that rotates at synchronous speed
    determined by the above eq.

13
Slip
  • We said the rotor reacts to the magnetic field,
    but does not travel at the same speed.
  • We also said the rotor speed actually lags behind
    the speed of the magnetic field. It runs at the
    speed Nr which is close to the speed of the
    stator field, Ns when the motor is running light,
    but decreases as the load is increased
  • The term slip quantifies the slower speed of the
    rotor in comparison with the rotating speed of
    the stator magnetic field and is expressed
    mathematically as
  • S(Ns-Nr)/Ns

14
Slip
  • The rotor is not locked into any position and
    therefore will continue to slip throughout the
    motion.
  • The speed of the rotor depends upon the torque
    requirements of the load. The bigger the load,
    the stronger the turning force needed to rotate
    the rotor.
  • The turning force can increase only if the
    rotor-induced e.m.f. increases
  • This e.m.f. can increase only if the magnetic
    field cuts through the rotor at a faster rate.
  • To increase the relative speed between the field
    and the rotor, the rotor must slow down.
  • Therefore, for heavier loads the induction motor
    turns slower than for lighter loads. The amount
    of slip increases proportionally with increase in
    load

15
Slip
  • Actually only a slight change in speed is
    necessary to produce the current changes required
    to accommodate the changes in load. This is
    because the rotor windings have a low resistance.
  • As a result, induction motors are called
    constant-speed motors
  • A typical T-w characteristic for the cage-type
    induction motor is shown on the following slide

16
Speed-Torque Characteristics
torque
17
Analysis of operation
  • On start-up the slip is s1 and the starting
    torque (also known as a breakaway torque) is
    sufficiently large to accelerate the rotor (the
    rotor has previously been 'locked' - stationary)
  • As the rotor runs up to its full-load speed the
    torque increases in essentially inverse
    proportion to the slip
  • the start-up and running curves merge to give the
    characteristic as shown on the previous slide
  • After the torque reached its maximum, it rapidly
    falls to zero, at the synchronous speed, Ns
  • Looking backwards as rotor speed falls below Ns
    the torque increases almost linearly to a maximum
    dictated by the full load (plus rotor losses)
  • the speed only falls a little when the load is
    raised from 0 to its full value - this is a
    normal operating region

18
Analysis of operation
  • the induction motor may be regarded as a
    constant speed machine (similarly to a shunt DC
    motor)
  • Other key features
  • The maximum speed is a synchronous speed, Ns,
    independent of the applied voltage
  • Torque is proportional to the V2 at an arbitrary
    speed
  • When operating at 90-95 Ns heat losses are at
    minimum

19
Types Applications
  • There are a variety of different types of
    induction motors, differing mainly by the number
    of phases and the winding type.
  • Some of the more common names are
  • shaded pole, split phase, capacitor start, two
    value capacitor, permanent split capacitor, two
    phase, three phase star, three phase delta, and
    three phase single voltage
  • APPLICATIONS
  • Most widely used AC motor squirrel-cage
  • Big squirrel-cage motors - in factories
  • small squirrel-cage motors - in home appliances

20
Important considerations
  • Factors to be considered when selecting an
    induction motor
  • speed range and speed variation
  • acceleration/deceleration characteristics
    (starting torque/full load torque ratio this can
    vary a lot from a few percent to several times)
    to have enough starting torque to overcome
    static friction, accelerate the load up to the
    full working speed and handle the maximum
    overload
  • duty cycle the percentage of the time the motor
    is loaded
  • the power required to drive the load
  • The operating speed of the motor is determined by
    the point at which the power (or torque) that the
    motor can supply intersects with the power (or
    torque) that the load can absorb, mechanically
  • the motor must satisfy mechanical requirements
  • heating properties
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