Induction motor

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Three-phase induction motors

Animation of a squirrel-cage AC motor

An induction motor (or asynchronous motor or squirrel-cage motor) is a type of

alternating current motor where power is supplied to the rotor by means of electromagnetic
induction.

An electric motor converts electrical power to mechanical power in its rotor (rotating part).
There are several ways to supply power to the rotor. In a DC motor this power is supplied to
the armature directly from a DC source, while in an induction motor this power is induced in
the rotating device. An induction motor is sometimes called a rotating transformer because
the stator (stationary part) is essentially the primary side of the transformer and the rotor
(rotating part) is the secondary side. Unlike the normal transformer which changes the current
by using time varying flux, induction motor uses rotating magnetic field to transform the
voltage. The primary side's currents evokes a magnetic field which interacts with the
secondary side's emf to produce a resultant torque, henceforth serving the purpose of
producing mechanical energy. Induction motors are widely used, especially polyphase
induction motors, which are frequently used in industrial drives.
Induction motors are now the preferred choice for industrial motors due to their rugged
construction, absence of brushes (which are required in most DC motors) and — thanks to
modern power electronics — the ability to control the speed of the motor.

[edit] History
The induction motor was first realized by Galileo Ferraris in 1885 in Italy. In 1888, Ferraris
published his research in a paper to the Royal Academy of Sciences in Turin (later, in the
same year, Tesla gained U.S. Patent 381,968) where he exposed the theoretical foundations
for understanding the way the motor operates. The induction motor with a cage was invented
by Mikhail Dolivo-Dobrovolsky about a year later. Technological development in the field
has improved to where a 100 hp (74.6 kW) motor from 1976 takes the same volume as a
7.5 hp (5.5 kW) motor did in 1897. Currently, the most common induction motor is the cage
rotor motor

[edit] Principle of operation and comparison to

synchronous motors

A 3-phase power supply provides a rotating magnetic field in an induction motor.

The basic difference between an induction motor and a synchronous AC motor is that in the
latter a current is supplied into the rotor (usually a DC current) which in turn creates a
(circular uniform) magnetic field around the rotor. The rotating magnetic field of the stator
will impose an electromagnetic torque on the still magnetic field of the rotor causing it to
move (about a shaft) and rotation of the rotor is produced. It is called synchronous because at
steady state the speed of the rotor is the same as the speed of the rotating magnetic field in the
stator.

By way of contrast, the induction motor does not have any direct supply onto the rotor;
instead, a secondary current is induced in the rotor. To achieve this, stator windings are
arranged around the rotor so that when energised with a polyphase supply they create a
rotating magnetic field pattern which sweeps past the rotor. This changing magnetic field
pattern induces current in the rotor conductors. These currents interact with the rotating
magnetic field created by the stator and in effect causes a rotational motion on the rotor.

However, for these currents to be induced, the speed of the physical rotor must be less than
the speed of the rotating magnetic field in the stator, or else the magnetic field will not be
moving relative to the rotor conductors and no currents will be induced. If by some chance
this happens, the rotor typically slows slightly until a current is re-induced and then the rotor
continues as before. This difference between the speed of the rotor and speed of the rotating
magnetic field in the stator is called slip. It is unitless and is the ratio between the relative
speed of the magnetic field as seen by the rotor (the slip speed) to the speed of the rotating
stator field. Due to this an induction motor is sometimes referred to as an asynchronous
machine.

[edit] AC Induction Motor

where

n = Revolutions per minute (rpm)

f = AC power frequency (hertz)

p = Number of poles per phase (an even number)

Slip is calculated using:

where s is the slip.

The rotor speed is:

[edit] Synchronous Motor

A synchronous motor always runs at synchronous speed with 0% slip. The speed of a
synchronous motor is determined by the following formula:

where as p= no. of magnetic poles

For example a 6 pole motor operating on 60Hz power would have speed:

where v is the speed of the rotor (in rpm), f is the frequency of the AC supply (in Hz) and p is
the number of magnetic poles.

Note on the use of p: Some texts refer to number of pole pairs per phase instead of number of
poles per phase. For example a 6 pole motor, operating on 60Hz power, would have 3 pole
pairs. The equation of synchronous speed then becomes: P=3 ,P = no. of magnetic pole pairs.
 right

[edit] Construction
The stator consists of wound 'poles' that carry the supply current to induce a magnetic field
that penetrates the rotor. In a very simple motor, there would be a single projecting piece of
the stator (a salient pole) for each pole, with windings around it; in fact, to optimize the
distribution of the magnetic field, the windings are distributed in many slots located around
the stator, but the magnetic field still has the same number of north-south alternations. The
number of 'poles' can vary between motor types but the poles are always in pairs (i.e. 2, 4, 6,
etc.).

Induction motors are most commonly built to run on single-phase or three-phase power, but
two-phase motors also exist. In theory, two-phase and more than three phase induction
motors are possible; many single-phase motors having two windings and requiring a
capacitor can actually be viewed as two-phase motors, since the capacitor generates a second
power phase 90 degrees from the single-phase supply and feeds it to a separate motor
winding. Single-phase power is more widely available in residential buildings, but cannot
produce a rotating field in the motor (the field merely oscillates back and forth), so single-
phase induction motors must incorporate some kind of starting mechanism to produce a
rotating field. They would, using the simplified analogy of salient poles, have one salient pole
per pole number; a four-pole motor would have four salient poles. Three-phase motors have
three salient poles per pole number, so a four-pole motor would have twelve salient poles.
This allows the motor to produce a rotating field, allowing the motor to start with no extra
equipment and run more efficiently than a similar single-phase motor.

There are three types of rotor:

 Squirrel-cage rotor

The most common rotor is a squirrel-cage rotor. It is made up of bars of either solid copper
(most common) or aluminum that span the length of the rotor, and those solid copper or
aluminium strips can be shorted or connected by a ring or some times not, i.e. the rotor can be
closed or semiclosed type. The rotor bars in squirrel-cage induction motors are not straight,
but have some skew to reduce noise and harmonics.

 Slip ring rotor

A slip ring rotor replaces the bars of the squirrel-cage rotor with windings that are connected
to slip rings. When these slip rings are shorted, the rotor behaves similarly to a squirrel-cage
rotor; they can also be connected to resistors to produce a high-resistance rotor circuit, which
can be beneficial in starting

 Solid core rotor

A rotor can be made from a solid mild steel. The induced current causes the rotation.

[edit] Speed control

The synchronous rotational speed of the rotor (i.e. the theoretical unloaded speed with no
slip) is controlled by the number of pole pairs (number of windings in the stator) and by the
frequency of the supply voltage. Before the development of cheap power electronics, it was
difficult to vary the frequency to the motor and therefore the uses for the induction motor
were limited. As an induction motor has no brushes and is easy to control, many older DC
motors are being replaced with induction motors and accompanying inverters in industrial
applications.The induction motor runs on induced current.speed of induction motor varies
according to the load supplied to the induction motor.As the load on the induction motor is
increased the speed of the motor gets decreased and vice versa.

[edit] Starting of induction motors

[edit] Three Phase
[edit] Direct-on-line starting

The simplest way to start a three-phase induction motor is to connect its terminals to the line.
This method is often called "direct on line" and abbreviated DOL.

In an induction motor, the magnitude of the induced emf in the rotor circuit is proportional to
the stator field and the slip speed (the difference between synchronous and rotor speeds) of
the motor, and the rotor current depends on this emf. When the motor is started, the rotor
speed is zero. The synchronous speed is constant, based on the frequency of the supplied AC
voltage. So the slip speed is equal to the synchronous speed, the slip ratio is 1, and the
induced emf in the rotor is large. As a result, a very high current flows through the rotor. This
is similar to a transformer with the secondary coil short circuited, which causes the primary
coil to draw a high current from the mains.

When an induction motor starts DOL, a very high current is drawn by the stator, in the order
of 5 to 9 times the full load current. This high current can, in some motors, damage the
windings; in addition, because it causes heavy line voltage drop, other appliances connected
to the same line may be affected by the voltage fluctuation. To avoid such effects, several
other strategies are employed for starting motors.

[edit] Star-delta starters

An induction motor's windings can be connected to a 3-phase AC line in two different ways:

 wye (star in Europe), where the windings are connected from phases of the supply to
the neutral;
 delta (sometimes mesh in Europe), where the windings are connected between phases
of the supply.
A delta connection of the machine winding results in a higher voltage at each winding
compared to a wye connection (the factor is ). A star-delta starter initially connects the
motor in wye, which produces a lower starting current than delta, then switches to delta when
the motor has reached a set speed. Disadvantages of this method over DOL starting are:

 Lower starting torque, which may be a serious issue with pumps or any devices with
significant breakaway torque
 Increased complexity, as more contactors and some sort of speed switch or timers are
needed
 Two shocks to the motor (one for the initial start and another when the motor switches
from wye to delta)

[edit] Variable-frequency drives

Variable-frequency drives (VFD) can be of considerable use in starting as well as running

motors. A VFD can easily start a motor at a lower frequency than the AC line, as well as a
lower voltage, so that the motor starts with full rated torque and with no inrush of current.
The rotor circuit's impedance increases with slip frequency, which is equal to supply
frequency for a stationary rotor, so running at a lower frequency actually increases torque.

[edit] Resistance starters

A resistance starter and its 4MW / 11kV induction motor, driving a ball mill.

This method is used with slip ring motors where the rotor poles can be accessed by way of
the slip rings. Using brushes, variable power resistors are connected in series with the poles.
During start-up the resistance is large and then reduced to zero at full speed.

At start-up the resistance directly reduces the rotor current and so rotor heating is reduced.
Another important advantage is the start-up torque can be controlled. As well, the resistors
generate a phase shift in the field resulting in the magnetic force acting on the rotor having a
favorable angle[citation needed].

[edit] Autotransformer starters

such starters are called as auto starters or compensators, consists of an auto-transformer.

[edit] Series Reactor starters

In series reactor starter technology, an impedance in the form of a reactor is introduced in

series with the motor terminals, which as a result reduces the motor terminal voltage resulting
in a reduction of the starting current; the impedance of the reactor, a function of the current
passing through it, gradually reduces as the motor accelerates, and at 95 % speed the reactors
are bypassed by a suitable bypass method which enables the motor to run at full voltage and
full speed. Air core series reactor starters or a series reactor soft starter is the most common
and recommended method for fixed speed motor starting. The applicable standards are [IEC
289] AND [IS 5553 (PART 3) ]

[edit] Single Phase

In a single phase induction motor, it is necessary to provide a starting circuit to start rotation
of the rotor. If this is not done, rotation may be commenced by manually giving a slight turn
to the rotor. The single phase induction motor may rotate in either direction and it is only the
starting circuit which determines rotational direction.

For small motors of a few watts the start rotation is done by means of a single turn of heavy
copper wire around one corner of the pole. The current induced in the single turn is out of
phase with the supply current and so causes an out-of-phase component in the magnetic field,
which imparts to the field sufficient rotational character to start the motor. Starting torque is
very low and efficiency is also reduced. Such shaded-pole motors are typically used in low-
power applications with low or zero starting torque requirements, such as desk fans and
record players.

Larger motors are provided with a second stator winding which is fed with an out-of-phase
current to create a rotating magnetic field. The out-of-phase current may be derived by
feeding the winding through a capacitor, or it may derive from the winding having different
values of inductance and resistance from the main winding.

In some designs the second winding is disconnected once the motor is up to speed, usually
either by means of a switch operated by centrifugal force acting on weights on the motor
shaft, or by a positive temperature coefficient thermistor which after a few seconds of
operation heats up and increases its resistance to a high value, reducing the current through
the second winding to an insignificant level. Other designs keep the second winding
continuously energised during running, which improves torque.

Control of speed in induction motor can be obtained in 3 ways:

1.scalar control 2.vector control 3.direct torque control