Basic Induction Motor Concepts
The Development of
Induced Torque in an Induction Motor
When current flows in
the stator, it will produce a magnetic field in stator as such
that Bs (stator magnetic
Field) will rotate at
a speed:
N sync =(120
Fe)/( P)
Where Fe is
the system frequency in hertz and P is the number of poles in the machine. This
rotating
Magnetic
field Bs passes over the rotor bars and induces a voltage in them.
The voltage induced in the
Rotor is given by:
e ind =
(v x B) l
Hence there will be
rotor current flow which would be lagging due to the fact that the rotor has an
Inductive element. In
addition, this rotor current will produce a magnetic field at the
rotor, Br. Hence the
Interaction between
both magnetic field would give torque:
The torque induced
would generate acceleration to the rotor, hence the rotor will spin.
However, there is a
finite upper limit to the motor’s speed.
SPEED-TORQUE
CHARACTERISTICS OF
INDUCTION MOTORS
The X axis shows speed and
Slip. The Y-axis shows the torque and current.
The
Characteristics are drawn with rated voltage
and
Frequency supplied to the stator.
During start-up, the motor typically draws up
to seven
times the rated current. This high current is
a result of
Stator and rotor flux, the losses in the
stator and rotor
Windings and losses in the bearings due to
friction.
This high starting current overcomes these
Components and produces the momentum to rotate
the rotor.
At start-up, the motor delivers 1.5 times the
rated
Torque of the motor. This starting torque is
also
Locked rotor torque (L RT). As the speed
increases,
The Current drawn by the motor reduces
slightly (see
The current drops significantly, when the
motor speed
Approaches ~80% of the rated speed. At base
speed,
The motor draws the rated current and delivers
the
Rated torque.
At base speed, if the load on the motor shaft
is
Increased beyond its rated torque, the speed
starts
Dropping and slip increases. When the motor is
Running at approximately 80% of the
synchronous
Speed, the load can increase up to 2.5 times
the rated torque.
This torque is called breakdown torque. If the
load on
The motor is increased further; it will not be
able to
Take any further load and the motor will
stall.
In addition, when the load is increased beyond
the
Rated load, the load current increases
following the
Current characteristic path. Due to this
higher current
Flow in the windings, inherent losses in the
windings
Increase as well. This leads to a higher
temperature in
The motor windings. Motor windings can
withstand
Different temperatures, based on the class of
Insulation used in the windings and cooling
system
Used in the motor. Some motor manufacturers
provide
The data on overload capacity and load over
duty cycle.
If the motor is overloaded for longer than
Recommended, then the motor may burn out.
As seen in the speed-torque characteristics,
torque is
Highly nonlinear as the speed varies. In many
applications,
The speed needs to be varied, which makes the
Torque vary. We will discuss a simple open
loop
Method of speed control called, Variable
Voltage
Variable Frequency (VF or V/f) in this
application note.
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