To study the torque in three phase induction motor, it is necessary to have the understanding of the basics
of torque. So before moving forward to the concept of torque in induction
machine, let us revise some basics of torque.
Torque is nothing but the force
that is applied to an object around a circular axis. This force or torque tends
to move an object around the circumference of the circular axis. It is also
known as rotational force.
Torque in three phase induction motor
Similarly, torque in an
induction machine is the force which tends the rotor to rotate in a circular
axis.
In three phase induction motor
torque is produced by the interaction of magnetic field produced by stator
winding and magnetic field produced by rotor winding. These two magnetic fields
are sinusoidal distributed along the air gap and also they both rotate at
synchronous speed with respect to the stator.
These two fields produce north pole and south pole on both the stator and the rotor shown in the figure.
Initially the stator magnetic
field axes and the rotor magnetic field axes are at some angle that is
delta.
These two field axes tend to
align due to the magnetic force between poles on the rotor and the stator.
For the torque development it is
necessary that the both stator field and rotor field have the same number of
poles and these two are stationary with respect to each other.
When there is no angle between
these two magnetic field axes then no torque is produced. For the torque
development this condition is also necessary that these two field axes
initially have some angle.
So, we can say torque produced
in induction motor depends on the Fs (stator magnetic field) and Fr (rotor
magnetic field) and δ.
So,
T α Fs. Fr. Sin&
In three phase induction motor
Fs produced by the supply voltage V and it induced the voltage Er in the rotor
conductor.
So, we can say that,
V α Fs
α Er
And the rotor magnetic field Fr
is produced due to rotor current and this rotor current is produced because the
rotor is short circuited.
So, we can say that
Fr α Ir
And the & is the angle
between Fr and Fs. From equation (1) and (2) it is assumed that & is the
angle between Er and Ir.
So, the angle between Er and Ir
is ɸr
So, we can say that
T α Er . Ir.
cosɸr
where cosɸr is the rotor power factor
Equation (3) represents the
torque equation of three phase induction motor.
Maximum Torque of Three Phase Induction Motor
To get the maximum torque,
differentiate equation (3) with respect to Rr because Rr can be varied by
adding external resistance to the rotor circuit.
After differentiating we get the
condition for maximum torque i.e.
Rr =
s.Xr
Slip at which maximum torque
occurs is
s (max) =
Rr / Xr
Starting Torque of Three Phase Induction Motor
At starting slip = 1
So, the torque equation at
starting of three phase induction motor
For getting maximum torque at
starting, Rr must be equal to Xr at starting. It is achieved by adding external
resistance to the rotor circuit. It is only possible in the case of slip ring
induction motors.
Torque Under Running Condition
Under running condition equation
(3) represents the torque in three phase induction motor.
The slip under running condition is very low. So sXr is also very low and it can be neglected.
Under running condition, Torque
is inversely proportional to the rotor resistance and directly proportional to
the induced emf in the rotor circuit and slip.
As,
Er α
Fs α V
So, we can say,
T
α V2
Under running conditions torque
has a direct relation to slip in induction motor. This relation between torque and slip is studied
with the help of torque slip characteristics of three phase induction motor.
related posts
#_starting methods of induction motor
#_speed control methods of three phase induction motor
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