Rotor emf
- When the three
phase supply is given to the three phase induction motor, the rotating magnetic field is produced which rotates at synchronous speed.
Starting
condition
- The speed of the
rotor during starting condition is zero therefore the relative speed between
stator rotating magnetic field and rotor speed is
Ns –
N = Ns
- When the rotor
conductors cut the rotating magnetic field, an emf will be induced in it. Let
us consider that the induced emf in the rotor is E2
Running
condition
- Let us assume
that the induced emf in the rotor is E2’.
- The relative speed between
stator rotating magnetic field and rotor speed is Ns – N.
- The
induced emf in the rotor condition is
Relative speed Rotor emf
Ns E2
Ns – N E2’
E2’ = [ Ns
– N / Ns ] E2
E2’ = s E2
- The slip at
starting is unity therefore the rotor induced emf is same as that of starting
condition.
- However the rotor induced emf decreases as the speed increases or
slip decreases.
Effect of slip
on rotor parameters
- The effect of
slip on rotor parameter is summarized as below.
- As the slip decreases during
running condition, all the parameter decreases during running condition.
Rotor parameter
|
Starting condition
|
Running condition
|
Frequency of rotor
emf
|
f
|
f’
= sf
|
Rotor induced emf
|
E2
|
E2’=
s E2
|
Rotor resistance
|
R2
|
R2
|
Rotor reactance
|
X2
= 2πfL
|
X2’
= s X2 = s( 2πfL )
|
Rotor impedance
|
Z2
= √ R22 + X22
|
Z2’
= √ R22 + X2’2
=
√ R22 + ( sX2 )2
|
Rotor current
|
I2
= E2 / Z2
I2
= E2 / √ R22 + X22
|
I2’
= E2’/Z2
I2’=
s E2 / √ R22 + ( sX2 )2
|
Rotor power factor
|
Cos
F2
= R2 / Z2
=
R2 / √ R22 + X22
|
Cos
F2’
= R2 / Z2’
=
R2 / √ R22 + ( sX2 )2
|
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