An expression for the torque of an induction motor may be derived from the equation of the mechanical power, Pm , available at. its shaft
T = Pm/ɷrot (14.22)
where ɷrot is the angular velocity of the rotor.
Since the angular velocity of the rotor is
ɷrot = 2πn/60
it. follows that the angular velocity of the magnetic field of a motor, ɷf , and that of its rotor, ɷrot are connected by the slip
s = (nl - n)/ nl = (ɷf - ɷrot)/ɷf
or
ɷrot = ɷf (1 - s)
The angular velocity of the rotating magnetic field, ɷf , is equal to the angular frequency of the sinewave current in the stator phase windings, 00, for a two-pole motor (p = 1). In the general case of a multipole motor the angular velocity of the rotating magnetic field is
ɷf = ɷ/p
where p is the number of pole pairs.
On expressing ɷrot in terms of W in Eq. (14.22), we get
T = P/(1-s)*Pm (14.23)
From the equivalent circuit of a motor phase, Fig 18 , it follows that the mechanical power at the. shaft is
Substituting Eq. (14.24) into Eq. (14.23) yields an expression for the torque. of an induction motor
T = m2prw2I22/ɷs (14.25)
Since, on the basis of the phasor diagram in Fig 15
rw2I2 = E2 cos φ2
and
E2/s = E2,st
it follows that
T = E2,stI2 (m2P/ɷ) cos φ2 (14.26)
On recalling Eq. (14.12),
E2,st =4.44fw2kw2Φr = ɷw2kw2Φr/√2
Eq. (14.26) may be re-cast as follows
T =(1/√2) m2Pw2kw2ΦrI2 cos φ2=const X ΦrI2 cos φ2 (14.27)
That is, the torque of an induction motor is proportional to the product of the rotating magnetic flux and the current in the rotor winding.
Labels: Electricity and Magnetism