YASKAWA VS-626M5 Instruction Manual page 276

Appendix
15.1.3 Squirrel Cage Induction Motor Characteristics
15
Magnetic field
winding
+
Magnetic
field
−
(a) DC Motor
Short-circuit ring
Terminal U
(b) Squirrel Cage Induction Motor
Fig 15.5 Motor Model Diagrams
As shown in Fig. 15.5, the rotator is positioned inside the stator; i.e., within the rotation magnetic field.
When there is a difference between the angular velocity ω
the rotation magnetic field, the rotator conductor cuts the alternating magnetic field of the differential an-
gular velocity. Consequently, secondary induction electromotive force E
ductor due to the effect of magnetic field induction. Also, counterelectromotive force E
the stator due to the effects of electromagnetic induction, and interlinkage between the magnetic flux of
the rotation magnetic field and the stator winding.
E = kω = 2πkf
φ φ
1 m 1 m
1
Both tips of the rotator conductor are connected to the short-circuit ring, hence the name "squirrel cage."
The secondary current I thus flows due to the secondary induction electromotive force E
2
lent to the armature current of the DC motor.
Torque is generated using electromagnetic force proportional to the accumulation of secondary current I
and magnetic flux φ in the same way as the DC motor, causing the rotator to rotate. The ratio of the rotator
m
to the speed differential of the rotator magnetic field is called the induction motor "slip." If the rotator is
rotating at the same speed as the rotation magnetic field, the relative position of both will not change, so
the electromagnetic induction effect does not occur, and torque will not be generated. This is called syn-
chronous speed. Synchronous speed and slip are expressed using the following formulas.
120f
N =
Synchronous speed
P
N − N
r
S =
Slip
N
Stator
Flange
Commutator
Torque
Magnetic flux φ
Stator winding
Stator winding
Rotator conductor
Stator
I
2
Magnetic
Torque
flux φ
m
ω
r
ω
1
Terminal W
of the rotator and the angular velocity ω
r
−1
(min )
15 -4
+
m
−
Rotator
Terminal V
is generated in the rotator con-
2
is generated in
1
. This is equiva-
2
of
1
2