Rotating Magnetic Field
- When three phase supply is given to three
phase winding, it produces rotating magnetic field which rotates and
synchronous speed.
- Similarly, when two phase supply is given to the two-phase
winding, the rotating magnetic field produced by the winding is given here.
Rotating Magnetic Field: Two Phase Winding
- Let us consider that the two windings P
and Q are placed at 90o with respect to each other.
- We assume that
when the two phase supply is given to the winding, flux produces in each
winding is purely sinusoidal.
- The waveform of the flux is shown in the figure
B.
- The direction of the flux is assumed as positive whereas its opposite sides indicate
negative values. The instantaneous value of flux can be given by
FP
= Fm
Sin θ
FQ
= Fm
Sin ( θ – 90o )
- The voltage of the winding P is taken as reference
or zero degree and winding Q is taken at 90 degree with respect to winding P.
Rotating Magnetic Field: Point 1
The voltage of winding P is zero whereas
winding Q is negative as shown in the figure. The voltage of the winding Q negative
sign is taken because we assume that the direction of voltage for winding P and
winding Q is positive in the first quadrant.
FP
= 0 and
FQ
= – Fm
Resultant flux F
= √ P2 + Q2 – 2PQCos θ
= √ 0 + ( – Fm
)2 – 0
= Fm
Rotating Magnetic Field: Point 2
The voltage of the winding P and winding Q
is 45 degrees but both are in the opposite direction.
FP
= Fm
/ √ 2 and
FQ
= – Fm
/ √ 2
Resultant flux F
= √ P2 + Q2 – 2PQCos θ
= √ Fm2
/ 2 + Fm2
/ 2 + 0
= Fm
Rotating Magnetic Field: Point 3
The voltage of the winding P is at 90 degree
but voltage of the winding Q is at and winding Q is 180 degree.
FP
= Fm
and
FQ
= 0
Resultant flux F
= √ P2 + Q2 – 2PQCos θ
= √ ( Fm
)2 + 0
= Fm
Rotating Magnetic Field: Point 4
The voltage of the winding P is at 135 degree
but voltage of the winding Q is at and winding Q is 45 degree but both are in
the opposite direction.
FP
= – Fm
/ √ 2 and
FQ
= Fm
/ √ 2
Resultant flux F
= √ P2 + Q2 – 2PQCos θ
= √ Fm2
/ 2 + Fm2
/ 2 + 0
= Fm