If a balanced 3ϕ voltage is applied to a balanced 3ϕ winding, it produced a rotating magnetic field of constant amplitude.
CONCEPT
OF ROTATING MAGNETIC FIELD
If
a balanced 3ϕ voltage is applied to a balanced 3ϕ winding, it produced a
rotating magnetic field of constant amplitude. This speed is called synchronous
speed.
The
speed of the rotating magnetic field is
Ns
= 120ƒ/P
f-
is the frequency of the supply
P
- is the number of stator poles
The
stator may be star or delta connected. The 3ϕ windings are displaced from each
other by an angle 120°.
Fig.
3.88 shows that the 3ϕ windings are supplied by a balanced 3f supply having
phase sequence RYB.
The current through the windings are displaced from each other by an angle of 120°.
The
instantaneous values of three fluxes are
ϕR
= ϕm m sin ωt ………(1)
ϕΥ
= ϕm sin (ωt - 120°) ………..(2)
ϕВ
= ϕm sin (ωt - 240°) …..…….(3)
The
resultant flux is
Case
1
If
ωt = Ɵ = 0
Substitute
ωt = 0 in equations (1), (2) and (3)
ϕR
= ϕm sin 0 = 0
ϕY
= ϕm sin (0-120°) = - 0.866 ϕm
ϕB=
ϕm (0-240°) = + 0.866 ϕm
Fig.
shows the phasor addition of fluxes
From
the above fig
OD
= DA = ϕRes/2
ϕRes
= 2 × 0.866 ϕm × cos 30°
=
1.5 ϕm
The
magnitude of ϕRes is 1.5 ϕm and it is vertivally placed.
Case
2
If
ωt = Ꮎ = 60°
Substitute
Ɵ = 60° in equations (1), (2) and (3)
ϕR
= ϕm sin 60° = 0.866 ϕm
ϕΥ
= ϕm sin (60° - 120°) = - 0.866 ϕm
ϕВ
= ϕm sin (60° - 240°) = 0
Fig.3.90
shows the phasor addition of the above three fluxes
From
the fig
OD
= DA = ϕRes/2
ϕRes
= 2 × 0.866 ϕm × cos 30°
=
1.5 ϕm
The
magnitude of ϕRes is 1.5 ϕm and it is rotated through 60°
in space in clockwise
direction
compared to its previous position
Case
3
ωt
= Ө = 120°
Substitute
Ɵ = 120° in equations (1), (2) and (3)
ϕR
= ϕm sin 120° = + 0.866 ϕm
ϕY
= ϕm sin (120° - 120°) = 0
ϕB
= ϕm (120° - 240°) = - 0.866 ϕm
Fig.3.91
shows the phasor addition of the above three fluxes
From
the fig
OD
= DA = ϕRes/2
ϕRes
= 2 × 0.866 ϕm × cos 30°
=
1.5 ϕm
The
magnitude of ϕRes is 1.5ϕm and it is rotated through 120°
in space on clockwise direction compared to its previous position.
Case
4
ωt
= Ө = 180°
Substitute
Ɵ = 180° in equations (1), (2) and (3)
ϕR
= ϕm sin 180° = 0
ϕY
= ϕm sin (180° - 120°) = + 0.866 ϕm
ϕB
= ϕm (180° - 240°) = - 0.866 ϕm
Fig.
3.92 shows the phasor addition of the above three fluxes
From the fig
OD
= DA = ϕRes/2
ϕRes
= 2 × 0.866 ϕm × cos 30°
=
1.5 ϕm
The
magnitude of ϕRes is 1.5 ϕm, and is rotated through 180°
in space in clockwise direction compaced to its previous position.
Basic Electrical and Electronics Engineering: Unit II: Electrical Machines : Tag: : Induction Motor - Concept of Rotating Magnetic Field
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