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What is Armature Reaction??
Armature reaction is the effect of armature produced
flux on the main field flux. The armature mmf
produces two undesirable effects on the main field
flux and these are:-
1) Net reduction in the main field flux per pole.
2)Distortion of the main field flux wave along the air-
gap periphery.
How it takes place??
From the fig(A) it shows that the flux path for the main
poles of a 2-pole DC machine at no load ie. With no
armature currents.
This main field flux, produced by GNA
field mmf If Nf , is shown by horizontal MNA
Phasor OA= . O A
fΦ
fΦ
Now when the DC machine is loaded, current flows in the
armature windings.
These currents are as shown in the figure (B), these
currents set up armature flux shown by the vertical flux
lines, with the field winding unexcited.
The other figure represent armature flux Φa by a vertical
phasor OB.
GNA
 O
 B aΦ
Now by examination of the above two figures reveals that
the path of armature flux Φa is perpendicular to the main
flux path Φf .
In other words, the path of the armature flux crosses the
path of the main field flux.
O A
B
Thus the effect of armature flux on the main field flux is
entirely ‘cross-magnetizing’ and it is for this reason that
the flux produced by armature mmf is called cross-flux.
fΦ
aΦ
Now when the current flows in both the armature and
field windings, the resultant flux distribution is obtained
by superimposing the two fluxes of fig (A) and fig(B).
From the fig(C)shown below, it is seen that the armature
flux aids the main field flux at the lower end of the N-pole
and at the upper end of the S-pole, therefore at these two
poles, the armature flux strengthens the main field flux.
 GNA MNA
Likewise, the armature flux weakens the main field flux at
Upper end of the N-pole and at lower end of the S-pole.
fΦ
aΦ RΦ
θ
Now, if there is no magnetic saturation, then the amount
of strengthening and weakening of the main field flux are
equal and the resultant flux per pole remains unaltered
from its no load value.
Actually, the magnetic saturation does occurs and as a
consequence, the strengthening effect is less as compared
to the weakening effect and the resultant flux is decreased
from its no-load value. This is called ‘Demagnetizing
effect of armature reaction’
Conclusion
It may therefore be stated from the above that net effect of
armature flux on the main field flux is:-
1) To distort the main field flux thereby causing non-uniform
distribution of flux under the main poles.
2)To shift the MNA in the direction of the rotation for a
generator and against the direction of rotation for a
motor.
3)To reduce the main field flux from its no-load value due to
magnetic saturation.

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Armature reaction

  • 1. What is Armature Reaction?? Armature reaction is the effect of armature produced flux on the main field flux. The armature mmf produces two undesirable effects on the main field flux and these are:- 1) Net reduction in the main field flux per pole. 2)Distortion of the main field flux wave along the air- gap periphery.
  • 2. How it takes place?? From the fig(A) it shows that the flux path for the main poles of a 2-pole DC machine at no load ie. With no armature currents. This main field flux, produced by GNA field mmf If Nf , is shown by horizontal MNA Phasor OA= . O A fΦ fΦ
  • 3. Now when the DC machine is loaded, current flows in the armature windings. These currents are as shown in the figure (B), these currents set up armature flux shown by the vertical flux lines, with the field winding unexcited. The other figure represent armature flux Φa by a vertical phasor OB. GNA  O  B aΦ
  • 4. Now by examination of the above two figures reveals that the path of armature flux Φa is perpendicular to the main flux path Φf . In other words, the path of the armature flux crosses the path of the main field flux. O A B Thus the effect of armature flux on the main field flux is entirely ‘cross-magnetizing’ and it is for this reason that the flux produced by armature mmf is called cross-flux. fΦ aΦ
  • 5. Now when the current flows in both the armature and field windings, the resultant flux distribution is obtained by superimposing the two fluxes of fig (A) and fig(B).
  • 6. From the fig(C)shown below, it is seen that the armature flux aids the main field flux at the lower end of the N-pole and at the upper end of the S-pole, therefore at these two poles, the armature flux strengthens the main field flux.  GNA MNA Likewise, the armature flux weakens the main field flux at Upper end of the N-pole and at lower end of the S-pole. fΦ aΦ RΦ θ
  • 7. Now, if there is no magnetic saturation, then the amount of strengthening and weakening of the main field flux are equal and the resultant flux per pole remains unaltered from its no load value. Actually, the magnetic saturation does occurs and as a consequence, the strengthening effect is less as compared to the weakening effect and the resultant flux is decreased from its no-load value. This is called ‘Demagnetizing effect of armature reaction’
  • 8. Conclusion It may therefore be stated from the above that net effect of armature flux on the main field flux is:- 1) To distort the main field flux thereby causing non-uniform distribution of flux under the main poles. 2)To shift the MNA in the direction of the rotation for a generator and against the direction of rotation for a motor. 3)To reduce the main field flux from its no-load value due to magnetic saturation.