Blondel's Two Reaction Theory (Theory of Salient Pole Machine) : part 1
It is known that in case of nonsalient pole type alternators the air gap is uniform. Due to uniform air gap, the field flux as well as armature flux very sinusoidally in the air gap. In nonsalient rotor alternators, air gap length is constant and reactance is also constant. Due to this the m.m.f.s of armature and field act upon the same magnetic circuit all the time hence can be added vectorially. But in salient pole type alternators the length of the air gap varies and the reluctance also varies. Hence the armature flux and field flux cannot vary sinusoidally in the air gap. The reluctances of the magnetic circuits on which m.m.fs act are different in case of salient pole alternators.
It is known that in case of nonsalient pole type alternators the air gap is uniform. Due to uniform air gap, the field flux as well as armature flux very sinusoidally in the air gap. In nonsalient rotor alternators, air gap length is constant and reactance is also constant. Due to this the m.m.f.s of armature and field act upon the same magnetic circuit all the time hence can be added vectorially. But in salient pole type alternators the length of the air gap varies and the reluctance also varies. Hence the armature flux and field flux cannot vary sinusoidally in the air gap. The reluctances of the magnetic circuits on which m.m.fs act are different in case of salient pole alternators.
Hence the armature and field m.m.f.s cannot be treated in a simple way as they can be in a nonsalient pole alternators.
The theory which gives the method of analysis of the distributing
effects caused by salient pole construction is called two reaction
theory. Professor Andre Blondel has put forward the two reaction theory.
Note : According to this theory the armature m.m.f. can be divided into two components as,
1. Components acting along the pole axis called direct axis
2. Component acting at right angles to the pole axis called quadrature axis.
FAR : }
Fq = Component along quadrature axis
Id = Component along direct axis
Ia : }
Iq = Component along quadrature axis
2. Component acting at right angles to the pole axis called quadrature axis.
The component acting along
direct axis can be magnetising or demagnetising. The component acting
along quadrature axis is cross magnetising. These components produces
the effects of different kinds.
The Fig. 1 shows the stator m.m.f. wave and the flux distribution in
the air gap along direct axis and quadrature axis of the pole.
Fig. 1 Flux distribution in air gap for salient pole machine |
The relucatnce offered to
the m.m.f. wave is lowest when it is aligned with the field pole axis.
This axis is called direct axis of pole i.e. d-axis. The relucatnce
offered is highest when the m.m.f. wave is oriented at 90 to the field
pole axis which is called quadrature axis i.e. q-axis. The air gap is
least in the centre of the poles and progressively increases on moving
away from the centre. Due to such shape of the pole-shoes, the field
winding wound on salient poles produces the m.m.f. wave which is nearly
sinusoidal and it always acts along the pole axis which is direct axis.
Let Ff
be the m.m.f. wave produced by field winding, then it always acts along
the direct axis. This m.m.f. is responsible to produce an excitation
e.m.f. Ef which lags Ff by an angle 90o .
When armature carries current, it produces its own m.m.f. wave FAR. This can be resolved in two components, one acting along d-axis (cross-magnetising). Similarly armature current Ia also can be divided into two components, one along direct axis and along quadrature axis. These components are denoted as,
: Fd = Component along direct axisFAR : }
Fq = Component along quadrature axis
Id = Component along direct axis
Ia : }
Iq = Component along quadrature axis
The positions of FAR, Fd and Fq in
space are shown in the Fig. 2. The instant chosen to show these
positions is such that the current in phase R is maximum positive and is
lagging Ef by angle Ψ.
Fig. 2 M.M.F. wave positions in salient pole machine |
The phasor diagram corresponding to the positions considered is shown in the Fig. 3. The Ia lags Ef by angle Ψ.
It can be observed that Fd is produced by Id which is at 90o to Ef while Fq is produced by Iq which is in phase with Ef .
The flux components of ΦAR which are Φd and Φq along
the direct and quadrature axis respectively are also shown in the
Fig.3. It can be denoted that the reactance offered to flux along direct
axis is less than the reactance offered to flux along quadrature axis.
Due to this, the flux ΦAR is no longer along FAR or Ia. Depending upon the reluctances offered along the direct and quadrature axis, the flux ΦAR lags behind Ia.
Fig 3 Basic phasor diagram for salient pole machine |
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