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Synchronous Machines - E-Courses

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Electrical <strong>Machines</strong> II Prof. Krishna Vasudevan, Prof. G. Sridhara Rao, Prof. P. Sasidhara Rao<br />

Thus Eo is the e.m.f. corresponding to the flux produced by the field winding only,<br />

while E is that actually produced by the resultant flux due to the combined effect of stator<br />

and rotor ampere-turns. The actual e.m.f. E can be considered as Eo plus a fictitious e.m.f.<br />

proportional to the armature current.<br />

Eo<br />

Eo Er<br />

E<br />

Er<br />

Er<br />

E<br />

Indian Institute of Technology Madras<br />

I<br />

Er<br />

Er<br />

(a)Generator (b)Motor unity power factor<br />

I<br />

(c) Generator (d)Generator zero power factor<br />

Figure 25: Pertaining to <strong>Synchronous</strong> Reactance<br />

I<br />

I<br />

Er<br />

E Eo<br />

Fig. 25 is redrawn in this manner to correspond with part (b) of Figures 1 to<br />

4, introducing the fictitious emf. Er such that the following phasor relationship is satisfied:<br />

E = Eo + Er<br />

It can be seen from Fig. 25, that Er, is always in phase-quadrature with armature current and<br />

proportional to it (as per the four assumptions (1) to (4) above). The emf Er is thus similar<br />

36<br />

V<br />

Er<br />

Eo<br />

Eo<br />

E<br />

Er<br />

(20)

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