Synchronous Machines - E-Courses
Synchronous Machines - E-Courses
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)