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 />
2.8.4 Unsaturated <strong>Synchronous</strong> Impedance<br />
The open circuit and short-circuit characteristics are represented on the same graph<br />
in Fig. 29. The field current 08 produces a line-to line voltage oc on the air- gap line, which<br />
would be the open-circuit voltage if there were no saturation. The same value of field current<br />
produces the armature current o’d and the unsaturated synchronous reactance is<br />
Indian Institute of Technology Madras<br />
Zdu = oc<br />
√ 3o ′ d Ω phase,forastar connected armature (24)<br />
When the open-circuit characteristic, air-gap line, and the short-circuit characteristic<br />
are plotted in per-unit, then the per unit value of unsaturated synchronous reactance equals<br />
the per-unit voltage on the air-gap line which results from the same value of field current<br />
as that which produces rated short-circuit (one-per unit) armature current. In Fig. 29 this<br />
would be the per-unit value on the air gap line corresponding to the field current og.<br />
3 <strong>Synchronous</strong> Generator Operation<br />
3.1 Cylindrical Rotor Machine<br />
The synchronous generator, under the assumption of constant synchronous reactance,<br />
may be considered as representable by an equivalent circuit comprising an ideal winding<br />
in which an e.m.f. Et proportional to the field excitation is developed, the winding being<br />
connected to the terminals of the machine through a resistance r and reactance (X+Xa) = Xs<br />
all per phase. This is shown in fig. 30. the principal characteristics of the synchronous<br />
generator will be obtained qualitatively from this circuit.<br />
3.1.1 Generator Load Characteristics<br />
Consider a synchronous generator driven at constant speed and with constant excitation.<br />
On open circuit the terminal voltage V is the same as the open circuit e.m.f. Et<br />
Suppose a unity-power-factor load be connected to the machine. The .flow of load current<br />
produces a voltage drop Izs in the synchronous impedance, and terminal voltage V is reduced.fig.<br />
31 shows the complexor diagram for three values of load. It will be seen that<br />
the angle σ between Et and V increases with load, indicating a shift of he flux across the<br />
pole faces due to cross- magnetization. The terminal voltage is obtained from the complex<br />
summation<br />
V + Iz, = EtorV = E − Iz8<br />
(25)<br />
42