The equivalent-circuit model for one armature phase of a cylindrical rotor three phase synchronous motor is shown in Figure below exactly similar to that of a synchronous generator except that the current flows in to the armature from the supply. Applying Kirchhoff’s voltage law to Figure below
VT = IaRa + jIaXl + jIaXas +
Ef
Combining reactances, Xs = Xl +
Xas
VT = Ef + Ia(Ra + jXs)
or VT = Ef + IaZs
where:
Ra = armature resistance (/phase)
Zs = synchronous impedance
(/phase)
VT = applied voltage/phase (V)
Ia = armature current/phase (A)
A phasor diagram shown in Figure above,
illustrates the method of determining the counter EMF which is obtained from
the phasor equation;
Ef = VT − IaZs
The
phase angle δ between the terminal voltage VT and the excitation voltage Ef in
Figure above is usually termed the torque angle. The
torque angle is also called the load angle or power angle.
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