Short notes

Synchronous Machine Short Notes

The 11 kV turbo-alternator in a thermal power plant has a cylindrical rotor spinning at 3000 RPM (for 2-pole, 50 Hz operation). A hydro plant running at 150 RPM needs 40 poles to achieve 50 Hz output — that is why hydro alternators are large-diameter salient-pole machines while turbo-alternators are long and thin.

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How it works

The synchronous machine's rotor field (set by DC excitation current If) interacts with the stator rotating MMF to produce torque. The phasor diagram for a cylindrical rotor generator gives V = E − jIaXs − IaRa (Ra usually negligible). Active power P = (EV sinδ)/Xs per phase, where δ is the power angle between E and V; reactive power Q = (EV cosδ − V²)/Xs. If excitation is increased (over-excitation), Q becomes positive — machine supplies reactive power to the grid, acting like a capacitor bank. Under-excitation absorbs reactive power.

Key points to remember

Synchronising power is the restoring power when δ deviates from steady state: dP/dδ = (EV cosδ)/Xs, maximum at δ = 0° and zero at δ = 90°. Steady-state stability limit is P = EV/Xs at δ = 90°. Salient-pole machines have two reactances: Xd (direct axis, 0.8–1.2 pu) and Xq (quadrature axis, 0.5–0.8 pu), giving higher reluctance torque. V-curves show armature current Ia vs field current If at constant power: the minimum of each V-curve corresponds to unity power factor operation.

Exam tip

The examiner always asks you to draw the phasor diagram for a salient-pole synchronous generator at lagging power factor and identify the power angle δ — practice this diagram including both the Id and Iq components.

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