School of Electrical and Computer Engineering Applied Electronics and Electrical Machines (ELEC 365) Fall 2015 Synchronous Machines 1 INTRODUCTION ο The bulk of electric power is generated by synchronous generators. ο They operate at constant speed (ππ ) and constant frequency under steadystate conditions. ο Can operate either as a generator or as a motor. ο Power ratings up to several hundred MVA are common. ο Many generators operate in parallel, even if one generator does not supply any load, this m/c is kept on the bus. 2 CONSTRUCTION DETAILS Stator: Similar to induction motor, 3-phase distributed windings. Rotor: Field winding (DC supply). Two types of m/c. (a) High speed m/c Round or cylindrical rotor. No protruding parts. Used in turbo-generators (steam and gas turbines). [e.g.: 2-pole, 60-Hz, ππ = 3600 rpm]. (b) Low-speed m/c Salient pole rotors. Hydro-electric and diesel electric generators. [e.g.: 12-pole, 60-Hz, ππ = 600 rpm. Large number of poles to produce desired frequency at low speed.] Cooling: Air + coolant (water, hydrogen and helium). To cool both windings and magnetic structures. 3 CONSTRUCTION DETAILS Basic structure of the three-phase synchronous machine. 4 CONSTRUCTION DETAILS Salient rotor The rotating speed delivered to the 4-pole generator needs to be 1500 RPM (50 hertz) or 1800 RPM (60 hertz). Cylindrical rotor 15 MW 11 KV 3000 RPM 2 Pole rotor for Paper Mills company. 5 CONSTRUCTION DETAILS Damper Bars: Under steady-state m/c runs at synchronous speed (ππ ). However, synchronous machine undergoes transients during starting and abnormal conditions – rotor may undergo mechanical oscillations and speed may vary from synchronous speed. This is not desirable. To overcome this problem: additional windings (similar to cage of an induction motor) on the rotor, currents are induced in the damper bars, producing a restoring torque to bring the speed to ππ . They also provide a starting torque, 6 CONSTRUCTION DETAILS Synchronous motor rotor with amortisseur winding. 7 Field Supply Field Supply: (a) Supply through slip rings and brushes. (i) DC excitation by self-excited DC m/c mounted on the same shaft. (ii) In low speed machines (hydro-electric generator): A pilot exciter excites the main exciter. (iii) Solid state excitation systems: ac-to-dc or dc-to-dc power electronic converters supply the field through brushes and slip rings. (b) Rotating rectifier (Brushless system): no brushes or slip rings, rectifier on the shaft. 10 Field Supply A brushless exciter circuit 11 Field Supply To make the excitation of a generator completely independent of any external power source, a small pilot exciter is often added to the circuit. The pilot exciter is an AC generator with a permanent magnet mounted on the rotor shaft and a 3-phase winding on the stator producing the power for the field circuit of the exciter. 12 Example 1 In a factory a 3 phase, 4 kV, 400 kVA synchronous machine is installed along with other induction motors. The following are the loads on the machines: Induction motors: 500 kVA at 0.8 PF Lagging. Synchronous motor: 300 kVA at 1.0PF. a) Compute the overall power factor of the factory loads. b) To improve the factory power factor, the synchronous machine is overexcited (to draw leading current) without any change in its load. Without over loading the motor, to what extent can the factory power factor be improved? Find the current and power factor of synchronous motor for this condition. 13 Example 1 Solution : (a) Induction motors: Power = 500 × 0.8 = 400 kW Reactive Power = 500 × 0.6 = 300 kVAR Synchronous motor: Power = 300 kW Reactive Power = 0.0 Factory : Power = 700 kW Reactive Power = 300 kVAR Complex Power = 7002 + 3002 = 762 kVA Power factor = 700 762 = 0.92 lagging 14 Example 1 (b)The maximum leading kVAR that the synchronous motor can draw without exceeding its rating is 4002 − 3002 = 264.58 kVAR Factory kVAR = j300 – j 264.48 = j35.42 (i.e., lagging) New factory kVA = 7002 + 35.422 = 700.9 kVA 700 Improved factory factor = 700.9 = 0.996 Synchronous motor current: ISM = 400 kVA 3×4 kV = 57.75 A Synchronous motor power factor: PFSM = 300 kW 400 kVA = 0.75 lead 15 SYNCHRONOUS GENERATOR OPERATION Basis: Faraday’s law. Flux linking the coil changes in time. Therefore, voltage is induced in a coil. Voltage induced in Phase a: φ = flux per pole; ω = 2πf rad/sec.; f = frequency of induced voltage. Voltage induced in Phase b: Voltage induced in Phase c: General: πΈ0 = KΙΈf (rms or peak). 16 PERFORMANCE OF ROUND-ROTOR SYNCHRONOUS GENERATOR Fig.1: Per-phase equivalent circuit of armature. where ππ = synchronous impedance. = π π + jππ Ω ππ is called as synchronous reactance. 18 VOLTAGE REGULATION IN GENERATOR For the per-phase equivalent circuit shown in Fig.1: Generally ππ β« π π βΆ ∴ ππ ≅ πππ Percent voltage regulation= πΈ0 −|ππ‘ | |ππ‘ | × 100 Regulation can be positive, zero or negative depending on the power factor (PF) and the load. 21 PHASOR DIAGRAMS (Neglecting Ra) Per-phase armature equivalent circuit of a synchronous m/c neglecting the armature resistance π π . ππ is the per-phase synchronous reactance. 22 PHASOR DIAGRAMS (Neglecting Ra) Phasor diagram for a synchronous generator (neglecting π π ) with a lagging PF load. 23 GENERATOR From phasor diagram: δ = angle between πΈ0 and ππ‘ , called as POWER-ANGLE. Here generator action is assumed (δ > 0): Terminal (here load) voltage, ππ‘ , lags internal voltage, πΈ0 , by δ. Power developed (per-phase) ππ , is applied to the load. (Called as Power-Angle relation) 24 MOTOR Phasor diagram for a synchronous motor (neglecting Ra) with a lagging PF current 25 MOTOR Same as generator equation but with negative δ! Terminal (here supply) voltage, ππ‘ , leads internal voltage, πΈ0 , by δ. Power developed, ππ versus δ: δ < 0, motoring and δ > 0, generator 26 Taking the armature resistance Ra into account (GENERATOR) Per-phase armature equivalent circuit of a synchronous generator including the armature resistance π π . ππ is the per-phase synchronous reactance. 27 PHASOR DIAGRAM (Including Ra), Unity PF load Phasor diagram for a synchronous generator (including π π ) with a unity PF load 28 PHASOR DIAGRAM (Including Ra), Lagging PF (Generator) Phasor diagram for a synchronous generator (including Ra) with a lagging PF load. 29 PHASOR DIAGRAM (Including Ra), Leading PF (Generator) Phasor diagram for a synchronous generator (including π π ) with a leading PF load 30 EXPRESSIONS FOR ACTIVE AND REACTIVE POWERS (Taking Ra into account) Per-phase armature equivalent circuit of a synchronous generator including the armature resistance π π . ππ is the per-phase synchronous reactance Phasor diagram for a synchronous generator (including Ra) with a lagging PF load. 31 EXPRESSIONS FOR ACTIVE AND REACTIVE POWERS From the per-phase equivalent circuit: * From (*): 32 EXPRESSIONS FOR ACTIVE AND REACTIVE POWERS where Using the definition of complex power, where real power (per-phase) is given by and reactive power (per-phase) is given by 33 EXPRESSIONS FOR ACTIVE AND REACTIVE POWERS If Xs >> Ra : Torque (per-phase), Reactive power: 34 TORQUE – SPEED – POWER CHARACTEROSTICS Power and torque angel characteristics Torque – speed characteristic 35