LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES

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ET 332b Ac Motors, Generators and Power Systems LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES 1 LEARNING OBJECTIVES After this presentation you will be able to: Interpret alternator phasor diagrams under different load conditions. Explain the infinite bus concept and compute power delivered to an infinite bus. Explain how alternators are synchronized. Define alternator stiffness. 2 1

ALTERNATOR OPERATION Synchronous machines can convert from motor to generator operation by having the shaft driven by a source of mechanical power Current exits for generator operation Note: reversal of current direction in machine electrical model 3 PHASOR DIAGRAMS OF MACHINE OPERATION Motor operation: d lags the terminal voltage V T. Armature current I a can either lead or lag V T depending on value of excitation. Leading I a Lagging I a 4 2

PHASOR DIAGRAMS OF MACHINE OPERATION Machine with no mechanical load or power output. The torque/power angle, d is 0 in this case E f1 d = 0 5 PHASOR DIAGRAMS OF MACHINE OPERATION Generator operation (Alternator) E f1 leads the terminal voltage for generator operation Power factor angle can either lag or lead depending on field excitation 6 3

ALTERNATOR CIRCUIT MODEL Synchronous Generator Equations and Model Circuit Power equation (Watts/phase) P in V T E X s f sin( d) I a reversed Note: equation is positive and d is positive for Alternator (generator) operation Voltage equation VT Ef Ia jx s Where: V T = terminal voltage/phase (V) E f = excitation voltage/phase (V) I a = armature current/phase (A) X s = synchronous reactance/phase (ohms) 7 GENERATOR LOADING Mechanical power converted to active power Exciter Excess field flux converted to reactive power P mech I dc Pe Prime Mover Generator ELECTRIC LOADS Prime Mover Torque Governor Electrical load produces counter-torque Q Speed Governor device that regulates speed to match electric load Increased electrical load produces counter torque that prime mover must overcome or prime mover slows down 8 4

INFINITE BUS CONCEPT In large power systems, V T and system frequency are assumed constant. Individual generators added to large system can not change V T and f. Good approximation when generator small with respect to all other generation connected Power Grid (100 s of interconnected generators. P sys = sum of all generator s outputs) System Tie Bus V T and f constant here Local Generator P o <<< P sys 9 INFINITE BUS EXAMPLE Example 20-1: 3-phase, 460 V, 2-pole, 60 Hz, wye-connected, synchronous alternator. X s = 1.26 ohm/phase. Connected to an infinite bus and supplies 117 kw with a power angle of 25 degrees. Neglect losses and find: a.) turbine torque supplied to alternator; b.) excitation voltage; c.) active, reactive power and machine power factor; d.) neglecting saturation effects of the field, the excitation voltage if the field current is reduced to 85% of its original value in part a; e.) the turbine speed for 60 Hz operation 10 5

EXAMPLE 20-1 SOLUTION (1) Find torque developed by prime mover to generate 117 kw neglecting losses Need synchronous speed 11 EXAMPLE 20-1 SOLUTION (2) Find the excitation voltage E f Solve for E f 12 6

EXAMPLE 20-1 SOLUTION (3) Part c.) Find S out P out and Q out of generator. Need armature current 13 EXAMPLE 20-1 SOLUTION (4) Find the power phasor using the following formulas 14 7

EXAMPLE 20-1 SOLUTION (5) Find the power factor and the change in excitation voltage 15 PARALLELING SYNCHRONOUS GENERATORS :Required initial conditions : Machines must have same phase sequence (order of voltages) (ABC) or (BAC). Incorrect phase sequence causes short circuit. Turbine speed should be a fraction of Hz faster than system to prevent motoring of generator V T 1.) Adjust voltage of incoming machine to match system voltage 3.) Close generator breaker 2.) Adjust frequency of incoming generator to match system f (Synchronize to system) 16 8

MEASURING SYSTEM/MACHINE FREQUENCY Synchroscope - instrument to determine if machine frequency is the same as system frequency. Instrument indicates fast-slow operation by comparing the frequencies of the two voltages (system-generator) Mathematically, phase shift is integral of frequency change t f f 0 s g (t) dt Where: = phase shift f s = system frequency f g (t) = generator frequency 17 SYNCH EXAMPLE Generator voltage lagging system voltage - crosses zero later in time Also cause rotor oscillations which cause the generator to be unstable D Closing Generator breaker with phase shifts of greater than 10 degrees causes high armature currents and will trip the generator off line 18 9

SYNCHRONIZING GENERATOR TO SYSTEM Increasing speed of prime mover increases frequency which reduces phase difference 19 SYNCHRONIZING GENERATOR TO SYSTEM Phase shift near zero at t s. Prime mover is accelerating the rotor ahead of the system voltage after this point. (V g leads V s ) Close generator breaker when phase is slightly leading system Machine will remain locked to system frequency after breaker is closed assuming infinite bus 20 10

STIFFNESS OF SYNCHRONOUS MACHINES Stiffness -Ability of a synchronous machine to resist forces that pull it out of synchronism. Slope of the power-angle curve around a given operating point Operating point in graph above is at d o 21 STIFFNESS OF SYNCHRONOUS MACHINES Remember power equation 3 VT P X E s f sin( d) To find slope, take derivative of P with respect to d. This is defined as the stiffness DP dp 3 VT Ef Ps Dd dd X s cos( d) Units of P s are watts/radian (or degree) 22 11

STIFFNESS OF SYNCHRONOUS MACHINES Example 20-2: A 3-phase 13.2 kv 60 Hz, 50 MVA wyeconnected cylindrical rotor synchronous generator has X s = 2.49 ohms/phase and an internally generated voltage at the operating point of 15,767 V LL with a power angle of 11.1 degrees. The machine has 8 poles. Determine: a.) the synchronizing power in MW/rad and MW/ mechanical degree b.) synchronizing torque in N-n/radian 23 EXAMPLE 20-2 SOLUTION (1) Find the per phase quantities of V T and E f from the line-to-line values 24 12

EXAMPLE 20-2 SOLUTION (2) Number of poles is 8, so... d e = (d m ) (P/2) b.) Now compute the synchronizing torque Compute synchronous speed Convert to Radians/second 25 ET 332b Ac Motors, Generators and Power Systems END LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES 26 13