power system fundamentals ee 317 lecture 8 25 october 2010

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Power System Power System Fundamentals Fundamentals EE 317 EE 317 Lecture 8 Lecture 8 25 October 2010

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Page 1: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Power System Power System FundamentalsFundamentalsPower System Power System FundamentalsFundamentals

EE 317 EE 317 Lecture 8Lecture 8

25 October 2010

Page 2: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Chapter 5Chapter 5

Synchronous Machine Construction Speed of Rotation Voltage of a Synchronous Generator Phasor Diagrams of a Synchronous Generator Synchronous Generator Operating Alone Synchronous Motors Synchronous Machine Construction

Page 3: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Synchronous MachinesSynchronous Machines

Motors and generators whose magnetic field current for the rotor is supplied by a separate DC power source

Synchronous generators are used to produce nearly all the electric power produced in the world

Page 4: Power System Fundamentals EE 317 Lecture 8 25 October 2010

ConstructionConstruction

STATOR or

Armature Windings

ROTOR or

Field Windings

N

S

N S

Page 5: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Field windings…Field windings… Salient pole: constructed in a manner that it

protrudes from the surface of rotor

Page 6: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Field windings…Field windings… Nonsalient pole: constructed flush with the

surface of the rotor (see Figure 5-1, p. 193)

Page 7: Power System Fundamentals EE 317 Lecture 8 25 October 2010

How we create the DC current for the Rotor Magnetic field…

How we create the DC current for the Rotor Magnetic field…

External Source: DC currents created by slip rings and brushes (lead to higher maintenance and power/voltage drop across brushes)

Brushless Exciter: small AC generator with field circuit mounted on stator and the armature mounted on the rotor creating 3- AC currents. A 3- rectifier changes AC to DC for the main field

Page 8: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Completely independentCompletely independent Pilot Exciter – uses permanent magnets on

rotor to induce 3- AC currents in the armature which then produce exciter fields in armature leading to 3- AC currents in the rotor…etc.

Redundancy – many synchronous generators that use brushless exciters also have slip rings and brushes so that an auxiliary method for making DC is available in emergencies

Page 9: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Exciter circuit diagramsExciter circuit diagrams

See board

Page 10: Power System Fundamentals EE 317 Lecture 8 25 October 2010

What is relationship?What is relationship? Of electrical frequency and speed of the

mechanical (prime mover) device?

Where:fe = electrical frequency in Hznm = mechanical speed of field in rpm (rotor speed)P = number of magnetic poles

Page 11: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Voltage of a Sync. Gen.Voltage of a Sync. Gen. From chapter 4:

Simplifying for what is controllable during operation:

Page 12: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Equivalent circuit of a sync. gen.Equivalent circuit of a sync. gen. The internal voltage EA is not usually equal to the output

voltage V of a synchronous generator due to 4 factors:Armature reactionSelf-inductance of armature coilsResistance of armature coilsEffects of salient pole rotor shapes

The revised equation for output voltage V :

Page 13: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Phasor Diagrams of Sync. MachinesPhasor Diagrams of Sync. Machines

.a a a sV E jI X

Page 14: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Power and Torque in sync. gen.Power and Torque in sync. gen.

Page 15: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Measuring sync. gen. parametersMeasuring sync. gen. parameters The model equation for sync gen output voltage V :

To model the overall sync gen we need to know:Relationship between field current and fluxSynchronous reactance (XS) of the generator

Armature resistance (RA)

Page 16: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Measuring the model parametersMeasuring the model parameters Open-circuit test: loads are disconnected

(terminals are open), field current is zero, construct plot of EA = V vs. field current IF this determines air-gap line and overall OCC

Short-circuit test: loads are disconnected terminals are shorted, field current is zero, construct plot of IA vs. field current IF this determines the overall SCC

Page 17: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Modeling sync. gen. parametersModeling sync. gen. parameters The model equation for sync gen armature current IA :

Since R is much smaller than X we can approximate X at any given point by the following process:

Get EA from OCC at given field current

Find short circuit current flow (IA) from SCC at field current

Calculate Synchronous reactance (XS) of the generator

Page 18: Power System Fundamentals EE 317 Lecture 8 25 October 2010

EquationsEquations

Page 19: Power System Fundamentals EE 317 Lecture 8 25 October 2010

LimitationsLimitationsThis approximation only is accurate up

to the knee in the saturation curve of the OCC, its value as a true approximation of X reduces as saturation increases

Page 20: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Sync. gen. Operating alone

Sync. gen. Operating alone

What happens as load (of constant power factor) is increased on generator?

(a) lagging power factor (inductive loads)(b) unity power factor(c) leading power factor (capacitive loads)

Page 21: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Generator responseGenerator response (a) V and VT decrease significantly

(b) slight decrease in V and VT

(c) a rise in V and VT

Page 22: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Voltage regulationVoltage regulation Normally desirable to keep the voltage out of a

generator constant even when loads are varying. How can this be done? Since EA = K which one do you think we can

most easily vary? Why? and How?

Page 23: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Changing the Field Resistor FR

Changing the Field Resistor FR

1. Decreasing field resistance increases field current

2. Increases in field current increase flux 3. Increase in flux increases EA

4. An increase in EA leads to increase in V and VT

PROCESS IS REVERSIBLE

Page 24: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Comparing voltage regulation

Comparing voltage regulation

the model equation for voltage regulation is defined as:

Since R is much smaller than X we can approximate X at any given point by the following process:

Get EA from OCC at given field currentFind short circuit current flow (IA) from SCC at field currentCalculate Synchronous reactance (XS) of the generator

Page 25: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Synchronous motorsSynchronous motors Same as generators All the same equations apply Only differences are in phasor diagrams

Also when maximum torque is exceeded rotor will start to slip

Page 26: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Chapter 6Chapter 6 Rationale for paralleling Conditions for paralleling Procedure for paralleling Characteristics of a Synchronous Generator Operation with an Infinite Bus Operating with another of similar size

Page 27: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Paralleling generatorsParalleling generatorsWhy?

Higher loadsIncreased reliability under failureMaintenanceMore efficient operation of the fleet

Page 28: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Conditions for parallelingConditions for paralleling Rms line voltages must be equal Same phase sequence Phase angles must be equal Frequency of new generator (oncoming unit)

must be slightly higher the frequency of the running system

Page 29: Power System Fundamentals EE 317 Lecture 8 25 October 2010

procedureprocedure First – verify terminal voltage of oncoming

generator equals line voltage of system Second – verify that the phase sequence of the

oncoming generator is the same as the phase sequence of the running system (motor, bulbs, synchroscope)

Third – adjust the frequency of the oncoming unit to be slightly higher than the frequency of the running system

Page 30: Power System Fundamentals EE 317 Lecture 8 25 October 2010

Ch. 7 - Induction MachinesCh. 7 - Induction Machines Motors and generators whose magnetic field

current is supplied by magnetic induction (transformer action) into the field windings of the rotor (a DC power source is not required)

Although induction machines can be motors or generators they have many disadvantages as generators. Thus, they are referred to typically as induction motors. Most popular type of AC motor