ems ch13 ppt

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UNIVERSITY OF TECHNOLOGY, SYDNEY UNIVERSITY OF TECHNOLOGY, SYDNEY FACULTY OF ENGINEERING FACULTY OF ENGINEERING 48531 Electromechanical Systems 48531 Electromechanical Systems Introduction to Conventional Introduction to Conventional AC and DC Machines AC and DC Machines Topics to cover: 1. Introduction 2. DC Machines 3. Synchronous Machines 4. Induction Machines Introduction Introduction Conventional rotating machines are very commonly used in industrial drive systems. They can be energized either directly by conventional AC and DC power supplies, or by power electronic converters/inverters, especially in varibale speed drives. According to the operational principles and power supplies, they can be classified as: DC machines, -- DC power supplies; Synchronous machines, -- speeds proportional to the supply frequency; and Induction machines, -- rotor emf and current are induced by rotating magnetic field DC Machines DC Machines - Basic Principles: Induced emf - Basic Principles: Induced emf Induced emf in elementary AC and DC machines DC Machines DC Machines - Basic Principles: Electromagnetic Torque - Basic Principles: Electromagnetic Torque Uni-directional torque in an elementary DC machine

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Page 1: Ems Ch13 Ppt

UNIVERSITY OF TECHNOLOGY, SYDNEYUNIVERSITY OF TECHNOLOGY, SYDNEYFACULTY OF ENGINEERINGFACULTY OF ENGINEERING

48531 Electromechanical Systems48531 Electromechanical Systems

Introduction to ConventionalIntroduction to ConventionalAC and DC MachinesAC and DC Machines

Topics to cover:

1. Introduction 2. DC Machines

3. Synchronous Machines 4. Induction Machines

IntroductionIntroductionConventional rotating machines are very commonly used inindustrial drive systems. They can be energized either directly byconventional AC and DC power supplies, or by power electronicconverters/inverters, especially in varibale speed drives.

According to the operational principles and power supplies, they canbe classified as:

DC machines, -- DC power supplies;

Synchronous machines, -- speeds proportional to the supply

frequency; and

Induction machines, -- rotor emf and current are induced by

rotating magnetic field

DC MachinesDC Machines- Basic Principles: Induced emf- Basic Principles: Induced emf

Induced emf in elementary AC and DC machines

DC MachinesDC Machines- Basic Principles: Electromagnetic Torque- Basic Principles: Electromagnetic Torque

Uni-directional torque inan elementary DC machine

Page 2: Ems Ch13 Ppt

DC MachinesDC Machines- Structures: Electromagnet Poles- Structures: Electromagnet Poles Cut away view of

a DC Machine

DC MachinesDC Machines- Structures: Electromagnetic Poles (Cont.)- Structures: Electromagnetic Poles (Cont.)

Cross section ofa DC machine

DC MachinesDC Machines- Structures: Permanent Magnet Poles- Structures: Permanent Magnet Poles

Dis-assembled view ofa PM DC Machine

DC MachinesDC Machines- Structures: Permanent Magnet Poles (Cont.)- Structures: Permanent Magnet Poles (Cont.)

Cross section of aPM DC Machine

Page 3: Ems Ch13 Ppt

DC MachinesDC Machines- Structures: Permanent Magnet Poles (Cont.)- Structures: Permanent Magnet Poles (Cont.)

Dis-assembled view ofa PM DC Machine

DC MachinesDC Machines- Structures: Permanent Magnet Poles (Cont.)- Structures: Permanent Magnet Poles (Cont.)

Dis-assembled view ofa PM DC Machine

DC MachinesDC Machines- Windings- Windings

A DC machinewinding (lap)

DC MachinesDC Machines- Induced Emf- Induced Emf

Waveforms of induced emf

Page 4: Ems Ch13 Ppt

DC MachinesDC Machines- Schematic Representation- Schematic Representation

Symbol of a DC machine

DC MachinesDC Machines- Field Circuit Connection- Field Circuit Connection

Four field circuit connections

DC MachinesDC Machines- Emf and Torque- Emf and Torque

Assume the flux linkage of a single turn coil due to the stator magnetsvaries with time sinusoidally:

The induced emf then can be calculated by

The commutator rectifies AC into DC, and

therefore,

λ λ ωs m m t= 2 s in

ed

d ttm= =

ΦΦω ωco s

e td ta m m= =∫1 2

2

3 2

πω ω ω

πω

π

πΦ Φco s

For an armature winding of a great number of coils, the emf is

The electromagnetic power must balance the internal mechanicalpower, or Therefore,P E I Tem a a em r= = ω

TP

K Iemem

ra m a= =

ωΦ

E Ka a m r= Φ ω

DC MachinesDC Machines- Equivalent Circuit: Generator- Equivalent Circuit: Generator

Equivalent circuit of a separateexcited generator

Page 5: Ems Ch13 Ppt

DC MachinesDC Machines- Equivalent Circuit: Motor- Equivalent Circuit: Motor

Equivalent circuit of aseparately excited DC motor

DC MachinesDC Machines- DC Generators- DC Generators

Conditions for terminalvoltage build-up:

1) Residual magnetism

2) Connection ofarmature winding tofield winding such thatthe generated field aidsthe residual magneticfield;

3) The field circuitresistance smaller thanthe critical resistance

DC MachinesDC Machines- DC Generators (Cont.)- DC Generators (Cont.)

External characteristics of different DC generators

DC MachinesDC Machines- Drive Systems- Drive Systems

Ward-Leonard System

Page 6: Ems Ch13 Ppt

DC MachinesDC Machines- Drive Systems (Cont.)- Drive Systems (Cont.)

Power Electronic Drive System

0

Separately Excited

Shunt Motor

Series Motor

Motor

Compound Motorω0

DC MachinesDC Machines- Torque/Speed Curves- Torque/Speed Curves

Torque/speed curves of different DC motors

Synchronous MachinesSynchronous Machines- Structures: Generators- Structures: Generators

Hydroelectric synchronous generator

Synchronous MachinesSynchronous Machines- Structures: Generators- Structures: Generators

Hydroelectricsynchronousgenerator

Page 7: Ems Ch13 Ppt

Synchronous MachinesSynchronous Machines- Structures: Generators- Structures: Generators

Stator of aturbinegenerator

Synchronous MachinesSynchronous Machines- Structures: Generators- Structures: Generators

Rotor of a turbine generator

Synchronous MachinesSynchronous Machines- Structures: Motors- Structures: Motors

Synchronous motor

Synchronous MachinesSynchronous Machines- Structures: Motors- Structures: Motors

Permanent magnet motors

Page 8: Ems Ch13 Ppt

Synchronous MachinesSynchronous Machines- Electrical and Mechanical Engles- Electrical and Mechanical Engles

Elementary two polesynchronous machine

Synchronous MachinesSynchronous Machines- Electrical and Mechanical Engles (Cont.)- Electrical and Mechanical Engles (Cont.)

Elementary four polesynchronous machine

θ θ=P

m2ω ω=

Pm2and

Synchronous MachinesSynchronous Machines- Rotating Field (Cont.)- Rotating Field (Cont.)

Phase winding positionsand phase currents

Synchronous MachinesSynchronous Machines- Rotating Field (Cont.)- Rotating Field (Cont.)

Positions of rotating field at different time

Page 9: Ems Ch13 Ppt

t=0

θπ/ 2 π π/ 23 π20

F1

t= ωπ

Synchronous MachinesSynchronous Machines- Rotating Field (Cont.)- Rotating Field (Cont.)

Rotating mmf wave

( )F F F FF

ta b cm

1 1 1 1

3

2= + + = −cosθ ω

Synchronous MachinesSynchronous Machines- Rotating Field (Cont.)- Rotating Field (Cont.)

The speed in electrical rad/s of the rotating field is

ωθ π

π ωωf

d

dt= = =

2

2

ωω

f P=

2

nf

Pf

f= =60

2

120ωπ

In rev/min, it is

In mechanical rad/s,

Synchronous MachinesSynchronous Machines- Equivalent Circuit- Equivalent Circuit

Equivalent Circuit for synchronous (a) genarators and (b) motors

(Xs>>Ra for large synchronous machines)

Ea

jXs Ra Ia

Va Ea

jXs Ra Ia

Va

(a) (b)

Synchronous MachinesSynchronous Machines- Phasor Diagrams- Phasor Diagrams

Phasor diagrams for synchronous (a) genarators and (b) motors(a) (b)

Va

I a

jXsI a

δEaϕVa

I a

jXsI a

δϕ

Ea

Page 10: Ems Ch13 Ppt

Synchronous MachinesSynchronous Machines- Generator Characteristics- Generator Characteristics Synchronous MachinesSynchronous Machines

- Torque/Load Angle Curve- Torque/Load Angle Curve

TE V

Xa a

f s

=3

ωδsin

InductiveLoad

SynchronousCondenser

Three PhasePower Supply I loadI s

I cmp

Synchronous MachinesSynchronous Machines- Power factor Compensation- Power factor Compensation

Schematic illustration of power factor compensationusing synchronous condensers

( ) ( )Im ImI Icmp load= −

Ea sinδ

I a cosϕ

I a2

δδ 1

ϕ3

Ea1 Ea2 Ea3

Va

jX sI a1 jX sI a2

jX sI a3

I a3

δδ 2 δδ 3ϕ

1

I a1

Synchronous MachinesSynchronous Machines- Power factor Compensation (Cont.)- Power factor Compensation (Cont.)

Phasoe diagram of power factor control by controlingrotor excitation of a synchronous machine

Page 11: Ems Ch13 Ppt

Synchronous MachinesSynchronous Machines- V Curves- V Curves Synchronous MachinesSynchronous Machines

- Speed Control- Speed Control

Synchonous motor speedcontrol: Variable Voltageand Variable Frequency(VVVF)

Induction MachinesInduction Machines- Structures- Structures

Cut away viewof a wound rotorinduction motor

Induction MachinesInduction Machines- Structures- Structures

Wound rotorof an inductionmotor

Page 12: Ems Ch13 Ppt

Induction MachinesInduction Machines- Structures (Cont.)- Structures (Cont.)

Cut away view ofa squirrel cageinduction motor

Induction MachinesInduction Machines- Structures (Cont.)- Structures (Cont.)

Squirrel cagerotor of aninduction motor

Induction MachinesInduction Machines- Equivalent Circuit- Equivalent Circuit

T equivalent circuit of induction motors

V 1

I 1R1 jX l1

jX m

jX'l2R'2 I'2

E 1R'2

1-ss

where slip sf r

f

=−ω ω

ω

Induction MachinesInduction Machines- Torque/Speed Curve- Torque/Speed Curve

( )T

VR

s

RR

sX Xf

l l

=+

+ +

3 12 2

12

2

1 2

'

''

Page 13: Ems Ch13 Ppt

Induction MachinesInduction Machines- Speed Control- Speed Control

Methods for induction motor speed control:

1) Varying number of poles,

2) Varying terminal voltage,

3) Varying rotor winding resistance,

4) Rotor power recovery, and

5) Variable voltage variable frequency (VVVF).

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motor speed control by varying number of poles

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motor speed control by varying number of poles

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motorspeed control byvarying terminalvoltage

Page 14: Ems Ch13 Ppt

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motorspeed control byvarying rotorwinding resistance

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motor speed control by rotor power recovery

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Induction motor speed control by variable voltagevariable frequency (VVVF).

Induction MachinesInduction Machines- Speed Control (Cont.)- Speed Control (Cont.)

Torque/speedcurve of VVVFspeed control