ars p es 99slides jan10
TRANSCRIPT
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Recommended Text Books
1) Power Electronics - circuits, devices &applications by M H Rashid
2) Power Electronics - Principles andApplications by J Vithayathil
3) Introduction to Power Electronics byDenis Fewson
Topic1: Introduction
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This course deals with the techniques of designing high current
electronic circuits using power semiconductor devices, likeDiodes, Transistors and Thyristors.
The subject covers:
Power semiconductor devices, their working, characteristics,
protection, and drive circuits.
Power electronic converters for controlled rectification,
inversion, dc-dc conversion, and ac-ac conversion, are covered.
Applications of power electronic equipment with emphasis on
dc and ac motor drives.
Course Objectives:
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What is Power Electronics ?
Conversion and control of electricpower using semiconductor electronicdevices and related control techniques
Conversion: ac to dc ( rectification ), dc to ac ( inversion )
Control: To vary voltage, current, Hz, power etc
Note:
In Power Electronics applications, the devices operate in
switching (ON/OFF) mode only, rather than in the linear (active)
mode.
Topic1: Introduction
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What is Power Electronics? Contd.
Load
Controller
Power Circuit(Power Electronic
Converter)
Source
A C Mains ,
Battery,
etc
Motor
Power Input Power Output
Light
Heating
etc, etc
Ref Measurement
s
Control Signals
E
l
e
Electronic
Equipment
Topic1: Introduction
http://img.alibaba.com/photo/50160597/Waterproof_Electric_Heater.jpghttp://mirror-us-ga1.gallery.hd.org/_exhibits/light/_more2003/_more05/light-bulb-glowing-filament-light-blue-uncropped-3-AHD.jpg -
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ControlsDigital | Analog
ControlsDigital | Analog
Power ElectronicsPower Electronics
PowerEquipment
Static | Rotating
PowerEquipment
Static | Rotating
ElectronicsDevices | Circuits
ElectronicsDevices | Circuits
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Diodes, Transistors and Thyristors
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Comparison of Transistors & Thyristors
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DEVICE CLASSIFICATION according to
degree of controllability
Group I: Uncontrollable,
eg: Diodes
Group II: Semi-controllable,
eg: SCR, TRIAC
Group III:Fully-controllable,
eg: BJT, MOSFET, IGBT, GTO
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CONTROL CHARACTERISTICS
OF POWER DEVICES
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CONTROL CHARACTERISTICS OF POWER DEVICES (contd.)
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CONTROL CHARACTERISTICS OF POWER
DEVICES (contd.)
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CONTROL CHARACTERISTICS OF POWER
DEVICES (contd.)
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Voltage and Current Capabilities
Bipolar voltage withstanding capability(e.g. SCR, GTO,TRIAC).
Unipolar voltage withstanding capability
(e.g. BJT,MOSFET, IGBT, GTO, ).
Bidirectional current capability
(e.g. TRIAC, MOSFET ).
Unidirectional current capability
(e.g. SCR, GTO, BJT, IGBT, & Diode).
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What is Power Electronic
Converter ?
An Equipment whichaccepts electric powerfrom the existing
source (fixed V/Hz a.c,Battery etc.) andconverts it in acontrolled manner into
a suitable formcompatible with theparticular load.
Source
Converter
Set
Load
Source
Prof A Rashid, PNEC/NUST
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Power Electronic Converters
A C
A C D C
D C
RECTIFIERS(Controlled / Uncontrolled)
DC-DCCONVERTERS
INVERTERS
AC-AC
CONVERTERS
(DC Choppers)
AC Voltage
Controllers
Cycloconverters
DC Link
Converters
Prof A Rashid, PNEC/NUST
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POWER ELECTRONIC CONVERTERS
AC to DC: RECTIFIERAC to DC: RECTIFIER
DC to DC: CHOPPERDC to DC: CHOPPER
DC to AC: INVERTERDC to AC: INVERTER
AC to AC:AC to AC:
CYCLOCONVERTER, ACCYCLOCONVERTER, AC
VOTAGE CONTROLLERVOTAGE CONTROLLER
AC Input DC Output
DC Input DC Output
DC Input AC Output
AC Input AC Output
Prof A Rashid, PNEC/NUST
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Why Power Semiconductor
Converters?
1) High efficiency
2) Long Life
3) Low maintenance
4) Compact size
5) Low Cost
6) Fast response7) Low power consumption in their
control circuits
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A Si l Ph F ll W U t ll d R tifi Ci it (Di d F ll
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A Single Phase Full Wave Uncontrolled Rectifier Circuit (Diode Full
Wave Rectifier) using a Center Tapped Transformer
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Half-WaveControlled Rectifier
(a) Cicuit
V
(b) Waveforms
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A Single Phase Full Wave Controlled Rectifier
Circuit using a Center Tapped Transformer
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Full-Wave
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Single-Phase ac-ac converter
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CHOPPERS
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INVERTERS
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Static Switches
bidirectional
voltage blocking
and current
conduction
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INVERSIONUncontrolled and half-controlled rectifiers will
permit power to flow only from the a.c systemto d.c load and are therefore referred to asunidirectionalconverters.
In case of fully controlled rectifiers, it ispossible to transfer power from d.c side of therectifier back into the a.c system by controllingthe phase angle .
Such mode is known as inverting mode. Thefully controlled converter may therefore be
called as a Bidirectional converter.
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Inductive Smoothing of D.C Without L, the voltage waveform at M and N
has Ripple Voltage component in additionto dc component.
L will smooth out Ripple Voltage and makeit negligibly small.
Capacitor can also be connected in parallel,but in high power applications the capacitorwill draw too much charging current fromsupply band cause other problems.
In electronic circuits( light current)application capacitor is preferred.
(Ref. VIT p. 142)
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Applications of Controlled Rectifiers
1) DC Motor speed control
2) Electrochemical andElectrometallurgical
processes
3) Magnetic power supplies
4) Converters at the input end of dc
transmission line
5) Portable handtool drives
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Generalized Power Converter System
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Design of Power Electronics Equipment
1) Design of power circuits( Devices,
their ratings and configuration)
2) Protection of power devices (Fuse,Heat-Sink etc.)
3) Determination of control strategy
(Phase-angle control, ON-OFF control etc)
4) Design of logic and gating circuit.
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(c) Appearance
SCR Structure, Symbol and Appearance
A
K
G
PJ1
N
P
NJ2
J3
(a) Structure
Lesson Plan Topic 2.1
(b) Symbol
Anode
Cathode
Gate
Low
Power
Medium
Power
http://images.google.com.pk/imgres?imgurl=https://www.alliedelec.com/Images/Products/Small/935-3546.jpg&imgrefurl=https://www.alliedelec.com/Search/ProductDetail.aspx%3FSKU%3D9353546%26MPN%3DNTE5569%26R%3D9353546%26SEARCH%3D9353546%26DESC%3DNTE5569&h=200&w=200&sz=6&hl=en&start=38&usg=__n6jdEoIXLreFjd9x7wKShkZcdeQ=&tbnid=3_54I90sV8ksOM:&tbnh=104&tbnw=104&prev=/images%3Fq%3Dsilicon%2Bcontrolled%2Brectifier%26start%3D20%26gbv%3D2%26ndsp%3D20%26hl%3Den%26sa%3DNhttp://images.google.com.pk/imgres?imgurl=https://www.alliedelec.com/Images/Products/Small/935-3546.jpg&imgrefurl=https://www.alliedelec.com/Search/ProductDetail.aspx%3FSKU%3D9353546%26MPN%3DNTE5569%26R%3D9353546%26SEARCH%3D9353546%26DESC%3DNTE5569&h=200&w=200&sz=6&hl=en&start=38&usg=__n6jdEoIXLreFjd9x7wKShkZcdeQ=&tbnid=3_54I90sV8ksOM:&tbnh=104&tbnw=104&prev=/images%3Fq%3Dsilicon%2Bcontrolled%2Brectifier%26start%3D20%26gbv%3D2%26ndsp%3D20%26hl%3Den%26sa%3DNhttp://images.google.com.pk/imgres?imgurl=http://www.smcelectronics.com/SCR1.JPG&imgrefurl=http://www.smcelectronics.com/semi.htm&h=187&w=90&sz=11&hl=en&start=85&usg=__5KOZr_-rIlOpqij_Jd6Y4BbWrEg=&tbnid=8hDPhSof7S37pM:&tbnh=102&tbnw=49&prev=/images%3Fq%3Dsilicon%2Bcontrolled%2Brectifier%26start%3D80%26gbv%3D2%26ndsp%3D20%26hl%3Den%26sa%3DNhttp://images.google.com.pk/imgres?imgurl=https://www.alliedelec.com/Images/Products/Small/935-3546.jpg&imgrefurl=https://www.alliedelec.com/Search/ProductDetail.aspx%3FSKU%3D9353546%26MPN%3DNTE5569%26R%3D9353546%26SEARCH%3D9353546%26DESC%3DNTE5569&h=200&w=200&sz=6&hl=en&start=38&usg=__n6jdEoIXLreFjd9x7wKShkZcdeQ=&tbnid=3_54I90sV8ksOM:&tbnh=104&tbnw=104&prev=/images%3Fq%3Dsilicon%2Bcontrolled%2Brectifier%26start%3D20%26gbv%3D2%26ndsp%3D20%26hl%3Den%26sa%3DN -
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Thyristor Construction
C
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BJT Characteristics
T f Ch t i ti f NPN
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Transfer Characteristics of NPN
Transistor
Lesson Plan Topic 2.2
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EFFECT OF GATE CURRENT
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EFFECT OF GATE CURRENT on
FORWARD BLOCKING VOLTAGE
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TURN-ON CHARACTERISTICS
on d r t t t= +
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Reverse Recovery Characteristic of
Diode
t1
t2
tr r
0 . 2 5 IR R
t
IR R
IF
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Methods of Thyristor Turn-on
1) Gate Current : Normal method
2) Light: Normal method for LASCR ( Light
Activated SCR)
3) High Voltage: False Turn-on (If appliedvoltage exceeds the rated value)
4) dv/dt :False Turn-on (If applied dv/dt exceedsthe rated value)
5) Thermal Turn-on: False Turn-on
Zener Diode
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Zener Diode
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Zener-Diode Application
Uni Junction Transistor
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Uni-Junction Transistor
E
B 2
B 1B 1
A
B 2
E
R B 2
R B 1n - t y p e
p - t y p e
E t a - p o i n t
B a s i c S t r u c t u r e S y m b o l
1 2 BB B B R R R= +
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UJT Relaxation Oscillator
R R 2
V B B
R 1C
E
B 2
B 1V e v o
V e
V p
V V
V o
t
t
C a p a c i t o r
c h a r g i n g
1 = R C
T
V + V
B B
V P
2 1= R C
C a p a c i t o
d i s c h a r g
Vv
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UJT Firing Circit
(Synchronised UJT Oscillator)
R
C
+
-
D 1 D 3
D 4 D 2
V d c
R 1
V Z
+
-
Z
i 1
v c
+
-
R 2
G 1
C 1
G 2
C 2
P u l s e T r a nE
B 2
B 1
T o SG a t e
V lt f A
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Voltage-waveforms Across
Zener, Capacitor, Output
1 2 1 2 1 2
P u l s eV o l t a g e
v c ,
v d c
v c v c v c
V d cV Z
V Z
t
t
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UJT FIRING CIRCUIT
Triggering Circuits Using ICs
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Triggering Circuits Using ICs
Resistance Firing Circuit (Half-Wave)
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Resistance Firing Circuit (Half Wave)
L O A D
v Oa b
i R 1
R 2
D
R V g
V T
v = V s i n tS m
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Waveforms for Resistance Firing Circuit (Half-Wave)
V S
2 3 4
t
V s i n tm
V g V g t
t
t
t
t
V o
i o
V T
V g p V g tV g p
( a )
t
t
t
t
t
t
t
t
t
t
2 3 4
2 3 4
V S
V g
V o
i o
V T
V S
V g
V o
i o
V T
V = Vg p g t
2 7 00
2
3 4
9 00 = 9 0
0
( c )( b )
< 9 00
V > Vg p g t
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R C Half-Wave Trigger Circuit
L O A D
v O
R
C
V T
v = V s i n tS m
D 2
V C
+
-
D 1
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Waveformsfor R C Half-Wave Trigger Circuit
v s
0
V s i n tm
0 t
t t
av c
- / 2
a
v c
Vg t
v o
v T
2 3
V m
- Vm
v s
0
V s i n tm
0 t
av c
- / 2
a
v c
Vg t
0
0
v o
v T
V m V m
2 3 - Vm
( 2 + )
( a ) ( b )
t t
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RC Triggering
L O A D
v O
R
C
V T
v = V s i n tS m
D 2
V C
+
-
D 1
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R C Full-Wave Trigger Circuitv O
R
C
V T
v = V s i n tS m
+
-
L O A D+
-
D 1 D 3
D 4 D 2
v d
Waveforms of RC full-wave triggering
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v s
v d
v o
v T
t
t
t
V s i n tm
v d
v c v c v cv g t
gg gwith Rat high value
Waveforms of RC full-wave triggering( ) ith R HIGH l (b) ith R LOW l
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(a) with R, HIGH value (b) with R, LOW value
v s
vd
v o
v T
t
t
t
t
V s i n tm
v d
v c v c v cv g t
V s i n tm v s
vd
v o
v T
t
t
t
v g t
( a ) ( b )
Triggering Device
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Triggering Device
A device is classified as triggering device
if it changes from one stable off-state toanother stable on-state upon sensing a
particular voltage level called the Trigger,
FiringorPeak-Pointvoltage.
In most applications triggering devices
sense voltage magnitude across a
capacitor. When the capacitor voltage
reaches the trigger voltage, the deviceturns on and provides a discharge path
for capacitor.
Si l G t T i
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Simple Gate Trigger
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SCR Triggered by Light Pulse
PhotoTransistor
Light
V I Ch t i ti f TRIAC
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V-I Characteristics of TRIAC
C
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DIAC is a two terminal five layer semi-conductor bi-directional switching device.
P
N N
N
N
P
PP
T 1
T1
T2
T 2
DIAC can conduct in both directions when the
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DIAC can conduct in both directions when thevoltage applied across the device terminals
exceeds its break over voltage.
T1
T1T 2 T 2
RL
RL
V V
I
I
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Diac Characteristics
V B 0 2
V B 0 1
B l o c k i n g s t a t e
F o r w a r dc o n d u c t i o n
R e v e r s ec o n d u c t i o n r e g i o n
I
V
Circuit Turn-off Time t
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Circuit Turn-off Time tc
It is the turn-off time that the circuit
presents to the SCR.
The circuit turn-off time tc must always be
greater than the turn-off time of SCR
(tqor toff), otherwise the SCR may revert to
the on-state.
Losses in Thyristor
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y
1) Load current forward conduction loss
= IA x VF
2) Forward leakage power loss = IFB x VS
( due to forward leakage current)
3) Reverse leakage power loss ( only in a.c;
due to reverse leakage current )
4) Gate power loss: It is due to energy input
from firing circuit. Pulse firing reduces
this loss.
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Losses in Thyristor ( contd.)
5) Switching loss (or Dynamic loss)
Loss during turn-on and turn-off periods.
At high frequency ( above 1 kHz ) this
loss is significant.
For high frequency operation, thyristors ofInverter-grade are used.
H t Si k
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Heat Sinks
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Comparison between different types of Diodes
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p ypGeneral PurposeDiodes
Fast Recovery DiodesSchottky Diodes
Upto 6000V &3500A Upto 6000V and1100A Upto 100V and300A
Reverse recoverytime High
Reverse recoverytime Low
Reverse recoverytime Extremely
low.
Switching frequency Low
(Max 1KHz)
Switching frequency High
(Max 20KHz)
Switching frequency Very high. (Max
30KHz)
0.7 to 1.2VF
V = 0 . 8 t o 1 . 5 VFV =
25rr
t s 0.1 s to 5 srrt = a few nano sec
rrt =
73
0.4 to 0.6VFV
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POWER DIODES APPEARANCE
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Bipolar Junction Transistor (BJT)Bipolar Junction Transistor (BJT)
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Bipolar Junction Transistor (BJT)Bipolar Junction Transistor (BJT)
Ratings: Voltage: VVCECE
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Ratings: VoltageVoltage VVDSDS
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Combination of BJT and MOSFET characteristics.
Compromises include:
Gate behaviour similar to MOSFET - easy to turn on and off. Low losses like BJT due to low on-state Collector-Emitter
voltage (2-3V).
IGBT
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IGBT
Ad f IGBT
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Advantages of IGBT
Combines the advantages of BJT & MOSFET
High input impedance like MOSFET
Voltage controlled device like MOSFET
Simple gate drive, Lower switching loss Low on state conduction power loss like BJT
Higher current capability & higher switching speed
than a BJT. ( Switching speed lower than MOSFET)
Gate-Turn-Off Thyristors (GTO)
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Gate-Turn-Off Thyristors (GTO)
Slow switching speeds
Used at very high power levels
Require elaborate gate control circuitry
Switching Waveforms for
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Switching Waveforms for
GTOs
tt
tt
iiGG
tt
iiAA
vvSS
large in magnitude ~ 1/3 ilarge in magnitude ~ 1/3 iAA
Neededtoturn-offNeededtoturn-off
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di/dt Protection
S
S
Vdidt L
=
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Static & Dynamic Equalization
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PARALLEL OPERATION
Switches comparison
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Switches comparisonDevice Type Year
madeRated
VoltageRated
CurrentSwitchingFrequency
RatedPower
DriveCircuit
Comments
SCR 1957 6kV 3.5kA 500Hz 100s MW Simple Cannot turn-off usinggate signal
GTO 1962 4.5kV 3kA 2kHz 10s MW VeryDifficult
King in very highpower
BJT 1960s 1.2kV 400A 5kHz 1 MW Difficult Phasing out in newproduct
MOSFET 1976 500V 200A 1MHz 100 kW VerySimple
Good performance inhigh frequency
IGBT 1983 3.3kV 1.2kA 100kHz 100s kW VerySimple
Best overallperformance
Harmonics
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( )
=
++=1
0 )sin()cos()(n
nn tnbtnaatf
=
tdtntfan )(cos)(1
=
tdtntfbn )(sin)(1
It can be defined as a sinusoidal component of a periodic waves or quality
having frequencies that are an integral multiple of the fundamental frequency.
=
2
0
0 )(2
1tdtfa =
2
0
)(cos)(1
tdtntfan=
2
0
)(sin)(1
tdtntfbn
For Odd Functions: =
0
)(sin)(2
tdtntfbn00 == naa
For Even Functions: =
0
)(cos)(2
tdtntfan=
0
0 )(1
tdtfa 0=nb
A Simple Circuit (R-L Load) Current continues to flows for a while even after the input
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Current continues to flows for a while even after the input
voltage has gone negative
ADVANTAGES OF THYRISTORISED
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POWER CONTROLLERS
1) High efficiency due to low losses in the Thyristors.
2) Long life and reduced/minimal maintenance due to
the absence of mechanical wear.
3) Control equipments using Thyristors are compact in
size.4) Easy and flexibility in operation due to digital
controls.
5) Faster dynamic response compared to the electro
mechanical converters.6) Lower acoustic noise when compared to electro
magnetic controllers, relays and contactors.
DISADVANTAGES OF THYRISTORISED
POWER CONTROLLERS
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POWER CONTROLLERS
1) All the thyristorised power controllers generate
harmonics (unwanted frequency components) due to theswitching ON and OFF of the thyristors. These harmonics
adversely affect the performance of the load connected to
them. For example when the load are motors, there are
additional power losses (harmonic power loss) torqueharmonics, and increase in acoustic noise.
2) The generated harmonics are injected into the supply
lines and thus adversely affect the other loads/equipments
connected to the supply lines.
3) In some applications example: traction, there is
interference with the commutation circuits due to the
power supply line harmonics and due to electromagnetic
radiation.
DISADVANTAGES OF THYRISTORISED
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POWER CONTROLLERS( contd.)
4) The thyristorised AC to DC converters and AC to ACconverters can operate at low power factor under some
conditions.
5)Special steps are then taken for correcting the line supply
power factor (by installing PF improvement apparatus).
6) The thyristorised power controllers have no short time over
loading capacity and therefore they must be rated for
maximum loading conditions. This leads to an increase in the
cost of the equipment.
7) Special protection circuits must be employed inthyristorised power controllers in order to protect and safe
guard the expensive thyristor devices. This again adds to the
system cost.
Synchronous Speed
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Synchronous Speed
pfNs
120=
s is syncronous speed [rad/sec]
Ns is syncronous speed [rpm]
p is numbers of poles
is the supply frequency [rad/sec]f is the supply frequency [Hz]
Nm is motor speed
A t d N i l th th d f th t ti fi ld N
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Armature speed N is less than the speed of the rotating field Ns
by an amount equal to theslip speed s.
The frequency of an induction machine at the rotor side isnt
the same as the frequency at primary side.
Rotor Frequency,
where fr
and fs
are rotor current frequency and mains supply
frequency, respectively.
s
s
N
NNs =
sr sff =
TorqueSpeedCharacteristic
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Characteristic
For small values of slip,developed torque is proportional
to slip.
TORQUE-SPEED CHARACERISTIC
f I d ti M t
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of Induction Motor
Tmax
Smax
Tst
Td
S=0sNs
S=1
TL
S=SmmNmNm =0
Tm=TLOperating point
Stator Voltage Control
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gControlling Induction Motor Speed by Adjusting The Stator Voltage
Tmax
S=0sNs
S=1
TL
Nm =0
Td
Vs1Vs Vs2> >
1 2
Tst
Tst1
Tst2
Varying supply voltage and supply
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98MZS
FKEE, UMP
98
The best method since supplyvoltage and supply frequency is
varied to keep VV//ff constant
Maintain speed regulation
uses power electronics circuit forfrequency and voltage controller
Constant maximum torque
y g pp y g pp y
frequency
T
nNL1
T
nr1nr2nr3 n
f
decreasing
nNL2nNL3
Frequency Voltage Control
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Frequency Voltage ControlControlling Induction Motor Speed by Adjusting The Frequency Stator Voltage
Tmax
S=0
TL
Td