power electronics ppts_0
TRANSCRIPT
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SINGLE PHASE HALF CONTROLLEDCONVERTERS
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Sl.
No.
Module as per Session Planner Lecture
No.
PPT Slide No.
1 Introduction to Line commutated Inverter L-1 3-12
2 Principle of Phase Controlled Rectifier Operation L-2 13-19
3 Expression for the RMS Value of Output Voltage
of a Single Phase Half Wave Controlled RectifierWith Resistive Load
L-3 20-33
4 Performance Parameters
Of Phase Controlled RectifiersL-4 34-45
5 Single Phase Half Wave Controlled Rectifier
With An RL LoadL-5 46-61
6 Single Phase Half Wave Controlled Rectifier
With RL Load & Free Wheeling DiodeL-6 62-80
7 Single Phase Full Wave Controlled Rectifier
Using A Center Tapped TransformerL-7 81-113
8 Single Phase Full Wave Bridge Controlled
RectifierL-8 114-129
LECTURE PLAN
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Lecture-1
Introduction to Line commutatedInverter
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4
Type of input: Fixed voltage, fixed
frequency ac power supply.
Type of output: Variable dc output voltage
Type of commutation: Natural / AC line
commutation
Line
CommutatedConverter
+
-
DC Output
V0(dc)
AC
Input
Voltage
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5
Different types of
Line Commutated Converters
AC to DC Converters (Phase controlled
rectifiers) AC to AC converters (AC voltage controllers)
AC to AC converters (Cyclo-converters) at
low output frequency.
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6
Differences Between
Diode Rectifiers&
Phase Controlled Rectifiers
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Cntd
7
The diode rectifiers are referred to asuncontrolled rectifiers .
The diode rectifiers give a fixed dc outputvoltage .
Each diode conducts for one half cycle.
Diode conduction angle = 1800or radians.
We can not control the dc output voltage orthe average dc load current in a dioderectifier circuit.
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8
Single phase half wave diode rectifier gives an
Average dc output voltage
Single phase full wave diode rectifier gives an
2Average dc output voltage
m
O dc
mO dc
V
V
VV
Cntd
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9
Applications of
Phase Controlled Rectifiers
DC motor control in steel mills, paper and
textile mills employing dc motor drives. AC fed traction system using dc traction
motor.
Electro-chemical and electro-metallurgicalprocesses.
Magnet power supplies.
Portable hand tool drives.
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10
Classification of
Phase Controlled Rectifiers
Single Phase Controlled Rectifiers. Three Phase Controlled Rectifiers.
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11
Different types of Single
Phase Controlled Rectifiers. Half wave controlled rectifiers.
Full wave controlled rectifiers.
Using a center tapped transformer.Full wave bridge circuit.
Semi converter.
Full converter.
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12
Different Types of
Three Phase Controlled Rectifiers
Half wave controlled rectifiers.
Full wave controlled rectifiers.
Semi converter (half controlled
bridge converter).
Full converter (fully controlled
bridge converter).
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Lecture-2
Principle of Phase Controlled Rectifier
Operation
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14
Principle of Phase Controlled
Rectifier Operation
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15
Single Phase Half-Wave Thyristor
Converter with a Resistive Load
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16
Supply Voltage
Output Voltage
Output (load)
Current
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17
Supply
Voltage
Thyristor Voltage
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18
Equations
sin i/p ac supply voltage
max. value of i/p ac supply voltage
RMS value of i/p ac supply voltage2
output voltage across the load
s m
m
mS
O L
v V t
VV
V
v v
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19
When the thyristor is triggered at
sin ; to
Load current; to
sinsin ; to
Where max. value of load current
O L m
O
O L
mO L m
mm
t
v v V t t
v
i i tR
V ti i I t t
RV
IR
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20
To Derive an Expression for the
Average (DC)Output Voltage Across The
Load
Lecture-3
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21
2
0
1. ;2
sin
1sin .
2
1sin .
2
dc OO dc
O m
dc mO dc
mO dc
V V v d t
v V t for t to
V V V t d t
V V t d t
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22
sin .2
cos2
cos cos ; cos 1
2
1 cos ; 22
m
O dc
m
O dc
m
O dc
mm SO dc
VV t d t
VV t
VV
VV V V
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23
max
max
Maximum average (dc) o/pvoltage is obtained when 0
and the maximum dc output voltage
1 cos0 ; cos 0 12
mdmdc
mdmdc
VV V
VV V
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24
0
1 cos ; 22
The average dc output voltage can be varied
by varying the trigger angle from 0 to a
maximum of 180 radians
We can plot the control characteristic
v by using the eq
mm SO dc
O dc
VV V V
V s
uation for
O dcV
Cntd
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25
Control Characteristicof
Single Phase Half Wave PhaseControlled Rectifier
with
Resistive Load
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26
The average dc output voltage is given by the
expression
1 cos2
We can obtain the control characteristic by
plotting the expression for the dc output
voltage as a function of trigger angle
mO dc
VV
Cntd
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27
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Control CharacteristicVO(dc)
Trigger angle in degrees
0 60 120 180
Vdm
0.2 Vdm
0.6Vdm
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Normalizing the dc output
voltage with respect to , the
Normalized output voltage
1 cos2
11 cos
2
dm
m
dcn
mdm
dcn dcn
dm
V
V
VV
VV
VV V
V
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30
To Derive An Expression for the RMS Value
of Output Voltage of a Single Phase HalfWave Controlled Rectifier With Resistive
Load
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2
2
0
1
22 2
The RMS output voltage is given by
1.
2
Output voltage sin ; for to
1sin .
2
OO RMS
O m
mO RMS
V v d t
v V t t
V V t d t
Cntd
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32
2
1
22
1
2 2
12 2
1 cos 2By substituting sin , we get
2
1 cos 21.
2 2
1 cos 2 .4
cos 2 .4
mO RMS
m
O RMS
m
O RMS
tt
tV V d t
VV t d t
VV d t t d t
Cntd
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1
2
1
2
1
2
1
2
1 sin2
22
sin 2 sin 21;sin2 0
2 2
1 sin 2
2 2
sin2
22
m
O RMS
m
O RMS
m
O RMS
m
O RMS
V t
V t
VV
VV
VV
Cntd
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34
Performance Parameters
OfPhase Controlled Rectifiers
Lecture-4
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Output dc power (avg. or dc o/p
power delivered to the load)
; . .,
Where
avg./ dc value of o/p voltage.
avg./dc value of o/p current
dc dc dcO dc O dc O dc
dcO dc
dcO dc
P V I i e P V I
V V
I I
Cntd
C
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Output ac power
Efficiency of Rectification (Rectification Ratio)
Efficiency ; % Efficiency 100
The o/p voltage consists of two components
The dc component
The ac
O ac O RMS O RMS
O dc O dc
O ac O ac
O dc
P V I
P PP P
V
/ripple component
ac r rmsV V
Cntd
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2 2
2 2
The total RMS value of output voltage is given by
Form Factor (FF) which is a measure of the
shape of the output voltage is given by
RMS output l
O RMS O dc r rms
ac r rms O RMS O dc
O RMS
O dc
V V V
V V V V
VFF
V
oad voltage
DC load output load voltage
Cntd
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22 2
2
The Ripple Factor (RF) w.r.t. o/p voltage w/f
1
1
r rms acv
dcO dc
O RMS O dc O RMS
v
O dc O dc
v
V Vr RF
V V
V V Vr
V V
r FF
Cntd
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2 2
max min
max min
Current Ripple Factor
Where
peak to peak ac ripple output voltage
peak to peak ac ripple load current
r rms ac
idcO dc
acr rms O RMS O dc
r pp
r pp O O
r pp
r pp O O
I Ir
I I
I I I I
V
V V V
I
I I I
Cntd
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Transformer Utilization Factor (TUF)
Where
RMS supply (secondary) voltage
RMS supply (secondary) current
O dc
S S
S
S
PTUF
V I
V
I
Cntd
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Cntd
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1
Where
Supply voltage at the transformer secondary side
i/p supply current
(transformer secondary winding current)
Fundamental component of the i/p supply current
Peak value of the input s
S
S
S
P
v
i
i
I
upply current
Phase angle difference between (sine wavecomponents) the fundamental components of i/p
supply current & the input supply voltage.
Cntd
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1
Displacement angle (phase angle)
For an RL load
Displacement angle = Load impedance angle
tan for an RL load
Displacement Factor (DF) orFundamental Power Factor
L
R
DF Cos
Cntd
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11
2 22 2 21
2
1 1
1
Harmonic Factor (HF) or
Total Harmonic Distortion Factor ; THD
1
Where
RMS value of input supply current.
RMS value of fundamental component of
the i
S S S
S S
S
S
I I IHF
I I
I
I
/p supply current.
Cntd
Cntd
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1 1
Input Power Factor (PF)
cos cos
The Crest Factor (CF)
Peak input supply c
For an Ide
urrent
RMS input supply current
1; 100% ;
al Controlled Rectifier
0 ; 1;
S S S
S S S
S peak
S
ac r rms
V I IPFV I I
ICF
I
FF V V TUF
R
0 ; 0; 1v
F r HF THD PF DPF
Cntd
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Single Phase Half Wave ControlledRectifier With An RL Load
Lecture -5
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Cntd
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Input Supply Voltage (Vs)
&Thyristor (Output) Current
Waveforms
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Cntd
O t t (L d)
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Output (Load)
Voltage Waveform
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1
To Derive An Expression For
The Output(Load) Current, During to
When Thyristor Conducts
t
T
Cntd
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1
1
Assuming is triggered ,
we can write the equation,
sin ;
General expression for the output current,
sin
OO m
t
mO
T t
diL Ri V t tdt
Vi t A e
Z
Cntd
Cntd
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53
22
1
1
2 maximum supply voltage.
=Load impedance.
tan Load impedance angle.
Load circuit time constant.
general expression for the output load current
sin
m S
Rt
m LO
V V
Z R L
L
RL
R
Vi t A e
Z
Cntd
Cntd
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1
1
1
1
1
Constant is calculated from
initial condition 0 at ; t=
0 sin
sin
We get the value of constant as
sin
O
Rt
m L
O
Rt
mL
R
mL
A
i t
V
i A eZ
VA e
Z
A
VA e
Z
Cntd
Cntd
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1Substituting the value of constant in the
general expression for
sin sin
we obtain the final expression for the
inductive load current
sin sin
O
Rt
m mLO
Rt
m LO
A
i
V Vi t e
Z Z
Vi t eZ
;
Where t
Cntd
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Extinction angle can be calculated by using
the condition that 0
sin sin 0
sin sin
can be calculated by solving the above eqn.
O
Rtm L
O
R
L
i at t
Vi t eZ
e
Cntd
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To Derive An ExpressionFor
Average (DC) Load Voltage of aSingle Half Wave Controlled
Rectifier with
RL Load
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2
0
2
0
1
.2
1. . .
20 for 0 to & for to 2
1
. ;2
sin for to
L OO dc
L O O OO dc
O
L OO dc
O m
V V v d t
V V v d t v d t v d t
v t t
V V v d t
v V t t
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1sin .
2
cos
2
cos cos2
cos cos2
L mO dc
mLO dc
mLO dc
mLO dc
V V V t d t
VV V t
VV V
VV V
Effect of Load
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During the period to the
instantaneous o/p voltage is negative
reduces the average or the dc output
vo
and
this
when compared to a purely
resist
ltage
ive load.
t
Effect of Load
Inductance on the Output
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Average DC Load Current
cos cos2O dc
mO dc L Avg
L L
V VI I
R R
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Lecture-6
Single Phase Half Wave Controlled RectifierWith RL Load & Free Wheeling Diode
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V0
i0T
R
L
Vs ~+
+
FWD
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0
0
0
0
vS
iG
vO
t
t
t
t
Supply voltage
Load current
Load voltage
t=
2
Gate pulses
iO
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The followi
The average
ng points a
output voltage
1 cos which is the same as that2
of a purely resistive load.
For low value of inductance, the load currenttends to become dis
re to be noted
cont
mdc
VV
inuous.
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During the period to
the load current is carried by the SCR.
During the period to load current is
carried by the free wheeling diode.
The value of depends on the value of
R and L and the forwa
rd resistanceof the FWD.
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Single Phase Half Wave
Controlled Rectifier With
A
General Load
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R
vS~+
L
E+
vO
iO
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1sin
For trigger angle ,the Thyristor conducts from to
For trigger angle ,
the Thyristor conducts from to
m
EV
t
t
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0
0
iO
t
t
Load current
E
vO
Load voltage
Vm
Im
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Equations
sin Input supply voltage.
sin o/p load voltagefor to .
for 0 to &for to 2 .
S m
O m
O
v V t
v V tt
v E tt
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Expression for the Load Current
When the thyristor is triggered at a delay angle of
, the eqn. for the circuit can b
sin +E
e written as
The general expression for the output load
current can be writte
;
n
Om O
diV t i R L t dt
s
as
int
mO
V Ei t Ae
Z R
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22
1
Where
= Load Impedance.
tan Load impedance angle.
Load circuit time constant.
The general expression for the o/p current can
be written as sinR
tm L
O
V Ei t Ae
Z
Z R
L
R
L
R
R
L
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We obtain the value of constant 'A' as
Substituting the value of the constant 'A' in theexpression for the load current; we get the
complete expression for the output load c
si
ur
nR
m LVE
A eR Z
sin
rent
in
s
as
R tm m L
O
V VE Ei t e
Z R R Z
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To Derive
An
Expression For The AverageOr
DC Load Voltage
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2
0
2
0
2
0
sin Output load voltage
1
.2
1.
for 0 to & for to 2
for
. .
to
2
1. sin .
2
O
OO dc
O O OO d
m
m
c
O dc
O
V v d t
V v d t v d t v d t
V E d t V t E d t
v V t
v E t t
t
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2
0
1 cos2
10 cos cos 2
2
cos cos 22 2
2cos cos2 2
mO dc
mO dc
m
O dc
m
O dc
V E t V t E t
V E V E
V EV
VV E
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2
2
0
Conduction angle of thyristor
RMS Output Voltage can be calculatedby using the expres
1 .
sion
2 OO RMS
V v d t
L t 7
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Lecture-7
Single Phase Full Wave Controlled
Rectifier Using A Center Tapped
Transformer
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ACSupply
O
A
B
T1
T2
R L
vO
+
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DiscontinuousLoad Current Operation
without FWDfor
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vO Vm
0
( ) ( )
iO
t
t0
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1
To Derive An Expression For
The Output(Load) Current, During to
When Thyristor Conducts
t
T
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1
1
Assuming is triggered ,
we can write the equation,
sin ;
General expression for the output current,
sin
OO m
t
mO
T t
diL Ri V t tdt
Vi t A e
Z
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22
1
1
2 maximum supply voltage.
=Load impedance.
tan Load impedance angle.
Load circuit time constant.
general expression for the output load current
sin
m S
Rt
m LO
V V
Z R L
L
RL
R
Vi t A e
Z
Constant is calculated fromA
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1
1
1
1
1
Constant is calculated from
initial condition 0 at ; t=
0 sin
sin
We get the value of constant as
sin
O
Rt
m LO
Rt
mL
R
mL
A
i t
Vi A e
Z
VA e
Z
AV
A eZ
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1Substituting the value of constant in the
general expression for
sin sin
we obtain the final expression for the
inductive load current
sin sin
O
Rt
m mLO
Rt
m LO
A
i
V Vi t e
Z Z
Vi t eZ
;
Where t
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Extinction angle can be calculated by using
the condition that 0
sin sin 0
sin sin
can be calculated by solving the above eqn.
O
R
tm LO
R
L
i at t
Vi t eZ
e
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91
To Derive An Expression For The
DC Output Voltage OfA Single Phase Full Wave
Controlled Rectifier With RL Load
(Without FWD)
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vO Vm
0
( ) ( )
iO
t
t0
1
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1.
1sin .
cos
cos cos
dc OO dc
t
dc mO dc
mdcO dc
mdcO dc
V V v d t
V V V t d t
VV V t
VV V
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When the load inductance is negligible i.e., 0
Extinction angle radians
Hence the average or dc output voltage for R load
cos cos
cos 1
1 cos ; for R load, when
mO dc
m
O dc
m
O dc
L
VV
VV
VV
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2 2
To calculate the RMS output voltage we use
the expression
1sin .mO RMSV V t d t
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Discontinuous Load Current
Operation with FWD
V
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vO Vm
0
( ) ( )
iO
t
t0
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2
2
1
1
Thyristor is trigger
Thyristor is triggered at ;conducts from to
FWD conducts from to &0 during discontinuous loa
ed at ;conducts from t
d current.
o 2
O
T tT
T t
t
T t
tv
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To Derive an Expression
For The
DC Output Voltage For
ASingle Phase Full Wave
Controlled RectifierWith RL Load & FWD
1
-
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100
0
1.
1sin .
cos
cos cos ; cos 1
1 cos
dc OO dc
t
dc mO dc
mdcO dc
m
dcO dc
mdcO dc
V V v d t
V V V t d t
VV V t
VV V
VV V
-
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101
The load current is discontinuous for low
values of load inductance and for large
values of trigger angles.
For large values of load inductance the load
current flows continuously without falling to
zero.
Generally the load current is continuous for
large load inductance and for low trigger
angles.
-
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102
Continuous Load Current
Operation(Without FWD)
-
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103
vO Vm
0
( )
iO
t
t0
( )
-
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104
To DeriveAn Expression For
Average / DC Output Voltage
OfSingle Phase Full Wave Controlled
Rectifier For Continuous Current
Operation without FWD
-
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105
vO Vm
0
( )
iO
t
t0
( )
-
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106
1
.
1 sin .
cos
dc OO dc
t
dc mO dc
mdcO dc
V V v d t
V V V t d t
VV V t
V V
-
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107
cos cos ;
cos cos
cos cos
2cos
dcO dc
m
mdcO dc
mdcO dc
V V
V
VV V
VV V
-
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108
By plotting VO(dc)versus ,
we obtain the control characteristic of a
single phase full wave controlled rectifier
with RL load for continuous load currentoperation without FWD
-
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109
cosdc dmV V
V V V
-
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110
VO(dc)
Trigger angle in degrees
030 60 90
Vdm
0.2 Vdm
0.6Vdm
-0.6 Vdm
-0.2Vdm
-Vdm
120 150 180
cosdc dmV V
-
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111
00
By varying the trigger angle we can vary theoutput dc voltage across the load. Hence we can
control the dc output power flow to the load.
For trigger a . .,ngle , 0 to 90
cos is positive
0 90 ;
i e
and hence is positive
Converter
& are positive ; is positive
Controlled Rectifoperates as a
Power flow is from the
ie
ac source to the d.
r.
loa
dc dc dc dc d
d
c
cV
V I P V I
0 0F t i l 90 t 180
-
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112
0
0
0
0
. ., 90 180 ,
is negative; is positive
For trigger angle , 90
;
is negative.
Line
to 180
cos is negative and hence
In this case the conve
Co
rte
mmutated In
r operates
s vea a
dc dc
dc dc dc
i e
V I
P V I
Power flows from the load ckt. to the i/p ac source.The inductive load energy is fed back to the
i/p sou
rter.
rce.
Drawbacks Of Full Wave
-
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113
Drawbacks Of Full Wave
Controlled RectifierWith Centre Tapped Transformer We require a centre tapped transformer
which is quite heavier and bulky. Cost of the transformer is higher for the
required dc output voltage & output power.
Hence full wave bridge converters arepreferred.
-
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Single Phase
-
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115
Single Phase
Full Wave Bridge Controlled
Rectifier2 types of FW Bridge Controlled Rectifiers are
Half Controlled Bridge Converter
(Semi-Converter)
Fully Controlled Bridge Converter
(Full Converter)
The bridge full wave controlled rectifier does
not require a centre tapped transformer
-
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116
Single Phase
Full Wave Half ControlledBridge Converter
(Single Phase Semi Converter)
-
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117
Trigger Pattern of Thyristors
-
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118
Trigger Pattern of Thyristors
1
2
0
1 2
, 2 ,...
, 3 ,...
& 180
Thyristor T is triggered at
t at t
Thyristor T is triggered at
t at t
The time delay between the gating
signals of T T radians or
-
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119
Waveforms of
single phase semi-converter
with general load & FWD
for > 900
-
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120
Single Quadrant
Operation
-
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121
-
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122
-
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123
1 1
2 2
Thyristor & conductfrom
Thyristor & conductfrom 2
FWD conducts during0 to , ,...
T Dt to
T Dt to
t to
-
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124
Load Voltage & Load CurrentWaveform of Single Phase Semi
Converter for< 900
& Continuous load current
operation
v Vm
-
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125
vO Vm
0
iO
t
( )
t0
( )
To Derive an Expression
-
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126
To Derive an Expression
For TheDC Output Voltage of
A
Single Phase Semi-Converter
With R,L, & E Load & FWD
For Continuous, Ripple FreeLoad Current Operation
1
V V d t
-
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127
0
.
1sin .
cos
cos cos ; cos 1
1 cos
dc OO dc
t
dc mO dc
mdcO dc
mdcO dc
mdcO dc
V V v d t
V V V t d t
VV V t
VV V
VV V
can be varied from a maxV
-
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128
max
can be varied from a max.
2value of 0 by varying from 0 to .
For 0, The max. dc o/p voltage obtained is
Normalized dc o/p voltage is
2
11 cos2
dc
m
m
dc
mdn
m
dmdc
dcn n
V
Vto
V
V
V V
VVV
V
V
1 cos2
RMS O/P Voltage VO(RMS)
-
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129
RMS O/P Voltage VO(RMS)
1
22 2
1
2 2
1
2
2sin .
2
1 cos 2 .2
1 sin 2
22
mO RMS
m
O RMS
m
O RMS
V V t d t
VV t d t
VV
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130
Single Phase Full Wave
Controlled Rectifier
LECTURE PLANSl.No Module as per Session Planner Lecture No. PPT Slide No.
-
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131
1 Single Phase Full Wave Controlled Rectifier
Using A Center Tapped Transformer
L 1 2-12
2 Derivation for Expression For The DC OutputVoltage Of A Single Phase Full Wave
Controlled Rectifier With RL Load
L2 13-20
3 Derivation for Expression For The DC Output
Voltage For A Single Phase Full Wave
Controlled Rectifier With RL Load & FWD
L3 21-34
4 Single Phase Full Wave Bridge ControlledRectifier
L 4 35-44
5 Load Voltage & Load Current Waveform of
Single Phase Semi Converter for < 900&
Continuous load current operation
L 5 45-51
6 Single Phase Full Converter L 6 52-58
7 Derivation for Expression For The Average DC
Output Voltage of a Single Phase Full
Converter assuming Continuous & Constant
Load Current
L 7 59-68
8 Two Quadrant Operation
of a Single Phase Full Converter
L 8 69-78
Lecture-1
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132
Single Phase Full Wave Controlled
Rectifier Using A Center TappedTransformer
Single Phase Midpoint type
Fully controlled Rectifier
-
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133133
ACSupply
O
A
B
T1
T2
R L
vO
+
Fully controlled Rectifier
-
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134134
DiscontinuousLoad Current Operation
without FWDfor
v Vm
-
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135135
vO Vm
0
( ) ( )
iO
t
t0
-
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136136
1
To Derive An Expression For
The Output
(Load) Current, During to
When Thyristor Conducts
t
T
-
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137137
1
1
Assuming is triggered ,
we can write the equation,
sin ;
General expression for the output current,
sin
OO m
tm
O
T t
diL Ri V t tdt
Vi t A e
Z
2 maximum supply voltageV V
-
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138138
22
1
1
2 maximum supply voltage.
=Load impedance.
tan Load impedance angle.
Load circuit time constant.
general expression for the output load current
sin
m S
Rt
m LO
V V
Z R L
L
R
L
R
Vi t A e
Z
1Constant is calculated fromA
-
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139139
1
1
1
1
initial condition 0 at ; t=
0 sin
sin
We get the value of constant as
sin
O
Rt
m LO
Rt
mL
R
mL
i t
Vi A e
Z
VA e
Z
A
VA e
Z
Substituting the value of constant in theA
-
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140140
1Substituting the value of constant in the
general expression for
sin sin
we obtain the final expression for the
inductive load current
sin sin
O
Rt
m mLO
Rt
m LO
A
iV V
i t eZ Z
V
i t eZ
;
Where t
-
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141141
Extinction angle can be calculated by usingthe condition that 0
sin sin 0
sin sincan be calculated by solving the above eqn.
O
Rt
m LO
R
L
i at t
Vi t eZ
e
Lecture-2
-
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142142
To Derive An Expression For The DC
Output Voltage OfA Single Phase Full Wave Controlled
Rectifier With RL Load
(Without FWD)
Lecture 2
vO Vm
-
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143143
vO m
0
( ) ( )
iO
t
t0
1
V V v d t
-
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144144
.
1sin .
cos
cos cos
dc OO dc
t
dc mO dc
mdcO dc
mdcO dc
V V v d t
V V V t d t
VV V t
VV V
-
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145145
When the load inductance is negligible i.e., 0
Extinction angle radians
Hence the average or dc output voltage for R load
cos cos
cos 1
1 cos ; for R load, when
mO dc
m
O dc
m
O dc
L
VV
VV
VV
-
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146146
2 2
To calculate the RMS output voltage we usethe expression
1 sin .mO RMSV V t d t
-
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147147
Discontinuous Load Current
Operation with FWD
vO Vm
-
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148148
0
( ) ( )
iO
t
t0
-
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149149
2
2
1
1
Thyristor is trigger
Thyristor is triggered at ;conducts from to
FWD conducts from to &0 during discontinuous loa
ed at ;conducts from t
d current.
o 2
O
T tT
T t
t
T t
tv
Lecture-3
-
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150150
To Derive an Expression For The DC
Output Voltage For A Single Phase FullWave Controlled Rectifier With
RL Load & FWD
Lecture 3
1
.dc OO dcV V v d t
-
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151151
0
1sin .
cos
cos cos ; cos 1
1 cos
dc OO dc
t
dc mO dc
mdcO dc
mdcO dc
mdcO dc
V V V t d t
VV V t
VV V
VV V
-
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152152
The load current is discontinuous for low
values of load inductance and for large
values of trigger angles.
For large values of load inductance the loadcurrent flows continuously without falling to
zero.
Generally the load current is continuous forlarge load inductance and for low trigger
angles.
-
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153153
Continuous Load Current
Operation(Without FWD)
vO Vm
-
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154154
O
0
( )
iO
t
t0
( )
-
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155155
To DeriveAn Expression For
Average / DC Output Voltage
OfSingle Phase Full Wave Controlled
Rectifier For Continuous Current
Operation without FWD
vO Vm
-
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156156
O
0
( )
iO
t
t0
( )
1
-
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157157
1
.
1sin .
cos
dc OO dc
t
dc mO dc
mdcO dc
V V v d t
V V V t d t
VV V t
dcO dcV V
-
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158158
cos cos ;
cos cos
cos cos
2cos
m
mdcO dc
mdcO dc
V
VV V
VV V
-
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159159
By plotting VO(dc)versus ,we obtain the control characteristic of a
single phase full wave controlled rectifier
with RL load for continuous load currentoperation without FWD
-
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160160
cosdc dmV V
VO(dc)
V
cosdc dmV V
-
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161161
Trigger angle in degrees
030 60 90
Vdm
0.2 Vdm
0.6Vdm
-0.6 Vdm
-0.2Vdm
-Vdm
120 150 180
By varying the trigger angle we can vary the
-
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162162
00
output dc voltage across the load. Hence we cancontrol the dc output power flow to the load.
For trigger a . .,ngle , 0 to 90
cos is positive
0 90 ;
i e
and hence is positive
Converter
& are positive ; is positive
Controlled Rectifoperates as aPower flow is from the
ieac source to the d.
r.loa
dc dc dc dc d
d
c
cV
V I P V I
0 0For trigger angle , 90 to 180
-
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163163
0 0. ., 90 180 ,
is negative; is positive ;
is negative.
Line
cos is negative and hence
In this case the conve
Co
rte
mmutated In
r operates
s vea a
dc dc
dc dc dc
i e
V I
P V I
Power flows from the load ckt. to the i/p ac source.The inductive load energy is fed back to the
i/p sou
rter.
rce.
Lecture-4
-
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164
Single PhaseFull Wave Bridge Controlled Rectifier
Drawbacks Of Full Wave
-
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165165
Controlled Rectifier
With Centre Tapped Transformer We require a centre tapped transformer
which is quite heavier and bulky. Cost of the transformer is higher for the
required dc output voltage & output power.
Hence full wave bridge converters arepreferred.
Single Phase Full Wave Bridge
Controlled Rectifier
-
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166166
Controlled Rectifier
2 types of FW Bridge Controlled Rectifiers are
Half Controlled Bridge Converter
(Semi-Converter)
Fully Controlled Bridge Converter
(Full Converter)
The bridge full wave controlled rectifier does
not require a centre tapped transformer
-
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167167
Single Phase
Full Wave Half Controlled
Bridge Converter
(Single Phase Semi Converter)
Single Phase Full Wave Half Controlled
Bridge Converter
-
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168168
g
Trigger Pattern of Thyristors
-
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169169
1
2
0
1 2
, 2 ,...
, 3 ,...
& 180
Thyristor T is triggered at
t at t
Thyristor T is triggered at
t at t
The time delay between the gating
signals of T T radians or
-
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170170
Waveforms of
single phase semi-converter
with general load & FWD
for > 900
-
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-
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172172
-
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173173
Th i & dT D
-
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174174
1 1
2 2
Thyristor & conduct
from
Thyristor & conduct
from 2
FWD conducts during0 to , ,...
T D
t to
T D
t to
t to
Lecture-5
-
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175175
Load Voltage & Load Current Waveform
of Single Phase Semi Converter for
< 900& Continuous load currentoperation
vO Vm
-
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176176
0
iO
t
( )
t0
( )
To Derive an Expression
-
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177177
For TheDC Output Voltage of
A
Single Phase Semi-Converter
With R,L, & E Load & FWD
For Continuous, Ripple FreeLoad Current Operation
0
1.dc OO dcV V v d t
-
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178178
0
1sin .
cos
cos cos ; cos 1
1 cos
t
dc mO dc
mdcO dc
mdcO dc
mdcO dc
V V V t d t
VV V t
VV V
VV V
can be varied from a max.
2
dcV
V
-
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179179
max
2
value of 0 by varying from 0 to .
For 0, The max. dc o/p voltage obtained is
Normalized dc o/p voltage is
2
11 cos
2
m
m
dc
mdn
m
dmdc
dcn n
V
to
V
V
V V
VVV
V
V
1 cos2
RMS O/P Voltage VO(RMS)1
-
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180180
1
22 2
1
2 2
1
2
2 sin .2
1 cos 2 .2
1 sin 2
22
mO RMS
m
O RMS
m
O RMS
V V t d t
VV t d t
VV
Lecture-6
-
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181
Single Phase Full Converter
Single Phase Full Converter
-
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182182
-
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183183
Waveforms ofSingle Phase Full Converter
Assuming Continuous
(Constant Load Current)
&
Ripple Free Load Current
-
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-
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185185
iOConstant Load Currenti =IO a
-
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186186
a
i
iT1
T2&
Ia
t
t
t
Iai
i
T3
T4&
Ia
Ia
-
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The average dc output voltage
b d t i d b i th i
-
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188188
2
0
can be determined by using the expression
1. ;
2
The o/p voltage waveform consists of two o/p
pulses during the input supply time period of
0 to 2 r
dc OO dcV V v d t
adians. Hence the Average or dco/p voltage can be calculated as
-
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Maximum average dc output voltage is
-
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190190
0
max
max
Maximum average dc output voltage is
calculated for a trigger angle 0
and is obtained as
2 2cos 0
2
m mdmdc
mdmdc
V VV V
VV V
The normalized average output voltage is given by
-
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191191
max
The normalized average output voltage is given by
2 cos
cos2
O dc dcdcn n
dmdc
m
dcn nm
V VV V
V V
V
V VV
-
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192192
By plotting VO(dc)versus ,
we obtain the control characteristic of
a single phase full wave fully
controlled bridge converter
(single phase full converter)
for constant & continuousload current operation.
-
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-
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194194
VO(dc)
Vdm
cosdc dmV V
-
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195195
Trigger angle in degrees
030 60 90
0.2 Vdm
0.6Vdm
-0.6 Vdm
-0.2Vdm
-Vdm
120 150 180
-
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196196
During the period from t = to the inputvoltage vSand the input current iSare both
positive and the power flows from the
supply to the load. The converter is said to be operated in the
rectification mode
Controlled Rectifier Operationfor 0 < < 900
-
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197197
During the period from t = to (+),the input voltage vSis negative and theinput current iSis positive and the outputpower becomes negative and there will be
reverse power flow from the load circuit tothe supply.
The converter is said to be operated in theinversion mode.
Line Commutated Inverter Operation
for 900 < < 1800
Lecture-8
-
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198
Two Quadrant Operation
of a Single Phase Full Converter
Two Quadrant Operationof a Single Phase Full Converter
-
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199199
0
-
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200200
p g
2
2
0
The rms value of the output voltage
is calculated as
1
.2 OO RMSV v d t
The single phase full converter gives two
-
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201201
The single phase full converter gives two
output voltage pulses during the input supply
time period and hence the single phase full
converter is referred to as a two pulse converter.
The rms output vo
2
ltage can be calculated as
2 .2
OO RMSV v d t
2 21 sin .mO RMSV V t d t
-
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202202
22
2
2
sin .
1 cos 2.
2
cos 2 .2
m
O RMS
m
O RMS
m
O RMS
VV t d t
tVV d t
VV d t t d t
2
-
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203203
2
2
2
sin222
sin 2 sin 2
2 2
sin 2 2 sin 2;
2 2
sin 2 2 sin 2
mO RMS
m
O RMS
m
O RMS
V tV t
V
V
VV
2
sin 2 sin 2mO RMS
VV
-
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204204
2 2
2 2
02 2 2
2
Hence the rms output voltage is same as therms input supply voltage
O RMS
m m m
O RMS
mSO RMS
V V VV
VV V
-
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iOConstant Load Currenti =IO a
I
-
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206206
i
i
T1
T2&
Ia
t
t
t
Iai
i
T3
T4&
Ia
Ia
The rms thyristor current can be
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207207
calculated as
2The average thyristor current can be
calculated as
2
O RMS
T RMS
O dc
T Avg
II
II
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power Electronics
unit-5
208
THREE PHASE LINE
COMMUTATED CONVERTERS
LECTURE PLAN
Sl.
No
Module as per Session Planner Lecture
No.
PPT Slide
No.
-
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209
No.
1Introduction to Three phase converters L 1 3-10
2 3-Phase Half Wave Converter
(3-Pulse Converter)L2 11-26
3 3 Phase Half WaveControlled Rectifier
Output Voltage Waveforms For RL
Load atDifferent Trigger AnglesL3 27-39
4 Three Phase Semi-converters L 4 40-52
5 Wave forms of 3 Phase Semi-converter
for600 and Discussion
L 5 52-63
6 Three Phase Full Converter L 6 64-77
7 Single Phase Dual Converter L 7 78-99
8 Three Phase Dual Converters L 8 100-119
Lecture-1
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power Electronics
unit-5
210
Introduction to
Three phase converters
1-phase Controlled Rectifiers
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power Electronics
unit-5
211
Single phase half controlled bridgeconverters & fully controlled bridgeconverters are used extensively inindustrial applications up to about
15kW of output power.
The single phase controlled rectifiersprovide a maximum dc output of
The output ripple frequency is equal tothe twice the ac supply frequency.
max
2 mdc
VV
Contd
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power Electronics
unit-5
212
The single phase full wave controlledrectifiers provide two output pulses during
every input supply cycle and hence are
referred to as two pulse converters
3 Phase Controlled Rectifiers
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power Electronics
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213
Three phase converters are 3-
phase controlled rectifiers
which are used to convert acinput power supply into dc
output power across the load
Features of 3-phase controlledrectifiers
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power Electronics
unit-5
214214
Operate from 3 phase ac supply voltage. They provide higher dc output voltage.
Higher dc output power.
Higher output voltage ripple frequency. Filtering requirements are simplified for
smoothing out load voltage and load
current.
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power Electronics
unit-5
215215
Extensively used in high power variablespeed industrial dc drives.
Three single phase half-wave converters
can be connected together to form a threephase half-wave converter.
Classification of 3-phaseconverters
-
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power Electronics
unit-5
216
3-phase half wave converter
3-phase semi converter
3-phase full converter 3- phase dual converter
Classification according tono of pulses in the output wave
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power Electronics
unit-5
217
3- pulse converter
6-pulse converter 12- pulse converter
3-Phase
Lecture-2
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power Electronics
unit-5
218218
Half Wave Converter(3-Pulse Converter)
withR-L Load
Continuous & Constant
Load Current Operation
Circuit Diagram of 3- pulse converter
-
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219219
Vector Diagram of
3 Phase Supply Voltages
-
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power Electronics
unit-5
220220
VAN
VCN
VBN
1200
1200
1200 RN AN
YN BN
BN CN
v v
v v
v v
3 Phase Supply Voltage
Equations
-
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unit-5
221221
q
We deifine three line to neutral voltages
(3 phase voltages) as follows
-
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-
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power Electronics
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223223
van vbn vcn van
Constant Load
Each thyristor conducts for 2/3 (1200)
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224224
io=I
a
Constant Load
Current
Ia
Ia
-
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power Electronics
unit-5
225225
To Derive anExpression for the
Average Output Voltage of a
3-Phase Half Wave Converterwith RL Load
for Continuous Load Current
0
1 30T is triggered at t
-
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power Electronics
unit-5
226226
1
0
2
0
3
0
6
5 150
6
7 270
6
2Each thytistor conducts for 120 or radians3
gg
T is triggered at t
T is triggered at t
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0 0 0 0cos 180 30 cos sin 180 30 sin
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power Electronics
unit-5
230230
0 0
0 0
0 0
0
0
0
0
0 0
Note: cos 1
cos 180 30 cos sin 180 30 sin32 cos 30 .cos sin 30 sin
cos 30 cos sin 30 sin3
2 cos 30 .cos sin 30 s
80 30 cos 30
sin 180 30 sin 30
in
mdc
m
dc
VV
VV
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The rms value of output voltage is found by
using the equation
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power Electronics
unit-5
233233
15 26
2 2
6
1
2
3sin .
2
and we obtain
1 33 cos 26 8
mO RMS
mO RMS
V V t d t
V V
3 Phase Half Wave
Lecture-3
-
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power Electronics
unit-5
234234
Controlled Rectifier Output
Voltage Waveforms For RL
Loadat
Different Trigger Angles
Van
V0
=300
Vbn Vcn
=300
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power Electronics
unit-5
235235
0
0
300
300
600
600
900
900
1200
1200
1500
1500
1800
1800
2100
2100
2400
2400
2700
2700
3000
3000
3300
3300
3600
3600
3900
3900
4200
4200
V0
Van
=600
Vbn Vcn
t
t
=600
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power Electronics
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236236
030
060
090
0120
0150
0180
0210
0240
0270
0300
0330
0360
0390
0420
0
V0
Van
=900
Vbn Vcn
t
=900
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power Electronics
unit-5
237237
3 Phase Half WaveControlled Rectifier With
R Loadand
RL Load with FWD
T1 T1
-
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power Electronics
unit-5
238238
a a
b b
c c
R
V0L
R V0
+
T2
T3
n n
T2
T3
3 Phase Half Wave
-
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power Electronics
unit-5
239239
Controlled Rectifier Output
Voltage Waveforms For R Load
or RL Load with FWDat
Different Trigger Angles
Vs
Van
=0
Vbn Vcn
=00
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power Electronics
unit-5
240240
0
0
300
300
600
600
900
900
1200
1200
1500
1500
1800
1800
2100
2100
2400
2400
2700
2700
3000
3000
3300
3300
3600
3600
3900
3900
4200
4200V0
=150
t
Van Vbn Vcn
t
=150
0
=300
Van Vbn Vcn
=300
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power Electronics
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241241
0
300
300
600
600
900
900
1200
1200
1500
1500
1800
1800
2100
2100
2400
2400
2700
2700
3000
3000
3300
3300
3600
3600
3900
3900
4200
4200
V0 t
V0
=600Van Vbn Vcn
t
=600
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power Electronics
unit-5
242242
To Derive An Expression For The
Average Or Dc Output Voltage Of A
3 Phase Half Wave Converter WithResistive Load Or RL Load With FWD
01 306
T is triggered at t
-
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power Electronics
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243243
0 0
1
0
2
0 0
2
0
30 180 ;
sin
5 150
6
150 300 ;
sin 120
O an m
O bn m
T conducts from to
v v V t
T is triggered at t
T conducts from to
v v V t
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power Electronics
unit-5
244244
0
3
0 03
0
0
7 270
6
270 420 ;
sin 240
sin 120
O cn m
m
T is triggered at t
T conducts from to
v v V t
V t
0
0
180
30
3.
2dc O
V v d t
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power Electronics
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245245
0
0
0
0
30
0 0
180
30
180
30
sin ; for 30 to 180
3 sin .2
3sin .2
O an m
dc m
mdc
v v V t t
V V t d t
VV t d t
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Lecture-4
-
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power Electronics
unit-5
247
Three Phase Semi-converters
Three Phase Semi-converters
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power Electronics
unit-5
248248
3 Phase semi-converters are used in
Industrial dc drive applications upto 120kW
power output.
Single quadrant operation is possible.
Power factor decreases as the delay angle
increases.
Power factor is better than that of 3 phase
half wave converter.
3 Phase
H lf C t ll d B id C t
-
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power Electronics
unit-5
249249
Half Controlled Bridge Converter(Semi Converter)
with Highly Inductive Load &
Continuous Ripple free Load
Current
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power Electronics
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250250
-
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power Electronics
unit-5
251251
Wave forms of 3 Phase
Semiconverter for
> 600
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252252
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253253
3 phase semiconverter output ripple frequency of
t t lt i 3 f
-
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power Electronics
unit-5
254254
0 0
1
output voltage is 3
The delay angle can be varied from 0 to
During the period
30 210
7 , thyristor T is forward biased6 6
Sf
t
t
1If thyristor is triggered at ,6
& d t t th d th li t li lt
T t
T D
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power Electronics
unit-5
255255
1 1& conduct together and the line to line voltage
appears across the load.
7At , becomes negative & FWD conducts.6
The load current contin
ac
ac m
T D
v
t v D
1 1
ues to flow through FWD ;
and are turned off.
mD
T D
1
2
If FWD is not used the would continue to
d t til th th i t i t i d t
mD T
T
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power Electronics
unit-5
256256
2
1 2
conduct until the thyristor is triggered at5
, and Free wheeling action would6
be accomplished through & .
If the delay angle , e3
T
t
T D
ach thyristor conducts
2for and the FWD does not conduct.
3 mD
-
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3 sin6
RB ac an cn mv v v v V t
-
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power Electronics
unit-5
258258
53 sin
6
3 sin2
3 sin6
YR ba bn an m
BY cb cn bn m
RY ab an bn m
v v v v V t
v v v v V t
v v v v V t
Lecture-5
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power Electronics
unit-5
259259
Wave forms of 3 Phase
Semiconverter for
600
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260260
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power Electronics
unit-5
261261
-
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power Electronics
unit-5
262262
To derive an Expression for the
-
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power Electronics
unit-5
263263
To derive an Expression for theAverage Output Voltage of 3 Phase
Semi-converter for > / 3
and Discontinuous Output Voltage
For and discontinuous output voltage:3
the Average output voltage is found from
-
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power Electronics
unit-5
264264
76
6
76
6
the Average output voltage is found from
3
.2
33 sin
2 6
dc ac
dc m
V v d t
V V t d t
3 31 cos
2
3 1
mdc
mL
VV
VV
-
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power Electronics
unit-5
265265
max
3 1 cos2
3 Max. value of line-to-line supply voltage
The maximum average output voltage that occurs at
a delay angle of 0 is
3 3
mLdc
mL m
mdmdc
VV
V V
VV V
The normalized average output voltage is
0 5 1 cosdcVV
-
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power Electronics
unit-5
266266
17 2
62
6
0.5 1 cos
The rms output voltage is found from
3.
2
dcn
dm
acO rms
VVV
V v d t
17
263
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power Electronics
unit-5
267267
262 2
6
1
2
33 sin
2 6
3 sin 23
4 2
mO rms
mO rms
V V t d t
V V
-
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For and continuous output voltage3
-
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power Electronics
unit-5
269269
562
6 2
For , and continuous output voltage3
3
. .2
3 31 cos2
dc ab ac
mdc
V v d t v d t
VV
0.5 1 cos
RMS value of o/p voltage is calculated by using
dcn
dm
VV
V
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power Electronics
unit-5
270270
15 2
62 2 2
6 2
1
22
RMS value of o/p voltage is calculated by usingthe equation
3 . .2
3 23 3 cos
4 3
ab acO rms
mO rms
V v d t v d t
V V
Lecture -6
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power Electronics
unit-5
271
Three Phase Full Converter
Three Phase Full Converter
3 Phase Fully Controlled Full Wave Bridge
Converter
-
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power Electronics
unit-5
272272
Converter.
Known as a 6-pulse converter.
Used in industrial applications up to120kW output power.
Two quadrant operation is possible.
-
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power Electronics
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273273
-
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274274
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unit-5
275275
The thyristors are triggered at an interval of
/ 3.
Th f f i l l i
-
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power Electronics
unit-5
276276
The frequency of output ripple voltage is
6fS.
T1is triggered at
t = (
/6 +
), T6isalready conducting when T1is turned ON.
During the interval (/6 + ) to (/2 + ),
T1and T6conduct together & the outputload voltage is equal to vab = (vanvbn)
T2is triggered at t = (/2 + ), T6turns
off naturally as it is reverse biased as soon
as T is triggered
-
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power Electronics
unit-5
277277
as T2is triggered.
During the interval (/2 + ) to (5/6 + ),
T1and T2conduct together & the output
load voltage vO= vac= (vanvcn)
Thyristors are numbered in the order in
which they are triggered.
The thyristor triggering sequence is 12,
23, 34, 45, 56, 61, 12, 23, 34,
We deifine three line neutral voltages
(3 phase voltages) as follows
sin ; Max Phase VoltageRN an m mv v V t V
-
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power Electronics
unit-5
278278
0
0
0
sin ; Max. Phase Voltage
2sin sin 120
3
2sin sin 120
3
sin 240
RN an m m
YN bn m m
BN cn m m
m
v v V t V
v v V t V t
v v V t V t
V t
V
is the peak phase voltage of a wye-connected source.
m
The corresponding line-to-line
supply voltages are
-
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power Electronics
unit-5
279279
3 sin6
3 sin2
3 sin2
RY ab an bn m
YB bc bn cn m
BR ca cn an m
v v v v V t
v v v v V t
v v v v V t
To Derive An Expression For
The Average Output Voltage
-
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power Electronics
unit-5
280280
The Average Output Voltage
Of
3-phase Full ConverterWith Highly Inductive Load
Assuming Continuous And
Constant Load Current
The output load voltage consists of 6
voltage pulses over a period of 2radians,
Hence the average output voltage is
-
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power Electronics
unit-5
281281
2
6
6. ;2
3 sin6
dc OO dc
O ab m
V V v d t
v v V t
Hence the average output voltage iscalculated as
2
6
33 sin .
6dc mV V t d t
-
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power Electronics
unit-5
282282
mL
max
3 3 3cos cos
Where V 3 Max. line-to-line supply voThe maximum average dc output voltage is
obtained for a delay angle
ltage
3 3
0,
3
m mLdc
m
m mdmdc
V VV
V
V VV V
L
The normalized average dc output voltage is
cosdcVV V
-
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power Electronics
unit-5
283283
1
22
2
6
cos
The rms value of the output voltage is found from
6.
2
dcn n
dm
OO rms
VV VV
V v d t
1
22
2
6
6.
2
abO rmsV v d t
-
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power Electronics
unit-5
284284
6
1
22
2 2
6
1
2
3 3 sin .2 6
1 3 33 cos 22 4
mO rms
mO rms
V V t d t
V V
Lecture-7
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power Electronics
unit-5
285
Single Phase Dual Converter
Single Phase Dual Converter
-
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power Electronics
unit-5
286286
-
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power Electronics
unit-5
287287
-
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288288
-
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power Electronics
unit-5
289289
Th d l f 1 i
-
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power Electronics
unit-5
290290
1 1
2 2
The average dc output voltage of converter 1 is
2cos
The average dc output voltage of converter 2 is
2
cos
m
dc
m
dc
VV
V
V
In the dual converter operation one
converter is operated as a controlled rectifier
-
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power Electronics
unit-5
291291
0
0
1
converter is operated as a controlled rectifier
with 90 & the second converter is
operated as a line commutated inverter
in the inversion mode with 90
dcV V
2dc
1 2 2
1 2
2 2 2cos cos cos
cos cos
m m mV V V
-
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power Electronics
unit-5
292292
2 1 1
2 1
1 2
2 1
or
cos cos cos
or
radians
Which gives
To Obtain an Expression
-
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power Electronics
unit-5
293293
To Obtain an Expression
for the
Instantaneous CirculatingCurrent
vO1 = Instantaneous o/p voltage of converter 1.
vO2= Instantaneous o/p voltage of converter 2.
The circulating current ir can be determined byi t ti th i t t lt diff
-
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power Electronics
unit-5
294294
g yintegrating the instantaneous voltage difference
(which is the voltage drop across the circulating
current reactor Lr), starting from t = (2- 1). As the two average output voltages during the
interval t = (+1)to (2- 1)are equal and
opposite their contribution to the instantaneouscirculating current iris zero.
1
1 2
2
1. ;
t
r r r O O
r
i v d t v v v
L
-
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power Electronics
unit-5
295295
1
2
1 2
1 2
2
1 1
As the o/p voltage is negative
1. ;
sin for 2 to
O
r O O
t
r O O
r
O m
v
v v v
i v v d t L
v V t t
t t
-
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power Electronics
unit-5
296296
1 12 2
1
sin . sin .
2cos cos
The instantaneous value of the circulating currentdepends on the delay angle.
t t
mr
r
mr
r
Vi t d t t d t
L
Vi t
L
1For trigger angle (delay angle) 0,
the magnitude of circulating current becomes min.
when , 0,2,4,.... & magnitude becomest n n
-
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power Electronics
unit-5
297297
g
max. when , 1,3,5,....
If the peak load current is , one ofp
t n n
I
the
converters that controls the power flow
may carry a peak current of
4 ,mp
r
VIL
where
-
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power Electronics
unit-5
298298
max
max
where
,
&
4
max. circulating current
mp L
L
m
r
r
VI I
R
V
i L
Different Modes Of Operation of
Dual converter
-
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power Electronics
unit-5
299299
Non-circulating current (circulating current
free) mode of operation.
Circulating current mode of operation.
-
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CirculatingCurrent Mode Of Operation
-
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power Electronics
unit-5
301301
In this mode, both the converters are
switched ON and operated at the same
time. The trigger angles 1and 2are adjusted
such that (1+ 2) = 1800; 2= (180
0-
1).
When 0
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p 2
In this case Vdcand Idc, both are positive.
When 900 900
Conv. 2
Rectifyin
g
2 < 900
Rectifyin
g
1 < 900
Conv. 1
Inverting1 > 90
0
Contd
There are two different modes of
operation.
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Circulating current free
(non circulating) mode of operation
Circulating current mode of operation
Non CirculatingCurrent Mode Of Operation
In this mode of operation only oneconverter is switched on at a time
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When the converter 1 is switched on,
For 1< 900the converter 1 operates in
the Rectification mode
Vdcis positive, Idcis positive and hence theaverage load power Pdcis positive.
Power flows from ac source to the load
When the converter 1 is on,For 1 > 90
0 the converter 1 operates in
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For 1> 90 the converter 1 operates in
the Inversion mode
Vdcis negative, Idcis positive and theaverage load power Pdcis negative.
Power flows from load circuit to ac source.
When the converter 2 is switched on,For 2< 90
0the converter 2 operates in
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2 pthe Rectification mode
Vdc
is negative, Idc
is negative and theaverage load power Pdcis positive.
The output load voltage & load currentreverse when converter 2 is on.
Power flows from ac source to the load
When the converter 2 is switched on,For 2> 90
0the converter 2 operates in
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2 pthe Inversion mode
Vdc
is positive, Idc
is negative and theaverage load power Pdcis negative.
Power flows from load to the ac source.
Energy is supplied from the load circuit to
the ac supply.
Circulating CurrentMode Of Operation Both the converters are switched on at the
same time. One converter operates in the rectification
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One converter operates in the rectificationmode while the other operates in the
inversion mode. Trigger angles 1& 2are adjusted such
that (1+ 2) = 1800
When 1< 900, converter 1 operates as a
controlled rectifier. 2 is made greaterth 900 d t 2 t
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than 900 and converter 2 operates as an
Inverter.
Vdcis positive & Idcis positive and Pdcispositive.
When 2< 900, converter 2 operates as a
controlled rectifier. 1 is made greaterthan 900 and con erter 1 operates as an
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than 900 and converter 1 operates as an
Inverter.
Vdcis negative & Idcis negative and Pdcispositive.
A C Voltage Controller
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Power Electronics Unit-6 327
A.C Voltage Controller
And
Cyclo-Converter
LECTURE PLANSl. No Module as per Session Planner Lecture No. PPT Slide No.
1 Introduction to AC voltage controllers L-1 3-12
2 Expression For The RMS Value OfOutput Voltage, For ON-OFF Control
Method
L-2 13-27
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Power Electronics Unit-6 328
3 Principle Of AC Phase Control And
Operation of single Phase half-Wave
Ac Voltage controller with R-Load
L-3 28-43
4 Single Phase Full Wave Ac VoltageController (Bidirectional Controller)
With R-Load
L-4 44-59
5 TRIAC and Its Modes of Operation L-5 60-73
6 Single phase full wave ac voltage
controller (Bi-directional Controller) usingTRIAC L-6 74-91
7 Cycloconverter Midpoint Type L-7 92-101
8 1-to 1-Bridge type Cyclo-converter
with R and R-L loadL-8 101-109
Lecture-1
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Ac Voltage Controllers
Ac Voltage controller circuits(RMS voltage controllers)
An ac voltage controller is a type of thyristor
power converter which is used to convert a
fi d l fi d f i l
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fixed voltage, fixed frequency ac input supply
to obtain a variable voltage ac output
Applications Of Ac Voltage
Controllers
Lighting / Illumination control in ac powercircuits.
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Power Electronics Unit-6 331
Induction heating.
Industrial heating & Domestic heating.
Transformer tap changing (on load
transformer tap changing).
Speed control of induction motors C
magnet controls.
Type Of Ac Voltage Controllers
Single phase half wave ac voltage controller(Uni-directional controller)
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Power Electronics Unit-6 332
(Uni-directional controller).
Single phase full wave ac voltage controller
(Bi-directional controller). Three phase half wave ac voltage controller
(Uni-directional controller).
Three phase full wave ac voltage controller(Bi-directional Controller)
A.C voltage control technique
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Principle of ON-OFF ControlTechnique
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Vs
Vo
i
wt
n m
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io
ig1
ig2
wt
wt
wt
Gate pulse of T1
Gate pulse of T2
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Lecture-2
Expression For The RMS Value Of
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Expression For The RMS Value Of
Output Voltage, For ON-OFF
Control Method
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