A chopper is a static device that uses pulse width modulation or variable frequency control to obtain a variable DC output voltage from a constant DC input voltage. Choppers are widely used to control motors and regenerate braking energy. The document describes different types of choppers - Type A chops the input voltage to produce positive output voltage and current. Type B allows regenerative braking by producing negative current. Type C operates in both quadrants while Type D's output voltage can be positive or negative.

1. Choppers
Fixed DC Supply Variable DC Output
?
A. K. Gautam
By: Aniruddha Kr. Gautam

2. • A chopper is a static device which is used to
obtain a variable dc voltage from a constant dc
voltage source.
• Also known as dc‐to‐dc converter.
• It offers greater efficiency, faster response, lower
maintenance, smaller size and smooth control.
• Widely used in trolley cars, battery operated
vehicles, traction motor control, control of large
number of dc motors, etc…
• Also used in regenerative braking of dc motors to
return energy back to supply and also as dc
voltage regulators.
A. K. Gautam

3. METHODS OF CONTROL:
The output dc voltage can be verified by the following methods.
• Constant Frequency Control or Pulse width modulation control
• Variable Frequency Control
PULSE WIDTH MODULATION
In Pulse width modulation the pulse width ton of the output waveform
is varied keeping chopping frequency ’f’ and hence chopping period ‘T’
constant. Therefore output voltage is varied by varying the ON time, ton .
Figure shows the output voltage waveform for different ON times.
VARIABLE FREQUENCY CONTROL
In this method of control, chopping frequency f is varied keeping
either ton or toff constant. This method is also known as frequency
modulation.
In frequency modulation to obtain full output voltage, range of
frequency has to be varied over a wide range. This method produces
harmonics in the output and for large toff load current may be
discontinuous.
A. K. Gautam

4. A. K. Gautam
V0
V
V
V0
t
t
tON
tON tOFF
tOFF
T

5. A. K. Gautam
v0
V
V
v0
t
t
tON
tON
T
T
tOFF
tOFF

6. Basic DC to DC converters
• Buck converter (Step-down converter)
• Boost converter (Step-up converter)
• Buck-Boost converter (Step-down/step-up converter)
and
• Cuk converter
A. K. Gautam

7. Buck converter (Step-down converter)
A. K. Gautam

8. A. K. Gautam

9. • Diode is reversed biased.
Switch conducts inductor
current
• This results in positive
inductor voltage, i.e.:
VL=Vd-VO
• It causes linear increase in
the inductor current.
A. K. Gautam
Circuit operation when switch is turned on (closed)

10. Operation when switch turned off (opened)
• Because of inductive energy
storage, iL continues to flow.
• Diode is forward biased.
• Current now flows through
the diode and,
A. K. Gautam

11. Analysis for switch closed
• The inductor voltage
• Since the derivative if iL is a
positive constant. Therefore
iL must increase linearly.
A. K. Gautam

12. A. K. Gautam
Analysis for switch opened

13. Steady-state operation
• Steady state operation
requires that iL
• Steady state operation
requires that iL at the end of
switching cycle is the same
at the beginning of the next
cycle. That is change of iL
over one period is zero. i.e.
A. K. Gautam

14. Steady State Time Domain Analysis of Type-A Chopper
A. K. Gautam
Output
voltage
Output
current
v0
V
i0
Imax
Imin
t
t
tON
T
tOFF
Continuous
current
Output
current
t
Discontinuous
current
i0

15. Expressions For Load Current iO For Continuous Current
Operation When Chopper is ON (0 t tON)
A. K. Gautam
V
i0
V0
R
L
E
+
-

16. A. K. Gautam

17. A. K. Gautam

18. A. K. Gautam

19. Steady State Ripple
A. K. Gautam
)26.2.........(....................
1
11
1
1
1
1
1
1
1
1
)(
minmax
a
aonaon
aa
aonaon
a
aon
a
aon
a
aon
TT
TTTTT
S
TTTT
TTTT
TT
TT
S
TT
TT
TT
TT
S
e
ee
R
V
ee
ee
e
e
R
V
e
e
e
e
R
V
II
The ripple current given by the equation is seen to be independent of load
current emf E With Ton= αT and T-Ton = (1-α)T can be written as
a
a
T
a
T
T
TT
T
S
e
ee
R
V
II
1
11
1
minmax

20. Limit of Continuous Conduction
• In a chopper if Ton is reduced , Toff increases for a constant chopping period
T.
• As Ton gets low and Toff goes high so current I may fall to zero.
• As in step down chopper current cannot go reverse so for limit current can
go to only zero from Imin (Eqn. 2.20)
• We can get value of α is obtain by equating the above equation.
A. K. Gautam
)27.2.......(....................11ln
1
1
0
1
1
'
min
a
a
a
on
a
a
on
T
T
aon
ST
T
T
T
T
T
T
T
S
em
T
T
T
T
m
V
E
e
e
R
E
e
e
R
V
I

21. • So for Given Value of E, VS, T and Ta; if duty cycle is α’ then
current goes at just continuous point.
• If actual duty cycle is less than α’ , load current will be
discontinuous.
A. K. Gautam

22. CCM and DCM of Buck Converter
A. K. Gautam

23. Step Up (Boost)Chopper
A. K. Gautam

24. • A boost converter (step-up converter) is a DC-to-
DC power converter with an output voltage greater
than its input voltage.
• It is a class of switched-mode power supply (SMPS)
containing at least two semiconductor switches
(a diode and a transistor) and at least one energy
storage element, a capacitor, inductor, or the two in
combination.
• Boost converter is also used as the voltage increase
mechanism in the circuit known as the 'Joule thief'.
• For a step-up chopper we can obtain an average
output voltage V0 greater than input voltage.
A. K. Gautam

25. • Step-up chopper is used to obtain a load voltage higher
than the input voltage V.
• The values of L and C are chosen depending upon the
requirement of output voltage and current.
• When the chopper is ON, the inductor L is connected
across the supply.
• The inductor current ‘I’ rises and the inductor stores
energy during the ON time of the chopper, tON.
• When the chopper is off, the inductor current I is forced
to flow through the diode D and load for a period, tOFF.
• The current tends to decrease resulting in reversing the
polarity of induced EMF in L.
• Therefore voltage across load is given by:
A. K. Gautam

26. • A large capacitor ‘C’ connected across the load, will provide a
continuous output voltage .
• Diode D prevents any current flow from capacitor to the
source.
A. K. Gautam
. .,O O
dI
V V L i e V V
dt

27. Operating Principle
• The key principle that drives the boost converter is the
tendency of an inductor to resist changes in current.
Mode 1 (On State):
When the switch is closed, current flows through the inductor in
clockwise direction and the inductor stores the energy. Polarity
of the left side of the inductor is positive.
A. K. Gautam

28. Mode 2 (Off State)
When the switch is opened, current will be reduced as the
impedance is higher. Therefore, change or reduction in current
will be opposed by the inductor. Thus the polarity will be
reversed (means left side of inductor will be negative now). As
a result two sources will be in series causing a higher voltage
to charge the capacitor through the diode D.
Here the switch is open and the only path offered to inductor
current is through the flyback diode D, the capacitor C and the
load R.
A. K. Gautam

29. Mode of conduction
Continuous Conduction mode:
• When a boost converter operates in continuous mode, the current through
the inductor (IL) never falls to zero.
• During the On-state, the switch S is closed, which makes the input voltage
(Vi) appear across the inductor.
• Change in current (IL) flowing through the inductor during a time period (t)
by the formula:
• At the end of the On-state, the increase of IL is therefore:
A. K. Gautam
L
V
t
I iL
i
DT
iL V
L
DT
dtV
L
I on
0
1

30. • D is the duty cycle. It represents the fraction of the
commutation period T during which the switch is On.
• D ranges between 0 (S is never on) and 1 (S is always on).
• During the Off-state, the switch S is open, so the inductor
current flows through the load. If we consider zero voltage
drop in the diode, and a capacitor large enough for its voltage
to remain constant, the evolution of IL is:
• Therefore, the variation of IL during the Off-period is:
A. K. Gautam
dt
dI
LVV L
oi
L
TDVV
L
dtVV
I oi
T
DT
oi
Loff
1)()(

31. • considering that the converter operates in steady-state
conditions, so the amount of energy stored in each of its
components has to be the same at the beginning and at the end
of a commutation cycle. In particular, the energy stored in the
inductor is given by:
• So, the inductor current has to be the same at the start and end
of the commutation cycle. This means the overall change in
the current (the sum of the changes) is zero:
A. K. Gautam
2
2
1
LLIE
0
1
0
L
TDVV
L
DTV
II
II
oii
Ll
Ll
offon
offon

32. • Expression shows that the output voltage is
always higher than the input voltage (as the
duty cycle goes from 0 to 1), and that it
increases with D,
A. K. Gautam
o
i
i
o
V
V
D
DV
V
1
1
1

33. A. K. Gautam

34. Discontinuous Conduction mode:
• If the ripple amplitude of the current is too high, the
inductor may be completely discharged before the
end of a whole commutation cycle.
• Occurs under light loads.
• Here the current through the inductor falls to zero
during part of the period.
• As the inductor current at the beginning of the cycle
is zero, its maximum value:
A. K. Gautam
)( DTtat
L
DTV
I i
LMax

35. • During the off-period, IL falls to zero after :
• The load current Io is equal to the average diode current (ID).
Also the diode current is equal to the inductor current during
the off-state. Therefore the output current can be written as:
A. K. Gautam
io
i
i
L
VV
DV
So
L
TVV
I Max
,
0
)( 0
o
i
i
o
io
i
io
ii
o
L
Do
LI
TDV
V
V
So
VVL
TDV
VV
DV
L
DTV
ISo
I
II Maz
2
1,
22
,
2
2
22

36. A. K. Gautam

37. (CCM) and (DCM) of boost
A. K. Gautam

38. Types of Choppers
• Type A Chopper or First–Quadrant Chopper
• Type B Chopper or Second-Quadrant Chopper
• Type-C chopper or Two-quadrant type-A
Chopper
• Type-D Chopper or Two-Quadrant Type–B
Chopper
• Type-E chopper or the Fourth-Quadrant
Chopper
A. K. Gautam

39. Type A Chopper or First–Quadrant Chopper
A. K. Gautam

40. • When chopper is ON, supply voltage V is connected across the
load.
• When chopper is OFF, vO = 0 and the load current continues to
flow in the same direction through the FWD.
• The average values of output voltage and current are always
positive.
• Class A Chopper is a step-down chopper in which power
always flows form source to load.
• It is used to control the speed of dc motor.
• The output current equations obtained in step down chopper
• with R-L load can be used to study the performance of Class A
Chopper
A. K. Gautam

41. Type B Chopper or Second-Quadrant Chopper
A. K. Gautam

42. • When chopper is ON, E drives a current through L and
R in a direction opposite to that shown in figure.
• During the ON period of the chopper, the inductance L
stores energy.
• When Chopper is OFF, diode D conducts, and part of
the energy stored in inductor L is returned to the supply.
• Average output voltage is positive and average output
current is negative.
• In this chopper, power flows from load to source.
• Class B Chopper is used for regenerative braking of dc
motor.
• Class B Chopper is a step-up chopper.
A. K. Gautam

43. Type-C chopper or Two-quadrant type-A Chopper
A. K. Gautam

44. • Class C Chopper is a combination of Class A and Class B
Choppers.
• For first quadrant operation, CH1 is ON or D2 conducts.
• For second quadrant operation, CH2 is ON or D1 conducts.
• When CH1 is ON, the load current is positive.
• The output voltage is equal to ‘V’ & the load receives power
from the source.
• When CH1 is turned OFF, energy stored in inductance L forces
current to flow through the diode D2 and the output voltage is
zero.
• Current continues to flow in positive direction.
• When CH2 is triggered, the voltage E forces current to flow in
opposite direction through L and CH2
• The output voltage is zero.
A. K. Gautam

45. • On turning OFF CH2, the energy stored in the inductance
drives current through diode D1 and the supply Output voltage
is V, the input current becomes negative and power flows from
load to source.
• Average output voltage is positive
• Average output current can take both positive and negative
values.
• Choppers CH1 & CH2 should not be turned ON
simultaneously as it would result in short circuiting the supply.
• Class C Chopper can be used both for dc motor control and
regenerative braking of dc motor.
• Class C Chopper can be used as a step-up or step-down
chopper.
A. K. Gautam

46. Type-D Chopper or Two-Quadrant Type –B Chopper
A. K. Gautam

47. • Class D is a two quadrant chopper.
• When both CH1 and CH2 are triggered simultaneously,
the output voltage vO = V and output current flows
through the load.
• When CH1 and CH2 are turned OFF, the load current
continues to flow in the same direction through load, D1
and D2, due to the energy stored in the inductor L.
• Output voltage vO = - V
• Average load voltage is positive if chopper ON time is
more than the OFF time
• Average output voltage becomes negative if tON < tOFF .
• Hence the direction of load current is always positive but
load voltage can be positive or negative.
A. K. Gautam

48. Type-E chopper or the Fourth-Quadrant Chopper
A. K. Gautam

49. • Class E is a four quadrant chopper
• When CH1 and CH4 are triggered, output current
iO flows in positive direction through CH1 and
CH4 , and with output voltage vO = V.
• This gives the first quadrant operation.
• When both CH1 and CH4 are OFF, the energy
stored in the inductor L drives iO through D2 and
D3 in the same direction, but output voltage vO = -
V.
• Therefore the chopper operates in the fourth
quadrant.
A. K. Gautam

50. • When CH2 and CH3 are triggered, the load current iO
flows in opposite direction & output voltage vO = -V.
• Since both iO and vO are negative, the chopper
operates in third quadrant.
• When both CH2 and CH3 are OFF, the load current iO
continues to flow in the same direction D1 andD4 and
the output voltage vO = V.
• Therefore the chopper operates in second quadrant as
vO is positive but iO is negative.
A. K. Gautam