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Power Electronics
Dr. Imtiaz Hussain
Assistant Professor
email: imtiaz.hussain@faculty.muet.edu.pk
URL :http://imtiazhussainkalwar.weebly.com/
Lecture-10
D.C to D.C Converters (Choppers)
1
Power Electronic Interface
• Power Electronics is an enabling technology providing the
needed interface between the electrical source and electrical
load.
• The source and load often do differ in frequency, voltage
amplitudes and number of phases.
2
Powering the information Technology
• Figure shows the distributed
architecture typically used in
computers.
• In which incoming voltage from
the utility is converted into dc
voltage (24V).
• This semi regulated voltage is
distributed within the computer
where on-board power supplies
convert this 24V into tightly
regulated lower voltage.
3
• Most of the consumer electronics equipment supplied from
the mains, internally needed very load dc voltages.
Powering the information Technology
• However, the electronic circuitry requires higher voltages.
• Thus necessitating a circuit to boost input dc to higher dc
voltages
4
• Many devices such as cell phones operates from low battery
voltages.
Introduction to D.C to D.C Converters (Choppers)
• DC to DC converters are important in portable electronic
devices such as cellular phones and laptop computers, which
are supplied with power from batteries primarily.
• Such electronic devices often contain several sub-circuits,
each with its own voltage level requirement different from
that supplied by the battery or an external supply.
• They are also widely used in dc-motor drive applications.
• Often input to these converters is an unregulated dc
voltage, which is obtained by rectifying the line voltage.
Introduction
Uncontrolled
Diode Rectifier
Load
D.C to D.C
Converter
Battery
Filter
AC Line
Voltage
1-Phase or
3-Phase
DC
Unregulated
DC
Unregulated
DC
Unregulated
DC
Regulated
vc
D.C to D.C Converter System
Efficiency & Power Losses
• High efficiency is essential in any power processing
application.
in
out
P
P


• The efficiency of a converter is
)
1
1
( 




out
out
in
loss P
P
P
P
• The power lost in converter is
Efficiency & Power Losses
• Efficiency is a good measure of the success of a given
converter technology.
• With very small amount of power lost, the converter
elements can be packaged with high density, leading to a
converter of small size and weight, and of low temperature
rise.
• How can we build a circuit that changes the voltage, yet
dissipates negligible power?
Efficiency & Power Losses
• The various conventional circuit elements are illustrated in
Following figure.
• The available circuit elements fall broadly into the classes of
resistive elements, capacitive elements, magnetic devices
including inductors and transformers, semiconductor devices
operated in the linear mode and semiconductor devices operated
in the switched mode.
Types of dc-dc Converters
• Types of D.C to D.C converters
– AC Link Choppers
– Linear Converters
– Switch Mode
– Magnetic
– E.t.c
AC Link Choppers
• First dc is converted to ac with the help of an inverter.
• After that, AC is stepped-up or stepped-down by a
transformer, which is then converted back to dc by a diode
rectifier.
• Ac link chopper is costly, bulky and less efficient as the
conversion is done in two stages.
Simple dc-dc Converters
• Let us now construct a simple dc-dc converter.
The input voltage vg is 100 V. It is desired to
supply 50 V to an effective 5Ω load, such that
the dc load current is 10 A.
Resistive dc-dc Converters
• Using Voltage divided rule.
Linear dc-dc Converters
• Linear Mode dc-dc converter
Switch Mode dc-dc Converters
Conclusion
• Capacitors and magnetic devices are important elements of
switching converters, because ideally they do not consume
power.
• It is the resistive element, as well as the linear-mode
semiconductor device, that is avoided.
• Semiconductor in switch mode however dissipate
comparatively low power in either states (ON and OFF).
• So capacitive and inductive elements, as well as switched-
mode semiconductor devices, are available for synthesis of
high-efficiency converters.
Switch Mode D.C to D.C Converters
• Switch-mode DC to DC converters convert one DC voltage
level to another, by storing the input energy temporarily
and then releasing that energy to the output at a different
voltage.
• This conversion method is more power efficient (often 75%
to 98%) than linear voltage regulation (which dissipates
unwanted power as heat).
• This efficiency is beneficial to increasing the running time
of battery operated devices.
Switch Mode D.C to D.C Converters
• PWM or PFM regulates the output dc voltage.
• The power flow through these converters is only in one
direction thus their voltages and currents remain unipolar.
Switch Mode D.C to D.C Converters
• A Chopper is a high speed on/off semiconductor switch.
• It connects source to load and disconnects source from load
at very high speed.
• In this manner a chopped dc voltage is obtained from a
constant dc supply Vs is obtained.
Switch Mode D.C to D.C Converters
• During the period Ton, the chopper is on and load voltage Vo
is equal to source voltage Vs.
• During the period Toff, the chopper is off and load current io
flows through the freewheeling diode.
Switch Mode D.C to D.C Converters
• The load voltage is given by
• Thus the load voltage can be varied by varying the switching
duty ratio D.
𝑉
𝑜 =
𝑇𝑜𝑛
𝑇𝑜𝑛 + 𝑇𝑜𝑓𝑓
𝑉
𝑠
𝑉
𝑜 =
𝑇𝑜𝑛
𝑇
𝑉
𝑠
𝑉
𝑜 = 𝐷𝑉
𝑠
𝑤ℎ𝑒𝑟𝑒, 𝐷 =
𝑇𝑜𝑛
𝑇
𝑖𝑠 𝑐𝑎𝑙𝑙𝑒𝑑 𝑠𝑤𝑖𝑡𝑐ℎ𝑖𝑛𝑔 𝑑𝑢𝑡𝑦 𝑟𝑎𝑡𝑖𝑜
𝑉
𝑜 = 𝑓𝑇𝑜𝑛𝑉
𝑠
Control of D.C to D.C Converters
• Average value of output voltage Vo can be controlled by
opening and closing the semiconductor switch periodically.
• The control strategies for varying duty ratio D are
1. Constant frequency system
2. Variable frequency system
22
Constant frequency system
• In this scheme Ton is varied but frequency is kept constant.
• Variation of Ton means adjustment of pulse width.
Therefore, this scheme is called PWM scheme.
𝑇𝑜𝑛 =
1
4
𝑇
𝑇𝑜𝑛 =
3
4
𝑇
𝑉
𝑜 =
1
4
𝑉
𝑠
𝑉
𝑜 =
3
4
𝑉
𝑠
Constant frequency system (PWM)
st
control
s
on
V
V
T
t
D 

amplifier
+
-
Comparator
Vo (desired)
Vo (actual)
Sawtooth Wave
Switch
Control Signal
Vcontrol
vcontrol
t
Ts
vst
Ton
Toff
Switch
Control
Signal
Variable frequency system
• In this scheme Ton is kept constant but the frequency is
varied.
Variable frequency system
• Or Toff is kept constant but the frequency is varied.
Switch Mode D.C to D.C Converters
• Types of Switch Mode D.C to D.C Converters
– Step-Down (Buck) converter
– Step-up (Boost) converter
– Step Down/Up (Buck-Boost) converter
Step-Down Converter (Buck Converter)
• As name implies a step-down converter produces a lower
average output voltage than the dc input voltage Vd.
• Its main application is in regulated dc power supplies and
dc-motor speed control.
Step-Down Converter (Buck Converter)
• Circuit operation when S is ON (closed)
– Diode is reversed biased. Switch conducts inductor current 𝑖𝐿.
– This results in positive inductor voltage, i.e:
– It causes linear increase in inductor current
𝑣𝐿 = 𝑉𝑑 − 𝑉
𝑜
𝑖𝐿 =
1
𝐿
𝑣𝐿 𝑑𝑡
Step-Down Converter (Buck Converter)
• Circuit operation when S is OFF (open)
– Because of inductive energy storage, 𝑖𝐿 continues to flow.
– Diode is reversed biased. Therefore current flows through
the diode.
𝑣𝐿 = −𝑉
𝑜
Step-Down Converter (Buck Converter)
dt
t
v
T
V
s
T
o
s
o 

0
)
(
1
dt
dt
t
V
T
V
off
on
on
t
t
t
d
s
o 
 
 0
)
(
1
0
d
s
on
o V
T
t
V 
d
o DV
V 
• Continuous conduction mode
– A buck converter operates in continuous mode if the current
through the inductor (IL) never falls to zero during the
commutation cycle.
Step-Down Converter (Buck Converter)
• Calculate D to obtain required output voltage.
• Select a particular switching frequency:
– –preferably >20KHz for negligible acoustic noise
• Higher fs results in smaller L, but higher device losses.
– Thus lowering efficiency and larger heat sink.
Design procedure for Buck Converter
• Inductor requirement
• C Calculation
• Possible switching devices: MOSFET, IGBT and BJT. Low power
MOSFET can reach MHz range.
Design procedure for Buck Converter
𝑟 =
1 − 𝐷
8𝐿𝐶𝑓2
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 𝐷
2𝑓
𝑅
Example-1
• A buck converter is supplied from a 50V battery source.
Given L=400uH, C=100uF, R=20 Ohm, f=20KHz and D=0.4.
Calculate: (a) output voltage (b) output voltage ripple.
35
Solution
(a) output voltage
𝑉
𝑜 = 𝐷𝑉
𝑠
𝑉
𝑜 = 0.4 × 50
𝑉
𝑜 = 20𝑉
Example-1
36
(b) Output Ripple
𝑟 =
1 − 𝐷
8𝐿𝐶𝑓2
𝑟 =
1 − 0.4
8 × 400𝜇 × 100𝜇 × (20𝐾)2
𝑟 = 4.6%
Example-2
• A buck converter has an input voltage of 50V and output of 25V.
The switching frequency is 10KHz. The power output is 125W. (a)
Determine the duty ratio, (b) value of L to ensure continuous
current, (c) value of capacitance to limit the output voltage ripple
factor to 0.5%.
37
Solution
(a) output voltage
𝑉
𝑜 = 𝐷𝑉
𝑠
(b) Value of L
𝐷 =
𝑉
𝑜
𝑉
𝑠
𝐷 =
25
50
= 0.5
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 𝐷
2𝑓
𝑅
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 0.5
2 × 10𝐾
𝑅
𝑃𝑜 =
𝑉2
𝑅
Example-2
• Resistance is calculated as
• L must at least be 10 times greater than Lmin.
38
𝑅 =
𝑉2
𝑃𝑜
=
252
125
= 5Ω
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 0.5
2 × 10𝐾
× 5
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
2.5
20𝐾
= 125𝜇𝐻
𝐿 = 1.25𝑚𝐻
Example-2
• Value of capacitance to limit the output voltage ripple factor to
0.5% can be calculated using following equation.
39
(c) Value of C
𝑟 =
1 − 𝐷
8𝐿𝐶𝑓2
0.005 =
1 − 0.5
8 × 1.25𝑚 × 𝐶 × (10𝐾)2
𝐶 =
1 − 0.5
8 × 1.25𝑚 × 0.005 × (10𝐾)2
𝐶 =
0.5
5000
= 100𝜇𝐹
Example-3
• Design a buck converter such that the output voltage is 28V when
the input is 48V. The load is 8Ohm. Design the converter such
that it will be in continuous current mode. The output voltage
ripple must not be more than 0.5%. Specify the frequency and
the values of each component. Suggest the power switch also.
40
Solution:
𝑉
𝑜 = 𝐷𝑉
𝑠
𝐷 =
28
48
= 0.58
• Then calculate the switching duty ratio
• First of all determine the switching frequency.
𝑓 = 25𝐾𝐻𝑧
Example-3
41
• Now value of inductor can be chosen to ensure continuous conduction
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 𝐷
2𝑓
𝑅
𝐿 ≥ 𝐿𝑚𝑖𝑛 =
1 − 0.58
2 × 25𝐾
× 80
𝐿 ≥ 𝐿𝑚𝑖𝑛 = 0.67𝑚𝐻
𝐿 = 6.7𝑚𝐻
Example-3
42
• Value of capacitance to limit the output voltage ripple factor to
0.5% can be calculated using following equation.
𝑟 =
1 − 𝐷
8𝐿𝐶𝑓2
𝐶 =
1 − 0.58
8 × 6.7𝑚 × 0.005 × (25𝐾)2
𝐶 =
0.42
167500
= 2.5𝜇𝐹
Example-3
43
• Selection of Power semiconductor switch
𝑓 = 25𝐾𝐻𝑧 𝑇 = 40𝜇𝑠
Step-Up Converter (Boost Converter)
• A boost converter (step-up converter) is a DC-to-DC power
converter with an output voltage greater than its input
voltage.
Step-Up Converter (Boost Converter)
• 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.
𝑣𝐿 = 𝑉𝑑
𝑑𝑖𝐿
𝑑𝑡
=
𝑉𝑑
𝐿
Step-Up Converter (Boost Converter)
• When switch is opened, the output receives energy from
the input as well as from the inductor.
• Hence output is large.
𝑣𝐿 = 𝑉𝑑 − 𝑉
𝑜
𝑑𝑖𝐿
𝑑𝑡
=
𝑉𝑑 − 𝑉
𝑜
𝐿
Step-Up Converter (Boost Converter)
𝑣𝐿 = 𝑉𝑑 − 𝑉
𝑜
𝑑𝑖𝐿
𝑑𝑡
=
𝑉𝑑 − 𝑉
𝑜
𝐿
𝑣𝐿 = 𝑉𝑑
𝑑𝑖𝐿
𝑑𝑡
=
𝑉𝑑
𝐿
S Closed
S Open
Step-Up Converter (Boost Converter)
𝑣𝐿 =
0
𝐷𝑇
𝑉𝑑 𝑑𝑡 +
𝐷𝑇
𝑇
𝑉𝑑 − 𝑉0
0 = 𝑉𝑑 𝑡 0
𝐷𝑇
+ (𝑉𝑑−𝑉
𝑜) 𝑡 𝐷𝑇
𝑇
0 = 𝐷𝑇𝑉𝑑 + (𝑉𝑑−𝑉
𝑜)[𝑇 − 𝐷𝑇]
0 = 𝑇𝑉𝑑 − 𝑇𝑉
𝑜 + 𝐷𝑇𝑉
𝑜
𝑉
𝑜 =
𝑉𝑑
1 − 𝐷
Step-Up Converter (Boost Converter)
• Boost Converter Design
• Minimum inductor value
• Capacitor Value
𝐿𝑚𝑖𝑛 =
𝐷(1 − 𝐷)2𝑅
2𝑓
𝑟 =
𝐷
𝑅𝐶𝑓
Example-4
• The boost converter has the following
parameters: Vd=20V, D=0.6, R=12.5ohm, L=65uH,
C=200uF, fs=40KHz. Determine (a) output
voltage, (b) output voltage ripple.
50
𝑟 =
𝐷
𝑅𝐶𝑓
𝑉
𝑜 =
𝑉𝑑
1 − 𝐷
Solution
(a) output voltage
𝑉
𝑜 =
20
1 − 0.6
= 50𝑉
(b) output voltage ripple
𝑟 =
0.6
12.5 × 200𝜇 × 40𝐾
𝑟 = 0.6%
Example-5
• Design a boost converter to provide an output voltage of
36V from a 24V source. The load is 50W. The voltage
ripple factor must be less than 0.5%. Specify the duty cycle
ratio, switching frequency, inductor and capacitor size, and
power device.
51
Solution
• Then calculate the switching duty ratio
• First of all determine the switching frequency.
𝑓 = 30𝐾𝐻𝑧
36 =
24
1 − 𝐷
⇒ 36(1 − 𝐷) = 24 ⇒ 𝐷 = 0.33
𝑉
𝑜 =
𝑉𝑑
1 − 𝐷
Example-5
52
• Inductance must be greeter than or equal to Lmin
• Calculate the load resistance
𝑃𝑜 =
𝑉2
𝑅
𝑅 =
362
50
= 25.92Ω
• Calculate inductor value to ensure continuous current
𝐿𝑚𝑖𝑛 =
0.33(1 − 0.33)2× 25.92
2 × 30𝐾
= 63.9𝜇𝐻
𝐿𝑚𝑖𝑛 =
𝐷(1 − 𝐷)2𝑅
2𝑓
𝐿 ≥ 𝐿𝑚𝑖𝑛 = 63.9𝜇𝐻
𝐿 = 100𝜇𝐻
Example-5
53
• Then calculate the Capacitor Value for ripple factor less than 0.5%
𝑟 =
𝐷
𝑅𝐶𝑓
0.005 =
0.33
25.92 × 𝐶 × 30𝐾
𝐶 =
0.33
25.92 × 0.005 × 30𝐾
= 84.8𝜇𝐹
• While selecting the power device we must take into account the switching frequency
𝑓 = 30𝐾𝐻𝑧
𝑇 =
1
𝑓
=
1
30𝐾
= 33.3𝜇𝑠
Example-5
54
• Selection of Power semiconductor switch
𝑓 = 30𝐾𝐻𝑧 𝑇 = 33.3𝜇𝑠
Buck-Boost Converter
• The buck–boost converter is a type of DC-to-DC
converter that has an output voltage magnitude that is
either greater than or less than the input voltage
magnitude.
– If D>0.5, output is higher
– If D<0.5, output is lower
• Output voltage is always negative
Buck-Boost Converter
• while in the On-state, the input voltage source is
directly connected to the inductor (L). This results in
accumulating energy in L. In this stage, the capacitor
supplies energy to the output load.
Buck-Boost Converter
• In Off-state, the inductor is connected to the output
load and capacitor, so energy is transferred from L to C
and R.
Buck-Boost Converter
• In ON-state (Switch Closed)
𝑣𝐿 = 𝑉𝑑 = 𝐿
𝑑𝑖𝐿
𝑑𝑡
⇒
𝑑𝑖𝐿
𝑑𝑡
=
𝑉𝑑
𝐿
Buck-Boost Converter
• In OFF-state (Switch Opened)
𝑣𝐿 = 𝑉
𝑜 = 𝐿
𝑑𝑖𝐿
𝑑𝑡
⇒
𝑑𝑖𝐿
𝑑𝑡
=
𝑉
𝑜
𝐿
Buck-Boost Converter
𝑉𝑑𝐷𝑇
𝐿
+
𝑉
𝑜 1 − 𝐷 𝑇
𝐿
= 0
• Steady state operation
𝑉
𝑜 = −𝑉𝑑
𝐷
1 − 𝐷
Buck-Boost Converter
𝑟 =
𝐷
𝑅𝐶𝑓
𝐿𝑚𝑖𝑛 =
(1 − 𝐷)2𝑅
2𝑓
Example-6
• Determine the switching duty ratio of a buck-boost converter
such that the output voltage is -28V when the input is 100V. The
load is 1Ohm. Design the converter such that it will be in
continuous current mode. The output voltage ripple must not be
more than 0.5%. Specify the frequency and the values of each
component. Suggest the power switch also.
62
Solution:
• Then calculate the switching duty ratio
• First of all determine the switching frequency.
𝑓 = 50 𝐾𝐻𝑧
𝑉
𝑜 = −𝑉𝑑
𝐷
1 − 𝐷
⇒
𝑉
𝑜
−𝑉𝑑
=
𝐷
1 − 𝐷
⇒ 0.28 =
𝐷
1 − 𝐷
⇒ 𝐷 =
0.28
1.28
= 0.2
Example-6
63
• Then calculate the Capacitor Value for ripple factor less than 0.5%
𝑟 =
𝐷
𝑅𝐶𝑓
0.005 =
0.2
10 × 𝐶 × 50𝐾
𝐶 =
0.2
10 × 0.005 × 50𝐾
= 80𝜇𝐹
• Value of inductor can be calculated as
𝐿𝑚𝑖𝑛 =
(1 − 𝐷)2𝑅
2𝑓
𝐿 > 𝐿𝑚𝑖𝑛 =
(1 − 0.2)2× 10
2 × 50𝐾
𝐿 >
6.4
100𝐾
𝐿 > 64𝜇𝐻
Example-6
64
• While selecting the power device we must take into account the switching frequency
𝑓 = 50𝐾𝐻𝑧 𝑇 =
1
𝑓
=
1
50𝐾
= 20𝜇𝑠
Switch mode vs Linear Power Supplies
• One of the major applications of switch mode dc-dc
converters is in switch mode power supplies (SMPs).
• SMPs offer several advantages over linear mode
power supplies.
– Efficient (70-95%)
– Weight and size reduction
• They also have some disadvantages
– Complex design
– EMI problems
65
Linear Mode Power Supply
66
Switch Mode Power Supply
67
END OF LECTURE-10
To download this lecture visit
http://imtiazhussainkalwar.weebly.com/
68

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lecture 10 - electrical machines - dc to dc converters 1.pptx

  • 1. Power Electronics Dr. Imtiaz Hussain Assistant Professor email: imtiaz.hussain@faculty.muet.edu.pk URL :http://imtiazhussainkalwar.weebly.com/ Lecture-10 D.C to D.C Converters (Choppers) 1
  • 2. Power Electronic Interface • Power Electronics is an enabling technology providing the needed interface between the electrical source and electrical load. • The source and load often do differ in frequency, voltage amplitudes and number of phases. 2
  • 3. Powering the information Technology • Figure shows the distributed architecture typically used in computers. • In which incoming voltage from the utility is converted into dc voltage (24V). • This semi regulated voltage is distributed within the computer where on-board power supplies convert this 24V into tightly regulated lower voltage. 3 • Most of the consumer electronics equipment supplied from the mains, internally needed very load dc voltages.
  • 4. Powering the information Technology • However, the electronic circuitry requires higher voltages. • Thus necessitating a circuit to boost input dc to higher dc voltages 4 • Many devices such as cell phones operates from low battery voltages.
  • 5. Introduction to D.C to D.C Converters (Choppers) • DC to DC converters are important in portable electronic devices such as cellular phones and laptop computers, which are supplied with power from batteries primarily. • Such electronic devices often contain several sub-circuits, each with its own voltage level requirement different from that supplied by the battery or an external supply. • They are also widely used in dc-motor drive applications. • Often input to these converters is an unregulated dc voltage, which is obtained by rectifying the line voltage.
  • 6. Introduction Uncontrolled Diode Rectifier Load D.C to D.C Converter Battery Filter AC Line Voltage 1-Phase or 3-Phase DC Unregulated DC Unregulated DC Unregulated DC Regulated vc D.C to D.C Converter System
  • 7. Efficiency & Power Losses • High efficiency is essential in any power processing application. in out P P   • The efficiency of a converter is ) 1 1 (      out out in loss P P P P • The power lost in converter is
  • 8. Efficiency & Power Losses • Efficiency is a good measure of the success of a given converter technology. • With very small amount of power lost, the converter elements can be packaged with high density, leading to a converter of small size and weight, and of low temperature rise. • How can we build a circuit that changes the voltage, yet dissipates negligible power?
  • 9. Efficiency & Power Losses • The various conventional circuit elements are illustrated in Following figure. • The available circuit elements fall broadly into the classes of resistive elements, capacitive elements, magnetic devices including inductors and transformers, semiconductor devices operated in the linear mode and semiconductor devices operated in the switched mode.
  • 10. Types of dc-dc Converters • Types of D.C to D.C converters – AC Link Choppers – Linear Converters – Switch Mode – Magnetic – E.t.c
  • 11. AC Link Choppers • First dc is converted to ac with the help of an inverter. • After that, AC is stepped-up or stepped-down by a transformer, which is then converted back to dc by a diode rectifier. • Ac link chopper is costly, bulky and less efficient as the conversion is done in two stages.
  • 12. Simple dc-dc Converters • Let us now construct a simple dc-dc converter. The input voltage vg is 100 V. It is desired to supply 50 V to an effective 5Ω load, such that the dc load current is 10 A.
  • 13. Resistive dc-dc Converters • Using Voltage divided rule.
  • 14. Linear dc-dc Converters • Linear Mode dc-dc converter
  • 15. Switch Mode dc-dc Converters
  • 16. Conclusion • Capacitors and magnetic devices are important elements of switching converters, because ideally they do not consume power. • It is the resistive element, as well as the linear-mode semiconductor device, that is avoided. • Semiconductor in switch mode however dissipate comparatively low power in either states (ON and OFF). • So capacitive and inductive elements, as well as switched- mode semiconductor devices, are available for synthesis of high-efficiency converters.
  • 17. Switch Mode D.C to D.C Converters • Switch-mode DC to DC converters convert one DC voltage level to another, by storing the input energy temporarily and then releasing that energy to the output at a different voltage. • This conversion method is more power efficient (often 75% to 98%) than linear voltage regulation (which dissipates unwanted power as heat). • This efficiency is beneficial to increasing the running time of battery operated devices.
  • 18. Switch Mode D.C to D.C Converters • PWM or PFM regulates the output dc voltage. • The power flow through these converters is only in one direction thus their voltages and currents remain unipolar.
  • 19. Switch Mode D.C to D.C Converters • A Chopper is a high speed on/off semiconductor switch. • It connects source to load and disconnects source from load at very high speed. • In this manner a chopped dc voltage is obtained from a constant dc supply Vs is obtained.
  • 20. Switch Mode D.C to D.C Converters • During the period Ton, the chopper is on and load voltage Vo is equal to source voltage Vs. • During the period Toff, the chopper is off and load current io flows through the freewheeling diode.
  • 21. Switch Mode D.C to D.C Converters • The load voltage is given by • Thus the load voltage can be varied by varying the switching duty ratio D. 𝑉 𝑜 = 𝑇𝑜𝑛 𝑇𝑜𝑛 + 𝑇𝑜𝑓𝑓 𝑉 𝑠 𝑉 𝑜 = 𝑇𝑜𝑛 𝑇 𝑉 𝑠 𝑉 𝑜 = 𝐷𝑉 𝑠 𝑤ℎ𝑒𝑟𝑒, 𝐷 = 𝑇𝑜𝑛 𝑇 𝑖𝑠 𝑐𝑎𝑙𝑙𝑒𝑑 𝑠𝑤𝑖𝑡𝑐ℎ𝑖𝑛𝑔 𝑑𝑢𝑡𝑦 𝑟𝑎𝑡𝑖𝑜 𝑉 𝑜 = 𝑓𝑇𝑜𝑛𝑉 𝑠
  • 22. Control of D.C to D.C Converters • Average value of output voltage Vo can be controlled by opening and closing the semiconductor switch periodically. • The control strategies for varying duty ratio D are 1. Constant frequency system 2. Variable frequency system 22
  • 23. Constant frequency system • In this scheme Ton is varied but frequency is kept constant. • Variation of Ton means adjustment of pulse width. Therefore, this scheme is called PWM scheme. 𝑇𝑜𝑛 = 1 4 𝑇 𝑇𝑜𝑛 = 3 4 𝑇 𝑉 𝑜 = 1 4 𝑉 𝑠 𝑉 𝑜 = 3 4 𝑉 𝑠
  • 24. Constant frequency system (PWM) st control s on V V T t D   amplifier + - Comparator Vo (desired) Vo (actual) Sawtooth Wave Switch Control Signal Vcontrol vcontrol t Ts vst Ton Toff Switch Control Signal
  • 25. Variable frequency system • In this scheme Ton is kept constant but the frequency is varied.
  • 26. Variable frequency system • Or Toff is kept constant but the frequency is varied.
  • 27. Switch Mode D.C to D.C Converters • Types of Switch Mode D.C to D.C Converters – Step-Down (Buck) converter – Step-up (Boost) converter – Step Down/Up (Buck-Boost) converter
  • 28. Step-Down Converter (Buck Converter) • As name implies a step-down converter produces a lower average output voltage than the dc input voltage Vd. • Its main application is in regulated dc power supplies and dc-motor speed control.
  • 29. Step-Down Converter (Buck Converter) • Circuit operation when S is ON (closed) – Diode is reversed biased. Switch conducts inductor current 𝑖𝐿. – This results in positive inductor voltage, i.e: – It causes linear increase in inductor current 𝑣𝐿 = 𝑉𝑑 − 𝑉 𝑜 𝑖𝐿 = 1 𝐿 𝑣𝐿 𝑑𝑡
  • 30. Step-Down Converter (Buck Converter) • Circuit operation when S is OFF (open) – Because of inductive energy storage, 𝑖𝐿 continues to flow. – Diode is reversed biased. Therefore current flows through the diode. 𝑣𝐿 = −𝑉 𝑜
  • 31. Step-Down Converter (Buck Converter) dt t v T V s T o s o   0 ) ( 1 dt dt t V T V off on on t t t d s o     0 ) ( 1 0 d s on o V T t V  d o DV V 
  • 32. • Continuous conduction mode – A buck converter operates in continuous mode if the current through the inductor (IL) never falls to zero during the commutation cycle. Step-Down Converter (Buck Converter)
  • 33. • Calculate D to obtain required output voltage. • Select a particular switching frequency: – –preferably >20KHz for negligible acoustic noise • Higher fs results in smaller L, but higher device losses. – Thus lowering efficiency and larger heat sink. Design procedure for Buck Converter
  • 34. • Inductor requirement • C Calculation • Possible switching devices: MOSFET, IGBT and BJT. Low power MOSFET can reach MHz range. Design procedure for Buck Converter 𝑟 = 1 − 𝐷 8𝐿𝐶𝑓2 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 𝐷 2𝑓 𝑅
  • 35. Example-1 • A buck converter is supplied from a 50V battery source. Given L=400uH, C=100uF, R=20 Ohm, f=20KHz and D=0.4. Calculate: (a) output voltage (b) output voltage ripple. 35 Solution (a) output voltage 𝑉 𝑜 = 𝐷𝑉 𝑠 𝑉 𝑜 = 0.4 × 50 𝑉 𝑜 = 20𝑉
  • 36. Example-1 36 (b) Output Ripple 𝑟 = 1 − 𝐷 8𝐿𝐶𝑓2 𝑟 = 1 − 0.4 8 × 400𝜇 × 100𝜇 × (20𝐾)2 𝑟 = 4.6%
  • 37. Example-2 • A buck converter has an input voltage of 50V and output of 25V. The switching frequency is 10KHz. The power output is 125W. (a) Determine the duty ratio, (b) value of L to ensure continuous current, (c) value of capacitance to limit the output voltage ripple factor to 0.5%. 37 Solution (a) output voltage 𝑉 𝑜 = 𝐷𝑉 𝑠 (b) Value of L 𝐷 = 𝑉 𝑜 𝑉 𝑠 𝐷 = 25 50 = 0.5 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 𝐷 2𝑓 𝑅 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 0.5 2 × 10𝐾 𝑅 𝑃𝑜 = 𝑉2 𝑅
  • 38. Example-2 • Resistance is calculated as • L must at least be 10 times greater than Lmin. 38 𝑅 = 𝑉2 𝑃𝑜 = 252 125 = 5Ω 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 0.5 2 × 10𝐾 × 5 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 2.5 20𝐾 = 125𝜇𝐻 𝐿 = 1.25𝑚𝐻
  • 39. Example-2 • Value of capacitance to limit the output voltage ripple factor to 0.5% can be calculated using following equation. 39 (c) Value of C 𝑟 = 1 − 𝐷 8𝐿𝐶𝑓2 0.005 = 1 − 0.5 8 × 1.25𝑚 × 𝐶 × (10𝐾)2 𝐶 = 1 − 0.5 8 × 1.25𝑚 × 0.005 × (10𝐾)2 𝐶 = 0.5 5000 = 100𝜇𝐹
  • 40. Example-3 • Design a buck converter such that the output voltage is 28V when the input is 48V. The load is 8Ohm. Design the converter such that it will be in continuous current mode. The output voltage ripple must not be more than 0.5%. Specify the frequency and the values of each component. Suggest the power switch also. 40 Solution: 𝑉 𝑜 = 𝐷𝑉 𝑠 𝐷 = 28 48 = 0.58 • Then calculate the switching duty ratio • First of all determine the switching frequency. 𝑓 = 25𝐾𝐻𝑧
  • 41. Example-3 41 • Now value of inductor can be chosen to ensure continuous conduction 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 𝐷 2𝑓 𝑅 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 1 − 0.58 2 × 25𝐾 × 80 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 0.67𝑚𝐻 𝐿 = 6.7𝑚𝐻
  • 42. Example-3 42 • Value of capacitance to limit the output voltage ripple factor to 0.5% can be calculated using following equation. 𝑟 = 1 − 𝐷 8𝐿𝐶𝑓2 𝐶 = 1 − 0.58 8 × 6.7𝑚 × 0.005 × (25𝐾)2 𝐶 = 0.42 167500 = 2.5𝜇𝐹
  • 43. Example-3 43 • Selection of Power semiconductor switch 𝑓 = 25𝐾𝐻𝑧 𝑇 = 40𝜇𝑠
  • 44. Step-Up Converter (Boost Converter) • A boost converter (step-up converter) is a DC-to-DC power converter with an output voltage greater than its input voltage.
  • 45. Step-Up Converter (Boost Converter) • 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. 𝑣𝐿 = 𝑉𝑑 𝑑𝑖𝐿 𝑑𝑡 = 𝑉𝑑 𝐿
  • 46. Step-Up Converter (Boost Converter) • When switch is opened, the output receives energy from the input as well as from the inductor. • Hence output is large. 𝑣𝐿 = 𝑉𝑑 − 𝑉 𝑜 𝑑𝑖𝐿 𝑑𝑡 = 𝑉𝑑 − 𝑉 𝑜 𝐿
  • 47. Step-Up Converter (Boost Converter) 𝑣𝐿 = 𝑉𝑑 − 𝑉 𝑜 𝑑𝑖𝐿 𝑑𝑡 = 𝑉𝑑 − 𝑉 𝑜 𝐿 𝑣𝐿 = 𝑉𝑑 𝑑𝑖𝐿 𝑑𝑡 = 𝑉𝑑 𝐿 S Closed S Open
  • 48. Step-Up Converter (Boost Converter) 𝑣𝐿 = 0 𝐷𝑇 𝑉𝑑 𝑑𝑡 + 𝐷𝑇 𝑇 𝑉𝑑 − 𝑉0 0 = 𝑉𝑑 𝑡 0 𝐷𝑇 + (𝑉𝑑−𝑉 𝑜) 𝑡 𝐷𝑇 𝑇 0 = 𝐷𝑇𝑉𝑑 + (𝑉𝑑−𝑉 𝑜)[𝑇 − 𝐷𝑇] 0 = 𝑇𝑉𝑑 − 𝑇𝑉 𝑜 + 𝐷𝑇𝑉 𝑜 𝑉 𝑜 = 𝑉𝑑 1 − 𝐷
  • 49. Step-Up Converter (Boost Converter) • Boost Converter Design • Minimum inductor value • Capacitor Value 𝐿𝑚𝑖𝑛 = 𝐷(1 − 𝐷)2𝑅 2𝑓 𝑟 = 𝐷 𝑅𝐶𝑓
  • 50. Example-4 • The boost converter has the following parameters: Vd=20V, D=0.6, R=12.5ohm, L=65uH, C=200uF, fs=40KHz. Determine (a) output voltage, (b) output voltage ripple. 50 𝑟 = 𝐷 𝑅𝐶𝑓 𝑉 𝑜 = 𝑉𝑑 1 − 𝐷 Solution (a) output voltage 𝑉 𝑜 = 20 1 − 0.6 = 50𝑉 (b) output voltage ripple 𝑟 = 0.6 12.5 × 200𝜇 × 40𝐾 𝑟 = 0.6%
  • 51. Example-5 • Design a boost converter to provide an output voltage of 36V from a 24V source. The load is 50W. The voltage ripple factor must be less than 0.5%. Specify the duty cycle ratio, switching frequency, inductor and capacitor size, and power device. 51 Solution • Then calculate the switching duty ratio • First of all determine the switching frequency. 𝑓 = 30𝐾𝐻𝑧 36 = 24 1 − 𝐷 ⇒ 36(1 − 𝐷) = 24 ⇒ 𝐷 = 0.33 𝑉 𝑜 = 𝑉𝑑 1 − 𝐷
  • 52. Example-5 52 • Inductance must be greeter than or equal to Lmin • Calculate the load resistance 𝑃𝑜 = 𝑉2 𝑅 𝑅 = 362 50 = 25.92Ω • Calculate inductor value to ensure continuous current 𝐿𝑚𝑖𝑛 = 0.33(1 − 0.33)2× 25.92 2 × 30𝐾 = 63.9𝜇𝐻 𝐿𝑚𝑖𝑛 = 𝐷(1 − 𝐷)2𝑅 2𝑓 𝐿 ≥ 𝐿𝑚𝑖𝑛 = 63.9𝜇𝐻 𝐿 = 100𝜇𝐻
  • 53. Example-5 53 • Then calculate the Capacitor Value for ripple factor less than 0.5% 𝑟 = 𝐷 𝑅𝐶𝑓 0.005 = 0.33 25.92 × 𝐶 × 30𝐾 𝐶 = 0.33 25.92 × 0.005 × 30𝐾 = 84.8𝜇𝐹 • While selecting the power device we must take into account the switching frequency 𝑓 = 30𝐾𝐻𝑧 𝑇 = 1 𝑓 = 1 30𝐾 = 33.3𝜇𝑠
  • 54. Example-5 54 • Selection of Power semiconductor switch 𝑓 = 30𝐾𝐻𝑧 𝑇 = 33.3𝜇𝑠
  • 55. Buck-Boost Converter • The buck–boost converter is a type of DC-to-DC converter that has an output voltage magnitude that is either greater than or less than the input voltage magnitude. – If D>0.5, output is higher – If D<0.5, output is lower • Output voltage is always negative
  • 56. Buck-Boost Converter • while in the On-state, the input voltage source is directly connected to the inductor (L). This results in accumulating energy in L. In this stage, the capacitor supplies energy to the output load.
  • 57. Buck-Boost Converter • In Off-state, the inductor is connected to the output load and capacitor, so energy is transferred from L to C and R.
  • 58. Buck-Boost Converter • In ON-state (Switch Closed) 𝑣𝐿 = 𝑉𝑑 = 𝐿 𝑑𝑖𝐿 𝑑𝑡 ⇒ 𝑑𝑖𝐿 𝑑𝑡 = 𝑉𝑑 𝐿
  • 59. Buck-Boost Converter • In OFF-state (Switch Opened) 𝑣𝐿 = 𝑉 𝑜 = 𝐿 𝑑𝑖𝐿 𝑑𝑡 ⇒ 𝑑𝑖𝐿 𝑑𝑡 = 𝑉 𝑜 𝐿
  • 60. Buck-Boost Converter 𝑉𝑑𝐷𝑇 𝐿 + 𝑉 𝑜 1 − 𝐷 𝑇 𝐿 = 0 • Steady state operation 𝑉 𝑜 = −𝑉𝑑 𝐷 1 − 𝐷
  • 62. Example-6 • Determine the switching duty ratio of a buck-boost converter such that the output voltage is -28V when the input is 100V. The load is 1Ohm. Design the converter such that it will be in continuous current mode. The output voltage ripple must not be more than 0.5%. Specify the frequency and the values of each component. Suggest the power switch also. 62 Solution: • Then calculate the switching duty ratio • First of all determine the switching frequency. 𝑓 = 50 𝐾𝐻𝑧 𝑉 𝑜 = −𝑉𝑑 𝐷 1 − 𝐷 ⇒ 𝑉 𝑜 −𝑉𝑑 = 𝐷 1 − 𝐷 ⇒ 0.28 = 𝐷 1 − 𝐷 ⇒ 𝐷 = 0.28 1.28 = 0.2
  • 63. Example-6 63 • Then calculate the Capacitor Value for ripple factor less than 0.5% 𝑟 = 𝐷 𝑅𝐶𝑓 0.005 = 0.2 10 × 𝐶 × 50𝐾 𝐶 = 0.2 10 × 0.005 × 50𝐾 = 80𝜇𝐹 • Value of inductor can be calculated as 𝐿𝑚𝑖𝑛 = (1 − 𝐷)2𝑅 2𝑓 𝐿 > 𝐿𝑚𝑖𝑛 = (1 − 0.2)2× 10 2 × 50𝐾 𝐿 > 6.4 100𝐾 𝐿 > 64𝜇𝐻
  • 64. Example-6 64 • While selecting the power device we must take into account the switching frequency 𝑓 = 50𝐾𝐻𝑧 𝑇 = 1 𝑓 = 1 50𝐾 = 20𝜇𝑠
  • 65. Switch mode vs Linear Power Supplies • One of the major applications of switch mode dc-dc converters is in switch mode power supplies (SMPs). • SMPs offer several advantages over linear mode power supplies. – Efficient (70-95%) – Weight and size reduction • They also have some disadvantages – Complex design – EMI problems 65
  • 66. Linear Mode Power Supply 66
  • 67. Switch Mode Power Supply 67
  • 68. END OF LECTURE-10 To download this lecture visit http://imtiazhussainkalwar.weebly.com/ 68