1
Introduction
1.1
INTRODUCTION TO POWER PROCESSING
The  field  of  power  electronics  is  concerned  with  the  processing  of  electrical  power  using  electronic
devices [1–7]. The key element is the switching converter, illustrated in Fig.  1.1. In general, a switching
converter contains power input and control input ports, and a power output port. The raw input power is
processed as specified by the control  input, yielding the conditioned output power. One of several basic
functions  can  be performed  [2].  In  a dc–dc converter,  the dc  input  voltage  is  converted to  a dc  output
voltage  having  a  larger  or  smaller  magnitude,  possibly  with  opposite  polarity  or  with  isolation  of  the
input and output ground references. In an ac–dc rectifier, an ac input voltage is rectified, producing a dc
output voltage. The dc output voltage and/or ac input current waveform may be controlled. The inverse
process, dc–ac inversion, involves transforming a dc input voltage into an ac output voltage of controlla-
ble magnitude and frequency. Ac–ac cycloconversion involves converting an ac input voltage to a given
ac output voltage of controllable magnitude and frequency.
Control  is  invariably  required.  It  is  nearly  always  desired  to produce  a  well-regulated output
2
Introduction
voltage, in the presence of variations in the input voltage and load current. As  illustrated in  Fig.  1.2, a
controller block is an integral part of any power processing system.
High efficiency is essential in any power processing application. The primary reason for this is
usually not the desire to save money on one’s electric bills, nor to conserve energy, in spite of the nobility
of such pursuits. Rather, high efficiency converters are necessary because construction of low-efficiency
converters, producing substantial output power, is impractical. The efficiency of a converter having out-
put  power 
and input power 
is
The power lost in the converter is
Equation (1.2) is plotted in Fig. 1.3. In a con-
verter that  has  an  efficiency  of 50%, power
is  dissipated  by  the  converter elements
and  this  is  equal  to  the  output  power,
This  power  is  converted  into  heat,  which
must  be  removed from  the  converter.  If  the
output  power  is  substantial,  then  so  is  the
loss  power.  This  leads  to  a  large  and  expen-
sive  cooling  system,  it  causes  the  electronic
elements  within  the  converter  to  operate  at
high  temperature,  and  it  reduces  the  system
reliability.  Indeed, at high output powers,  it
may  be  impossible  to  adequately  cool  the
converter elements using current technology.
Increasing the efficiency  is the key
to obtaining higher output powers. For exam-
ple,  if the  converter efficiency  is  90%,  then
the converter loss power is equal to only  11%
1.1
Introduction to Power Processing
3
of the output power. Efficiency is a good measure of the success of a given converter technology.  Figure
1.4  illustrates  a  converter  that  processes  a  large  amount  of  power,  with  very  high  efficiency.  Since  very
little power is 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? The vari-
ous conventional  circuit elements  are  illustrated  in  Fig. 1.5. 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  (for  example,  as  class  A  or  class  B
amplifiers),  and  semiconductor devices  operated  in  the  switched  mode (such  as  in  logic devices where
transistors operate in either saturation or cutoff).  In conventional  signal  processing applications,  where
efficiency is  not the primary concern,  magnetic devices are usually avoided wherever possible, because
of their large size and the difficulty of incorporating them into integrated circuits. In contrast, capacitors
and  magnetic  devices  are  important elements  of switching  converters,  because  ideally  they  do  not con-
sume power. It is the resistive element, as well as the linear-mode semiconductor device, that is avoided
[2].  Switched-mode semiconductor devices  are also employed.  When  a semiconductor device operates  in
the off state, its current is zero and hence its power dissipation is zero. When the semiconductor device
operates in the on (saturated) state,  its voltage drop is small and hence its power dissipation is also small.
In either event, the power dissipated by the semiconductor device is low. So capacitive and inductive ele-
ments, as well as switched-mode semiconductor devices, are available for synthesis of high-efficiency
converters.
Let us now consider how to construct the simple dc-dc converter example illustrated in Fig. 1.6.
load,  such  that the dc  load
is  100 V. It is desired to supply 50 V to an effective 
The input voltage 
current is  10 A.
Introductory  circuits  textbooks  describe  a  low-efficiency method  to  perform  the  required func-
tion:  the  voltage divider circuit illustrated  in  Fig.  1.7(a). The dc–dc converter then consists simply of a
4
Introduction
variable resistor, whose value is adjusted such that the required output voltage is obtained. The load cur-
rent flows through the variable resistor. For the specified voltage and current levels, the  power 
dissi-
supplies  power
pated  in  the  variable  resistor  equals  the  load  power 
W.  Figure  1.7(b)  illustrates  a  more practical  implementation  known  as  the  linear  series-pass
regulator.  The  variable  resistor  of Fig.  1.7(a)  is  replaced  by  a  linear-mode  power transistor,  whose  base
current  is  controlled  by  a  feedback  system  such  that  the  desired  output  voltage  is  obtained.  The  power
dissipated by the linear-mode transistor of Fig.  1.7(b)  is approximately the same as the 500 W  lost by the
variable  resistor  in  Fig.  1.7(a).  Series-pass linear  regulators  generally  find  modern  application  only  at
low  power levels  of a few  watts.
W.  The  source 
Figure  1.8 illustrates another approach. A single-pole double-throw  (SPDT)  switch is connected
as shown. The switch output voltage 
is equal to the converter input voltage  when the switch is in
position  1,  and  is  equal  to zero when  the switch  is  in  position  2. The switch position  is  varied  periodi-
cally, as illustrated in Fig.  1.9, such that 
and  period
The  duty  cycle  D  is  defined  as  the  fraction  of time  in  which  the  switch  occupies  position  1.
In  practice,  the  SPDT  switch  is  realized  using switched-mode semiconductor devices,
is a rectangular waveform having frequency 
Hence, 
1.1 Introduction to Power Processing
5
which are controlled such that the  SPDT  switching  function  is attained.
The switch changes  the dc component of the voltage.  Recall  from  Fourier analysis that the dc
component of a periodic waveform is equal to its average value. Hence, the dc component of 
is
Thus,  the  switch  changes the dc  voltage,  by  a  factor equal  to the duty cycle  D.  To convert the  input volt-
age 
into the desired output voltage of V = 50 V, a duty cycle of D = 0.5 is required.
Again, the power dissipated by the switch is ideally zero. When the switch contacts are closed,
then  their  voltage  is  zero  and  hence  the  power dissipation  is  zero.  When  the  switch  contacts  are  open,
then the current is zero and again the power dissipation is zero. So we have succeeded in changing the dc
voltage component, using a device that is ideally lossless.
In addition to the desired dc component 
the switch output voltage waveform 
also  con-
tains  undesirable harmonics of the switching  frequency.  In  most applications,  these harmonics  must be
removed, such that the output voltage 
A low-pass fil-
ter can be employed for this purpose. Figure  1.10 illustrates the introduction of a single-section L–C low-
pass  filter.  If the  filter  corner  frequency 
then the  fil-
To the extent that the switch, inductor, and capacitor
ter essentially passes only the dc component of 
elements are ideal, the efficiency of this dc–dc converter can approach  100%.
is sufficiently less than the switching  frequency 
is essentially equal to the dc component 
In Fig.  1.11, a control system is introduced for regulation of the output voltage. Since the output
voltage is  a function  of the  switch duty  cycle,  a control  system can  be constructed  that varies  the duty
cycle to cause the output voltage to follow a given reference. Figure  1.11  also illustrates a typical way in
which  the  SPDT  switch  is  realized  using  switched-mode  semiconductor  devices.  The  converter  power
stage developed in Figs.  1.8 to 1.11 is called the buck converter, because it reduces the dc voltage.
Converters can be constructed that perform other power processing functions. For example, Fig.
6
Introduction
1.2
Several Applications of Power Electronics
7
1.12  illustrates  a  circuit known  as  the  boost converter,  in  which  the  positions  of the  inductor  and  SPDT
switch are interchanged. This converter is capable of producing output voltages that are greater in magni-
tude than the input voltage. In general, any given input voltage can be converted into any desired output
voltage,  using  a  converter containing  switching  devices  embedded  within  a  network  of reactive  elements.
inverter circuit.  As  illustrated  in  Fig.  1.13(b),  the
to contain a low-
is  selected  to  pass  the  desired  low-
but to attenuate the high-frequency switching harmonics. The controller
switch duty cycle is modulated sinusoidally. This causes the switch output voltage 
frequency sinusoidal component.  The  L–C  filter  cutoff frequency 
frequency  components  of 
modulates the duty cycle such that the desired output frequency and voltage magnitude are obtained.
Figure  1.13(a)  illustrates  a  simple 
1.2
SEVERAL APPLICATIONS OF POWER ELECTRONICS
The power levels encountered in high-efficiency switching converters range from (1) less than one watt,
in dc–dc  converters  within  battery-operated portable equipment,  to  (2)  tens,  hundreds,  or thousands of
watts in power supplies for computers and office equipment, to (3) kilowatts to Megawatts,  in variable-
speed motor drives, to (4) roughly  1000 Megawatts  in the rectifiers and inverters that interface dc trans-
mission lines to the ac utility power system. The converter systems of several applications are illustrated
in this section.
A power supply system for a laptop computer is illustrated in Fig.  1.14. A lithium battery pow-
ers the system, and several dc–dc converters change the battery  voltage into the  voltages required by the
loads.  A  buck converter produces  the  low-voltage dc  required  by  the  microprocessor.  A  boost converter
increases  the  battery  voltage  to  the  level  needed  by  the  disk  drive.  An  inverter  produces high-voltage
high-frequency ac to drive lamps that light the display. A charger with transformer isolation converts the
ac  line  voltage  into  dc  to  charge  the  battery.  The  converter  switching  frequencies  are  typically  in  the
vicinity  of several hundred  kilohertz;  this  leads  to  substantial  reductions  in  the  size  and  weight  of the
reactive  elements.  Power management is  used,  to  control  sleep modes  in  which  power consumption  is
reduced and battery life is extended. In a distributed power system, an intermediate dc voltage appears at
the  computer  backplane.  Each printed circuit card contains  high-density  dc–dc  converters  that  produce
8
Introduction
locally-regulated low voltages. Commercial applications of power electronics include off-line power sys-
tems for computers,  office and  laboratory equipment,  uninterruptable ac power supplies,  and electronic
ballasts for gas discharge lighting.
Figure  1.15  illustrates  a  power  system  of an  earth-orbiting  spacecraft.  A  solar  array  produces
the  main  power  bus  voltage 
to  the  regulated  voltages  required  by
the  spacecraft  payloads.  Battery  charge/discharge  controllers  interface  the  main  power  bus  to  batteries;
these controllers  may  also contain dc–dc converters. Aerospace applications  of power electronics  include
the  power systems  of aircraft,  spacecraft,  and other aerospace vehicles.
DC–DC converters  convert 
Figure  1.16  illustrates  an electric vehicle power and  drive system.  Batteries  are charged by a
converter that draws high power-factor sinusoidal current from a single-phase or three-phase ac line. The
batteries supply power to variable-speed ac  motors to propel  the  vehicle. The speeds of the ac  motors are
controlled by variation of the electrical input frequency. Inverters produce three-phase ac output voltages
of variable  frequency  and  variable  magnitude,  to control  the  speed  of the  ac  motors  and  the  vehicle. A
dc–dc converter steps down  the  battery  voltage  to  the  lower dc  levels  required  by  the  electronics  of the
system.  Applications  of  motor drives  include  speed  control  of  industrial  processes,  such  as  control  of
compressors,  fans,  and pumps;  transportation applications such  as electric  vehicles,  subways,  and loco-
motives; and motion control applications in areas such as computer peripherals and industrial robots.
Power electronics also finds application in other diverse industries, including dc power supplies,