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16 Chapter 1
Voice Frequencies. Voice frequencies (VFs) are in the range of 300 to 3000 Hz. This
is the normal range of human speech. Although human hearing extends from approxi-
mately 20 to 20,000 Hz, most intelligible sound occurs in the VF range.
Very Low Frequencies. Very low frequencies (VLFs) extend from 9 kHz to 30 kHz
and include the higher end of the human hearing range up to about 15 or 20 kHz. Many
musical instruments make sounds in this range as well as in the ELF and VF ranges. The
VLF range is also used in some government and military communication. For example,
VLF radio transmission is used by the navy to communicate with submarines.
Low Frequencies. Low frequencies (LFs) are in the 30- to 300-kHz range. The pri-
mary communication services using this range are in aeronautical and marine navigation.
Frequencies in this range are also used as subcarriers, signals that are modulated by the
baseband information. Usually, two or more subcarriers are added, and the combination
is used to modulate the final high-frequency carrier.
Medium Frequencies. Medium frequencies (MFs) are in the 300- to 3000-kHz
(0.3- to 3.0-MHz) range. The major application of frequencies in this range is AM radio
broadcasting (535 to 1605 kHz). Other applications in this range are various marine and
amateur radio communication.
High Frequencies. High frequencies (HFs) are in the 3- to 30-MHz range. These
are the frequencies generally known as short waves. All kinds of simplex broadcast-
ing and half duplex two-way radio communication take place in this range. Broadcasts
from Voice of America and the British Broadcasting Company occur in this range.
Government and military services use these frequencies for two-way communication.
An example is diplomatic communication between embassies. Amateur radio and CB
communication also occur in this part of the spectrum.
Very High Frequencies. Very high frequencies (VHFs) encompass the 30- to 300-MHz
range. This popular frequency range is used by many services, including mobile radio, marine
and aeronautical communication, FM radio broadcasting (88 to 108 MHz), and television
channels 2 through 13. Radio amateurs also have numerous bands in this frequency range.
Ultrahigh Frequencies. Ultrahigh frequencies (UHFs) encompass the 300- to
3000-MHz range. This, too, is a widely used portion of the frequency spectrum. It
includes the UHF TV channels 14 through 51, and it is used for land mobile commu-
nication and services such as cellular telephones as well as for military communication.
Some radar and navigation services occupy this portion of the frequency spectrum, and
radio amateurs also have bands in this range.
Microwaves and SHFs. Frequencies between the 1000-MHz (1-GHz) and 30-GHz
range are called microwaves. Microwave ovens usually operate at 2.45 GHz. Superhigh
frequencies (SHFs) are in the 3- to 30-GHz range. These microwave frequencies are
widely used for satellite communication and radar. Wireless local-area networks (LANs)
and many cellular telephone systems also occupy this region.
Extremely High Frequencies. Extremely high frequencies (EHFs) extend from 30 to
300 GHz. Electromagnetic signals with frequencies higher than 30 GHz are referred to as
millimeter waves. Equipment used to generate and receive signals in this range is extremely
complex and expensive, but there is growing use of this range for satellite communication
telephony, computer data, short-haul cellular networks, and some specialized radar.
Frequencies Between 300 GHz and the Optical Spectrum. This portion
of the spectrum is virtually uninhabited. It is a cross between RF and optical. Lack of
hardware and components limits its use.
High frequency (HF)
Voice frequency (VF)
Very low frequency (VLF)
Low frequency (LF)
Medium frequency (MF)
Subcarrier
Very high frequency (VHF)
Ultrahigh frequency (UHF)
Microwave
Superhigh frequency (SHF)
Extremely high frequency (EHF)
Millimeter wave
Introduction to Electronic Communication 17
The Optical Spectrum
Right above the millimeter wave region is what is called the optical
spectrum, the region occupied by light waves. There are three different
types of light waves: infrared, visible, and ultraviolet.
Infrared. The infrared region is sandwiched between the highest
radio frequencies (i.e., millimeter waves) and the visible portion of
the electromagnetic spectrum. Infrared occupies the range between
approximately 0.1 millimeter (mm) and 700 nanometers (nm), or
100 to 0.7 micrometer (μm). One micrometer is one-millionth of
a meter. Infrared wavelengths are often given in micrometers or
nanometers.
Infrared radiation is generally associated with heat. Infrared is pro-
duced by light-bulbs, our bodies, and any physical equipment that gen-
erates heat. Infrared signals can also be generated by special types of
light-emitting diodes (LEDs) and lasers.
Infrared signals are used for various special kinds of communi-
cation. For example, infrared is used in astronomy to detect stars and
other physical bodies in the universe, and for guidance in weapons
systems, where the heat radiated from airplanes or missiles can be
picked up by infrared detectors and used to guide missiles to targets.
Infrared is also used in most new TV remote-control units where
special coded signals are transmitted by an infrared LED to the TV
receiver for the purpose of changing channels, setting the volume,
and performing other functions. Infrared is the basis for all iber-
optic communication.
Infrared signals have many of the same properties as signals in the
visible spectrum. Optical devices such as lenses and mirrors are often
used to process and manipulate infrared signals, and infrared light is
the signal usually propagated over iber-optic cables.
The Visible Spectrum. Just above the infrared region is the visible spectrum we
ordinarily refer to as light. Light is a special type of electromagnetic radiation that
has a wavelength in the 0.4- to 0.8-µm range (400 to 800 nm). Light wavelengths are
usually expressed in terms of angstroms (Å). An angstrom is one ten-thousandth of a
micrometer; for example, 1 Å 5 10210
m. The visible range is approximately 8000 Å
(red) to 4000 Å (violet). Red is low-frequency or long-wavelength light, whereas violet
is high-frequency or short-wavelength light.
Light is used for various kinds of communication. Light waves can be modulated
and transmitted through glass ibers, just as electric signals can be transmitted over wires.
The great advantage of light wave signals is that their very high frequency gives them
the ability to handle a tremendous amount of information. That is, the bandwidth of the
baseband signals can be very wide.
Light signals can also be transmitted through free space. Various types of commu-
nication systems have been created using a laser that generates a light beam at a speciic
visible frequency. Lasers generate an extremely narrow beam of light, which is easily
modulated with voice, video, and data information.
Ultraviolet. Ultraviolet light (UV) covers the range from about 4 to 400 nm. Ultravio-
let generated by the sun is what causes sunburn. Ultraviolet is also generated by mercury
vapor lights and some other types of lights such as fluorescent lamps and sun lamps.
Ultraviolet is not used for communication; its primary use is medical.
Beyond the visible region are the X-rays, gamma rays, and cosmic rays. These are
all forms of electromagnetic radiation, but they do not igure into communication systems
and are not covered here.
The tablet computer has become a popular
communications device thanks to Wi-Fi and
cellular links.
Optical spectrum
Infrared region
Visible spectrum
Light
Ultraviolet light (UV)
GOOD TO KNOW
Although it is expensive to build
a fiber-optic or wireless network,
servicing each additional user is
cost-effective. The more users
a network has, the lower the
overall cost.
18 Chapter 1
1-6 Bandwidth
Bandwidth (BW) is that portion of the electromagnetic spectrum occupied by a signal. It
is also the frequency range over which a receiver or other electronic circuit operates.
More speciically, bandwidth is the difference between the upper and lower frequency
limits of the signal or the equipment operation range. Fig. 1-16 shows the bandwidth of
the voice frequency range from 300 to 3000 Hz. The upper frequency is f2 and the lower
frequency is f1. The bandwidth, then, is
BW 5 f2 2 f1
Bandwidth (BW)
Example 1-5
A commonly used frequency range is 902 to 928 MHz. What is the width of this band?
f1 5 902 MHz f2 5 928 MHz
BW 5 f2 2 f1 5 928 2 902 5 26 MHz
Example 1-6
A television signal occupies a 6-MHz bandwidth. If the low-frequency limit of
channel 2 is 54 MHz, what is the upper-frequency limit?
BW 5 54 MHz f1 5 6 MHz
BW 5 f1 2 f2
f2 5 BW 1 f1 5 6 1 54 5 60 MHz
Bandwidth
(BW)
f1 ⫽ 300 Hz f2 ⫽ 3000 Hz
Frequency spectrum
BW ⫽ f2 ⫺ f1
⫽ 3000 ⫺ 300
⫽ 2700 Hz
Figure 1-16 Bandwidth is the frequency range over which equipment operates or
that portion of the spectrum occupied by the signal. This is the voice
frequency bandwidth.
Sideband
Channel Bandwidth
When information is modulated onto a carrier somewhere in the electromagnetic spectrum,
the resulting signal occupies a small portion of the spectrum surrounding the carrier fre-
quency. The modulation process causes other signals, called sidebands, to be generated at
Introduction to Electronic Communication 19
frequencies above and below the carrier frequency by an amount equal to the modulating
frequency. For example, in AM broadcasting, audio signals up to 5 kHz can be transmit-
ted. If the carrier frequency is 1000 kHz, or 1 MHz, and the modulating frequency is
5 kHz, sidebands will be produced at 1000 2 5 5 995 kHz and at 1000 1 5 5 1005 kHz.
In other words, the modulation process generates other signals that take up spectrum space.
It is not just the carrier at 1000 kHz that is transmitted. Thus the term bandwidth refers
to the range of frequencies that contain the information. The term channel bandwidth refers
to the range of frequencies required to transmit the desired information.
The bandwidth of the AM signal described above is the difference between the high-
est and lowest transmitting frequencies: BW 5 1005 kHz 2 995 kHz 5 10 kHz. In this
case, the channel bandwidth is 10 kHz. An AM broadcast signal, therefore, takes up a
10-kHz piece of the spectrum.
Signals transmitting on the same frequency or on overlapping frequencies do, of course,
interfere with one another. Thus a limited number of signals can be transmitted in the fre-
quency spectrum. As communication activities have grown over the years, there has been
a continuous demand for more frequency channels over which communication can be trans-
mitted. This has caused a push for the development of equipment that operates at the higher
frequencies. Prior to World War II, frequencies above 1 GHz were virtually unused, since
there were no electronic components suitable for generating signals at those frequencies.
But technological developments over the years have given us many microwave components
such as klystrons, magnetrons, and traveling-wave tubes, and today transistors, integrated
circuits, and other semiconductor devices that routinely work in the microwave range.
More Room at the Top
The beneit of using the higher frequencies for communication carriers is that a signal of
a given bandwidth represents a smaller percentage of the spectrum at the higher frequen-
cies than at the lower frequencies. For example, at 1000 kHz, the 10-kHz-wide AM
signal discussed earlier represents 1 percent of the spectrum:
% of spectrum 5
10 kHz
1000 KHz
3 100
5 1%
But at 1 GHz, or 1,000,000 kHz, it represents only one-thousandth of 1 percent:
% of spectrum 5
10 kHz
1,000,000 kHz
3 100
5 0.001%
In practice, this means that there are many more 10-kHz channels at the higher
frequencies than at the lower frequencies. In other words, there is more spectrum space
for information signals at the higher frequencies.
The higher frequencies also permit wider-bandwidth signals to be used. A TV signal,
e.g., occupies a bandwidth of 6 MHz. Such a signal cannot be used to modulate a carrier
in the MF or HF ranges because it would use up all the available spectrum space.
Television signals are transmitted in the VHF and UHF portions of the spectrum, where
suficient space is available.
Today, virtually the entire frequency spectrum between approximately 30 kHz and
30 GHz has been spoken for. Some open areas and portions of the spectrum are not
heavily used, but for the most part, the spectrum is illed with communication activities
of all kinds generated from all over the world. There is tremendous competition for
these frequencies, not only between companies, individuals, and government services in
individual carriers but also between the different nations of the world. The electromagnetic
spectrum is one of our most precious natural resources. Because of this, communication
engineering is devoted to making the best use of that inite spectrum. A considerable
amount of effort goes into developing communication techniques that will minimize the
bandwidth required to transmit given information and thus conserve spectrum space.
Channel bandwidth
GOOD TO KNOW
The Federal Communications
Commission (FCC) was formed in
1934 to regulate interstate and
foreign communication. A primary
function of the FCC is to allocate
bands of frequencies and set
limitations on broadcast power for
different types of radio and TV
operations. The FCC also monitors
broadcasts to detect unlicensed
operations and technical violations.
In addition to TV and radio stations,
the FCC licenses about 50 million
transmitters operated by
individuals, businesses, ships and
airplanes, emergency services, and
telephone systems. FCC policy
is set by five commissioners who
are appointed by the President
for five-year terms.
20 Chapter 1
This provides more room for additional communication channels and gives other ser-
vices or users an opportunity to take advantage of it. Many of the techniques discussed
later in this book evolved in an effort to minimize transmission bandwidth.
Spectrum Management
Governments of the United States and other countries recognized early on that the fre-
quency spectrum was a valuable and inite natural resource and so set up agencies to
control spectrum use. In the United States, Congress passed the Communications Act of
1934. This Act and its various amendments established regulations for the use of spec-
trum space. It also established the Federal Communications Commission (FCC), a regu-
latory body whose function is to allocate spectrum space, issue licenses, set standards,
and police the airwaves. The Telecommunications Act of 1996 has also greatly inluenced
the use of spectrum. The FCC controls all telephone and radio communications in this
country and, in general, regulates all electromagnetic emissions. The National Telecom-
munications and Information Administration (NTIA) performs a similar function for
government and military services. Other countries have similar organizations.
The International Telecommunications Union (ITU), an agency of the United
Nations that is headquartered in Geneva, Switzerland, comprises 189 member countries
that meet at regular intervals to promote cooperation and negotiate national interests.
Typical of these meetings are the World Administrative Radio Conferences, held
approximately every two years. Various committees of the ITU set standards for various
areas within the communication ield. The ITU brings together the various countries
to discuss how the frequency spectrum is to be divided up and shared. Because many
of the signals generated in the spectrum do not carry for long distances, countries can
use these frequencies simultaneously without interference. On the other hand, some
ranges of the frequency spectrum can literally carry signals around the world. As a
result, countries must negotiate with one another to coordinate usage of various por-
tions of the high-frequency spectrum to prevent mutual interference.
Standards
Standards are speciications and guidelines that companies and individuals follow to
ensure compatibility between transmitting and receiving equipment in communication
systems. Although the concepts of communication are simple, there are obviously many
ways to send and receive information. A variety of methods are used to modulate, mul-
tiplex, and otherwise process the information to be transmitted. If each system used
different methods created at the whim of the designing engineer, the systems would be
incompatible with one another and no communication could take place. In the real world,
standards are set and followed so that when equipment is designed and built, compatibil-
ity is ensured. The term used to describe the ability of equipment from one manufacturer
to work compatibly with that of another is interoperability.
Standards are detailed outlines of principles of operation, blueprints for construction,
and methods of measurement that deine communication equipment. Some of the specii-
cations covered are modulation methods, frequency of operation, multiplexing methods,
word length and bit formats, data transmission speeds, line coding methods, and cable and
connector types. These standards are set and maintained by numerous nonproit organiza-
tions around the world. Committees made up of individuals from industry and academia
meet to establish and agree upon the standards, which are then published for others to use.
Other committees review, revise, and enhance the standards over time, as needs change.
In working in the communication ield, you will regularly encounter many different stan-
dards. For example, there are standards for long-distance telephone transmission, digital cell
phones, local-area networks, and computer modems. Listed below are organizations that main-
tain standards for communication systems. For more details, go to the corresponding website.
American National Standards Institute (ANSI)—www.ansi.org
Electronic Industries Alliance (EIA)—www.eia.org
National Telecommunications and
Information Administration (NTIA)
International Telecommunications
Union (ITU)
Standards
Interoperability
Introduction to Electronic Communication 21
European Telecommunications Standards Institute (ETSI)—www.etsi.org
Institute of Electrical and Electronics Engineers (IEEE)—www.ieee.org
International Telecommunications Union (ITU)—www.itu.org
Internet Engineering Task Force (IETF)—www.ietf.org
Optical Internetworking Forum (IF)—www.oiforum.com
Telecommunications Institute of America (TIA)—www.tiaonline.org
1-7 A Survey of Communication
Applications
The applications of electronic techniques to communication are so common and pervasive
that you are already familiar with most of them. You use the telephone, listen to the radio,
and watch TV. You also use other forms of electronic communication, such as cellular
telephones, ham radios, CB and Family radios, home wireless networks for Internet access,
texting, electronic mail, and remote-control garage door openers. Fig. 1-17 lists all the
various major applications of electronic communication.
SIMPLEX (ONE-WAY)
1. AM and FM radio broadcasting. Stations broadcast
music, news, weather reports, and programs for
entertainment and information. It includes shortwave.
2. Digital radio. There is both satellite and terrestrial.
Radio programming is transmitted in digital format.
3. TV broadcasting. Stations broadcast entertainment,
informational, and educational programs by radio.
4. Digital television (DTV). Radio transmission of
television programming is performed by digital
methods, both satellite and terrestrial, e.g., high-
deinition television (HDTV) and Internet Protocol
Television (IPTV).
5. Cable television. Movies, sports events, and other
programs are distributed to subscribers by iber-optic
and coaxial cable.
6. Facsimile. Printed visual material is transmitted over
telephone lines. A facsimile, or fax, machine scans a
document and converts it to electronic signals that
are sent over the telephone system for reproduction
in printed form by another fax machine. Faxes can
also be sent from a computer.
7. Wireless remote control. This category includes a
device that controls any remote item by radio or
infrared. Examples are missiles, satellites, robots,
toys, and other vehicles or remote plants or
stations. A remote keyless entry device, garage
door opener, and the remote control on your TV
set are other examples.
8. Internet of Things (IoT). The monitoring or control
of remote devices, appliances, and other items
in a home, ofice or other facility is usually
accomplished by a combination of wireless
and Internet connectivity.
9. Navigation and direction-finding services. Special
stations transmit signals that can be picked up by
receivers for the purpose of identifying exact location
(latitude and longitude) or determining direction and/
or distance from a station. Such systems employ
both land-based and satellite stations. The services
are used primarily by boats and ships or airplanes,
although systems for cars and trucks are being
developed. The Global Positioning System (GPS)
which uses 24 satellites is the most widely used.
10. Telemetry. Measurements are transmitted over a long
distance. Telemetry systems use sensors to deter-
mine physical conditions (temperature, pressure, low
rate, voltages, frequency, etc.) at a remote location.
The sensors modulate a carrier signal that is sent by
wire or radio to a remote receiver that stores and/or
displays the data for analysis. Examples are satel-
lites, rockets, pipelines, plants, and factories.
Figure 1-17 Applications of electronic communication.
(continues on next page)
22 Chapter 1
11. Radio astronomy. Radio signals, including infrared,
are emitted by virtually all heavenly bodies such as
stars and planets. With the use of large directional
antennas and sensitive high-gain receivers, these
signals may be picked up and used to plot star
locations and study the universe. Radio astronomy
is an alternative and supplement to traditional
optical astronomy.
12. Surveillance. Surveillance means discreet monitoring
or “spying.” Electronic techniques are widely used by
police forces, governments, the military, business
and industry, and others to gather information for the
purpose of gaining some competitive advantage.
Techniques include phone taps, tiny wireless “bugs,”
clandestine listening stations, and reconnaissance
airplanes and satellites.
13. Music services. Continuous background music is
transmitted for doctors’ ofices, stores, elevators,
and so on by local FM radio stations on special
high-frequency subcarriers that cannot be picked
up by conventional FM receivers.
14. Internet radio and video. Music and video are
delivered on a computer via the Internet.
DUPLEX (TWO-WAY)
15. Telephones. One-on-one verbal communication is
transmitted over the vast worldwide telephone networks
employing wire, iber optics, radio, and satellites.
a. Cordless telephones provide short-distance
wireless communication for cord-free convenience.
b. Cell phones provide worldwide wireless communi-
cations via handsets and base stations and the
wired telephone system. In addition to voice
communications, cell phones facilitate e-mail,
Internet access, instant message service, video,
and games.
c. Internet telephones, known as voice over the
Internet protocol (VoIP) phones, use high-speed
broadband services (cable, DSL, wireless, iber)
over the Internet to provide digital voice
communications.
d. Satellite phones use low-earth-orbit satellites to
give worldwide voice service from any remote
location on earth.
16. Two-way radio. Commercial, industrial, and
government communication is transmitted
between vehicles, handheld units, and base stations.
Examples include police, ire, taxi, forestry service,
trucking companies, aircraft, marine, military, and
government.
17. Radar. This special form of communication
makes use of relected microwave signals for
the purpose of detecting ships, planes, and missiles
and for determining their range, direction, and speed.
Most radar is used in military applications, but civil-
ian aircraft and marine services also use it. Police
use radar in speed detection and enforcement.
18. Sonar. In underwater communication, audible base-
band signals use water as the transmission medium.
Submarines and ships use sonar to detect the
presence of enemy submarines. Passive sonar uses
audio receivers to pick up water, propeller, and other
noises. Active sonar is like an underwater radar with
which relections from a transmitted ultrasonic pulse
are used to determine the direction, range, and
speed of an underwater target.
19. Amateur radio. This is a hobby for individuals
interested in radio communication. Individuals may
become licensed “hams” to build and operate two-
way radio equipment for personal communication
with other hams.
20. Citizens radio. Citizens band (CB) radio is a special
service that any individual may use for personal
communication with others. Most CB radios are
used in trucks and cars for exchanging information
about trafic conditions, speed traps, and emergencies.
21. Family Radio Service. This is a two-way personal
communication with handheld units over short
distances (, 2 mi).
22. The Internet. Worldwide interconnections via iber-
optic networks, telecommunications companies, cable
TV companies, Internet service providers, and others
provide World Wide Web (WWW) access to millions
of websites and pages and electronic mail (e-mail).
23. Wide-Area Networks (WANs). Worldwide iber-optic
networks provide long-distance telephone and
Internet services.
24. Metropolitan-area networks (MANs). Networks of com-
puters transmit over a speciic geographic area such
as a college campus, company facility, or city. Nor-
mally they are implemented with iber-optic cable, but
may also be coaxial cable or wireless.
25. Local-area networks (LANs). Wired (or wireless)
interconnections of personal computers (PCs),
laptops, servers, or mainframe computers within an
ofice or building for the purpose of e-mail, Internet
access, or the sharing of mass storage, peripherals,
data, and software.
Figure 1-17 (continued)
Introduction to Electronic Communication 23
1-8 Jobs and Careers in the
Communication Industry
The electronics industry is roughly divided into four major specializations. The largest
in terms of people employed and the dollar value of equipment purchased is the com-
munications ield, closely followed by the computer ield. The industrial control and
instrumentation ields are considerably smaller. Hundreds of thousands of employees are
in the communication ield, and billions of dollars’ worth of equipment is purchased each
year. The growth rate varies from year to year depending upon the economy, techno-
logical developments, and other factors. But, as in most areas in electronics, the
communication ield has grown steadily over the years thanks to the Internet and the
exploding cellular industry, creating a relatively constant opportunity for employment. If
your interests lie in communication, you will be glad to know that there are many oppor-
tunities for long-term jobs and careers. The next section outlines the types of jobs avail-
able and the major kinds of employers.
Types of Jobs
The two major types of technical positions available in the communication ield are
engineer and technician.
Engineers. Engineers design communication equipment and systems. They have
bachelor’s (B.S.E.E.), master’s (M.S.E.E.), or doctoral (Ph.D.) degrees in electrical
engineering, giving them a strong science and mathematics background combined with
specialized education in electronic circuits and equipment. Engineers work from speci-
fications and create new equipment or systems, which are then manufactured.
Many engineers have a bachelor’s degree in electronics technology from a technical
college or university. Some typical degree titles are bachelor of technology (B.T.), bach-
elor of engineering technology (B.E.T.), and bachelor of science in engineering technol-
ogy (B.S.E.T.).
Bachelor of technology programs are sometimes extensions of two-year associate
degree programs. In the two additional years required for a bachelor of technology
degree, the student takes more complex electronics courses along with additional sci-
ence, math, and humanities courses. The main difference between the B.T. graduate and
the engineering graduate is that the technologist usually takes courses that are more
practical and hands-on than engineering courses. Holders of B.T. degrees can generally
design electronic equipment and systems but do not typically have the depth of back-
ground in analytical mathematics or science that is required for complex design jobs.
However, B.T. graduates are generally employed as engineers. Although many do design
work, others are employed in engineering positions in manufacturing and ield service
rather than design.
Some engineers specialize in design; others work in manufacturing, testing, quality
control, and management, among other areas. Engineers may also serve as ield service
personnel, installing and maintaining complex equipment and systems. If your interest
lies in the design of communication equipment, then an engineering position may be
for you.
Although a degree in electrical engineering is generally the minimum entrance
requirement for engineers’ jobs in most organizations, people with other educational
backgrounds (e.g., physics and math) do become engineers. Technicians who obtain
suficient additional education and appropriate experience may go on to become
engineers.
Technicians. Technicians have some kind of postsecondary education in electronics,
from a vocational or technical school, a community college, or a technical institute.
Many technicians are educated in military training programs. Most technicians have
Engineer
Technician
24 Chapter 1
an average of two years of formal post–high school education and an associate degree.
Common degrees are associate in arts (A.A.), associate in science (A.S.) or associate
of science in engineering technology or electronic engineering technology (A.S.E.T.
or A.S.E.E.T.), and associate in applied science (A.A.S.). The A.A.S. degrees tend to
cover more occupational and job-related subjects; the A.A. and A.S. degrees are more
general and are designed to provide a foundation for transfer to a bachelor’s degree
program. Technicians with an associate degree from a community college can usually
transfer to a bachelor of technology program and complete the bachelor’s degree in
another two years. However, associate degree holders are usually not able to transfer
to an engineering degree program but must literally start over if the engineering career
path is chosen.
Technicians are most often employed in service jobs. The work typically involves
equipment installation, troubleshooting and repair, testing and measuring, maintenance
and adjustment, or operation. Technicians in such positions are sometimes called ield
service technicians, ield service engineers, or customer representatives.
Technicians can also be involved in engineering. Engineers may use one or more
technicians to assist in the design of equipment. They build and troubleshoot pro-
totypes and in many cases actually participate in equipment design. A great deal of
the work involves testing and measuring. In this capacity, the technician is known
as an engineering technician, lab technician, engineering assistant, or associate
engineer.
Technicians are also employed in manufacturing. They may be involved in the actual
building and assembling of the equipment, but more typically are concerned with inal
testing and measurement of the inished products. Other positions involve quality control
or repair of defective units.
Other Positions. There are many jobs in the communication industry other than
those of engineer or technician. For example, there are many outstanding jobs in
technical sales. Selling complex electronic communication equipment often requires
a strong technical education and background. The work may involve determining cus-
tomer needs and related equipment specifications, writing technical proposals, making
sales presentations to customers, and attending shows and exhibits where equipment
is sold. The pay potential in sales is generally much higher than in the engineering or
service positions.
Another position is that of technical writer. Technical writers generate the technical
documentation for communication equipment and systems, producing installation and
service manuals, maintenance procedures, and customer operations manuals. This impor-
tant task requires considerable depth of education and experience.
Finally, there is the position of trainer. Engineers and technicians are often used
to train other engineers and technicians or customers. With the high degree of com-
plexity that exists in communication equipment today, there is a major need for
training. Many individuals ind education and training positions to be very desirable
and satisfying. The work typically involves developing curriculum and programs, gen-
erating the necessary training manuals and presentation materials, creating online
training, and conducting classroom training sessions in-house or at a customer site.
Major Employers
The overall structure of the communication electronics industry is shown in Fig. 1-18. The
four major segments of the industry are manufacturers, resellers, service organizations, and
end users.
Manufacturers. It all begins, of course, with customer needs. Manufacturers translate
customer needs into products, purchasing components and materials from other elec-
tronics companies to use in creating the products. Engineers design the products, and
Introduction to Electronic Communication 25
Figure 1-18 Structure of the communication electronics industry.
End users
Service
organizations
Resellers
Products and
services
Products and
services
Manufacturers
Components Materials
manufacturing produces them. There are jobs for engineers, technicians, salespeople,
field service personnel, technical writers, and trainers.
Resellers. Manufacturers who do not sell products directly to end users sell the prod-
ucts to reselling organizations, which in turn sell them to the end user. For example, a
manufacturer of marine communication equipment may not sell directly to a boat owner
but instead to a regional distributor or marine electronics store or shop. This shop not
only sells the equipment but also takes care of installation, service, and repairs. A cel-
lular telephone or fax machine manufacturer also typically sells to a distributor or dealer
who takes care of sales and service. Most of the jobs available in the reselling segment
of the industry are in sales, service, and training.
Service Organizations. These companies usually perform some kind of service, such
as repair, installation, or maintenance. One example is an avionics company that does
installation or service work on electronic equipment for private planes. Another is a sys-
tems integrator, a company that designs
and assembles a piece of communication
equipment or more often an entire system
by using the products of other companies.
Systems integrators put together systems
to meet special needs and customize
existing systems for particular jobs. Other
types of service organization are the
communications services providers like
cellular network carriers (e.g., AT&T,
Verizon), Internet providers, cable TV
companies, and Internet web companies
(e.g., Google, Yahoo, Amazon).
Most communication technicians
perform installation, maintenance,
and troubleshooting.
26 Chapter 1
End Users. The end user is the ultimate customer—and a major employer. Today,
almost every person and organization is an end user of communication equipment. The
major categories of end users in the communication field are:
Telephone companies
Radio users—mobile, marine, aircraft, etc.
Radio and TV broadcast stations and cable TV companies
Business and industry users of satellites, networks, etc.
Transportation companies (airlines, shipping, railroads)
Government and military
Internet companies
Personal and hobby
Consumers
There are an enormous number of communication jobs with end users. Most are of
the service type: installation, repair, maintenance, and operation of equipment.
Licensing and Certification
A good way to validate your knowledge of communications electronics is to obtain a
relevant license or certiication. Some jobs require an FCC license to ensure your com-
petence in electronics and knowledge of the related rules and regulations. Otherwise, the
main beneit of a license or certiication is to prove your knowledge and skills to a
prospective employer. Such a credential is an added bonus to any A.A.S. or B.S.E.T.
degree you may get. For some employers, a license or certiication may be acceptable
in lieu of a degree.
Licensing and certiication typically require taking an exam on communications
topics. The FCC exam includes tests on rules and regulations as well as electronic
fundamentals and communications circuits, equipment, and practices. Most certiica-
tions also have exams that cover the same electronic fundamentals and communications
circuits, equipment, and practices. Some certiications require a speciic amount of job
experience.
Listed below are some of the licenses and certiications available for communications.
• FCC General Radiotelephone Operators License (GROL)—Two-part exam on rules
and regulations and communications electronics. An optional exam on radar is avail-
able. No job experience is required.
• International Society of Certiied of Electronic Technicians (ISCET)—This organiza-
tion offers several basic certiications in electronic fundamentals as well as a journey-
man certiication in a variety of electronic specializations including communications.
No job experience is required.
• Electronic Technicians Association International (ETA-I)—This organization offers
a wide range of certiications on electronics with specializations in electronic fun-
damentals, communications, radar, iber optics, and several others.
• The International Association for Radio, Telecommunications and Electromagnetics
(iNARTE)—This organization offers multiple certiications in all phases of com-
munications, including telecommunications, electromagnetic compatibility, and
wireless devices at both the technician and the engineering level. These certiications
require various education levels (degrees) and job experience as well as exams.
• Cisco—This company is a major supplier of networking and wireless equipment and
offers certiications in many networking-related areas. An example is the Cisco Cer-
tiied Network Associate (CCNA) Wireless. Cisco certiication is widely recognized
throughout industry.
There are other certiications for a variety of specialties that you will discover. Many
of the certifying organizations, such as ETA-I, ISCET, and iNARTE, are also granted
Introduction to Electronic Communication 27
CHAPTER REVIEW
Online Activity
1-1 Exploring the Regulatory Agencies
Objective: Become familiar with the FCC and NTIA.
Procedure:
1. Go to the FCC website at www.fcc.gov.
2. Explore the website.
3. Go to the NTIA website at www.nita.doc.gov.
4. Explore the website.
5. Use these websites and their search feature to answer
the questions below.
Questions:
1. To whom does the FCC report within the government?
2. To whom does the NTIA report within the government?
3. What is the purpose and function of the FCC?
4. What is the purpose and function of the NTIA?
5. What is the FCC Code of Federal Regulations (CFR)
Title 47?
6. On the NTIA website, locate the large colorful fre-
quency spectrum chart. Examine it to see what ser-
vices are identiied and where they are located. Is the
chart available as a wall chart for purchase?
1-2 Examining FCC Rules and Regulations
Objective: Investigate FCC CFR Title 47 and ind answers
to electronic communication rules and regulations.
Procedure:
1. Go to the FCC website www.fcc.gov.
2. Click on the rules and regulations link on the left.
3. Access FCC CFR Title 47.
4. Study the different parts.
5. Use this reference to answer the questions below.
Questions:
1. What is contained in Subpart A of Part 2 that may be
useful?
2. In Part 2, what communications services can occupy
the spectrum from 108 to 138 MHz?
3. What part pertains to commercial operators’ licenses?
4. Describe briely what is in Part 15.
5. Describe briely what is in Part 18.
6. Which part covers TV broadcasting?
7. What part covers radar?
8. What parts cover Citizens’ Band radio and the Family
Radio Service? State the frequency bands of each.
9. Is cable TV regulated by the FCC? Which part if so?
10. List all of the modes and modulation methods allowed
by amateur radio operation.
11. Which part covers RF interference and electromag-
netic compatibility?
12. Which parts cover cell phones and wireless local area
networks?
authority to give the FCC GROL exams. The GROL is probably the best overall credential
to have for wireless jobs, and you may wish to complement it with a certiication appro-
priate to the work you are seeking.
Certiication and licensing is an excellent way to prove to yourself and any employer
that you are knowledgeable and competent in communications. Give serious consideration
to this opportunity.
1-3 Investigate Licensing and Certification
Objective: To learn more about the beneits of licensing and
certiication and how to obtain them.
Procedure:
1. Go to the FCC website www.fcc.gov.
2. On the FCC site, locate the information on commercial
operators’ licenses (GROL).
3. Go to each of the following websites and investigate
these major certiication sources:
a. International Society of Certiied Electronic
Technicians—www.iset.org.
b. Electronic Technician Association International—
www.eta-i.org.
28 Chapter 1
Questions
1. In what century did electronic communication begin?
2. Name the four main elements of a communication
system, and draw a diagram that shows their
relationship.
3. List ive types of media used for communication, and
state which three are the most commonly used.
4. Name the device used to convert an information sig-
nal to a signal compatible with the medium over
which it is being transmitted.
5. What piece of equipment acquires a signal from a
communication medium and recovers the original in-
formation signal?
6. What is a transceiver?
7. What are two ways in which a communication me-
dium can affect a signal?
8. What is another name for communication medium?
9. What is the name given to undesirable interference
that is added to a signal being transmitted?
10. Name three common sources of interference.
11. What is the name given to the original information or
intelligence signals that are transmitted directly via a
communication medium?
12. Name the two forms in which intelligence signals can
exist.
13. What is the name given to one-way communication?
Give three examples.
14. What is the name given to simultaneous two-way
communication? Give three examples.
15. What is the term used to describe two-way communi-
cation in which each party takes turns transmitting?
Give three examples.
16. What type of electronic signals are continuously vary-
ing voice and video signals?
17. What are on/off intelligence signals called?
18. How are voice and video signals transmitted digitally?
19. What terms are often used to refer to original voice,
video, or data signals?
20. What technique must sometimes be used to make an
information signal compatible with the medium over
which it is being transmitted?
21. What is the process of recovering an original signal called?
22. What is a broadband signal?
23. Name the process used to transmit two or more base-
band signals simultaneously over a common medium.
24. Name the technique used to extract multiple intelli-
gence signals that have been transmitted simultane-
ously over a single communication channel.
25. What is the name given to signals that travel through
free space for long distances?
26. What does a radio wave consist of?
27. Calculate the wavelength of signals with frequencies
of 1.5 kHz, 18 MHz, and 22 GHz in miles, feet, and
centimeters, respectively.
28. Why are audio signals not transmitted directly by
electromagnetic waves?
29. What is the human hearing frequency range?
30. What is the approximate frequency range of the hu-
man voice?
31. Do radio transmissions occur in the VLF and LF
ranges?
32. What is the frequency range of AM radio broadcast
stations?
33. What is the name given to radio signals in the
high-frequency range?
34. In what segment of the spectrum do TV channels 2 to
13, and FM broadcasting, appear?
35. List ive major uses of the UHF band.
36. What are frequencies above 1 GHz called?
37. What are the frequencies just above the EHF range
called?
38. What is a micrometer, and what is it used to measure?
39. Name the three segments of the optical frequency
spectrum.
40. What is a common source of infrared signals?
41. What is the approximate spectrum range of infrared
signals?
42. Deine the term angstrom and explain how it is used.
43. What is the wavelength range of visible light?
44. Which two channels or media do light signals use for
electronic communication?
45. Name two methods of transmitting visual data over a
telephone network.
46. What is the name given to the signaling of individuals
at remote locations by radio?
c. The International Association for Radio, Telecommu-
nications and Electromagnetics—www.narte.org.
4. Check out the certiication options at Cisco at www.
cisco.com.
5. Answer the questions below.
Questions:
1. What is the GROL and who is required to have one?
2. What is the procedure for getting a GROL?
3. List any available supplements to the GROL.
4. List the basic requirements for a communications-
related certiication from each of the organizations
listed above. Which one appeals to you most?
5. Which certiication requires education and job experi-
ence qualiications?
Introduction to Electronic Communication 29
47. What term is used to describe the process of making
measurements at a distance?
48. List four ways radio is used in the telephone system.
49. What principle is used in radar?
50. What is underwater radar called? Give two examples.
51. What is the name of a popular radio communication
hobby?
52. What device enables computers to exchange digital
data over the telephone network?
53. What do you call the systems of interconnections of
PCs and other computers in ofices or buildings?
54. What is a generic synonym for radio?
55. Name the three main types of technical positions
available in the communication ield.
56. What is the main job of an engineer?
57. What is the primary degree for an engineer?
58. What is the primary degree for a technician?
59. Name a type of technical degree in engineering other
than engineer or technician.
60. Can the holder of an associate of technology degree trans-
fer the credits to an engineering degree program?
61. What types of work does a technician ordinarily do?
62. List three other types of jobs in the ield of electronic
communication that do not involve engineering or
technician’s work.
63. What are the four main segments of the communica-
tion industry? Explain briely the function of each.
64. Why are standards important?
65. What types of characteristics do communication stan-
dards deine?
1. Calculate the frequency of signals with wavelengths
of 40 m, 5 m, and 8 cm. ◆
2. In what frequency range does the common ac power
line frequency fall?
3. What is the primary use of the SHF and EHF ranges? ◆
◆ Answers to Selected Problems follow Chap. 22.
1. Name three ways that a higher-frequency signal called
the carrier can be varied to transmit the intelligence.
2. Name two common household remote-control units,
and state the type of media and frequency ranges used
for each.
3. How is radio astronomy used to locate and map stars
and other heavenly bodies?
4. In what segment of the communication ield are you
interested in working, and why?
5. Assume that all the electromagnetic spectrum from ELF
through microwaves was fully occupied. Explain some
ways that communication capability could be added.
6. What is the speed of light in feet per microsecond? In
inches per nanosecond? In meters per second?
7. Make a general statement comparing the speed of
light with the speed of sound. Give an example of how
the principles mentioned might be demonstrated.
8. List ive real-life communication applications not
speciically mentioned in this chapter.
9. “Invent” ive new communication methods, wired or
wireless, that you think would be practical.
10. Assume that you have a wireless application you
would like to design, build, and sell as a commercial
product. You have selected a target frequency in the
UHF range. How would you decide what frequency to
use, and how would you get permission to use it?
11. Make an exhaustive list of all the electronic communi-
cation products that you own, have access to at home
or in the ofice, and/or use on a regular basis.
12. You have probably seen or heard of a simple commu-
nication system made of two paper cups and a long
piece of string. How could such a simple system
work?
Problems
Critical Thinking
30
chapter
2
Electronic Fundamentals
for Communications
To understand communication electronics as presented in this book, you
need a knowledge of certain basic principles of electronics, including the
fundamentals of alternating-current (ac) and direct-current (dc) circuits,
semiconductor operation and characteristics, and basic electronic circuit
operation (amplifiers, oscillators, power supplies, and digital logic circuits).
Some of the basics are particularly critical to understanding the chapters
that follow. These include the expression of gain and loss in decibels, LC
tuned circuits, resonance and filters, and Fourier theory. The purpose of
this chapter is to briefly review all these subjects. If you have studied the
material before, it will simply serve as a review and reference. If, because
of your own schedule or the school’s curriculum, you have not previously
covered this material, use this chapter to learn the necessary information
before you continue.
Objectives
After completing this chapter, you will be able to:
■ Calculate voltage, current, gain, and attenuation in decibels and
apply these formulas in applications involving cascaded circuits.
■ Explain the relationship between Q, resonant frequency, and bandwidth.
■ Describe the basic configuration of the diferent types of filters that
are used in communication networks and compare and contrast
active filters with passive filters.
■ Explain how using switched capacitor filters enhances selectivity.
■ Explain the benefits and operation of crystal, ceramic, and SAW filters.
■ Calculate bandwidth by using Fourier analysis.
Electronic Fundamentals for Communications 31
2-1 Gain, Attenuation, and Decibels
Most electronic circuits in communication are used to process signals, i.e., to manipulate
signals to produce a desired result. All signal processing circuits involve either gain or
attenuation.
Gain
Gain means ampliication. If a signal is applied to a circuit such as the ampliier shown
in Fig. 2-1 and the output of the circuit has a greater amplitude than the input signal,
the circuit has gain. Gain is simply the ratio of the output to the input. For input (Vin)
and output (Vout) voltages, voltage gain AV is expressed as follows:
AV 5
output
input
5
Vout
Vin
The number obtained by dividing the output by the input shows how much larger
the output is than the input. For example, if the input is 150 µV and the output is
75 mV, the gain is AV 5 (75 3 1023
)y(150 3 1026
) 5 500.
The formula can be rearranged to obtain the input or the output, given the other two
variables: Vout 5 Vin 3 AV and Vin 5 Vout/AV.
If the output is 0.6 V and the gain is 240, the input is Vin 5 0.6/240 5
2.5 3 1023
5 2.5 mV.
Gain
Vin
Input signal
A ⫽ gain ⫽
Vout
Output signal
Amplifier
Vout
Vin
Figure 2-1 An amplifier has
gain.
Example 2-1
What is the voltage gain of an ampliier that produces an output of 750 mV for a
30-µV input?
AV 5
Vout
Vin
5
750 3 1023
30 3 1026
5 25,000
Example 2-2
The power output of an ampliier is 6 watts (W). The power gain is 80. What is the
input power?
AP 5
Pout
Pin
therefore Pin 5
Pout
AP
Pin 5
6
80
5 0.075 W 5 75 mW
Since most ampliiers are also power ampliiers, the same procedure can be used to
calculate power gain AP:
AP 5
Pout
Pin
where Pin is the power input and Pout is the power output.
32 Chapter 2
When two or more stages of ampliication or other forms of signal processing are
cascaded, the overall gain of the combination is the product of the individual circuit
gains. Fig. 2-2 shows three ampliiers connected one after the other so that the output
of one is the input to the next. The voltage gains of the individual circuits are marked.
To ind the total gain of this circuit, simply multiply the individual circuit gains:
AT 5 A1 3 A2 3 A3 5 5 3 3 3 4 5 60.
If an input signal of 1 mV is applied to the irst ampliier, the output of the third
ampliier will be 60 mV. The outputs of the individual ampliiers depend upon their
individual gains. The output voltage from each ampliier is shown in Fig. 2-2.
Figure 2-2 Total gain of cascaded circuits is the product of individual stage gains.
Vin ⫽ 1 mV 5 mV 15 mV Vout ⫽ 60 mV
A1 ⫽ 5
AT ⫽ A1 ⫻ A2 ⫻ A3 ⫽ 5 ⫻ 3 ⫻ 4 ⫽ 60
A2 ⫽ 3 A3 ⫽ 4
Example 2-3
Three cascaded ampliiers have power gains of 5, 2, and 17. The input power is
40 mW. What is the output power?
AP 5 A1 3 A2 3 A3 5 5 3 2 3 17 5 170
AP 5
Pout
Pin
therefore Pout 5 APPin
Pout 5 170(40 3 1023
) 5 6.8 W
Example 2-4
A two-stage ampliier has an input power of 25 µW and an output power of 1.5 mW.
One stage has a gain of 3. What is the gain of the second stage?
AP 5
Pout
Pin
5
1.5 3 1023
25 3 1026
5 60
AP 5 A1 3 A2
If A1 5 3, then 60 5 3 3 A2 and A2 5 60y3 5 20.
Electronic Fundamentals for Communications 33
Attenuation
Attenuation refers to a loss introduced by a circuit or component. Many electronic circuits,
sometimes called stages, reduce the amplitude of a signal rather than increase it. If the
output signal is lower in amplitude than the input, the circuit has loss, or attenuation. Like
gain, attenuation is simply the ratio of the output to the input. The letter A is used to
represent attenuation as well as gain:
Attenuation A 5
output
input
5
Vout
Vin
Circuits that introduce attenuation have a gain that is less than 1. In other words,
the output is some fraction of the input.
An example of a simple circuit with attenuation is a voltage divider such as that
shown in Fig. 2-3. The output voltage is the input voltage multiplied by a ratio based
on the resistor values. With the resistor values shown, the gain or attenuation factor of
the circuit is A 5 R2/(R1 1 R2) 5 100/(200 1 100) 5 100/300 5 0.3333. If a signal of
10 V is applied to the attenuator, the output is Vout 5 Vin A 5 10(0.3333) 5 3.333 V.
When several circuits with attenuation are cascaded, the total attenuation is, again,
the product of the individual attenuations. The circuit in Fig. 2-4 is an example. The
attenuation factors for each circuit are shown. The overall attenuation is
AT 5 A1 3 A2 3 A3
With the values shown in Fig. 2-4, the overall attenuation is
AT 5 0.2 3 0.9 3 0.06 5 0.0108
Given an input of 3 V, the output voltage is
Vout 5 ATVin 5 0.0108(3) 5 0.0324 5 32.4 mV
R1 ⫽ 200 ⍀
R2 ⫽ 100 ⍀
Vout ⫽ Vin
Vin
R2
R1 ⫹ R2
A ⫽ ⫽ ⫽
R2
R1 ⫹ R2
100
0.3333
300
Figure 2-3 A voltage divider introduces attenuation.
Figure 2-4 Total attenuation is the product of individual attenuations of each
cascaded circuit.
Loss
stage
AT ⫽ A1 ⫻ A2 ⫻ A3 ⫽ 0.2 ⫻ 0.9 ⫻ 0.06 ⫽ 0.0108
Vout ⫽ ATVin ⫽ 0.0324 ⫽ 32.4 mV
A1 ⫽ 0.2 A2 ⫽ 0.9 A3 ⫽ 0.06
Vin ⫽ 3 V Vout
Loss
circuit
Loss
component
Attenuation
34 Chapter 2
It is common in communication systems and equipment to cascade circuits and
components that have gain and attenuation. For example, loss introduced by a circuit can
be compensated for by adding a stage of ampliication that offsets it. An example of this
is shown in Fig. 2-5. Here the voltage divider introduces a 4-to-1 voltage loss, or an
attenuation of 0.25. To offset this, it is followed with an ampliier whose gain is 4. The
overall gain or attenuation of the circuit is simply the product of the attenuation and gain
factors. In this case, the overall gain is AT 5 A1A2 5 0.25(4) 5 1.
Another example is shown in Fig. 2-6, which shows two attenuation circuits and
two ampliier circuits. The individual gain and attenuation factors are given. The overall
circuit gain is AT 5 A1 A2 A3 A4 5 (0.1)(10)(0.3)(15) 5 4.5.
For an input voltage of 1.5 V, the output voltage at each circuit is shown in
Fig. 2-6.
In this example, the overall circuit has a net gain. But in some instances, the overall
circuit or system may have a net loss. In any case, the overall gain or loss is obtained
by multiplying the individual gain and attenuation factors.
Figure 2-5 Gain exactly ofsets the attenuation.
Vin
750 ⍀
250 ⍀
A2 ⫽ 4
A1 ⫽ AT ⫽ A1A2 ⫽ 0.25(4) ⫽ 1
Vout ⫽ Vin
250
750 ⫹ 250
A1 ⫽
250
1000
⫽ 0.25
Example 2-5
A voltage divider such as that shown in Fig. 2-5 has values of R1 5 10 kV and
R2 5 470 V.
a. What is the attenuation?
A1 5
R2
R1 1 R2
5
470
10,470
A1 5 0.045
b. What amplifier gain would you need to offset the loss for an overall gain of 1?
AT 5 A1A2
where A1 is the attenuation and A2 is the amplifier gain.
1 5 0.045A2 A2 5
1
0.045
5 22.3
Note: To ind the gain that will offset the loss for unity gain, just take the
reciprocal of attenuation: A2 5 1yA1.
Electronic Fundamentals for Communications 35
Decibels
The gain or loss of a circuit is usually expressed in decibels (dB), a unit of measurement
that was originally created as a way of expressing the hearing response of the human
ear to various sound levels. A decibel is one-tenth of a bel.
When gain and attenuation are both converted to decibels, the overall gain or atten-
uation of an electronic circuit can be computed by simply adding the individual gains or
attenuations, expressed in decibels.
It is common for electronic circuits and systems to have extremely high gains or
attenuations, often in excess of 1 million. Converting these factors to decibels and using
logarithms result in smaller gain and attenuation igures, which are easier to use.
Decibel Calculations. The formulas for computing the decibel gain or loss of a
circuit are
dB 5 20 log
Vout
Vin
(1)
dB 5 20 log
Iout
Iin
(2)
dB 5 10 log
Pout
Pin
(3)
Formula (1) is used for expressing the voltage gain or attenuation of a circuit; for-
mula (2), for current gain or attenuation. The ratio of the output voltage or current to
the input voltage or current is determined as usual. The base-10 or common log of the
input/output ratio is then obtained and multiplied by 20. The resulting number is the
gain or attenuation in decibels.
Figure 2-6 The total gain is the product of the individual stage gains and attenuations.
Loss
stage
Loss
stage
Vin ⫽ 1.5 V
A1 ⫽ 0.1 A2 ⫽ 10 A3 ⫽ 0.3 A4 ⫽ 15
AT ⫽ A1A2A3A4 ⫽ (0.1)(10)(0.3)(15) ⫽ 4.5
0.15 V 1.5 V 0.45 V Vout ⫽ 6.75 V
Example 2-6
An ampliier has a gain of 45,000, which is too much for the application. With an
input voltage of 20 µV, what attenuation factor is needed to keep the output voltage
from exceeding 100 mV? Let A1 5 ampliier gain 5 45,000; A2 5 attenuation factor;
AT 5 total gain.
AT 5
Vout
Vin
5
100 3 1023
20 3 1026
5 5000
AT 5 A1A2 therefore A2 5
AT
A1
5
5000
45,000
5 0.1111
Decibel (dB)
36 Chapter 2
Formula (3) is used to compute power gain or attenuation. The ratio of the power
output to the power input is computed, and then its logarithm is multiplied by 10.
Example 2-7
a. An amplifier has an input of 3 mV and an output of 5 V. What is the gain in
decibels?
dB 5 20 log
5
0.003
5 20 log 1666.67 5 20(3.22) 5 64.4
b. A filter has a power input of 50 mW and an output of 2 mW. What is the gain
or attenuation?
dB 5 10 log
2
50
5 10 log 0.04 5 10(21.398) 5 213.98
Note that when the circuit has gain, the decibel igure is positive. If the gain is
less than 1, which means that there is an attenuation, the decibel igure is negative.
Now, to calculate the overall gain or attenuation of a circuit or system, you simply add
the decibel gain and attenuation factors of each circuit. An example is shown in Fig. 2-7,
where there are two gain stages and an attenuation block. The overall gain of this circuit is
AT 5 A1 1 A2 1 A3 5 15 2 20 1 35 5 30 dB
Decibels are widely used in the expression of gain and attenuation in communication
circuits. The table on the next page shows some common gain and attenuation factors
and their corresponding decibel igures.
Ratios less than 1 give negative decibel values, indicating attenuation. Note that a
2:1 ratio represents a 3-dB power gain or a 6-dB voltage gain.
Antilogs. To calculate the input or output voltage or power, given the decibel gain
or attenuation and the output or input, the antilog is used. The antilog is the number
obtained when the base is raised to the logarithm, which is the exponent:
dB 5 10 log
Pout
Pin
and
dB
10
5 log
Pout
Pin
and
Pout
Pin
5 antilog
dB
10
5 log21 dB
10
The antilog is simply the base 10 raised to the dB/10 power.
Antilog
Figure 2-7 Total gain or attenuation is the algebraic sum of the individual stage
gains in decibels.
AT ⫽ A1 ⫹ A2 ⫹ A3
AT ⫽ 15 ⫺ 20 ⫹ 35 ⫽ 30 dB
A1 ⫽ 15 dB
A2 ⫽ ⫺20 dB
A3 ⫽ 35 dB
Loss
stage
Electronic Fundamentals for Communications 37
Remember that the logarithm y of a number N is the power to which the base 10
must be raised to get the number.
N 5 10y
and y 5 log N
Since
dB 5 10 log
Pout
Pin
dB
10
5 log
Pout
Pin
Therefore
Pout
Pin
5 10dB/10
5 log21 dB
10
The antilog is readily calculated on a scientiic calculator. To ind the antilog for a
common or base-10 logarithm, you normally press the Inv or 2nd
function key on the
calculator and then the log key. Sometimes the log key is marked with 10x
, which is the
antilog. The antilog with base e is found in a similar way, by using the Inv
or 2nd
function on the In key. It is sometimes marked ex
, which is the same as the
antilog.
d B G A I N O R A T T E N U A T I O N
Ratio (Power or Voltage) Power Voltage
0.000001 260 2120
0.00001 250 2100
0.0001 240 280
0.001 230 260
0.01 220 240
0.1 210 220
0.5 23 26
1 0 0
2 3 6
10 10 20
100 20 40
1000 30 60
10,000 40 80
100,000 50 100
38 Chapter 2
Example 2-8
A power ampliier with a 40-dB gain has an output power of 100 W. What is the input
power?
dB 5 10 log
Pout
Pin
antilog 5 log21
dB
10
5 log
Pout
Pin
40
10
5 log
Pout
Pin
4 5 log
Pout
Pin
antilog 4 5 antilog alog
Pout
Pin
b
log21
4 5
Pout
Pin
Pout
Pin
5 104
5 10,000
Pin 5
Pout
10,000
5
100
10,000
5 0.01 W 5 10 mW
Example 2-9
An ampliier has a gain of 60 dB. If the input voltage is 50 µV, what is the output
voltage?
Since
dB 5 20 log
Vout
Vin
dB
20
5 log
Vout
Vin
Therefore
Vout
Vin
5 log21 dB
20
510dB/20
Vout
Vin
5 1060/20
5 103
Vout
Vin
5 103
5 1000
Vout 5 1000Vin 5 1000 (50 3 1026
) 5 0.05 V 5 50 mV
Electronic Fundamentals for Communications 39
dBm. When the gain or attenuation of a circuit is expressed in decibels, implicit is a
comparison between two values, the output and the input. When the ratio is computed,
the units of voltage or power are canceled, making the ratio a dimensionless, or relative,
figure. When you see a decibel value, you really do not know the actual voltage or
power values. In some cases, this is not a problem; in others, it is useful or necessary
to know the actual values involved. When an absolute value is needed, you can use
a reference value to compare any other value.
An often used reference level in communication is 1 mW. When a decibel value is
computed by comparing a power value to 1 mW, the result is a value called the dBm. It
is computed with the standard power decibel formula with 1 mW as the denominator of
the ratio:
dBm 5 10 log
Pout(W)
0.001(W)
Here Pout is the output power, or some power value you want to compare to 1 mW, and
0.001 is 1 mW expressed in watts.
The output of a 1-W ampliier expressed in dBm is, e.g.,
dBm 5 10 log
1
0.001
5 10 log 1000 5 10(3) 5 30 dBm
Sometimes the output of a circuit or device is given in dBm. For example, if a micro-
phone has an output of 250 dBm, the actual output power can be computed as follows:
250 dBm 5 10 log
Pout
0.001
250 dBm
10
5 log
Pout
0.001
Therefore
Pout
0.001
5 10250 dBm/10
5 1025
5 0.00001
Pout 5 0.001 3 0.00001 5 1023
3 1025
5 1028
W 5 10 3 1029
5 10 nW
Example 2-10
A power ampliier has an input of 90 mV across 10 kV. The output is 7.8 V across
an 8-V speaker. What is the power gain, in decibels? You must compute the input and
output power levels irst.
P 5
V2
R
Pin 5
(90 3 1023
)2
104
5 8.1 3 1027
W
Pout 5
(7.8)2
8
5 7.605 W
AP 5
Pout
Pin
5
7.605
8.1 3 1027 5 9.39 3 106
AP (dB) 5 10 log AP 5 10 log 9.39 3 106
5 69.7 dB
GOOD TO KNOW
From the standpoint of sound
measurement, 0 dB is the least
perceptible sound (hearing
threshold), and 120 dB equals the
pain threshold of sound. This list
shows intensity levels for com-
mon sounds. (Tippens, Physics,
6th ed., Glencoe/McGraw-Hill,
2001, p. 497)
Intensity
Sound level, dB
Hearing threshold 0
Rustling leaves 10
Whisper 20
Quiet radio 40
Normal conversation 65
Busy street corner 80
Subway car 100
Pain threshold 120
Jet engine 140–160
Reference value
dBm
40 Chapter 2
dBc. This is a decibel gain attenuation figure where the reference is the carrier. The
carrier is the base communication signal, a sine wave that is modulated. Often the ampli-
tude’s sidebands, spurious or interfering signals, are referenced to the carrier. For exam-
ple, if the spurious signal is 1 mW compared to the 10-W carrier, the dBc is
dBc 5 10 log
Psignal
Pcarrier
dBc 5 10 log
0.001
10
5 10(24) 5 240
Example 2-11
An ampliier has a power gain of 28 dB. The input power is 36 mW. What is the
output power?
Pout
Pin
5 10dBy10
5 102.8
5 630.96
Pout 5 630.96Pin 5 630.96(36 3 1023
) 5 22.71 W
Example 2-12
A circuit consists of two ampliiers with gains of 6.8 and 14.3 dB and two ilters with
attenuations of 216.4 and 22.9 dB. If the output voltage is 800 mV, what is the input
voltage?
AT 5 A1 1 A2 1 A3 1 A4 5 6.8 1 14.3 2 16.4 2 2.9 5 1.8 dB
AT 5
Vout
Vin
5 10dBy20
5 101.8y20
5 100.09
Vout
Vin
5 100.09
5 1.23
Vin 5
Vout
1.23
5
800
1.23
5 650.4 mV
Example 2-13
Express Pout 5 12.3 dBm in watts.
Pout
0.001
5 10dBmy10
5 1012.3y10
5 101.23
5 17
Pout 5 0.001 3 17 5 17 mW
Electronic Fundamentals for Communications 41
2-2 Tuned Circuits
Virtually all communication equipment contains tuned circuits, circuits made up of
inductors and capacitors that resonate at speciic frequencies. In this section, you will
review how to calculate the reactance, resonant frequency, impedance, Q, and bandwidth
of series and parallel resonance circuits.
Reactive Components
All tuned circuits and many ilters are made up of inductive and capacitive
elements, including discrete components such as coils and capacitors and
the stray and distributed inductance and capacitance that appear in all elec-
tronic circuits. Both coils and capacitors offer an opposition to alternating-
current low known as reactance, which is expressed in ohms (abbreviated
Ω). Like resistance, reactance is an opposition that directly affects the
amount of current in a circuit. In addition, reactive effects produce a phase
shift between the currents and voltages in a circuit. Capacitance causes the
current to lead the applied voltage, whereas inductance causes the current
to lag the applied voltage. Coils and capacitors used together form tuned,
or resonant, circuits.
Capacitors. A capacitor used in an ac circuit continually charges and dis-
charges. A capacitor tends to oppose voltage changes across it. This translates
to an opposition to alternating current known as capacitive reactance XC.
The reactance of a capacitor is inversely proportional to the value of capacitance C
and operating frequency f. It is given by the familiar expression
XC 5
1
2πfC
The reactance of a 100-pF capacitor at 2 MHz is
XC 5
1
6.28(2 3 106
)(100 3 10212
)
5 796.2 V
The formula can also be used to calculate either frequency or capacitance depending
on the application. These formulas are
f 5
1
2πXCC
and C 5
1
2πf XC
The wire leads of a capacitor have resistance and inductance, and the dielectric has
leakage that appears as a resistance value in parallel with the capacitor. These character-
istics, which are illustrated in Fig. 2-8, are sometimes referred to as residuals or parasit-
ics. The series resistance and inductance are very small, and the leakage resistance is
Tuned circuit
Chip capacitors.
Reactance
Capacitor
Capacitive reactance
Residual
GOOD TO KNOW
Stray and distributed capaci-
tances and inductances can
greatly alter the operation and
performance of a circuit.
Figure 2-8 What a capacitor looks like at high frequencies.
R
Rleakage
C
Lead inductance
R
L L
Lead resistance
42 Chapter 2
very high, so these factors can be ignored at low frequencies. At radio frequencies,
however, these residuals become noticeable, and the capacitor functions as a complex
RLC circuit. Most of these effects can be greatly minimized by keeping the capacitor
leads very short. This problem is mostly eliminated by using the newer chip capacitors,
which have no leads as such.
Capacitance is generally added to a circuit by a capacitor of a speciic value, but
capacitance can occur between any two conductors separated by an insulator. For exam-
ple, there is capacitance between the parallel wires in a cable, between a wire and a
metal chassis, and between parallel adjacent copper patterns on a printed-circuit board.
These are known as stray, or distributed, capacitances. Stray capacitances are typically
small, but they cannot be ignored, especially at the high frequencies used in communica-
tion. Stray and distributed capacitances can signiicantly affect the performance of a
circuit.
Inductors. An inductor, also called a coil or choke, is simply a winding of multiple
turns of wire. When current is passed through a coil, a magnetic ield is produced around
the coil. If the applied voltage and current are varying, the magnetic ield alternately
expands and collapses. This causes a voltage to be self-induced into the coil winding,
which has the effect of opposing current changes in the coil. This effect is known as
inductance.
The basic unit of inductance is the henry (H). Inductance is directly affected by the
physical characteristics of the coil, including the number of turns of wire in the induc-
tor, the spacing of the turns, the length of the coil, the diameter of the coil, and the
type of magnetic core material. Practical inductance values are in the millihenry
(mH 5 1023
H), microhenry (µH 5 1026
H), and nanohenry (nH 5 1029
H) regions.
Fig. 2-9 shows several different types of inductor coils.
● Fig. 2-9(a) is an inductor made of a heavy, self-supporting wire coil.
● In Fig. 2-9(b) the inductor is formed of a copper spiral that is etched right onto the
board itself.
● In Fig. 2-9(c) the coil is wound on an insulating form containing a powdered iron
or ferrite core in the center, to increase its inductance.
● Fig. 2-9(d) shows another common type of inductor, one using turns of wire on a
toroidal or doughnut-shaped form.
● Fig. 2-9(e) shows an inductor made by placing a small ferrite bead over a wire; the
bead effectively increases the wire’s small inductance.
● Fig. 2-9( f ) shows a chip inductor. It is typically no more than 1
⁄8 to 1
⁄4 in long.
A coil is contained within the body, and the unit is soldered to the circuit board
with the end connections. These devices look exactly like chip resistors and
capacitors.
In a dc circuit, an inductor will have little or no effect. Only the ohmic resistance
of the wire affects current low. However, when the current changes, such as during the
time the power is turned off or on, the coil will oppose these changes in current.
When an inductor is used in an ac circuit, this opposition becomes continuous and
constant and is known as inductive reactance. Inductive reactance XL is expressed in
ohms and is calculated by using the expression
XL 5 2πfL
For example, the inductive reactance of a 40-µH coil at 18 MHz is
XL 5 6.28(18 3 106
)(40 3 1026
) 5 4522 V
In addition to the resistance of the wire in an inductor, there is stray capacitance
between the turns of the coil. See Fig. 2-10(a). The overall effect is as if a small capac-
itor were connected in parallel with the coil, as shown in Fig. 2-10(b). This is the equivalent
circuit of an inductor at high frequencies. At low frequencies, capacitance may be
Stray (or distributed) capacitance
Inductor (coil or choke)
Inductance
Inductive reactance
Electronic Fundamentals for Communications 43
ignored, but at radio frequencies, it is suficiently large to affect circuit operation. The
coil then functions not as a pure inductor, but as a complex RLC circuit with a self-
resonating frequency.
Any wire or conductor exhibits a characteristic inductance. The longer the wire, the
greater the inductance. Although the inductance of a straight wire is only a fraction of
Figure 2-9 Types of inductors. (a) Heavy self-supporting wire coil. (b) Inductor made
as copper pattern. (c) Insulating form. (d) Toroidal inductor. (e) Ferrite
bead inductor. (f ) Chip inductor.
(a)
Printed circuit (PC)
board
Component
lead or wire
(e)
Ferrite
bead
Insulating
form
Core moves in or
out to vary inductance
Powdered
iron or ferrite
core
(c)
(b)
PC board
Toroidal
inductor
Turns
of wire
(d )
(f )
Toroidal
core
Body
Solder
connection
Figure 2-10 Equivalent circuit of an inductor at high frequencies. (a) Stray capacitance between turns. (b) Equivalent
circuit of an inductor at high frequencies.
Stray capacitance
between turns
Winding (coil) resistance
L ⫽ inductor
C ⫽ stray capacitance
(a) (b)
R
44 Chapter 2
a microhenry, at very high frequencies the reactance can be signiicant. For this reason,
it is important to keep all lead lengths short in interconnecting components in RF circuits.
This is especially true of capacitor and transistor leads, since stray or distributed induc-
tance can signiicantly affect the performance and characteristics of a circuit.
Another important characteristic of an inductor is its quality factor Q, the ratio of
inductive power to resistive power:
Q 5
I2
XL
I2
R
5
XL
R
This is the ratio of the power returned to the circuit to the power actually dissipated by
the coil resistance. For example, the Q of a 3-µH inductor with a total resistance of 45V
at 90 MHz is calculated as follows:
Q 5
2πfL
R
5
6.28(90 3 106
)(3 3 1026
)
45
5
1695.6
45
5 37.68
Resistors. At low frequencies, a standard low-wattage color-coded resistor offers nearly
pure resistance, but at high frequencies its leads have considerable inductance, and stray
capacitance between the leads causes the resistor to act as a complex RLC circuit, as
shown in Fig. 2-11. To minimize the inductive and capacitive effects, the leads are kept
very short in radio applications.
The tiny resistor chips used in surface-mount construction of the electronic circuits
preferred for radio equipment have practically no leads except for the metallic end pieces
soldered to the printed-circuit board. They have virtually no lead inductance and little
stray capacitance.
Many resistors are made from a carbon-composition material in powdered form
sealed inside a tiny housing to which leads are attached. The type and amount of
carbon material determine the value of these resistors. They contribute noise to the
circuit in which they are used. The noise is caused by thermal effects and the granular
nature of the resistance material. The noise contributed by such resistors in an ampliier
used to amplify very low level radio signals may be so high as to obliterate the desired
signal.
To overcome this problem, ilm resistors were developed. They are made by depos-
iting a carbon or metal ilm in spiral form on a ceramic form. The size of the spiral
and the kind of metal ilm determine the resistance value. Carbon ilm resistors are
quieter than carbon-composition resistors, and metal ilm resistors are quieter than
carbon ilm resistors. Metal ilm resistors should be used in ampliier circuits that must
deal with very low level RF signals. Most surface-mount resistors are of the metallic
ilm type.
Skin Efect. The resistance of any wire conductor, whether it is a resistor or capacitor
lead or the wire in an inductor, is primarily determined by the ohmic resistance of the
wire itself. However, other factors inluence it. The most signiicant one is skin effect,
the tendency of electrons lowing in a conductor to low near and on the outer surface
Quality factor Q
Resistor
Skin effect
Figure 2-11 Equivalent circuit of a resistor at high (radio) frequencies.
Resistor Lead inductance
Stray capacitance
Electronic Fundamentals for Communications 45
of the conductor frequencies in the VHF, UHF, and microwave regions (Fig. 2-12). This
has the effect of greatly decreasing the total cross-sectional area of the conductor, thus
increasing its resistance and signiicantly affecting the performance of the circuit in
which the conductor is used. For example, skin effect lowers the Q of an inductor at
the higher frequencies, causing unexpected and undesirable effects. Thus many
high-frequency coils, particularly those in high-powered transmitters, are made with cop-
per tubing. Since current does not low in the center of the conductor, but only on the
surface, tubing provides the most eficient conductor. Very thin conductors, such as a
copper pattern on a printed-circuit board, are also used. Often these conductors are sil-
ver- or gold-plated to further reduce their resistance.
Tuned Circuits and Resonance
A tuned circuit is made up of inductance and capacitance and resonates at a speciic
frequency, the resonant frequency. In general, the terms tuned circuit and resonant circuit
are used interchangeably. Because tuned circuits are frequency-selective, they respond
best at their resonant frequency and at a narrow range of frequencies around the resonant
frequency.
Series Resonant Circuits. A series resonant circuit is made up of inductance,
capacitance, and resistance, as shown in Fig. 2-13. Such circuits are often referred to as
LCR circuits or RLC circuits. The inductive and capacitive reactances depend upon the
frequency of the applied voltage. Resonance occurs when the inductive and capacitive
reactances are equal. A plot of reactance versus frequency is shown in Fig. 2-14, where
fr is the resonant frequency.
Tuned (resonant) circuit
Series resonant circuit
LCR circuit
RLC circuit
Figure 2-12 Skin efect increases wire and inductor resistance at high frequencies.
Electrons
flow on or
near surface
No current flow in center of wire
Wire
Figure 2-13 Series RLC circuit.
VL
Vs
XL
XC
VR
R
VC
Figure 2-14 Variation of reactance with
frequency.
Reactance
Frequency
XC XL
XL ⫽ XC
fr
46 Chapter 2
The total impedance of the circuit is given by the expression
Z 5 2R2
1 (XL 2 XC)2
When XL equals XC, they cancel each other, leaving only the resistance of the circuit
to oppose the current. At resonance, the total circuit impedance is simply the value of
all series resistances in the circuit. This includes the resistance of the coil and the
resistance of the component leads, as well as any physical resistor in the circuit.
The resonant frequency can be expressed in terms of inductance and capacitance. A
formula for resonant frequency can be easily derived. First, express XL and XC as an
equivalence: XL 5 XC. Since
XL 5 2πfr L and XC 5
1
2πfr C
we have
2πfr L 5
1
2πfrC
Solving for fr gives
fr 5
1
2π1LC
In this formula, the frequency is in hertz, the inductance is in henrys, and the capacitance
is in farads.
Example 2-14
What is the resonant frequency of a 2.7-pF capacitor and a 33-nH inductor?
fr 5
1
2π1LC
5
1
6.28233 3 1029
3 2.7 3 10212
5 5.33 3 108
Hz or 533 MHz
It is often necessary to calculate capacitance or inductance, given one of those val-
ues and the resonant frequency. The basic resonant frequency formula can be rearranged
to solve for either inductance and capacitance as follows:
L 5
1
4π2
f 2
C
and C 5
1
4π2
f 2
L
For example, the capacitance that will resonate at a frequency of 18 MHz with a
12-µH inductor is determined as follows:
C 5
1
4π2
fr
2
L
5
1
39.478(18 3 106
)2
(12 3 1026
)
5
1
39.478(3.24 3 1014
)(12 3 1026
)
5 6.5 3 10212
F or 6.5 pF
Electronic Fundamentals for Communications 47
As indicated earlier, the basic deinition of resonance in a series tuned circuit is
the point at which XL equals XC. With this condition, only the resistance of the circuit
impedes the current. The total circuit impedance at resonance is Z 5 R. For this reason,
resonance in a series tuned circuit can also be deined as the point at which the circuit
impedance is lowest and the circuit current is highest. Since the circuit is resistive at
resonance, the current is in phase with the applied voltage. Above the resonant fre-
quency, the inductive reactance is higher than the capacitive reactance, and the induc-
tor voltage drop is greater than the capacitor voltage drop. Therefore, the circuit is
inductive, and the current will lag the applied voltage. Below resonance, the capacitive
reactance is higher than the inductive reactance; the net reactance is capacitive, thereby
producing a leading current in the circuit. The capacitor voltage drop is higher than
the inductor voltage drop.
The response of a series resonant circuit is illustrated in Fig. 2-15, which is a plot
of the frequency and phase shift of the current in the circuit with respect to frequency.
At very low frequencies, the capacitive reactance is much greater than the induc-
tive reactance; therefore, the current in the circuit is very low because of the high
impedance. In addition, because the circuit is predominantly capacitive, the current
leads the voltage by nearly 90°. As the frequency increases, XC goes down and XL
goes up. The amount of leading phase shift decreases. As the values of reactances
approach one another, the current begins to rise. When XL equals XC, their effects
cancel and the impedance in the circuit is just that of the resistance. This produces a
current peak, where the current is in phase with the voltage (0°). As the frequency
Example 2-15
What value of inductance will resonate with a 12-pF capacitor at 49 MHz?
L 5
1
4π2
fr
2
C
5
1
39.478(49 3 106
)2
(12 3 10212
)
5 8.79 3 1027
H or 879 nH
Figure 2-15 Frequency and phase response curves of a series resonant circuit.
Circuit
current
I
fr
Below resonance (capacitive) Above resonance (inductive)
I
␪
⫹90⬚ (lead)
0⬚
⫺90⬚ (lag)
Phase
shift
angle
(␪)
48 Chapter 2
continues to rise, XL becomes greater than XC. The impedance of the circuit increases
and the current decreases. With the circuit predominantly inductive, the current lags
the applied voltage. If the output voltage were being taken from across the resistor in
Fig. 2-13, the response curve and phase angle of the voltage would correspond to those
in Fig. 2-15. As Fig. 2-15 shows, the current is highest in a region centered on the
resonant frequency. The narrow frequency range over which the current is highest is
called the bandwidth. This area is illustrated in Fig. 2-16.
The upper and lower boundaries of the bandwidth are deined by two cutoff frequen-
cies designated f1 and f2. These cutoff frequencies occur where the current amplitude is
70.7 percent of the peak current. In the igure, the peak circuit current is 2 mA, and
the current at both the lower ( f1) and upper ( f2) cutoff frequency is 0.707 of 2 mA, or
1.414 mA.
Current levels at which the response is down 70.7 percent are called the half-power
points because the power at the cutoff frequencies is one-half the power peak of the
curve.
P 5 I2
R 5 (0.707 Ipeak)2
R 5 0.5 Ipeak
2
R
The bandwidth BW of the tuned circuit is deined as the difference between the
upper and lower cutoff frequencies:
BW 5 f2 2 f1
For example, assuming a resonant frequency of 75 kHz and upper and lower cutoff
frequencies of 76.5 and 73.5 kHz, respectively, the bandwidth is BW 5 76.5 2 73.5 5
3 kHz.
The bandwidth of a resonant circuit is determined by the Q of the circuit. Recall
that the Q of an inductor is the ratio of the inductive reactance to the circuit resistance.
This holds true for a series resonant circuit, where Q is the ratio of the inductive reactance
to the total circuit resistance, which includes the resistance of the inductor plus any
additional series resistance:
Q 5
XL
RT
Recall that bandwidth is then computed as
BW 5
fr
Q
If the Q of a circuit resonant at 18 MHz is 50, then the bandwidth is BW 5 18/50 5
0.36 MHz 5 360 kHz.
Bandwidth
Half-power points
Figure 2-16 Bandwidth of a series resonant circuit.
0.707Ipeak ⫽ 1.414 mA
Ipeak ⫽ 2 mA
f1 fr f2
BW = f2 ⫺ f1
Electronic Fundamentals for Communications 49
The formula can be rearranged to compute Q, given the frequency and the
bandwidth:
Q 5
fr
BW
Thus the Q of the circuit whose bandwidth was computed previously is Q 5
75 kHz/3kHz 5 25.
Since the bandwidth is approximately centered on the resonant frequency, f1 is the
same distance from fr as f2 is from fr. This fact allows you to calculate the resonant
frequency by knowing only the cutoff frequencies:
fr 5 2f1 3 f2
For example, if f1 5 175 kHz and f2 5 178 kHz, the resonant frequency is
fr 5 2175 3 103
3 178 3 103
5 176.5 kHz
For a linear frequency scale, you can calculate the center or resonant frequency by
using an average of the cutoff frequencies.
fr 5
f1 1 f2
2
If the circuit Q is very high (.100), then the response curve is approximately sym-
metric around the resonant frequency. The cutoff frequencies will then be roughly equi-
distant from the resonant frequency by the amount of BW/2. Thus the cutoff frequencies
can be calculated if the bandwidth and the resonant frequency are known:
f1 5 fr 2
BW
2
and f2 5 fr 1
BW
2
For instance, if the resonant frequency is 49 MHz (49,000 kHz) and the bandwidth
is 10 kHz, then the cutoff frequencies will be
f1 5 49,000 kHz 2
10k
2
5 49,000 kHz 2 5 kHz 5 48,995 kHz
f2 5 49,000 kHz 1 5 kHz 5 49,005 kHz
Keep in mind that although this procedure is an approximation, it is useful in many
applications.
The bandwidth of a resonant circuit deines its selectivity, i.e., how the circuit
responds to varying frequencies. If the response is to produce a high current only over
a narrow range of frequencies, a narrow bandwidth, the circuit is said to be highly selec-
tive. If the current is high over a broader range of frequencies, i.e., the bandwidth is
wider, the circuit is less selective. In general, circuits with high selectivity and narrow
bandwidths are more desirable. However, the actual selectivity and bandwidth of a circuit
must be optimized for each application.
Example 2-16
What is the bandwidth of a resonant circuit with a frequency of 28 MHz and a Q of 70?
BW 5
fr
Q
5
28 3 106
70
5 400,000 Hz 5 400 kHz
Selectivity
50 Chapter 2
The relationship between circuit resistance Q and bandwidth is extremely impor-
tant. The bandwidth of a circuit is inversely proportional to Q. The higher Q is, the
smaller the bandwidth. Low Qs produce wide bandwidths or less selectivity. In turn,
Q is a function of the circuit resistance. A low resistance produces a high Q, a nar-
row bandwidth, and a highly selective circuit. A high circuit resistance produces a
low Q, wide bandwidth, and poor selectivity. In most communication circuits, circuit
Qs are at least 10 and typically higher. In most cases, Q is controlled directly by the
resistance of the inductor. Fig. 2-17 shows the effect of different values of Q on
bandwidth.
Example 2-17
The upper and lower cutoff frequencies of a resonant circuit are found to be 8.07 and
7.93 MHz. Calculate (a) the bandwidth, (b) the approximate resonant frequency,
and (c) Q.
a. BW 5 f2 2 f1 5 8.07 MHz 2 7.93 MHz 5 0.14 MHz 5 140 kHz
b. fr 5 1f1 f2 5 1(8.07 3 106
) (7.93 3 106
) 5 8 MHz
c. Q 5
fr
BW
5
8 3 106
140 3 103
5 57.14
Example 2-18
What are the approximate 3-dB down frequencies of a resonant circuit with a Q of
200 at 16 MHz?
BW 5
fr
Q
5
16 3 106
200
5 80,000 Hz 5 80 kHz
f1 5 fr 2
BW
2
5 16,000,000 2
80,000
2
5 15.96 MHz
f2 5 fr 1
BW
2
5 16,000,000 1
80,000
2
5 16.04 MHz
Resonance produces an interesting but useful phenomenon in a series RLC circuit.
Consider the circuit in Fig. 2-18(a). At resonance, assume XL 5 XC 5 500 V. The total
circuit resistance is 10 V. The Q of the circuit is then
Q 5
XL
R
5
500
10
5 50
If the applied or source voltage Vs is 2 V, the circuit current at resonance will be
I 5
Vs
R
5
2
10
5 0.2 A
Electronic Fundamentals for Communications 51
When the reactances, the resistances, and the current are known, the voltage drops
across each component can be computed:
VL 5 IXL 5 0.2(500) 5 100 V
VC 5 IXC 5 0.2(500) 5 100 V
VR 5 IR 5 0.2(10) 5 2 V
As you can see, the voltage drops across the inductor and capacitor are signiicantly
higher than the applied voltage. This is known as the resonant step-up voltage. Although
the sum of the voltage drops around the series circuit is still equal to the source voltage,
at resonance the voltage across the inductor leads the current by 90° and the voltage across
the capacitor lags the current by 90° [see Fig. 2-18(b)]. Therefore, the inductive and reac-
tive voltages are equal but 180° out of phase. As a result, when added, they cancel each
other, leaving a total reactive voltage of 0. This means that the entire applied voltage
appears across the circuit resistance.
The resonant step-up voltage across the coil or capacitor can be easily computed by
multiplying the input or source voltage by Q:
VL 5 VC 5 QVs
In the example in Fig. 2-18, VL 5 50(2) 5 100 V.
Resonant step-up voltage
Figure 2-17 The efect of Q on bandwidth and selectivity in a resonant circuit.
fr
BW 1
⫺3 dB points
BW 2
BW 3
High Q1, narrow
bandwidth
Medium Q2,
medium bandwidth
Low Q3, wide
bandwidth
Gain, dB
Figure 2-18 Resonant step-up voltage in a series resonant circuit.
Vs⫽ 2 V
VC ⫽ 100 V
VL ⫽ 100 V
VL ⫽ 100 V
VR ⫽ Vs ⫽ 2 V
Equal and 180°
out of phase
I
VC ⫽ 100 V
VR ⫽ 2 V
XC ⫽ 500 ⍀
XL ⫽ 500 ⍀
R ⫽ 10 ⍀
I ⫽ 0.2 A
(a) (b)
52 Chapter 2
Parallel Resonant Circuits. A parallel resonant circuit is formed when the inductor
and capacitor are connected in parallel with the applied voltage, as shown in Fig. 2-19(a).
In general, resonance in a parallel tuned circuit can also be deined as the point at which
the inductive and capacitive reactances are equal. The resonant frequency is therefore
calculated by the resonant frequency formula given earlier. If we assume lossless compo-
nents in the circuit (no resistance), then the current in the inductor equals the current in
the capacitor:
IL 5 IC
Although the currents are equal, they are 180° out of phase, as the phasor diagram
in Fig. 2-19(b) shows. The current in the inductor lags the applied voltage by 90°, and
the current in the capacitor leads the applied voltage by 90°, for a total of 180°.
Now, by applying Kirchhoff’s current law to the circuit, the sum of the individual branch
currents equals the total current drawn from the source. With the inductive and capacitive
currents equal and out of phase, their sum is 0. Thus, at resonance, a parallel tuned circuit
appears to have ininite resistance, draws no current from the source and thus has ininite
impedance, and acts as an open circuit. However, there is a high circulating current between
the inductor and capacitor. Energy is being stored and transferred between the inductor and
capacitor. Because such a circuit acts as a kind of storage vessel for electric energy, it is
often referred to as a tank circuit and the circulating current is referred to as the tank current.
In a practical resonant circuit where the components do have losses (resistance), the
circuit still behaves as described above. Typically, we can assume that the capacitor has
practically zero losses and the inductor contains a resistance, as illustrated in Fig. 2-20(a).
At resonance, where XL 5 XC, the impedance of the inductive branch of the circuit is
higher than the impedance of the capacitive branch because of the coil resistance. The
capacitive current is slightly higher than the inductive current. Even if the reactances are
Parallel resonant circuit
Tank circuit
Tank current
Example 2-19
A series resonant circuit has a Q of 150 at 3.5 MHz. The applied voltage is 3 µV.
What is the voltage across the capacitor?
VC 5 QVs 5 150(3 3 1026
) 5 450 3 1026
5 450 µV
Figure 2-19 Parallel resonant circuit currents. (a) Parallel resonant circuit. (b) Current
relationships in parallel resonant circuit.
Vs
IC IL
Line current
IC
Vs
IL
⫺90°
⫹90°
(b)
(a)
冪苴苴苴苴苳
IT ⫽ (IL)2
⫹ (IC)2
This interesting and useful phenomenon means that small applied voltages can essen-
tially be stepped up to a higher voltage—a form of simple ampliication without active
circuits that is widely applied in communication circuits.
Electronic Fundamentals for Communications 53
equal, the branch currents will be unequal and therefore there will be some net current
low in the supply line. The source current will lead the supply voltage, as shown in
Fig. 2-20(b). Nevertheless, the inductive and capacitive currents in most cases will cancel
because they are approximately equal and of opposite phase, and consequently the line
or source current will be signiicantly lower than the individual branch currents. The
result is a very high resistive impedance, approximately equal to
Z 5
Vs
IT
The circuit in Fig. 2-20(a) is not easy to analyze. One way to simplify the mathematics
involved is to convert the circuit to an equivalent circuit in which the coil resistance is
translated to a parallel resistance that gives the same overall results, as shown in Fig. 2-21.
The equivalent inductance Leq and resistance Req are calculated with the formulas
Leq 5
L(Q2
1 1)
Q2
and Req 5 RW(Q2
1 1)
and Q is determined by the formula
Q 5
XL
RW
where RW is the coil winding resistance.
If Q is high, usually more than 10, Leq is approximately equal to the actual induc-
tance value L. The total impedance of the circuit at resonance is equal to the equivalent
parallel resistance:
Z 5 Req
Figure 2-20 A practical parallel resonant circuit. (a) Practical parallel resonant circuit
with coil resistance RW. (b) Phase relationships.
Vs IC
RW
IL
Line current
C
IT
(a)
L
IC
Vs
IL
IT
(b)
(Vector sum of IC and IL
leads Vs because IC ⬎ IL)
(lags Vs by less than
90° because of RW)
Figure 2-21 An equivalent circuit makes parallel resonant circuits easier to analyze.
C
C
L
RW
Req
Req = RW (Q 2 + 1)
Leq = L (Q 2 + 1)
Z = Req
Leq
Actual circuit Equivalent circuit
Q 2
Lossless
resonant circuit
54 Chapter 2
If the Q of the parallel resonant circuit is greater than 10, the following simpliied
formula can be used to calculate the resistive impedance at resonance:
Z 5
L
CRW
The value of RW is the winding resistance of the coil.
Example 2-20
What is the impedance of a parallel LC circuit with a resonant frequency of 52 MHz
and a Q of 12? L 5 0.15 µH.
Q 5
XL
RW
XL 5 2πfL 5 6.28(52 3 106
)(0.15 3 1026
) 5 49 V
RW 5
XL
Q
5
49
12
5 4.1 V
Z 5 Req 5 RW (Q2
1 1) 5 4.1(122
1 1) 5 4.1(145) 5 592 V
Example 2-21
Calculate the impedance of the circuit given in Example 2-20 by using the formula
Z 5 L/CR.
fr 5 52 MHz RW 5 4.1 V L 5 0.15 µH
C 5
1
4π2
fr
2
L
5
1
39.478(52 3 106
)2
(0.15 3 1026
)
5 6.245 3 10211
Z 5
L
CRW
5
0.15 3 1026
(62.35 3 10212
)(4.1)
5 586 V
This is close to the previously computed value of 592 V. The formula Z 5 L/CRW
is an approximation.
A frequency and phase response curve of a parallel resonant circuit is shown in
Fig. 2-22. Below the resonant frequency, XL is less than XC; thus the inductive current
is greater than the capacitive current, and the circuit appears inductive. The line current
lags the applied voltage. Above the resonant frequency, XC is less than XL; thus the
capacitive current is more than the inductive current, and the circuit appears capacitive.
Therefore, the line current leads the applied voltage. The phase angle of the impedance
will be leading below resonance and lagging above resonance.
At the resonant frequency, the impedance of the circuit peaks. This means that the
line current at that time is at its minimum. At resonance, the circuit appears to have a
very high resistance, and the small line current is in phase with the applied voltage.
GOOD TO KNOW
The bandwidth of a circuit is in-
versely proportional to the circuit Q.
The higher the Q, the smaller
the bandwidth. Low Q values
produce wide bandwidths or
less selectivity.
Electronic Fundamentals for Communications 55
Note that the Q of a parallel circuit, which was previously expressed as Q 5 XL/RW,
can also be computed with the expression
Q 5
RP
XL
where RP is the equivalent parallel resistance, Req in parallel with any other parallel
resistance, and XL is the inductive reactance of the equivalent inductance Leq.
You can set the bandwidth of a parallel tuned circuit by controlling Q. The Q can
be determined by connecting an external resistor across the circuit. This has the effect
of lowering RP and increasing the bandwidth.d
Figure 2-22 Response of a parallel resonant circuit.
Below
resonance
(inductive)
Above
resonance
(capacitive)
+90° (leading)
-90° (lagging)
Phase
shift
of
line
current
in
degrees
(red
curve
only)
0°
fr
Impedance
(blue
curve
only)
Z
Example 2-22
What value of parallel resistor is needed to set the bandwidth of a parallel tuned
circuit to 1 MHz? Assume XL 5 300 V, RW 5 10 V, and fr 5 10 MHz.
Q 5
XL
RW
5
300
10
5 30
RP 5 RW(Q2
1 1) 5 10(302
1 1) 5 10(901) 5 9010 V
(equivalent resistance of the parallel circuit at resonance)
BW 5
fr
Q
Q 5
fr
BW
5
10 MHz
1 MHz
5 10 (Q needed for 1-MHz bandwidth)
RPnew 5 QXL 5 10(300) 5 3000 V
(this is the total resistance of the circuit RPnew made up of the original RP and an
externally connected resistor Rext)
RPnew 5
RPRext
RP 1 Rext
Rext 5
RPnewRP
RP 2 RPnew
5
9010(3000)
9010 2 3000
5 4497.5V
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  • 1. 16 Chapter 1 Voice Frequencies. Voice frequencies (VFs) are in the range of 300 to 3000 Hz. This is the normal range of human speech. Although human hearing extends from approxi- mately 20 to 20,000 Hz, most intelligible sound occurs in the VF range. Very Low Frequencies. Very low frequencies (VLFs) extend from 9 kHz to 30 kHz and include the higher end of the human hearing range up to about 15 or 20 kHz. Many musical instruments make sounds in this range as well as in the ELF and VF ranges. The VLF range is also used in some government and military communication. For example, VLF radio transmission is used by the navy to communicate with submarines. Low Frequencies. Low frequencies (LFs) are in the 30- to 300-kHz range. The pri- mary communication services using this range are in aeronautical and marine navigation. Frequencies in this range are also used as subcarriers, signals that are modulated by the baseband information. Usually, two or more subcarriers are added, and the combination is used to modulate the final high-frequency carrier. Medium Frequencies. Medium frequencies (MFs) are in the 300- to 3000-kHz (0.3- to 3.0-MHz) range. The major application of frequencies in this range is AM radio broadcasting (535 to 1605 kHz). Other applications in this range are various marine and amateur radio communication. High Frequencies. High frequencies (HFs) are in the 3- to 30-MHz range. These are the frequencies generally known as short waves. All kinds of simplex broadcast- ing and half duplex two-way radio communication take place in this range. Broadcasts from Voice of America and the British Broadcasting Company occur in this range. Government and military services use these frequencies for two-way communication. An example is diplomatic communication between embassies. Amateur radio and CB communication also occur in this part of the spectrum. Very High Frequencies. Very high frequencies (VHFs) encompass the 30- to 300-MHz range. This popular frequency range is used by many services, including mobile radio, marine and aeronautical communication, FM radio broadcasting (88 to 108 MHz), and television channels 2 through 13. Radio amateurs also have numerous bands in this frequency range. Ultrahigh Frequencies. Ultrahigh frequencies (UHFs) encompass the 300- to 3000-MHz range. This, too, is a widely used portion of the frequency spectrum. It includes the UHF TV channels 14 through 51, and it is used for land mobile commu- nication and services such as cellular telephones as well as for military communication. Some radar and navigation services occupy this portion of the frequency spectrum, and radio amateurs also have bands in this range. Microwaves and SHFs. Frequencies between the 1000-MHz (1-GHz) and 30-GHz range are called microwaves. Microwave ovens usually operate at 2.45 GHz. Superhigh frequencies (SHFs) are in the 3- to 30-GHz range. These microwave frequencies are widely used for satellite communication and radar. Wireless local-area networks (LANs) and many cellular telephone systems also occupy this region. Extremely High Frequencies. Extremely high frequencies (EHFs) extend from 30 to 300 GHz. Electromagnetic signals with frequencies higher than 30 GHz are referred to as millimeter waves. Equipment used to generate and receive signals in this range is extremely complex and expensive, but there is growing use of this range for satellite communication telephony, computer data, short-haul cellular networks, and some specialized radar. Frequencies Between 300 GHz and the Optical Spectrum. This portion of the spectrum is virtually uninhabited. It is a cross between RF and optical. Lack of hardware and components limits its use. High frequency (HF) Voice frequency (VF) Very low frequency (VLF) Low frequency (LF) Medium frequency (MF) Subcarrier Very high frequency (VHF) Ultrahigh frequency (UHF) Microwave Superhigh frequency (SHF) Extremely high frequency (EHF) Millimeter wave
  • 2. Introduction to Electronic Communication 17 The Optical Spectrum Right above the millimeter wave region is what is called the optical spectrum, the region occupied by light waves. There are three different types of light waves: infrared, visible, and ultraviolet. Infrared. The infrared region is sandwiched between the highest radio frequencies (i.e., millimeter waves) and the visible portion of the electromagnetic spectrum. Infrared occupies the range between approximately 0.1 millimeter (mm) and 700 nanometers (nm), or 100 to 0.7 micrometer (μm). One micrometer is one-millionth of a meter. Infrared wavelengths are often given in micrometers or nanometers. Infrared radiation is generally associated with heat. Infrared is pro- duced by light-bulbs, our bodies, and any physical equipment that gen- erates heat. Infrared signals can also be generated by special types of light-emitting diodes (LEDs) and lasers. Infrared signals are used for various special kinds of communi- cation. For example, infrared is used in astronomy to detect stars and other physical bodies in the universe, and for guidance in weapons systems, where the heat radiated from airplanes or missiles can be picked up by infrared detectors and used to guide missiles to targets. Infrared is also used in most new TV remote-control units where special coded signals are transmitted by an infrared LED to the TV receiver for the purpose of changing channels, setting the volume, and performing other functions. Infrared is the basis for all iber- optic communication. Infrared signals have many of the same properties as signals in the visible spectrum. Optical devices such as lenses and mirrors are often used to process and manipulate infrared signals, and infrared light is the signal usually propagated over iber-optic cables. The Visible Spectrum. Just above the infrared region is the visible spectrum we ordinarily refer to as light. Light is a special type of electromagnetic radiation that has a wavelength in the 0.4- to 0.8-µm range (400 to 800 nm). Light wavelengths are usually expressed in terms of angstroms (Å). An angstrom is one ten-thousandth of a micrometer; for example, 1 Å 5 10210 m. The visible range is approximately 8000 Å (red) to 4000 Å (violet). Red is low-frequency or long-wavelength light, whereas violet is high-frequency or short-wavelength light. Light is used for various kinds of communication. Light waves can be modulated and transmitted through glass ibers, just as electric signals can be transmitted over wires. The great advantage of light wave signals is that their very high frequency gives them the ability to handle a tremendous amount of information. That is, the bandwidth of the baseband signals can be very wide. Light signals can also be transmitted through free space. Various types of commu- nication systems have been created using a laser that generates a light beam at a speciic visible frequency. Lasers generate an extremely narrow beam of light, which is easily modulated with voice, video, and data information. Ultraviolet. Ultraviolet light (UV) covers the range from about 4 to 400 nm. Ultravio- let generated by the sun is what causes sunburn. Ultraviolet is also generated by mercury vapor lights and some other types of lights such as fluorescent lamps and sun lamps. Ultraviolet is not used for communication; its primary use is medical. Beyond the visible region are the X-rays, gamma rays, and cosmic rays. These are all forms of electromagnetic radiation, but they do not igure into communication systems and are not covered here. The tablet computer has become a popular communications device thanks to Wi-Fi and cellular links. Optical spectrum Infrared region Visible spectrum Light Ultraviolet light (UV) GOOD TO KNOW Although it is expensive to build a fiber-optic or wireless network, servicing each additional user is cost-effective. The more users a network has, the lower the overall cost.
  • 3. 18 Chapter 1 1-6 Bandwidth Bandwidth (BW) is that portion of the electromagnetic spectrum occupied by a signal. It is also the frequency range over which a receiver or other electronic circuit operates. More speciically, bandwidth is the difference between the upper and lower frequency limits of the signal or the equipment operation range. Fig. 1-16 shows the bandwidth of the voice frequency range from 300 to 3000 Hz. The upper frequency is f2 and the lower frequency is f1. The bandwidth, then, is BW 5 f2 2 f1 Bandwidth (BW) Example 1-5 A commonly used frequency range is 902 to 928 MHz. What is the width of this band? f1 5 902 MHz f2 5 928 MHz BW 5 f2 2 f1 5 928 2 902 5 26 MHz Example 1-6 A television signal occupies a 6-MHz bandwidth. If the low-frequency limit of channel 2 is 54 MHz, what is the upper-frequency limit? BW 5 54 MHz f1 5 6 MHz BW 5 f1 2 f2 f2 5 BW 1 f1 5 6 1 54 5 60 MHz Bandwidth (BW) f1 ⫽ 300 Hz f2 ⫽ 3000 Hz Frequency spectrum BW ⫽ f2 ⫺ f1 ⫽ 3000 ⫺ 300 ⫽ 2700 Hz Figure 1-16 Bandwidth is the frequency range over which equipment operates or that portion of the spectrum occupied by the signal. This is the voice frequency bandwidth. Sideband Channel Bandwidth When information is modulated onto a carrier somewhere in the electromagnetic spectrum, the resulting signal occupies a small portion of the spectrum surrounding the carrier fre- quency. The modulation process causes other signals, called sidebands, to be generated at
  • 4. Introduction to Electronic Communication 19 frequencies above and below the carrier frequency by an amount equal to the modulating frequency. For example, in AM broadcasting, audio signals up to 5 kHz can be transmit- ted. If the carrier frequency is 1000 kHz, or 1 MHz, and the modulating frequency is 5 kHz, sidebands will be produced at 1000 2 5 5 995 kHz and at 1000 1 5 5 1005 kHz. In other words, the modulation process generates other signals that take up spectrum space. It is not just the carrier at 1000 kHz that is transmitted. Thus the term bandwidth refers to the range of frequencies that contain the information. The term channel bandwidth refers to the range of frequencies required to transmit the desired information. The bandwidth of the AM signal described above is the difference between the high- est and lowest transmitting frequencies: BW 5 1005 kHz 2 995 kHz 5 10 kHz. In this case, the channel bandwidth is 10 kHz. An AM broadcast signal, therefore, takes up a 10-kHz piece of the spectrum. Signals transmitting on the same frequency or on overlapping frequencies do, of course, interfere with one another. Thus a limited number of signals can be transmitted in the fre- quency spectrum. As communication activities have grown over the years, there has been a continuous demand for more frequency channels over which communication can be trans- mitted. This has caused a push for the development of equipment that operates at the higher frequencies. Prior to World War II, frequencies above 1 GHz were virtually unused, since there were no electronic components suitable for generating signals at those frequencies. But technological developments over the years have given us many microwave components such as klystrons, magnetrons, and traveling-wave tubes, and today transistors, integrated circuits, and other semiconductor devices that routinely work in the microwave range. More Room at the Top The beneit of using the higher frequencies for communication carriers is that a signal of a given bandwidth represents a smaller percentage of the spectrum at the higher frequen- cies than at the lower frequencies. For example, at 1000 kHz, the 10-kHz-wide AM signal discussed earlier represents 1 percent of the spectrum: % of spectrum 5 10 kHz 1000 KHz 3 100 5 1% But at 1 GHz, or 1,000,000 kHz, it represents only one-thousandth of 1 percent: % of spectrum 5 10 kHz 1,000,000 kHz 3 100 5 0.001% In practice, this means that there are many more 10-kHz channels at the higher frequencies than at the lower frequencies. In other words, there is more spectrum space for information signals at the higher frequencies. The higher frequencies also permit wider-bandwidth signals to be used. A TV signal, e.g., occupies a bandwidth of 6 MHz. Such a signal cannot be used to modulate a carrier in the MF or HF ranges because it would use up all the available spectrum space. Television signals are transmitted in the VHF and UHF portions of the spectrum, where suficient space is available. Today, virtually the entire frequency spectrum between approximately 30 kHz and 30 GHz has been spoken for. Some open areas and portions of the spectrum are not heavily used, but for the most part, the spectrum is illed with communication activities of all kinds generated from all over the world. There is tremendous competition for these frequencies, not only between companies, individuals, and government services in individual carriers but also between the different nations of the world. The electromagnetic spectrum is one of our most precious natural resources. Because of this, communication engineering is devoted to making the best use of that inite spectrum. A considerable amount of effort goes into developing communication techniques that will minimize the bandwidth required to transmit given information and thus conserve spectrum space. Channel bandwidth GOOD TO KNOW The Federal Communications Commission (FCC) was formed in 1934 to regulate interstate and foreign communication. A primary function of the FCC is to allocate bands of frequencies and set limitations on broadcast power for different types of radio and TV operations. The FCC also monitors broadcasts to detect unlicensed operations and technical violations. In addition to TV and radio stations, the FCC licenses about 50 million transmitters operated by individuals, businesses, ships and airplanes, emergency services, and telephone systems. FCC policy is set by five commissioners who are appointed by the President for five-year terms.
  • 5. 20 Chapter 1 This provides more room for additional communication channels and gives other ser- vices or users an opportunity to take advantage of it. Many of the techniques discussed later in this book evolved in an effort to minimize transmission bandwidth. Spectrum Management Governments of the United States and other countries recognized early on that the fre- quency spectrum was a valuable and inite natural resource and so set up agencies to control spectrum use. In the United States, Congress passed the Communications Act of 1934. This Act and its various amendments established regulations for the use of spec- trum space. It also established the Federal Communications Commission (FCC), a regu- latory body whose function is to allocate spectrum space, issue licenses, set standards, and police the airwaves. The Telecommunications Act of 1996 has also greatly inluenced the use of spectrum. The FCC controls all telephone and radio communications in this country and, in general, regulates all electromagnetic emissions. The National Telecom- munications and Information Administration (NTIA) performs a similar function for government and military services. Other countries have similar organizations. The International Telecommunications Union (ITU), an agency of the United Nations that is headquartered in Geneva, Switzerland, comprises 189 member countries that meet at regular intervals to promote cooperation and negotiate national interests. Typical of these meetings are the World Administrative Radio Conferences, held approximately every two years. Various committees of the ITU set standards for various areas within the communication ield. The ITU brings together the various countries to discuss how the frequency spectrum is to be divided up and shared. Because many of the signals generated in the spectrum do not carry for long distances, countries can use these frequencies simultaneously without interference. On the other hand, some ranges of the frequency spectrum can literally carry signals around the world. As a result, countries must negotiate with one another to coordinate usage of various por- tions of the high-frequency spectrum to prevent mutual interference. Standards Standards are speciications and guidelines that companies and individuals follow to ensure compatibility between transmitting and receiving equipment in communication systems. Although the concepts of communication are simple, there are obviously many ways to send and receive information. A variety of methods are used to modulate, mul- tiplex, and otherwise process the information to be transmitted. If each system used different methods created at the whim of the designing engineer, the systems would be incompatible with one another and no communication could take place. In the real world, standards are set and followed so that when equipment is designed and built, compatibil- ity is ensured. The term used to describe the ability of equipment from one manufacturer to work compatibly with that of another is interoperability. Standards are detailed outlines of principles of operation, blueprints for construction, and methods of measurement that deine communication equipment. Some of the specii- cations covered are modulation methods, frequency of operation, multiplexing methods, word length and bit formats, data transmission speeds, line coding methods, and cable and connector types. These standards are set and maintained by numerous nonproit organiza- tions around the world. Committees made up of individuals from industry and academia meet to establish and agree upon the standards, which are then published for others to use. Other committees review, revise, and enhance the standards over time, as needs change. In working in the communication ield, you will regularly encounter many different stan- dards. For example, there are standards for long-distance telephone transmission, digital cell phones, local-area networks, and computer modems. Listed below are organizations that main- tain standards for communication systems. For more details, go to the corresponding website. American National Standards Institute (ANSI)—www.ansi.org Electronic Industries Alliance (EIA)—www.eia.org National Telecommunications and Information Administration (NTIA) International Telecommunications Union (ITU) Standards Interoperability
  • 6. Introduction to Electronic Communication 21 European Telecommunications Standards Institute (ETSI)—www.etsi.org Institute of Electrical and Electronics Engineers (IEEE)—www.ieee.org International Telecommunications Union (ITU)—www.itu.org Internet Engineering Task Force (IETF)—www.ietf.org Optical Internetworking Forum (IF)—www.oiforum.com Telecommunications Institute of America (TIA)—www.tiaonline.org 1-7 A Survey of Communication Applications The applications of electronic techniques to communication are so common and pervasive that you are already familiar with most of them. You use the telephone, listen to the radio, and watch TV. You also use other forms of electronic communication, such as cellular telephones, ham radios, CB and Family radios, home wireless networks for Internet access, texting, electronic mail, and remote-control garage door openers. Fig. 1-17 lists all the various major applications of electronic communication. SIMPLEX (ONE-WAY) 1. AM and FM radio broadcasting. Stations broadcast music, news, weather reports, and programs for entertainment and information. It includes shortwave. 2. Digital radio. There is both satellite and terrestrial. Radio programming is transmitted in digital format. 3. TV broadcasting. Stations broadcast entertainment, informational, and educational programs by radio. 4. Digital television (DTV). Radio transmission of television programming is performed by digital methods, both satellite and terrestrial, e.g., high- deinition television (HDTV) and Internet Protocol Television (IPTV). 5. Cable television. Movies, sports events, and other programs are distributed to subscribers by iber-optic and coaxial cable. 6. Facsimile. Printed visual material is transmitted over telephone lines. A facsimile, or fax, machine scans a document and converts it to electronic signals that are sent over the telephone system for reproduction in printed form by another fax machine. Faxes can also be sent from a computer. 7. Wireless remote control. This category includes a device that controls any remote item by radio or infrared. Examples are missiles, satellites, robots, toys, and other vehicles or remote plants or stations. A remote keyless entry device, garage door opener, and the remote control on your TV set are other examples. 8. Internet of Things (IoT). The monitoring or control of remote devices, appliances, and other items in a home, ofice or other facility is usually accomplished by a combination of wireless and Internet connectivity. 9. Navigation and direction-finding services. Special stations transmit signals that can be picked up by receivers for the purpose of identifying exact location (latitude and longitude) or determining direction and/ or distance from a station. Such systems employ both land-based and satellite stations. The services are used primarily by boats and ships or airplanes, although systems for cars and trucks are being developed. The Global Positioning System (GPS) which uses 24 satellites is the most widely used. 10. Telemetry. Measurements are transmitted over a long distance. Telemetry systems use sensors to deter- mine physical conditions (temperature, pressure, low rate, voltages, frequency, etc.) at a remote location. The sensors modulate a carrier signal that is sent by wire or radio to a remote receiver that stores and/or displays the data for analysis. Examples are satel- lites, rockets, pipelines, plants, and factories. Figure 1-17 Applications of electronic communication. (continues on next page)
  • 7. 22 Chapter 1 11. Radio astronomy. Radio signals, including infrared, are emitted by virtually all heavenly bodies such as stars and planets. With the use of large directional antennas and sensitive high-gain receivers, these signals may be picked up and used to plot star locations and study the universe. Radio astronomy is an alternative and supplement to traditional optical astronomy. 12. Surveillance. Surveillance means discreet monitoring or “spying.” Electronic techniques are widely used by police forces, governments, the military, business and industry, and others to gather information for the purpose of gaining some competitive advantage. Techniques include phone taps, tiny wireless “bugs,” clandestine listening stations, and reconnaissance airplanes and satellites. 13. Music services. Continuous background music is transmitted for doctors’ ofices, stores, elevators, and so on by local FM radio stations on special high-frequency subcarriers that cannot be picked up by conventional FM receivers. 14. Internet radio and video. Music and video are delivered on a computer via the Internet. DUPLEX (TWO-WAY) 15. Telephones. One-on-one verbal communication is transmitted over the vast worldwide telephone networks employing wire, iber optics, radio, and satellites. a. Cordless telephones provide short-distance wireless communication for cord-free convenience. b. Cell phones provide worldwide wireless communi- cations via handsets and base stations and the wired telephone system. In addition to voice communications, cell phones facilitate e-mail, Internet access, instant message service, video, and games. c. Internet telephones, known as voice over the Internet protocol (VoIP) phones, use high-speed broadband services (cable, DSL, wireless, iber) over the Internet to provide digital voice communications. d. Satellite phones use low-earth-orbit satellites to give worldwide voice service from any remote location on earth. 16. Two-way radio. Commercial, industrial, and government communication is transmitted between vehicles, handheld units, and base stations. Examples include police, ire, taxi, forestry service, trucking companies, aircraft, marine, military, and government. 17. Radar. This special form of communication makes use of relected microwave signals for the purpose of detecting ships, planes, and missiles and for determining their range, direction, and speed. Most radar is used in military applications, but civil- ian aircraft and marine services also use it. Police use radar in speed detection and enforcement. 18. Sonar. In underwater communication, audible base- band signals use water as the transmission medium. Submarines and ships use sonar to detect the presence of enemy submarines. Passive sonar uses audio receivers to pick up water, propeller, and other noises. Active sonar is like an underwater radar with which relections from a transmitted ultrasonic pulse are used to determine the direction, range, and speed of an underwater target. 19. Amateur radio. This is a hobby for individuals interested in radio communication. Individuals may become licensed “hams” to build and operate two- way radio equipment for personal communication with other hams. 20. Citizens radio. Citizens band (CB) radio is a special service that any individual may use for personal communication with others. Most CB radios are used in trucks and cars for exchanging information about trafic conditions, speed traps, and emergencies. 21. Family Radio Service. This is a two-way personal communication with handheld units over short distances (, 2 mi). 22. The Internet. Worldwide interconnections via iber- optic networks, telecommunications companies, cable TV companies, Internet service providers, and others provide World Wide Web (WWW) access to millions of websites and pages and electronic mail (e-mail). 23. Wide-Area Networks (WANs). Worldwide iber-optic networks provide long-distance telephone and Internet services. 24. Metropolitan-area networks (MANs). Networks of com- puters transmit over a speciic geographic area such as a college campus, company facility, or city. Nor- mally they are implemented with iber-optic cable, but may also be coaxial cable or wireless. 25. Local-area networks (LANs). Wired (or wireless) interconnections of personal computers (PCs), laptops, servers, or mainframe computers within an ofice or building for the purpose of e-mail, Internet access, or the sharing of mass storage, peripherals, data, and software. Figure 1-17 (continued)
  • 8. Introduction to Electronic Communication 23 1-8 Jobs and Careers in the Communication Industry The electronics industry is roughly divided into four major specializations. The largest in terms of people employed and the dollar value of equipment purchased is the com- munications ield, closely followed by the computer ield. The industrial control and instrumentation ields are considerably smaller. Hundreds of thousands of employees are in the communication ield, and billions of dollars’ worth of equipment is purchased each year. The growth rate varies from year to year depending upon the economy, techno- logical developments, and other factors. But, as in most areas in electronics, the communication ield has grown steadily over the years thanks to the Internet and the exploding cellular industry, creating a relatively constant opportunity for employment. If your interests lie in communication, you will be glad to know that there are many oppor- tunities for long-term jobs and careers. The next section outlines the types of jobs avail- able and the major kinds of employers. Types of Jobs The two major types of technical positions available in the communication ield are engineer and technician. Engineers. Engineers design communication equipment and systems. They have bachelor’s (B.S.E.E.), master’s (M.S.E.E.), or doctoral (Ph.D.) degrees in electrical engineering, giving them a strong science and mathematics background combined with specialized education in electronic circuits and equipment. Engineers work from speci- fications and create new equipment or systems, which are then manufactured. Many engineers have a bachelor’s degree in electronics technology from a technical college or university. Some typical degree titles are bachelor of technology (B.T.), bach- elor of engineering technology (B.E.T.), and bachelor of science in engineering technol- ogy (B.S.E.T.). Bachelor of technology programs are sometimes extensions of two-year associate degree programs. In the two additional years required for a bachelor of technology degree, the student takes more complex electronics courses along with additional sci- ence, math, and humanities courses. The main difference between the B.T. graduate and the engineering graduate is that the technologist usually takes courses that are more practical and hands-on than engineering courses. Holders of B.T. degrees can generally design electronic equipment and systems but do not typically have the depth of back- ground in analytical mathematics or science that is required for complex design jobs. However, B.T. graduates are generally employed as engineers. Although many do design work, others are employed in engineering positions in manufacturing and ield service rather than design. Some engineers specialize in design; others work in manufacturing, testing, quality control, and management, among other areas. Engineers may also serve as ield service personnel, installing and maintaining complex equipment and systems. If your interest lies in the design of communication equipment, then an engineering position may be for you. Although a degree in electrical engineering is generally the minimum entrance requirement for engineers’ jobs in most organizations, people with other educational backgrounds (e.g., physics and math) do become engineers. Technicians who obtain suficient additional education and appropriate experience may go on to become engineers. Technicians. Technicians have some kind of postsecondary education in electronics, from a vocational or technical school, a community college, or a technical institute. Many technicians are educated in military training programs. Most technicians have Engineer Technician
  • 9. 24 Chapter 1 an average of two years of formal post–high school education and an associate degree. Common degrees are associate in arts (A.A.), associate in science (A.S.) or associate of science in engineering technology or electronic engineering technology (A.S.E.T. or A.S.E.E.T.), and associate in applied science (A.A.S.). The A.A.S. degrees tend to cover more occupational and job-related subjects; the A.A. and A.S. degrees are more general and are designed to provide a foundation for transfer to a bachelor’s degree program. Technicians with an associate degree from a community college can usually transfer to a bachelor of technology program and complete the bachelor’s degree in another two years. However, associate degree holders are usually not able to transfer to an engineering degree program but must literally start over if the engineering career path is chosen. Technicians are most often employed in service jobs. The work typically involves equipment installation, troubleshooting and repair, testing and measuring, maintenance and adjustment, or operation. Technicians in such positions are sometimes called ield service technicians, ield service engineers, or customer representatives. Technicians can also be involved in engineering. Engineers may use one or more technicians to assist in the design of equipment. They build and troubleshoot pro- totypes and in many cases actually participate in equipment design. A great deal of the work involves testing and measuring. In this capacity, the technician is known as an engineering technician, lab technician, engineering assistant, or associate engineer. Technicians are also employed in manufacturing. They may be involved in the actual building and assembling of the equipment, but more typically are concerned with inal testing and measurement of the inished products. Other positions involve quality control or repair of defective units. Other Positions. There are many jobs in the communication industry other than those of engineer or technician. For example, there are many outstanding jobs in technical sales. Selling complex electronic communication equipment often requires a strong technical education and background. The work may involve determining cus- tomer needs and related equipment specifications, writing technical proposals, making sales presentations to customers, and attending shows and exhibits where equipment is sold. The pay potential in sales is generally much higher than in the engineering or service positions. Another position is that of technical writer. Technical writers generate the technical documentation for communication equipment and systems, producing installation and service manuals, maintenance procedures, and customer operations manuals. This impor- tant task requires considerable depth of education and experience. Finally, there is the position of trainer. Engineers and technicians are often used to train other engineers and technicians or customers. With the high degree of com- plexity that exists in communication equipment today, there is a major need for training. Many individuals ind education and training positions to be very desirable and satisfying. The work typically involves developing curriculum and programs, gen- erating the necessary training manuals and presentation materials, creating online training, and conducting classroom training sessions in-house or at a customer site. Major Employers The overall structure of the communication electronics industry is shown in Fig. 1-18. The four major segments of the industry are manufacturers, resellers, service organizations, and end users. Manufacturers. It all begins, of course, with customer needs. Manufacturers translate customer needs into products, purchasing components and materials from other elec- tronics companies to use in creating the products. Engineers design the products, and
  • 10. Introduction to Electronic Communication 25 Figure 1-18 Structure of the communication electronics industry. End users Service organizations Resellers Products and services Products and services Manufacturers Components Materials manufacturing produces them. There are jobs for engineers, technicians, salespeople, field service personnel, technical writers, and trainers. Resellers. Manufacturers who do not sell products directly to end users sell the prod- ucts to reselling organizations, which in turn sell them to the end user. For example, a manufacturer of marine communication equipment may not sell directly to a boat owner but instead to a regional distributor or marine electronics store or shop. This shop not only sells the equipment but also takes care of installation, service, and repairs. A cel- lular telephone or fax machine manufacturer also typically sells to a distributor or dealer who takes care of sales and service. Most of the jobs available in the reselling segment of the industry are in sales, service, and training. Service Organizations. These companies usually perform some kind of service, such as repair, installation, or maintenance. One example is an avionics company that does installation or service work on electronic equipment for private planes. Another is a sys- tems integrator, a company that designs and assembles a piece of communication equipment or more often an entire system by using the products of other companies. Systems integrators put together systems to meet special needs and customize existing systems for particular jobs. Other types of service organization are the communications services providers like cellular network carriers (e.g., AT&T, Verizon), Internet providers, cable TV companies, and Internet web companies (e.g., Google, Yahoo, Amazon). Most communication technicians perform installation, maintenance, and troubleshooting.
  • 11. 26 Chapter 1 End Users. The end user is the ultimate customer—and a major employer. Today, almost every person and organization is an end user of communication equipment. The major categories of end users in the communication field are: Telephone companies Radio users—mobile, marine, aircraft, etc. Radio and TV broadcast stations and cable TV companies Business and industry users of satellites, networks, etc. Transportation companies (airlines, shipping, railroads) Government and military Internet companies Personal and hobby Consumers There are an enormous number of communication jobs with end users. Most are of the service type: installation, repair, maintenance, and operation of equipment. Licensing and Certification A good way to validate your knowledge of communications electronics is to obtain a relevant license or certiication. Some jobs require an FCC license to ensure your com- petence in electronics and knowledge of the related rules and regulations. Otherwise, the main beneit of a license or certiication is to prove your knowledge and skills to a prospective employer. Such a credential is an added bonus to any A.A.S. or B.S.E.T. degree you may get. For some employers, a license or certiication may be acceptable in lieu of a degree. Licensing and certiication typically require taking an exam on communications topics. The FCC exam includes tests on rules and regulations as well as electronic fundamentals and communications circuits, equipment, and practices. Most certiica- tions also have exams that cover the same electronic fundamentals and communications circuits, equipment, and practices. Some certiications require a speciic amount of job experience. Listed below are some of the licenses and certiications available for communications. • FCC General Radiotelephone Operators License (GROL)—Two-part exam on rules and regulations and communications electronics. An optional exam on radar is avail- able. No job experience is required. • International Society of Certiied of Electronic Technicians (ISCET)—This organiza- tion offers several basic certiications in electronic fundamentals as well as a journey- man certiication in a variety of electronic specializations including communications. No job experience is required. • Electronic Technicians Association International (ETA-I)—This organization offers a wide range of certiications on electronics with specializations in electronic fun- damentals, communications, radar, iber optics, and several others. • The International Association for Radio, Telecommunications and Electromagnetics (iNARTE)—This organization offers multiple certiications in all phases of com- munications, including telecommunications, electromagnetic compatibility, and wireless devices at both the technician and the engineering level. These certiications require various education levels (degrees) and job experience as well as exams. • Cisco—This company is a major supplier of networking and wireless equipment and offers certiications in many networking-related areas. An example is the Cisco Cer- tiied Network Associate (CCNA) Wireless. Cisco certiication is widely recognized throughout industry. There are other certiications for a variety of specialties that you will discover. Many of the certifying organizations, such as ETA-I, ISCET, and iNARTE, are also granted
  • 12. Introduction to Electronic Communication 27 CHAPTER REVIEW Online Activity 1-1 Exploring the Regulatory Agencies Objective: Become familiar with the FCC and NTIA. Procedure: 1. Go to the FCC website at www.fcc.gov. 2. Explore the website. 3. Go to the NTIA website at www.nita.doc.gov. 4. Explore the website. 5. Use these websites and their search feature to answer the questions below. Questions: 1. To whom does the FCC report within the government? 2. To whom does the NTIA report within the government? 3. What is the purpose and function of the FCC? 4. What is the purpose and function of the NTIA? 5. What is the FCC Code of Federal Regulations (CFR) Title 47? 6. On the NTIA website, locate the large colorful fre- quency spectrum chart. Examine it to see what ser- vices are identiied and where they are located. Is the chart available as a wall chart for purchase? 1-2 Examining FCC Rules and Regulations Objective: Investigate FCC CFR Title 47 and ind answers to electronic communication rules and regulations. Procedure: 1. Go to the FCC website www.fcc.gov. 2. Click on the rules and regulations link on the left. 3. Access FCC CFR Title 47. 4. Study the different parts. 5. Use this reference to answer the questions below. Questions: 1. What is contained in Subpart A of Part 2 that may be useful? 2. In Part 2, what communications services can occupy the spectrum from 108 to 138 MHz? 3. What part pertains to commercial operators’ licenses? 4. Describe briely what is in Part 15. 5. Describe briely what is in Part 18. 6. Which part covers TV broadcasting? 7. What part covers radar? 8. What parts cover Citizens’ Band radio and the Family Radio Service? State the frequency bands of each. 9. Is cable TV regulated by the FCC? Which part if so? 10. List all of the modes and modulation methods allowed by amateur radio operation. 11. Which part covers RF interference and electromag- netic compatibility? 12. Which parts cover cell phones and wireless local area networks? authority to give the FCC GROL exams. The GROL is probably the best overall credential to have for wireless jobs, and you may wish to complement it with a certiication appro- priate to the work you are seeking. Certiication and licensing is an excellent way to prove to yourself and any employer that you are knowledgeable and competent in communications. Give serious consideration to this opportunity. 1-3 Investigate Licensing and Certification Objective: To learn more about the beneits of licensing and certiication and how to obtain them. Procedure: 1. Go to the FCC website www.fcc.gov. 2. On the FCC site, locate the information on commercial operators’ licenses (GROL). 3. Go to each of the following websites and investigate these major certiication sources: a. International Society of Certiied Electronic Technicians—www.iset.org. b. Electronic Technician Association International— www.eta-i.org.
  • 13. 28 Chapter 1 Questions 1. In what century did electronic communication begin? 2. Name the four main elements of a communication system, and draw a diagram that shows their relationship. 3. List ive types of media used for communication, and state which three are the most commonly used. 4. Name the device used to convert an information sig- nal to a signal compatible with the medium over which it is being transmitted. 5. What piece of equipment acquires a signal from a communication medium and recovers the original in- formation signal? 6. What is a transceiver? 7. What are two ways in which a communication me- dium can affect a signal? 8. What is another name for communication medium? 9. What is the name given to undesirable interference that is added to a signal being transmitted? 10. Name three common sources of interference. 11. What is the name given to the original information or intelligence signals that are transmitted directly via a communication medium? 12. Name the two forms in which intelligence signals can exist. 13. What is the name given to one-way communication? Give three examples. 14. What is the name given to simultaneous two-way communication? Give three examples. 15. What is the term used to describe two-way communi- cation in which each party takes turns transmitting? Give three examples. 16. What type of electronic signals are continuously vary- ing voice and video signals? 17. What are on/off intelligence signals called? 18. How are voice and video signals transmitted digitally? 19. What terms are often used to refer to original voice, video, or data signals? 20. What technique must sometimes be used to make an information signal compatible with the medium over which it is being transmitted? 21. What is the process of recovering an original signal called? 22. What is a broadband signal? 23. Name the process used to transmit two or more base- band signals simultaneously over a common medium. 24. Name the technique used to extract multiple intelli- gence signals that have been transmitted simultane- ously over a single communication channel. 25. What is the name given to signals that travel through free space for long distances? 26. What does a radio wave consist of? 27. Calculate the wavelength of signals with frequencies of 1.5 kHz, 18 MHz, and 22 GHz in miles, feet, and centimeters, respectively. 28. Why are audio signals not transmitted directly by electromagnetic waves? 29. What is the human hearing frequency range? 30. What is the approximate frequency range of the hu- man voice? 31. Do radio transmissions occur in the VLF and LF ranges? 32. What is the frequency range of AM radio broadcast stations? 33. What is the name given to radio signals in the high-frequency range? 34. In what segment of the spectrum do TV channels 2 to 13, and FM broadcasting, appear? 35. List ive major uses of the UHF band. 36. What are frequencies above 1 GHz called? 37. What are the frequencies just above the EHF range called? 38. What is a micrometer, and what is it used to measure? 39. Name the three segments of the optical frequency spectrum. 40. What is a common source of infrared signals? 41. What is the approximate spectrum range of infrared signals? 42. Deine the term angstrom and explain how it is used. 43. What is the wavelength range of visible light? 44. Which two channels or media do light signals use for electronic communication? 45. Name two methods of transmitting visual data over a telephone network. 46. What is the name given to the signaling of individuals at remote locations by radio? c. The International Association for Radio, Telecommu- nications and Electromagnetics—www.narte.org. 4. Check out the certiication options at Cisco at www. cisco.com. 5. Answer the questions below. Questions: 1. What is the GROL and who is required to have one? 2. What is the procedure for getting a GROL? 3. List any available supplements to the GROL. 4. List the basic requirements for a communications- related certiication from each of the organizations listed above. Which one appeals to you most? 5. Which certiication requires education and job experi- ence qualiications?
  • 14. Introduction to Electronic Communication 29 47. What term is used to describe the process of making measurements at a distance? 48. List four ways radio is used in the telephone system. 49. What principle is used in radar? 50. What is underwater radar called? Give two examples. 51. What is the name of a popular radio communication hobby? 52. What device enables computers to exchange digital data over the telephone network? 53. What do you call the systems of interconnections of PCs and other computers in ofices or buildings? 54. What is a generic synonym for radio? 55. Name the three main types of technical positions available in the communication ield. 56. What is the main job of an engineer? 57. What is the primary degree for an engineer? 58. What is the primary degree for a technician? 59. Name a type of technical degree in engineering other than engineer or technician. 60. Can the holder of an associate of technology degree trans- fer the credits to an engineering degree program? 61. What types of work does a technician ordinarily do? 62. List three other types of jobs in the ield of electronic communication that do not involve engineering or technician’s work. 63. What are the four main segments of the communica- tion industry? Explain briely the function of each. 64. Why are standards important? 65. What types of characteristics do communication stan- dards deine? 1. Calculate the frequency of signals with wavelengths of 40 m, 5 m, and 8 cm. ◆ 2. In what frequency range does the common ac power line frequency fall? 3. What is the primary use of the SHF and EHF ranges? ◆ ◆ Answers to Selected Problems follow Chap. 22. 1. Name three ways that a higher-frequency signal called the carrier can be varied to transmit the intelligence. 2. Name two common household remote-control units, and state the type of media and frequency ranges used for each. 3. How is radio astronomy used to locate and map stars and other heavenly bodies? 4. In what segment of the communication ield are you interested in working, and why? 5. Assume that all the electromagnetic spectrum from ELF through microwaves was fully occupied. Explain some ways that communication capability could be added. 6. What is the speed of light in feet per microsecond? In inches per nanosecond? In meters per second? 7. Make a general statement comparing the speed of light with the speed of sound. Give an example of how the principles mentioned might be demonstrated. 8. List ive real-life communication applications not speciically mentioned in this chapter. 9. “Invent” ive new communication methods, wired or wireless, that you think would be practical. 10. Assume that you have a wireless application you would like to design, build, and sell as a commercial product. You have selected a target frequency in the UHF range. How would you decide what frequency to use, and how would you get permission to use it? 11. Make an exhaustive list of all the electronic communi- cation products that you own, have access to at home or in the ofice, and/or use on a regular basis. 12. You have probably seen or heard of a simple commu- nication system made of two paper cups and a long piece of string. How could such a simple system work? Problems Critical Thinking
  • 15. 30 chapter 2 Electronic Fundamentals for Communications To understand communication electronics as presented in this book, you need a knowledge of certain basic principles of electronics, including the fundamentals of alternating-current (ac) and direct-current (dc) circuits, semiconductor operation and characteristics, and basic electronic circuit operation (amplifiers, oscillators, power supplies, and digital logic circuits). Some of the basics are particularly critical to understanding the chapters that follow. These include the expression of gain and loss in decibels, LC tuned circuits, resonance and filters, and Fourier theory. The purpose of this chapter is to briefly review all these subjects. If you have studied the material before, it will simply serve as a review and reference. If, because of your own schedule or the school’s curriculum, you have not previously covered this material, use this chapter to learn the necessary information before you continue. Objectives After completing this chapter, you will be able to: ■ Calculate voltage, current, gain, and attenuation in decibels and apply these formulas in applications involving cascaded circuits. ■ Explain the relationship between Q, resonant frequency, and bandwidth. ■ Describe the basic configuration of the diferent types of filters that are used in communication networks and compare and contrast active filters with passive filters. ■ Explain how using switched capacitor filters enhances selectivity. ■ Explain the benefits and operation of crystal, ceramic, and SAW filters. ■ Calculate bandwidth by using Fourier analysis.
  • 16. Electronic Fundamentals for Communications 31 2-1 Gain, Attenuation, and Decibels Most electronic circuits in communication are used to process signals, i.e., to manipulate signals to produce a desired result. All signal processing circuits involve either gain or attenuation. Gain Gain means ampliication. If a signal is applied to a circuit such as the ampliier shown in Fig. 2-1 and the output of the circuit has a greater amplitude than the input signal, the circuit has gain. Gain is simply the ratio of the output to the input. For input (Vin) and output (Vout) voltages, voltage gain AV is expressed as follows: AV 5 output input 5 Vout Vin The number obtained by dividing the output by the input shows how much larger the output is than the input. For example, if the input is 150 µV and the output is 75 mV, the gain is AV 5 (75 3 1023 )y(150 3 1026 ) 5 500. The formula can be rearranged to obtain the input or the output, given the other two variables: Vout 5 Vin 3 AV and Vin 5 Vout/AV. If the output is 0.6 V and the gain is 240, the input is Vin 5 0.6/240 5 2.5 3 1023 5 2.5 mV. Gain Vin Input signal A ⫽ gain ⫽ Vout Output signal Amplifier Vout Vin Figure 2-1 An amplifier has gain. Example 2-1 What is the voltage gain of an ampliier that produces an output of 750 mV for a 30-µV input? AV 5 Vout Vin 5 750 3 1023 30 3 1026 5 25,000 Example 2-2 The power output of an ampliier is 6 watts (W). The power gain is 80. What is the input power? AP 5 Pout Pin therefore Pin 5 Pout AP Pin 5 6 80 5 0.075 W 5 75 mW Since most ampliiers are also power ampliiers, the same procedure can be used to calculate power gain AP: AP 5 Pout Pin where Pin is the power input and Pout is the power output.
  • 17. 32 Chapter 2 When two or more stages of ampliication or other forms of signal processing are cascaded, the overall gain of the combination is the product of the individual circuit gains. Fig. 2-2 shows three ampliiers connected one after the other so that the output of one is the input to the next. The voltage gains of the individual circuits are marked. To ind the total gain of this circuit, simply multiply the individual circuit gains: AT 5 A1 3 A2 3 A3 5 5 3 3 3 4 5 60. If an input signal of 1 mV is applied to the irst ampliier, the output of the third ampliier will be 60 mV. The outputs of the individual ampliiers depend upon their individual gains. The output voltage from each ampliier is shown in Fig. 2-2. Figure 2-2 Total gain of cascaded circuits is the product of individual stage gains. Vin ⫽ 1 mV 5 mV 15 mV Vout ⫽ 60 mV A1 ⫽ 5 AT ⫽ A1 ⫻ A2 ⫻ A3 ⫽ 5 ⫻ 3 ⫻ 4 ⫽ 60 A2 ⫽ 3 A3 ⫽ 4 Example 2-3 Three cascaded ampliiers have power gains of 5, 2, and 17. The input power is 40 mW. What is the output power? AP 5 A1 3 A2 3 A3 5 5 3 2 3 17 5 170 AP 5 Pout Pin therefore Pout 5 APPin Pout 5 170(40 3 1023 ) 5 6.8 W Example 2-4 A two-stage ampliier has an input power of 25 µW and an output power of 1.5 mW. One stage has a gain of 3. What is the gain of the second stage? AP 5 Pout Pin 5 1.5 3 1023 25 3 1026 5 60 AP 5 A1 3 A2 If A1 5 3, then 60 5 3 3 A2 and A2 5 60y3 5 20.
  • 18. Electronic Fundamentals for Communications 33 Attenuation Attenuation refers to a loss introduced by a circuit or component. Many electronic circuits, sometimes called stages, reduce the amplitude of a signal rather than increase it. If the output signal is lower in amplitude than the input, the circuit has loss, or attenuation. Like gain, attenuation is simply the ratio of the output to the input. The letter A is used to represent attenuation as well as gain: Attenuation A 5 output input 5 Vout Vin Circuits that introduce attenuation have a gain that is less than 1. In other words, the output is some fraction of the input. An example of a simple circuit with attenuation is a voltage divider such as that shown in Fig. 2-3. The output voltage is the input voltage multiplied by a ratio based on the resistor values. With the resistor values shown, the gain or attenuation factor of the circuit is A 5 R2/(R1 1 R2) 5 100/(200 1 100) 5 100/300 5 0.3333. If a signal of 10 V is applied to the attenuator, the output is Vout 5 Vin A 5 10(0.3333) 5 3.333 V. When several circuits with attenuation are cascaded, the total attenuation is, again, the product of the individual attenuations. The circuit in Fig. 2-4 is an example. The attenuation factors for each circuit are shown. The overall attenuation is AT 5 A1 3 A2 3 A3 With the values shown in Fig. 2-4, the overall attenuation is AT 5 0.2 3 0.9 3 0.06 5 0.0108 Given an input of 3 V, the output voltage is Vout 5 ATVin 5 0.0108(3) 5 0.0324 5 32.4 mV R1 ⫽ 200 ⍀ R2 ⫽ 100 ⍀ Vout ⫽ Vin Vin R2 R1 ⫹ R2 A ⫽ ⫽ ⫽ R2 R1 ⫹ R2 100 0.3333 300 Figure 2-3 A voltage divider introduces attenuation. Figure 2-4 Total attenuation is the product of individual attenuations of each cascaded circuit. Loss stage AT ⫽ A1 ⫻ A2 ⫻ A3 ⫽ 0.2 ⫻ 0.9 ⫻ 0.06 ⫽ 0.0108 Vout ⫽ ATVin ⫽ 0.0324 ⫽ 32.4 mV A1 ⫽ 0.2 A2 ⫽ 0.9 A3 ⫽ 0.06 Vin ⫽ 3 V Vout Loss circuit Loss component Attenuation
  • 19. 34 Chapter 2 It is common in communication systems and equipment to cascade circuits and components that have gain and attenuation. For example, loss introduced by a circuit can be compensated for by adding a stage of ampliication that offsets it. An example of this is shown in Fig. 2-5. Here the voltage divider introduces a 4-to-1 voltage loss, or an attenuation of 0.25. To offset this, it is followed with an ampliier whose gain is 4. The overall gain or attenuation of the circuit is simply the product of the attenuation and gain factors. In this case, the overall gain is AT 5 A1A2 5 0.25(4) 5 1. Another example is shown in Fig. 2-6, which shows two attenuation circuits and two ampliier circuits. The individual gain and attenuation factors are given. The overall circuit gain is AT 5 A1 A2 A3 A4 5 (0.1)(10)(0.3)(15) 5 4.5. For an input voltage of 1.5 V, the output voltage at each circuit is shown in Fig. 2-6. In this example, the overall circuit has a net gain. But in some instances, the overall circuit or system may have a net loss. In any case, the overall gain or loss is obtained by multiplying the individual gain and attenuation factors. Figure 2-5 Gain exactly ofsets the attenuation. Vin 750 ⍀ 250 ⍀ A2 ⫽ 4 A1 ⫽ AT ⫽ A1A2 ⫽ 0.25(4) ⫽ 1 Vout ⫽ Vin 250 750 ⫹ 250 A1 ⫽ 250 1000 ⫽ 0.25 Example 2-5 A voltage divider such as that shown in Fig. 2-5 has values of R1 5 10 kV and R2 5 470 V. a. What is the attenuation? A1 5 R2 R1 1 R2 5 470 10,470 A1 5 0.045 b. What amplifier gain would you need to offset the loss for an overall gain of 1? AT 5 A1A2 where A1 is the attenuation and A2 is the amplifier gain. 1 5 0.045A2 A2 5 1 0.045 5 22.3 Note: To ind the gain that will offset the loss for unity gain, just take the reciprocal of attenuation: A2 5 1yA1.
  • 20. Electronic Fundamentals for Communications 35 Decibels The gain or loss of a circuit is usually expressed in decibels (dB), a unit of measurement that was originally created as a way of expressing the hearing response of the human ear to various sound levels. A decibel is one-tenth of a bel. When gain and attenuation are both converted to decibels, the overall gain or atten- uation of an electronic circuit can be computed by simply adding the individual gains or attenuations, expressed in decibels. It is common for electronic circuits and systems to have extremely high gains or attenuations, often in excess of 1 million. Converting these factors to decibels and using logarithms result in smaller gain and attenuation igures, which are easier to use. Decibel Calculations. The formulas for computing the decibel gain or loss of a circuit are dB 5 20 log Vout Vin (1) dB 5 20 log Iout Iin (2) dB 5 10 log Pout Pin (3) Formula (1) is used for expressing the voltage gain or attenuation of a circuit; for- mula (2), for current gain or attenuation. The ratio of the output voltage or current to the input voltage or current is determined as usual. The base-10 or common log of the input/output ratio is then obtained and multiplied by 20. The resulting number is the gain or attenuation in decibels. Figure 2-6 The total gain is the product of the individual stage gains and attenuations. Loss stage Loss stage Vin ⫽ 1.5 V A1 ⫽ 0.1 A2 ⫽ 10 A3 ⫽ 0.3 A4 ⫽ 15 AT ⫽ A1A2A3A4 ⫽ (0.1)(10)(0.3)(15) ⫽ 4.5 0.15 V 1.5 V 0.45 V Vout ⫽ 6.75 V Example 2-6 An ampliier has a gain of 45,000, which is too much for the application. With an input voltage of 20 µV, what attenuation factor is needed to keep the output voltage from exceeding 100 mV? Let A1 5 ampliier gain 5 45,000; A2 5 attenuation factor; AT 5 total gain. AT 5 Vout Vin 5 100 3 1023 20 3 1026 5 5000 AT 5 A1A2 therefore A2 5 AT A1 5 5000 45,000 5 0.1111 Decibel (dB)
  • 21. 36 Chapter 2 Formula (3) is used to compute power gain or attenuation. The ratio of the power output to the power input is computed, and then its logarithm is multiplied by 10. Example 2-7 a. An amplifier has an input of 3 mV and an output of 5 V. What is the gain in decibels? dB 5 20 log 5 0.003 5 20 log 1666.67 5 20(3.22) 5 64.4 b. A filter has a power input of 50 mW and an output of 2 mW. What is the gain or attenuation? dB 5 10 log 2 50 5 10 log 0.04 5 10(21.398) 5 213.98 Note that when the circuit has gain, the decibel igure is positive. If the gain is less than 1, which means that there is an attenuation, the decibel igure is negative. Now, to calculate the overall gain or attenuation of a circuit or system, you simply add the decibel gain and attenuation factors of each circuit. An example is shown in Fig. 2-7, where there are two gain stages and an attenuation block. The overall gain of this circuit is AT 5 A1 1 A2 1 A3 5 15 2 20 1 35 5 30 dB Decibels are widely used in the expression of gain and attenuation in communication circuits. The table on the next page shows some common gain and attenuation factors and their corresponding decibel igures. Ratios less than 1 give negative decibel values, indicating attenuation. Note that a 2:1 ratio represents a 3-dB power gain or a 6-dB voltage gain. Antilogs. To calculate the input or output voltage or power, given the decibel gain or attenuation and the output or input, the antilog is used. The antilog is the number obtained when the base is raised to the logarithm, which is the exponent: dB 5 10 log Pout Pin and dB 10 5 log Pout Pin and Pout Pin 5 antilog dB 10 5 log21 dB 10 The antilog is simply the base 10 raised to the dB/10 power. Antilog Figure 2-7 Total gain or attenuation is the algebraic sum of the individual stage gains in decibels. AT ⫽ A1 ⫹ A2 ⫹ A3 AT ⫽ 15 ⫺ 20 ⫹ 35 ⫽ 30 dB A1 ⫽ 15 dB A2 ⫽ ⫺20 dB A3 ⫽ 35 dB Loss stage
  • 22. Electronic Fundamentals for Communications 37 Remember that the logarithm y of a number N is the power to which the base 10 must be raised to get the number. N 5 10y and y 5 log N Since dB 5 10 log Pout Pin dB 10 5 log Pout Pin Therefore Pout Pin 5 10dB/10 5 log21 dB 10 The antilog is readily calculated on a scientiic calculator. To ind the antilog for a common or base-10 logarithm, you normally press the Inv or 2nd function key on the calculator and then the log key. Sometimes the log key is marked with 10x , which is the antilog. The antilog with base e is found in a similar way, by using the Inv or 2nd function on the In key. It is sometimes marked ex , which is the same as the antilog. d B G A I N O R A T T E N U A T I O N Ratio (Power or Voltage) Power Voltage 0.000001 260 2120 0.00001 250 2100 0.0001 240 280 0.001 230 260 0.01 220 240 0.1 210 220 0.5 23 26 1 0 0 2 3 6 10 10 20 100 20 40 1000 30 60 10,000 40 80 100,000 50 100
  • 23. 38 Chapter 2 Example 2-8 A power ampliier with a 40-dB gain has an output power of 100 W. What is the input power? dB 5 10 log Pout Pin antilog 5 log21 dB 10 5 log Pout Pin 40 10 5 log Pout Pin 4 5 log Pout Pin antilog 4 5 antilog alog Pout Pin b log21 4 5 Pout Pin Pout Pin 5 104 5 10,000 Pin 5 Pout 10,000 5 100 10,000 5 0.01 W 5 10 mW Example 2-9 An ampliier has a gain of 60 dB. If the input voltage is 50 µV, what is the output voltage? Since dB 5 20 log Vout Vin dB 20 5 log Vout Vin Therefore Vout Vin 5 log21 dB 20 510dB/20 Vout Vin 5 1060/20 5 103 Vout Vin 5 103 5 1000 Vout 5 1000Vin 5 1000 (50 3 1026 ) 5 0.05 V 5 50 mV
  • 24. Electronic Fundamentals for Communications 39 dBm. When the gain or attenuation of a circuit is expressed in decibels, implicit is a comparison between two values, the output and the input. When the ratio is computed, the units of voltage or power are canceled, making the ratio a dimensionless, or relative, figure. When you see a decibel value, you really do not know the actual voltage or power values. In some cases, this is not a problem; in others, it is useful or necessary to know the actual values involved. When an absolute value is needed, you can use a reference value to compare any other value. An often used reference level in communication is 1 mW. When a decibel value is computed by comparing a power value to 1 mW, the result is a value called the dBm. It is computed with the standard power decibel formula with 1 mW as the denominator of the ratio: dBm 5 10 log Pout(W) 0.001(W) Here Pout is the output power, or some power value you want to compare to 1 mW, and 0.001 is 1 mW expressed in watts. The output of a 1-W ampliier expressed in dBm is, e.g., dBm 5 10 log 1 0.001 5 10 log 1000 5 10(3) 5 30 dBm Sometimes the output of a circuit or device is given in dBm. For example, if a micro- phone has an output of 250 dBm, the actual output power can be computed as follows: 250 dBm 5 10 log Pout 0.001 250 dBm 10 5 log Pout 0.001 Therefore Pout 0.001 5 10250 dBm/10 5 1025 5 0.00001 Pout 5 0.001 3 0.00001 5 1023 3 1025 5 1028 W 5 10 3 1029 5 10 nW Example 2-10 A power ampliier has an input of 90 mV across 10 kV. The output is 7.8 V across an 8-V speaker. What is the power gain, in decibels? You must compute the input and output power levels irst. P 5 V2 R Pin 5 (90 3 1023 )2 104 5 8.1 3 1027 W Pout 5 (7.8)2 8 5 7.605 W AP 5 Pout Pin 5 7.605 8.1 3 1027 5 9.39 3 106 AP (dB) 5 10 log AP 5 10 log 9.39 3 106 5 69.7 dB GOOD TO KNOW From the standpoint of sound measurement, 0 dB is the least perceptible sound (hearing threshold), and 120 dB equals the pain threshold of sound. This list shows intensity levels for com- mon sounds. (Tippens, Physics, 6th ed., Glencoe/McGraw-Hill, 2001, p. 497) Intensity Sound level, dB Hearing threshold 0 Rustling leaves 10 Whisper 20 Quiet radio 40 Normal conversation 65 Busy street corner 80 Subway car 100 Pain threshold 120 Jet engine 140–160 Reference value dBm
  • 25. 40 Chapter 2 dBc. This is a decibel gain attenuation figure where the reference is the carrier. The carrier is the base communication signal, a sine wave that is modulated. Often the ampli- tude’s sidebands, spurious or interfering signals, are referenced to the carrier. For exam- ple, if the spurious signal is 1 mW compared to the 10-W carrier, the dBc is dBc 5 10 log Psignal Pcarrier dBc 5 10 log 0.001 10 5 10(24) 5 240 Example 2-11 An ampliier has a power gain of 28 dB. The input power is 36 mW. What is the output power? Pout Pin 5 10dBy10 5 102.8 5 630.96 Pout 5 630.96Pin 5 630.96(36 3 1023 ) 5 22.71 W Example 2-12 A circuit consists of two ampliiers with gains of 6.8 and 14.3 dB and two ilters with attenuations of 216.4 and 22.9 dB. If the output voltage is 800 mV, what is the input voltage? AT 5 A1 1 A2 1 A3 1 A4 5 6.8 1 14.3 2 16.4 2 2.9 5 1.8 dB AT 5 Vout Vin 5 10dBy20 5 101.8y20 5 100.09 Vout Vin 5 100.09 5 1.23 Vin 5 Vout 1.23 5 800 1.23 5 650.4 mV Example 2-13 Express Pout 5 12.3 dBm in watts. Pout 0.001 5 10dBmy10 5 1012.3y10 5 101.23 5 17 Pout 5 0.001 3 17 5 17 mW
  • 26. Electronic Fundamentals for Communications 41 2-2 Tuned Circuits Virtually all communication equipment contains tuned circuits, circuits made up of inductors and capacitors that resonate at speciic frequencies. In this section, you will review how to calculate the reactance, resonant frequency, impedance, Q, and bandwidth of series and parallel resonance circuits. Reactive Components All tuned circuits and many ilters are made up of inductive and capacitive elements, including discrete components such as coils and capacitors and the stray and distributed inductance and capacitance that appear in all elec- tronic circuits. Both coils and capacitors offer an opposition to alternating- current low known as reactance, which is expressed in ohms (abbreviated Ω). Like resistance, reactance is an opposition that directly affects the amount of current in a circuit. In addition, reactive effects produce a phase shift between the currents and voltages in a circuit. Capacitance causes the current to lead the applied voltage, whereas inductance causes the current to lag the applied voltage. Coils and capacitors used together form tuned, or resonant, circuits. Capacitors. A capacitor used in an ac circuit continually charges and dis- charges. A capacitor tends to oppose voltage changes across it. This translates to an opposition to alternating current known as capacitive reactance XC. The reactance of a capacitor is inversely proportional to the value of capacitance C and operating frequency f. It is given by the familiar expression XC 5 1 2πfC The reactance of a 100-pF capacitor at 2 MHz is XC 5 1 6.28(2 3 106 )(100 3 10212 ) 5 796.2 V The formula can also be used to calculate either frequency or capacitance depending on the application. These formulas are f 5 1 2πXCC and C 5 1 2πf XC The wire leads of a capacitor have resistance and inductance, and the dielectric has leakage that appears as a resistance value in parallel with the capacitor. These character- istics, which are illustrated in Fig. 2-8, are sometimes referred to as residuals or parasit- ics. The series resistance and inductance are very small, and the leakage resistance is Tuned circuit Chip capacitors. Reactance Capacitor Capacitive reactance Residual GOOD TO KNOW Stray and distributed capaci- tances and inductances can greatly alter the operation and performance of a circuit. Figure 2-8 What a capacitor looks like at high frequencies. R Rleakage C Lead inductance R L L Lead resistance
  • 27. 42 Chapter 2 very high, so these factors can be ignored at low frequencies. At radio frequencies, however, these residuals become noticeable, and the capacitor functions as a complex RLC circuit. Most of these effects can be greatly minimized by keeping the capacitor leads very short. This problem is mostly eliminated by using the newer chip capacitors, which have no leads as such. Capacitance is generally added to a circuit by a capacitor of a speciic value, but capacitance can occur between any two conductors separated by an insulator. For exam- ple, there is capacitance between the parallel wires in a cable, between a wire and a metal chassis, and between parallel adjacent copper patterns on a printed-circuit board. These are known as stray, or distributed, capacitances. Stray capacitances are typically small, but they cannot be ignored, especially at the high frequencies used in communica- tion. Stray and distributed capacitances can signiicantly affect the performance of a circuit. Inductors. An inductor, also called a coil or choke, is simply a winding of multiple turns of wire. When current is passed through a coil, a magnetic ield is produced around the coil. If the applied voltage and current are varying, the magnetic ield alternately expands and collapses. This causes a voltage to be self-induced into the coil winding, which has the effect of opposing current changes in the coil. This effect is known as inductance. The basic unit of inductance is the henry (H). Inductance is directly affected by the physical characteristics of the coil, including the number of turns of wire in the induc- tor, the spacing of the turns, the length of the coil, the diameter of the coil, and the type of magnetic core material. Practical inductance values are in the millihenry (mH 5 1023 H), microhenry (µH 5 1026 H), and nanohenry (nH 5 1029 H) regions. Fig. 2-9 shows several different types of inductor coils. ● Fig. 2-9(a) is an inductor made of a heavy, self-supporting wire coil. ● In Fig. 2-9(b) the inductor is formed of a copper spiral that is etched right onto the board itself. ● In Fig. 2-9(c) the coil is wound on an insulating form containing a powdered iron or ferrite core in the center, to increase its inductance. ● Fig. 2-9(d) shows another common type of inductor, one using turns of wire on a toroidal or doughnut-shaped form. ● Fig. 2-9(e) shows an inductor made by placing a small ferrite bead over a wire; the bead effectively increases the wire’s small inductance. ● Fig. 2-9( f ) shows a chip inductor. It is typically no more than 1 ⁄8 to 1 ⁄4 in long. A coil is contained within the body, and the unit is soldered to the circuit board with the end connections. These devices look exactly like chip resistors and capacitors. In a dc circuit, an inductor will have little or no effect. Only the ohmic resistance of the wire affects current low. However, when the current changes, such as during the time the power is turned off or on, the coil will oppose these changes in current. When an inductor is used in an ac circuit, this opposition becomes continuous and constant and is known as inductive reactance. Inductive reactance XL is expressed in ohms and is calculated by using the expression XL 5 2πfL For example, the inductive reactance of a 40-µH coil at 18 MHz is XL 5 6.28(18 3 106 )(40 3 1026 ) 5 4522 V In addition to the resistance of the wire in an inductor, there is stray capacitance between the turns of the coil. See Fig. 2-10(a). The overall effect is as if a small capac- itor were connected in parallel with the coil, as shown in Fig. 2-10(b). This is the equivalent circuit of an inductor at high frequencies. At low frequencies, capacitance may be Stray (or distributed) capacitance Inductor (coil or choke) Inductance Inductive reactance
  • 28. Electronic Fundamentals for Communications 43 ignored, but at radio frequencies, it is suficiently large to affect circuit operation. The coil then functions not as a pure inductor, but as a complex RLC circuit with a self- resonating frequency. Any wire or conductor exhibits a characteristic inductance. The longer the wire, the greater the inductance. Although the inductance of a straight wire is only a fraction of Figure 2-9 Types of inductors. (a) Heavy self-supporting wire coil. (b) Inductor made as copper pattern. (c) Insulating form. (d) Toroidal inductor. (e) Ferrite bead inductor. (f ) Chip inductor. (a) Printed circuit (PC) board Component lead or wire (e) Ferrite bead Insulating form Core moves in or out to vary inductance Powdered iron or ferrite core (c) (b) PC board Toroidal inductor Turns of wire (d ) (f ) Toroidal core Body Solder connection Figure 2-10 Equivalent circuit of an inductor at high frequencies. (a) Stray capacitance between turns. (b) Equivalent circuit of an inductor at high frequencies. Stray capacitance between turns Winding (coil) resistance L ⫽ inductor C ⫽ stray capacitance (a) (b) R
  • 29. 44 Chapter 2 a microhenry, at very high frequencies the reactance can be signiicant. For this reason, it is important to keep all lead lengths short in interconnecting components in RF circuits. This is especially true of capacitor and transistor leads, since stray or distributed induc- tance can signiicantly affect the performance and characteristics of a circuit. Another important characteristic of an inductor is its quality factor Q, the ratio of inductive power to resistive power: Q 5 I2 XL I2 R 5 XL R This is the ratio of the power returned to the circuit to the power actually dissipated by the coil resistance. For example, the Q of a 3-µH inductor with a total resistance of 45V at 90 MHz is calculated as follows: Q 5 2πfL R 5 6.28(90 3 106 )(3 3 1026 ) 45 5 1695.6 45 5 37.68 Resistors. At low frequencies, a standard low-wattage color-coded resistor offers nearly pure resistance, but at high frequencies its leads have considerable inductance, and stray capacitance between the leads causes the resistor to act as a complex RLC circuit, as shown in Fig. 2-11. To minimize the inductive and capacitive effects, the leads are kept very short in radio applications. The tiny resistor chips used in surface-mount construction of the electronic circuits preferred for radio equipment have practically no leads except for the metallic end pieces soldered to the printed-circuit board. They have virtually no lead inductance and little stray capacitance. Many resistors are made from a carbon-composition material in powdered form sealed inside a tiny housing to which leads are attached. The type and amount of carbon material determine the value of these resistors. They contribute noise to the circuit in which they are used. The noise is caused by thermal effects and the granular nature of the resistance material. The noise contributed by such resistors in an ampliier used to amplify very low level radio signals may be so high as to obliterate the desired signal. To overcome this problem, ilm resistors were developed. They are made by depos- iting a carbon or metal ilm in spiral form on a ceramic form. The size of the spiral and the kind of metal ilm determine the resistance value. Carbon ilm resistors are quieter than carbon-composition resistors, and metal ilm resistors are quieter than carbon ilm resistors. Metal ilm resistors should be used in ampliier circuits that must deal with very low level RF signals. Most surface-mount resistors are of the metallic ilm type. Skin Efect. The resistance of any wire conductor, whether it is a resistor or capacitor lead or the wire in an inductor, is primarily determined by the ohmic resistance of the wire itself. However, other factors inluence it. The most signiicant one is skin effect, the tendency of electrons lowing in a conductor to low near and on the outer surface Quality factor Q Resistor Skin effect Figure 2-11 Equivalent circuit of a resistor at high (radio) frequencies. Resistor Lead inductance Stray capacitance
  • 30. Electronic Fundamentals for Communications 45 of the conductor frequencies in the VHF, UHF, and microwave regions (Fig. 2-12). This has the effect of greatly decreasing the total cross-sectional area of the conductor, thus increasing its resistance and signiicantly affecting the performance of the circuit in which the conductor is used. For example, skin effect lowers the Q of an inductor at the higher frequencies, causing unexpected and undesirable effects. Thus many high-frequency coils, particularly those in high-powered transmitters, are made with cop- per tubing. Since current does not low in the center of the conductor, but only on the surface, tubing provides the most eficient conductor. Very thin conductors, such as a copper pattern on a printed-circuit board, are also used. Often these conductors are sil- ver- or gold-plated to further reduce their resistance. Tuned Circuits and Resonance A tuned circuit is made up of inductance and capacitance and resonates at a speciic frequency, the resonant frequency. In general, the terms tuned circuit and resonant circuit are used interchangeably. Because tuned circuits are frequency-selective, they respond best at their resonant frequency and at a narrow range of frequencies around the resonant frequency. Series Resonant Circuits. A series resonant circuit is made up of inductance, capacitance, and resistance, as shown in Fig. 2-13. Such circuits are often referred to as LCR circuits or RLC circuits. The inductive and capacitive reactances depend upon the frequency of the applied voltage. Resonance occurs when the inductive and capacitive reactances are equal. A plot of reactance versus frequency is shown in Fig. 2-14, where fr is the resonant frequency. Tuned (resonant) circuit Series resonant circuit LCR circuit RLC circuit Figure 2-12 Skin efect increases wire and inductor resistance at high frequencies. Electrons flow on or near surface No current flow in center of wire Wire Figure 2-13 Series RLC circuit. VL Vs XL XC VR R VC Figure 2-14 Variation of reactance with frequency. Reactance Frequency XC XL XL ⫽ XC fr
  • 31. 46 Chapter 2 The total impedance of the circuit is given by the expression Z 5 2R2 1 (XL 2 XC)2 When XL equals XC, they cancel each other, leaving only the resistance of the circuit to oppose the current. At resonance, the total circuit impedance is simply the value of all series resistances in the circuit. This includes the resistance of the coil and the resistance of the component leads, as well as any physical resistor in the circuit. The resonant frequency can be expressed in terms of inductance and capacitance. A formula for resonant frequency can be easily derived. First, express XL and XC as an equivalence: XL 5 XC. Since XL 5 2πfr L and XC 5 1 2πfr C we have 2πfr L 5 1 2πfrC Solving for fr gives fr 5 1 2π1LC In this formula, the frequency is in hertz, the inductance is in henrys, and the capacitance is in farads. Example 2-14 What is the resonant frequency of a 2.7-pF capacitor and a 33-nH inductor? fr 5 1 2π1LC 5 1 6.28233 3 1029 3 2.7 3 10212 5 5.33 3 108 Hz or 533 MHz It is often necessary to calculate capacitance or inductance, given one of those val- ues and the resonant frequency. The basic resonant frequency formula can be rearranged to solve for either inductance and capacitance as follows: L 5 1 4π2 f 2 C and C 5 1 4π2 f 2 L For example, the capacitance that will resonate at a frequency of 18 MHz with a 12-µH inductor is determined as follows: C 5 1 4π2 fr 2 L 5 1 39.478(18 3 106 )2 (12 3 1026 ) 5 1 39.478(3.24 3 1014 )(12 3 1026 ) 5 6.5 3 10212 F or 6.5 pF
  • 32. Electronic Fundamentals for Communications 47 As indicated earlier, the basic deinition of resonance in a series tuned circuit is the point at which XL equals XC. With this condition, only the resistance of the circuit impedes the current. The total circuit impedance at resonance is Z 5 R. For this reason, resonance in a series tuned circuit can also be deined as the point at which the circuit impedance is lowest and the circuit current is highest. Since the circuit is resistive at resonance, the current is in phase with the applied voltage. Above the resonant fre- quency, the inductive reactance is higher than the capacitive reactance, and the induc- tor voltage drop is greater than the capacitor voltage drop. Therefore, the circuit is inductive, and the current will lag the applied voltage. Below resonance, the capacitive reactance is higher than the inductive reactance; the net reactance is capacitive, thereby producing a leading current in the circuit. The capacitor voltage drop is higher than the inductor voltage drop. The response of a series resonant circuit is illustrated in Fig. 2-15, which is a plot of the frequency and phase shift of the current in the circuit with respect to frequency. At very low frequencies, the capacitive reactance is much greater than the induc- tive reactance; therefore, the current in the circuit is very low because of the high impedance. In addition, because the circuit is predominantly capacitive, the current leads the voltage by nearly 90°. As the frequency increases, XC goes down and XL goes up. The amount of leading phase shift decreases. As the values of reactances approach one another, the current begins to rise. When XL equals XC, their effects cancel and the impedance in the circuit is just that of the resistance. This produces a current peak, where the current is in phase with the voltage (0°). As the frequency Example 2-15 What value of inductance will resonate with a 12-pF capacitor at 49 MHz? L 5 1 4π2 fr 2 C 5 1 39.478(49 3 106 )2 (12 3 10212 ) 5 8.79 3 1027 H or 879 nH Figure 2-15 Frequency and phase response curves of a series resonant circuit. Circuit current I fr Below resonance (capacitive) Above resonance (inductive) I ␪ ⫹90⬚ (lead) 0⬚ ⫺90⬚ (lag) Phase shift angle (␪)
  • 33. 48 Chapter 2 continues to rise, XL becomes greater than XC. The impedance of the circuit increases and the current decreases. With the circuit predominantly inductive, the current lags the applied voltage. If the output voltage were being taken from across the resistor in Fig. 2-13, the response curve and phase angle of the voltage would correspond to those in Fig. 2-15. As Fig. 2-15 shows, the current is highest in a region centered on the resonant frequency. The narrow frequency range over which the current is highest is called the bandwidth. This area is illustrated in Fig. 2-16. The upper and lower boundaries of the bandwidth are deined by two cutoff frequen- cies designated f1 and f2. These cutoff frequencies occur where the current amplitude is 70.7 percent of the peak current. In the igure, the peak circuit current is 2 mA, and the current at both the lower ( f1) and upper ( f2) cutoff frequency is 0.707 of 2 mA, or 1.414 mA. Current levels at which the response is down 70.7 percent are called the half-power points because the power at the cutoff frequencies is one-half the power peak of the curve. P 5 I2 R 5 (0.707 Ipeak)2 R 5 0.5 Ipeak 2 R The bandwidth BW of the tuned circuit is deined as the difference between the upper and lower cutoff frequencies: BW 5 f2 2 f1 For example, assuming a resonant frequency of 75 kHz and upper and lower cutoff frequencies of 76.5 and 73.5 kHz, respectively, the bandwidth is BW 5 76.5 2 73.5 5 3 kHz. The bandwidth of a resonant circuit is determined by the Q of the circuit. Recall that the Q of an inductor is the ratio of the inductive reactance to the circuit resistance. This holds true for a series resonant circuit, where Q is the ratio of the inductive reactance to the total circuit resistance, which includes the resistance of the inductor plus any additional series resistance: Q 5 XL RT Recall that bandwidth is then computed as BW 5 fr Q If the Q of a circuit resonant at 18 MHz is 50, then the bandwidth is BW 5 18/50 5 0.36 MHz 5 360 kHz. Bandwidth Half-power points Figure 2-16 Bandwidth of a series resonant circuit. 0.707Ipeak ⫽ 1.414 mA Ipeak ⫽ 2 mA f1 fr f2 BW = f2 ⫺ f1
  • 34. Electronic Fundamentals for Communications 49 The formula can be rearranged to compute Q, given the frequency and the bandwidth: Q 5 fr BW Thus the Q of the circuit whose bandwidth was computed previously is Q 5 75 kHz/3kHz 5 25. Since the bandwidth is approximately centered on the resonant frequency, f1 is the same distance from fr as f2 is from fr. This fact allows you to calculate the resonant frequency by knowing only the cutoff frequencies: fr 5 2f1 3 f2 For example, if f1 5 175 kHz and f2 5 178 kHz, the resonant frequency is fr 5 2175 3 103 3 178 3 103 5 176.5 kHz For a linear frequency scale, you can calculate the center or resonant frequency by using an average of the cutoff frequencies. fr 5 f1 1 f2 2 If the circuit Q is very high (.100), then the response curve is approximately sym- metric around the resonant frequency. The cutoff frequencies will then be roughly equi- distant from the resonant frequency by the amount of BW/2. Thus the cutoff frequencies can be calculated if the bandwidth and the resonant frequency are known: f1 5 fr 2 BW 2 and f2 5 fr 1 BW 2 For instance, if the resonant frequency is 49 MHz (49,000 kHz) and the bandwidth is 10 kHz, then the cutoff frequencies will be f1 5 49,000 kHz 2 10k 2 5 49,000 kHz 2 5 kHz 5 48,995 kHz f2 5 49,000 kHz 1 5 kHz 5 49,005 kHz Keep in mind that although this procedure is an approximation, it is useful in many applications. The bandwidth of a resonant circuit deines its selectivity, i.e., how the circuit responds to varying frequencies. If the response is to produce a high current only over a narrow range of frequencies, a narrow bandwidth, the circuit is said to be highly selec- tive. If the current is high over a broader range of frequencies, i.e., the bandwidth is wider, the circuit is less selective. In general, circuits with high selectivity and narrow bandwidths are more desirable. However, the actual selectivity and bandwidth of a circuit must be optimized for each application. Example 2-16 What is the bandwidth of a resonant circuit with a frequency of 28 MHz and a Q of 70? BW 5 fr Q 5 28 3 106 70 5 400,000 Hz 5 400 kHz Selectivity
  • 35. 50 Chapter 2 The relationship between circuit resistance Q and bandwidth is extremely impor- tant. The bandwidth of a circuit is inversely proportional to Q. The higher Q is, the smaller the bandwidth. Low Qs produce wide bandwidths or less selectivity. In turn, Q is a function of the circuit resistance. A low resistance produces a high Q, a nar- row bandwidth, and a highly selective circuit. A high circuit resistance produces a low Q, wide bandwidth, and poor selectivity. In most communication circuits, circuit Qs are at least 10 and typically higher. In most cases, Q is controlled directly by the resistance of the inductor. Fig. 2-17 shows the effect of different values of Q on bandwidth. Example 2-17 The upper and lower cutoff frequencies of a resonant circuit are found to be 8.07 and 7.93 MHz. Calculate (a) the bandwidth, (b) the approximate resonant frequency, and (c) Q. a. BW 5 f2 2 f1 5 8.07 MHz 2 7.93 MHz 5 0.14 MHz 5 140 kHz b. fr 5 1f1 f2 5 1(8.07 3 106 ) (7.93 3 106 ) 5 8 MHz c. Q 5 fr BW 5 8 3 106 140 3 103 5 57.14 Example 2-18 What are the approximate 3-dB down frequencies of a resonant circuit with a Q of 200 at 16 MHz? BW 5 fr Q 5 16 3 106 200 5 80,000 Hz 5 80 kHz f1 5 fr 2 BW 2 5 16,000,000 2 80,000 2 5 15.96 MHz f2 5 fr 1 BW 2 5 16,000,000 1 80,000 2 5 16.04 MHz Resonance produces an interesting but useful phenomenon in a series RLC circuit. Consider the circuit in Fig. 2-18(a). At resonance, assume XL 5 XC 5 500 V. The total circuit resistance is 10 V. The Q of the circuit is then Q 5 XL R 5 500 10 5 50 If the applied or source voltage Vs is 2 V, the circuit current at resonance will be I 5 Vs R 5 2 10 5 0.2 A
  • 36. Electronic Fundamentals for Communications 51 When the reactances, the resistances, and the current are known, the voltage drops across each component can be computed: VL 5 IXL 5 0.2(500) 5 100 V VC 5 IXC 5 0.2(500) 5 100 V VR 5 IR 5 0.2(10) 5 2 V As you can see, the voltage drops across the inductor and capacitor are signiicantly higher than the applied voltage. This is known as the resonant step-up voltage. Although the sum of the voltage drops around the series circuit is still equal to the source voltage, at resonance the voltage across the inductor leads the current by 90° and the voltage across the capacitor lags the current by 90° [see Fig. 2-18(b)]. Therefore, the inductive and reac- tive voltages are equal but 180° out of phase. As a result, when added, they cancel each other, leaving a total reactive voltage of 0. This means that the entire applied voltage appears across the circuit resistance. The resonant step-up voltage across the coil or capacitor can be easily computed by multiplying the input or source voltage by Q: VL 5 VC 5 QVs In the example in Fig. 2-18, VL 5 50(2) 5 100 V. Resonant step-up voltage Figure 2-17 The efect of Q on bandwidth and selectivity in a resonant circuit. fr BW 1 ⫺3 dB points BW 2 BW 3 High Q1, narrow bandwidth Medium Q2, medium bandwidth Low Q3, wide bandwidth Gain, dB Figure 2-18 Resonant step-up voltage in a series resonant circuit. Vs⫽ 2 V VC ⫽ 100 V VL ⫽ 100 V VL ⫽ 100 V VR ⫽ Vs ⫽ 2 V Equal and 180° out of phase I VC ⫽ 100 V VR ⫽ 2 V XC ⫽ 500 ⍀ XL ⫽ 500 ⍀ R ⫽ 10 ⍀ I ⫽ 0.2 A (a) (b)
  • 37. 52 Chapter 2 Parallel Resonant Circuits. A parallel resonant circuit is formed when the inductor and capacitor are connected in parallel with the applied voltage, as shown in Fig. 2-19(a). In general, resonance in a parallel tuned circuit can also be deined as the point at which the inductive and capacitive reactances are equal. The resonant frequency is therefore calculated by the resonant frequency formula given earlier. If we assume lossless compo- nents in the circuit (no resistance), then the current in the inductor equals the current in the capacitor: IL 5 IC Although the currents are equal, they are 180° out of phase, as the phasor diagram in Fig. 2-19(b) shows. The current in the inductor lags the applied voltage by 90°, and the current in the capacitor leads the applied voltage by 90°, for a total of 180°. Now, by applying Kirchhoff’s current law to the circuit, the sum of the individual branch currents equals the total current drawn from the source. With the inductive and capacitive currents equal and out of phase, their sum is 0. Thus, at resonance, a parallel tuned circuit appears to have ininite resistance, draws no current from the source and thus has ininite impedance, and acts as an open circuit. However, there is a high circulating current between the inductor and capacitor. Energy is being stored and transferred between the inductor and capacitor. Because such a circuit acts as a kind of storage vessel for electric energy, it is often referred to as a tank circuit and the circulating current is referred to as the tank current. In a practical resonant circuit where the components do have losses (resistance), the circuit still behaves as described above. Typically, we can assume that the capacitor has practically zero losses and the inductor contains a resistance, as illustrated in Fig. 2-20(a). At resonance, where XL 5 XC, the impedance of the inductive branch of the circuit is higher than the impedance of the capacitive branch because of the coil resistance. The capacitive current is slightly higher than the inductive current. Even if the reactances are Parallel resonant circuit Tank circuit Tank current Example 2-19 A series resonant circuit has a Q of 150 at 3.5 MHz. The applied voltage is 3 µV. What is the voltage across the capacitor? VC 5 QVs 5 150(3 3 1026 ) 5 450 3 1026 5 450 µV Figure 2-19 Parallel resonant circuit currents. (a) Parallel resonant circuit. (b) Current relationships in parallel resonant circuit. Vs IC IL Line current IC Vs IL ⫺90° ⫹90° (b) (a) 冪苴苴苴苴苳 IT ⫽ (IL)2 ⫹ (IC)2 This interesting and useful phenomenon means that small applied voltages can essen- tially be stepped up to a higher voltage—a form of simple ampliication without active circuits that is widely applied in communication circuits.
  • 38. Electronic Fundamentals for Communications 53 equal, the branch currents will be unequal and therefore there will be some net current low in the supply line. The source current will lead the supply voltage, as shown in Fig. 2-20(b). Nevertheless, the inductive and capacitive currents in most cases will cancel because they are approximately equal and of opposite phase, and consequently the line or source current will be signiicantly lower than the individual branch currents. The result is a very high resistive impedance, approximately equal to Z 5 Vs IT The circuit in Fig. 2-20(a) is not easy to analyze. One way to simplify the mathematics involved is to convert the circuit to an equivalent circuit in which the coil resistance is translated to a parallel resistance that gives the same overall results, as shown in Fig. 2-21. The equivalent inductance Leq and resistance Req are calculated with the formulas Leq 5 L(Q2 1 1) Q2 and Req 5 RW(Q2 1 1) and Q is determined by the formula Q 5 XL RW where RW is the coil winding resistance. If Q is high, usually more than 10, Leq is approximately equal to the actual induc- tance value L. The total impedance of the circuit at resonance is equal to the equivalent parallel resistance: Z 5 Req Figure 2-20 A practical parallel resonant circuit. (a) Practical parallel resonant circuit with coil resistance RW. (b) Phase relationships. Vs IC RW IL Line current C IT (a) L IC Vs IL IT (b) (Vector sum of IC and IL leads Vs because IC ⬎ IL) (lags Vs by less than 90° because of RW) Figure 2-21 An equivalent circuit makes parallel resonant circuits easier to analyze. C C L RW Req Req = RW (Q 2 + 1) Leq = L (Q 2 + 1) Z = Req Leq Actual circuit Equivalent circuit Q 2 Lossless resonant circuit
  • 39. 54 Chapter 2 If the Q of the parallel resonant circuit is greater than 10, the following simpliied formula can be used to calculate the resistive impedance at resonance: Z 5 L CRW The value of RW is the winding resistance of the coil. Example 2-20 What is the impedance of a parallel LC circuit with a resonant frequency of 52 MHz and a Q of 12? L 5 0.15 µH. Q 5 XL RW XL 5 2πfL 5 6.28(52 3 106 )(0.15 3 1026 ) 5 49 V RW 5 XL Q 5 49 12 5 4.1 V Z 5 Req 5 RW (Q2 1 1) 5 4.1(122 1 1) 5 4.1(145) 5 592 V Example 2-21 Calculate the impedance of the circuit given in Example 2-20 by using the formula Z 5 L/CR. fr 5 52 MHz RW 5 4.1 V L 5 0.15 µH C 5 1 4π2 fr 2 L 5 1 39.478(52 3 106 )2 (0.15 3 1026 ) 5 6.245 3 10211 Z 5 L CRW 5 0.15 3 1026 (62.35 3 10212 )(4.1) 5 586 V This is close to the previously computed value of 592 V. The formula Z 5 L/CRW is an approximation. A frequency and phase response curve of a parallel resonant circuit is shown in Fig. 2-22. Below the resonant frequency, XL is less than XC; thus the inductive current is greater than the capacitive current, and the circuit appears inductive. The line current lags the applied voltage. Above the resonant frequency, XC is less than XL; thus the capacitive current is more than the inductive current, and the circuit appears capacitive. Therefore, the line current leads the applied voltage. The phase angle of the impedance will be leading below resonance and lagging above resonance. At the resonant frequency, the impedance of the circuit peaks. This means that the line current at that time is at its minimum. At resonance, the circuit appears to have a very high resistance, and the small line current is in phase with the applied voltage. GOOD TO KNOW The bandwidth of a circuit is in- versely proportional to the circuit Q. The higher the Q, the smaller the bandwidth. Low Q values produce wide bandwidths or less selectivity.
  • 40. Electronic Fundamentals for Communications 55 Note that the Q of a parallel circuit, which was previously expressed as Q 5 XL/RW, can also be computed with the expression Q 5 RP XL where RP is the equivalent parallel resistance, Req in parallel with any other parallel resistance, and XL is the inductive reactance of the equivalent inductance Leq. You can set the bandwidth of a parallel tuned circuit by controlling Q. The Q can be determined by connecting an external resistor across the circuit. This has the effect of lowering RP and increasing the bandwidth.d Figure 2-22 Response of a parallel resonant circuit. Below resonance (inductive) Above resonance (capacitive) +90° (leading) -90° (lagging) Phase shift of line current in degrees (red curve only) 0° fr Impedance (blue curve only) Z Example 2-22 What value of parallel resistor is needed to set the bandwidth of a parallel tuned circuit to 1 MHz? Assume XL 5 300 V, RW 5 10 V, and fr 5 10 MHz. Q 5 XL RW 5 300 10 5 30 RP 5 RW(Q2 1 1) 5 10(302 1 1) 5 10(901) 5 9010 V (equivalent resistance of the parallel circuit at resonance) BW 5 fr Q Q 5 fr BW 5 10 MHz 1 MHz 5 10 (Q needed for 1-MHz bandwidth) RPnew 5 QXL 5 10(300) 5 3000 V (this is the total resistance of the circuit RPnew made up of the original RP and an externally connected resistor Rext) RPnew 5 RPRext RP 1 Rext Rext 5 RPnewRP RP 2 RPnew 5 9010(3000) 9010 2 3000 5 4497.5V