Module 10—Introduction to Wave Propagation, Transmission Lines, and Antennas
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, 1-1 to 1-10
1-11 to 1-20
, 1-21 to 1-30
1-31 to 1-40
1-41 to 1-47
2-1 to 2-10
, 2-11 to 2-20
2-21 to 2-30
, 2-31 to 2-40
2-40 to 2-47
, 3-1 to 3-10
3-11 to 3-20
3-21 to 3-30
3-31 to 3-40
, 3-41 to 3-50
3-51 to 3-58
, 4-1 to 4-10
4-11 to 4-20
, 4-21 to 4-30
4-31 to 4-40
, 4-41 to 4-50
4-51 to 4-60
speeds in different
transparent substances. For example, water never appears as deep as it really is, and objects under water appear
to be closer to the surface than they really are. A bending of the light rays causes these impressions.
Another example of refraction is the apparent bending of a spoon when it is immersed in a cup of water. The
bending seems to take place at the surface of the water, or exactly at the point where there is a change of
density. Obviously, the spoon does not bend from the pressure of the water. The light forming the image of the
spoon is bent as it passes from the water (a medium of high density) to the air (a medium of comparatively low
Without refraction, light waves would pass in straight lines through transparent substances
without any change of direction. Refer back to figure 1-10, which shows refraction of a wave. As you can see, all
rays striking the glass at any angle other than perpendicular are refracted. However, the perpendicular ray, which
enters the glass normal to the surface, continues through the glass and into the air in a straight line no
refraction takes place. Diffusion of Light
When light is reflected from a mirror,
the angle of reflection of each ray equals the angle of incidence. When light is reflected from a piece of plain
white paper, however, the reflected beam is scattered, or DIFFUSED, as shown in figure 1-21. Because the surface
of the paper is not smooth, the reflected light is broken up into many light beams that are reflected in all
Figure 1-21.—Diffusion of light.
Absorption of Light
You have just seen that a light beam is reflected and
diffused when it falls onto a piece of white paper. If a light beam falls onto a piece of black paper, the black
paper absorbs most of the light rays and very little light is reflected from the paper. If the surface on which
the light beam falls is perfectly black, there is no reflection; that is, the light is totally absorbed. No matter
what kind of surface light falls on, however, some of the light is absorbed.
Q40. A light wave enters a
sheet of glass at a perfect right angle to the surface. Is the majority of the wave reflected, refracted,
transmitted, or absorbed?
Q41. When light strikes a piece of white paper, the light is reflected in all
directions. What do we call this scattering of light?
COMPARISON OF LIGHT WAVES WITH SOUND WAVES
There are two main differences
between sound waves and light waves. The first difference is in velocity. Sound waves travel through air at the
speed of approximately 1,100 feet per second; light waves travel through air and empty space at a speed of
approximately 186,000 miles per second. The second difference is that sound is composed of longitudinal waves
(alternate compressions and expansions of matter) and light is composed of transverse waves in an electromagnetic
Although both are forms of wave motion, sound requires a solid, liquid, or gaseous medium; whereas
light travels through empty space. The denser the medium, the greater the speed of sound. The opposite is true of
light. Light travels approximately one-third slower in water than in air. Sound travels through all substances,
but light cannot pass through opaque materials.
Frequency affects both sound and light. A certain range of
sound frequencies produces sensations that you can hear. A slow vibration (low frequency) in sound gives the
sensation of a low note. A more rapid sound vibration (higher frequency) produces a higher note. Likewise, a
certain range of light frequencies produces sensations that you can see. Violet light is produced at the
high-frequency end of the light spectrum, while red light is produced at the low-frequency end of the light
spectrum. A change in frequency of sound waves causes an audible sensation—a difference in pitch. A change in the
frequency of a light wave causes a visual sensation—a difference in color.
For a comparison of light waves with sound waves, see table 1-2.
Table 1-2.—Comparison of Light Waves and Sound Waves
Q42. What three examples of electromagnetic energy are mentioned in the text?
What is the main difference between the bulk of the electromagnetic spectrum and the visual spectrum?
Light is one kind of electromagnetic energy. There
are many other types, including heat energy and radio energy. The only difference between the various types of
electromagnetic energy is the frequency of their waves (rate of vibration). The term SPECTRUM is used to designate
the entire range of electromagnetic waves arranged in order of their frequencies. The VISIBLE SPECTRUM contains
only those waves which stimulate the sense of sight. You, as a technician, might be expected to maintain equipment
that uses electromagnetic waves within, above, and below the visible spectrum.
There are neither sharp
dividing lines nor gaps in the ELECTROMAGNETIC SPECTRUM. Figure
1-22 illustrates how portions of the
electromagnetic spectrum overlap. Notice that only a small portion of the electromagnetic spectrum contains
visible waves, or light, which can be seen by the human eye.
Figure 1-22.—Electromagnetic spectrum.
In general, the same principles and properties of light
waves apply to the communications electromagnetic waves you are about to study. The electromagnetic field is used
to transfer energy (as communications) from point to point. We will introduce the basic ANTENNA as the propagation
source of these electromagnetic waves.
THE BASIC ANTENNA
The study of antennas and electromagnetic wave propagation is
essential to a complete understanding of radio communication, radar, loran, and other electronic systems. Figure
1-23 shows a simple radio communication system. In the illustration, the transmitter is an electronic device that
generates radio-frequency energy. The energy travels through a transmission line (we will discuss this in chapter
3) to an antenna. The antenna converts the energy into radio waves that radiate into space from the antenna at the
speed of light. The radio waves travel through the atmosphere or space until they are either reflected by an
object or absorbed. If another antenna is placed in the path of the radio waves, it absorbs part of the waves and
converts them to energy. This energy travels through another transmission line and is fed to a receiver. From this
example, you can see that the requirements for a simple communications system are (1) transmitting equipment, (2)
transmission line, (3) transmitting antenna, (4) medium, (5) receiving antenna, and (6) receiving equipment.
Figure 1-23.—Simple radio communication system.
An antenna is a conductor or a set of conductors used either to radiate electromagnetic energy into
space or to collect this energy from space. Figure 1-24 shows an antenna. View A is a drawing of an actual
antenna; view B is a cut-away view of the antenna; and view C is a simplified diagram of the antenna.
COMPONENTS OF THE ELECTROMAGNETIC WAVE
An electromagnetic wave consists of two
primary components—an ELECTRIC FIELD and a MAGNETIC FIELD. The electric field results from the force of voltage,
and the magnetic field results from the flow of current.
Although electromagnetic fields that are radiated
are commonly considered to be waves, under certain circumstances their behavior makes them appear to have some of
the properties of particles. In general, however, it is easier to picture electromagnetic radiation in space as
horizontal and vertical lines of force oriented at right angles to each other. These lines of force are made up of
an electric field (E) and a magnetic field (H), which together make up the electromagnetic field in space.
The electric and magnetic fields radiated from an antenna form the electromagnetic field. This field is
responsible for the transmission and reception of electromagnetic energy through free space. An antenna, however,
is also part of the electrical circuit of a transmitter or a receiver and is equivalent to a circuit containing
inductance, capacitance, and resistance. Therefore, the antenna can be expected to display definite voltage and
current relationships with respect to a given input. A current through the antenna produces a magnetic field, and
a charge on the antenna produces an electric field. These two fields combine to form the INDUCTION field. To help
you gain a better understanding of antenna theory, we must review some basic electrical concepts. We will review
voltage and its electric field, current and its magnetic field, and their relationship to propagation of
Q44. What are the two components (fields) that make up the electromagnetic wave?
Q45. What do we call a conductor (or set of conductors) that radiates electromagnetic energy into
space? Electric Field
Around every electrically charged object is a force field
that can be detected and measured. This force field can cause electric charges to move in the field. When an
object is charged electrically, there is either a greater or a smaller concentration of electrons than normal.
Thus, a difference of potential exists between a charged object and an uncharged object. An electric field is,
therefore, associated with a difference of potential, or a voltage.
This invisible field of force is
commonly represented by lines that are drawn to show the paths along which the force acts. The lines representing
the electric field are drawn in the direction that a single positive charge would normally move under the
influence of that field. A large electric force is shown by a large concentration of lines; a weak force is
indicated by a few lines.
When a capacitor is connected across a source of voltage, such as a battery, it is charged by a particular amount,
depending on the voltage and the value of capacitance. (See figure 1-25.) Because of the emf (electromotive force)
of the battery, negative charges flow to the lower plate, leaving the upper plate positively charged. Along with
the growth of charge, the electric field is also building up. The flux lines are directed from the positive to the
negative charges and at right angles to the plates. When the capacitor is fully charged, the voltage of the
capacitor is equal to the voltage of the source and opposite in polarity. The charged capacitor stores the energy
in the form of an electric field. It can be said, therefore, that an electric field indicates voltage.
Figure 1-25.—Electric fields between plates.
If the two plates of the capacitor are spread farther apart, the electric field must curve to meet the
plates at right angles (fig. 1-26). The straight lines in view A of figure 1-26 become arcs in view B, and
approximately semicircles in view C, where the plates are in a straight line. Instead of flat metal plates, as in
the capacitor, the two elements can take the form of metal rods or wires and form the basic antenna.
Figure 1-26.—Electric fields between plates at different angles.
In figure 1-27, two rods replace the plates of the capacitor, and the battery is replaced by an ac
source generating a 60-hertz signal. On the positive alternation of the 60-hertz generator, the electric field
extends from the positively charged rod to the negatively charged rod, as shown. On the negative alternation, the
charge is reversed. The previous explanation of electrons moving from one plate to the other of the capacitor in
figure 1-25 can also be applied to the rods in figure 1-27.
Figure 1-27.—Electric fields between elements.
The polarity of charges and the direction of the electric fields will reverse polarity and direction
periodically at the frequency of the voltage source. The electric field will build up from zero to maximum in one
direction and then collapse back to zero. Next, the field will build up to maximum in the opposite direction and
then collapse back to zero. This complete reversal occurs during a single cycle of the source voltage. The
HALF-WAVE DIPOLE ANTENNA (two separate rods in line as illustrated in figure 1-27)
is the fundamental element
normally used as a starting point of reference in any discussion concerning the radiation of electromagnetic
energy into space. If rf energy from the ac generator (or transmitter) is supplied to the element of an antenna,
the voltage across the antenna lags the current by 90 degrees. The antenna acts as if it were a capacitor.
When current flows through a conductor, a magnetic field is set up in the area surrounding the conductor. In fact,
any moving electrical charge will create a magnetic field. The magnetic field is a region in space where a
magnetic force can be detected and measured. There are two other fields involved—an INDUCTION FIELD, which exists
close to the conductor carrying the current, and the RADIATION FIELD, which becomes detached from the
current-carrying rod and travels through space.
To represent the magnetic field, lines of force are again
used to illustrate the energy. Magnetic lines are not drawn between the rods, nor between high- and low-potential
points, as the E lines that were discussed earlier. Magnetic lines are created by the flow of current rather than
the force of voltage. The magnetic lines of force, therefore, are drawn at right angles to the direction of
The magnetic fields that are set up around two parallel rods, as shown in figure 1-28 view
A, are in maximum opposition. Rod 1 contains a current flowing from the generator, while rod 2 contains a current
flowing toward the generator. As a result, the direction of the magnetic field surrounding rod 1 is opposite the
direction of the magnetic field surrounding rod 2. This will cause cancellation of part or all of both magnetic
fields with a resultant decrease in radiation of the electromagnetic energy. View B illustrates the fact that if
the far ends of rods 1 and 2 are separated from each other while the rods are still connected to the generator at
the near ends, more space, and consequently less opposition, will occur between the magnetic fields of the two
rods. View C illustrates the fact that placing the rods in line makes the currents through both rods flow in the
same direction. Therefore, the two magnetic fields are in the same direction; thus, maximum electromagnetic
radiation into space can be obtained.
Figure 1-28.—Magnetic fields around elements.
Magnetic lines of force are indicated by the letter H and are called H lines. The direction of the
magnetic lines may be determined by use of the left-hand rule for a conductor: If you grasp the conductor in your
left hand with the thumb extended in the direction of the current flow, your fingers will point in the direction
of the magnetic lines of force. In view C of figure 1-28, the direction of current flow is upward along both
halves of the elements (conductors). The lines of magnetic force (flux) form concentric loops that are
perpendicular to the direction of current flow. The arrowheads on the loops indicate the direction of the field.
The left-hand rule is used to determine the direction of the magnetic field and is illustrated in figure 1-29. If
the thumb of the left hand is extended in the direction of current flow and the fingers clenched, then the rough
circles formed by the fingers indicate the direction of the magnetic field.
Figure 1-29.—Left-hand rule for conducting elements.
Q46. What do we call the field that is created between two rods when a voltage is applied to them?
Q47. When current flows through a conductor, a field is created around the conductor. What do we call this
field? Combined Electric and Magnetic Fields
The generator, shown in figure 1-30,
provides the voltage, which creates an electric field, and current, which creates a magnetic field. This source
voltage and current build up to maximum values in one direction during one half-cycle, and then build up to
maximum values in the other direction during the next half-cycle. Both the electric and magnetic fields alternate
from minimum through maximum values in synchronization with the changing voltage and current. The electric and
magnetic fields reach their maximum intensity a quarter-cycle apart. These fields form the induction field. Since
the current and voltage that produce these E and H fields are 90 degrees out of phase, the fields will also be 90
degrees out of phase.
Figure 1-30.—Relationship of E-lines, and current flow.
Q48. An induction field is created around a conductor when current flows through it. What do we call
the field that detaches itself from the conductor and travels through space?
Introduction to Matter, Energy, and Direct Current,
to Alternating Current and Transformers, Introduction to Circuit Protection,
Control, and Measurement
, Introduction to Electrical Conductors, Wiring Techniques,
and Schematic Reading
, Introduction to Generators and Motors
Introduction to Electronic Emission, Tubes, and Power Supplies,
Introduction to Solid-State Devices and Power Supplies
Introduction to Amplifiers, Introduction to
Wave-Generation and Wave-Shaping Circuits
, Introduction to Wave Propagation, Transmission
Lines, and Antennas
, Microwave Principles,
, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros
Introduction to Test Equipment
, Radar Principles,
The Technician's Handbook,
Master Glossary, Test Methods and Practices,
Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics