Module 11—Microwave Principles
Pages i - ix
1-1 to 1-10
, 1-11 to 1-20
1-21 to 1-30
, 1-31 to 1-40
1-41 to 1-50
, 1-51 to 1-60
1-61 to 1-68
, 2-1 to 2-10
2-11 to 2-20
21 to 2-30
2-31 to 2-40
, 2-41 to 2-50
2-51 to 2-60
, 2-61 to 2-66
3-1 to 3-10
, 3-11 to 3-20
AI-1 to AI-6
, Index-1 to Index-2
Assignment 1 - 1-8
Assignment 2 - 9-16
WAVEGUIDE THEORY AND APPLICATION
Upon completion of this chapter the student will be able to:
1. Describe the
development of the various types of waveguides in terms of their advantages and
the physical dimensions of the various types of waveguides and explain the effects of
those dimensions on
power and frequency.
3. Explain the propagation of energy in waveguides in terms of electromagnetic field
4. Identify the modes of operation in waveguides.
5. Explain the basic input/output methods used in
6. Describe the basic principles of waveguide plumbing.
7. Explain the reasons for and the methods of
8. Explain the basic theory of operation and applications of directional couplers.
9. Describe the basic theory of operation, construction, and applications of cavity resonators.
the basic theory of operation of waveguide junctions.
11. Explain the operation of ferrite devices in terms of
INTRODUCTION TO WAVEGUIDE THEORY AND APPLICATION
That portion of the electromagnetic spectrum which falls between 1000 megahertz and 100,000 megahertz is
referred to as the MICROWAVE region. Before discussing the principles and applications of microwave frequencies,
the meaning of the term microwave as it is used in this module must be established. On the surface, the definition
of a microwave would appear to be simple because, in electronics, the prefix "micro" normally means a millionth
part of a unit. Micro also means small, which is a relative term, and it is used in that sense in this module.
Microwave is a term loosely applied to identify electromagnetic waves above 1000 megahertz in frequency because of
the short physical wavelengths of these frequencies. Short wavelength energy offers distinct advantages in many
applications. For instance, excellent directivity can be obtained using relatively small antennas and
low-power transmitters. These features are ideal for use in both military and civilian radar and
applications. Small antennas and other small components are made possible by microwave frequency applications.
This is an important consideration in shipboard equipment planning where space and weight are major problems.
Microwave frequency usage is especially important in the design of shipboard radar because it makes possible the
detection of smaller targets.
Microwave frequencies present special problems in transmission, generation, and circuit design that
are not encountered at lower frequencies. Conventional circuit theory is based on voltages and currents while
microwave theory is based on electromagnetic fields. The concept of electromagnetic field interaction is not
entirely new, since electromagnetic fields form the basis of all antenna theory. However, many students of
electronics find electromagnetic field theory very difficult to visualize and understand. This module will present
the principles of microwave theory in the simplest terms possible but many of the concepts are still somewhat
difficult to thoroughly understand. Therefore, you must realize that this module will require very careful study
for you to properly understand microwave theory. Antenna fundamentals were covered in NEETS, Module 10,
Introduction to Wave Propagation, Transmission Lines, and Antennas.
This module will show you the solutions to problems encountered at microwave frequencies, beginning with the
transmission of microwave energy and continuing through to waveguides in chapter 1. Later chapters will cover the
theory of operation of microwave components, circuits, and antennas. The application of these concepts will be
discussed more thoroughly in later NEETS modules on radar and communications.
Q-1. What is the region of
the frequency spectrum from 1,000 MHz to 100,000 MHz called?
Q-2. Microwave theory is based upon what
The two-wire transmission line used in conventional circuits is inefficient
for transferring electromagnetic energy at microwave frequencies. At these frequencies, energy escapes by
radiation because the fields are not confined in all directions, as illustrated in figure 1-1. Coaxial lines are
more efficient than two-wire lines for transferring electromagnetic energy because the fields are completely
confined by the conductors, as illustrated in figure 1-2.
Figure 1-1.—Fields confined in two directions only.
Figure 1-2.—Fields confined in all directions.
Waveguides are the most efficient way to transfer electromagnetic energy. WAVEGUIDES are essentially
coaxial lines without center conductors. They are constructed from conductive material and may be rectangular,
circular, or elliptical in shape, as shown in figure 1-3.
Figure 1-3.—Waveguide shapes.
Waveguides have several advantages over two-wire and coaxial
transmission lines. For example, the large surface area of waveguides greatly reduces COPPER (I2R) LOSSES.
Two-wire transmission lines have large copper losses because they have a relatively small surface area. The
surface area of the outer conductor of a coaxial cable is large, but the surface area of the inner conductor is
relatively small. At microwave frequencies, the current-carrying area of the inner conductor is restricted to a
very small layer at the surface of the conductor by an action called SKIN EFFECT.
Skin effect was discussed in NEETS, Module 10, Introduction to Wave Propagation, Transmission Lines, and
Antennas, Chapter 3. Skin effect tends to increase the effective resistance of the conductor. Although energy
transfer in coaxial cable is caused by electromagnetic field motion, the magnitude of the field is limited by the
size of the current-carrying area of the inner conductor. The small size of the center conductor is even further
reduced by skin effect and energy transmission by coaxial cable becomes less efficient than by waveguides.
DIELECTRIC LOSSES are also lower in waveguides than in two-wire and coaxial transmission lines. Dielectric losses
in two-wire and coaxial lines are caused by the heating of the insulation between the conductors. The insulation
behaves as the dielectric of a capacitor formed by the two wires of the transmission line. A voltage potential
across the two wires causes heating of the dielectric and results in a power loss. In practical applications, the
actual breakdown of the insulation between the conductors of a transmission line is more frequently a problem than
is the dielectric loss.
This breakdown is usually caused by stationary voltage spikes or "nodes" which are
caused by standing waves. Standing waves are stationary and occur when part of the energy traveling down the line
is reflected by an impedance mismatch with the load. The voltage potential of the standing waves at the points of
greatest magnitude can become large enough to break down the insulation between transmission line conductors.
The dielectric in waveguides is air, which has a much lower dielectric loss than conventional insulating
materials. However, waveguides are also subject to dielectric breakdown caused by standing waves. Standing waves
in waveguides cause arcing which decreases the efficiency of energy transfer and can severely damage the
waveguide. Also since the electromagnetic fields are completely contained within the waveguide, radiation losses
are kept very low.
Power-handling capability is another advantage of waveguides. Waveguides can handle more
power than coaxial lines of the same size because power-handling capability is directly related to the distance
between conductors. Figure 1-4 illustrates the greater distance between conductors in a waveguide.
Figure 1-4.—Comparison of spacing in coaxial cable and a circular waveguide.
In view of the advantages of waveguides, you would think that waveguides should be the only type of
transmission lines used. However, waveguides have certain disadvantages that make them practical for use only at
Physical size is the primary lower-frequency limitation
of waveguides. The width of a waveguide must be approximately a half wavelength at the frequency of the wave to be
transported. For example, a waveguide for use at 1 megahertz would be about 500 feet wide. This makes the use of
waveguides at frequencies below 1000 megahertz increasingly impractical. The lower frequency range of any system
using waveguides is limited by the physical dimensions of the waveguides.
Waveguides are difficult to install
because of their rigid, hollow-pipe shape. Special couplings at the joints are required to assure proper
operation. Also, the inside surfaces of waveguides are often plated with silver or gold to reduce skin effect
losses. These requirements increase the costs and decrease the practicality of waveguide systems at any other than
Q-3. Why are coaxial lines more efficient at microwave frequencies than two-wire transmission lines?
Q-4. What kind of material must be used in the construction of waveguides?
Q-5. The large surface
area of a waveguide greatly reduces what type of loss that is common in two-wire and coaxial lines?
Q-6. What causes the current-carrying area at the center conductor of a coaxial line to be restricted to a small
layer at the surface?
Q-7. What is used as a dielectric in waveguides?
Q-8. What is the
primary lower-frequency limitation of waveguides?
Developing the Waveguide from Parallel Lines
You may better understand the transition from ordinary transmission line concepts to waveguide
theories by considering the development of a waveguide from a two-wire transmission line. Figure 1-5 shows a
section of two-wire transmission line supported on two insulators. At the junction with the line, the insulators
must present a very high impedance to ground for proper operation of the line. A low impedance insulator would
obviously short-circuit the line to ground, and this is what happens at very high frequencies. Ordinary insulators
display the characteristics of the dielectric of a capacitor formed by the wire and ground. As the frequency
increases, the overall impedance decreases. A better high- frequency insulator is a quarter-wave section of
transmission line shorted at one end. Such an insulator is shown in figure 1-6. The impedance of a shorted
quarter-wave section is very high at the open-end junction with the two-wire transmission line. This type of
insulator is known as a METALLIC INSULATOR and may be placed anywhere along a two-wire line. Note that
quarter-wave sections are insulators at only one frequency. This severely limits the bandwidth, efficiency, and
application of this type of two-wire line.
Figure 1-5.—Two-wire transmission line using ordinary insulators.
Figure 1-6.—Quarter-wave section of transmission line shorted at one end.
Figure 1-7 shows several metallic insulators on each side of a two-wire transmission line. As more
insulators are added, each section makes contact with the next, and a rectangular waveguide is formed. The lines
become part of the walls of the waveguide, as illustrated in figure 1-8. The energy is then conducted within the
hollow waveguide instead of along the two-wire transmission line.
Figure 1-7.—Metallic insulators on each side of a two-wire line.
Figure 1-8.—Forming a waveguide by adding quarter-wave sections.
The comparison of the way electromagnetic fields work on a transmission line and in a waveguide is not
exact. During the change from a two-wire line to a waveguide, the electromagnetic field configurations also
undergo many changes. These will be discussed later in this chapter. As a result of these changes, the waveguide
does not actually operate like a two-wire line that is completely shunted by quarter-wave sections. If it did, the
use of a waveguide would be limited to a single-frequency wavelength that was four times the length of the
quarter-wave sections. In fact, waves of this length cannot pass efficiently through waveguides. Only a small
range of frequencies of somewhat shorter wavelength (higher frequency) can pass efficiently.
As shown in
figure 1-9, the widest dimension of a waveguide is called the "a" dimension and determines the range of operating
frequencies. The narrowest dimension determines the power-handling capability of the waveguide and is called the
Figure 1-9.—Labeling waveguide dimensions.
This method of labeling waveguides is not standard in all texts. Different
methods may be used in other texts on microwave principles, but this method is in accordance with Navy Military
The ability of a waveguide of a given dimension to transport more than one frequency may
be better understood by analyzing the actions illustrated in figure 1-10A, B, and C. A waveguide may be considered
as having upper and lower quarter-wave sections and a central section which is a solid conductor called a BUS BAR.
In figure 1-10A, distance mn is equal to distance pq, and both are equal to one quarter-wavelength (λ/4).
Figure 1-10A.—Frequency effects on a waveguide. NORMAL OPERATING FREQUENCY.
Throughout NEETS, 1/4λ and λ/4 are both used to represent one
quarter-wavelength and are used interchangeably. Also, λ/2 and 3/2λ will be used to represent one half-wavelength
and 1 1/2 wavelengths, respectively.
Distance np is the width of the bus bar. If the overall dimensions of the
waveguide are held constant, the required length of the quarter-wave sections DECREASES as the frequency
increases. As illustrated in figure 1-10B, this causes the width of the bus bar to INCREASE. In theory the
waveguide could function at an infinite number of frequencies higher than the designed frequency; as the length of
quarter-wave section approaches zero, the bus bar continues to widen to fill the available space.
However, in practice, an upper frequency limit is caused by modes of operation, which will be discussed later.
Figure 1-10B.—Frequency effects on a waveguide. INCREASING FREQUENCY.
Figure 1-10C.—Frequency effects on a waveguide. DECREASING FREQUENCY.
If the frequency of a signal is decreased so much that two quarter-wavelengths are longer than the wide
dimension of a waveguide, energy will no longer pass through the waveguide. This is the lower frequency limit, or
CUT-OFF FREQUENCY, of a given waveguide. In practical applications, the wide dimension of a waveguide is usually
0.7 wavelength at the operating frequency. This allows the waveguide to handle a small range of frequencies both
above and below the operating frequency. The "b" dimension is governed by the breakdown potential of the
dielectric, which is usually air. Dimensions ranging from 0.2 to 0.5 wavelength are common for the "b" sides of a
Q-9. At very high frequencies, what characteristics are displayed by ordinary insulators?
Q-10. What type of insulator works well at very high frequencies?
Q-11. The frequency range of a waveguide is determined by what dimension?
Q-12. What happens
to the bus bar dimensions of the waveguide when the frequency is increased?
Q-13. When the frequency is
decreased so that two quarter-wavelengths are longer than the "a" (wide) dimension of the waveguide, what will
Energy Propagation in Waveguides
Since energy is transferred through
waveguides by electromagnetic fields, you need a basic understanding of field theory. Both magnetic (H FIELD) and
electric field (E FIELD) are present in waveguides, and the interaction of these fields causes energy to travel
through the waveguide. This action is best understood by first looking at the properties of the two individual
E FIELD.—An electric field exists when a difference of potential causes a stress in the
dielectric between two points. The simplest electric field is one that forms between the plates of a capacitor
when one plate is made positive compared to the other, as shown in figure 1-11A. The stress created in the
dielectric is an electric field.
Electric fields are represented by arrows that point from the positive toward
the negative potential. The number of arrows shows the relative strength of the field. In figure 1-11A, for
example, evenly spaced arrows indicate the field is evenly distributed. For ease of explanation, the electric
field is abbreviated E field, and the lines of stress are called E lines.
Figure 1-11A.—Simple electric fields. CAPACITOR.
Figure 1-11B—Simple electric fields. TWO-WIRE TRANSMISSION LINE.
Introduction to Matter, Energy, and Direct Current, Introduction
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,
Modulation Principles, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros,
Introduction to Test Equipment, Radio-Frequency
Communications Principles, Radar Principles, The Technician's Handbook,
Master Glossary, Test Methods and Practices, Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics
Related Pages on RF Cafe
- Properties of Modes in a Rectangular Waveguide
- Properties of Modes in a Circular Waveguide
- Waveguide & Flange Selection Guide
Rectangular & Circular Waveguide: Equations & Fields
Rectangular waveguide TE1,0 cutoff frequency calculator.
- Waveguide Component
NEETS - Waveguide Theory and Application
- EWHBK, Microwave Waveguide
and Coaxial Cable