Module 11 - Microwave Principles
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
, 2−21 to
, 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
transmission line, illustrated in figure 1-11B, has an instantaneous standing wave of voltage applied to it by the
generator. The line is short-circuited at one-wavelength, at the positive and negative voltage peaks, but the
arrows, representing each field, point in opposite directions. The voltage across the line varies sinusoidally.
Therefore, the density of the E-lines varies sinusoidally.
The development of the E field in a waveguide can
be illustrated by a two-wire transmission line separated by several, double quarter-wave sections, called
half-wave frames, as illustrated in figure 1-12. As shown, the voltage across the two-wire line varies in a
sine-wave pattern and the density of the E field also varies in a sine-wave pattern. The half-wave frames located
at high-voltage points (1) and (3) have a strong E field. The frames at the zero-voltage points (2) have no E
fields present. Frame (4) has a weak E field and is located at a point between maximum and minimum voltage. This
illustration is a buildup to the three-dimensional aspect of the full E field in a waveguide.
Figure 1-12. - E fields on a two-wire line with half-wave frames.
Figure 1-13, view (A), shows the E-field pattern created by a voltage sine wave applied to a
one-wavelength section of waveguide shorted at one end. The electric fields are represented by the arrows shown in
views (B) and (C). In the top view of view (A), the tip of each arrow is represented by a dot and the tail of each
arrow is represented by an X. The E field varies in density at the same sine-wave rate as the applied voltage.
This illustration represents the instant that the applied voltage wave is at its peak. At other times, the voltage
and the E field in the waveguide vary continuously from zero to the peak value. Voltage and E-field polarity
reverse with every reversal of the input. Note that the end view shown in view (B) shows the E field is maximum at
the center and minimum near the walls of the waveguide. View (C) shows the arrangement of electromagnetic fields
within a three-dimensional waveguide.
Figure 1-13. - E field of a voltage standing wave across a 1-wavelength section of a waveguide.
H FIELD. - The magnetic field in a waveguide is made up of magnetic lines of force that
are caused by current flow through the conductive material of the waveguide. Magnetic lines of force, called H
lines, are continuous closed loops, as shown in figure 1-14. All of the H lines associated with current are
collectively called a magnetic field or H field. The strength of the H field, indicated by the number of H lines
in a given area, varies directly with the amount of current.
Figure 1-14. - Magnetic field on a single wire.
Although H lines encircle a single, straight wire, they behave differently when the wire is formed into
a coil, as shown in figure 1-15. In a coil the individual H lines tend to form around each turn of wire. Since the
H lines take opposite directions between adjacent turns, the field between the turns is cancelled. Inside and
outside the coil, where the direction of each H field is the same, the fields join and form continuous H lines
around the entire coil.
Figure 1-15. - Magnetic field on a coil.
A similar action takes place in a waveguide. In figure 1-16A, a two-wire line with quarter-wave sections
is shown. Currents flow in the main line and in the quarter-wave sections. The current direction produces the
individual H lines around each conductor as shown. When a large number of sections exist, the fields cancel
between the sections, but the directions are the same both inside and outside the waveguide. At half-wave
intervals on the main line, current will flow in opposite directions. This
produces H-line loops having
opposite directions. In figure 1-16A, current at the left end is opposite to the current at the right end. The
individual loops on the main line are opposite in direction. All around the framework they join so that the long
loop shown in figure 1-16B is formed. Outside the waveguide the individual loops cannot join to form a continuous
loop. Thus, no magnetic field exists outside a waveguide.
Figure 1-16A. - Magnetic fields on a two-wire line with half-wave frames.
Figure 1-16B. - Magnetic fields on a two-wire line with half-wave frames.
If the two-wire line and the half-wave frames are developed into a waveguide that is closed at both ends (as
shown in figure 1-16B), the distribution of H lines will be as shown in figure 1-17. If the waveguide is extended
to 1 1/2λ, these H lines form complete loops at half-wave intervals with each group reversed in direction. Again,
no H lines can form outside the waveguide as long as it is completely enclosed.
Figure 1-17. - Magnetic field pattern in a waveguide.
Figure 1-18 shows a cross-sectional view of the magnetic field pattern illustrated in figure 1-17. Note
in view (A) that the field is strongest at the edges of the waveguide where the current is highest. The minimum
field strength occurs at the zero-current points. View (B) shows the field pattern as it appears λ/4 from the end
view of the waveguide. As with the previously discussed E fields, the H fields shown in figures 1-17 and 1-18
represent a condition that exists at only one instant in time. During the peak of the next half cycle of the input
current, all field directions are reversed and the field will continue to change with changes in the input.
Figure 1-18. - Magnetic field in a waveguide three half-wavelengths long.
BOUNDARY CONDITIONS IN A WAVEGUIDE. - The travel of energy down a waveguide is similar,
but not identical, to the travel of electromagnetic waves in free space. The difference is that the energy in a
waveguide is confined to the physical limits of the guide. Two conditions, known as BOUNDARY CONDITIONS, must be
satisfied for energy to travel through a waveguide.
The first boundary condition (illustrated in figure 1-19A)
can be stated as follows:
For an electric field to exist at the surface of a conductor it must be perpendicular to the
Figure 1-19A. - E field boundary condition. MEETS BOUNDARY CONDITIONS.
The opposite of this boundary condition, shown in figure 1-19B, is also true. An electric field CANNOT
exist parallel to a perfect conductor.
Figure 1-19B. - E field boundary condition. DOES NOT MEET BOUNDARY CONDITIONS.
The second boundary condition, which is illustrated in figure 1-20, can be stated as follows:
For a varying magnetic field to exist, it must form closed loops in parallel with the conductors
perpendicular to the electric field.
Figure 1-20. - H field boundary condition.
Since an E field causes a current flow that in turn produces an H field, both fields always exist at the
same time in a waveguide. If a system satisfies one of these boundary conditions, it must also satisfy the other
since neither field can exist alone. You should briefly review the principles of electromagnetic propagation in
free space (NEETS, Module 10, Introduction to Wave Propagation, Transmission Lines, and Antennas). This review
will help you understand how a waveguide satisfies the two boundary conditions necessary for energy propagation in
WAVEFRONTS WITHIN A WAVEGUIDE. - Electromagnetic energy transmitted into space consists of
electric and magnetic fields that are at right angles (90 degrees) to each other and at right angles to the
direction of propagation. A simple analogy to establish this relationship is by use of the
right-hand rule for
electromagnetic energy, based on the POYNTING VECTOR. It indicates that a screw (right-hand thread) with its axis
perpendicular to the electric and magnetic fields will advance in the
direction of propagation if the E field
is rotated to the right (toward the H field). This rule is illustrated in
Figure 1-21. - The Poynting vector.
The combined electric and magnetic fields form a wavefront that can be represented by alternate
negative and positive peaks at half-wavelength intervals, as illustrated in figure 1-22. Angle " is the direction
of travel of the wave with respect to some reference axis.
Figure 1-22. - Wavefronts in space.
If a second wavefront, differing only in the direction of travel, is present at the same time, a
resultant of the two is formed. The resultant is illustrated in figure 1-23, and a close inspection reveals
important characteristics of combined wavefronts. Both wavefronts add at all points on the reference axis and
cancel at half-wavelength intervals from the reference axis. Therefore, alternate additions and cancellations of
the two wavefronts occur at progressive half-wavelength increments from the reference axis. In figure 1-23, the
lines labeled A, C, F, and H are addition points, and those labeled B, D, E, and G are cancellation points.
Figure 1-23. - Combined wavefronts.
If two conductive plates are placed along cancellation lines D and E or cancellation lines B and G, the
first boundary condition for waveguides will be satisfied; that is, the E fields will be zero at the surface of
the conductive plates. The second boundary condition is, therefore, automatically satisfied. Since these plates
serve the same purpose as the "b" dimension walls of a waveguide, the "a" dimension walls can be added without
affecting the magnetic or electric fields.
When a quarter-wavelength probe is inserted into a waveguide and
supplied with microwave energy, it will act as a quarter-wave vertical antenna. Positive and negative wavefronts
will be radiated, as shown in figure 1-24. Any portion of the wavefront traveling in the direction of arrow C will
rapidly decrease to zero because it does not fulfill either of the required boundary conditions. The parts of the
wavefronts that travel in the directions of arrows A and B will reflect from the walls and form reverse-phase
wavefronts. These two wavefronts, and those that follow, are illustrated in figure 1-25. Notice that the
wavefronts crisscross down the center of the waveguide and produce the same resultant field pattern that was shown
in figure 1-23.
Figure 1-24. - Radiation from probe placed in a waveguide.
Figure 1-25. - Wavefronts in a waveguide.
The reflection of a single wavefront off the "b" wall of a waveguide is shown in figure 1-26. The
wavefront is shown in view (A) as small particles. In views (B) and (C) particle 1 strikes the wall and is bounced
back from the wall without losing velocity. If the wall is perfectly flat, the angle at which it strikes the wall,
known as the angle of incidence ("), is the same as the angle of reflection (ø) and are measured perpendicular to
the waveguide surface. An instant after particle 1 strikes the wall, particle 2 strikes the wall, as shown in view
(C), and reflects in the same manner. Because all the particles are traveling at the same velocity, particles 1
and 2 do not change their relative position with respect to each other. Therefore, the reflected wave has the same
shape as the original. The remaining particles as shown in views (D), (E) and (F) reflect in the same manner. This
process results in a reflected wavefront identical in shape, but opposite in polarity, to the incident wave.
Figure 1-26. - Reflection of a single wavefront.
Figures 1-27A and 1-27B, each illustrate the direction of propagation of two different
electromagnetic wavefronts of different frequencies being radiated into a waveguide by a probe. Note that only the
direction of propagation is indicated by the lines and arrowheads. The wavefronts are at right angles to the
direction of propagation. The angle of incidence (") and the angle of reflection (ø) of the wavefronts vary in
size with the frequency of the input energy, but the angles of reflection are equal to each other in a waveguide.
The CUTOFF FREQUENCY in a waveguide is a frequency that would cause angles of incidence and reflection to be zero
degrees. At any frequency below the cutoff frequency, the wavefronts will be reflected back and forth across the
guide (setting up standing waves) and no energy will be conducted down the waveguide.
NEETS Table of Contents
- 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
- Introduction to Amplifiers
- Introduction to Wave-Generation and Wave-Shaping
- 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