Module 11—Microwave Principles
Pages i - ix
1-1 to 1-10
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1-21 to 1-30
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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
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AI-1 to AI-6
, Index-1 to Index-2
Assignment 1 - 1-8
Assignment 2 - 9-16
wide range of RF frequencies if it is terminated in the characteristic impedance of the line.
The electromagnetic waves traveling down the line produce electric fields that interact with the electrons of the
If the electrons of the beam were accelerated to travel faster than the waves traveling on the wire, bunching
would occur through the effect of velocity modulation. Velocity modulation would be caused by the interaction
between the traveling-wave fields and the electron beam. Bunching would cause the
electrons to give up energy
to the traveling wave if the fields were of the correct polarity to slow down the bunches. The energy from the
bunches would increase the amplitude of the traveling wave in a progressive action that would take place all along
the length of the TWT, as shown in figure 2-14.
Figure 2-14.—Simplified TWT.
However, because the waves travel along the wire at the speed of light, the simple TWT shown in figure 2-14
will not work. At present no way is known to accelerate an electron beam to the speed of light. Since the electron
beam cannot travel faster than the wave on the wire, bunching will not take place and the tube will not work. The
TWT is therefore designed with a delay structure to slow the traveling wave down to or below the speed of the
electrons in the beam. A common TWT delay structure is a wire, wound in the form of a long coil or helix, as shown
in figure 2-15, view (A). The shape of the helix slows the effective velocity of the wave along the common axis of
the helix and the tube to about one-tenth the speed of light. The wave still travels down the helix wire at the
speed of light, but the coiled shape causes the wave to travel a much greater total distance than the electron
beam. The speed at which the wave travels down the tube can be varied by changing the number of turns or the
diameter of the turns in the helix wire. The helical delay structure works well because it has the added advantage
of causing a large proportion of electric fields that are parallel to the electron beam. The parallel fields
provide maximum interaction between the fields and the electron beam.
Figure 2-15.—Functional diagram of a TWT.
In a typical TWT, the electron beam is directed down the center of the helix while, at the same time, an
RF signal is coupled onto the helix. The electrons of the beam are velocity-modulated by the electric fields
produced by the RF signal.
Amplification begins as the electron bunches form and release energy to the
signal on the helix. The slightly amplified signal causes a denser electron bunch which, in turn, amplifies the
signal even more. The amplification process is continuous as the RF wave and the electron beam travel down the
length of the tube.
Any portion of the TWT output signal that reflects back to the input will cause oscillations within the
tube which results in a decrease in amplification. Attenuators are placed along the length of the helix to prevent
reflections from reaching the input. The attenuator causes a loss in amplitude, as can be seen in figure 2-15,
view (B), but it can be placed so as to minimize losses while still isolating the input from the output.
The relatively low efficiency of the TWT partially offsets the advantages of high gain and wide bandwidth. The
internal attenuator reduces the gain of the tube, and the power required to energize the focusing magnet is an
operational loss that cannot be recovered. The TWT also produces heat which must be dissipated by either
air-conditioning or liquid-cooling systems. All of these factors reduce the overall efficiency of the TWT, but the
advantages of high gain and wide bandwidth are usually enough to overcome the disadvantages.
The Backward-Wave Oscillator
The BACKWARD-WAVE OSCILLATOR (BWO) is a microwave-frequency, velocity-modulated tube that operates on the
same principle as the TWT. However, a traveling wave that moves from the
electron gun end of the tube toward the collector is not used in the BWO. Instead, the BWO extracts energy
from the electron. beam by using a backward wave that travels from the collector toward the electron gun
(cathode). Otherwise, the electron bunching action and energy extraction from the electron beam is very similar to
the actions in a TWT.
The typical BWO is constructed from a folded transmission line or waveguide that
winds back and forth across the path of the electron beam, as shown in figure 2-16. The folded waveguide in the
illustration serves the same purpose as the helix in a TWT. The fixed spacing of the folded waveguide limits the
bandwidth of the BWO. Since the frequency of a given waveguide is constant, the frequency of the BWO is controlled
by the transit time of the electron beam. The transit time is controlled by the collector potential. Thus, the
output frequency can be changed by varying the collector voltage, which is a definite advantage. As in the TWT,
the electron beam in the BWO is focused by a magnet placed around the body of the tube.
Figure 2-16.—Typical BWO.
Q-26. What is the primary use of the TWT?
Q-27. The magnet surrounding the body of a TWT serves
Q-28. How are the input and output directional couplers in a TWT connected to the helix?
Q-29. What relationship must exist between the electron beam and the traveling wave for bunching to occur in
the electron beam of a TWT?
Q-30. What structure in the TWT delays the forward progress of the traveling
wave? The Magnetron
The MAGNETRON, shown in figure 2-17A, is a
self-contained microwave oscillator that operates differently from the linear-beam tubes, such as the TWT and the
klystron. Figure 2-17B is a simplified drawing of the magnetron. CROSSED-ELECTRON and MAGNETIC fields are used in
the magnetron to produce the high-power output required in radar and communications equipment.
The magnetron is classed as a diode because it has no grid. A magnetic field located in the space between
the plate (anode) and the cathode serves as a grid. The plate of a magnetron does not have the same physical
appearance as the plate of an ordinary electron tube. Since conventional inductive- capacitive (LC) networks
become impractical at microwave frequencies, the plate is fabricated into a cylindrical copper block containing
resonant cavities which serve as tuned circuits. The magnetron base differs considerably from the conventional
tube base. The magnetron base is short in length and has large diameter leads that are carefully sealed into the
tube and shielded.
The cathode and filament are at the center of the tube and are supported by the
filament leads. The filament leads are large and rigid enough to keep the cathode and filament structure fixed in
output lead is usually a probe or loop extending into one of the tuned cavities and coupled into a
waveguide or coaxial line. The plate structure, shown in figure 2-18, is a solid block of copper. The cylindrical
holes around its circumference are resonant cavities. A narrow slot runs from each cavity into the central portion
of the tube dividing the inner structure into as many segments as there are cavities. Alternate segments are
strapped together to put the cavities in parallel with regard to the output. The cavities control the output
frequency. The straps are circular, metal bands that are placed across the top of the block at the entrance slots
to the cavities. Since the cathode must operate at high power, it must be fairly large and must also be able to
withstand high operating temperatures. It must also have good emission characteristics, particularly under return
bombardment by the electrons. This is because most of the output power is provided by the large number of
electrons that are emitted when high-velocity electrons return to strike the cathode. The cathode is indirectly
heated and is constructed of a high- emission material. The open space between the plate and the cathode is called
the INTERACTION SPACE. In this space the electric and magnetic fields interact to exert force upon the electrons.
Figure 2-18.—Cutaway view of a magnetron.
The magnetic field is usually provided by a strong, permanent magnet mounted around the magnetron so that
the magnetic field is parallel with the axis of the cathode. The cathode is mounted in the center of the
BASIC MAGNETRON OPERATION.—Magnetron theory of operation is based on the motion of
electrons under the influence of combined electric and magnetic fields. The following information presents the
laws governing this motion.
The direction of an electric field is from the positive electrode to the
negative electrode. The law governing the motion of an electron in an electric field (E field) states:
force exerted by an electric field on an electron is proportional to the strength of the field. Electrons tend to
move from a point of negative potential toward a positive potential.
This is shown in figure 2-19. In other words, electrons tend to move against the E field. When an
electron is being accelerated by an E field, as shown in figure 2-19, energy is taken from the field by the
Figure 2-19.—Electron motion in an electric field.
The law of motion of an electron in a magnetic field (H field) states:
The force exerted on an
electron in a magnetic field is at right angles to both the field and the path of the electron. The direction of
the force is such that the electron trajectories are clockwise when viewed in the direction of the magnetic field.
This is shown in figure 2-20.
Figure 2-20.—Electron motion in a magnetic field.
In figure 2-20, assume that a south pole is below the figure and a north pole is above the figure so that
the magnetic field is going into the paper. When an electron is moving through space, a magnetic field builds
around the electron just as it would around a wire when electrons are flowing through a wire. In figure 2-20 the
magnetic field around the moving electron adds to the permanent magnetic field on the
left side of the electron's path and subtracts from the permanent magnetic field on the right side.
This action weakens the field on the right side; therefore, the electron path bends to the right (clockwise). If
the strength of the magnetic field is increased, the path of the electron will have a sharper bend. Likewise, if
the velocity of the electron increases, the field around it increases and the path will bend more sharply.
A schematic diagram of a basic magnetron is shown in figure 2-21A. The tube consists of a cylindrical plate with a
cathode placed along the center axis of the plate. The tuned circuit is made up of cavities in which oscillations
take place and are physically located in the plate.
When no magnetic field exists, heating the cathode
results in a uniform and direct movement of the field from the cathode to the plate, as illustrated in figure
2-21B. However, as the magnetic field surrounding the tube is increased, a single electron is affected, as shown
in figure 2-22. In figure 2-22, view (A), the magnetic field has been increased to a point where the electron
proceeds to the plate in a curve rather than a direct path.
Figure 2-21A.—Basic magnetron. SIDE VIEW.
Figure 2-21B.—Basic magnetron. END VIEW OMITTING MAGNETS.
Figure 2-22.—Effect of a magnetic field on a single electron.
In view (B) of figure 2-22, the magnetic field has reached a value great enough to cause the electron to just
miss the plate and return to the filament in a circular orbit. This value is the CRITICAL VALUE of field strength.
In view (C), the value of the field strength has been increased to a point beyond the critical value; the electron
is made to travel to the cathode in a circular path of smaller diameter.
View (D) of figure 2-22. shows
how the magnetron plate current varies under the influence of the varying magnetic field. In view (A), the
electron flow reaches the plate, so a large amount of plate current is flowing. However, when the critical field
value is reached, as shown in view (B), the electrons are deflected away from the plate and the plate current then
drops quickly to a very small value. When the field strength is made still greater, as shown in view (C), the
plate current drops to zero.
When the magnetron is adjusted to the cutoff, or critical value of the plate
current, and the electrons just fail to reach the plate in their circular motion, it can produce oscillations at
microwave frequencies. These oscillations are caused by the currents induced electrostatically by the moving
electrons. The frequency is determined by the time it takes the electrons to travel from the cathode toward the
plate and back again. A transfer of microwave energy to a load is made possible by connecting an external circuit
between the cathode and the plate of the magnetron. Magnetron oscillators are divided into two classes:
NEGATIVE-RESISTANCE and ELECTRON-RESONANCE MAGNETRON OSCILLATORS.
A negative-resistance magnetron oscillator is operated by a static negative resistance between its
electrodes. This oscillator has a frequency equal to the frequency of the tuned circuit connected to the tube.
An electron-resonance magnetron oscillator is operated by the electron transit time required for electrons to
travel from cathode to plate. This oscillator is capable of generating very large peak power outputs at
frequencies in the thousands of megahertz. Although its average power output over a period of time is low, it can
provide very high-powered oscillations in short bursts of pulses.
Q-31. The folded waveguide in a BWO
serves the same purpose as what component in a TWT?
Q-32. What serves as a grid in a magnetron?
Q-33. A cylindrical copper block with resonant
cavities around the circumference is used as what component of a magnetron?
Q-34. What controls the
output frequency of a magnetron?
Q-35. What element in the magnetron causes the curved path of electron
Q-36. What is the term used to identify the amount of field strength required to cause the
electrons to just miss the plate and return to the filament in a circular orbit?
Q-37. A magnetron will
produce oscillations when the electrons follow what type of path? NEGATIVE-RESISTANCE
.—The split-anode, negative-resistance magnetron is a variation of the basic magnetron which
operates at a higher frequency. The negative-resistance magnetron is capable of greater power output than the
basic magnetron. Its general construction is similar to the basic magnetron except that it has a split plate, as
shown in figure 2-23A and B. These half plates are operated at different potentials to provide an electron motion,
as shown in figure 2-24. The electron leaving the cathode and progressing toward the high-potential plate is
deflected by the magnetic field and follows the path shown in figure 2-24. After passing the split between the two
plates, the electron enters the electrostatic field set up by the lower-potential plate.
Figure 2-23A.—Split-anode magnetron.
Figure 2-23B.—Split-anode magnetron.
Figure 2-24.—Movement of an electron in a split-anode magnetron.
Here the magnetic field has more effect on the electron and deflects it into a tighter curve. The
electron then continues to make a series of loops through the magnetic field and the electric field until it
finally arrives at the low-potential plate.
Oscillations are started by applying the proper magnetic field
to the tube. The field value required is slightly higher than the critical value. In the split-anode tube, the
critical value is the field value required to cause all the electrons to miss the plate when its halves are
operating at the same potential. The alternating voltages impressed on the plates by the oscillations generated in
the tank circuit will cause electron motion, such as that shown in figure 2-24, and current will flow. Since a
very concentrated magnetic field is required for the negative-resistance magnetron oscillator, the length of the
tube plate is limited to a few centimeters to keep the magnet at reasonable dimensions. In addition, a small
diameter tube is required to make the magnetron operate efficiently at microwave frequencies. A heavy-walled plate
is used to increase the radiating properties of the tube. Artificial cooling methods, such as forced-air or
water-cooled systems, are used to obtain still greater dissipation in these high-output tubes.
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