WAVEGUIDES Flashcards

(61 cards)

1
Q

use electromagnetic waves that travel through
air, space, transmission lines, and waveguides. Understanding these systems requires knowledge of how electromagnetic waves propagate in these
mediums.

A

Radio communication systems

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2
Q

become inefficient at high frequencies due to
increased losses, making waveguides a better alternative for microwave
signals.

A

Transmission lines

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3
Q

are hollow, conductive tubes—rectangular, elliptical, or
circular in shape—that confine the waves and minimize losses.

A

Waveguides

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4
Q

They act as
high-pass filters, only allowing frequencies above a certain cutoff to
propagate.

A

Waveguides

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5
Q

They’re impractical at low frequencies but ideal in the
gigahertz range and above.

A

Waveguides

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6
Q

Types of Waveguides

A

Rectangular
Circular
Elliptical

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7
Q

are a number of ways in which electrical energy can propagate along a waveguide

A

Modes

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8
Q

It requires a certain boundary condition, for instance:
there cannot be any electric field along the wall in ideal conductors for the waveguide.

A

Modes

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9
Q

It requires a certain boundary condition, for instance:
Voltage gradient along the wall would have to be needed but is impossible since there cannot be any voltage across a short circuit.

A

Modes

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10
Q

_______ in a waveguide can be understood by imagining waves as rays of light reflecting inside the guide

A

Modes

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11
Q

Each mode corresponds to a different reflection angle. As the angle increases, the ray travels a longer path, which slows down the effective velocity along the guide, even though the wave still moves at the speed of light.

A
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12
Q

Each mode in a waveguide has a cutoff
frequency below which it won’t propagate

A
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13
Q

Single-mode operation, known as the ________, which uses the lowest cutoff frequency

A

Dominant mode

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14
Q

operate between the cutoff of the dominant mode and the
next higher mode

A

Waveguides

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15
Q

are classified as transverse electric (TE) or transverse
magnetic (TM) based on the field patterns inside the guide.

A

Modes

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16
Q

occurs when multiple modes propagate through a waveguide at the same time. If a short pulse of microwave energy is sent into the waveguide, each mode travels at a slightly different speed, causing the pulse to arrive at the other end spread out over time

A

Dispersion

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17
Q

This spreading _______ can lead to signal distortion, especially if another pulse follows closely behind, as the overlapping pulses may interfere with each other

A

Dispersion

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18
Q

To avoid this, it’s best to operate the waveguide in single-mode, allowing only one mode to propagate and preserving the integrity of the signal.

A

Dispersion

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19
Q

In an air-filled rectangular waveguide, electromagnetic waves reflect off the walls rather than traveling straight, causing the signal to move at a slower pace than the speed of light. This slower speed is called _________, and it’s significantly less than the speed of light due to the zigzag path the wave takes.

A

group velocity

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20
Q

The variation in group velocity can be physically explained by the angle at which the wave reflects off the waveguide walls, which changes with frequency. Near the cutoff frequency, the wave bounces more frequently across the guide while covering the same distance along its length compared to higher frequencies.

A
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21
Q

It is often necessary to calculate the wavelength of a signal in a waveguide. For instance, it may be required for impedance matching. It might seem that the wavelength along the guide could be found using the group velocity, in much the same way that the velocity factor of a transmission line is used. However, this common-sense approach does not work because what is really important in impedance-matching calculations is the change in phase angle along the line.

A
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22
Q

refers to the rate at which the phase of a wave appears to move along a waveguide, and it can exceed the speed of light because it doesn’t represent the movement of any physical object or energy

A

Phase velocity

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23
Q

This is similar to how a water wave crest can appear to travel along the shore faster than the actual wave motion—it’s just an effect of the wave’s angle and not a true high-speed motion.

A

Phase velocity

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24
Q

Like any transmission line, a waveguide has a characteristic
impedance. Unlike wire lines, the _______ is a
function of frequency. You might expect that the impedance of a waveguide with an air dielectric would have some relationship to the impedance of free space, which is 377 Ω, and that is true.

A

waveguide impedance

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25
Techniques for matching impedances using waveguides also differ from those used with conventional transmission lines. Shorted stubs of adjustable length can be used, but a simpler method is to add capacitance or inductance by inserting a tuning screw into the guide. As the screw is inserted farther into the guide, the effect is first capacitive, then series-resonant, and finally inductive.
26
The three basic ways to launch a wave down a guide
- Probe - Loop - Hole
27
To launch a wave in one direction within a waveguide, a ______ is placed at an electric-field maximum— typically at the center of the wide dimension for the TE₁₀ mode—and positioned a quarter guidewavelength from the shorted end. This setup ensures that the reflected wave, after two 180° phase shifts, adds constructively to the forward wave.
probe
28
A _______ couples to the magnetic field in a waveguide and is placed where the magnetic field is strongest— near the end wall for the TE₁₀ mode. This is similar to how current peaks at the shorted end of a conventional transmission line, with magnetic and electric fields in the guide analogous to current and voltage, respectively.
loop
29
A _______ can be made in the waveguide to allow electromagnetic energy to enter or exit from the surrounding space. Since waveguides are reciprocal devices—like transmission lines—the same methods used to couple power into a waveguide can also be used to extract it
hole
30
use variations like two holes spaced a quarter-wavelength apart to ensure wave propagation in only one direction. This setup causes signals in the undesired direction to cancel due to a 180° phase difference, while allowing constructive interference in the desired direction. Additional holes can be used to enhance coupling, and resistive material absorbs unwanted signals at the end of the secondary guide.
Directional couplers
31
are characterized by their insertion loss, coupling, and directivity.
Directional couplers
32
All three are normally specified in decibels
insertion loss, coupling, and directivity
33
is the amount by which a signal in the main guide will be attenuated
insertion loss
34
gives the amount by which the signal in the main guide is greater than that coupled to the secondary waveguide
coupling specification
35
refers to the ratio between the power coupled to the secondary guide, for signals travelling in the two possible directions along the main guide
directivity
36
The use of waveguides requires redesign of some of the ordinary components that are used with feedlines. The lowly tee connector is an example. In addition, other components, such as resonant cavities, are too large to be practical at lower frequencies
37
Waveguide components
- Bends - TEES - Cavity Resonators
38
Changes in a waveguide’ s shape or size affect its internal electric and magnetic fields, potentially altering its characteristic impedance if the change is significant. However, gradual bends or twists have minimal impact.
BENDS
39
are classified as E-plane or H-plane, depending on whether they affect the direction of the electric or magnetic field, respectively, with reference to the TE₁₀ mode
BENDS
40
with its carefully designed gradual bends, resembles plumbing and is just as tricky to install
Rigid waveguide
41
is used for awkward installations
Flexible waveguide
42
like their transmission line counterparts, split a signal into two paths and come in E-plane and H-plane types
Waveguide tees
43
produces in-phase outputs
H-plane tee (shunt tee)
44
gives out-of-phase signals
E-plane tee (series tee)
45
combines both types, offering features like signal isolation—e.g., an input at one port results in outputs at two ports but none at a fourth, depending on the input configuration
hybrid or "magic" tee
46
is a short section where waves reflect back and forth. If its length is exactly half a wavelength, the reflections reinforce each other, creating resonance and a buildup of energy. This resonant behavior, like in other systems, is characterized by a high quality factor (Q), often in the thousands.
Waveguide Cavity or Cavity Resonators
47
can be tuned by adjusting their size, and various shapes exist beyond the rectangular type
Cavities
48
are widely used in microwave systems and even in VHF applications where high Q justifies their larger size
Resonant Cavities
49
At lower frequencies, loads and attenuators use resistors, but at microwave frequencies, traditional resistors become impractical due to unwanted inductance and capacitance.
50
use resistive materials like carbon to absorb energy
Waveguide Attenuators
51
Inserts a carbon vane into the guide
Flap Attenuator
52
varies loss based on the vane’s orientation to the electric field
Rotating Vane Attenuator
53
use carbon inserts to absorb energy without reflections
Terminating loads
54
also known as a dummy load
Waveguide Termination
55
is a component used in waveguide systems to absorb RF energy and prevent reflections. It's a resistive load matched to the waveguide's characteristic impedance, ensuring the waveguide operates effectively and prevents standing waves. This is crucial for maintaining signal integrity and overall system performance.
Waveguide Termination
56
are useful microwave components that generally use ferrites in their operation
Isolators and circulators
57
is a device that allows a signal to pass in only one direction. In the other direction, it is greatly attenuated
ISOLATOR
58
can be used to shield a source from a mismatched load. Energy will still be reflected from the load, but instead of reaching the source, the reflected power is dissipated in this component
ISOLATOR
59
is a multi-port device that directs signals from one port to the next in a counterclockwise direction, allowing signal separation. In a common three-port setup, a signal from port 1 goes only to port 2, and so on
CIRCULATOR
60
A typical use of this is as a transmit-receive switch, where it routes the transmitter output to the antenna and the received signal to the receiver, while preventing the strong transmit signal from damaging the receiver
CIRCULATOR
61
Isolators and Circulators Applications
- Optical Fiber - Waveguide Components for Medical Linear Accelerators - Photonic Integrated Circuits - Optical interferometers