MATCHING TRANSMISSION LINE Flashcards

(64 cards)

1
Q

is crucial for efficient power transfer and minimal
signal reflection.

A

Matching transmission lines

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2
Q

When transmission lines are mismatched, power loss occurs
due to

A

standing waves

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3
Q

maximizes power transfer from the source to the load,
minimizing reflections that could distort the signal.

A

Impedance matching

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4
Q

are widely used in communication systems to transmit electrical signals.

A

Metallic cables

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5
Q

The primary types of metallic cables include:

A

Coaxial Cable
Twisted Pair Cable
Power Cables

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6
Q

Consists of a central conductor, insulating dielectric, metallic shield, and outer insulating jacket. It offers high bandwidth and resistance to electromagnetic
interference

A

Coaxial Cable

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7
Q

Comprises pairs of insulated copper wires twisted together. It’s cost- effective and commonly used in telephone and Ethernet networks

A

Twisted Pair Cable

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8
Q

Used for electrical power transmission, these cables are typically thicker and insulated for high-voltage applications

A

Power Cables

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9
Q

The inherent impedance of a transmission line,
determined by its geometry and the properties of the dielectric material

A

Characteristic Impedance (Z₀)

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10
Q

The speed at which a signal propagates along the transmission line, influenced by the dielectric constant of the insulating material.

A

Propagation Velocity (v)

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11
Q

Why is Impedance Matching Important?

A
  1. Minimizes Signal Reflection
  2. Maximizes Power Transfer
  3. Reduces Signal Distortion and Noise
  4. Improving System Efficiency
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12
Q

Impedance Matching Networks

A

L-Network
T-Network
Pi-Network

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13
Q

It is a basic impedance-matching circuit made up of two passive components, one in series
and one in parallel.

A

L-Network

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14
Q

widely used in RF circuits, audio systems,
and power electronics to optimize power transfer and minimize signal reflection between a
source and a load.

A

L-Network

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15
Q

Types of L-Networks

A

Low-Pass L-Network
High-Pass L-Network

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16
Q

Uses an inductor and a capacitor to pass low-frequency signals while blocking high frequencies, often used in RF applications

A

Low-Pass L-Network

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17
Q

Uses a capacitor and an inductor in the opposite configuration to allow high-frequency
signals to pass while blocking low frequencies

A

High-Pass L-Network

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18
Q

It is an electrical circuit configuration used for impedance matching, filtering, and attenuation. It
consists of three passive components typically resistors, capacitors, or inductors arranged in the
shape of the letter “T”

A

T-Network

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19
Q

Types of T-Networks

A

Low-Pass T-Network
High-Pass T-Network
Attenuator T-Network
Balanced T-Network

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20
Q

Uses two inductors in series and a capacitor in
parallel to allow low frequencies while blocking
high frequencies

A

Low-Pass T-Network

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21
Q

Uses two capacitors in series and an inductor in
parallel to pass high frequencies while blocking low
frequencies.

A

High-Pass T-Network

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22
Q

Uses resistors to reduce signal strength while maintaining
impedance matching, often used in RF and audio
applications

A

Attenuator T-Network

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23
Q

A symmetrical version used for balanced signal
transmission, minimizing distortion and interference.

A

Balanced T-Network

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24
Q

A symmetrical arrangement of three components (inductors or capacitors) with one in series and
two in shunt, offering wider bandwidth matching capabilities. Moreover, It is an electrical circuit
used for impedance matching, filtering, and signal attenuation

A

Pi-Network

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25
Types of T-Networks
Low-Pass Pi-Network High-Pass Pi-Network Attenuator Pi-Network
26
Uses two capacitors in parallel with an inductor in series to allow low frequencies to pass while blocking high frequencies.
Low-Pass Pi-Network
27
Uses two inductors in parallel with a capacitor in series to pass high frequencies while blocking low frequencies
High-Pass Pi-Network
28
Uses resistors to reduce signal strength while maintaining impedance matching, often used in RF circuits.
Attenuator Pi-Network
29
A special transmission line section of λ/4 (one-quarter of the wavelength) helps match different impedances.
Quarter-Wave Transformer
30
Open or short-circuited transmission line segments (stubs) provide impedance tuning.
Stub Matching
31
Uses one stub to achieve impedance matching
Single stub
32
More flexible, uses two adjustable stubs
Double stub
33
Convert between balanced and unbalanced lines or step-up/down impedance levels. Commonly used when connecting a coaxial cable to a balanced antenna system
Baluns and Transformers
34
- A graphical method for impedance matching. - Helps visualize impedance transformation and find solutions easily. - Used to design stub matching and L-networks.
Smith Chart Matching
35
is defined as the ratio of the maximum voltage to the minimum voltage or the maximum current to the minimum current of a standing wave on a transmission line.
STANDING WAVE RATIO (SWR)
36
SWR is often called the
voltage standing-wave ratio (VSWR)
37
Indicates the severity of impedance mismatch
STANDING WAVE RATIO (SWR)
38
Applications in Telecommunications
1. RF and Microwave Circuits 2. Optical Fiber Communications 3. Wireless Networks
39
Key points to remember
The choice of matching network depends on the desired impedance transformation, frequency range, and desired power handling capabilities. Impedance matching is crucial in telecommunications to minimize signal reflections and maximize power transfer from the source to the load.
40
must be used for long lines, high frequencies, or a combination of the two.
transmission line techniques
41
if a line is longer than about one-sixteenth of the signal wavelength, it should be considered a
transmission line
42
When Zo = ZL all the incident power is absorbed by the load. This is called a
matched line
43
When Zo ≠ ZL some of the incident power is absorbed by the load, and some is returned (reflected) to the source. This is called an
unmatched or mismatched line
44
With a mismatched line, there are two electromagnetic waves, traveling in opposite directions, present on the line at the same time (these waves are in fact called ______)
traveling waves
45
The two traveling waves set up an interference pattern known as a
standing wave
46
has minima (nodes) separated by a half wavelength of the traveling waves and maxima (antinodes) also separated by a half wavelength
standing wave
47
is a vector quantity that represents the ratio of reflected voltage to incident voltage or reflected current to incident current
reflection coefficient (sometimes called the coefficient of reflection)
48
can cause the power delivered to the load to be less than it would be with a matched line for the same source because some of the power is reflected back to the source
Reflections
49
travels through a waveguide in different modes, each following specific boundary conditions, where no electric field can exist along ideal conductor walls.
Electrical energy
50
propagates near the speed of light, but the increased path length reduces its effective velocity.
Energy
51
has the lowest cutoff frequency, should be used to prevent dispersion, with modes classified as transverse electric (TE) or transverse magnetic (TM), depending on field orientation
dominant mode
52
In an air-filled waveguide, the wave propagates at the speed of light but does not travel in a straight line; instead, it reflects back and forth off the walls. This reflection affects the actual speed at which the signal moves along the waveguide, known as
group velocity
53
is inefficient at low frequencies but highly effective in the microwave range
waveguide
54
are the recommended transmission lines for microwave systems operating between 1.7 GHz and 23.6 GHz, with an elliptical cross section ideal for minimizing VSWR and eliminating signal distortion
Elliptical waveguides
55
are ideal for rotating antennas, such as those used in radar systems, due to their symmetrical design
Circular waveguides
56
is essential for efficient energy transfer in microwave and optical communication systems
Coupling power into and out of waveguides
57
Uses a metallic probe (antenna-like structure) inserted into the waveguide to interact with the electric field of the guided wave.
Probe Coupling (Electric Field Coupling)
58
Uses a small wire loop to couple power to the magnetic field inside the waveguide
Loop Coupling (Magnetic Field Coupling)
59
is made in the waveguide wall to allow electromagnetic waves to pass between adjacent waveguides or between a waveguide and free space
Aperture Coupling (Hole or Slot Coupling)
60
Adjusts impedance by using a section of waveguide or transmission line with specific length and properties
Quarter-wavelength transformers
61
Short or open-circuited stubs adjust phase and impedance
Matching stubs
62
Used in optical waveguides to transition between different refractive indices
Dielectric matching layers
63
63
Ensure smooth transitions between different waveguide modes to minimize losses
Mode converters