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TRANSMISSION LINES
K.SARAVANA KUMAR
CONTENT
OVERVIEW1
HISTORY2
APPLICABILITY3
GENERALAPPLICATIONS4
OVERVIEW
5 Waveguide
4 Optical fibre
3 Strip line
2 Coaxial cable
1 Ladder line
HISTORY
 Mathematical Analysis Of The Behavior Of Electrical
Transmission Lines Grew Out Of The Work Of James
Clerk Maxwell, Lord Kelvin And Oliver Heaviside. In
1855 Lord Kelvin Formulated A Diffusion Model Of The
Current In A Submarine Cable.
 The Model Correctly Predicted The Poor Performance
Of The 1858 Trans-Atlantic Submarine Telegraph Cable.
In 1885 Heaviside Published The First Papers That
Described His Analysis Of Propagation In Cables And
The Modern Form Of The Telegrapher's Equations.
APPLICABILITY
The length of
the wires
connecting
the
components
can for the
most part be
ignored
He voltage on
the wire at a
given time
can be
assumed to
be the same
at all points
When the
voltage
changes in a
time interval
comparable to
the time it
takes for the
signal to travel
down the wire
A common rule
of thumb is
that the cable
or wire should
be treated as a
transmission
line if the
length is
greater than
1/10 of the
wavelength
4 Cases
Special case of a
lossless line
The elements R and G are negligibly
small
General case of a
line with losses
In the general case the loss terms r and g are
both included
Matched load
The load impedance is equal to the characteristic
impedance of the line
Short
The input impedance is purely imaginary
and a periodic function of position and
wavelength (frequency)
5 Outcomes from an Event
TWISTED PAIR Telecommunication
STAR QUAD Microphone cables
Twin-lead Lower resistive losses
Lecher lines
UHF for creating
resonant circuits
Single-wire line Telegraph transmission
General applications
Signal transfer
Widely used to
transmit high
frequency
signals
Pulse generation
charging the
transmission
line and then
discharging it
into load.
Stub filters
Wired in
parallel with a
line used to
transfer signals
K. SARAVANA KUMAR
+91-9944773483
ksaravana636@gmail.
com
Saravjc

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Saravjc

  • 4. 5 Waveguide 4 Optical fibre 3 Strip line 2 Coaxial cable 1 Ladder line
  • 5. HISTORY  Mathematical Analysis Of The Behavior Of Electrical Transmission Lines Grew Out Of The Work Of James Clerk Maxwell, Lord Kelvin And Oliver Heaviside. In 1855 Lord Kelvin Formulated A Diffusion Model Of The Current In A Submarine Cable.  The Model Correctly Predicted The Poor Performance Of The 1858 Trans-Atlantic Submarine Telegraph Cable. In 1885 Heaviside Published The First Papers That Described His Analysis Of Propagation In Cables And The Modern Form Of The Telegrapher's Equations.
  • 6.
  • 7. APPLICABILITY The length of the wires connecting the components can for the most part be ignored He voltage on the wire at a given time can be assumed to be the same at all points When the voltage changes in a time interval comparable to the time it takes for the signal to travel down the wire A common rule of thumb is that the cable or wire should be treated as a transmission line if the length is greater than 1/10 of the wavelength
  • 8. 4 Cases Special case of a lossless line The elements R and G are negligibly small General case of a line with losses In the general case the loss terms r and g are both included Matched load The load impedance is equal to the characteristic impedance of the line Short The input impedance is purely imaginary and a periodic function of position and wavelength (frequency)
  • 9.
  • 10. 5 Outcomes from an Event TWISTED PAIR Telecommunication STAR QUAD Microphone cables Twin-lead Lower resistive losses Lecher lines UHF for creating resonant circuits Single-wire line Telegraph transmission
  • 11.
  • 12. General applications Signal transfer Widely used to transmit high frequency signals Pulse generation charging the transmission line and then discharging it into load. Stub filters Wired in parallel with a line used to transfer signals
  • 13.