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The Complex
Reflection Coefficient
Parameters Plotted on SMITH CHART
โžข Paraneters plotted on the Smith Chart include the following:
โ Reflection coefficient magnitude ,ฮ“
โ Reflection coefficient phase angle ,Q
โ Lenght of transmission line between any two points in wavelength
โ VSWR
โ Input Impedance Zin
โ The location of Vmax and Vmin (dmax - dmin)
Imaging of a transmission line in a microwave circuit
TRANSMISSION STATISTICS AND
TRANSMISSION STATISTICS EQUATIONS
The impedance
properties of
conductors can
not be neglected
The voltage values on a transmission line in microwave frequencies
When the source is open
When connected to the source ZL
load,
Voltage source equivalentIf the ZL load is short-circuited
n =integer
Input impedance of a transmission line
LOSSLESS TRANSMISSION LINES
This equation gives a first
order differential equation
for voltage.
This equation gives a first order differential equation for
curret.
General solution for voltage
equation is ;
Here, the propagation
constant of the waveguide,
By differentiating the result obtained
for the voltage
We can take the new
coordinate variable d= -z
the voltage load reflection coefficient;
Thus, line equations
SHORT CIRCUIT (ZL=0) TRANSMISSION LINE
Due to the short circuit,
the load limit V (0) = 0
and as a result
Thus, the phasor of the line voltage
Thus, line impedance;
ZL = 0
Tangent function will vary between (-โˆž) and (โˆž)
OPEN CIRCUIT (ZL = โˆž) TRANSMISSION M
HATTI
Because of the open circuit, the load
limit condition is I (0) = 0,
Thus, the line current phase
image
Thus, line voltage;
since the impedance function is
also periodic, the impedance will
repeat the behavior identical at
every lambda / 2 distance.
Cotanjant function will vary between (-โˆž) and (โˆž)
Standing Wave
SW represents the maximum value of
the voltage or current that occurs at
each point of the transmission line.
Incoming and reflected waves.Due to the structure and destructive
interventions, it is repeated in space with the ฮป / 2 period.
Generalized reflection coefficient,
The amplitude of an exponential
term with an image argument is
always one (Maximum)
Minimum point
( ZL=Z0)
If the load impedance is real and
ZL> Z0, the VDD pattern starts with
a maximum at load
If the load impedance is real and Z
<Z0, the VDD pattern begins with a
minimum of load
VSWR(VOLATGE STANDING WAVE)
That is, an indicator of maximum energy transfer and is denoted by the letter S.
If the load impedance is perfectly matched to the transmission line;
If the load is terminated by short circuit, open circuit or pure reactance
PHASE
For inductive reactance, the nearest extremity
is the dot voltage maximum, the phase of the
reflection coefficient
For capacitive reactance, the nearest extremity
is the dot voltage minimum, the phase of the
reflection coefficient
The complex reflection coefficient

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The complex reflection coefficient

  • 2. Parameters Plotted on SMITH CHART โžข Paraneters plotted on the Smith Chart include the following: โ Reflection coefficient magnitude ,ฮ“ โ Reflection coefficient phase angle ,Q โ Lenght of transmission line between any two points in wavelength โ VSWR โ Input Impedance Zin โ The location of Vmax and Vmin (dmax - dmin)
  • 3. Imaging of a transmission line in a microwave circuit
  • 4. TRANSMISSION STATISTICS AND TRANSMISSION STATISTICS EQUATIONS The impedance properties of conductors can not be neglected The voltage values on a transmission line in microwave frequencies
  • 5. When the source is open When connected to the source ZL load, Voltage source equivalentIf the ZL load is short-circuited
  • 6. n =integer Input impedance of a transmission line
  • 7. LOSSLESS TRANSMISSION LINES This equation gives a first order differential equation for voltage. This equation gives a first order differential equation for curret.
  • 8. General solution for voltage equation is ; Here, the propagation constant of the waveguide, By differentiating the result obtained for the voltage
  • 9. We can take the new coordinate variable d= -z
  • 10. the voltage load reflection coefficient; Thus, line equations
  • 11.
  • 12. SHORT CIRCUIT (ZL=0) TRANSMISSION LINE Due to the short circuit, the load limit V (0) = 0 and as a result Thus, the phasor of the line voltage
  • 14. Tangent function will vary between (-โˆž) and (โˆž)
  • 15. OPEN CIRCUIT (ZL = โˆž) TRANSMISSION M HATTI Because of the open circuit, the load limit condition is I (0) = 0,
  • 16. Thus, the line current phase image Thus, line voltage; since the impedance function is also periodic, the impedance will repeat the behavior identical at every lambda / 2 distance.
  • 17. Cotanjant function will vary between (-โˆž) and (โˆž)
  • 18. Standing Wave SW represents the maximum value of the voltage or current that occurs at each point of the transmission line. Incoming and reflected waves.Due to the structure and destructive interventions, it is repeated in space with the ฮป / 2 period. Generalized reflection coefficient, The amplitude of an exponential term with an image argument is always one (Maximum) Minimum point
  • 19. ( ZL=Z0) If the load impedance is real and ZL> Z0, the VDD pattern starts with a maximum at load If the load impedance is real and Z <Z0, the VDD pattern begins with a minimum of load
  • 20.
  • 21. VSWR(VOLATGE STANDING WAVE) That is, an indicator of maximum energy transfer and is denoted by the letter S. If the load impedance is perfectly matched to the transmission line; If the load is terminated by short circuit, open circuit or pure reactance
  • 22. PHASE For inductive reactance, the nearest extremity is the dot voltage maximum, the phase of the reflection coefficient For capacitive reactance, the nearest extremity is the dot voltage minimum, the phase of the reflection coefficient