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Microwave Network Analysis

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Title: Microwave Network Analysis


1
Chapter 4
  • Microwave Network Analysis

2
Equivalent Voltage and Current
  • For non-TEM lines, the quantities of voltage,
    current, and impedance are not unique, and are
    difficult to measured. Following considerations
    can provide useful result
  • 1) Voltage and current are defined only for a
    particular mode, and are defined so that the
    voltage is proportional to the transverse
    electric field, and the current is proportional
    to transverse magnetic field.
  • 2) The product of equivalent voltage and current
    equals to the power flow of the mode.
  • 3) The ratio of the voltage to the current for a
    single traveling wave should be equal to the
    characteristic impedance of the line. This
    impedance is usually selected as equal to the
    wave impedance of the line.

3
The Concept of Impedance
  • Various types of impedance
  • 1) ?(?/?)1/2 intrinsic impedance of medium.
    This impedance is dependent only on the material
    parameters of medium, and is equal to the wave
    impedance of plane wave.
  • 2) ZwEt /Ht1/Yw wave impedance, e.g. ZTEM,
    ZTM, ZTE. It may depend on the type of line or
    guide, the material, and the operating frequency.
  • 3) Z0 (L /C)1/2 1/Y0 characteristic
    impedance. It is the ratio of voltage to current.
    The characteristic impedance is unique definition
    for TEM mode but not for TM or TE modes.
  • The real and imaginary parts of impedance and
    reflection coefficient are even and odd in ?0
    respectively.

4
Impedance and Admittance Matrices
  • The terminal plane (e.g. tN) is important in
    providing a phase reference for the voltage and
    current phasors.
  • At the nth terminal (reference) plane, the
    relations are given as
  • Reciprocal Networks
  • If the arbitrary network is reciprocal ( no
    active devices, ferrites, or plasmas), Y and
    Z are symmetric matrices .

5
  • Lossless Networks
  • If the arbitrary network is lossless, then the
    net real power delivered to the network must be
    zero. Thus

Example4.1 Find the Z parameters of the two-port
network?
Solution
6
The Scattering Matrices
  • The scattering parameter Sij is the transmission
    coefficient from j port to port i when all other
    ports are terminated in matched loads.
  • Z or Y ? S
  • S ? Z

7
Example4.2 Find the S parameters of the 3 dB
attenuator circuit?
Solution
A matched 3B attenuator with a 50 O
Characteristic impedance
8
  • Reciprocal Networks
  • Lossless Networks
  • No real power delivers to network.Besides
  • S is symmetric matrix

Example4.3 Determine if the network is
reciprocal, and lossless? If port 2 terminated
with a matched load, what is the return loss at
port 1? If port 2terminated with a short circuit,
what is the return loss seen at port 1?
Solution
  • Since S is not symmetric, the network is not
    reciprocal.
  • So the network is not lossless.

9
When port 2 terminated with a matched load,
?S110.15.
When port 2 terminated with a short circuit,
10
Summary
  • Reciprocal Networks (symmetric)
  • No active elements, no anisotropic material
  • Lossless Networks
  • No resistive material, no radiation
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