Introduction To Modern Planar Transmission Lines. Anand K. Verma

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      The network also follows images. The S‐parameters are complex quantities. The S‐parameters are written in the phasor form: images, images and S12 = |S12| ej ϕ. From the above equation, the phase relation is obtained:

      (3.1.60)equation

      Therefore, once the complex S11 and S22 are measured, both the magnitude and phase of the S21 are determined. However, usually, both S11 and S21 are obtained from a VNA and also from the circuit simulator or EM‐simulator. The magnitude of S21 provides the insertion‐loss of the network and ϕ is the phase shift at the output of the network.

      Example 3.9

      Solution

      To compute S11 that is the reflection coefficient of a network under the matched condition, the port‐2 is terminated in Z0. Thus, Zin = Z + Z0 and the reflection coefficient at port‐1 is

Schematic illustration of network of series impedance.

      Likewise, to compute S22, the port‐1 is terminated in Z0. It gives Zout = Z + Z0 at the port‐2. The S22 is

      (3.1.62)equation

      The total port voltage at the port‐1 is a sum of the forward and reflected voltages:

equation

      To compute S21, i.e. the transmission coefficient from the port‐1 to the port‐2 under the matched termination, at first, the total port voltage at the port‐2 is obtained:

equation

      Therefore, from equations (i) and (ii):

equation

      However, the port voltage V2 computed from the port current is

equation

      Finally, S21 is obtained from equations :

      (3.1.64)equation

      The [S] matrix of the series impedance is

      (3.1.65)equation

      The attenuation and phase shift of a signal, applied at the input port‐1 of series impedance Z = R + jX, are computed below.

      (3.1.66)equation

      The lagging phase shift of the signal at the output port‐2, due to the series element, is

      (3.1.67)equation

      Example 3.10

      Solution

      The shunt admittance is Y = G + jB. To compute S11, the port‐2 is terminated in Z0 (=1/Y0) giving Yin = Y + Y0. The reflection coefficient of the shunt admittance under matched termination is

      (3.1.68)equation

      Likewise, to compute S22 of the shunt admittance, the port‐1 is terminated in Z0:

      (3.1.69)equation

      Following the previous case of the series impedance, the S21 is computed:

      images Fig (3.16) shows V1 = V2; therefore,

      (3.1.70)equation

Schematic illustration of network of shunt admittance.

      The [S] matrix of the shunt admittance is

      (3.1.71)equation

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