EE316 Microwave Engineering

Lab 4: Design of impedance transformers

记录微波作业,从我做起????
这次作业需要查阅一篇论文、具体需要的部分在theory部分已经给出。

Problem.

Design impedance transformers to match a source of 50 Ω 50\Omega 50Ω to a load of 110 Ω 110\Omega 110Ω at a frequency of 2 G H z 2GHz 2GHz (See the attached paper). Plot the simulated S-parameter.

Solution.

1. Theory.

In order to design an impedance transformer with wide-band, maximally flat real-to-real impedance
matching, we consider the following two-section quarter-wave transformer: [ 1 ] {}^{[1]} [1]

[ADS] Design of impedance transformers
Fig.1 Two-section quarter-wave transformer

In Fig.1, we have following parameters:

1️⃣ f 0 f_0 f0 is the center frequency at which electrical length of two transmission lines Z 1 Z_1 Z1 and Z 2 Z_2 Z2 is equal to 9 0 ∘ 90^{\circ} 90 ;
2️⃣ R L R_L RL is the load impedance, Z L Z_L ZL is is the impedance seen at the input of the transmission line;
3️⃣ Z i n Z_{in} Zin is the input impedance, and Z i n Z_{in} Zin equals to Z 0 Z_0 Z0 at the center frequency f 0 f_0 f0;

There is a formula to calculate Z 1 Z_1 Z1 and Z 2 Z_2 Z2: [ 1 ] {}^{[1]} [1]
Z 0 = Z 1 2 R L Z 2 2 (1) Z_0=\frac{Z_1^2R_L}{Z_2^2}\tag{1} Z0=Z22Z12RL(1)

Z 1 = Z 0 2 1 + 1 k 1 + k (2) Z_{1} = {Z_{0}\over\sqrt{2}}{1 + {1\over\sqrt{k}}\over\sqrt{1 + \sqrt{k}}}\tag{2} Z1=2 Z01+k 1+k 1(2)

Z 2 = Z 1 k (3) Z_{2} = {Z_{1}\over\sqrt{k}}\tag{3} Z2=k Z1(3)

where k is the ratio of Z 0 Z_0 Z0 and R L R_L RL such that :
k = Z 0 / R L (4) k=Z_0/R_L\tag{4} k=Z0/RL(4)

2. Simulation.

A. Simulation settings:

  • Set f 0 = 2 G H z f_0=2GHz f0=2GHz, Z 0 = 50 Ω Z_0=50\Omega Z0=50Ω, R L = 110 Ω R_L=110\Omega RL=110Ω.

  • According to equation ( 1 ) (1) (1) to ( 4 ) (4) (4), we have:
    k = Z 0 / R L = 5 11 Z 1 = Z 0 2 1 + 1 k 1 + k = 50 2 1 + 1 5 / 11 1 + 5 / 11 = 67.85314747 Ω Z 2 = Z 1 k = 100.642819 Ω \begin{aligned} k&=Z_0/R_L=\frac{5}{11}\\ Z_1&={Z_{0}\over\sqrt{2}}{1 + {1\over\sqrt{k}}\over\sqrt{1 + \sqrt{k}}}={50\over\sqrt{2}}{1 + {1\over\sqrt{5/11}}\over\sqrt{1 + \sqrt{5/11}}}=67.85314747\Omega\\ Z_2&={Z_{1}\over\sqrt{k}}=100.642819\Omega \end{aligned} kZ1Z2=Z0/RL=115=2 Z01+k 1+k 1=2 501+5/11 1+5/11 1=67.85314747Ω=k Z1=100.642819Ω

  • Substrate Properties:

    Dielectric constant Substrate thickness Loss tangent Copper thickness
    2.2 2.2 2.2 0.508 m m 0.508 mm 0.508mm 0.0009 0.0009 0.0009 0.018 m m 0.018mm 0.018mm
Table.1 Substrate Properties

B. ADS Design:

  • Set substrate and conductor parameters in MSUB according to table 1.
  • Use Line Calculator to synthesize the width and Length of transmission lines Z 1 Z_1 Z1 and Z 2 Z_2 Z2:
    • Width of Z 1 Z_1 Z1: 0.936261 m m 0.936261 mm 0.936261mm; Length of Z 1 Z_1 Z1: 27.805300 m m 27.805300 mm 27.805300mm;
    • Width of Z 2 Z_2 Z2: 0.421578 m m 0.421578 mm 0.421578mm; Length of Z 2 Z_2 Z2: 28.395000 m m 28.395000 mm 28.395000mm;
[ADS] Design of impedance transformers[ADS] Design of impedance transformers
Fig.2 Line Calculator result
  • Schematic considered in this lab:

[ADS] Design of impedance transformers

Fig.3 Circuit Schematic
  • Plot of S parameters:

[ADS] Design of impedance transformers

Fig.4 Rectangular Plot of S Parameter
  • Analysis: When frequency equals 2.0 G H z 2.0GHz 2.0GHz, it could be seen that S ( 1 , 1 ) ≪ − 30 d B S(1,1)\ll -30dB S(1,1)30dB , and S ( 1 , 2 ) ≈ 0 d B S(1,2)\approx0dB S(1,2)0dB. In other word, the design of impedance transformer is quite successful.

Reference

[1] R. Darraji, M. M. Honari, R. Mirzavand, F. M. Ghannouchi and P. Mousavi, “Wideband Two-Section Impedance Transformer With Flat Real-to-Real Impedance Matching,” in IEEE Microwave and Wireless Components Letters, vol. 26, no. 5, pp. 313-315, May 2016, doi: 10.1109/LMWC.2016.2548997.

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