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CHAPTER 5 Impedance Matching and Smith Chart

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5-19<br />

Microstrip Line <strong>Matching</strong> Networks (Ludwig P431)<br />

<br />

In the mid-GHz <strong>and</strong> higher frequency range, the wavelength becomes<br />

sufficiently small <strong>and</strong> the distributed components are widely used. Also, the<br />

discrete R/L/C lumped elements will have more noticeable parasitic effects (see<br />

chapter 2) <strong>and</strong> let to complicating the circuit design process<br />

Distributed componenets (such as transmission line segments) can be used<br />

to mix with lumped elements<br />

From Discrete Components to Microstrip Lines<br />

<br />

Avoid using inductors (if possible) due to higher resistive loss (& higher price)<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

In general, one shunt capacitor & two series transmission lines is<br />

sufficiently to transform any load to any input impedance.<br />

EX: transform load ZL to an input impedance Z in<br />

Z<br />

L 30 j10<br />

<br />

<br />

Zin<br />

60 j80<br />

<br />

f 1.<br />

5 GHz<br />

zL<br />

0.<br />

6 <br />

zin<br />

1.<br />

2 <br />

Identify input & load SWR circles<br />

j0.<br />

2 <br />

Choose A (yA= 1-j0.6) & transform zL to<br />

A by a series TL (l1)<br />

=>Transform A to B (on the input SWR circle)<br />

by a parallel C1<br />

=> Transform B to zin by a series TL (l2)<br />

zL + series-TL (l1)<br />

=> A + shunt C1<br />

=> B + series-TL (l2)<br />

=> zin<br />

j1.<br />

6 <br />

2011-12 H.-R. Chuang EE NCKU

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