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Chapter Six<br />

Impedance Matching<br />

Impedance matching is the design <strong>of</strong> a network or transducer so that a<br />

terminating impedance is transformed exactly to a desired impedance at a<br />

frequency, or is transformed approximately over a band <strong>of</strong> frequencies. Figure<br />

6.1 shows the situation where load impedance Z, may be specified as some LC<br />

subnetwork terminated by a resistance or by complex numbers associated with<br />

arbitrary frequencies. The desired input impedance Z;" may be similarly<br />

specified or may be contained in a neighborhood described as some maximum<br />

standing-wave ratio (4.59). Section 9.6 will consider dissipative network transformations;<br />

in this chapter only lossless, passive networks are considered.<br />

Impedance transformation is usually desired for control <strong>of</strong> power transfer<br />

from a fiuite impedance source, and is thus related to the same requirements<br />

discussed in Chapter Three for doubly terminated filters. There is one important<br />

difference: impedance matching usually is concerned with given terminating<br />

impedances that are complex, not simple resistances. This results in simple<br />

restrictions for single-frequency transformations. There are complicated constraints<br />

when matching complex impedances over a band <strong>of</strong> frequencies.<br />

These problems will be considered in order <strong>of</strong> increasing generality.<br />

Chapter Six begins with impedance matching at a single steady-state<br />

frequency, first with two- and three-element networks composed <strong>of</strong> a combination<br />

<strong>of</strong> inductors and capacitors, and then with one or two cascaded<br />

transmission lines. It is remarkable that these subjects are seldom treated in<br />

modern electrical engineering curricula, even though they appear in almost all<br />

pertinent texts and hand<strong>book</strong>s published before 1960. Practicing engineers<br />

responsible for radio frequency circuit design invariably query prospective<br />

employees about L, T, pi, and perhaps transmission line matching because it is<br />

a matter <strong>of</strong> frequent concern. The treatment here includes tried and true<br />

concepts, which will be extended to broadband matching and direct-coupled<br />

filters (Chapter Eight) as well, especially the idea <strong>of</strong> the loaded Q <strong>of</strong> an<br />

impedance. The Smith chart as a means <strong>of</strong> visualizing the matching process<br />

170

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