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182 Impedance Matching<br />

Example 6.1, which involves negative reactance and susceptance travel on the<br />

Smith chart. Negative travel is toward the bottom half <strong>of</strong> the chart instead <strong>of</strong><br />

toward the top half (positive half-plane).<br />

It is strongly recommended that the reader write a small program to<br />

accomplish the calculation <strong>of</strong> (6.22) and its inverse, so that Smith chart<br />

plotting is simply a matter <strong>of</strong> locating rectangular and/or polar computed_<br />

numbers. Cases involving complex sources may be treated as in the analysis<br />

above and in Example 6.4. However, a more general treatment will be <strong>of</strong>fered<br />

in the next chapter, where the chart center can represent a complex number.<br />

Many engineers associate the Smith chart with transmission line solutions; this<br />

will be shown in Section 6.2.<br />

6.1.6. Summary <strong>of</strong> L, T, and Pi Matching. The topic <strong>of</strong> L, T, and pi<br />

matching began with a comment on the fact that lossless matching networks<br />

exhibit conjugate impedance matches at every interface because <strong>of</strong> conservation<br />

<strong>of</strong> power. Then, functionally similar equations were given and verified for<br />

solving T and pi resistive matching network problems in terms <strong>of</strong> the currenttransfer-angle<br />

parameter. The two possible L-section configurations were<br />

treated as special cases <strong>of</strong> the T and pi configurations when the output branch<br />

was omitted. A small BASIC language program was provided to calculate<br />

element reactance at an assumed frequency.<br />

Series-to-parallel impedance conversions and parallel combination <strong>of</strong> reactances<br />

were described in order to always work with impedances as opposed to<br />

mixed impedance/admittance units. The former strategy has been found<br />

superior because engineers more readily recognize practical ranges <strong>of</strong> elements<br />

in a single unit <strong>of</strong> measure. A hand-held computer program was provided for<br />

these simple relationships, and examples were worked. These tools are vital<br />

parts <strong>of</strong> the complete set <strong>of</strong> solutions obtained for an example that involves<br />

both complex load and complex source, utilizing L-section matching networks.<br />

Finally, a brief comment was provided on the value <strong>of</strong> graphic visualizations<br />

in general and the Smith chart in particular. A much more general<br />

treatment <strong>of</strong> the Smith chart will be furnished in the next chapter.<br />

6.2. Llssless Uniform Transmission Lines<br />

The matching network in these sections will consist <strong>of</strong> a lossless, uniform<br />

transmission line, as shown in Figure 6.11. The load impedance Z, and the<br />

desired input impedance Zl are given; the unknowns are the real transmission<br />

line characteristic impedance Zo and electrical length O.<br />

An expression for the input impedance Z, will be derived from Chapter<br />

Four equations. A related reflection equation will be derived for relationship<br />

to the Smith chart. The lossless case will then be examined to produce<br />

solutions for a complex source and a complex load. A more simple result will<br />

be obtained for the case <strong>of</strong> a real source and complex load; this will result in a

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