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Prohle"" 227<br />

Third, an objective function for optimizing the resistance excursions need<br />

not be limited to gain; it might be noise figure, noise measure, or any other<br />

function that can be formulated in terms <strong>of</strong> impedances or admittances.<br />

Equally important, an arbitrary goal/target function may be employed so that<br />

sloped gain functions may be matched. Like most applications <strong>of</strong> nonlinear<br />

programming (optimization), there are several choices to be made from<br />

experience rather than by analysis.<br />

The optimal piecewise linear resistance function must be fitted with an even<br />

rational polynomial, so that a matching network may be synthesized. The<br />

Gewertz method then provides the input impedance polynomial for the<br />

network at the load interface. Standard network synthesis techniques will<br />

produce the LC element values.<br />

There are two features <strong>of</strong> Carlin's broadband-matching method that distinguish<br />

it from Fano's classical method. The discrete load impedance versus<br />

frequency data set does not have to be identified with a resistively terminated<br />

LC load network; i.e., load classification is not required. Also, the wellconditioned<br />

optimization process allows sloped-gain or other arbitrary fit <strong>of</strong><br />

the objective function. Fano's method has been adapted by Mellor (1975) to<br />

obtain similar results at the expense <strong>of</strong> considerable ad hoc procedures.<br />

Network synthesis is required in these and other methods which are more<br />

versatile than the direct design-matching method in Section 6.4.<br />

Problems<br />

6.1. Find four different lossless, lumped-element L-section matching networks<br />

that transform a load impedance <strong>of</strong> 36 - j324 ohms to match a<br />

50 +jO generator impedance.<br />

6.2. Conjugately match a 6+j25-ohm load impedance to a 7+j20-ohm<br />

generator using only capacitors in an L section. Obtain two different<br />

solutions.<br />

6.3. Plot a 2: I SWR load-locus circle on a Smith chart, and explain why<br />

Equation (6.19) is true.<br />

6.4. A T section is composed <strong>of</strong> the two types <strong>of</strong> L sections.<br />

(a) Write an expression for the parallel resistance level across the<br />

shunt reactance (X b ) as a function <strong>of</strong> the T section's terminating<br />

resistances and transfer phase angle.<br />

(b) A conjugately matched T section delivers I watt from a 50-ohm'<br />

source to a 21-ohm load with a lagging current transfer phase <strong>of</strong><br />

155 degrees. What is the rms voltage across the shunt reactance?

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