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Pseudobandpass Matching Networks 217<br />

1---------1<br />

0.2439 (0.2937 ~ O.3142J :<br />

I<br />

I<br />

r<br />

I<br />

0.2500 : I<br />

1<br />

r<br />

• I<br />

I<br />

3.172 ;::: :: 1.568<br />

I :<br />

~ 1.000 I<br />

+ I<br />

I<br />

?<br />

I<br />

r<br />

I<br />

I<br />

I,<br />

I<br />

IL<br />

Load --JJ<br />

Figure 6.37. Synthesized lumped-elemen! matching network for Examples 6.18 and 6.J9. [Fmm<br />

COHee, R. M., and Joines, W. T., <strong>IEEE</strong> Trans. <strong>Circuit</strong>s Syst., Vol. CAS-26, No.5, p. 321, May<br />

1979. © 1979 <strong>IEEE</strong>.)<br />

(6.109) are shown in Table 6.5. The synthesized network is shown in Figure<br />

6.37. Note that the load inductance is a part <strong>of</strong> the total g2 element.<br />

6.6.4. Summary <strong>of</strong> Pseudobandpass Matching. The narrow bandpass response<br />

<strong>of</strong> matching L sections suggested the use <strong>of</strong> lowpass networks (cas·<br />

caded L sections) for broadband matching witb resistance transformation. A<br />

quadratic frequency mapping function doubled the number <strong>of</strong> network elements<br />

while providing the appropriate correlation between the conventional<br />

Chebyshev lowpass, flat-loss function and the pseudobandpass function.<br />

Numerical integration over the frequency axis determined the broadband<br />

load-reactance functional values. In practice; the two load-reactance values<br />

are given, and trial evaluation <strong>of</strong> the one-reactance Fano integral determines<br />

the flat-loss and ripple factors. Then a solution exists if the two-reactance<br />

Fano integral value is less than the corresponding load function requires. If<br />

not, a greater number <strong>of</strong> elements (n) is assumed, and the process repeated.<br />

When the values <strong>of</strong> conventional Chebyshev constants are found acceptable,<br />

the pole/zero locations in the conventional s' plane are computed by<br />

formula. The quadratic frequency-mapping function then transforms these n'<br />

values into n=2n' new values. Selection <strong>of</strong> left-half-plane poles and zeros<br />

enables the construction <strong>of</strong> the Feldtkeller polynomials, and thus network<br />

synthesis can proceed.<br />

Cottee and Joines (1979) concede that the integration step can be avoided<br />

by proceeding with trial synthesis. However. they claim that the integration<br />

approach allows restrictions to be visualized; to that end, they include a dozen<br />

design charts. More significantly, their article further considers distributed<br />

(transmission line) matching networks terminated by a lumped-element load.<br />

The transmission line elements are commensurate-all having the same length<br />

-so that a resistively terminated network response would have harmonic

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