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Doubly Termi/lllted Elliptic Filters 353<br />

Amstutz's subtle step depends on the equivalence <strong>of</strong> any two networks<br />

having the same topology but permuted trap positions. The key to his method<br />

is to permute each <strong>of</strong> the traps into the input position and apply a recursive<br />

algorithm that yields all <strong>of</strong> the element values. An additional feature <strong>of</strong> his<br />

type-s symmetric filter program is the calculation <strong>of</strong> the critical unloaded Q<br />

(uniform in both inductors and capacitors) that just erases the trap notch<br />

nearest the passBand.<br />

This section begins with the application <strong>of</strong> the input impedance and its<br />

derivative with respect to frequency. The basis <strong>of</strong> the trap permutation scheme<br />

is then described. Finally, examples using the symmetric and the antimetric<br />

programs are discussed.<br />

9.3.1. Input Impedanee Relationships. The analysis will employ the midseries<br />

topology in Figure 9.120 without loss <strong>of</strong> generality. It was remarked in<br />

Section 8.1.1 that the impedance <strong>of</strong> a series LC branch resonant at w n is<br />

simply jwnLF (for example, see the admittance case in (8.28), Section 8.3.2).<br />

Suppose that the (M" K,) branch in Figure 9.120 is resonant at s, =jw,. Then<br />

the input impedance in the neighborhood <strong>of</strong> that frequency is<br />

Z;n(S)=SL,+M,(S- :i). (9.32)<br />

Note that impedance Z, seen to the right <strong>of</strong> the (M" K,) branch in Figure<br />

9.120, is not zero in practical cases. Differentiating (9.32) with respect to<br />

complex frequency s yields<br />

Zin = L, + M,( I

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