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362 Other Direct Filter <strong>Design</strong> Methods<br />

ANTIMET<br />

ELLIP FLTR~CT12/78,1008<br />

REJECTION,RIPPLE(DS),1/2-DEG(2-15l ~TYPE(A,B,OR C):<br />

83.3068 .17728767 4 C<br />

u- .392699067 AO~ .253168244 EP= .414213539<br />

E= .383100151<br />

E= .293985074<br />

E= .159524088<br />

RE=-.0941605422 SE= .447245616<br />

RE=-.232749695 SE= .187680214<br />

RF=-.0417918631 SF= 1.01712478<br />

RF=-.138269216 SF= .902058076<br />

RF=-.260576346 SF= .637014303<br />

RF=-.390335577 SF= .21738535<br />

LD RESIS= 1 (1 )<br />

L(C) C(L) PEAK<br />

1 1.20340853<br />

2 1.09152826 1.37701951 2.47036986<br />

3 1.35005027 1.5232667 1.68577457<br />

4 1.58486991 1.32003532 1.47480406<br />

5 1.39727972 STPED ED8E=.1.45323639<br />

TESTS 1.2381468E-(15 1.28149986E-06<br />

Figure 9.25.<br />

Sample run for an antimetric type-c filter.<br />

9.3.6. Summary <strong>of</strong> Doubly Tenninated Elliptic Filters. The effect <strong>of</strong> trap<br />

resonance on elliptic filter input impedance is such that it is easy to determine<br />

the first lumped-element and the next trap-branch-element values. All that is<br />

required is the input impedance and its time delay at that trap's frequency;<br />

both are available from the poles and zeros <strong>of</strong> the elliptic transfer function.<br />

The computation is made easier by the fact that the input reflection coefficient<br />

is necessarily unity at any trap frequency. The poles and zeros are Jacobian<br />

elliptic functions that are easy to compute. Improved accuracy is obtained by<br />

using the infinite-product formulation <strong>of</strong> Amstutz.<br />

Amstutz's remarkable permutation algorithm determines all element values<br />

without the round-<strong>of</strong>f error typical <strong>of</strong> all other realization methods. It is based<br />

on the fact that two-port networks having the same geometry may have the<br />

same response even when the three-element sets responsible for the notches<br />

are permuted. This fact was developed by writing continued fraction expansions<br />

for two such equivalent networks, each having a different trap subsection<br />

at their input port. By equating expressions for their impedances and for<br />

their time delays at all frequencies, and at the second trap frequency in<br />

particular, a method was determined for finding the element values <strong>of</strong> the trap<br />

subsection that is once removed from the input port.<br />

The development for permuting just two trap subsections enabled the<br />

construction <strong>of</strong> a table and its generating algorithm to determine all element<br />

values in a network. Once again, the only required data are the input<br />

impedance and time delay at each trap frequency.<br />

Two Amstutz (1978) FORTRAN programs were translated into BASIC<br />

and included for use on personal computers. Reasonably sized elliptic filters

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