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62 Some Tools and Examples <strong>of</strong>Filter Synthesis<br />

Utilization <strong>of</strong> the continued fraction expansion <strong>of</strong> reactance functions from<br />

Section 3.4 requires the conversion <strong>of</strong> ZRLC to its corresponding ZLC" This is<br />

obtained by inspection <strong>of</strong> ZRLC behavior at s=O and reference to a standard<br />

table, which was derived. The worked example relates to the looking-back<br />

impedance at the output <strong>of</strong> a resistively driven LC two-port network. Starting<br />

from a given resistance function polynomial, which could have been obtained<br />

by the fitting procedure <strong>of</strong> Section 2.5, pi-network element values that realized<br />

this behavior versus frequency were obtained. This example will be <strong>of</strong> cen tral<br />

importance as the final operation in a relatively new broadband impedancematching<br />

procedure considered in Section 6.7.<br />

3.6. Long Division and Partial Fraction Expansion<br />

The last section <strong>of</strong> Chapter Three describes an important design tool that is<br />

useful for network synthesis in the frequency domain as well as for Laplace<br />

analysis in the time domain. The former is illustrated by Bode's alternative to<br />

the Gewertz procedure (see Guillemin, 1957). The time domain application <strong>of</strong><br />

partial fraction expansions will be illustrated next (from Blinchik<strong>of</strong>f and<br />

Zverev, 1976).<br />

Suppose that a given system transfer function is<br />

H,(s)= s4+6s'+22s'+30s+ 14. (3.109)<br />

S4 + 6s' + 22s' + 30s + 13<br />

As will be demonstrated, it can also be expressed in the form<br />

H,(s)=I+ 0.1 0.02 + 0.02s+0.04 (3.110)<br />

(s+ I)' (s+ I) (S-SI)(S-Sf)'<br />

where s is the Laplace complex frequency variable, and root SI is S, = -2+j3.<br />

Using a standard table <strong>of</strong> Laplace transforms for time and frequency functions,<br />

it is easy to show that the time response corresponding to (3.110) is<br />

h,(t) = 8(t) + [O.lte-'-0.02e-'+ 2e-'(0.01 cos 3t - si~t) ]U(t), (3.111)<br />

where 8(t) is an impulse function, and u(t) is a unit-step function.<br />

The algorithm to be described operates on proper rational functions, i.e.,<br />

those whose numerator degree is lower than the denominator degree. Clearly,<br />

(3.109) is not proper, but would be if one long-division step were accomplished.<br />

The first subject treated in this section will be a compact long-division<br />

algorithm, botb for obtaining proper fractions and to convince the reader that<br />

it is not complicated to program. This is important, because long division is<br />

one <strong>of</strong> two main features <strong>of</strong> the partial fraction expansion algorithm to follow.<br />

3.6.1. Long Division. Vlach (1969) gives a brief FORTRAN program for<br />

long division; it is adapted to BASIC language in Appendix-B Program B3-6.<br />

The calculation occurs in the last 10 lines <strong>of</strong> the program.

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