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

l<br />

-l<br />

-L<br />

x<br />

r<br />

)<br />

l<br />

vAs(x, L)<br />

L<br />

x<br />

x<br />

n n<br />

n-l<br />

-l<br />

Figure 9.13. Low-order Chebyshev rational functions. [From Daniels, 1974. Copyright 1974 Bell<br />

Telephone Laboratories. Reprinted by permission.]<br />

the Jacobian elliptic sine function, which is doubly periodic and only slightly<br />

harder to evaluate than the trigonometric sine function. This calculation is<br />

included in BASIC Program B9- I. It requires less than II lines <strong>of</strong> code. The<br />

rational functions so obtained behave as indicated in Figure 9.13. It is easy to<br />

imagine how the square <strong>of</strong> these functions produces the frequency response in<br />

Figure 9.1 I b.<br />

9.2.2. Eltiptic Filter Degree, Attenuation, and Pole Frequencies. Zverev<br />

(1967) published the well-known nomogram in Figure 9.14, which relates the<br />

elliptic filter degree and attenuation to the bandwidth parameters. Figures<br />

9.I1b and 9.14 show that the passband ripple (Am,,=O.1 dB) and the<br />

stopband shelf attenuation (Amin =43 dB) require N = 5 for a stopband/passband<br />

transition ratio (WH/WB) <strong>of</strong> 1.5. Program B9-1 has been translated to<br />

BASIC from a program by Daniels (1974). It duplicates the calculations<br />

illustrated in Figure 9.14 and computes the attenuation pole (trap) frequencies.<br />

A word <strong>of</strong> caution: Program B9-l is inaccurate for the solution in the<br />

upper-left corner <strong>of</strong> Figure 9.14 because <strong>of</strong> the round-<strong>of</strong>f error in the complete<br />

elliptic integral calculation (another Jacobian function). A more accurate

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