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- - ----------'<br />

98 Ladder Network Analysis<br />

4.6.1. Rea4 Causal Fourier Integrals. The familiar Fourier integral<br />

h(l)= _Ifoo H(w)ejw'dw<br />

271 - 00<br />

(4.69)<br />

may produce values <strong>of</strong> h(t) that are complex and nonzero in negative time.<br />

The system frequency response is H(w) and the corresponding time impulse<br />

response is h(t). Those wishing to review its applications should see Blinchik<strong>of</strong>f<br />

and Zverev (1976). When h(t) must be real and also causal (zero in<br />

negative time), (4.69) may be written as<br />

h(t) = 1 (OOR(w)coswtdw, (4.70)<br />

"')0<br />

where R(w) is the real part <strong>of</strong> the system frequency response function H. In<br />

practice, the integration is completed only to some finite frequency on the<br />

assumption that H is band limited, e.g., is zero above some limiting frequency.<br />

Example 4.4. Suppose that H(w) is the impedance <strong>of</strong> a parallel RC network,<br />

i.e., the response function V/1. This could be calculated by an analysis<br />

program in the general case. Here, use the equation<br />

Then the real part is<br />

H(s)=_I_ l<br />

·<br />

s+<br />

(4.71)<br />

R(w)=_I_,. (4.72)<br />

I+w<br />

Appendix B BASIC Program.B4-2 calculates 25 values <strong>of</strong> R(w) from 0 to 12<br />

radians in program lines 130-190. Clearly, (4.72) is a band-limited function.<br />

Running Program B4-2 shows that the real part is only 0.0069 (21.6 dB loss) at<br />

12 radians. Program lines 200-350 evaluate (4.70) for the impulse response;<br />

particularly, lines 300-329 implement Simpson's rule (2.32) for the numerical<br />

integration required. Running Program B4-2 from the beginning shows the<br />

frequency samples and then 'the impulse response samples. They correspond<br />

reasonably well with<br />

(4.73)<br />

which is the exact impulse function corresponding to (4.71), the Laplace<br />

transform pair. The BASIC function on line 115 is there simply to slow the<br />

program output rate.<br />

4.6.2. Numerical Convolution <strong>of</strong> Time Functions. The convolution integral is<br />

defined by<br />

(4.74)<br />

where T is the dummy variable <strong>of</strong> integration, F, is the excitation function, and<br />

F" is the system output function. The system impulse response is h(t). The case<br />

<strong>of</strong> (4.73) is shown in Figure 4.17. Convolution involves folding, shifting,<br />

I

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