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DESIGN AND ANALYSIS OF ANALOG FILTERS A Signal ...

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40 <strong>DESIGN</strong> <strong>AND</strong> <strong>ANALYSIS</strong> <strong>OF</strong> <strong>ANALOG</strong> <strong>FILTERS</strong>:<br />

Summary of the Paley-Wiener Theorem<br />

Some of the more important concepts of this section are as follows:<br />

A given magnitude frequency response that is square-integrable<br />

and satisfies (2.11) has, with an appropriate phase response,<br />

a corresponding causal impulse response.<br />

The inequality of (2.11), for square-integrable magnitude<br />

frequency responses, is a necessary and sufficient condition in<br />

order for the impulse response to be causal.<br />

If the magnitude frequency response is not square-integrable,<br />

then the inequality of (2.11) is neither necessary nor sufficient<br />

for the impulse response to be causal.<br />

A consequence of the Paley-Wiener Theorem is that no finiteenergy<br />

signal can be both time-limited and frequency-limited.<br />

Therefore all causal impulse response filters cannot be frequencylimited,<br />

i.e., there can be no bands where the frequency response<br />

is zero.<br />

2.3 TIME-B<strong>AND</strong>WIDTH PRODUCTS<br />

For the ideal filters presented in Section 2.1, the location of the center of the<br />

impulse response is obviously at t = 0 for the zero phase response case, or at<br />

if an ideal linear phase response of is assumed, since h(t) has<br />

even symmetry about But if h(t) does not have even symmetry, the location of<br />

the center of the impulse response could be defined in various ways, such as the time<br />

at which the response is maximum. A more useful definition for the center is the time<br />

where the “center of gravity” of occurs along the time axis:<br />

Chapter 2 Analog Filter Design and Analysis Concepts

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