02.10.2019 Views

UploadFile_6417

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

CHAPTER 3<br />

The Discrete-time<br />

Fourier Analysis<br />

We have seen how a linear and time-invariant system can be represented<br />

using its response to the unit sample sequence. This response, called the<br />

unit impulse response h(n), allows us to compute the system response to<br />

any arbitrary input x(n) using the linear convolution:<br />

x(n) −→ h(n) −→ y(n) =h(n) ∗ x(n)<br />

This convolution representation is based on the fact that any signal<br />

can be represented by a linear combination of scaled and delayed unit<br />

samples. Similarly, we can also represent any arbitrary discrete signal<br />

as a linear combination of basis signals introduced in Chapter 2. Each<br />

basis signal set provides a new signal representation. Each representation<br />

has some advantages and some disadvantages depending upon the type<br />

of system under consideration. However, when the system is linear and<br />

time-invariant, only one representation stands out as the most useful. It<br />

is based on the complex exponential signal set {e jωn } and is called the<br />

discrete-time Fourier transform.<br />

3.1 THE DISCRETE-TIME FOURIER TRANSFORM (DTFT)<br />

|x(n)| < ∞, then its discrete-<br />

If x(n)isabsolutely summable, that is, ∑ ∞<br />

time Fourier transform is given by<br />

∞∑<br />

X(e jω ) = △ F[x(n)] =<br />

−∞<br />

n=−∞<br />

x(n)e −jωn (3.1)<br />

59<br />

Copyright 2010 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).<br />

Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!