02.10.2019 Views

UploadFile_6417

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

82 Chapter 3 THE DISCRETE-TIME FOURIER ANALYSIS<br />

x a (t)<br />

1<br />

CTFT<br />

X a (jΩ )<br />

A<br />

0<br />

t<br />

−Ω 0 0<br />

Ω 0<br />

Ω<br />

Sample<br />

eq. (3.27)<br />

x(n)<br />

1<br />

T s < π/Ω 0<br />

DTFT<br />

A /T s<br />

X(e jw )<br />

−Ω 0 /T s<br />

Ω 0 /T s<br />

−5<br />

0<br />

5<br />

n<br />

−2π −π 0 π 2π<br />

w<br />

x(n)<br />

X(e jw )<br />

A /T s<br />

T s > π/Ω 0<br />

−Ω 0 /T s<br />

Ω 0 /T s<br />

−2 −1 0 1 2<br />

n<br />

−2π<br />

−π<br />

0 π 2π<br />

w<br />

FIGURE 3.10<br />

Sampling operation in the time and frequency domains<br />

signal x a (t) from its samples x(n)] if the infinite “replicas” of X a (jΩ) do<br />

not overlap with each other to form X(e jω ). This is true for band-limited<br />

analog signals.<br />

DEFINITION 2<br />

[Band-limited Signal] A signal is band-limited if there exists a finite radian<br />

frequency Ω 0 such that X a (jΩ) is zero for |Ω| > Ω 0 . The frequency<br />

F 0= Ω 0 /2π is called the signal bandwidth in Hz.<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!