symmetry and the dtft n.
Download
Skip this Video
Loading SlideShow in 5 Seconds..
Symmetry and the DTFT PowerPoint Presentation
Download Presentation
Symmetry and the DTFT

Loading in 2 Seconds...

play fullscreen
1 / 20

Symmetry and the DTFT - PowerPoint PPT Presentation


  • 153 Views
  • Uploaded on

Symmetry and the DTFT. If we know a few things about the symmetry properties of the DTFT, it can make life simpler. First, for a real-valued sequence x(n), the amplitude spectrum (magnitude of the DTFT) is an EVEN function of w . To show this first show that,. Symmetry and the DTFT.

loader
I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
capcha
Download Presentation

PowerPoint Slideshow about 'Symmetry and the DTFT' - acton


An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.


- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript
symmetry and the dtft
Symmetry and the DTFT

If we know a few things about the symmetry properties of the DTFT, it can make life simpler.

First, for a real-valued sequence x(n), the amplitude spectrum (magnitude of the DTFT) is an EVEN function of w.

To show this first show that,

slide2

Symmetry and the DTFT

But we’ve assumed that x(n) is a real sequence, so

and the relationship is proven

slide3

Symmetry and the DTFT

The amplitude spectrum is

If w is replaced by –w, th amplitude spectrum is unchanged. X(ejw) = X(e-jw), so the amplitude spectrum is an even function of w.

slide4

Symmetry and the DTFT

The phase function is

For this to be an odd function of w, the imaginary part must be odd and the real part must be even. By euler’s formula,

slide5

Symmetry and the DTFT

Since cos(wn) = cos(-wn), Re(X(ejw)) is an even function of w. Likewise, since sin(wn) = -sin(-wn), Im(X(ejw)) is an even function of w. Therefore, it is shown that the phase function is an odd function of w:

slide6

Symmetry and the DTFT

Suppose x(n) has even symmetry about the origin:

Then

Which means that X(ejw) is a real-valued function

slide7

Periodicity and the DTFT

The DTFT is a periodic function of w, with period = 2p

So the frequency response function and all other DTFT’s are periodic.

One period of a DTFT completely describes the function for all values of w, so it Is usually plotted only for the interval [-p, p]

slide8

Periodicity and the DTFT

If x(n) is a real-valued sequence, the amplitude spectrum is an even function of w, AND periodic. Therefore, it is completely described by the interval [0,p]. Since the phase function is an odd function, it is also completely described by the interval [0,p].

Since the phase function is an odd function, it is also completely described by the interval [0,p].

slide9

DTFT of a Sinusoid

Suppose x(n) is the complex exponential, ejfn

This delta function is the Dirac (continuous time) delta function, so it has the sifting property.

Taking the inverse DTFT,

slide10

DTFT of a Sinusoid

So the complex exponential sequenc looks like this in the frequency domain:

2p

2p

2p

-2p

-2p+f

-p

0

f

p

2p

2p+f

slide11

DTFT of a Sinusoid

If x(n) is a sinusoid:

slide12

DTFT of a Sinusoid

So the DTFT of a sinusoid is a pair of impulses int the frequency domain, at the positive and negative frequency of the sinusoid, then repeated every 2p radians per sample

p

p

p

p

p

p

-2p-f

-2p

-2p+f

-p

-f

0

f

p

2p

2p+f

2p-f

slide13

The DTFT and the Fourier Transform

Suppose we have a continuous time signal xa(t), and its Fourier transform:

We sample xa(t) at a sampling frequency fs, creating a discrete time signal (a sequence):

This sequence has a spectrum (DTFT):

slide14

The DTFT and the Fourier Transform

I will state the following relationship now, without proof. The proof comes later:

In other words, whatever the continuous time spectrum is, the spectrum of the discrete time signal obtained by sampling has the same shape, but it is periodic in frequency with period = fs

slide15

The DTFT and the Fourier Transform

If the continuous time signal has this spectrum

Xa(f)

-2fs

-fs

0

fs

2fs

f

Then the discrete time signal (sequence) has this spectrum:

X(ej2pf)

-2fs

-fs

0

fs

2fs

f

slide16

The DTFT and the Fourier Transform

If the continuous time signal is bandlimited (has no significant spectral content above some frequency f=B),

Xa(f)

-2fs

-fs

-B

0

B

fs

2fs

f

Then the sequence obtained by sampling the continuous time signal looks like this in the frequency domain:

slide17

The DTFT and the Fourier Transform

X(ej2pf)

-B

B

-2fs

-fs

0

fs

2fs

f

As long as fs > 2B, no problem. But if fs < 2B, it looks like this:

X(ej2pf)

-B

B

-4fs

-3fs

-2fs

-fs

0

fs

2fs

3fs

4fs

f

slide18

The DTFT and the Fourier Transform

Note that the spectral replicas created by sampling overlap

X(ej2pf)

-B

B

-4fs

-3fs

-2fs

-fs

0

fs

2fs

3fs

4fs

f

This is called aliasing

To avoid aliasing, the minimum sample frequency is given by the Nyquist criterion:

slide19

The DTFT and the Fourier Transform

And the minimum sampling frequency is called the Nyquist frequency or Nyquist rate.

If the Nyquist criterion is met, the original continuous time signal xa(t) can be completely recovered from the sequence x(n) by an ideal digital to analog converter.

slide20

The DTFT and the Fourier Transform

To make sure the Nyquist criterion is met, the signal should pass through an antialiasing filter before it is sampled by the analog to digital converter (ADC):

xa(t)

Antiasing Filter

ADC

x(n)

The antialising filter must be designed to cut off any spectral content above ½ the sampling frequency.