Fourier Transforms-Communication Systems-Lecture Slides, Slides of Data Communication Systems and Computer Networks

Sir Chiranjeev Mehta delivered this lecture at Alagappa University for Communication Systems course. It includes: Midterm, Average, Paper, Weight, Probably, Bridge, Fourier, Aperiodic, Domain, Periodic, Impulse

Typology: Slides

2011/2012

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Assignment # 04
1) Solution to Midterm Exam (already
discussed) [For undergrad only]
2) Example 3.6, 3.8, 3.12, 3.17
3) Problems 3.3. 3.4, 3.13, 3.14, 3.15,
3.22(a), 3.30, 3.38
Due Date (29th Nov & 1st Dec for DL students)
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Download Fourier Transforms-Communication Systems-Lecture Slides and more Slides Data Communication Systems and Computer Networks in PDF only on Docsity!

Assignment # 04 1) Solution to Midterm Exam (already

discussed) [For undergrad only]

2) Example 3.6, 3.8, 3.12, 3.17 3) Problems 3.3. 3.4, 3.13, 3.14, 3.15,

3.22(a), 3.30, 3.

Due Date (

th

Nov

st

Dec

for

DL

students

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Midterm Papers Checked Finally „

Minimum marks

Î

08 / 70

Maximum

Î

55 / 70

(79%)

Average (approx)

Î

31 / 70

(45 %)

Therefore, I will not change the weight-age most probably

Bridge to Fourier Transform „

So far only Periodic Signals have been discussed andtheir corresponding frequency domain

Æ

Fourier Series

„

What about non-periodic Signals

Æ

Fourier Transform

Bridging Fourier Series and Transform „

Consider a periodic signal below:

„

We know that the Fourier coefficients will be:

sin(

1 0

1

k k

k

T

k

T T

a

k

ω π

x

T

(t)

t

-T

1

T

1

T

0

-T

0

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What happens in frequency domain !?!?

„

As the period

Æ

, the fundamental frequency

ω

0

Æ

  1. So,

the distance between the two consecutive a

k s becomes

zero, and the sketch of a

k

becomes continuous, what is

called as Fourier Transform.

„

At the other side, the signal x(t) becomes non-periodicand takes the form:

„

This means the Fourier Transform can represent a non-periodic signal on the frequency-domain.

x(t)

t

-T

1

0 T

1

Center for Advanced Studies in

Engineering

9

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We have represented a non-periodic signal by a Fourier Integral rather than a Fourier series ƒ

We call X(w) the direct Fourier transform of x(t), and x(t) the Inverse Fourier transform of X(w) ƒ

x(t) and X(w) are a Fourier transform pair “

)

(

) (

w

X

t x

∞ ∞−

dw

e

w

X

t

x

jwt

π

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What does it tell you about the signal?

„

What it doesn’t tell you about the signal?

„

Given a signal x(t) in time-domain, its Fouriercoefficients (a

k ) or its Fourier Transform (X(

ω

)) are

called as its “

frequency (or line) spectrum

”.

„

If a

k

or X(

ω

) is complex, then frequency spectrum

is observed by their

magnitude

(|a

k

| or |X(

ω

)|) and

phase

( ∠

a

k

or

X(

ω

)) plots, e.g.:

θ

ω

ω ω

θ

=

= =

) (

) (

) (

X

A

X

Ae

X

j

Examples

t

t

x

)

(

) (

t^0

t

t x

=

δ

Fourier Transform of a PeriodicSignal

∞ −

+∞

∞ −

=

) ( 2 ) ( ,

) (

,

0

0

ω

k

a

X

Then

e a

t x

if

t k

jk

k

t

j

IFFT

e

0

)

(

2 ,

0

ω

ω

ω

πδ

⎯ ⎯ →

FT of a sinusoidal function

FT of a Pulse Train

train

pulse

Periodic

t

x

sin(

1 0

1

k k

k

T

k

T T

a

k

FT Property: „

Differentiation in Time:

)

(

/ ) (

ω

ω

X

j

dt

t

dx