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ةبيط ةعماج

EE 372 – Communication Theory and Systems I Lecture 3: Review of Signals

Omar Siddiqui

Department of Electrical Engineering College of Engineering

Taibah University

(2)

Signals

Periodic and aperiodic

Deterministic or Random Analog and Digital (amplitude)

Continuous or Discrete (time)

Signal Classification

Energy and Power

(3)

Signal Classification: Analog Vs Digital (in amplitude)

Analog: The signal amplitude can take any value at each instant of time

Amplitude t

Digital: The signal amplitude can take only specific values at each instant of time

Time: continuous, Amplitude: continuous

t

Amplitude

Time: continuous, Amplitude: Discrete

(4)

Signal Classification: Continuous or Discrete (in time)

Continuous-time Signal: x(t) where t can take any real value

V(t)

Voltage

Time (t)

Discrete time Signal:x[n] where n  {...-3,-2,-1,0,1,2,3...}

n can only be integer

Example: cos(t)

V(t)

Voltage

Time (t) Example: cos(n)

(5)

Signal Classification: Deterministic or Random

Deterministic Signal: The value of the signal can be predicted.

- Usually they have a mathematical form

V(t)

Voltage

Random Signal: The signal values cannot be predicted - No Mathematical form

Example: cos(t)

V(t)

Voltage

(6)

Signal Classification: Periodic and Aperiodic

Aperiodic Signal: It does not repeat itse. The time period can be defined as:

Examples: cos(t) sin(t)

V(t) g(t) = g(t+To)

Periodic Signal: It repeats itself with a time period of To such that:

o

T

(7)

Signal Classification: Energy and Power Signals

Energy Signal: A Signal with finite energy an energy signal

dt t

g



)

2

(  

Power Signal: A Signal with finite power is a power signal

dt t

T g

T

T T

2 /

2 /

)

2

1 (

lim  

0 

(8)

Some Basic Signal Operations

Time Shifting

) ( t T g  )

(t

g g ( tT )

Time Scaling

) (t

g g ( t 2 ) g (t / 2 )

(9)

Some Basic Signal Operations

Time Inversion (folding)

) ( t g  )

(t g

) (t

g g ( t  )

(10)

The Unit Step Function

 

 

0 0

0 ) 1

( t

t t u

Definition

1

) (t u

0 t

(11)

The Unit Step Function (To resolve the discontinuity)

- There is a discontinuity at time t = 0

- To resolve the dicontinuity, the u(t) can be assumed to be an increasing function

- u(t) can be defined as:

) ( lim

)

( t

0

u t

u

1

) (t u

1

) (t u

0 t

t

(12)

The Unit impulse function

Lets take the derivative of u(t). Because of the sudden jump at t=0, the rate of change

approaches infinite

0 0 1

) 0

(   dt

du  

The derivative of u(t) is called an impulse function and is represented by an arrow

1

) (t u

0 t

Sudden jump

1

)

(t

0 t

dt t t du ( )

) ( 

(13)

The Unit impulse function as a limiting form of a ‘pulse’

Start from the Limiting Unit step function and find its derivative assuming  approaches zero

dt t t du( )

) ( 

dt

t

t du ( )

lim )

(

0

 

) ( lim )

(

0

u t t

u

But

1

) (t u

1

) (t u

1

) (t u

1

dt t du( )

1

1 dt

t du( )

1 1

dt t

du( ) 1

1

) (t u

dt 1 t

du )( Area

 

(14)

Sifting Properties of Impulse Function Multiplication of a function by an Impulse

 ) ( ) ( tt

0

)

(t )

(t 0

x =

)

(t )

( tT

=

)

(T

 ) (

)

( tt T

  ( T )( t T )

0

) 0

 (  (t ) )

0

 (  (t )

) (

)

( TtT ) 

(T

(15)

Sifting Properties of Impulse Function Integration of a function by an Impulse

)

(t )

( tT

 0

=

0 )

(T

 ) (

)

( tt T

  ( T )( t T )

) (

)

( TtT

dt T t

t ) ( )

( 



 

dt T t

t ) ( )

( 



 



T T T

(16)

The Trigonometric Fourier Series

Trigonometric Form of Fourier Series: Any periodic function can be decomposed into sum of sine and cosine functions with frequencies that are multiples of the fundamental frequency

 

1

) 2

sin(

) 2

cos(

) (

n

o n

o n

o

a nf t b nf t

a t

g  

Where the coefficients ao, an, bn are the integrals given by:

2 /

2 /

) 1 o (

o

T

o T

o g t dt

a T

2 /

2 /

) 2

cos(

) 2 o (

o

T

T

o o

n g t nf t dt

a T

2 /

2 /

) 2

sin(

) 2 o (

o

T

T

o o

n g t nf t dt

b T

Graphical Representation

= + +

(17)

The Compact Trigonometric Fourier Series

The compact form is obtained by combining the sine and cosine terms

 

1

) 2

sin(

) 2

cos(

) (

n

o n

o n

o a nf t b nf t

a t

g  

1

) 2

cos(

n

n o

n

o C nf t

C  

) 2

cos( o n

n nf t

C  

 ) 2

sin(

) 2

cos( nf t b nf t

anono

2 2

n n

n a b

C  

 

 

  

n n

n a

1 b

 tan

o

o a

C

(18)

Example of the Compact Trigonometric Fourier Series

Example 2.8: Find the trigonometric Fourier series

Solution

(19)

Example of the Compact Trigonometric Fourier Series

Example 2.8: Find the compact trigonometric Fourier series

bn=0

2 2

n n

n a b

C  

ao=1/2

C  2

o

o a

C

2

 1

Co

To find the compact form:

...

9 , 7 , 5 , 3 ,

1 n

forCn  0 for n  2,4,6,8,10...

(20)

Example of the Compact Trigonometric Fourier Series



 

 

n n

n a

1 b

 tan

 

 

 

n n

/ 2 tan 1 0



 

 

 

n n

/ 2 tan 1 0

,...

9 , 5 ,

1

 n for

,...

11 , 7 ,

 3 forn

x y

 0

 0

n

n  

or

2

1 1 1 1

bn=0

(21)

Example of the Compact Trigonometric Fourier Series

2 2 ) 1

(t

w cos2fot 3cos6 ( )

1

fo t cos10fot 5

1 cos14 ( )

7

1

fo t cos18 ...

9

1

fot

Spectrum of the Compact Fourier Series

Cnn2 2

 1 Co

...

9 , 7 , 5 , 3 ,

1 n for

 0

Cn for n  2,4,6,8,10...

In terms of 

(22)

Demonstration of how the harmonics add up

2 2 ) 1

(t

w cos2fot cos2 (3 )( ) 3

1

fo t cos2 (5fo)t 5

1

cos2 (7 )( )

7

1

fo t cos2 (9 ) ...

9

1

fo t

0 1

2

1

0 f

Fourier Components N

1

3

3 30

2 3f0 3

1

0 2

2

0 1

0 2

2

0

1

2 A

3

2 A

=

N

n

o n

o a nf t

a

1

) 2

cos( 

ao

=

ao

0 2

2

1

1

First

0 2

2

01

2

1

0 f

1

1

2 A

First

01

2

1

0 f

1

2 A

+

0 2

2

1

1

Third

3 30

2 3f0 3

1 3 1

2

A 505

2 5f0 5

5

2 A

(23)

Demonstration of how the harmonics add up

2 2 ) 1

(t

w cos2fot cos2 (3 )( ) 3

1

fo t cos2 (5fo)t 5

1

cos2 (7 )( )

7

1

fo t cos2 (9 ) ...

9

1

fo t

Fourier Components

N

n

o n

o a nf t

a

1

) 2

cos( 

N

0 2

2

01

2

1

0 f

5

+

0 2

2

3 30

2 3f0 3

0 2

2

5

50

2 5f0 5

+

7

0 2

2

0 2

2

0

2

2

0

1 0

1

1 1

1

1

2

A 5

2 A

ao

=

=

ao

Third Fifth

+ 3rd + 5th

7 70

2 7f0 7

+

1

1 7

2 A

Seventh First

0 2

2

01

2

1

0 f

1

1

2 A

First

1 A 2 19

(24)

Gibb’s Phenomenon

0 2

2

0 1

0 2

2

(25)

Gibb’s Phenomenon

(26)

The Exponential Fourier Series

0

2 0

0

) 1 (

T

t f jn

n

g t e dt

D T

A periodic function x(t) can be decomposed into a linear combination of the harmonically related exponentials:

t jn n

n

e D t

g ( ) 

 0



The constants (weight of each harmonic) can be calculated as:

t f jn n

n

e D t

g ( ) 

 2 0



(27)

The Exponential Fourier Series

Examples 2.7 and 2.10

Find the trignometric and exponential Fourier series of the following function

Solution of Trigonometric Series Solution of Exponential Series

(28)

Reading from the book

 Chapter 2: Signals and Signal Space, Pages 20 - 67

B.P. Lathi, “Modern Digital and analog Communication Systems”, 4th Edition

References

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