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1 Chapter 2 Introduction to Signals and systems
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Page 1: Chapter 2

1

Chapter 2

Introduction to Signals and systems

Page 2: Chapter 2

2

Outlines

• Classification of signals and systems

• Some useful signal operations

• Some useful signals.

• Frequency domain representation for periodic signals

• Fourier Series Coefficients

• Power content of a periodic signal and Parseval’ s theorem for the Fourier series

Page 3: Chapter 2

3

Classification of Signals

• Continuous-time and discrete-time signals• Analog and digital signals• Deterministic and random signals• Periodic and aperiodic signals• Power and energy signals• Causal and non-causal.• Time-limited and band-limited.• Base-band and band-pass.• Wide-band and narrow-band.

Page 4: Chapter 2

4

Continuous-time and discrete-time periodic signals

Page 5: Chapter 2

5

Continuous-time and discrete-time aperiodic signals

Page 6: Chapter 2

6

Analog & digital signals

• If a continuous-time signal can take on any values in a continuous time interval, then is called an analog signal.

• If a discrete-time signal can take on only a finite number of distinct values, { }then the signal is called a digital signal.

)(tg

)(tg

( )g n

Page 7: Chapter 2

7

Analog and Digital Signals

0 1 1 1 1 0 1

Page 8: Chapter 2

8

Deterministic signal

• A Deterministic signal is uniquely described by a mathematical expression.

• They are reproducible, predictable and well-behaved mathematically.

• Thus, everything is known about the signal for all time.

Page 9: Chapter 2

9

A deterministic signal

Page 10: Chapter 2

10

Deterministic signal

Page 11: Chapter 2

11

Random signal

• Random signals are unpredictable.

• They are generated by systems that contain randomness.

• At any particular time, the signal is a random variable, which may have well defined average and variance, but is not completely defined in value.

Page 12: Chapter 2

12

A random signal

Page 13: Chapter 2

13

Periodic and aperiodic Signals

• A signal is a periodic signal if

• Otherwise, it is aperiodic signal.

0( ) ( ), , is integer.x t x t nT t n

( )x t

0

00

: period(second)

1( ), fundamental frequency

2 (rad/sec), angulr(radian) frequency

T

f HzT

f

Page 14: Chapter 2

14-2 0 2-3

-2

-1

0

1

2

3

Time (s)

Square signal

Page 15: Chapter 2

15-1 0 1

-2

-1

0

1

2

Time (s)

Square signal

Page 16: Chapter 2

16-1 0 1

-2

-1

0

1

2

Time (s)

Sawtooth signal

Page 17: Chapter 2

17

• A simple harmonic oscillation is mathematically described by

x (t)= A cos (t+ ), for - ∞ < t < ∞

• This signal is completely characterized by three parameters:

A: is the amplitude (peak value) of x(t).

is the radial frequency in (rad/s),

: is the phase in radians (rad)

Page 18: Chapter 2

18

Example:Determine whether the following signals are

periodic. In case a signal is periodic, specify its fundamental period.

a) x1(t)= 3 cos(3 t+/6),

b) x2(t)= 2 sin(100 t),

c) x3(t)= x1(t)+ x2(t)

d) x4(t)= 3 cos(3 t+/6) + 2 sin(30 t),

e) x5(t)= 2 exp(-j 20 t)

Page 19: Chapter 2

19

Power and Energy signals

• A signal with finite energy is an energy signal

• A signal with finite power is a power signal

dttgEg2

)(

2/

2/

2)(

1lim

T

TT

g dttgT

P

Page 20: Chapter 2

20

Power of a Periodic Signal

• The power of a periodic signal x(t) with period T0 is defined as the mean- square value over a period

0

0

/ 22

0 / 2

1( )

T

x

T

P x t dtT

Page 21: Chapter 2

21

Example• Determine whether the signal g(t) is power or

energy signals or neither

0 2 4 6 80

1

2

g(t)

2 exp(-t/2)

Page 22: Chapter 2

22

Exercise• Determine whether the signals are power or

energy signals or neither

1) x(t)= u(t)

2) y(t)= A sin t

3) s(t)= t u(t)

4)z(t)=

5)

6)

)(t( ) cos(10 ) ( )v t t u t( ) sin 2 [ ( ) ( 2 )]w t t u t u t

Page 23: Chapter 2

23

Exercise

• Determine whether the signals are power or energy signals or neither

1)

2)

3)

1 1 2 2( ) cos( ) cos( )x t a t b t

1 1 1 2( ) cos( ) cos( )x t a t b t

1

( ) cos( )n n nn

y t c t

Page 24: Chapter 2

24-1 0 1

-2

-1

0

1

2

Time (s)

Sawtooth signalDetermine the suitable measures for the signal x(t)

Page 25: Chapter 2

25

Some Useful Functions

• Unit impulse function • Unit step function • Rectangular function • Triangular function• Sampling function• Sinc function• Sinusoidal, exponential and logarithmic

functions

Page 26: Chapter 2

26

Unit impulse function• The unit impulse function, also known as the

dirac delta function, (t), is defined by

0,0

0,)(

t

tt 1)(

dttand

Page 27: Chapter 2

27

0

Page 28: Chapter 2

28

• Multiplication of a function by (t)

• We can also prove that

)0()()( sdttts

)()0()()( tgttg )()()()( tgttg

)()()( sdttts

Page 29: Chapter 2

29

Unit step function

• The unit step function u(t) is

• u(t) is related to (t) by

0,0

0,1)(

t

ttu

t

dtu )()( )(tdt

du

Page 30: Chapter 2

30

Unit step

Page 31: Chapter 2

31

Rectangular function

• A single rectangular pulse is denoted by

2/,0

2/,5.0

2/,1

t

t

tt

rect

Page 32: Chapter 2

32-3 -2 -1 0 1 2 3

0

0.5

1

1.5

2

2.5

3

Time (s)

Rectangular signal

Page 33: Chapter 2

33

Triangular function

• A triangular function is denoted by

2

1,0

2

1,21

t

tt

t

Page 34: Chapter 2

34

• Sinc function

• Sampling function

sin( )sinc( )

xx

x

( ) ( ), : samplig intervalsT s s

n

t t nT T

Page 35: Chapter 2

35-5 0 5

-0.5

0

0.5

1

1.5

2

2.5

3

Time (s)

Sinc signal

Page 36: Chapter 2

36

Some Useful Signal Operations• Time shifting

(shift right or delay)

(shift left or advance)• Time scaling

( )g t

( )g t

ta

ta

( ), 1 is compression

( ), 1 is expansion

g( ), 1 is expansion

g( ), 1 is compression

g at a

g at a

a

a

Page 37: Chapter 2

37

Signal operations cont.

• Time inversion

( ) : mirror image of ( ) about Y-axisg t g t

( ) : shift right of ( )

( ) : shift left of ( )

g t g t

g t g t

Page 38: Chapter 2

38-10 -5 0 5

0

1

2

3

Time (s)

g(t)g(t-5)g(t)g(t-5)g(t)g(t-5)

Page 39: Chapter 2

39-10 -5 0 5

0

1

2

3

Time (s)

g(t+5)

Page 40: Chapter 2

40

Scaling

-5 0 5

0

2

4

-5 0 5

0

2

4

-5 0 5

0

2

4

g(t)

g(2t)

g(t/2)

Page 41: Chapter 2

41

Time Inversion

-5 -4 -3 -2 -1 0 1 2 3 4 50

0.5

1

1.5

2

-5 -4 -3 -2 -1 0 1 2 3 4 50

0.5

1

1.5

2

g(t)

g(-t)

Page 42: Chapter 2

42

Inner product of signals

• Inner product of two complex signals x(t), y(t) over the interval [t1,t2] is

If inner product=0, x(t), y(t) are orthogonal.

2

1

( ( ), ( )) ( ) ( )t

t

x t y t x t y t dt

Page 43: Chapter 2

43

Inner product cont.

• The approximation of x(t) by y(t) over the interval

is given by

• The optimum value of the constant C that minimize the energy of the error signal

is given by

( ) ( ) ( )e t x t cy t 2

1

1( ) ( )

t

y t

C x t y t dtE

1 2[ , ]t t

( ) ( )x t cy t

Page 44: Chapter 2

44

Power and energy of orthogonal signals

• The power/energy of the sum of mutually orthogonal signals is sum of their individual powers/energies. i.e if

Such that are mutually orthogonal, then

1

( ) ( )n

ii

x t g t

( ), 1,....ig t i n

1i

n

x gi

p p

Page 45: Chapter 2

45

Time and Frequency Domainsrepresentations of signals

• Time domain: an oscilloscope displays the amplitude versus time

• Frequency domain: a spectrum analyzer displays the amplitude or power versus frequency

• Frequency-domain display provides information on bandwidth and harmonic components of a signal.

Page 46: Chapter 2

46

Benefit of Frequency Domain Representation

• Distinguishing a signal from noise

x(t) = sin(250t)+sin(2 120t);

y(t) = x(t) + noise;

• Selecting frequency bands in Telecommunication system

Page 47: Chapter 2

470 10 20 30 40 50-5

0

5Signal Corrupted with Zero-Mean Random Noise

Time (seconds)

Page 48: Chapter 2

480 200 400 600 800 10000

20

40

60

80Frequency content of y

Frequency (Hz)

Page 49: Chapter 2

49

Fourier Series Coefficients

• The frequency domain representation of a periodic signal is obtained from the Fourier series expansion.

• The frequency domain representation of a non-periodic signal is obtained from the Fourier transform.

Page 50: Chapter 2

50

The Fourier series is an effective technique for describing periodic functions. It provides a method for expressing a periodic function as a linear combination of sinusoidal functions.

Trigonometric Fourier Series

Compact trigonometric Fourier Series

Complex Fourier Series

Page 51: Chapter 2

51

Trigonometric Fourier Series

0

00

2( ) cos(2 )n

T

a x t n f t dtT

0 0 01

( ) cos 2 sin 2n nn

x t a a n f t b n f t

0

00

2( ) sin(2 )n

T

b x t n f t dtT

Page 52: Chapter 2

52

Trigonometric Fourier Seriescont.

0

00

1( )

T

a x t dtT

Page 53: Chapter 2

53

Compact trigonometric Fourier series

0 01

2 20 0

1

( ) cos(2 )

,

tan

n nk

n n n

nn

n

x t c c n f t

c a b c a

b

a

Page 54: Chapter 2

54

Complex Fourier Series

If x(t) is a periodic signal with a fundamental period T0=1/f0

are called the Fourier coefficients

2( ) oj n f tn

n

x t D e

0

0

2

0

1( ) j n f t

n

T

D x t e dtT

nD

Page 55: Chapter 2

55

Complex Fourier Series cont.

1

21

2

n

n

n n

jn n

jn n

j jn n n n

D c e

D c e

D D e and D D e

Page 56: Chapter 2

56

Frequency Spectra

• A plot of |Dn| versus the frequency is called the amplitude spectrum of x(t).

• A plot of the phase versus the frequency is called the phase spectrum of x(t).

• The frequency spectra of x(t) refers to the amplitude spectrum and phase spectrum.

n

Page 57: Chapter 2

57

Example• Find the exponential Fourier series and sketch

the corresponding spectra for the sawtooth signal with period 2

-10 -5 0 5 100

0.5

1

1.5

2

Page 58: Chapter 2

58

• Dn= j/( n); for n0

• D0= 1;

02

0

1( )

o

j n f tn

T

D x t e dtT

12

taa

edtet

tata

Page 59: Chapter 2

59

-5 0 50

0.5

1

1.5 Amplitude Spectrum

-5 0 5-100

0

100 Phase spectrum

Page 60: Chapter 2

60

Power Content of a Periodic Signal

• The power content of a periodic signal x(t) with period T0 is defined as the mean- square value over a period

2/

2/

2

0

0

0

)(1

T

T

dttxT

P

Page 61: Chapter 2

61

Parseval’s Power Theorem

• Parseval’ s power theorem series states that if x(t) is a periodic signal with period T0, then

0

0

2

/ 2 22 2

010 / 2

2 220

1 1

1( )

2

2 2

nn

T

n

nT

n n

n n

D

cx t dt c

T

a ba

Page 62: Chapter 2

62

Example 1

• Compute the complex Fourier series coefficients for the first ten positive harmonic frequencies of the periodic signal f(t) which has a period of 2 and defined as

( ) 5 ,0 2tf t e t

Page 63: Chapter 2

63

Example 2

• Plot the spectra of x(t) if T1= T/4

Page 64: Chapter 2

64

Example 3

• Plot the spectra of x(t).

0( ) ( )n

x t t nT

Page 65: Chapter 2

65

Classification of systems

• Linear and non-linear:

-linear :if system i/o satisfies the superposition principle. i.e.

1 2 1 2

1 1

2 2

[ ( ) ( )] ( ) ( )

where ( ) [ ( )]

and ( ) [ ( )]

F ax t bx t ay t by t

y t F x t

y t F x t

Page 66: Chapter 2

66

Classification of sys. Cont.

• Time-shift invariant and time varying

-invariant: delay i/p by the o/p delayed by same a mount. i.e

0 0

if ( ) [ ( )]

then ( ) [ ( )]

y t F x t

y t t F x t t

0t

Page 67: Chapter 2

67

Classification of sys. Cont.

• Causal and non-causal system

-causal: if the o/p at t=t0 only depends on the present and previous values of the i/p. i.e

LTI system is causal if its impulse response is causal.

i.e.

0 0( ) [ ( ), ]y t F x t t t

( ) 0, 0h t t

Page 68: Chapter 2

68

Suggested problems

• 2.1.1,2.1.2,2.1.4,2.1.8

• 2.3.1,2.3.3,2.3.4

• 2.4.2,2.4.3

• 2.5.2, 2.5.5

• 2.8.1,2.8.4,2.8.5

• 2.9.2,2.9.3


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