Chapter 2 Signals and Linear Systems (I)

45
1 Chapter 2 Signals and Linear Systems (I)

Transcript of Chapter 2 Signals and Linear Systems (I)

Page 1: Chapter 2 Signals and Linear Systems (I)

1

Chapter 2 Signals and Linear

Systems (I)

Page 2: Chapter 2 Signals and Linear Systems (I)

Chapter Outline

2

Basic Concepts

Fourier Series

Fourier Transform

Filter Design

Power and Energy

Hilbert Transform and Its Properties

Lowpass and Bandpass Signals

Further reading

Page 3: Chapter 2 Signals and Linear Systems (I)

Basic Operations on Signals (1/4)

3

Page 4: Chapter 2 Signals and Linear Systems (I)

Basic Operations on Signals (2/4)

4

Page 5: Chapter 2 Signals and Linear Systems (I)

Basic Operations on Signals (3/4)

5

Page 6: Chapter 2 Signals and Linear Systems (I)

Basic Operations on Signals (4/4)

6

Page 7: Chapter 2 Signals and Linear Systems (I)

Continuous-Time and Discrete-Time

Signals (1/3)

7

Page 8: Chapter 2 Signals and Linear Systems (I)

Continuous-Time and Discrete-Time

Signals (2/3)

8

Example 2.1.1 x(t)=Acos(2πf0t+θ) is an example of a

continuous-time signal called a sinusoidal signal.

Page 9: Chapter 2 Signals and Linear Systems (I)

Continuous-Time and Discrete-Time

Signals (3/3)

9

Example 2.1.2 x[n]=Acos(2πf0n+θ), where n belongs to the

set of integers.

Page 10: Chapter 2 Signals and Linear Systems (I)

Real and Complex Signals (1/3)

10

A real signal takes its values in the set of real numbers, i.e.,

R

A complex signal takes its values in the set of complex

number, i.e., C

A complex signal can be represented by two real signals.

These two real signals can be either the real and imaginary

parts or the absolute value (or modulus or magnitude) and

phase

)(tx

)(tx

Page 11: Chapter 2 Signals and Linear Systems (I)

Real and Complex Signals (2/3)

11

Example 2.1.3 The signal x(t)=Aej(2πf0t+θ), is a complex

signal. Its real part is

and its imaginary part is

The absolute value of x(t) is

and its phase is

)2cos()( 0 tfAtxr

).2sin()( 0 tfAtxi

||)()(|)(| 22 Atxtxtx ir

.2)( 0 tftx

Page 12: Chapter 2 Signals and Linear Systems (I)

Real and Complex Signals (3/3)

12

Example 2.1.3 (Cont’d)

Page 13: Chapter 2 Signals and Linear Systems (I)

Deterministic and Random Signals

(1/1)

13

In a deterministic signal at any time instant t, the value of x(t)

is given as a real or a complex number

In a random (or stochastic) signal at any given time instant t,

x(t) is a random variable. It is defined by a probability density

function

Page 14: Chapter 2 Signals and Linear Systems (I)

Periodic and Nonperiodic Signals (1/3)

14

A periodic signal repeats in time

The minimum repeating interval is called period

A periodic signal is a signal x(t) that satisfies the property

x(t+T0)=x(t)

for all t, and some positive real number T0 (called the period

of the signal)

For a discrete-time period signal, we have

x[n+T0]=x[n]

for all integers n, and a positive integer T0 (called the period)

A signal that does not satisfy the conditions of periodicity is

called nonperiodic

Page 15: Chapter 2 Signals and Linear Systems (I)

Periodic and Nonperiodic Signals (2/3)

15

The signal x(t)=Acos(2πf0t+θ) and x(t)=Aej(2πf0t+θ) are

periodic signals with identical period T0=1/f0

The unit-step signal

is a nonperiodic signal

0,0

0,1)(1 t

ttu

Page 16: Chapter 2 Signals and Linear Systems (I)

Periodic and Nonperiodic Signals (3/3)

16

Example 2.1.5 The signal x[n]=Acos(2πf0n+θ) is not

periodic for all values of f0. For this signal to be periodic, we

must have

2πf0(n+N0)+θ=2πf0n+θ+2mπ

for all integers n, some positive integer N0, and some integer

m. Thus, we conclude that

2πf0N0=2mπ

or

f0=m/N0

The discrete sinusoidal signal is periodic only for rational

values of f0

Page 17: Chapter 2 Signals and Linear Systems (I)

Causal and Noncausal Signals (1/2)

17

A signal x(t) is called causal if for all t<0, we have x(t)=0;

otherwise, the signal is noncausal

A discrete-time signal is a causal signal if it is identically equal

to zero for n<0

Page 18: Chapter 2 Signals and Linear Systems (I)

Causal and Noncausal Signals (2/2)

18

Example 2.1.6 The signal

is a causal signal

otherwise

ttfAtx

,0

0),2cos()(

0

Page 19: Chapter 2 Signals and Linear Systems (I)

Even and Odd Signals (1/3)

19

A signal x(t) is even if it has mirror symmetry with respect to

the vertical axis. A signal is odd if it is symmetric with respect

to the origin

The signal x(t) is even if and only if, for all t,

x(-t)=x(t),

and is odd if and only if, for all t,

x(-t)=-x(t)

Page 20: Chapter 2 Signals and Linear Systems (I)

Even and Odd Signals (2/3)

20

In general, any signal x(t) can be written as the sum of its

even and odd parts as

x(t)=xe(t)+xo(t),

where ,

2

)()()(

txtxtxe

2

)()()(

txtxtxo

Page 21: Chapter 2 Signals and Linear Systems (I)

Even and Odd Signals (3/3)

21

Page 22: Chapter 2 Signals and Linear Systems (I)

Hermitian Symmetry for Complex

Signals (1/1)

22

A complex signal x(t) is called Hermitian if its real part is

even and its imaginary part is odd

We can easily show that its magnitude is even and its phase is

odd.

The signal x(t)=Aej2πf0t is an example of a Hermitian signal

Page 23: Chapter 2 Signals and Linear Systems (I)

Energy-Type and Power-Type Signals

(1/5)

23

This classification deals with the energy content and the

power content of signals. Before classifying these signals, we

need to define the energy content (or simply the energy) and

the power content (or power)

The energy content of the signal is defined by

The power content is defined by

For real signal, |x(t)|2 is replaced by x2(t)

2

2

22 |)(|lim|)(|T

TdttxdttxE

Tx

2

2

2|)(|1

limT

Tdttx

TP

Tx

Page 24: Chapter 2 Signals and Linear Systems (I)

Energy-Type and Power-Type Signals

(2/5)

24

A signal x(t) is an energy-type signal if and only if Ex is finite

A signal x(t) is a power-type signal if and only if 0<Px<∞

Example 2.1.9 Find the energy in the signal described by

We have

This signal is an energy-type signal

.,0

3||,3)(

otherwise

ttx

.549|)(|3

3

2

dtdttxEx

Page 25: Chapter 2 Signals and Linear Systems (I)

Energy-Type and Power-Type Signals

(3/5)

25

Example 2.1.10 The energy content of Acos(2πf0t+θ) is

This signal is not an energy-type signal. The power of this

signal is

Hence, x(t) is a power-type signal and its power is

2

2

)2(coslim 0

22T

TdttfAE

Tx

2

2

)2(coslim 0

221T

TdttfAP

TT

x

2

2A

2

2A

Page 26: Chapter 2 Signals and Linear Systems (I)

Energy-Type and Power-Type Signals

(4/5)

26

Example 2.1.11 For any periodic signal with period T0, the

energy is

Therefore, periodic signals are not energy-type signals

2

2

2|)(|limT

TdttxE

Tx

20

20

2|)(|limnT

nTdttx

n

20

20

2|)(|limT

Tdttxn

n

Page 27: Chapter 2 Signals and Linear Systems (I)

Energy-Type and Power-Type Signals

(5/5)

27

Example 2.1.11 (Cont’d) The power content of any

periodic signal is

The power content of a periodic signal is equal to the

average power in one period

2

2

2|)(|1

limT

Tdttx

TP

Tx

20

20

2

0

|)(|1

limnT

nTdttx

nTn

20

20

2

0

|)(|limT

Tdttx

nT

n

n

2

0

20

2

0

|)(|1 T

Tdttx

T

Page 28: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (1/18)

28

The Sinusoidal Signal. The sinusoidal signal is defined by

where the parameters A, f0, and θ are the amplitude,

frequency, and phase of the signal

The period is T0=1/f0

)2cos()( 0 tfAtx

Page 29: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (2/18)

29

The complex exponential signal. The complex

exponential signal is defined by x(t)=Aej(2πf0t+θ)

A, f0, and θ are the amplitude, frequency, and phase of the

signal

Page 30: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (3/18)

30

The Unit-Step Signal. The unit step multiplied by any

signal produces a “causal version” of the signal

For positive a, we have u-1(at)=u-1(t)

Page 31: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (4/18)

31

Page 32: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (5/18)

32

The Rectangular Pulse. This signal is defined as

otherwise

tt

,0

,1)( 2

121

Page 33: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (6/18)

33

Page 34: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (7/18)

34

The Triangular Signal. The signal is defined as

otherwise

tt

tt

t

,0

10,1

01,1

)(

Page 35: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (8/18)

35

Example 2.1.14. Plot )()(24tt

Page 36: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (9/18)

36

The Sinc Signals. The sinc signal is defined as

sinc(t)

0,,1

0,)sin(

t

tt

t

Page 37: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (10/18)

37

The Sign or the Signum Signal. The sign or the signum

signal is defined as

The signum signal can be expressed as the limit of the signal

xn(t), which is defined by

when

0,0

0,1

0,1

)sgn(

t

t

t

t

0,0

0,

0,

)(

t

te

te

tx nt

nt

n

n

Page 38: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties (11/18)

38

Page 39: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (12/18)

39

The Impulse or Delta Signal. The impulse signal is not a

function (or signal). It is a distribution or a generalized function.

A distribution is defined in terms of its effect on another

function under the integral sign

The impulse distribution can be defined by the relation

Sometimes it is helpful to visualize δ(t) as the limit of certain

known signals such as

and

)0()()( dttt

tt

1lim)(

0

tct sin

1lim)(

0

Page 40: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (13/18)

40

Page 41: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (14/18)

41

δ(t)=0 for all t ≠ 0 and δ(0)=∞

x(t)δ(t-t0)=x(t0)δ(t-t0)

For any φ(t) continuous at t0,

For any φ(t) continuous at t0,

For all a ≠ 0,

)()()( 00 tdtttt

)()()( 00 tdtttt

)(||

1)( t

aat

Page 42: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (15/18)

42

The result of the convolution of any signal with the impulse signal

is the signal itself

The unit-step signal is the integral of the impulse signal. The

impulse signal is the generalized derivatives of the unit-step signal

)()()( txttx

)()()( 00 ttxtttx

t

dtu )()(1

)()( 1 tudt

dt

Page 43: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (16/18)

43

We define the generalized derivatives of δ(t) by

We can generalize this result to

[Hint of proof]

0

)( )()1()()(

t

n

nnn t

dt

ddttt

0

)()1()()( 0

)(

tt

n

nnn t

dt

ddtttt

dtttt )()( 0

)1(

)()( 0ttdt

)()()()( 00 tdttttt

)( 0

)1( t

Page 44: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (17/18)

44

The result of the convolution of any signal with nth derivative

of x(t) is the nth derivative of x(t)

[Hint of proof] By mathematical induction,

)()()( )()( txttx nn

)()( )1( ttx

dtx )()( )1(

)()( tdx

)()()()( dxttx

)()1( tx

Page 45: Chapter 2 Signals and Linear Systems (I)

Some Important Signals and Their

Properties — Properties of δ(t) (18/18)

45

The result of the convolution of any signal x(t) with the unit-

step signal is the integral of the signal x(t)

For even values of n, δ(n)(t) is even; for odd values of n, it is

odd

t

dxtutx )()()( 1