chapter 6 bandpass random processes

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EEE 461 1 Chapter 6 Chapter 6 Bandpass Random Processes Bandpass Random Processes Huseyin Bilgekul EEE 461 Communication Systems II Department of Electrical and Electronic Engineering Eastern Mediterranean University Bandpass Random Processes PSD of bandpass random processes BP Filtered White Noise Sinusoids in Gaussian Noise

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Chapter 6 Bandpass Random Processes. Bandpass Random Processes PSD of bandpass random processes BP Filtered White Noise Sinusoids in Gaussian Noise. Huseyin Bilgekul EEE 461 Communication Systems II Department of Electrical and Electronic Engineering Eastern Mediterranean University. - PowerPoint PPT Presentation

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Page 1: Chapter 6 Bandpass Random Processes

EEE 461 1

Chapter 6Chapter 6Bandpass Random Processes Bandpass Random Processes

Huseyin BilgekulEEE 461 Communication Systems II

Department of Electrical and Electronic Engineering Eastern Mediterranean University

Bandpass Random Processes PSD of bandpass random processes BP Filtered White Noise Sinusoids in Gaussian Noise

Page 2: Chapter 6 Bandpass Random Processes

EEE 461 2

Homework AssignmentsHomework Assignments

• Return date: December 13, 2005.

• Assignments:

Problem 6-38

Problem 6-41

Problem 6-45

Problem 6-48

Problem 6-50

Page 3: Chapter 6 Bandpass Random Processes

EEE 461 3

Equivalent Representations of Bandpass Equivalent Representations of Bandpass SignalsSignals

• Remind: Equivalent representations of a bandpass signal

Px(f)

f0 fcfc

( ) ( )

Envelope and Phase form

Inphase and Quadrature (IQ) form

Complex

Re cos

Envelope of (

cos si

( ))

n

( )

c

c c

j j t

jc

t

t

gg t x

v t

t jy t g t e R t e

g t e R t t t

v t x t t y t

t

t

v

Re ( )cos ( )

Im ( )sin ( )

x t g t R t t

y t g t R t t

2 2

1

( ) ( ) ( )

( )( ) ( ) tan ( )

( )

R t g t x t y t

y tt g t

x t

Page 4: Chapter 6 Bandpass Random Processes

EEE 461 4

Bandpass Random ProcessBandpass Random Process• If x(t) and y(t) are jointly WSS processes, the real bandpass process

Will be WSS stationary if and only if:

Re cos sincj tc cv t g t e x t t y t t

• If v(t) is a Gaussian random process then g(t), x(t) and y(t) are Gaussian processes since they are linear functions v(t). However R(t) θ(t) are NOT Gaussian because they are NONLIEAR functions of v(t).

Page 5: Chapter 6 Bandpass Random Processes

EEE 461 5

Bandpass Random ProcessBandpass Random Process• What happens to a signal at a receiver? How does the PSD of the

signal after a BPF correspond to the signal before the BPF?

• Remind: Equivalent representations of a bandpass signal

Px(f)

f0 fcfc

( ) ( )

Envelope and Phase form

Inphase and Quadrature (IQ) form

Complex

Re cos

Envelope of (

cos si

( ))

n

( )

c

c c

j j t

jc

t

t

gg t x

v t

t jy t g t e R t e

g t e R t t t

v t x t t y t

t

t

v

Re ( )cos ( )

Im ( )sin ( )

x t g t R t t

y t g t R t t

2 2

1

( ) ( ) ( )

( )( ) ( ) tan ( )

( )

R t g t x t y t

y tt g t

x t

Page 6: Chapter 6 Bandpass Random Processes

EEE 461 6

BPF System BPF System • Bandpass random process can be written as:

• With the impulse response: Re cos sincj t

c cv t g t e x t t y t t

Ideal LPFH0(f)

v(t)

BP ProcessIdeal LPF

H0(f)

x

x x

x

+

Basebandx(t)

Inphase

Basebandy(t)

Quadrature

2cos(ct+)

2sin(ct+) sin(ct+)

cos(ct+)

0 02 cosh t h t t

v(t)

BP Process

Page 7: Chapter 6 Bandpass Random Processes

EEE 461 7

Impulse ResponseImpulse Response

• Impulse Response

• Transfer Function

• So, x(t) and y(t) are low-pass random processes, what else can be deduced?

• Assume theta is uniformly distributed phase noise

0 02 cosh t h t t

0 0c cH f H f f H f f

1

H0(f )1

2H (f )

0 fcfc

Page 8: Chapter 6 Bandpass Random Processes

EEE 461 8

PSD of BP Random ProcessesPSD of BP Random Processes• PSD of x(t) and y(t)

Pv(f )

ffcfc

Px(f) or Py(f)

f0 fcfc

0

v c v c o

x y

o

P f f P f f f BP f P f

f B

Pv(ffc)

f0 fcfc

LPFPv(ffc)

Page 9: Chapter 6 Bandpass Random Processes

EEE 461 9

PSD of BP Random ProcessesPSD of BP Random Processes

Page 10: Chapter 6 Bandpass Random Processes

EEE 461 10

PSD of BP Random ProcessesPSD of BP Random Processes

Page 11: Chapter 6 Bandpass Random Processes

EEE 461 11

Properties of WSS BP ProcessesProperties of WSS BP Processes• If the narrowband noise is Gaussian, then the in-phase x(t) and quadrature y(t)

components are jointly Gaussian

• If the narrow band noise is wide-sense stationary (WSS), then the in-phase and quadrature components are jointly WSS.

• In-phase and quadrature components have the same PSD.

• In-phase and quadrature components of narrowband noise are zero-mean

– Noise comes original signal being passed through a narrowband linear filter

• Variance of the processes is the same (area under PSD same)

________ ________ ________

22 2 2 1( )

21

(0) (0) (0) (0)2v x y g

v t x t y t g t

R R R R

( ) ( ) 0x t y t

Page 12: Chapter 6 Bandpass Random Processes

EEE 461 12

Properties of WSS BP Processes Properties of WSS BP Processes ContinuedContinued

• Bandpass PSD from baseband PSD.

• PSD of I and Q from bandpass PSD

1

4v g c g cP f P f f P f f

0

v c v c o

x y

o

P f f P f f f BP f P f

f B

Page 13: Chapter 6 Bandpass Random Processes

EEE 461 13

BP White Noise ProcessBP White Noise Process

• The PSD of a BP white noise process is No/2. What is the PSD and variance of the in-phase and quadrature components?

• From the SNR calculations, it is clear that the variance of the white noise is:

cos sin

0

0

x c y c

n c n c

x y

o

x y

n t n t t n t t

S f f S f f f BP f P f

f B

N f BP f P f

f B

___ ____ ____2 2 22 2

2

c

c

f Bo

x yf B

Nn df NB n n

Page 14: Chapter 6 Bandpass Random Processes

EEE 461 14

Sinusoids in Gaussian NoiseSinusoids in Gaussian Noise

• Signal is a sinusoid mixed with narrow-band additive white Gaussian noise (AWGN)

• Can be written in terms of ENVELOPE and PHASE terms as:

tntAty c cos

2 2

21

cos sin

cos

Envelope

tan Phase

x c y c

c

x y

y

x

y t A n t t n t t

R t t t

R t A n t n t

n tt

A n t

Page 15: Chapter 6 Bandpass Random Processes

EEE 461 15

• In-phase and Quadrature terms of noise Gaussian with variance 2.

• Similar transformation to that used for calculating the dart board example, the joint density can be found in polar coordinates.

• Marginal density of the Envelope is Rician type.

• Approaches a Gaussian if A >>

2 2 22 cos / 2

2,

2

R AR A

R

Rf R e

Sinusoids in Gaussian NoiseSinusoids in Gaussian Noise

2 2 2 2

2 2 2

/ 2 cos /

2

/ 2

02 2

1,

2

R A ARR R

R A

Rf R f R d e e d

R ARe I