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1 Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved. Chapter 3 Mobile Radio Propagation

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Page 1: Chapt 03

1Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Chapter 3

Mobile Radio Propagation

Page 2: Chapt 03

2Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Outline Speed, Wavelength, Frequency Types of Waves Radio Frequency Bands Propagation Mechanisms Radio Propagation Effects Free-Space Propagation Land Propagation Path Loss Fading: Slow Fading / Fast Fading Delay Spread Doppler Shift Co-Channel Interference The Near-Far Problem Digital Wireless Communication System Analog and Digital Signals Modulation Techniques

Page 3: Chapt 03

3Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Speed, Wavelength, Frequency

System Frequency Wavelength

AC current 60 Hz 5,000 km

FM radio 100 MHz 3 m

Cellular 800 MHz 37.5 cm

Ka band satellite 20 GHz 15 mm

Ultraviolet light 1015 Hz 10-7 m

Light speed = Wavelength x Frequency

= 3 x 108 m/s = 300,000 km/s

Page 4: Chapt 03

4Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Types of Waves

Transmitter Receiver

Earth

Sky wave

Space wave

Ground waveTroposphere

(0 - 12 km)

Stratosphere (12 - 50 km)

Mesosphere (50 - 80 km)

Ionosphere (80 - 720 km)

Page 5: Chapt 03

5Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Radio Frequency Bands

Classification Band

Initials Frequency Range Characteristics

Extremely low ELF < 300 Hz

Ground waveInfra low ILF 300 Hz - 3 kHz

Very low VLF 3 kHz - 30 kHz

Low LF 30 kHz - 300 kHz

Medium MF 300 kHz - 3 MHz Ground/Sky wave

High HF 3 MHz - 30 MHz Sky wave

Very high VHF 30 MHz - 300 MHz

Space waveUltra high UHF 300 MHz - 3 GHz

Super high SHF 3 GHz - 30 GHz

Extremely high EHF 30 GHz - 300 GHz

Tremendously high THF 300 GHz - 3000 GHz

Page 6: Chapt 03

6Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Propagation Mechanisms

Reflection Propagation wave impinges on an object which is large as

compared to wavelength

- e.g., the surface of the Earth, buildings, walls, etc.

Diffraction Radio path between transmitter and receiver obstructed

by surface with sharp irregular edges Waves bend around the obstacle, even when LOS (line of sight)

does not exist

Scattering Objects smaller than the wavelength of the

propagation wave

- e.g. foliage, street signs, lamp posts

Page 7: Chapt 03

7Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Radio Propagation Effects

Transmitterd

Receiver

hb

hm

Diffracted Signal

Reflected Signal

Direct Signal

Building

Page 8: Chapt 03

8Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Free-space Propagation

The received signal power at distance d:

where Pt is transmitting power, Ae is effective area, and Gt is the transmitting antenna gain. Assuming that the radiated power is uniformly distributed over the surface of the sphere.

Transmitter Distance dReceiver

hb

hm

2r

4P

d

PGA tte

Page 9: Chapt 03

9Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Antenna Gain For a circular reflector antenna Gain G = ( D / )2

= net efficiency (depends on the electric field distribution over the antenna aperture, losses, ohmic heating , typically 0.55)

D = diameter thus, G = ( D f /c )2, c = f (c is speed of light)

Example: Antenna with diameter = 2 m, frequency = 6 GHz, wavelength = 0.05 m G = 39.4 dB Frequency = 14 GHz, same diameter, wavelength = 0.021 m G = 46.9 dB * Higher the frequency, higher the gain for the same size antenna

Page 10: Chapt 03

10Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Land Propagation

The received signal power:

where Gr is the receiver antenna gain,

L is the propagation loss in the channel, i.e.,

L = LP LS LF

L

PGGP trt

r

Fast fading

Slow fading

Path loss

Page 11: Chapt 03

11Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Path Loss (Free-space)

Definition of path loss LP :

Path Loss in Free-space:

where fc is the carrier frequency.

This shows greater the fc , more is the loss.

,r

tP P

PL

),(log20)(log2045.32)( 1010 kmdMHzfdBL cPF

Page 12: Chapt 03

12Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Path Loss (Land Propagation)

Simplest Formula:

Lp = A d-α

where

A and α: propagation constants

d : distance between transmitter and receiver

α : value of 3 ~ 4 in typical urban area

Page 13: Chapt 03

13Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Example of Path Loss (Free-space)

Path Loss in Free-space

70

80

90

100

110

120

130

0 5 10 15 20 25 30

Distance d (km)

Path

Los

s Lf

(dB)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

Page 14: Chapt 03

14Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Path Loss (Urban, Suburban and Open areas)

Urban area:

where

Suburban area:

Open area:

)(log)(log55.69.44

)()(log82.13)(log16.2655.69)(

1010

1010

kmdmh

mhmhMHzfdBL

b

mbcPU

citymediumsmallfor

MHzfformh

MHzfformh

cityelforMHzfmhMHzf

mh

cm

cm

cmc

m &,400,97.4)(75.11log2.3

200,1.1)(54.1log29.8

arg,8.0)(log56.1)(7.0)(log1.1

)(2

10

210

1010

4.528

)(log2)()(

2

10

MHzfdBLdBL c

PUPS

94.40)(log33.18)(log78.4)()( 102

10 MHzfMHzfdBLdBL ccPUPO

Page 15: Chapt 03

15Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Path Loss

Path loss in decreasing order: Urban area (large city) Urban area (medium and small city) Suburban area Open area

Page 16: Chapt 03

16Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Example of Path Loss (Urban Area: Large City)

Path Loss in Urban Area in Large City

100

110

120

130

140

150

160

170

180

0 10 20 30

Distance d (km)

Pat

h Lo

ss L

pu (

dB)

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

fc=150MHz

Page 17: Chapt 03

17Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Example of Path Loss (Urban Area: Medium and Small Cities)

Path Loss in Urban Area for Small & Medium Cities

100

110

120

130

140

150

160

170

180

0 10 20 30

Distance d (km)

Pat

h Lo

ss L

pu (

dB) fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

Page 18: Chapt 03

18Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Example of Path Loss (Suburban Area)

Path Loss in Suburban Area

90

100

110

120

130

140

150

160

170

0 5 10 15 20 25 30

Distance d (km)

Path

Los

s Lp

s (d

B)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

Page 19: Chapt 03

19Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Example of Path Loss (Open Area)

Path Loss in Open Area

80

90

100

110

120

130

140

150

0 5 10 15 20 25 30

Distance d (km)

Path

Los

s Lp

o (d

B)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

Page 20: Chapt 03

20Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Fading

Signal Strength

(dB)

Distance

Path Loss

Slow Fading (Long-term fading)

Fast Fading (Short-term fading)

Page 21: Chapt 03

21Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Slow Fading

The long-term variation in the mean level is known as slow fading (shadowing or log-normal fading). This fading caused by shadowing.

Log-normal distribution:

- The pdf of the received signal level is given in decibels by

where M is the true received signal level m in decibels, i.e., 10log10m, M is the area average signal level, i.e., the mean of M,

is the standard deviation in decibels

,2

1 2

2

2

MM

eMp

Page 22: Chapt 03

22Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Log-normal Distribution

MM

2

p(M)

The pdf of the received signal level

Page 23: Chapt 03

23Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Fast Fading The signal from the transmitter may be reflected from

objects such as hills, buildings, or vehicles. When MS far from BS, the envelope distribution of received signal

is Rayleigh distribution. The pdf is

where is the standard deviation. Middle value rm of envelope signal within sample range to be

satisfied by

We have rm = 1.777

0,2

2

22

rer

rpr

.5.0)( mrrP

Page 24: Chapt 03

24Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Rayleigh Distribution

The pdf of the envelope variation

r2 4 6 8 10

P(r)

0

0.2

0.4

0.6

0.8

1.0

=1

=2

=3

Page 25: Chapt 03

25Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Fast Fading (Continued)

When MS far from BS, the envelope distribution of received signal is Rician distribution. The pdf is

where is the standard deviation,

I0(x) is the zero-order Bessel function of the first kind,

is the amplitude of the direct signal

0,02

2

2

22

rr

Ier

rpr

Page 26: Chapt 03

26Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Rician Distribution

r

Pdf

p(r

)

r86420

0.6

0.5

0.4

0.3

0.2

0.1

0

= 2 = 1= 0 (Rayleigh)

= 1

= 3

The pdf of the envelope variation

Page 27: Chapt 03

27Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Characteristics of Instantaneous Amplitude

Level Crossing Rate: Average number of times per second that the signal

envelope crosses the level in positive going direction. Fading Rate:

Number of times signal envelope crosses middle value in positive going direction per unit time.

Depth of Fading: Ratio of mean square value and minimum value of

fading signal. Fading Duration:

Time for which signal is below given threshold.

Page 28: Chapt 03

28Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Doppler Shift Doppler Effect: When a wave source and a receiver are moving towards

each other, the frequency of the received signal will not be the same as the source.

When they are moving toward each other, the frequency of the received signal is higher than the source.

When they are opposing each other, the frequency decreases.

Thus, the frequency of the received signal is

where fC is the frequency of source carrier,

fD is the Doppler frequency. Doppler Shift in frequency:

where v is the moving speed, is the wavelength of carrier.

cosv

fD

DCR fff

MS

Signal

Moving speed v

Page 29: Chapt 03

29Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Delay Spread

When a signal propagates from a transmitter to a receiver, signal suffers one or more reflections.

This forces signal to follow different paths. Each path has different path length, so the time of

arrival for each path is different. This effect which spreads out the signal is called

“Delay Spread”.

Page 30: Chapt 03

30Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Moving Speed Effect

Time

V1 V2 V3 V4

Sig

nal s

tren

gth

Page 31: Chapt 03

31Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Delay Spread

Delay

Sig

nal S

tren

gth

The signals from close by reflectors

The signals from intermediate reflectors

The signals from far away reflectors

Page 32: Chapt 03

32Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Intersymbol Interference (ISI)

Caused by time delayed multipath signals Has impact on burst error rate of channel Second multipath is delayed and is received

during next symbol For low bit-error-rate (BER)

R (digital transmission rate) limited by delay spread d.

dR

2

1

Page 33: Chapt 03

33Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Intersymbol Interference (ISI)

Time

Time

Time

Transmission signal

Received signal (short delay)

Received signal (long delay)

1

0

1

Propagation timeDelayed signals

Page 34: Chapt 03

34Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Coherence Bandwidth

Coherence bandwidth Bc: Represents correlation between 2 fading signal

envelopes at frequencies f1 and f2. Is a function of delay spread. Two frequencies that are larger than coherence

bandwidth fade independently. Concept useful in diversity reception

Multiple copies of same message are sent using different frequencies.

Page 35: Chapt 03

35Copyright © 2003, Dr. Dharma P. Agrawal and Dr. Qing-An Zeng. All rights reserved.

Cochannel Interference

Cells having the same frequency interfere with each other. rd is the desired signal

ru is the interfering undesired signal is the protection ratio for which

rd ru (so that the signals interfere the least)

If P(rd ru ) is the probability that rd ru ,

Cochannel probability Pco = P(rd ru )