Wireless Networks Ch2

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Ali BAZZI

Chapter 2

Mobile Radio Propagation


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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


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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


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Transmit

ter Receiver

Earth

Sky wave

Space wave

Ground waveTroposphere

(0 - 12 km)

Stratosphere

(12 - 50 km)

Mesosphere

(50 - 80 km)

Ionosphere

(80 - 720 km)


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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 wave

Ultra high UHF 300 MHz - 3 GHz

Super high SHF 3 GHz - 30 GHzExtremely high EHF 30 GHz - 300 GHz

Tremendously high THF 300 GHz - 3000 GHz


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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 thepropagation wave

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


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Transmitterd

Receiver

hb

hm

Diffracted

Signal

Reflected Signal

Direct Signal

Building


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The received signal power at distance d:

wherePtis transmitting power,Ae is effective area, and Gtis thetransmitting antenna gain. Assuming that the radiated power is uniformlydistributed over the surface of the sphere.

Transmitter Distance d Receiver

hb

hm

2r

4P

d

PGA tte

=


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For a circular reflector antenna

Gain G = (D /)2

= net efficiency (depends on the electric field distribution over theantenna 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 mG = 39.4 dB

Frequency = 14 GHz, same diameter, wavelength = 0.021 mG = 46.9 dB

* Higher the frequency, higher the gain for the same size antenna


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The received signal power:

where Gris the receiver antenna gain,L is the propagation loss in the channel, i.e.,

L = LPLSLF

L

PGGP

trt

r=

Fast fading

Slow fading

Path loss


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Definition of path lossLP:

Path Loss in Free-space:

wherefc is the carrier frequency.

This shows greater thefc ,

more is the loss.

,

r

t

P

P

PL =

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


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Simplest Formula:Lp = A d

-

whereA and : propagation constants

d: distance between transmitter and receiver

: value of 3 ~ 4 in typical urban area


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Path Loss in Free-space

70

80

90

100

110

120

130

0 5 10 15 20 25 30

Distance d (km)

Path

Loss

Lf

(dB) fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz


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Urban area:

where

Suburban area:

Open area:

[ ] )(log)(log55.69.44)()(log82.13)(log16.2655.69)(

1010

1010

kmdmh

mhmhMHzfdBL

b

mbcPU

+

+=

[ ]

[ ] [ ]

[ ][ ]

=

citymediumsmallforMHzfformh

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

LPS(dB) = LPU(dB) 2 log10fc(MHz)

28

"

#$%

&'

2

5.4

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

10 += MHzfMHzfdBLdBL ccPUPO


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


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Path Loss in Urban Area in Large City

100

110

120

130

140

150

160

170

180

0 10 20 30

Distance d (km)

Path

LossLpu

(dB)

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz

fc=150MHz


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Path Loss in Urban Area for Small & Medium Cities

100

110

120

130

140150

160

170

180

0 10 20 30

Distance d (km)

Path

Loss

Lp

u

(dB)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz


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Path Loss in Suburban Area

90

100

110

120

130140

150

160

170

0 5 10 15 20 25 30

Distance d (km)

Path

LossLp

s(dB)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz


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Path Loss in Open Area

80

90

100

110

120

130

140

150

0 5 10 15 20 25 30

Distance d (km)

Path

LossLp

o

(dB)

fc=150MHz

fc=200MHz

fc=400MHz

fc=800MHz

fc=1000MHz

fc=1500MHz


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Signal

Strength(dB)

Distance

Path Loss

Slow Fading(Long-term fading)

Fast Fading(Short-term fading)


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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

whereMis the true received signal level m in decibels, i.e., 10log10m,

Mis the area average signal level, i.e., the mean ofM,

is the standard deviation in decibels

( )

( )

,2

1 22

2

MM

eMp

=


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M

M

2

p(M)

The pdf of the received signal level


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The signal from the transmitter may be reflected from objectssuch as hills, buildings, or vehicles.

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

where is the standard deviation.

Middle value rm of envelope signal within sample range to be satisfiedby

We have rm = 1.777

( ) 0,2

2

2

2 >=

re

r

rp

r

.5.0)( = mrrP


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r

2 4 6 8 10

P(r)

0

0.2

0.4

0.6

0.8

1.0

=1

=2

=3


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When MS is close to the BS, the envelope distribution ofreceived 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

( ) 0,0

2

2

2

22

=

+

rr

Ier

rp

r


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r

Pdfp(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


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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.


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Doppler Effect: When a wave source and a receiver are moving towardseach other, the frequency of the received signal will not be the same as thesource. 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

wherefCis 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.

cos

v

fD=

DCR fff

=

MS

Signal

Movingspeed v


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When a signal propagates from a transmitter to areceiver, 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 calledDelay Spread.


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Time

V1 V2 V3 V4

Signalstre

ngth


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Delay

SignalStre

ngth

The signals from

close by reflectors

The signals from

intermediate reflectors

The signals from

far away reflectors


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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.d

R2

1

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Wireless Networks Ch2