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EC744 Wireless Communication Fall 2008 Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview

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Page 1: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

EC744 Wireless Communication Fall 2008

Mohamed Essam KhedrDepartment of Electronics and Communications

Wireless Communication Channel Overview

Page 2: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Syllabus

� Tentatively

Channel coding techniquesWeek 6

Mid Term exam (take home), Diversity techniquesWeek 7

Equalization techniquesWeek 8

Spread spectrum, MIMO and OFDMWeek 9

Wireless networking: 802.11, 802.16, UWBWeek 10

Hot topicsWeek 11

PresentationsWeek 12

PresentationsWeek 13

Final ExamWeek 15

PresentationsWeek 14

Source coding techniquesWeek 5

Modulation techniquesDemodulation techniques (coherent and non-coherent)

Week 4

Channel characteristics (AWGN, fading)Week 3

Digital Communication fundamentalsWeek 2

Overview wireless communications, Probabilities Week 1

Page 3: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Antenna - Ideal - contd.

� The power density of an ideal loss-less antenna at a distance d away from the transmitting antenna:

24 dGP

P tta π

=

• Gt is the transmitting antenna gain• The product PtGt : Equivalent Isotropic Radiation Power

(EIRP)which is the power fed to a perfect isotropic antenna to get the same output power of the practical antenna in hand.

Note: the area is for asphere.W/m2

Page 4: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Signal Propagation(Channel Models)

Page 5: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Models

� High degree of variability (in time, space etc.)� Large signal attenuation� Non-stationary, unpredictable and random

– Unlike wired channels it is highly dependent on the environment,time space etc.

� Modelling is done in a statistical fashion� The location of the base station antenna has a significant

effect on channel modeling� Models are only an approximation of the actual signal

propagation in the medium.� Are used for:

– performance analysis– simulations of mobile systems– measurements in a controlled environment, to guarantee

repeatability and to avoid the expensive measurements in the field.

Page 6: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Models - Classifications

� System Model - Deterministic

� Propagation Model- Deterministic– Predicts the received signal strength at a distance from the

transmitter– Derived using a combination of theoretical and empirical method.

� Stochastic Model - Rayleigh channel

� Semi-empirical (Practical +Theoretical) Models

Page 7: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Models

� Is almost always linear, and also time-variant because of its mobility. Thus, fully described by its impulse response h(τ, t),where τ is the delay parameter and t is the time.

� The complex impulse response h(τ, t) is a low-pass equivalent model of the actual real band-pass impulse response.

� Equivalently, the channel is characterized by its transfer function which is the Fourier transform of the h(τ, t):

�∞

∞−

−= ττπτ dfjthtfH )exp(),(),( 2

The magnitude |H(f , t)| is changing randomly in time, so the mobile radio channel is described as a fading channel.The phase arg H(f , t) is also a random function of time.

Page 8: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Models

� Multi-path channel impulse response

))(())],()(2(exp[),(),(1

0

tttfjtath iii

N

icib ττδτφτπττ −+=�

=

Page 9: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation Path Loss

� The propagation path loss isLPE = LaLlf Lsf

where La is average path loss (attenuation): (1-10

km),Llf - long term fading (shadowing): 100 m

ignoring variations over few wavelengths,Lsf - short term fading (multipath): over fraction

of wavelength to few wavelength.� Metrics (dBm, mW)

[P(dBm) = 10 * log[ P(mW) ]

Page 10: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation Path Loss – Free Space

� Power received at the receiving antenna

2

4��

���

πλ=d

GGPP rttr

• Isotropic antenna has unity gain (G = 1) for both transmitter and receiver.

Thus the free space propagation path loss is definedas:

��

πλ−=−= 2

2

1010 )4(10Log10

dGG

LogPP

L rt

t

rf

Page 11: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation - Free Space–contd.

The difference between two received signal powers infree space is:

dB21

log20log10 102

110 �

���

�=���

����

�=∆

dd

PP

Pr

r

If d2 = 2d1, the ∆P = -6 dB i.e 6 dB/octave or 20 dB/decade

Page 12: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation - Non-Line-of-Sight

• Generally the received power can be expressed as:

Pr ∝∝∝∝ d-v

• For line of sight v = 2, and the received powerPr ∝∝∝∝ d-2

• For non-line of sight with no shadowing, received power at any distance d can be expressed as:

��

��

�+=

refrr d

dvdPdP 10ref10 log10)]([log10)(

100 m< dref < 1000 m

Page 13: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation - Non-Line-of-Sight

� Log-normal Shadowing

Where X�: N(0,�) Gaussian distributed random variable

σXd

dvdPdP

refrr +

��

��

�+= 10ref10 log10)]([log10)(

Page 14: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Received Power for Different Value of Loss Parameter v

Distance (km)0 10 20 30 40 50

-70

-80

-90

-100

-110

-120

-130-135

Rec

eive

d po

wer

(dB

m)

v = 2, Free space

v = 3 Rural areas

v = 4,

City and urban areas

Page 15: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation Model- Free Space

dB)(log20)(log2044.32 1010 dfLf ++=

Expressing frequency in MHz and distance d in km:

dB)(log20)(log20)4/3.0(log20

)(log20)(log20)4/(log20

101010

101010

df

dfcLf

++π−=

++π−=

In terms of frequency f and the free space velocity of electromagnetic wave c = 3 x 108 m/s it is:

dB4

/log20 10 �

���

π−=

dfc

Lf

Page 16: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation Model- Free Space (non-ideal, path loss)

• Non-isotropic antenna gain ≠ unity, and there are additional losses Lad , thus the power received is:

ad

trtr Ld

PGGP

1)4( 2

2

⋅πλ= d > 0 and L≥ 0

Thus for Non-isotropic antenna the path loss is:

dB)(log10)(log20)(log20

)4/(log20)(log10)(log10

101010

101010

ad

rtnif

Ldf

cGGL

+++

π−−−=−

BS MU

Note: Interference margin can also be added

Page 17: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Propagation Model - Mechanisms

� Reflection � Diffraction� Scattering

Source: P M Shankar

Page 18: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss - 2 Ray Reflection

� In mobile radio systems the height of both antennas (Tx. and Rx.) << d (distance of separation)

From the geometry dd = √[d2 + (hb - hm )2]

hb

dd

dr

hm

Direct path (line of sight)

Ground reflected path

d

Page 19: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss -contd.

Using the binomial expansionNote d >> hb or hm.

��

���

��

���

��

���

� −+≅

2

5.01d

hhdd mb

d

The path difference ∆d = dr - dd = 2(hbhm )/d

Similarly��

���

��

���

��

���

� ++≅

2

5.01d

hhdd mb

r

The phase differencedhh

dhh mbmb

λπ

=×λπ=φ∆

422

Page 20: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss– contd.

Total received power

22

14

φ∆ρ+×��

���

πλ= j

rttr ed

GGPP

Where ρ is the reflection coefficient. For ρ = -1 (low angle of incident) and .

)2/(sin4

)cos1(2sin)cos1(1

sincos11

2

222

φ∆=

φ∆−=φ∆+φ∆−=−

φ∆+φ∆−=−φ∆−

φ∆−

j

j

eHence

je

Page 21: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss– contd.

Therefore: ��

���

λπ×�

���

πλ=

dhh

dGGPP mb

rttr2

42

2

sin

Assuming that d >> hm or hb, then 12

<<��

���

λπ

dhh mb

sin x = x for small x

Thus2

2 ��

���

�=dhh

GGPP mbrttr which is 4th power law

Page 22: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss– contd.

In a more general form (no fading due to multipath), path attenuation is

d�log40log20

log20log10log10

1010

101010

dh

hGGL

m

brtPE

+−−−−=

• LPE increases by 40 dB each time d increases by 10

Propagation path loss (mean loss)

��

���

���

�=���

����

�−=

2

2log10log10dhh

GGPP

L mbrt

t

rPE

Compared with the free space = Pr = 1/ d2

Page 23: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Channel Model- Plan Earth Path Loss– contd.

Vertical

Horizontal

Pr ~ 1/d2

Pr ~ 1/d4

Free space

S Loyka

Page 24: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

LOS Channel Model - Problems

� Simple theoretical models do not take into account many practical factors:– Rough terrain– Buildings– Refection– Moving vehicle– Shadowing

Thus resulting in bad accuracy

Solution: Semi- empirical Model

Page 25: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Sem-iempirical Model

Practical models are based on combination of measurement and theory. Correction factors are introduced to account for:– Terrain profile– Antenna heights– Building profiles– Road shape/orientation– Lakes, etc.

� Okumura model� Hata model

� Saleh model� SIRCIM model

Outdoor

Indoor

Y. Okumura, et al, Rev. Elec. Commun. Lab., 16( 9), 1968.M. Hata, IEEE Trans. Veh. Technol., 29, pp. 317-325, 1980.

Page 26: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Okumura Model

� Widely used empirical model (no analytical basis!) in macrocellular environment

� Predicts average (median) path loss� “Accurate” within 10-14 dB in urban and suburban

areas� Frequency range: 150-1500 MHz� Distance: > 1 km� BS antenna height: > 30 m.� MU antenna height: up to 3m. � Correction factors are then added.

Page 27: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model

� Consolidate Okumura’s model in standard formulas for macrocells in urban, suburban and open rural areas.

� Empirically derived correction factors are incorporated into the standard formula to account for:– Terrain profile– Antenna heights– Building profiles– Street shape/orientation– Lakes– Etc.

Page 28: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model – contd.

� The loss is given in terms of effective heights. � The starting point is an urban area. The BS

antennae is mounted on tall buildings. The effective height is then estimated at 3 - 15 km from the base of the antennae.

P M Shankar

Page 29: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model - Limits

� Frequency range: 150 - 1500 MHz� Distance: 1 – 20 km� BS antena height: 30- 200 m� MU antenna height: 1 – 10 m

Page 30: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model – Standard Formula forAverage Path Loss for Urban Areas

�������������������

� ���������

( ) ( )( ) (dB)log82.13

loglog55.69.44log16.2655.69

10

101010

mub

bupl

hah

dhfL

−−

−++=−

( ) ( )[ ] ( ) dBMHz400 97.475.11log2.3 210 ≥−= fhha mumu

( ) ( )[ ] ( )[ ] dB 8.0log56.17.0log1.1 1010 −−−= fhfha mumu

( ) ( )[ ] ( ) dBMHz200 1.15.1log3.8 210 ≤−= fhha mumu

� � �������������������

Page 31: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model – Average Path Loss for Urban Areas contd.

Carrier frequency • 900 MHz,

BS antenna height • 150 m,

MU antenna height • 1.5m.

P M Shankar

Page 32: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model – Average Path Loss for Suburban and Open Areas

� Suburban Areas

� Open Areas

94.40Log33.18)(Log78.4 210 −−−= −− ffLL uplopl

4.528

Log22

10 −

��

���

���

�−= −−f

LL uplsupl

Page 33: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Hata Model - Average Path Loss

S. Loyka, 2003, Introduction to Mobile Communications

Page 34: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Improved Model

� Hata-Okumura model are not suitable for lower BS antenna heights (2 m), and hilly or moderate-to-heavy wooded terrain.

� To correct for these limitations the following model is used [1]:

� For a given close-in distance dref. the average path loss is:

Lpl = A + 10 v log10 (d / dref) + s for d > dref, (dB)

where A = 20 log10(4 � dref / �) v is the path-loss exponent = (a – b hb + c / hb) hb is the height of the BS: between 10 m and 80 m dref = 100m and

a, b, c are constants dependent on the terrain categorys is representing the shadowing effect

[1] V. Erceg et. al, IEEE JSAC, 17 (7), July 1999, pp. 1205-1211.

Page 35: Mohamed Essam Khedrwebmail.aast.edu/~khedr/Courses/Graduate/Wireless...Mohamed Essam Khedr Department of Electronics and Communications Wireless Communication Channel Overview Syllabus

Improved Model

� Terrain A: The maximum path loss category is hilly terrain with moderate-to-heavy tree densities .

� Terrain B: Intermediate path loss condition� Terrain B: The minimum path loss category which is mostly flat terrain

with light tree densities

TerrainsModel Type A Type B Type Cparametera 4.6 4 3.6 b 0.0075 0.0065 0.005 c 12.6 17.1 20

The typical value of the standard deviation for s is between 8.2 And 10.6 dB, depending on the terrain/tree density type