AntennasPropagatiooooooooooooooooooooooooooooon.ppt

Wireless Networks Fall 2007
Antennas & Propagation
CSG 250
Fall 2007
Rajmohan Rajaraman

Introduction
An antenna is an electrical conductor or
system of conductors
o Transmission - radiates electromagnetic energy
into space
o Reception - collects electromagnetic energy
from space
In two-way communication, the same
antenna can be used for transmission and
reception

Radiation Patterns
 Radiation pattern
o Graphical representation of radiation properties of an
antenna
o Depicted as two-dimensional cross section
 Beam width (or half-power beam width)
o Measure of directivity of antenna
o Angle within which power radiated is at least half of that
in most preferred direction
 Reception pattern
o Receiving antenna’s equivalent to radiation pattern
 Omnidirectional vs. directional antenna

Types of Antennas
 Isotropic antenna (idealized)
o Radiates power equally in all directions
 Dipole antennas
o Half-wave dipole antenna (or Hertz antenna)
o Quarter-wave vertical antenna (or Marconi antenna)
 Parabolic Reflective Antenna
o Used for terrestrial microwave and satellite applications
o Larger the diameter, the more tightly directional is the
beam

Antenna Gain
Antenna gain
o Power output, in a particular direction,
compared to that produced in any direction by
a perfect omnidirectional antenna (isotropic
antenna)
Expressed in terms of effective area
o Related to physical size and shape of antenna

Antenna Gain
 Relationship between antenna gain and effective
area
• G = antenna gain
• Ae = effective area
• f = carrier frequency
• c = speed of light (≈ 3 x 108
m/s)
  = carrier wavelength
2
2
2
4
4
c
A
f
A
G e
e π
λ
π
=
=

Propagation Modes
Ground-wave propagation
Sky-wave propagation
Line-of-sight propagation

Ground Wave Propagation

Ground Wave Propagation
Follows contour of the earth
Can Propagate considerable distances
Frequencies up to 2 MHz
Example
o AM radio

Sky Wave Propagation

Sky Wave Propagation
 Signal reflected from ionized layer of atmosphere
back down to earth
 Signal can travel a number of hops, back and
forth between ionosphere and earth’s surface
 Reflection effect caused by refraction
 Examples
o Amateur radio
o CB radio
o International broadcasts

Line-of-Sight Propagation

Line-of-Sight Propagation
 Above 30 MHz neither ground nor sky wave
propagation operates
 Transmitting and receiving antennas must be
within line of sight
o Satellite communication – signal above 30 MHz not
reflected by ionosphere
o Ground communication – antennas within effective line
of site due to refraction
 Refraction – bending of microwaves by the
atmosphere
o Velocity of electromagnetic wave is a function of the
density of the medium
o When wave changes medium, speed changes
o Wave bends at the boundary between mediums

Line-of-Sight Equations
Optical line of sight
Effective, or radio, line of sight
• d = distance between antenna and horizon
(km)
• h = antenna height (m)
• K = adjustment factor to account for
refraction, rule of thumb K = 4/3
h
d 57
.
3
=
h
d Κ
= 57
.
3

Line-of-Sight Equations
Maximum distance between two antennas
for LOS propagation:
• h1 = height of antenna one
• h2 = height of antenna two
( )
2
1
57
.
3 h
h Κ
+
Κ

LOS Wireless Transmission
Impairments
Attenuation
o Free space loss
Distortion
Dispersion
Noise
Other effects:
o Atmospheric absorption
o Multipath
o Refraction

Attenuation
 Strength of signal falls off with distance over
transmission medium
 Attenuation factors for unguided media:
o Received signal must have sufficient strength so that
circuitry in the receiver can interpret the signal
o Signal must maintain a level sufficiently higher than
noise to be received without error
o Attenuation is greater at higher frequencies, causing
distortion

Free Space Loss
 Free space loss, ideal isotropic antenna
• Pt = signal power at transmitting antenna
• Pr = signal power at receiving antenna
  = carrier wavelength
• d = propagation distance between antennas
• c = speed of light (≈ 3 x 108
m/s)
where d and  are in the same units (e.g., meters)
( ) ( )
2
2
2
2
4
4
c
fd
d
P
P
r
t π
λ
π
=
=

Free Space Loss
Free space loss equation can be recast:
⎟
⎠
⎞
⎜
⎝
⎛
=
=
λ
πd
P
P
L
r
t
dB
4
log
20
log
10
( ) ( ) dB
98
.
21
log
20
log
20 +
+
−
= d
λ
( ) ( ) dB
56
.
147
log
20
log
20
4
log
20 −
+
=
⎟
⎠
⎞
⎜
⎝
⎛
= d
f
c
fd
π

Free Space Loss
 Free space loss accounting for gain of antennas
• Gt = gain of transmitting antenna
• Gr = gain of receiving antenna
• At = effective area of transmitting antenna
• Ar = effective area of receiving antenna
o In the above formula, the powers correspond to that of
the input signal at the transmitter and output at the
receiver, respectively
( ) ( ) ( ) ( )
t
r
t
r
t
r
r
t
A
A
f
cd
A
A
d
G
G
d
P
P
2
2
2
2
2
2
4
=
=
=
λ
λ
π

Free Space Loss
Free space loss accounting for gain of
other antennas can be recast as
( ) ( ) ( )
r
t
dB A
A
d
L log
10
log
20
log
20 −
+
= λ
( ) ( ) ( ) dB
54
.
169
log
10
log
20
log
20 +
−
+
−
= r
t A
A
d
f

Path Loss Exponents
 The free space path loss model is idealized
 Here the exponent  depends on the transmission
environment
o Urban vs suburban, medium-city vs large-city,
obstructed vs unobstructed, indoors vs outdoors
o Generally between 2 and 4
o Obtained empirically
€
Pt
Pr
= Adα

Distortion
Signals at higher frequencies attenuate
more than that at lower frequencies
Shape of a signal comprising of
components in a frequency band is
distorted
To recover the original signal shape,
attenuation is equalized by amplifying
higher frequencies more than lower ones

Dispersion
Electromagnetic energy spreads in space
as it propagates
Consequently, bursts sent in rapid
succession tend to merge as they
propagate
For guided media such as optical fiber,
fundamentally limits the product RxL,
where R is the rate and L is the usable
length of the fiber
Term generally refers to how a signal
spreads over space and time

Categories of Noise
Thermal Noise
Intermodulation noise
Crosstalk
Impulse Noise

Thermal Noise
Thermal noise due to agitation of electrons
Present in all electronic devices and
transmission media
Cannot be eliminated
Function of temperature
Particularly significant for satellite
communication

Thermal Noise
Amount of thermal noise to be found in a
bandwidth of 1Hz in any device or
conductor is:
• N0 = noise power density in watts per 1 Hz of
bandwidth
• k = Boltzmann's constant = 1.3803 x 10-23
J/K
• T = temperature, in kelvins (absolute temperature)
( )
W/Hz
k
0 T
N =

Thermal Noise
 Noise is assumed to be independent of frequency
 Thermal noise present in a bandwidth of B Hertz
(in watts):
or, in decibel-watts
TB
N k
=
B
T
N log
10
log
10
k
log
10 +
+
=
B
T log
10
log
10
dBW
6
.
228 +
+
−
=

Other Kinds of Noise
 Intermodulation noise – occurs if signals with
different frequencies share the same medium
o Interference caused by a signal produced at a
frequency that is the sum or difference of original
frequencies
 Crosstalk – unwanted coupling between signal
paths
 Impulse noise – irregular pulses or noise
spikes
o Short duration and of relatively high amplitude
o Caused by external electromagnetic disturbances, or
faults and flaws in the communications system
o Primary source of error for digital data transmission

Expression Eb/N0
 Ratio of signal energy per bit to noise power
density per Hertz
 The bit error rate for digital data is a function of
Eb/N0
o Given a value for Eb/N0 to achieve a desired error rate,
parameters of this formula can be selected
o As bit rate R increases, transmitted signal power must
increase to maintain required Eb/N0
TR
S
N
R
S
N
Eb
k
/
0
0
=
=

Other Impairments
Atmospheric absorption – water vapor and
oxygen contribute to attenuation
Multipath – obstacles reflect signals so that
multiple copies with varying delays are
received
Refraction – bending of radio waves as
they propagate through the atmosphere

Fading
Variation over time or distance of received
signal power caused by changes in the
transmission medium or path(s)
In a fixed environment:
o Changes in atmospheric conditions
In a mobile environment:
o Multipath propagation

Multipath Propagation
 Reflection - occurs when signal encounters a
surface that is large relative to the wavelength of
the signal
 Diffraction - occurs at the edge of an
impenetrable body that is large compared to
wavelength of radio wave
 Scattering – occurs when incoming signal hits an
object whose size is in the order of the
wavelength of the signal or less

AntennasPropagatiooooooooooooooooooooooooooooon.ppt

Effects of Multipath Propagation
Multiple copies of a signal may arrive at
different phases
o If phases add destructively, the signal level
relative to noise declines, making detection
more difficult
Intersymbol interference (ISI)
o One or more delayed copies of a pulse may
arrive at the same time as the primary pulse
for a subsequent bit

Types of Fading
 Fast fading
o Changes in signal strength in a short time period
 Slow fading
o Changes in signal strength in a short time period
 Flat fading
o Fluctuations proportionally equal over all frequency components
 Selective fading
o Different fluctuations for different frequencies
 Rayleigh fading
o Multiple indirect paths, but no dominant path such as LOS path
o Worst-case scenario
 Rician fading
o Multiple paths, but LOS path dominant
o Parametrized by K, ratio of power on dominant path to that on
other paths

Error Compensation Mechanisms
Forward error correction
Adaptive equalization
Diversity techniques

Forward Error Correction
 Transmitter adds error-correcting code to data
block
o Code is a function of the data bits
 Receiver calculates error-correcting code from
incoming data bits
o If calculated code matches incoming code, no error
occurred
o If error-correcting codes don’t match, receiver attempts
to determine bits in error and correct

Adaptive Equalization
 Can be applied to transmissions that carry analog
or digital information
o Analog voice or video
o Digital data, digitized voice or video
 Used to combat intersymbol interference
 Involves gathering dispersed symbol energy back
into its original time interval
 Techniques
o Lumped analog circuits
o Sophisticated digital signal processing algorithms

Diversity Techniques
 Space diversity:
o Use multiple nearby antennas and combine received
signals to obtain the desired signal
o Use collocated multiple directional antennas
 Frequency diversity:
o Spreading out signal over a larger frequency bandwidth
o Spread spectrum
 Time diversity:
o Noise often occurs in bursts
o Spreading the data out over time spreads the errors and
hence allows FEC techniques to work well
o TDM
o Interleaving

AntennasPropagatiooooooooooooooooooooooooooooon.ppt

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