Path Loss and Shadowing
We want to understand the following effect(s):
Wireless Communications - Path Loss and Shadowing
Image source: Theodore S. Rappaport, Wireless Communications, 2nd ed., Prentice Hall, 2002
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LOG-DISTANCE PATH-LOSS
MODEL
Wireless Communications - Path Loss and Shadowing
Motivation: model extension of what we derived so far
We assume that transmitter and receiver are stationary
Wave propagation in free space is basically straight (like light)
According to Friis equation: receive power decreases in a vacuum with 1 / d² (d = distance between transmitter and receiver)
If we assume obstacles in the room, then the reception power will also be influenced by
Shadowing by obstacles
Reflection on large surfaces
Refraction depending on the density of a medium
Scattering on small obstacles
Diffraction on sharp edges
Why is that a problem? We'll take a look at next:
all mentioned effects except shadowing (next slides)
and then we add shadowing (the slides afterwards)
Reflection Scattering Diffraction
Shadowing Refraction
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The multipath propagation problem
Line-of- sight path
Non-line-of-sight path
example shows reflection
(the same applies for all other effects
Remark: Multipath propagation can also be an advantage
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blocked LOS-Pfad sender
receiver
Phase reversed Increase distance
Two‐Ray Ground Reflection Model
frey
Sender Receiver
-1 -0.5 0 0.5 1
0 1 2 3 4 5 6
-1 -0.5
0 0.5
1
0 1
2 3
4 5
6 -1
-0.5 0 0.5 1
0 1
2 3
4 5
6 -1 -0.5 0 0.5 1
0 1 2 3 4 5 6
-1 -0.5 0 0.5 1
0 1 2 3 4 5 6
-1 -0.5 0 0.5 1
0 1 2 3 4 5 6
LOS signal
Reflected signal
Complete signal
Model parameters discussed
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rappaport02wireless: 4.9.1
Reference distance d0
• has to be in the far field
• should be less than “typical distances” of the considered system
• commonly used values
• 1km for large coverage cellular system
• much smaller (such as 100m or 1m) for microcellular systems Distance dbetween transmitter and receiver
Path loss PL(d0) at reference distance d0
• computed either from free space propagation model or
• determined empirically
Path loss exponent n(often also noted as α).
Typical path loss exponents obtained in various mobile radio environments
Image source: Theodore S. Rappaport, Wireless Communications, 2nd ed., Prentice Hall, 2002, page 139
Empirical path‐loss models
Okumura‐Hata Path‐Loss Model
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Original model after Okumura revised by Hata. Path‐loss model for cellular networks based on empirical data on measurements in Tokyo.
For urban areas :
L
dB,urban(d) = 69.55 + 26.16 log
10f
c– 13.82 log
10h
t– a(h
r) + (44.9 – 6.55 log h
t) log
10d
f
c= carrier frequency in MHz (100 to 1500 MHz)
h
t= height of the transmitting antenna (base station) in m (30 to 200 m) h
r= height of the receiving antenna (mobile unit) in m (1 to 10 m)
d = distance between the antennas in km (1 to 20 km)
a(h
r) = correction factor for mobile antenna height based on the size of the
coverage area
Okumura‐Hata Path‐Loss Model
The correction factor a(h r ) for small to medium sized cities:
a(h r ) = (1.1 log 10 f c – 0.7) h r – (1.56 log 10 f c – 0.8) dB
The correction factor a(h r ) for larger cities:
a(h r ) = 8.29 [log 10 (1.54 h r )] 2 – 1.1 dB for f c <= 300 MHz
a(h r ) = 3.2 [log 10 (11.75 h r )] 2 – 4.97 dB for f c > 300 MHz
Okumura‐Hata Path‐Loss Model
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For suburban areas:
L dB,suburban (d) = L dB,urban (d) – 2 [log 10 (f c / 28)] 2 – 5.4 For rural areas:
L dB,rural (d) = L dB,urban (d) – 4.78 (log 10 f c ) 2 – 18.733 (log 10 f c ) – K
where K ranges from 35.94 (countryside) to 40.94 (desert)
Log‐normal shadowing
Empirical Evidence (Example)
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saunders07wireless: 9.2
Driving around a base station at a constant distance.
Depicted is the local mean after subtracting the median (50%) level in decibles.
The typical shape of the probability density function of shadowing compared to the PDF of the log-normal distribution.
Image source: Saunders, S., & Aragón-Zavala, A. (2007). Antennas and Propagation for Wireless Communication Systems (2nd Edition). Wiley (Fig. 9.2 and Fig. 9.3)
Summarized
schwarz04wireless: 2.2 “shadow fading”
P
rdBm
d [m]
average received power due to path loss
• described by log-distance path loss model
• just depends on transmitter receiver separation
• called area mean
average received power when taking shadow fading into account
• called local mean
• depends on actual transmitter and receiver position
• however does not change rapidly when node positions are changed slightly
• variation typically in the order of many wavelengths
• decribed by log-normal shadowing model for an arbitrary transmitter receiver pair
Empirical Data for the Log-Normal-Shadowing Model
Determining PL(d 0 ), n and from empirical data
Choose a suitable d
0 in the far field
Transmitter-receiver distance usually > = d0
Determine PL(d
0)
e.g. theoretically according to Friis equation or
Empirical by means of many independent
measurements at distance d0
Determine independent
empirical measurement data for growing distance
For empirical measurement data, determine the best n and (e.g., linear
regression method (i.e., mean squared deviation of measurement data and
model data is minimal) for n, and then sample variance
PL of area mean is linear here since distance is plotted logarithmically
Simplified example (see Rappaport p. 143)
Distance to Sender Received power 100 m (reference distance) 0 dBm
200 m -20 dBm
1000 m -35 dBm
3000 m -70 dBm
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Example: typical parameters for lognormal shadowing model for near ground communication at 800-1000 MHz
Lognormal shadowing model is characterized by
,
2, PL(1m) (path loss at reference distance d
0)
FURTHER DISCUSSIONS
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Signal propagation areas
distance sender
communication
detection interference
Communication region
communication possible
low error rate Detection region
signal detection possible
no communication possible Interference region
signal can not be detected
signal contributes to
the background noise
Wireless Communications - Path Loss and Shadowing
Side note: ray tracing as an alternative to modeling signal propagation
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Recap
So far, we have only considered the problem of attenuation and overlapping waves of one symbol
Multipath propagation also leads to another problem
Inter symbol interference (ISI): Interference with neighboring symbols
signal at sender
signal at receiver LOS pulses multipath
pulses
Recap
Another fact that complicates wireless communication:
Signals often consist of many sinusoids of different frequencies (see discussion on Fourier transformation and the subject of modulation) The treated effects are usually also frequency selective
This means that the effects have different effects on the frequency spectrum of the signal; which additionally distorts the signal
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