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Signal Propagation Basics
EECS 4215
13 April 2024
2
Signal Propagation Ranges
• Transmission range
– communication possible
– low error rate
• Detection range
– detection of the signal
possible
– communication
not possible
• Interference range
– signals may not be
detected
– signals add to the
background noise
distance
sender
transmission
detection
interference
Note: These are not perfect
spheres in real life!
3
Signal Propagation
• Propagation in free space is always like light (straight line).
• Receiving power proportional to 1/d² in vacuum – much more in real
environments (d = distance between sender and receiver)
• Receiving power additionally influenced by
– fading (frequency dependent)
– Shadowing (blocking)
– reflection at large obstacles
– refraction depending on the density of a medium
– scattering at small obstacles
– diffraction at edges
reflection scattering diffraction
shadowing refraction
4
Propagation Modes
• Ground-wave (< 2MHz) propagation
• Sky-wave (2 – 30 MHz) propagation
• Line-of-sight (> 30 MHz) propagation
5
Ground Wave Propagation
6
Ground Wave Propagation
• Follows the contour of the earth
• Can propagate considerable distances
• Frequencies up to 2 MHz
• Example
– AM radio
– submarine communication (long waves)
7
Sky Wave Propagation
8
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
the earth surface
• Reflection effect caused by refraction
• Examples
– amateur radio
– International broadcasts
9
Line-of-Sight Propagation
10
Line-of-Sight Propagation
• Transmitting and receiving antennas must be within
line of sight
– Satellite communication – signal above 30 MHz
not reflected by ionosphere
– Ground communication – antennas within effective
line of sight due to refraction
• Refraction – bending of microwaves by the
atmosphere
– Velocity of an electromagnetic wave is a function
of the density of the medium
– When wave changes medium, speed changes
– Wave bends at the boundary between mediums
• Mobile phone systems, satellite systems, cordless
phones, etc.
11
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) (altitude relative to a
receiver at the sea level)
• K = adjustment factor to account for
refraction caused by atmospherics layers;
rule of thumb K = 4/3
h
d 57
.
3

h
d 
 57
.
3
12
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 


13
LOS Wireless Transmission
Impairments
• Attenuation and attenuation distortion
• Free space loss
• Atmospheric absorption
• Multipath (diffraction, reflection,
refraction…)
• Noise
• Thermal noise
14
Attenuation
• Strength of signal falls off with distance over
transmission medium
• Attenuation factors for unguided media:
– Received signal must have sufficient strength so
that circuitry in the receiver can interpret the signal
– Signal must maintain a level sufficiently higher
than noise to be received without error
– Attenuation is greater at higher frequencies,
causing distortion (attenuation distortion)
15
Free Space Path Loss
• Free space path 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 ´ 10 8 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 




16
Free Space Path Loss in dB
• Free space path loss equation can be
recast (decibel version):









d
P
P
L
r
t
dB
4
log
20
log
10
    dB
98
.
21
log
20
log
20 


 d

    dB
56
.
147
log
20
log
20
4
log
20 








 d
f
c
fd

Multipath Propagation
18
Multi-path Propagation
• Signal can take many different paths between sender
and receiver due to reflection, scattering, diffraction
• Time dispersion: signal is dispersed over time
– interference with “neighbor” symbols, Inter Symbol
Interference (ISI)
• The signal reaches a receiver directly and phase
shifted
– distorted signal depending on the phases of the different
parts
signal at sender
signal at receiver
LOS pulses
multipath
pulses
19
Atmospheric Absorption
• Water vapor and oxygen contribute most
• Water vapor: peak attenuation near 22GHz,
low below 15Ghz
• Oxygen: absorption peak near 60GHz, lower
below 30 GHz.
• Rain and fog may scatter (thus attenuate)
radio waves.
• Low frequency band usage helps.
20
Effects of Mobility
• Channel characteristics change over time and
location
– signal paths change
– different delay variations of different signal parts
– different phases of signal parts
–  quick changes in the power received (short term
fading)
• Additional changes in
– distance to sender
– obstacles further away
–  slow changes in the average
power received (long term fading)
short term fading
long term
fading
t
power
21
Fading Channels
• Fading: Time variation of received
signal power
• Mobility makes the problem of modeling
fading difficult
• Multipath propagation is a key reason
• Most challenging technical problem for
mobile communications
22
Types of Fading
• Short term (fast) fading
• Long term (slow) fading
• Flat fading – across all frequencies
• Selective fading – only in some frequencies
• Rayleigh fading – no LOS path, many other
paths
• Rician fading – LOS path plus many other
paths
23
Dealing with Fading Channels
• Error correction
• Adaptive equalization
– attempts to increase signal power as needed
– can be done with analog circuits or DSP
(digital signal processor)
Reading
• Mobile Communications (Jochen
Schiller), section 2.4
• Stallings, chapter 3
24

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fadingvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvvv

  • 1. Signal Propagation Basics EECS 4215 13 April 2024
  • 2. 2 Signal Propagation Ranges • Transmission range – communication possible – low error rate • Detection range – detection of the signal possible – communication not possible • Interference range – signals may not be detected – signals add to the background noise distance sender transmission detection interference Note: These are not perfect spheres in real life!
  • 3. 3 Signal Propagation • Propagation in free space is always like light (straight line). • Receiving power proportional to 1/d² in vacuum – much more in real environments (d = distance between sender and receiver) • Receiving power additionally influenced by – fading (frequency dependent) – Shadowing (blocking) – reflection at large obstacles – refraction depending on the density of a medium – scattering at small obstacles – diffraction at edges reflection scattering diffraction shadowing refraction
  • 4. 4 Propagation Modes • Ground-wave (< 2MHz) propagation • Sky-wave (2 – 30 MHz) propagation • Line-of-sight (> 30 MHz) propagation
  • 6. 6 Ground Wave Propagation • Follows the contour of the earth • Can propagate considerable distances • Frequencies up to 2 MHz • Example – AM radio – submarine communication (long waves)
  • 8. 8 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 the earth surface • Reflection effect caused by refraction • Examples – amateur radio – International broadcasts
  • 10. 10 Line-of-Sight Propagation • Transmitting and receiving antennas must be within line of sight – Satellite communication – signal above 30 MHz not reflected by ionosphere – Ground communication – antennas within effective line of sight due to refraction • Refraction – bending of microwaves by the atmosphere – Velocity of an electromagnetic wave is a function of the density of the medium – When wave changes medium, speed changes – Wave bends at the boundary between mediums • Mobile phone systems, satellite systems, cordless phones, etc.
  • 11. 11 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) (altitude relative to a receiver at the sea level) • K = adjustment factor to account for refraction caused by atmospherics layers; rule of thumb K = 4/3 h d 57 . 3  h d   57 . 3
  • 12. 12 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   
  • 13. 13 LOS Wireless Transmission Impairments • Attenuation and attenuation distortion • Free space loss • Atmospheric absorption • Multipath (diffraction, reflection, refraction…) • Noise • Thermal noise
  • 14. 14 Attenuation • Strength of signal falls off with distance over transmission medium • Attenuation factors for unguided media: – Received signal must have sufficient strength so that circuitry in the receiver can interpret the signal – Signal must maintain a level sufficiently higher than noise to be received without error – Attenuation is greater at higher frequencies, causing distortion (attenuation distortion)
  • 15. 15 Free Space Path Loss • Free space path 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 ´ 10 8 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     
  • 16. 16 Free Space Path Loss in dB • Free space path loss equation can be recast (decibel version):          d P P L r t dB 4 log 20 log 10     dB 98 . 21 log 20 log 20     d      dB 56 . 147 log 20 log 20 4 log 20           d f c fd 
  • 18. 18 Multi-path Propagation • Signal can take many different paths between sender and receiver due to reflection, scattering, diffraction • Time dispersion: signal is dispersed over time – interference with “neighbor” symbols, Inter Symbol Interference (ISI) • The signal reaches a receiver directly and phase shifted – distorted signal depending on the phases of the different parts signal at sender signal at receiver LOS pulses multipath pulses
  • 19. 19 Atmospheric Absorption • Water vapor and oxygen contribute most • Water vapor: peak attenuation near 22GHz, low below 15Ghz • Oxygen: absorption peak near 60GHz, lower below 30 GHz. • Rain and fog may scatter (thus attenuate) radio waves. • Low frequency band usage helps.
  • 20. 20 Effects of Mobility • Channel characteristics change over time and location – signal paths change – different delay variations of different signal parts – different phases of signal parts –  quick changes in the power received (short term fading) • Additional changes in – distance to sender – obstacles further away –  slow changes in the average power received (long term fading) short term fading long term fading t power
  • 21. 21 Fading Channels • Fading: Time variation of received signal power • Mobility makes the problem of modeling fading difficult • Multipath propagation is a key reason • Most challenging technical problem for mobile communications
  • 22. 22 Types of Fading • Short term (fast) fading • Long term (slow) fading • Flat fading – across all frequencies • Selective fading – only in some frequencies • Rayleigh fading – no LOS path, many other paths • Rician fading – LOS path plus many other paths
  • 23. 23 Dealing with Fading Channels • Error correction • Adaptive equalization – attempts to increase signal power as needed – can be done with analog circuits or DSP (digital signal processor)
  • 24. Reading • Mobile Communications (Jochen Schiller), section 2.4 • Stallings, chapter 3 24

Editor's Notes

  1. Universität Karlsruhe Institut für Telematik
  2. Universität Karlsruhe Institut für Telematik
  3. Universität Karlsruhe Institut für Telematik
  4. Universität Karlsruhe Institut für Telematik