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Lecture 4: Propagation Models, Antennas and Link
BudgetAnders Västberg
08-790 44 55
Digital Communication System
Source of Information
SourceEncoder
Modulator RF-Stage
Channel
RF-StageInformation
SinkSource
DecoderDemodulator
ChannelEncoder
DigitalModulator
ChannelDecoder
DigitalDemodulator
[Slimane]
Propagation between two antennas (not to scale)
No Ground Wave for Frequencies > ~2 MHzNo Ionospheric Wave for Frequencies > ~30 Mhz
Direct Wave
Ground ReflectedWave
Ground Wave
Sky Wave
The Radio Link
• Design considerations– The distance over which the system meets
the performance objectives– The capacity of the link.
• Performance determined by– Frequency– Transmitted Power– Antennas– Technology used
[Black et. al]
Performance of Radio Systems
• Signal attenuation– path loss– multipath fading
• Additive noise– Thermal noise– Atmospheric noise– Cosmic Noise– Man-made noise
Noise
• Thermal noise – White Noise• Spectral density: (W/Hz)
k Boltzmann’s constant (1.38 10-23 J/K)T Absolute temperature (in Kelvins)
• Noise power (in W)
B Bandwidth (Hz)
TBkN
TkN 0
Link Budget
𝑃𝑟=𝑃 𝑡 ∙𝐺𝑡 ∙𝐺𝑟
𝐿𝑏
PtG
tP
rL
b
r
Gr
SNR=𝑃𝑟
𝑁=𝑃𝑡 ∙𝐺𝑡 ∙𝐺𝑟
𝑁 𝐿𝑏
=𝑃 𝑡 ∙𝐺𝑡 ∙𝐺𝑟
𝑘𝑇0𝐵𝐿𝑏
SNR𝑑𝐵=(𝑃 ¿¿𝑡)𝑑𝐵+(𝐺¿¿𝑡)𝑑𝐵−(𝐿¿¿𝑏)𝑑𝐵+(𝐺¿¿𝑟 )𝑑𝐵−(𝑘𝑇 ¿¿ 0𝐵)𝑑𝐵¿¿¿¿¿
𝑃 𝐸𝐼𝑅𝑃=𝑃𝑡 ∙𝐺𝑡
EIRP=Effective Isotropic Radiated Power
Propagations Models
𝐿𝐹𝑆=( 4 𝜋𝑟𝜆 )2
=( 4𝜋 𝑓 𝑟𝑐 )
2
Free Space Model
𝐿𝑃𝐸=𝑟4
(h1h2 )2Plane Earth Model
𝐿=𝑟𝑛
𝑘Power Law Model
Dipole antennaOmnidirectional
L= /2l
I I
• Half-wave dipole– Gain 1,64 = 2.15 dBi– Linear Polarisation
• Quarter-wave dipole– Conducting plane below a
single quarter wave antenna. Acts like a half-wave dipole
L=l/4
I
Yagi-antennaDirectional
http://www.urel.feec.vutbr.cz/~raida/multimedia_en/chapter-4/4_3A.html
3-30 element and a gain of 8-20 dBi
Corner Reflectors
• Multiple images results in increased gain
• Example:G=12 dBi
/2l
Driven Element
Images
Loop-antenna - Directional
http://www.ycars.org/EFRA/Module%20C/AntLoop.htm
• Linear Polarisation
• Gain 1,76 dBi
Helical antennaDirectional
• Normal mode• Axial mode
http://hastingswireless.homeip.net/index.php?page=antennas&type=helical
Propagation in the Atmosphere
• The atmosphere around the earth contains a lot of gases (1044 molecules)
• It is most dense at the earth surface (90% of molecules below a height of 20 km).
• It gets thinner as we reach higher and higher attitudes.
• The refractive index of the air in the atmosphere changes with the Height
• This affects the propagation of radio waves.• The straight line propagation assumption may
not be valid especially for long distances.
[Slimane]