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8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
CS 414
Wireless Propagation Basics
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CS 414 Indian Institute of Technology, Bombay
Last Lecture
Radio waves 3KHz to 300 Ghz
Analog and Digita data and signals
Bandwidth and Data Rate
8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
Last Lecture
db relative measure
db = 10 log10
(ratio)
if Ps = 10 mW and Pr = 10mW ~ 0 db
1 mW ~ -10 db
100 mW ~ 10 db 1000 mW ~ 20 db
dbm, dbv, dbi, dbW ...
absolute measure
8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
dbW, dbm, dbi, dbv ...
db = relative maginutes Fix reference for to initial signal for absolute
compariton
dbm = 10 log (PowermW
/ 1mW)
1 mW = 0 dbm
10 mW = 10 dbm
30 dbm = ?
If P1 P2 = 10 dbm then, absolute differenceis ?
1 dbW = ? dbm
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CS 414 Indian Institute of Technology, Bombay
Antennas
Essential wireless propogation component Entry and end-points of RF signals
Two funtions
Transmission Converts electric energy to electro-magnetic
Receiver
Converts received electro-magnetic energy to
electric signal Passive element
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CS 414 Indian Institute of Technology, Bombay
Antenna Types
Omni-directional radiation in all directions
Directional
Focuses (more) power in certain direction
Does not amplify
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CS 414 Indian Institute of Technology, Bombay
Types of Antennas
/4
Quarter-wave Antenna
/4
/2Half-wave Dipole
www.cellamericas.com
Parabolic Antenna
8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
Antenna Gain
Isotropic Antenna Idealized omni-directional antenna
Tranmits power in all directions uniformly
Antenna Gain (G)
ratio of transmit/receive power in a particulardirection w.r.t to an isotropic antenna
G = Pdirection
/Pisotropic
Measure of reception/tranmission strength ofantenna
Transmit Gain = Receive Gain
Typical units: dBi (dB gain w.r.t to isotropic)
8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
Antenna Gain
Isotropic G = 1 in all directions
Non-uniform/Directional
Ga
= ?
Gb = ?
Gc
= ?
A
B
C
8/3/2019 Wireless Prop
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CS 414 Indian Institute of Technology, Bombay
Antenna Parameters
Radiation Pattern Spread of transmitter
power
(Half-power) Beam width
Angle between half power point (direction) andthe point (direction) of maximum power
Assumption: Reception beyond beam width ispoor and unreliable
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CS 414 Indian Institute of Technology, Bombay
Antenna Parameters
Antenna Polarization Orientation/plane of the electric field (E-plane)
w.r.t earth's surface
Horizontally polarizedVertically polarized
image source: wikipedia
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CS 414 Indian Institute of Technology, Bombay
RF Propagation
Questions: Relation between RF propogation & distance
different environments
quantification metrics
Goals: Provide connectivity, Estimate linkquality (Is this link good?)
Solution Design:
Antenna placement
Link quality mapping and monitoring
Tranmist power, antenna height
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CS 414 Indian Institute of Technology, Bombay
Propagation Phenomena
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CS 414 Indian Institute of Technology, Bombay
Path Loss Estimation
Isotropic Antenna Free space loss
PtPt
d
Pdensity=Pt
4d2
Pr=PdensityEffective Antenna Area
Aeff=2
4
FreeSpacePathLoss=Pr
Pt= 4d
2
Pr=Pt 4d 2
Aeff
= product of physical area (mW/m2)
and conversion efficiency
Prdbm=Ptdbm[20logf20log d32.5 ] d in Km and f in MHz
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CS 414 Indian Institute of Technology, Bombay
Free Space Loss
With antenna gains Gt and Gr
Pr=PtGtGr 4d 2
=PtGtGr c4df2
EIRP regulations to control radiated power
Prdbm=PtdbmGt dbGrdb[20logf20logd 32.5 ]
Effective isotropic radiated power (EIRP)
Free Space Loss
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CS 414 Indian Institute of Technology, Bombay
Path Loss Example
Pt = 50 mW, f = 2.4 Ghz, d = 2Km, Pr = ?
Gt = 24 dBi, Gr = 24 dBi, Pr = ?
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CS 414 Indian Institute of Technology, Bombay
Next Class
Loss proportional to d2 ... in reality ?
ReadingThe Mistaken axioms of wireless-network research, D. Kotz,C. Newport, C. Elliotthttp://pdos.csail.mit.edu/decouto/papers/kotz03.pdf
Most research on ad-hoc wireless networks makessimplifyingassumptions about radio propagation. The Flat Earthmodel of the world is surprisingly popular: all radioshave circularrange, have perfect coverage in thatrange, and travel on a two-dimensional plane.
...We then present a set of 802.11 measurements that clearlydemonstrate that these axioms are contrary to fact.
http://pdos.csail.mit.edu/decouto/papers/kotz03.pdfhttp://pdos.csail.mit.edu/decouto/papers/kotz03.pdf