giuseppe bianchi wireless cellular networks (basics) part 1 – propagation for dummies
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Giuseppe Bianchi
Wireless Cellular NetworksWireless Cellular Networks(basics) (basics)
Part 1 – Propagation for dummies
Giuseppe Bianchi
The Radio SpectrumThe Radio Spectrum
Radio waveWavelength = c/f Speed of light c=3x108 m/sFrequency: f
ftAts 2cos)(
f
f = 900 MHz = 33 cm
[V|U|S|E]HF = [Very|Ultra|Super|Extra] High Frequency
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The radio spectrumThe radio spectrum
ELF <3 KHz Remote control, Voice, analog phone
VLF 3-30 KHz Submarine, long-range
LF 30-300 KHz Long-range, marine beacon
MF 300 KHz –3 MHz AM radio, marine radio
HF 3-30 MHz Amateur radio, military, long-distance aircraft/ships
VHF 30-300 MHZ TV VHF, FM radio, AM x aircraft commun.
UHF 300 MHz - 3 GHz Cellular, TV UHF, radar
SHF 3-30 GHz Satellite, radar, terrestrial wireless links, WLL
EHF 30-300 GHz Experimental, WLL
IR 300 GHz – 400 THz
LAN infrared, consumer electronics
Light 400-900 THz Optical communications
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Spectrum AllocationSpectrum Allocation
Higher frequencies: more bandwidth less crowded spectrumbut greater attenuation through
wallsCurrent target: 60 GHz ultra high
throughput WLANs/WPANs Lower frequencies
bandwidth limitedlonger antennas requiredgreater antenna separation
requiredseveral sources of man-made
noise
Cellular Systems400-2200 MHz range (VHF-UHF)Simple, small antenna (few cm)With less than 1W transmit power,
can cover several floors within a building or several miles outside
wireless data systems2.4, 5 GHz zones (ISN band)Main interference from microwave
ovenslimitations due to absorption by
water and oxygen - weather dependent fading, signal loss due to by heavy rainfall etc.
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Antennas (ideal, free space)Antennas (ideal, free space)
Isotropic (omnidirectional) tx antenna in free spaceTransmitted power: Pt
Power attenuation Pa at distance d:down with sphere superficies
Power received by isotropic rx antennaPlanar waveAe = Effective Area
In two-way communication Same antenna may be used for tx and rx
24)(
d
PdP t
a
4
)()(2
e
ear
A
AdPdP
r
Idealization: Isotropic antennas cannot be practically built
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Antennas (real, free space)Antennas (real, free space)
Non isotropic tx antennaAntenna gain Gt
Gain = Power output, in a particular direction, compared to that produced in any direction by a perfect omni-directional (isotropic) antenna
Non isotropic rx antennaAntenna gain Gr
r
24)(
d
PGdP tt
a
44)()(
2
2 rtt
erar Gd
GPAGdPdP
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Friis Free-Space ModelFriis Free-Space Modelsummarizing all previous considerationssummarizing all previous considerations
Pt = transmitter power (W or mW)
Gt = transmitter antenna gain Gr = transmitter antenna gain
(dimensionless) = c/f = RF wavelength (m)
c = speed of light (3x108 m/s) f = RF frequency (Hz)
2
22
2
4)4()(
fd
c
L
GGP
Ld
GGPdP rt
trtt
r
0d
Pt Gt = Equivalent Isotropic Radiated Power (EIRP)
L = other system losses (hardware) L >=1 (dimensionless)
d = distance between transmitter and receiver (m)
2)( ddPrSummary: in free space,
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Power units – dB and dBmPower units – dB and dBm
Decibel (dB): log unit of intensity; indicates power lost or gained between two signals
Named after Alexander Graham Bell
dBm: absolute value (reference = 1 mW)Versus dB = relative value = ratio Power in dBm = 10 log(power/1mW)
21 /log10 PPPA = 1 WattPB = 50 milliWatt
PA = 13 dB greater than PB
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Decibels - dBmDecibels - dBm Examples
10 mW = 10 log10(0.01/0.001) = 10 dBm10 W = 10 log10(0.00001/0.001) = -20 dBm26 dBm = ___ 2W= ___ dBm?S/N ratio = -3dB S = ___ X N?
Transmit powerMeasured in dBm
Es. 33 dBm Receive Power
Measured in dBmEs. –10 dBm
Path LossReceive power / transmit powerMeasured in dBLoss (dB) = transmit (dBm) – receive (dBm)
Es. 43 dB = attenuation by factor 20.000
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Friis ExampleFriis Examplenormalized
frequency [MHz] 900 900000000speed of light [Km/s] 300000 300000000lambda (m) 0,333333333gain Tx 1Gain Rx 1Loss 1Ptx [W] 5distance (Km) Prx W Prx dBm
200 8,80E-08 -40,56400 2,20E-08 -46,58600 9,77E-09 -50,10800 5,50E-09 -52,60
1000 3,52E-09 -54,541200 2,44E-09 -56,121400 1,79E-09 -57,461600 1,37E-09 -58,621800 1,09E-09 -59,642000 8,80E-10 -60,562200 7,27E-10 -61,392400 6,11E-10 -62,142600 5,20E-10 -62,842800 4,49E-10 -63,483000 3,91E-10 -64,083200 3,44E-10 -64,643400 3,04E-10 -65,173600 2,71E-10 -65,663800 2,44E-10 -66,134000 2,20E-10 -66,584200 1,99E-10 -67,004400 1,82E-10 -67,414600 1,66E-10 -67,794800 1,53E-10 -68,165000 1,41E-10 -68,52
-70,00
-60,00
-50,00
-40,00
-30,00
0 1000 2000 3000 4000 5000
distance (m)
receiv
ed
po
wer
(dB
m)
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Reference distanceReference distance
If known received power at a reference distance do from tx can calculate Pr(d) for any d
Must be smaller than typical distances encountered in wireless communication systems;
Must fall in the far-field region of the antennaSo that losses beyond this point are purely distance-dependent
Typical d0 selection: 100-1000m
2
)()(
d
ddPdP o
orr
d
ddBmdP
d
ddPdBmdP o
oro
orr 101010 log20))((log20)(log10)()(
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More realistic propagation More realistic propagation modelsmodels
Inverse square power lawWay too optimistic (ideal case); valid only for very short
distancesReal world: -th power law
with ranging up to as much as If tough environment (e.g., lots of foliage),
typical values: for small distances (20 dB/decade)todB/decadefor mobile telephone distances
higher in cities and urban areas; lower in suburban or rural areas.
ddPr )(
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Formulae with ref. distanceFormulae with ref. distance
d
ddPdBmdP o
orr 1010 log10)(log10)()( d_ref 1 KmP_ref -51,5266 dBm (Ptx=10W; 900 MHz; 1000m)
distance prx (eta=2)prx (eta=3,5) prx (eta=4)1 -51,5266 -51,5266206 -51,5266
1,2 -53,1102 -54,2979642 -54,69391,4 -54,4492 -56,6411018 -57,37171,6 -55,609 -58,67082 -59,69141,8 -56,6321 -60,4611582 -61,7375
2 -57,5472 -62,0626704 -63,56782,2 -58,3751 -63,5114144 -65,22352,4 -59,1308 -64,834014 -66,73512,6 -59,8261 -66,0506877 -68,12562,8 -60,4698 -67,1771517 -69,4129
3 -61,069 -68,2258645 -70,61153,2 -61,6296 -69,2068698 -71,73263,4 -62,1562 -70,1283827 -72,78583,6 -62,6527 -70,9972081 -73,77873,8 -63,1223 -71,8190464 -74,718
4 -63,5678 -72,5987203 -75,6094,2 -63,9916 -73,3403457 -76,45664,4 -64,3957 -74,0474642 -77,26474,6 -64,7818 -74,7231447 -78,03694,8 -65,1514 -75,3700639 -78,7763
5 -65,506 -75,9905707 -79,4854
-85
-80
-75
-70
-65
-60
-55
-50
1 2 3 4 5distance (Km)
rec
eiv
ed
po
we
r (d
Bm
)
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Two-Ray Ground Two-Ray Ground Propagation ModelPropagation Model
Theoretical foundation for =4Two-ray model assumes one direct LOS path and one
reflection path reach receiver with significant powerEasy to solve
ht
hr
Line-Of-Sight ray
reflected ray
Transmit and receive antennas at different height (in general)
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Two-ray model – geometryTwo-ray model – geometry
hr
ht
( )
ddirect
dreflect
rt hhd ,
22/1222
22/1222
2
111
2
111
d
hhd
d
hhdhhdd
d
hhd
d
hhdhhdd
rtrtrtreflect
rtrtrtdirect
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Two ray model – path Two ray model – path analysisanalysis
EM waves travel for different distanceSum up with different phase!
A = attenuation along direct pathB = attenuation along reflected path (reflection not ideal, in general)
d
hh
d
hhd
d
hhddd rtrtrt
directreflect 22
11
2
11
22
c
dtfB
c
dtfA
reflect
direct
2cosrayreflect
2cosraydirect
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Two ray model – field Two ray model – field strengthstrengthPhase difference
Received field strength
Let Edirect be the field strength given by direct ray.Then
Assume ideal reflection (=-1)
d
hhd
c
df rt
42
2
jdirect eEE 1
2sin2
2
cos12
sincos2cos1
sincos112/122
directdirect
direct
directj
direct
EE
EE
jEeEE
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Two ray model – power Two ray model – power computationcomputation
Received power
Proportional to |E|2
d
hh
dL
GGPdP rtrtt
r
2
sin44
)( 22
2/sin4 2 directr EP
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Two ray model - conclusionTwo ray model - conclusion
Typical values:ht ~ few tens of m
hr ~ couple of meters ~ few tens of cmd ~ hundred meters – few km
22 22
sin2
d
hh
d
hhsmall
d
hh rtrtrt
4
22222
44
)(d
hh
L
GGP
d
hh
dL
GGPdP rtrttrtrtt
r
i.e. attenuation follows a 40 dB/decade rule! Versus 20 dB/decade of the free-space model
4)( ddPr
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Propagation impairmentsPropagation impairments
Line of sight
Reflection
Shadowing
BS
MS
Diffraction When the surface
encountered has sharp edges bending the wave
Scattering When the wave encounters
objects smaller than the wavelength (vegetation, clouds, street signs)BS
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Multipath CharacteristicsMultipath Characteristics(not just attenuation)(not just attenuation)
A signal may arrive at a receivermany different timesFrom many different directions
due to vector addition, signal mayReinforceCancel
signal strength differsfrom place to placefrom time to time!
(slow/fast fading)
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Attenuation + fadingAttenuation + fading
Signal power
Distance BS MS (km)
Distance BS MS (m)Slow fading
Fast fading
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Statistical nature of received Statistical nature of received powerpower
Sig
nal str
en
gth
(d
B)
Time (or movement)
Long term fading
Short term fading
Mean value predictedby attenuation model (constant at given d)
Different (statistical) mathematical models for slow and fast fading(details out of the goals of this lecture)
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Cell radiusCell radiusHow do we determine cell radius?
Seems very simple: givenPt = transmitted power (dBm)Pth = threshold power (dBm)
Sensitivity of the receiver, i.e. minimum amount of received power for acceptable performance
Path loss computed asLp = Pt - Pth
Radius computed from Lp
Via -law propagation formulaVia Okumura-Hata formula (or other empirical model)
But…
oop d
dddL 10log10
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Example (part 1)Example (part 1)
Received power at 10 mt: 0.1 WThreshold power: Pth = -50 dBm
= 3.7
mtR
RR
PR
mtPRP
mtP
thdBmrdBmr
dBmr
7801010
37
70
10log50
10log3720
10log10)10()(
20100log10)10(
37
70
1010
10
10
Result: because of statistical power fluctuation (fading) outage probability at cell border will be about 50%!!!
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Fading MarginFading Margin Previous computation does
not account for long-termfadingNeed to keep it in count, as it does not
reduce when the MS makes small moves IDEA: reduce cell radius to account for
a “fading margin” M
Fading Margin definition:M = average received power at cell border
(dBm) – threshold power (dBm)M=0 means that the power received at
cell border is equal to the threshold M=6 (dB) power received at cell
border is 4 x the power threshold
Fading Margin computationThrough appropriate statistical model of
long-term fading (typically lognormal)
thtp PPL
MPPL thtp
Powerat cellborder
Mean pathloss
1% - 2%
M
prob
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Example (part 2)Example (part 2)Received power at 10 mt: 0.1 WThreshold power: Pth = -50 dBm
= 3.7If we use a fading margin M=6
mtRR
MPR
mtPRP thdBmrdBmr
537101065010
log3720
10log10)10()(
37
64
10
10
What is the experienced outage at cell border?If we assume lognormal slow fading, with dB=4 dB…
%68.642
6erfc
2
1
2erfc
2
1
dB
out
MbordercellP
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Empirical attenuation Empirical attenuation modelsmodels
Consider specific scenarios Urban area (large-medium-small city), rural area Models generated by combining most likely ray traces
(LOS, reflected, diffracted, scattered) Based on large amount of empirical measurements
Account for parameters Frequency; antenna heights; distance
Account for correction factors (diffraction due to mountains, lakes, road shapes, hills, etc)
Many models for distance ranges, frequency ranges, indoor vs outdoor Okumura-Hata ; Lee’, others cellular frequencies, large distances > 1km Walfish-Ikegami 800-2000 MHz , microcellular distances (20m – 5 km)
Adopted by European Cooperation in the field of Scientific and Technical (COST) research as reference model for 3G systems
Indoor propagation models
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Example: Okumura-Hata Example: Okumura-Hata modelmodel
Hata (1980): very simple model to fit Okumura results
Provide formulas to evaluate path loss versus distance for various scenariosLarge cities; Small and medium cities; Rural areasLimit: d>=1km
Parameters:f = carrier frequency (MHz)d = distance BS MS (Km)hbs = (effective) heigh of base
station antenna (m)hms = height of mobile antenna (m)
Effective BSAntenna height
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Okumura-Hata: urban areaOkumura-Hata: urban area
msbs
bs
path
hah
dh
fdBL
10
1010
10
log82.13
loglog55.69.44
log16.2655.69)(
a(hms) = correction factor to differentiate large from medium-small cities;
depends on MS antenna height
8.0log56.17.0log1.1:cities med-small
40097.475.11log2.3:cities large
1010
210
fhfha
MHzfhha
msms
msms
Very small correction difference between large and small cities (about 1 dB)
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Okumura-Hata: suburban & Okumura-Hata: suburban & rural areasrural areas
Start from path loss Lp computed for small and medium cities
94.40log33.18log78.4)(:rural
4.528
log2)(:suburban
102
10
2
10
ffLdBL
fLdBL
ppath
ppath
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Okumura-Hata: examplesOkumura-Hata: examples
80
90
100
110
120
130
140
150
0 1 2 3 4 5 6 7 8 9 10
distance (km)
pa
th lo
ss
(d
B)
large cities
small cities
suburbs
rural area
F=900MHz, hbs=80m, hms=3m
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Okumura-Hata and Okumura-Hata and
Coefficient of Log(d) depends only on hbs
10 = attenuation (dB) in a decade (d=1 d=10)
The higher the BS, the lower the coefficient
30
32
34
36
38
40
42
44
0 20 40 60 80 100 120 140
base station height (m)
1
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Wireless Cellular NetworksWireless Cellular Networks(basics) (basics)
Part 2 – Cellular Coverage Concepts
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Coverage for a terrestrial Coverage for a terrestrial zonezone
1 Base StationN=12 channels •(e.g. 1 channel = 1 frequency)
N=12 simultaneous calls
d
Signal OK if Prx > -X dBmPrx = c Ptx d-4
greater Ptx greater d
BS
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Cellular coverageCellular coveragetarget: cover the same area with a larger number target: cover the same area with a larger number
of BSsof BSs
19 Base Station12 frequencies 4 frequencies/cell
Worst case:4 calls (all users in same cell)Best case:76 calls (4 users per cell)Average case >> 12 Low transmit power
Key advantages:•Increased capacity (freq. reuse)•Decreased tx power
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Cellular coverage Cellular coverage (microcells)(microcells)
many BS
Very low power!!Unlimited capacity!!
Usage of same spectrum(12 frequencies)(4 freq/cell)
Disadvantage: Location mobility management
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Cellular system architecture: Cellular system architecture: the GSM Network examplethe GSM Network example
high-level viewhigh-level view
Base Station
MSC
PSTNPublic switched
telephone network
PSTNPublic switched
telephone network
Base Station
MSC
PLMNPublic Land
Mobile Network
MSC = Mobile Switching Center = administrative region
MSC role: telephone switching central with special mobility management capabilities
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GSM system hierarchyGSM system hierarchy
BTS
BSCLOCATION AREA
MSC MSC region
Hierarchy: MSC region n x Location Areas m x BSC k x BTS
MSC: Mobile Switching CenterLA: Location AreaBSC: Base Station ControllerBTS: Base Transceiver Station
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GSM essential componentsGSM essential components
BTS
BTSBTS
BTS
BTS
BSC
BSC
MSC
VLRHLRAUCEIRGMSC
To fixed network (PSTN, ISDN, PDN)
OMC
MS Mobile StationBTS Base Transceiver StationBSC Base Station ControllerMSC Mobile Switching Center GMSC Gateway MSCOMC Operation and Maintenance CenterEIR Equipment Identity RegisterAUC Authentication CenterHLR Home Location RegisterVLR Visitor Location Register
MS
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Cellular capacityCellular capacity
Increased via frequency reuseFrequency reuse depends on interferenceneed to sufficiently separate cells
reuse pattern = cluster size (7 4 3): discussed later
Cellular system capacity: depends onoverall number of frequencies
Larger spectrum occupation frequency reuse patternCell size
Smaller cell (cell microcell picocell femtocell) = greater capacity
Smaller cell = lower transmission powerSmaller cell = increased handover management burden
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AB
CD
AB
CD
hexagonal cellshexagonal cells Hexagon:
Good approximation for circle
Ideal coverage patternno “holes” no cell superposition
AB
CD
AB
CD
AB
CA
AB
CD
AC
D
D
DB
Example case:Reuse pattern = 4
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Cells in real worldCells in real world
Shaped by terrain, shadowing, etcCell border: local threshold, beyond which neighboring BS signal
is received stronger than current one
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Reuse patternsReuse patternsReuse distance:
Key conceptIn the real world depends on
Territorial patterns (hills, etc)Transmitted power
» and other propagation issues such as antenna directivity, height of transmission antenna, etc
Simplified hexagonal cells model:reuse distance depends on reuse
pattern (cluster size)Possible clusters:
3,4,7,9,12,13,16,19,…
13
4
5
6
7
21
3
4
5
6
7
2
D R
Cluster: K = 7
12
3
4
12
3
4
12
3
4
D
K = 4
12
3
4
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Reuse distanceReuse distance
General formula Valid for hexagonal geometry K = cluster size D = reuse distance R = cell radius q = D/R =frequency reuse factor
3KRD
K q=D/R3 3,004 3,467 4,589 5,2012 6,0013 6,24
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ProofProof Distance between two cell
centers: (u1,v1) (u2,v2)
Simplifies to:
Distance of cell (i,j) from (0,0):
Cluster: easy to see that
hence:
21212
2
12 30sin)()(30cos)( oo uuvvuuD
30°
v
u
(1,1)
(3,2)
))(()()( 12122
122
12 vvuuvvuuD
RijjiD 322
ijjiDK R 222
KRD 3
ijjiDR 22
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K=7(i=2,j=1) K=4 (i=2,j=0)
K=13(i=3,j=1)
ClustersClustersClusters:• Number of BSs comprised in
a circle of diameter D• Number of BSs whose inter-
distance is lower than D
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Clusters (dim)Clusters (dim)
AB
CD
AB
CD
AB
CD
AB
CD
AB
CD
AB
C
AB
C
AB
CD
B
CD
AB
CD
AB
CD
B
CD
AB
CD
AB
CD
BD
BD
B
AB
AB
ABC
D
ABC
D
ABC
DABC
D
ABC
D
ABC
D
ABC
D2
2
2
2
2
2
3
2
323
23
2
3
32
3
RCK
K
C
DR
DKAKA
DH
HH
Aclusterarea
RAcellaarea
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Possible clustersPossible clustersall integer i,j valuesall integer i,j values
i j K=ii+jj+ij q=D/R1 0 1 1,731 1 3 3,002 0 4 3,462 1 7 4,582 2 12 6,003 0 9 5,203 1 13 6,243 2 19 7,553 3 27 9,004 0 16 6,934 1 21 7,944 2 28 9,174 3 37 10,544 4 48 12,005 0 25 8,665 1 31 9,64
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Co-Channel InterferenceCo-Channel Interference
Frequency reuse implies that remote cells interfere with tagged one
Co-Channel Interference (CCI) sum of interference from
remote cellsCB
AD
E
CB
AD
EF
G
C
AD
EF
AE
FG A
EF
G
CB
A
FG
CB
AD
small N as
(I)power signal ginterferin
(S)power signal
(I)power signal ginterferin )(Npower noise
(S)power signal
S
S
I
S
N
S
I
S
N
S
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CCI Computation - CCI Computation - assumptionsassumptions
Assumptions
NI=6 interfering cells NI=6: first ring interferers
onlywe neglect second-ring
interferers
Negligible Noise NS
S/N ~ S/I
d propagation law=4 (in general)
Same parameters for all BSsSame Ptx, antenna gains, etc
Key simplificationSignal for MS at distance RSignal from BS interferers at
distance D
RR
D
PowerPo
PowerPo
Dint
Dint ~ D
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CCI computationCCI computation
qNR
D
ND
R
N
D
R
I
S
N
S
III
N
k
I
111
cost
cost
1
Results depend on ratio q=D/R
(q=frequency reuse factor)
KRD 3
By using the assumptions of same cost and same D:
Alternative expression: recalling that
III N
KK
NKR
R
NI
S
N
S 22
33
1
3
1
USAGE: Given an S/I target, cluster size K is obtained
NI=6,=4 2
2
2
3
6
3K
K
I
S
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ExamplesExamples
target conditions: S/I=9 dB=4
Solution:
target conditions: S= 18dB=4.2
Solution:
33.2
3
2
6
3
894.710
4
2
9.0
KK
I
SK
K
I
S
I
S
763.53
10
23.121
78.7183log
6log103log5
23.1
KK
K
KdBI
S
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S/I computationS/I computationassuming assuming ηη=4 & 6 interferers only (first =4 & 6 interferers only (first
ring)ring)
K q=D/R S/I S/I dB3 3,00 13,5 11,34 3,46 24,0 13,87 4,58 73,5 18,79 5,20 121,5 20,812 6,00 216,0 23,313 6,24 253,5 24,016 6,93 384,0 25,819 7,55 541,5 27,321 7,94 661,5 28,225 8,66 937,5 29,7
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Additional interferersAdditional interferers
case K=4note that for each
cluster there are always NI=6 first-ring interferers
AB
CD
AB
CD
AB
CD
AB
CD
AB
CD
AB
C
AB
C
AB
CD
B
CD
AB
CD
AB
CD
B
CD
AB
CD
AB
CD
BD
BD
B
AB
AB
In CCI computation, contribute of additional interferers is marginal
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sectorizationsectorization
Directional antennas
Cell divided into sectors
Each sector uses different frequenciesTo avoid interference at sector
borders
PROS:CCI reduction
CONS: Increased handover rateLess effective “trunking” leads to
performnce impairments
Sector 1Laa ff ,1,
Sector 2LaLa ff 2,1,
Sector 3LaLa ff 3,12,
CELL a
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CCI reduction via CCI reduction via sectorizationsectorizationthree sectors casethree sectors case
CB D
E
CB D
EF
G
CD
EF
EF
G AE
FG
CB
A
FG
CB
AD
FG
Inferference from 2 cells, onlyInstead of 6 cells
A
A
A
A
77.4
32
120
120
dBI
SdB
I
S
I
S
D
R
I
S
omni
omni
o
o
With usual approxs (specifically, Dint ~ D)
Conclusion: 3 sectors = 4.77 dB improvement
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6 sectors6 sectors
60o Directional antennas
CCI reduction:1 interfereer only6 x S/I in the omni caseImprovement: 7.78 dB