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IN-BUILDING PROPAGATION MODELLING73 HAROLD ST.
John Litva
January 31, 2007
ALMONTE, ON.
K0A 1A09290(613) 256-9290
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he road ahead.1. Basic Beamformin
2. McMaster propagation trials3. Ottawa adaptive beamforming trials
4. Warehouse/Enterprise propagation trials
5. In-building propagation models1. one-s ope mo e
2. Motif model
3. ParFlow model
6. Modelling buildings
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32-element, Multi-frequency
Propagation measurements based on in-building AOA and time-of-flight measurements
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Characteristics of the arra NOS OF ELEMENTS 32
ELEMENT SPACING 5.71 cm FIRST GRATING LOBES 15
STARTING FREQUENCY 8.05 GHz
NOS OF FREQUENCY STEPS 70 z
TOTAL BANDWIDTH 280 MHz
RANGE RESOLUTION 1.0 M (3ns delay)
UNAMBIGUOUS RANGE 75 M
synthesized 128-element array.
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Pro a ation in a hallwa
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Formation of a doublet
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Moving into a stochastic
r
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Channel models Propagation is a purely random Phenomenon
Hence, people talk about fading and de-correlation
Propagation is not repeatable, look at a trace of fading;its completely random
The best propagation Models are stochastic in nature
Channel entropy is very high(Q/T)
One has to develop weight coefficients once every frame
Thats why one needs very fast DSPs
One cannot predict propagation in an Urban Environment
Within cell propagation is indistinguishable from Out-of-cell
Propagation There is no hope of distinguishing between them
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Much of the environment is
r When you walk along a street in a city, the perspective
,
identify the fact that you are still in the same city. Remember that the frequency being used is 100,000 time
The buildings are fixed, they dont move.
You cant build just anywhere, you have to conform to a
When the transmit antenna is located below the roof-tops, the signals are guided by street channels
When water flows in a river, there can be a lot of localcomplexity, but since the water is guided by the river banksthere is order.
,
In LOS propagation, there are fixed scattering points thatdont move
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Proof-of-concept for
v r
Data logger Telemetry unit
VSG (GSM with
2 timelots
active)
Type N
SMA
0.141 coax
0.141 coax MS2MS2
Com y
MS1MS1Com z
Data link to Base
(802.11b.)DuplexerFilter
IEEE
488
LNA
Type N
SMA
SMA
0.141 coax
Cat 5
12 VDC 110 VAC
Inverter (500W)
12 VDC 110 VAC
Inverter (500W)
Com x
Spectrum
Analyzer
GPS
&
Time
Type N
SMA
0.141 coax
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rial siteCoverage
Area Building
North F
Building
E
Terry Fox
Dr.
Trial BTS Site, 359 Terry Fox
Dr.
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E ui ment confi uration
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RSSI measurements Uplink CIR performance is demonstrated in real time by using a
GSM frame timing RSSI is measured on all Rx time slots from the wanted and interferer mobiles.
Signal level/RSSI of wanted
Beamforming Off Beamforming On
.
mobile (P1)
Signal level of interferer
without beamforming (P2)
beamforming (P3)
CIRUL w/o ABF = P1 P2
CIRUL w/ ABF = P1 P3 TSTSTS6CIRUL* = P2 P3
* Approximate.
4 53
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Drive route45.3498
Mobile locations (10:17:15 to 10:19:46, Sept.9)
45.35 1
141
Desired mobile
Interfere
BTS
The dashed linesDefine the region of
45.3502
45.3504
de(deg)
21 CogencyBuilding
s a ow ng
The dotted lines
45.3506
45.3508
Latitu
41
101
121
were the wantedand unwanted anglesare very close. TheyVary from 15 to
45.351
45.3512
61
81
InnovanceBuilding
. .
75.9175 75.918 75.9185 75.919 75.9195 75.92 75.9205 75.921
Longitude (deg)
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RSSI measurements-20
-10Uplink BF performance (9:50:47 to 9:55:10, Sept.9, one interferer)
slot4MSW w/BF
Bm)
-60
-50
-40
-30
RSSI(dB) slot7
MSW wo/BF
RSSI(d
Non-Line-of-Sight
-40
-30
-20
-10
SSI(
dB)
slot4
slot7
I(d
Bm)
Slot 5
Slot 2
MSI w/BF
MSI wo/BF
0 20 40 60 80 100 120 140 160 180 200-60
-50R
40CIR gain
))
RS
0 20 40 60 80 100 120 140 160 180 2000
10
20
CIR
gain(dB
CIRUL(d
Location
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Downlink BF erformance1
Downlink BF performance (9:50:47 to 9:55:10, Sept.9, one interferer)
0.8
0.9
issa)
0.5
0.6
0.7
CDFU
L 17 dB
0.3
0.4
(%
CI
0
0.1
0.2
Pro 90% CIRDL > 12 dB
0 5 10 15 20 25 30 35
CIR gain (dB)
CIRUL (dB)
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PDF for the downlink:
0.8
0.9
1
0.6
0.7
CD
F
0.3
0.4
.
0.1
0.2
0 5 10 15 20 25 30 35
CIR Gain (dB)
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0.8
0.9
1
0.5
0.6
0.7
0.3
0.4
0
0.1
0.2
CIR Gain (dB)
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est #2: Downlink CDFDownlink BF performance (13:38:9 to 13:41:24, Sept.24, two interferers)
0.8
0.9
1
0.6
0.7
0.3
0.4
0.5CD
0.1
0.2
0 5 10 15 20 25 30 350
CIR gain (dB)
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Intersection oints-20
-10Uplink BF performance (13:43:15 to 13:47:20, Sept.24, two interferers)
slot4
0 20 40 60 80 100 120 140 160 180 200-60
-50
-40
-30
RSS
I(dB) s o
-40
-30
-20
-10
RSSI(dB)
slot5
slot2
0 20 40 60 80 100 120 140 160 180 200-60
-50
30
40CIR gain
B)
0 20 40 60 80 100 120 140 160 180 2000
10
20
CIR
gain
(d
Intersection Points
D &1st I D &2ndI D &2ndI D &1st I D &1st I
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Uplink CDF for the cases where there isoverlap between the wanted and unwantedsignals
CDF Uplink - Overlapping LOSs
0.8
0.6
ofUplinkData
CDFs
0.2
0.4CDF
0 5 10 15 20 25 30 350
CIR Gain
ULs
Mean = 16.8 dBStandard Dev = 6.5 dB
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Boyd WarehousePanoramic view of the warehouse
oor :
TenXcs entranceThrough this door go the giants of radio location
1/31/2007
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Warehouse interior
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Comparison of measured and
Amplitude [dB] Phase []
10
5
100
200
Am
Phas
20
15
v ,
v
100
0
v ,
r arg v( )
litude[d
B]
[degre
es]
0.5 1 1.5 2 2.525
ye v
0.5 1 1.5 2 2.5200
ye v
Distance along array [m] Distance along array [m]
xx 43= y = 2 264.026=The red curves give simulated values of amplitude and phase at the outputs of16-elements of the array antenna. The blue curves give the measured values ofamplitude an phase at the antenna elements. There is a close agreement between
1/31/2007
s mu a ons an measuremen s.
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Correlation functionsX ef12:= Y :=
Complex number which givesthe simulated volta e at element
v, v , v
15
v at distance, designated by t
Complex number which givesthe measured voltage at elementv and at nominal distance
t
0n
n t, n
=
=
A A 0.15:=
Correlation function of the measured
and simulated phases
Bt
15
Xn t
Yn
:= 15
=
This correlation function is used to do the fine estimatesof x
0n= t
0n
n t, n=
Et
200 Et
:=B 70 B:=
Correlation function whichuses the amplitude and phaseof the measured and simulated
1/31/2007
simulated voltagesCorrelation function of the amplitudesof the measured and simulatedvoltages
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Correlation function, U, for fine
4
41.5 m: Boyd: April 21, 2006
Estimated value of Y Estimated valuesX = 88.75m
Y = 0.944m
3
3.5
ion
Nominal values
X = 88mY = 1m
2
2.5
llationCoefficient
U t
lat
ion
func
Notice that theside lobe is downby 8 dB
1
1.5Corr
Corr
0 0.5 1 1.5 2 2.5 30
0.5
0
2.7270 yb t-
Y [m]
Nominal value of Y
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Ambi uities.lots of them88
Boyd Warehouse: Apr. 25, 2006: 88m
90
Ambiguities
94
92
latio
nNumber
Nv 1,
Course estimate
96
Corr
100
98
Range [m]
Nv 0,
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RSSI Propagation modelsn oor o e ngn oor o e ng
mpiric
al
One-Slope Model
SemiEmp.
Multi-Wall Model
Dominant Path Model
H
bri
Ray Optical Models + Multi-Wall Model
SemiDet.
Motif Model ~ Wave Oriented Ray Model
inistic
brid
Method of Moment + Ra -O tical Models
Ray Optical Models Ray-TracingRay-Launching
Deter H
Transmission Line Matrix ParFlow
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COST231
(1)
where:
LOSM...........Predicted signal loss (dB)
L0(d0).........Signal loss at distance d0 from transmitter (dB) n ................ ower ecay ac or -
d ................Distance between antennas (m)
d0 ...............Reference distance between antennas (usually 1 m) (m)
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Multi-wall model
where:
LFloors = afkf (4)
LMWM .........Predicted signal loss (dB)
...............
LWalls..........Contribution of walls to total signal loss (dB)
LFloors.........Contribution of floors to total signal loss (dB)
awi..............Transmission loss factor of one wall of i-th kind (dB)
kwi..............Number of walls of i-th kind (-) I.................Number of wall kinds (-)
af...............Transmission loss factor of one floor (dB)
................ um er o oors
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Parsons Model
Qfi SAdY 5.27log6.17log6.177.37
1010900, ++=
Qfi SAdY 9.20log3.23log0.409.2710101800,
++=
i SAdY 3.27log1.16log0.409.7
10102300 ++=
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Motif ModelMartin Klepal, Czech Technical University in Prague
Motif 2D or 3D environments are composed of square or cubic grid elements,
res ectivel .
Each grid element characterises the local mean environment behaviour by appropriateprobabilistic parameters.Model - Describing an Environment (2)
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Motif Model
Common situationDrain
- a wall surrounded by many other
undefined obstacles
Door
Cabinet
CabinetCabinet
Shelf
TablePerson Cluster of obstaclesCluster of obstacles
Plane IncidentWave
M o t i f P a r a m e t e r s
P rA
P r o b a b i li ty o f A b s o r p t io n
Cluster of obstaclesCluster of obstacles -- MotifMotif
O v e ra l l P ro b a b i l it y
R a d i a t io n P a t t e rn
R
P rD S .. P r o b . o f D i f fu s e S c a t t e r in g
P l a n e I n c id e n t W a v e 3D power reradiation by a cluster3D power reradiation by a cluster
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Motif Model
Ray propagation takes advantages of the modified simple line-drawing technique
utilizing environment division into a grid.
no complicated calculations of reflection or diffraction are used while all theeffects including diffuse scattering are taken into account
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Motif Model e ng va ua on
BuildingBuilding ofof Hotel DiplomatHotel Diplomat
DifferenceDifferenceMeasurementMeasurement PredictionPrediction
MeanMeanErrorError(dB)(dB)
StandardStandardDeviationDeviation
(dB)(dB)
General MotifGeneral MotifParametersParameters 0.70.7 4.94.9
THE PARFLOW THEORY
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THE PARFLOW THEORY
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The binary tree is built starting from the head node (top).he division recursion acts on each node along the main
Comparison between predictions
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Comparison between predictions
.
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ParFlow simulations
What is a building?
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What is a building?>200 different t es buildin s listed for NYC
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Hi h-rise buildin s
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Ima e ca ture of buildin s
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Almonte hos ital
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Almonte hos ital extension
Court
CeilingHt. 11
Hallway
Brick,insulation,
11
7
11 x12.5
Patient room
supportwall, anddrywall
153
Window (partially tinted)External story ht.
= 12
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Almonte hos ital
Windows indicate location of rooms
Outer dimensions are captured from the image
Ratio of window area to wall area
Outer envelope of the building
Window area = 8 x 6.7 x 16 = 857.6 ft2
a area = x - . = .
Ratio = 5 dB
Propagation loss
Window ~ -5 dB (tinted) Walls ~ -14 dB
~
60% of the energy enters through the windows