project: ieee 802.15 study group for wireless personal area networks (wpans)
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Project: IEEE 802.15 Study Group for Wireless Personal Area Networks (WPANs) Submission Title: [ Ultra-Wideband Channel Model for Farm/Open-Area Applications ] Date Submitted: [ 11 May, 2004 ] - PowerPoint PPT PresentationTRANSCRIPT
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 1
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Project: IEEE 802.15 Study Group for Wireless Personal Area Networks (WPANs)Project: IEEE 802.15 Study Group for Wireless Personal Area Networks (WPANs)
Submission Title: [Ultra-Wideband Channel Model for Farm/Open-Area Applications]Date Submitted: [11 May, 2004]Source: [Shahriar Emami, Celestino A. Corral, Gregg Rasor]: Company1 [Freescale Semiconductor], Address [8000 W. Sunrise Blvd., Plantation, FL 33322], Voice:[(954) 723-3854], FAX: [(954) 723-3883]Re: [Channel Model Submission]Abstract: [An ultra-wideband channel model for open area/farm applications is submitted. The channel model is based on ray tracing that captures signal descriptors including frequencies. The rationale behind the channel model is developed and presented in support of the presentation.]
Purpose: [An understanding of the open area outdoor environment for ultra-wideband (UWB) signal coverage is needed for 802.15 TG4a. This channel model should assist in predicting UWB range and proper signal design for open area applications.]
Notice: This document has been prepared to assist the IEEE P802.15. It is offered as a basis for discussion and is not binding on the contributing individual(s) or organization(s). The material in this document is subject to change in form and content after further study. The contributor(s) reserve(s) the right to add, amend or withdraw material contained herein.Release: The contributor acknowledges and accepts that this contribution becomes the property of IEEE and may be made publicly available by P802.15.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 2
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Ultra-Wideband Channel Modelfor Farm/Open-Area Applications
Understanding UWB Propagation
in Open Areas Subject to
Selected Environmental Factors
The presenters wish to acknowledge the support and contributions of:
• Glafkos Stratis/Motorola
• Salvador Sibecas/Motorola
Shahriar Emami, Celestino A. Corral, Gregg Rasor
Freescale Semiconductor
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 3
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Outline
• Ultra-wideband Outdoor Channel Model Status• Special Considerations
– Approach– Frequency Selection– Simulation Setup
• Simulation Results– Ground conditions– Channel Impulse Response and Ray Statistics– Coverage
• Summary and Conclusions • Proposed Continuing Investigations
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 4
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Channel Model Status
• Prior Efforts:– Two-ray UWB path loss model:
• S. Sato and T. Kobayashi, “Path-loss exponents of ultra wideband signals in line-of-sight environments,” IEEE802.15-04-0111-00-004a, March 2004.
– Deterministic UWB channel model based on ray tracing approach:• B. Uguen, E. Plouhinec, Y. Lostanlen, and G. Chassay,
“A deterministic ultra wideband channel modeling,” 2002 IEEE Conf. Ultra Wideband Syst. Tech.
We shall show this in simulation
We use approach considered here
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 5
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Special Considerations
• Farm areas feature isolated clusters of scatterers
• Material properties may change with frequency. (For our simulations, we assume material properties constant over frequency.) In addition, the outdoor channel is subject to environmental changes– Seasonal changes (snow, ice, etc. in some
regions)– Rain/wet conditions
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 6
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Different Absorption Regions
-6 -4 -2 0 2 4 6 8 10 12 14 16 18
Conduction
Space
Charge
Polarization
Dipole and
Ionic
Relaxation
Atomic Electronic
Absorption
60Hz
Frequency Range
Of Interest
Dielectric practically constant over frequency range of interest.
Log frequency (Hz)
R. C. Dorf (Ed.), The Electrical Engineering Handbook, 2nd Ed., Boca Raton, Florida: CRC Press, 1997.
We assume no dielectric changes
over frequency
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 7
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Approach
• Use deterministic 3-D ray tracing simulator - Employs
– geometric optics– uniform theory of diffraction (UTD)
– Generates• Received signal strength• Ray statistics (path length/delay)• Signal descriptors include frequency, polarization, etc.
• UWB channel sounding is achieved by superposition of NB channel sounding
- Conventional channel sounding
- FCC emissions mask scaled channel sounding
M. F. Iskander and Z. Yun, “Propagation prediction models for wireless communication systems,” IEEE Trans. Microwave Theory Tech., vol. 50, pp. 662—673, March 2002.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 8
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Frequency Selection
Channel Sounding “High-Pass” Sounding
0 dBm
-14.8-13.8
-12.8 -11.4 -11.2
“Band-Pass” Sounding
-14.8-13.8
-12.8 -11.4 -11.2
Energy of band concentrated in high band frequency
Energy of band concentrated in geometric center frequency
3.10 4.24 5.34 6.72 8.64 10.6 3.10 4.24 5.34 6.72 8.64 10.6
3.62 4.76 5.99 7.62 9.57
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 9
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Set-Up3-D omni antenna pattern used
Omni pattern assumed at all frequencies
Provides worst-case delay modeling
Farm area consists of two-story wood home and metal grain silo. Ground is not flat; has slight variations in height.
omni antenna above house
omni antenna near ground
• Receiver grid placed around home, 200m X 200m
• Receiver spacing was 4m X 4m
• Receiver height was at 1.3m
• For omni antenna above house, antenna was at 12.5m height
• For omni antenna near ground, antenna was at 1.5m height.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 10
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Coverage ResultsLowest Frequency – 4.24 GHz
200 m
200 m
• Highest level -64.4 dBm
• Shadowing due to metal silo evident
• Ripple due to two-ray phenomenon evident
Dry soil Wet soil and wet roof
• Highest level -66.5 dBm
• Smoother ripple closer to antenna
• Impact of roof more significant
TX power = 0 dBm TX power = 0 dBm
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 11
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Coverage ResultsFull Frequencies -- Channel Sounding
Dry soil
• Highest level -64.4 dBm
• Some deep fades are eliminated, others softened
• Ripple due to two-ray phenomenon still evident, although smooth ripple closer
• Highest level -66.5 dBm
• Higher signals closer to antenna
• Shadowing due to silo and roof still significant
Wet soil
TX power = 0 dBm TX power = 0 dBm
Dry/wet conditions are fairly similar
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 12
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Coverage“High-pass” and “Band-pass” Sounding
Dry soil
• High-pass sounding
• Highest level -61.8 dBm
• Significant shading by house as well as silo
Dry soil
• Band-pass sounding
• Highest level -60.2 dBm
• Range for -75 dBm sensitivity is quite low, on the order of 15 m.
High-pass and band-pass sounding are
similar
TX antenna placed at 1.5m height and at the side of the house
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 13
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation--Validation
• Powers in the different frequency bands are summed together
• Received power profile in agreement with the work of Sato and Kobayashi
TX antenna placed at 1.5m height and at the side of the house
1 0 1 0 0 1 0 0 0
4 0
6 0
8 0
1 0 0
1 2 0
1 4 0
1 6 0
D i s t a n c e [ m ]
Pat
h lo
ss [
dB]
100
101
102
103
-120
-110
-100
-90
-80
-70
-60
-50
Po
wer
(d
Bm
)
Transmitter-Receiver Separation (m)
UWB Path Loss
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 14
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Ground Conditions
-180 -160 -140 -120 -100 -80 -600
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1Constrained Channel Sounding
Power (dBm)
Pro
bab
ilit
y (X
< X
o)
DryWet
• Ground conditions (wet or dry) has almost no impact on received signal power or delay spread.
• Subsequent simulations were assuming dry conditions
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 15
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Channel Impulse Response
• CIR is similar to two-ray model.
0 20 40 60 80 100 120 140 160 180-1
0
1
2
3
4
5x 10
-7
t (ns)
Rec
eive
d A
mp
litu
de
(V)
CIR of Real Part of the received signal
0 20 40 60 80 100 120 140 160 180-8
-6
-4
-2
0
2
4
6x 10
-8
Rec
eive
d A
mp
litu
de
(V)
CIR of Imaginary Part of the received signal
t (ns)
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 16
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Channel RF Parameters
Scenario
A
Scenario
B
Received Power
(dBm)
-83
-74
Scenario
A
Scenario
B
Mean
Excess
Delay
(ns)
380
365
RMS Delay
(ns)
19 26
- Scenario A: transmit antenna is placed on the top of farm house
- Scenario B: transmit antenna is placed along the side of the house
Table I. 90 percentile received power Table II. 90 percentile delay spread
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 17
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Ray Statistics
• Statistics of the two rays are found to be Rayleigh distributed.
0 0.5 1 1.5
x 10-6
0
100
200
300
400Histogram of I of the Largest Component
0 0.5 1 1.5
x 10-6
0
100
200
300
400Histogram of Q of the Largest Component
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5
x 10-7
0
100
200
300
400Histogram of I of the Second Largest Component
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5
x 10-7
0
100
200
300
400Histogram of Q of the Second Largest Component
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 18
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Channel Sounding
• Channel (uniform) sounding leads to larger received power as compared to constrained channel (FCC-mask compliant) sounding.
-180 -160 -140 -120 -100 -80 -600
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1Constrained Channel Sounding
Power (dBm)
Pro
bab
ilit
y (X
< X
o)
DryWet
-180 -160 -140 -120 -100 -80 -600
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Pro
bab
ilit
y (X
< X
o)
Power (dBm)
Channel Sounding
DryWet
Over 10dB difference
FCC-mask complaint
Uniform sounding
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 19
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—“High-pass” or “Band-pass” Sounding
• “Band-pass” sounding results in +1 dB higher received power compared to “high-pass” sounding.
-160 -140 -120 -100 -80 -60 -400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Power (dBm)
Pro
bab
ilit
y (X
< X
o)
High Pass Channel SoundingBand Pass Channel Sounding
High-pass and band-pass sounding are
similarHigh-pass Band-pass
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 20
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Coverage
100x100 30x30
Coverage
(%)
85 85
Table III. % grid Coverage, if the receiver sensitivity is -90 dBm.
-120 -110 -100 -90 -80 -70 -60 -500
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Power (dBm)
Pro
bab
ilit
y (X
< X
o)
Constrained Channel Sounding (30mx30m)
-120 -110 -100 -90 -80 -70 -60 -500
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1Constrained Channel Sounding
Power (dBm)
Pro
bab
ilit
y (X
< X
o)
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 21
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Simulation Results—Channel Model
CM1* CM2* CM3* I mean 1.4092e-007 3.1052e-008 -5.8368e-009
Q mean -1.8287e-008 5.9910e-009 -4.2345e-009
MED (ns) 22.654 35.491 251.53
RMS Delay
(ns)
20 3.5565 5.0733
* The transmitter receiver separation distances are 5, 15 and 75 meters in CM1, CM2 and CM3, respectively.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 22
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Summary and Conclusions
UWB Ray Tracing:• Ray tracing with realistic antennas and appropriate material properties was
implemented.• Analyses included all ray statistics/parameters (ray physics).• CIR of UWB channel is found by superposition of CIR of individual bands
with appropriate power weighting.
Channel Modeling Results:• 5-band approach is adequate for predicting outdoor coverage in farm
scenario as verified by prior two-ray modeling.• “High-pass” sounding yields most conservative results.• RF parameters appear almost insensitive to ground material/conditions.• 100m range achievable with -90dBm RX sensitivity.• CIR is similar to that of two-ray model. RMS delay depends on location of
antenna and statistics of the rays.• Two-ray statistics are verified to have Rayleigh distribution.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 23
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Ongoing Investigations
• Incorporate uplink simulations.
• Alternative frequency domain based approach.
• Measurement and verification.
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 24
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Back-up Slides
May 7, 2004
Shahriar Emami, Freescale SemiconductorSlide 25
doc.: IEEE 802.15-04-0215-00-004a
Contribution
Material PropertiesPellat-Debye Equations for loss at single relaxation time. Real permittivity exhibits low-
pass frequency response. Imaginary part exhibits band-pass response. Regions can be separated for different relaxation times.
Temperature effects are not modeled, but only affected by change in density of dielectric material.
Reference Data for Engineers: Radio, Electronics, Computer & Communications, 8th Ed., Carmel, Indiana: SAMS, Prentice-Hall Computer Pub., 1993.