modélisation électromagnétique des interactions ondes
TRANSCRIPT
Research & Development March 2006
Modélisationélectromagnétique des interactions ondes personnes
Man-Faï Wong, Joe WiartFrance Télécom Recherche & Dé[email protected]
Research & Development March 2006
Context
Tremendous development of mobile communicationsPublic concerns about health impactAuthorities have established guidelines and
recommendationsGuidelines exist (ICNIRP, IEEE)In 1999 EU council has output recommendationsState of the art dosimetry basis for the standards
No evidence of health effects below the limitsWorldwide Research goes on
High quality dosimetry needed
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Outline
The objectives of DosimetryMethodologySamples of dosimetry applied to
Mobile phonesBase station antennas
Challenges of future radio systems
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Estimate the field levels induced by a mobile phone and a base station in operational mode
Know the field levels in the tissues to allow biologists to conclude
The objectives of Dosimetry
Estimate the fields or theabsorbed power to analyse the complianceto standards
SAR < 2 Watts/kg ?
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Methodology
Characterisation of the sources
Physical Quantities
Methods
E field, H field, Power density, SAR
Distribution, Absolute Value
Frequency, Modulation, time-
varying characteristics
Near field/Far field
Huygens principle
Simulation tools : what if scenarios,
extrapolation, cost effective
Measurement tools : real, asked for
by the public
Complementary
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Mobile numerical dosimetry
MRI segmentation for head tissue modellingPhone modelling
FDTD (Finite Difference Time Domain, Yee 1966), method of choice
E field SAR averagedover 10g of tissue
²2ESA R σρ
=
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Dosimetry and Children exposure
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SAR in children head
RNRT RNRT
ADONIS ADONIS
The questionsIs child exposure comparable to adult exposure?Is SAM conservative for children?
To answer we need children head models to compare to adult and SAM
- heads derived from adult?- heads coming from MRI?
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Child Head model based on adult
Morphing based on external shape is possible
Nevertheless organs have specific growth and analysis
using morphing approach has to be handled
carefully.
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Phone positioning and ear shape influence
The positioning of the phone inducesuncertainties
Ear dimensions
Length auricle (mm)
Width auricle (mm)
Depth ear (mm)
Case 1 56 33 2 Case 2 58 35 4 Case 3 60 37 6 Case 4 63 38 8 Case 5 59 33 10
E ar L en g th o f th e au ric le
W id th o f th e au ric le
D ep th o f th e ear
1 2 y . o ld C h ild h ead
5 9 m m 3 3 m m 1 0 m m
1 2 yea rs a g e c la ss
5 9 ,6 ± 3 ,6 (m m )
3 5 ,3 ± 2 ,3 (m m )
6 ± 4 (m m )
T A B L E I: E A R D IM E N S IO N S O F C H IL D H E A D O F 1 2 Y E A R S O L D
The ear shape inducesuncertainties
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Handset model
PATCHPATCH
Monopole + boxMonopole + box
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Child like versus SAM
Normalized Max SAR over 10 g at 1900 MHz
00,20,40,6
0,81
1,2
Sam cheek Sam Tilt Child cheek Child tilt
Normalized Max SAR over 10 g at 835 MHz
00,20,40,6
0,81
1,2
Sam cheek Sam Tilt Child cheek Child tilt
Study carried out with the international intercomparison
SAM can be considered as conservative
The IEEE Child like head is coming from Japan (Nagoya Institute of Technology)
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Children Head models based on MRI
December 2004 model developped- 4 years old- 5 years old- 9 years old- 12 years old
4 yearsold
5 yearsold
12 yearsold
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Comparisons
Modèle tête
Freq. (MHz)
Tête Adulte
CL 12 ans
Child 12 ans
CL 4ans
Child 4 ans
900 58 % 59 % 53 % 55 % 58 % 1800 32 % 34 % 32 % 28 % 36 % 2100 42 % 45 % 40 % 42 % 46 % 835 55 % 51 % 60 % 53 % 60 % 1900 35 % 37 % 44 % 30 % 50 %
adulte 12 ans 4 ans CL 12 ans CL 4 ans
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Comparisons
0
0,5
1
1,5
2
900 1800 2100 835 1900Frequency "MHz"
Peak
SA
R o
ver
10g
(W/k
g) Adult head CL 12 years old 12 years oldCL 4 years old 4 years old
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Adult head CL 12 y.o 12 y.o CL 4 y.o 4 y.o
Peak
SA
R ov
er 1
g (W
/kg)
Skin Muscle Bone CSF Brain
900 MHz
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Whole body exposure ofworkers
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Hybrid MoM/FDTD
Two stepsSource modeling with MoM or
other technique or measurementFDTD calculation of SAR with
incident field on Huygens box
One-way coupling
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Exposure to UMTS antenna
177 cm
"Zubal"• 3.6 mm x 3.6 mm x 3.6 mm• 78 kg• 31 tissues
56.6 cm
12.6 cm
14 cm
4.2 cm
5.6 cm
UMTS (2140 MHz)• FEKO •7 cm dipoles (4)• Quarter wavelength fromreflector
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Antenna modeling comparison
FDTD FEKO + FDTD Différence S (W/m2)
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Electric field strength distribution comparison
Antenna in free space Antenna with the body
Observation plane
Observation plane
30cm
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SAR distribution comparison
FDTD FEKO + FDTD
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Comparisons FDTD vs FEKO+FDTD
0 20 40 60 80 1002
2.5
3
3.5
4
4.5
5
5.5
who
le b
ody
SA
R (
mW
/Kg)
Distance (cm)
FDTDFDTD + FEKO
0 20 40 60 80 1000
0.1
0.2
0.3
0.4
0.5
0.6
0.7
SA
R10
g with
in th
e tr
unc
(W/K
g)
Distance (cm)
FDTDFDTD + FEKO
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Dosimetry and new usage
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Dosimetry and body worn
Body Worn: Is the "head" liquid applicable to body worn estimation?
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Multilayer model : plane waves
Layers thickness and occurrence coming from VHMulti-layers approachComparison to homogeneous structure
Plane Wave
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Plane waves results
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Multlayer model: dipole
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Dipole results (1/3)
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Dipole results (2/3)
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Dipole results (3/3)
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Dosimetry and base station antennas
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Human exposure from Base station
Public concerns on fields emitted by BSA close to living areasExpert groups recommend information
EMF VisualEMF Visual
Field levelsPublic Compliance Boundary
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Specific antenna model is needed
Near field is able to be described using full wave analysis
These approaches ( MoM, FDTD, FEM…) - Are accurate - Quite heavy compared to the objective- Should be waste of time if the environment is not perfectly known
Far field gain is easy to use but inaccurate in the near fieldNew and specific approach is needed in the vicinity of the base station
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Specificity of radio base station
Sub-antenna
λλ
λ 22;2=≥≈
DRD
∑=
≅cellsN
i
icell PEPE
1)()(
Far field zone of sub-antenna :
( ) ( )iijkR
i
iiicell
icelli
cellie
RGP
PE φθρφθ
,ˆ,30)( −≅
the field is the superposition of the field emitted by each sub-antenna
P
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Synthesis problemGiven the antenna characteristics (sub-antennas are known), find the power distribution
Genetic Algorithm can be used
The cost function based on the maxima of the far field gain
p
r1
r2
r3
r4
α12 Pin
α22 Pin
α32 Pin
α42 Pin
(b)
(a)
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Real antenna model K739636
Optimized power feedpattern (amplitude)
Optimized power feed pattern (phase)
E field 5m in front of the antennaon a vertical line
Compliance distance vs Input Power
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Perfectly matched model
Synthesis problem : “Given the antenna characteristics, find
the sub-antennas (sub-antenna gain patterns and the power
distribution)”
Spherical harmonics decomposition of the sub-antennas and
of the whole antenna
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Spherical waves expansion
Spherical modes spectrum: optimal representation of the EM fields
∑∑ ∑= = −=
=2
1 1),,(
s
N
n
n
nmsmnsmn rFE φθζr
y
x
O
O'
x'
y'
z'A
[ ]⎟⎟⎟⎟⎟
⎠
⎞
⎜⎜⎜⎜⎜
⎝
⎛
=
⎟⎟⎟⎟⎟
⎠
⎞
⎜⎜⎜⎜⎜
⎝
⎛
×
−
NNN
N
sub
subMM MM
2
101
111
2
1
321
ζ
ζζ
χ
χχ
MML
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K 739662
MeasurementMeasurement
Optimal modelOptimal model
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Reduced modelBase station antenna
8 cells96 modes / cell1 λ spaced
4 cells160 modes / cell2 λ spaced
P
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Challenges in Electromagnetic ModellingFine details of the field (distribution and absolute levels)
from the source (close to tissues)in the tissues
Need of fine tissue modellingSegmentation <1mmHead models for children
Staircasing of FDTD issue, modelling of the sourceSubgriddingAdvanced numerical algorithmsHybridization of techniquesCoupling to other physics
(thermal, cellular, …)