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Validation of Specific Absorption Rate (SAR) Calculation in XFdtd® 6.0.
The recently published IEEE document P1528/D1.2 titled Recommended
Practice for Determining the Peak Spatial-Average Specific
Absorption Rate (SAR) in the Human Head from Wireless Communications
Devices: Measurement Techniques, sets standards for measuring
the SAR generated by wireless devices. One section of this
document regarding the calibration of the measurement system
contains a table of reference SAR values. Here the calibration
approach is simulated in XFdtd for comparison of the reference
SAR values.
The subject under test is a flat phantom comprised of a plastic
shell and a tissue-equivalent liquid. The phantom size is
set in the document as 22.5x15 cm for the frequency range
of 835-3000MHz. For lower frequencies a phantom of size 0.6x0.4
wavelengths is used. The material parameters for the tissue
equivalent liquid vary with frequency and are given in Table
1. The plastic shell should have a relative permittivity
less than 5 and a loss tangent less than 0.05. The plastic
shell thickness is defined as 2mm for frequencies in the 800-3000MHz
range and 6.5mm for lower frequencies. The tissue equivalent
liquid shall have a minimum depth of 15cm.
The phantom is to be exposed to the fields of an appropriately
sized dipole (see Table 2) which is
spaced 15 mm from the shell/liquid interface for frequencies
less than or equal to 1000MHz and 10 mm from the interface
for higher frequencies. The local SAR and 1 and 10 gram average
SAR values are to be determined for the location directly
above the feed of the dipole for a 1 W input power.
For the XFdtd simulation a 1mm cubical grid was chosen for
all simulation except 300MHz where a 1.5mm grid was used.
The plastic shell was defined as a dielectric with a relative
permittivity of 3.7 and no electrical conductivity. The phantom
and shell were sized appropriately based on the requirements
of the document. The dipole antenna was defined as two cylinders
of the specified radius with a single FDTD cell space between
them for the feed. The solid view of the XFdtd 6.0 geometry
is shown in Figure
1 while Figure
2 shows the actual mesh used in the calculation. The applied
excitation was a voltage source with a sinusoidal input. All
calculations were run for 16 full-amplitude cycles of the
sine wave. Following the simulation, the input power was adjusted
from the computed value to the specified 1W. The resulting
values are shown in Table 3 compared
to the reference values in the P1528 document. Images of the
Local SAR, 1g Averaged SAR, and 10g Averaged SAR in the first
plane of the liquid (with the shell hidden) for the 1800MHz
case are shown in Figures 3,
4, and 5.
Table 1. Tissue-equivalent
liquid parameters.
| Frequency (MHz) |
Relative Permittivity |
Electrical Conductivity |
| 300 |
45.3 |
0.87 |
| 450 |
43.5 |
0.87 |
| 835 |
41.5 |
0.90 |
| 900 |
41.5 |
0.97 |
| 1450 |
40.5 |
1.20 |
| 1800-2000 |
40.0 |
1.40 |
| 2450 |
39.2 |
1.80 |
| 3000 |
38.5 |
2.40 |
Table 2: Dipole antenna
dimensions
| Frequency (MHz) |
Length (mm) |
Diameter (mm) |
| 300 |
396.0 |
6.0 |
| 450 |
270.0 |
6.0 |
| 835 |
161.0 |
3.6 |
| 900 |
149.0 |
3.6 |
| 1450 |
89.1 |
3.6 |
| 1800 |
72.0 |
3.6 |
| 1900 |
68.0 |
3.6 |
| 2000 |
64.5 |
3.6 |
| 2450 |
51.5 |
3.6 |
| 3000 |
41.5 |
3.6 |
Table 3: Comparison of
Reference and Computed (with XFdtd 6.0) SAR Results for the
Flat Phantom test object
| Frequency (MHz) |
Reference Peak 1g SAR |
XFdtd Peak 1g SAR |
Reference Peak 10g SAR |
XFdtd Peak 10g SAR |
Reference Local SAR |
XFdtd Local SAR |
| 300 |
3.0 |
3.1 |
2.0 |
2.1 |
4.4 |
4.5 |
| 450 |
4.9 |
4.9 |
3.3 |
3.2 |
7.2 |
7.4 |
| 835 |
9.5 |
9.2 |
6.2 |
5.9 |
14.1 |
14.1 |
| 900 |
10.8 |
10.5 |
6.9 |
6.6 |
16.4 |
16.3 |
| 1450 |
29.0 |
28.0 |
16.0 |
15.2 |
50.2 |
50.5 |
| 1800 |
38.1 |
36.0 |
19.8 |
18.4 |
69.5 |
68.3 |
| 1900 |
39.7 |
37.8 |
20.5 |
19.1 |
72.1 |
71.4 |
| 2000 |
41.1 |
39.7 |
21.1 |
19.9 |
74.6 |
75.1 |
| 2450 |
52.4 |
52.4 |
24.0 |
23.3 |
104.2 |
109.9 |
| 3000 |
63.8 |
61.6 |
25.7 |
23.8 |
140.2 |
150.0 |
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